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md_nvt_lj.f90
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md_nvt_lj.f90
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! md_nvt_lj.f90
! Molecular dynamics, NVT ensemble
PROGRAM md_nvt_lj
!------------------------------------------------------------------------------------------------!
! This software was written in 2016/17 !
! by Michael P. Allen <[email protected]>/<[email protected]> !
! and Dominic J. Tildesley <[email protected]> ("the authors"), !
! to accompany the book "Computer Simulation of Liquids", second edition, 2017 ("the text"), !
! published by Oxford University Press ("the publishers"). !
! !
! LICENCE !
! Creative Commons CC0 Public Domain Dedication. !
! To the extent possible under law, the authors have dedicated all copyright and related !
! and neighboring rights to this software to the PUBLIC domain worldwide. !
! This software is distributed without any warranty. !
! You should have received a copy of the CC0 Public Domain Dedication along with this software. !
! If not, see <http://creativecommons.org/publicdomain/zero/1.0/>. !
! !
! DISCLAIMER !
! The authors and publishers make no warranties about the software, and disclaim liability !
! for all uses of the software, to the fullest extent permitted by applicable law. !
! The authors and publishers do not recommend use of this software for any purpose. !
! It is made freely available, solely to clarify points made in the text. When using or citing !
! the software, you should not imply endorsement by the authors or publishers. !
!------------------------------------------------------------------------------------------------!
! Takes in a configuration of atoms (positions, velocities)
! Cubic periodic boundary conditions
! Conducts molecular dynamics using a measure-preserving algorithm for the Nose-Hoover equations
! Nose-Hoover chains are used, following Martyna et al, Molec Phys, 87, 1117 (1996)
! and Tuckerman et al J Phys A, 39, 5629 (2006)
! To keep this example reasonably simple, we do not subdivide the timesteps with a
! Suzuki-Yoshida decomposition, as described in those papers
! Uses no special neighbour lists
! Reads several variables and options from standard input using a namelist nml
! Leave namelist empty to accept supplied defaults
! Positions r are divided by box length after reading in and we assume mass=1 throughout
! However, input configuration, output configuration, most calculations, and all results
! are given in simulation units defined by the model
! For example, for Lennard-Jones, sigma = 1, epsilon = 1
! Despite the program name, there is nothing here specific to Lennard-Jones
! The model is defined in md_module
USE, INTRINSIC :: iso_fortran_env, ONLY : input_unit, output_unit, error_unit, iostat_end, iostat_eor, &
& COMPILER_VERSION, COMPILER_OPTIONS
USE config_io_module, ONLY : read_cnf_atoms, write_cnf_atoms
USE maths_module, ONLY : random_normals
USE averages_module, ONLY : run_begin, run_end, blk_begin, blk_end, blk_add
USE md_module, ONLY : introduction, conclusion, allocate_arrays, deallocate_arrays, &
& force, r, v, f, n, potential_type
IMPLICIT NONE
! Most important variables
REAL :: box ! Box length
REAL :: dt ! Time step
REAL :: r_cut ! Potential cutoff distance
REAL :: temperature ! Specified temperature
REAL :: g ! Number of degrees of freedom
REAL :: tau ! Thermostat time scale
INTEGER, PARAMETER :: m = 3 ! Number of Nose-Hoover chain variables
REAL, DIMENSION(m) :: q ! Thermal inertias
REAL, DIMENSION(m) :: eta ! Thermal coordinates (needed only to calculate conserved quantity)
REAL, DIMENSION(m) :: p_eta ! Thermal momenta
! Composite interaction = pot & cut & vir & lap & ovr variables
TYPE(potential_type) :: total
INTEGER :: blk, stp, nstep, nblock, ioerr
REAL, DIMENSION(3) :: vcm
CHARACTER(len=4), PARAMETER :: cnf_prefix = 'cnf.'
CHARACTER(len=3), PARAMETER :: inp_tag = 'inp', out_tag = 'out'
CHARACTER(len=3) :: sav_tag = 'sav' ! may be overwritten with block number
NAMELIST /nml/ nblock, nstep, r_cut, dt, temperature, tau
WRITE ( unit=output_unit, fmt='(a)' ) 'md_nvt_lj'
WRITE ( unit=output_unit, fmt='(2a)' ) 'Compiler: ', COMPILER_VERSION()
WRITE ( unit=output_unit, fmt='(2a/)' ) 'Options: ', COMPILER_OPTIONS()
WRITE ( unit=output_unit, fmt='(a)' ) 'Molecular dynamics, constant-NVT ensemble'
WRITE ( unit=output_unit, fmt='(a)' ) 'Particle mass=1 throughout'
CALL introduction
! Set sensible default run parameters for testing
nblock = 10
nstep = 20000
r_cut = 2.5
dt = 0.005
temperature = 1.0 ! specified temperature
tau = 2.0 ! desired thermostat timescale
! Read run parameters from namelist
! Comment out, or replace, this section if you don't like namelists
READ ( unit=input_unit, nml=nml, iostat=ioerr )
IF ( ioerr /= 0 ) THEN
WRITE ( unit=error_unit, fmt='(a,i15)') 'Error reading namelist nml from standard input', ioerr
IF ( ioerr == iostat_eor ) WRITE ( unit=error_unit, fmt='(a)') 'End of record'
IF ( ioerr == iostat_end ) WRITE ( unit=error_unit, fmt='(a)') 'End of file'
STOP 'Error in md_nvt_lj'
END IF
! Write out run parameters
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Number of blocks', nblock
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Number of steps per block', nstep
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'Potential cutoff distance', r_cut
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'Time step', dt
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'Specified temperature', temperature
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'Thermostat timescale', tau
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Nose-Hoover chain length', m
! Read in initial configuration and allocate necessary arrays
CALL read_cnf_atoms ( cnf_prefix//inp_tag, n, box ) ! First call is just to get n and box
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Number of particles', n
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'Simulation box length', box
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'Density', REAL(n) / box**3
CALL allocate_arrays ( box, r_cut )
CALL read_cnf_atoms ( cnf_prefix//inp_tag, n, box, r, v ) ! Second call gets r and v
r(:,:) = r(:,:) / box ! Convert positions to box units
r(:,:) = r(:,:) - ANINT ( r(:,:) ) ! Periodic boundaries
vcm(:) = SUM ( v(:,:), dim=2 ) / REAL(n) ! Centre-of mass velocity
v(:,:) = v(:,:) - SPREAD ( vcm(:), dim = 2, ncopies = n ) ! Set COM velocity to zero
! Initial values of thermal variables
CALL RANDOM_INIT ( .FALSE., .TRUE. ) ! Initialize random number generator
g = REAL ( 3*(n-1) )
q = temperature * tau**2
q(1) = g * temperature * tau**2
WRITE ( unit=output_unit, fmt='(a,t40,*(f15.6))' ) 'Thermal inertias Q', q
eta(:) = 0.0
CALL random_normals ( 0.0, SQRT(temperature), p_eta(:) )
p_eta(:) = p_eta(:) * SQRT(q(:))
! Initial forces, potential, etc plus overlap check
CALL force ( box, r_cut, total )
IF ( total%ovr ) THEN
WRITE ( unit=error_unit, fmt='(a)') 'Overlap in initial configuration'
STOP 'Error in md_nvt_lj'
END IF
! Initialize arrays for averaging and write column headings
CALL run_begin ( calc_variables() )
DO blk = 1, nblock ! Begin loop over blocks
CALL blk_begin
DO stp = 1, nstep ! Begin loop over steps
CALL u4_propagator ( dt/4.0, m, 1 ) ! Inwards order
CALL u3_propagator ( dt/2.0 )
CALL u4_propagator ( dt/4.0, 1, m ) ! Outwards order
CALL u2_propagator ( dt/2.0 )
CALL u1_propagator ( dt )
CALL force ( box, r_cut, total )
IF ( total%ovr ) THEN
WRITE ( unit=error_unit, fmt='(a)') 'Overlap in configuration'
STOP 'Error in md_nvt_lj'
END IF
CALL u2_propagator ( dt/2.0 )
CALL u4_propagator ( dt/4.0, m, 1 ) ! Inwards order
CALL u3_propagator ( dt/2.0 )
CALL u4_propagator ( dt/4.0, 1, m ) ! Outwards order
! Calculate and accumulate variables for this step
CALL blk_add ( calc_variables() )
END DO ! End loop over steps
CALL blk_end ( blk ) ! Output block averages
IF ( nblock < 1000 ) WRITE(sav_tag,'(i3.3)') blk ! Number configuration by block
CALL write_cnf_atoms ( cnf_prefix//sav_tag, n, box, r*box, v ) ! Save configuration
END DO ! End loop over blocks
CALL run_end ( calc_variables() ) ! Output run averages
CALL force ( box, r_cut, total )
IF ( total%ovr ) THEN ! should never happen
WRITE ( unit=error_unit, fmt='(a)') 'Overlap in final configuration'
STOP 'Error in md_nvt_lj'
END IF
CALL write_cnf_atoms ( cnf_prefix//out_tag, n, box, r*box, v ) ! Write out final configuration
CALL deallocate_arrays
CALL conclusion
CONTAINS
SUBROUTINE u1_propagator ( t ) ! U1: velocity Verlet drift step propagator
IMPLICIT NONE
REAL, INTENT(in) :: t ! Time over which to propagate (typically dt)
r(:,:) = r(:,:) + t * v(:,:) / box ! Positions in box=1 units
r(:,:) = r(:,:) - ANINT ( r(:,:) ) ! Periodic boundaries
END SUBROUTINE u1_propagator
SUBROUTINE u2_propagator ( t ) ! U2: velocity Verlet kick step propagator
IMPLICIT NONE
REAL, INTENT(in) :: t ! Time over which to propagate (typically dt/2)
v(:,:) = v(:,:) + t * f(:,:)
END SUBROUTINE u2_propagator
SUBROUTINE u3_propagator ( t ) ! U3: thermostat propagator
IMPLICIT NONE
REAL, INTENT(in) :: t ! Time over which to propagate (typically dt/2)
v(:,:) = v(:,:) * EXP ( -t * p_eta(1) / q(1) )
eta(:) = eta(:) + t * p_eta(:) / q(:)
END SUBROUTINE u3_propagator
SUBROUTINE u4_propagator ( t, j_start, j_stop ) ! U4: thermostat propagator
USE maths_module, ONLY : exprel
IMPLICIT NONE
REAL, INTENT(in) :: t ! Time over which to propagate (typically dt/4)
INTEGER, INTENT(in) :: j_start, j_stop ! Order in which to tackle variables
INTEGER :: j, j_stride
REAL :: gj, x, c
IF ( j_start > j_stop ) THEN
j_stride = -1
ELSE
j_stride = 1
END IF
DO j = j_start, j_stop, j_stride ! Loop over each momentum in turn
IF ( j == 1 ) THEN ! The driver Gj for p_eta(1) is different
gj = SUM(v**2) - g*temperature
ELSE
gj = ( p_eta(j-1)**2 / q(j-1) ) - temperature
END IF
IF ( j == m ) THEN ! The equation for p_eta(M) is different
p_eta(j) = p_eta(j) + t * gj
ELSE
x = t * p_eta(j+1)/q(j+1)
c = exprel(-x) ! (1-exp(-x))/x, preserving accuracy for small x
p_eta(j) = p_eta(j)*EXP(-x) + t * gj * c
END IF
END DO ! End loop over each momentum in turn
END SUBROUTINE u4_propagator
FUNCTION calc_variables ( ) RESULT ( variables )
USE lrc_module, ONLY : potential_lrc, pressure_lrc
USE averages_module, ONLY : variable_type, msd
IMPLICIT NONE
TYPE(variable_type), DIMENSION(10) :: variables ! The 10 variables listed below
! This routine calculates all variables of interest and (optionally) writes them out
! They are collected together in the variables array, for use in the main program
TYPE(variable_type) :: e_s, p_s, e_f, p_f, t_k, t_c, conserved, c_s, c_f, conserved_msd
REAL :: vol, rho, kin, fsq, ext, eng
! Preliminary calculations
vol = box**3 ! Volume
rho = REAL(n) / vol ! Density
kin = 0.5*SUM(v**2) ! Kinetic energy
fsq = SUM(f**2) ! Total squared force
ext = SUM(0.5*p_eta**2/q) + temperature * ( g*eta(1) + SUM(eta(2:m)) ) ! Extra terms for conserved variable
eng = kin + total%pot ! Total energy
! Variables of interest, of type variable_type, containing three components:
! %val: the instantaneous value
! %nam: used for headings
! %method: indicating averaging method
! If not set below, %method adopts its default value of avg
! The %nam and some other components need only be defined once, at the start of the program,
! but for clarity and readability we assign all the values together below
! Internal energy (cut-and-shifted ) per atom
! Total KE plus total cut-and-shifted PE divided by N
e_s = variable_type ( nam = 'E/N cut&shifted', val = eng/REAL(n) )
! Internal energy (full, including LRC) per atom
! LRC plus total KE plus total cut (but not shifted) PE divided by N
e_f = variable_type ( nam = 'E/N full', val = potential_lrc(rho,r_cut) + (kin+total%cut)/REAL(n) )
! Pressure (cut-and-shifted)
! Ideal gas contribution plus total virial divided by V
p_s = variable_type ( nam = 'P cut&shifted', val = rho*temperature + total%vir/vol )
! Pressure (full, including LRC)
! LRC plus ideal gas contribution plus total virial divided by V
p_f = variable_type ( nam = 'P full', val = pressure_lrc(rho,r_cut) + rho*temperature + total%vir/vol )
! Kinetic temperature
t_k = variable_type ( nam = 'T kinetic', val = 2.0*kin/g )
! Configurational temperature
! Total squared force divided by total Laplacian
t_c = variable_type ( nam = 'T config', val = fsq/total%lap )
! Conserved energy-like quantity per atom
! Energy plus extra terms defined above
conserved = variable_type ( nam = 'Conserved/N', val = (eng+ext)/REAL(n) )
! Heat capacity (cut-and-shifted)
! Total energy divided by temperature and sqrt(N) to make result intensive
c_s = variable_type ( nam = 'Cv/N cut&shifted', val = (kin+total%pot)/(temperature*SQRT(REAL(n))), &
& method = msd, instant = .FALSE. )
! Heat capacity (full)
! Total energy divided by temperature and sqrt(N) to make result intensive; LRC does not contribute
c_f = variable_type ( nam = 'Cv/N full', val = (kin+total%cut)/(temperature*SQRT(REAL(n))), &
& method = msd, instant = .FALSE. )
! Mean-squared deviation of conserved energy-like quantity
! Energy plus extra terms defined above
conserved_msd = variable_type ( nam = 'Conserved MSD', val = (eng+ext)/REAL(n), &
& method = msd, e_format = .TRUE., instant = .FALSE. )
! Collect together for averaging
variables = [ e_s, p_s, e_f, p_f, t_k, t_c, conserved, c_s, c_f, conserved_msd ]
END FUNCTION calc_variables
END PROGRAM md_nvt_lj