[gmx-users] Changes in the simulation box after the production run
Mahsa E
ebadi.mahsa at gmail.com
Sun Sep 17 22:31:51 CEST 2017
Dear gmx-users,
I did a 200 ns production md run in NVT ensemble for a simulation box of
polymer chains. Before this step, I did the energy minimisation, NVT and
NPT equilibration on the system. The problem is after the production run, I
don't get the initial equilibrated packed box of polymer and it seems more
like a circular shape with some parts of the chains out of the box. What is
the reason for getting this result?
For the MD run I used the mdp file below:
; 7.3.2 Preprocessing
;define = ; defines to pass to the preprocessor
; 7.3.3 Run Control
integrator = md ; md integrator
tinit = 0 ; [ps] starting time for run
dt = 0.002 ; [ps] time step for
integration
nsteps = 100000000 ; maximum number of
steps to integrate, 0.002 * 100000000 = 200000 ps
comm_mode = Linear ; remove center of mass
translation
nstcomm = 100 ; [steps] frequency of
mass motion removal
;comm_grps = Protein Non-Protein ; group(s) for center of
mass motion removal
; 7.3.8 Output Control
nstxout = 0 ; [steps] freq to write coordinates to
trajectory
nstvout = 0 ; [steps] freq to write velocities to
trajectory
nstfout = 0 ; [steps] freq to write forces to
trajectory
nstlog = 1000 ; [steps] freq to write energies
to log file
nstenergy = 1000 ; [steps] freq to write energies
to energy file
nstxtcout = 1000 ; [steps] freq to write
coordinates to xtc trajectory
xtc_precision = 1000 ; [real] precision to write xtc
trajectory
xtc_grps = System ; group(s) to write to xtc
trajectory
energygrps = System ; group(s) to write to energy file
cutoff-scheme = verlet
; 7.3.9 Neighbor Searching
nstlist = 20 ; [steps] freq to update neighbor
list
ns_type = grid ; method of updating neighbor list
pbc = xyz ; periodic boundary conditions in
all directions
rlist = 0.8 ; [nm] cut-off distance for the
short-range neighbor list
; 7.3.10 Electrostatics
coulombtype = PME ; Particle-Mesh Ewald electrostatics
rcoulomb = 1.2 ; [nm] distance for Coulomb cut-off
; 7.3.11 VdW
vdwtype = cut-off ; twin-range cut-off with rlist
where rvdw >= rlist
vdw-modifier = potential-switch
rvdw-switch = 1.1
rvdw = 1.2 ; [nm] distance for LJ cut-off
DispCorr = EnerPres ; apply long range dispersion
corrections
; 7.3.13 Ewald
fourierspacing = 0.12 ; [nm] grid spacing for FFT grid
when using PME
pme_order = 4 ; interpolation order for PME, 4 =
cubic
ewald_rtol = 1e-6 ; relative strength of
Ewald-shifted potential at rcoulomb
ewald-rtol-lj = 0.001
lj-pme-comb-rule = Geometric
ewald-geometry = 3d
epsilon_surface = 0
; 7.3.14 Temperature Coupling
tcoupl = v-rescale ; temperature
coupling with
tc_grps = system ; groups to couple seperately to
temperature bath
tau_t = 0.1 ; [ps] time constant
for coupling
ref_t = 303 ; [K] reference
temperature for coupling
; 7.3.17 Velocity Generation
gen_vel = no ; generate velocities according to
Maxwell distribution of temperature
gen_temp = 303 ; [K] temperature for Maxwell
distribution
gen_seed = -1 ; [integer] used to initialize
random generator for random velocities
; 7.3.18 Bonds
constraints = h-bonds
constraint_algorithm = LINCS ; LINear Constraint Solver
continuation = no ; no = apply constraints to the
start configuration
lincs_order = 4 ; highest order in the expansion of
the contraint coupling matrix
lincs_iter = 1 ; number of iterations to correct
for rotational lengthening
lincs_warnangle = 30 ; [degrees] maximum angle that a
bond can rotate before LINCS will complain
Best regards,
Mahsa
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