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md_nvt_poly_lj.f90
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md_nvt_poly_lj.f90
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! md_nvt_poly_lj.f90
! Molecular dynamics, NVT ensemble (NVE option), polyatomic molecules
PROGRAM md_nvt_poly_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, quaternions, velocities and angular momenta)
! Cubic periodic boundary conditions
! Conducts molecular dynamics with optional velocity thermalization
! Uses no special neighbour lists
! The rotational algorithm is described in the text, section 3.3. See A Dullweber, B Leimkuhler,
! R McLachlan, J Chem Phys 107, 5840 (1997) and TF Miller, M Eleftheriou, P Pattnaik,
! A Ndirango, D Newns, GJ Martyna, J Chem Phys 116, 8649 (2002).
! 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_mols, write_cnf_mols
USE averages_module, ONLY : run_begin, run_end, blk_begin, blk_end, blk_add
USE maths_module, ONLY : q_to_a
USE md_module, ONLY : introduction, conclusion, allocate_arrays, deallocate_arrays, &
& force, r, e, d, v, ell, f, tau, n, na, db, inertia, potential_type
IMPLICIT NONE
! Most important variables
REAL :: box ! Box length
REAL :: dt ! Time step
REAL :: temperature ! Specified temperature
LOGICAL :: nvt ! Flag to indicate NVT ensemble
! Composite interaction = pot & vir & ovr variables
TYPE(potential_type) :: total
INTEGER :: blk, stp, nstep, nblock, t_interval, ioerr, i, a
REAL :: norm
REAL, DIMENSION(3) :: vcm
REAL, DIMENSION(3,3) :: ai
CHARACTER(len=4), PARAMETER :: cnf_prefix = 'cnf.'
CHARACTER(len=3), PARAMETER :: inp_tag = 'inp'
CHARACTER(len=3), PARAMETER :: out_tag = 'out'
CHARACTER(len=3) :: sav_tag = 'sav' ! May be overwritten with block number
NAMELIST /nml/ nblock, nstep, dt, temperature, t_interval
WRITE ( unit=output_unit, fmt='(a)' ) 'md_nvt_poly_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/NVE ensemble'
WRITE ( unit=output_unit, fmt='(a)' ) 'Molecular mass=1 throughout'
CALL introduction
CALL RANDOM_INIT ( .FALSE., .TRUE. ) ! Initialize random number generator
! Set sensible default run parameters for testing
nblock = 10
nstep = 20000
dt = 0.003
temperature = 1.0
t_interval = 0
! 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_poly_lj'
END IF
! Write out run parameters
nvt = t_interval > 0 .AND. t_interval < nstep
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)' ) 'Time step', dt
IF ( nvt ) THEN
WRITE ( unit=output_unit, fmt='(a)' ) 'NVT ensemble'
WRITE ( unit=output_unit, fmt='(a,t40,i15)' ) 'Thermalization interval', t_interval
WRITE ( unit=output_unit, fmt='(a,t40,f15.6)' ) 'Temperature', temperature
ELSE
WRITE ( unit=output_unit, fmt='(a)' ) 'NVE ensemble'
t_interval = nstep+1
END IF
! Read in initial configuration and allocate necessary arrays
CALL read_cnf_mols ( 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 )
IF ( nvt ) THEN
CALL read_cnf_mols ( cnf_prefix//inp_tag, n, box, r, e ) ! Second call gets r, e
CALL ran_velocities
ELSE
CALL read_cnf_mols ( cnf_prefix//inp_tag, n, box, r, e, v, ell ) ! Second call gets r, e, v and ell
vcm(:) = SUM ( v(:,:), dim=2 ) / REAL(n) ! Centre-of mass velocity
v(:,:) = v(:,:) - SPREAD ( vcm(:), dim = 2, ncopies = n ) ! Set COM velocity to zero
END IF
r(:,:) = r(:,:) / box ! Convert positions to box units
r(:,:) = r(:,:) - ANINT ( r(:,:) ) ! Periodic boundaries
! Calculate all bond vectors
DO i = 1, n ! Loop over molecules
norm = SQRT(SUM(e(:,i)**2))
e(:,i) = e(:,i) / norm ! Ensure normalized quaternions
ai = q_to_a ( e(:,i) ) ! Rotation matrix for i
DO a = 1, na ! Loop over all atoms
d(:,a,i) = MATMUL ( db(:,a), ai ) ! NB: equivalent to ai_T*db, ai_T=transpose of ai
END DO ! End loop over all atoms
END DO ! End loop over molecules
! Initial forces, potential, etc plus overlap check
CALL force ( box, total )
IF ( total%ovr ) THEN
WRITE ( unit=error_unit, fmt='(a)') 'Overlap in initial configuration'
STOP 'Error in md_poly_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
IF ( nvt .AND. MOD(stp,t_interval) == 0 ) THEN
CALL ran_velocities
END IF
CALL kick_propagator ( 0.5 * dt ) ! Half-kick step
CALL drift_translate ( dt ) ! Drift step for positions
! Succession of drift steps for rotation about body-fixed axes
! Depending on the values of the moments of inertia, a different nested
! sequence of axes may produce better or worse energy conservation
CALL drift_rotate ( 1, 0.5*dt )
CALL drift_rotate ( 2, 0.5*dt )
CALL drift_rotate ( 3, dt )
CALL drift_rotate ( 2, 0.5*dt )
CALL drift_rotate ( 1, 0.5*dt )
! Calculate all bond vectors
DO i = 1, n ! Loop over molecules
norm = SQRT(SUM(e(:,i)**2))
e(:,i) = e(:,i) / norm ! Guard against cumulative roundoff
ai = q_to_a ( e(:,i) ) ! Rotation matrix for i
DO a = 1, na ! Loop over all atoms
d(:,a,i) = MATMUL ( db(:,a), ai ) ! NB: equivalent to ai_T*db, ai_T=transpose of ai
END DO ! End loop over all atoms
END DO ! End loop over molecules
CALL force ( box, total ) ! Force evaluation
IF ( total%ovr ) THEN
WRITE ( unit=error_unit, fmt='(a)') 'Overlap in configuration'
STOP 'Error in md_poly_lj'
END IF
CALL kick_propagator ( 0.5 * dt ) ! Half-kick step
! 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_mols ( cnf_prefix//sav_tag, n, box, r*box, e, v, ell ) ! Save configuration
END DO ! End loop over blocks
CALL run_end ( calc_variables() ) ! Output run averages
CALL force ( box, total )
IF ( total%ovr ) THEN ! should never happen
WRITE ( unit=error_unit, fmt='(a)') 'Overlap in final configuration'
STOP 'Error in md_poly_lj'
END IF
CALL write_cnf_mols ( cnf_prefix//out_tag, n, box, r*box, e, v, ell ) ! Write out final configuration
CALL deallocate_arrays
CALL conclusion
CONTAINS
SUBROUTINE kick_propagator ( t )
IMPLICIT NONE
REAL, INTENT(in) :: t ! Time over which to propagate (typically dt/2)
! Advances velocities and body-fixed angular momenta
v(:,:) = v(:,:) + t * f(:,:) ! Linear momenta are equivalent to linear velocities
ell(:,:) = ell(:,:) + t * tau(:,:) ! Space-fixed angular momenta ell and torques tau
END SUBROUTINE kick_propagator
SUBROUTINE drift_translate ( t )
IMPLICIT NONE
REAL, INTENT(in) :: t ! Time over which to propagate (typically dt)
! Advances positions
r(:,:) = r(:,:) + t * v(:,:) / box ! Drift step (positions in box=1 units)
r(:,:) = r(:,:) - ANINT ( r(:,:) ) ! Periodic boundaries
END SUBROUTINE drift_translate
SUBROUTINE drift_rotate ( xyz, t )
USE maths_module, ONLY : q_to_a, rotate_quaternion
IMPLICIT NONE
INTEGER, INTENT(in) :: xyz ! Body-fixed axis about which to rotate
REAL, INTENT(in) :: t ! Time over which to propagate (typically dt or dt/2)
! Advances quaternion orientations about a specified axis
INTEGER :: i
REAL :: w_mag
REAL, DIMENSION(3) :: w_hat
REAL, DIMENSION(3,3) :: ai
DO i = 1, n
ai = q_to_a ( e(:,i) ) ! Rotation matrix
w_hat = ai(xyz,:) ! Space-fixed axis about which to rotate
w_mag = DOT_PRODUCT ( ell(:,i), w_hat ) / inertia(xyz) ! Angular velocity about this axis
e(:,i) = rotate_quaternion ( w_mag*t, w_hat, e(:,i) ) ! Rotate by specified angle
END DO
END SUBROUTINE drift_rotate
SUBROUTINE ran_velocities
USE maths_module, ONLY : random_normals
INTEGER :: i
REAL :: factor
REAL, DIMENSION(3) :: v_cm, factors
REAL, DIMENSION(3,3) :: ai
CALL random_normals ( 0.0, 1.0, v ) ! Random velocities
v_cm(:) = SUM ( v(:,:), dim=2 ) / REAL ( n ) ! Compute centre of mass velocity
v(:,:) = v(:,:) - SPREAD ( v_cm(:), dim=2, ncopies=n ) ! Set net momentum to zero
factor = SUM ( v**2 ) / REAL(3*n-3) ! Estimate of kinetic temperature
factor = SQRT ( temperature / factor ) ! Necessary correction factor
v = factor * v ! Make correction
CALL random_normals ( 0.0, 1.0, ell ) ! Random body-fixed angular momenta
factors = SUM ( ell**2, dim=2 ) / (REAL(n)*inertia(:)) ! Estimate of kinetic temperatures
factors = SQRT ( temperature / factors ) ! Necessary correction factors
ell = SPREAD(factors,dim=2,ncopies=n) * ell ! Make corrections
! Convert to space-fixed angular momenta
DO i = 1, n ! Loop over molecules
ai = q_to_a ( e(:,i) ) ! Rotation matrix for i
ell(:,i) = MATMUL ( ell(:,i), ai ) ! NB: equivalent to ell_s = ai_T*ell_b, ai_T=transpose of ai
END DO ! End loop over molecules
END SUBROUTINE ran_velocities
FUNCTION calc_variables ( ) RESULT ( variables )
USE averages_module, ONLY : variable_type, msd
USE maths_module, ONLY : q_to_a
IMPLICIT NONE
TYPE(variable_type), DIMENSION(5) :: variables ! The 5 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_sf, p_sf, t_t, t_r, conserved_msd
REAL :: vol, rho, kin_t, kin_r, eng, tmp_t, tmp_r
INTEGER :: i
REAL, DIMENSION(3) :: ell_i
REAL, DIMENSION(3,3) :: ai
! Preliminary calculations
vol = box**3 ! Volume
rho = REAL(n) / vol ! Density
kin_t = 0.5*SUM(v**2) ! Translational kinetic energy
kin_r = 0.0
DO i = 1, n ! Loop over molecules
ai = q_to_a ( e(:,i) ) ! Rotation matrix for i
ell_i = MATMUL ( ai, ell(:,i) ) ! Get body-fixed angular momentum
kin_r = kin_r + SUM((ell_i**2)/inertia)
END DO ! End loop over molecules
kin_r = 0.5*kin_r ! Rotational kinetic energy
tmp_t = 2.0 * kin_t / REAL(3*n-3) ! Remove three degrees of freedom for momentum conservation
tmp_r = 2.0 * kin_r / REAL(3*n) ! 3N degrees of rotational freedom
eng = kin_t + kin_r + total%pot ! Total energy for simulated system
! 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 (shifted-force potential) per atom
! Total translational and rotational KE plus total PE divided by N
IF ( nvt ) THEN
e_sf = variable_type ( nam = 'E/N shifted force', val = 3.0*temperature+total%pot/REAL(n) )
ELSE
e_sf = variable_type ( nam = 'E/N shifted force', val = eng/REAL(n) )
END IF
! Pressure (shifted-force potential)
! Ideal gas contribution plus total virial divided by V
IF ( nvt ) THEN
p_sf = variable_type ( nam = 'P shifted force', val = rho*temperature + total%vir/vol )
ELSE
p_sf = variable_type ( nam = 'P shifted force', val = rho*tmp_t + total%vir/vol )
END IF
! Kinetic translational temperature
t_t = variable_type ( nam = 'T translational', val = tmp_t )
! Kinetic rotational temperature
t_r = variable_type ( nam = 'T rotational', val = tmp_r )
! Mean-squared deviation of conserved energy per atom
conserved_msd = variable_type ( nam = 'Conserved MSD', val = eng/REAL(n), &
& method = msd, e_format = .TRUE., instant = .FALSE. )
! Collect together for averaging
variables = [ e_sf, p_sf, t_t, t_r, conserved_msd ]
END FUNCTION calc_variables
END PROGRAM md_nvt_poly_lj