[gmx-users] Gromacs version for polarizable model
Luca Banetta
luca.banetta at gmail.com
Wed Jun 22 09:11:15 CEST 2016
Dear all,
I am trying to use a polarizable model for acetone molecule. After
lots of attempts we created a stable model for a single acetone
molecule in a sea of water running the simulation on one core.
So then we started new simulations with a certain number of acetone
molecules and the simulation appeared to run, but unfortunately it
doesn't write anything in log file, xtc or trr files.
Is this a problema connected with an old version of the code (4.5.4)
that I used?
If yes, which code should I get?
In thw following lines I show:
TOPOLOGY
#include "oplsaaff.itp"
#include "oplsaa.ff/spc.itp"
[ moleculetype ]
; Name nrexcl
acetone 3
[ atoms ]
; nr type resnr residue atom cgnr
charge mass typeB chargeB massB
1 opls_280 1 LIG C 1 -0.47 12.011
2 opls_135 1 LIG C 2 -0.18 12.011
3 opls_135 1 LIG C 3 -0.18 12.011
4 opls_281 1 LIG O 1 0.47
15.5994
5 opls_282 1 LIG H 2 0.06 1.008
6 opls_282 1 LIG H 2 0.06 1.008
7 opls_282 1 LIG H 2 0.06 1.008
8 opls_282 1 LIG H 3 0.06 1.008
9 opls_282 1 LIG H 3 0.06 1.008
10 opls_282 1 LIG H 3 0.06 1.008
11 SP 1 LIG SP 1 -0.47 0.400
12 VS 1 LIG VS 1 0.47 0.000
[ polarization ]
; atom shell functiontype alpha nm^3
4 11 1 0.001
[ bonds ]
; ai aj funct c0 c1 c2 c3
1 2 1
1 3 1
1 4 1
1 12 6
2 5 1
2 6 1
2 7 1
2 12 6
3 8 1
3 9 1
3 10 1
3 12 6
4 11 1
[ pairs ]
; ai aj funct c0 c1 c2 c3
2 8 1
2 9 1
2 10 1
3 5 1
3 6 1
3 7 1
4 5 1
4 6 1
4 7 1
4 8 1
4 9 1
4 10 1
[ angles ]
; ai aj ak funct c0 c1 c2 c3
2 1 3 1
2 1 4 1
3 1 4 1
1 2 5 1
1 2 6 1
1 2 7 1
5 2 6 1
5 2 7 1
6 2 7 1
1 3 8 1
1 3 9 1
1 3 10 1
8 3 9 1
8 3 10 1
9 3 10 1
[ dihedrals ]
; ai aj ak al funct c0 c1
c2 c3 c4 c5
3 1 2 5 3
3 1 2 6 3
3 1 2 7 3
4 1 2 5 3
4 1 2 6 3
4 1 2 7 3
2 1 3 8 3
2 1 3 9 3
2 1 3 10 3
4 1 3 8 3
4 1 3 9 3
4 1 3 10 3
[ exclusions ]
; interazioni di non legame tra il primo atomo e i successivi non sono
considerate
1 2 3 4 5 6 7 8 9 10 11 12
2 3 4 5 6 7 8 9 10 11 12
3 4 5 6 7 8 9 10 11 12
4 5 6 7 8 9 10 11 12
5 6 7 8 9 10 11 12
6 7 8 9 10 11 12
7 8 9 10 11 12
8 9 10 11 12
9 10 11 12
10 11 12
11 12
[ virtual_sites2 ]
; site ai aj funct a
12 1 4 1 -0.30
[ system ]
mixture
[ molecules ]
acetone 150
SOL 1359
MDP FILE
; VARIOUS PREPROCESSING OPTIONS
title = Yo
cpp = /usr/bin/cpp
include =
define =
; RUN CONTROL PARAMETERS
integrator = md
; Start time and timestep in ps
tinit = 0
dt = 0.0001
nsteps = 1000000
; For exact run continuation or redoing part of a run
init_step = 0
; mode for center of mass motion removal
comm-mode = Linear
; number of steps for center of mass motion removal
nstcomm = 1
; group(s) for center of mass motion removal
comm-grps =
; LANGEVIN DYNAMICS OPTIONS
; Temperature, friction coefficient (amu/ps) and random seed
;ref-t = 300
bd-fric = 0
ld-seed = 1993
; ENERGY MINIMIZATION OPTIONS
; Force tolerance and initial step-size
emtol = 100
emstep = 0.01
; Max number of iterations in relax_shells
niter = 20
; Step size (1/ps^2) for minimization of flexible constraints
fcstep = 0
; Frequency of steepest descents steps when doing CG
nstcgsteep = 1000
nbfgscorr = 10
; OUTPUT CONTROL OPTIONS
; Output frequency for coords (x), velocities (v) and forces (f)
nstxout =
nstvout =
nstfout =
; Checkpointing helps you continue after crashes
nstcheckpoint = 1000
; Output frequency for energies to log file and energy file
nstlog = 50
nstenergy = 50
; Output frequency and precision for xtc file
nstxtcout = 1
xtc-precision = 1000
; This selects the subset of atoms for the xtc file. You can
; select multiple groups. By default all atoms will be written.
xtc-grps =
; Selection of energy groups
energygrps =
; NEIGHBORSEARCHING PARAMETERS
; nblist update frequency
nstlist = 20
; ns algorithm (simple or grid)
ns_type = grid
; Periodic boundary conditions: xyz (default), no (vacuum)
; or full (infinite systems only)
pbc = xyz
; nblist cut-off
rlist = 1.2
domain-decomposition = no
; OPTIONS FOR ELECTROSTATICS AND VDW
; Method for doing electrostatics
coulombtype = PME
rcoulomb-switch = 0
rcoulomb = 1.2
; Dielectric constant (DC) for cut-off or DC of reaction field
epsilon-r = 1
; Method for doing Van der Waals
vdw-type = Cut-off
; cut-off lengths
rvdw-switch = 0
rvdw = 1.2
; Apply long range dispersion corrections for Energy and Pressure
DispCorr = EnerPres
; Extension of the potential lookup tables beyond the cut-off
table-extension = 1
; Spacing for the PME/PPPM FFT grid
fourierspacing = 0.16
; FFT grid size, when a value is 0 fourierspacing will be used
fourier_nx = 0
fourier_ny = 0
fourier_nz = 0
; EWALD/PME/PPPM parameters
pme_order = 4
ewald_rtol = 1e-05
ewald_geometry = 3d
epsilon_surface = 0
optimize_fft = no
; GENERALIZED BORN ELECTROSTATICS
; Algorithm for calculating Born radii
gb_algorithm = Still
; Frequency of calculating the Born radii inside rlist
nstgbradii = 1
; Cutoff for Born radii calculation; the contribution from atoms
; between rlist and rgbradii is updated every nstlist steps
rgbradii = 2
; Salt concentration in M for Generalized Born models
gb_saltconc = 0
; IMPLICIT SOLVENT (for use with Generalized Born electrostatics)
implicit_solvent = No
; OPTIONS FOR WEAK COUPLING ALGORITHMS
; Temperature coupling
Tcoupl = v-rescale
; Groups to couple separately
tc-grps = System
; Time constant (ps) and reference temperature (K)
tau_t = 0.1
ref_t = 300
; Pressure coupling
Pcoupl = berendsen
Pcoupltype = isotropic
; Time constant (ps), compressibility (1/bar) and reference P (bar)
tau_p = 1.0
compressibility = 4.5e-5
ref_p = 1.0
; Random seed for Andersen thermostat
andersen_seed = 815131
; SIMULATED ANNEALING
; Type of annealing for each temperature group (no/single/periodic)
annealing = no
; Number of time points to use for specifying annealing in each group
annealing_npoints =
; List of times at the annealing points for each group
annealing_time =
; Temp. at each annealing point, for each group.
annealing_temp =
; GENERATE VELOCITIES FOR STARTUP RUN
gen_vel = yes
gen_temp = 300
gen_seed = 1993
; OPTIONS FOR BONDS
constraints = h-bonds
; Type of constraint algorithm
constraint-algorithm = Lincs
; Do not constrain the start configuration
unconstrained-start = no
; Use successive overrelaxation to reduce the number of shake iterations
Shake-SOR = no
; Relative tolerance of shake
shake-tol = 1e-04
; Highest order in the expansion of the constraint coupling matrix
lincs-order = 4
; Number of iterations in the final step of LINCS. 1 is fine for
; normal simulations, but use 2 to conserve energy in NVE runs.
; For energy minimization with constraints it should be 4 to 8.
lincs-iter = 1
; Lincs will write a warning to the stderr if in one step a bond
; rotates over more degrees than
lincs-warnangle = 30
; Convert harmonic bonds to morse potentials
morse = no
; ENERGY GROUP EXCLUSIONS
; Pairs of energy groups for which all non-bonded interactions are excluded
energygrp_excl =
; NMR refinement stuff
; Distance restraints type: No, Simple or Ensemble
disre = No
; Force weighting of pairs in one distance restraint: Conservative or Equal
disre-weighting = Conservative
; Use sqrt of the time averaged times the instantaneous violation
disre-mixed = no
disre-fc = 1000
disre-tau = 0
; Output frequency for pair distances to energy file
nstdisreout = 100
; Orientation restraints: No or Yes
orire = no
; Orientation restraints force constant and tau for time averaging
orire-fc = 0
orire-tau = 0
orire-fitgrp =
; Output frequency for trace(SD) to energy file
nstorireout = 100
; Dihedral angle restraints: No, Simple or Ensemble
dihre = No
dihre-fc = 1000
dihre-tau = 0
; Output frequency for dihedral values to energy file
nstdihreout = 100
; Free energy control stuff
free-energy = no
init-lambda = 0
delta-lambda = 0
sc-alpha = 0
sc-sigma = 0.3
; Non-equilibrium MD stuff
acc-grps =
accelerate =
freezegrps =
freezedim =
cos-acceleration = 0
; Electric fields
; Format is number of terms (int) and for all terms an amplitude (real)
; and a phase angle (real)
E-x =
E-xt =
E-y =
E-yt =
E-z =
E-zt =
; User defined thingies
user1-grps =
user2-grps =
userint1 = 0
userint2 = 0
userint3 = 0
userint4 = 0
userreal1 = 0
userreal2 = 0
userreal3 = 0
userreal4 = 0
LOG FILE
Log file opened on Wed Jun 22 09:00:54 2016
Host: compute-0-2.local pid: 9075 nodeid: 0 nnodes: 1
The Gromacs distribution was built Tue Nov 27 15:50:05 PST 2012 by
root at centos-6-3.localdomain (Linux 2.6.32-279.14.1.el6.x86_64 x86_64)
:-) G R O M A C S (-:
Grunge ROck MAChoS
:-) VERSION 4.5.4 (-:
Written by Emile Apol, Rossen Apostolov, Herman J.C. Berendsen,
Aldert van Buuren, Pär Bjelkmar, Rudi van Drunen, Anton Feenstra,
Gerrit Groenhof, Peter Kasson, Per Larsson, Pieter Meulenhoff,
Teemu Murtola, Szilard Pall, Sander Pronk, Roland Schulz,
Michael Shirts, Alfons Sijbers, Peter Tieleman,
Berk Hess, David van der Spoel, and Erik Lindahl.
Copyright (c) 1991-2000, University of Groningen, The Netherlands.
Copyright (c) 2001-2010, The GROMACS development team at
Uppsala University & The Royal Institute of Technology, Sweden.
check out http://www.gromacs.org for more information.
This program is free software; you can redistribute it and/or
modify it under the terms of the GNU General Public License
as published by the Free Software Foundation; either version 2
of the License, or (at your option) any later version.
:-) mdrun (-:
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
B. Hess and C. Kutzner and D. van der Spoel and E. Lindahl
GROMACS 4: Algorithms for highly efficient, load-balanced, and scalable
molecular simulation
J. Chem. Theory Comput. 4 (2008) pp. 435-447
-------- -------- --- Thank You --- -------- --------
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
D. van der Spoel, E. Lindahl, B. Hess, G. Groenhof, A. E. Mark and H. J. C.
Berendsen
GROMACS: Fast, Flexible and Free
J. Comp. Chem. 26 (2005) pp. 1701-1719
-------- -------- --- Thank You --- -------- --------
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
E. Lindahl and B. Hess and D. van der Spoel
GROMACS 3.0: A package for molecular simulation and trajectory analysis
J. Mol. Mod. 7 (2001) pp. 306-317
-------- -------- --- Thank You --- -------- --------
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
H. J. C. Berendsen, D. van der Spoel and R. van Drunen
GROMACS: A message-passing parallel molecular dynamics implementation
Comp. Phys. Comm. 91 (1995) pp. 43-56
-------- -------- --- Thank You --- -------- --------
Input Parameters:
integrator = md
nsteps = 1000000
init_step = 0
ns_type = Grid
nstlist = 20
ndelta = 2
nstcomm = 20
comm_mode = Linear
nstlog = 50
nstxout = 100
nstvout = 100
nstfout = 0
nstcalcenergy = 20
nstenergy = 60
nstxtcout = 1
init_t = 0
delta_t = 0.0001
xtcprec = 1000
nkx = 25
nky = 25
nkz = 25
pme_order = 4
ewald_rtol = 1e-05
ewald_geometry = 0
epsilon_surface = 0
optimize_fft = FALSE
ePBC = xyz
bPeriodicMols = FALSE
bContinuation = FALSE
bShakeSOR = FALSE
etc = V-rescale
nsttcouple = 20
epc = Berendsen
epctype = Isotropic
nstpcouple = 20
tau_p = 1
ref_p (3x3):
ref_p[ 0]={ 1.00000e+00, 0.00000e+00, 0.00000e+00}
ref_p[ 1]={ 0.00000e+00, 1.00000e+00, 0.00000e+00}
ref_p[ 2]={ 0.00000e+00, 0.00000e+00, 1.00000e+00}
compress (3x3):
compress[ 0]={ 4.50000e-05, 0.00000e+00, 0.00000e+00}
compress[ 1]={ 0.00000e+00, 4.50000e-05, 0.00000e+00}
compress[ 2]={ 0.00000e+00, 0.00000e+00, 4.50000e-05}
refcoord_scaling = No
posres_com (3):
posres_com[0]= 0.00000e+00
posres_com[1]= 0.00000e+00
posres_com[2]= 0.00000e+00
posres_comB (3):
posres_comB[0]= 0.00000e+00
posres_comB[1]= 0.00000e+00
posres_comB[2]= 0.00000e+00
andersen_seed = 815131
rlist = 1.2
rlistlong = 1.2
rtpi = 0.05
coulombtype = PME
rcoulomb_switch = 0
rcoulomb = 1.2
vdwtype = Cut-off
rvdw_switch = 0
rvdw = 1.2
epsilon_r = 1
epsilon_rf = 1
tabext = 1
implicit_solvent = No
gb_algorithm = Still
gb_epsilon_solvent = 80
nstgbradii = 1
rgbradii = 2
gb_saltconc = 0
gb_obc_alpha = 1
gb_obc_beta = 0.8
gb_obc_gamma = 4.85
gb_dielectric_offset = 0.009
sa_algorithm = Ace-approximation
sa_surface_tension = 2.05016
DispCorr = EnerPres
free_energy = no
init_lambda = 0
delta_lambda = 0
n_foreign_lambda = 0
sc_alpha = 0
sc_power = 0
sc_sigma = 0.3
sc_sigma_min = 0.3
nstdhdl = 10
separate_dhdl_file = yes
dhdl_derivatives = yes
dh_hist_size = 0
dh_hist_spacing = 0.1
nwall = 0
wall_type = 9-3
wall_atomtype[0] = -1
wall_atomtype[1] = -1
wall_density[0] = 0
wall_density[1] = 0
wall_ewald_zfac = 3
pull = no
disre = No
disre_weighting = Conservative
disre_mixed = FALSE
dr_fc = 1000
dr_tau = 0
nstdisreout = 100
orires_fc = 0
orires_tau = 0
nstorireout = 100
dihre-fc = 1000
em_stepsize = 0.01
em_tol = 100
niter = 20
fc_stepsize = 0
nstcgsteep = 1000
nbfgscorr = 10
ConstAlg = Lincs
shake_tol = 0.0001
lincs_order = 4
lincs_warnangle = 30
lincs_iter = 1
bd_fric = 0
ld_seed = 1993
cos_accel = 0
deform (3x3):
deform[ 0]={ 0.00000e+00, 0.00000e+00, 0.00000e+00}
deform[ 1]={ 0.00000e+00, 0.00000e+00, 0.00000e+00}
deform[ 2]={ 0.00000e+00, 0.00000e+00, 0.00000e+00}
userint1 = 0
userint2 = 0
userint3 = 0
userint4 = 0
userreal1 = 0
userreal2 = 0
userreal3 = 0
userreal4 = 0
grpopts:
nrdf: 11751
ref_t: 300
tau_t: 0.1
anneal: No
ann_npoints: 0
acc: 0 0 0
nfreeze: N N N
energygrp_flags[ 0]: 0
efield-x:
n = 0
efield-xt:
n = 0
efield-y:
n = 0
efield-yt:
n = 0
efield-z:
n = 0
efield-zt:
n = 0
bQMMM = FALSE
QMconstraints = 0
QMMMscheme = 0
scalefactor = 1
qm_opts:
ngQM = 0
Table routines are used for coulomb: TRUE
Table routines are used for vdw: FALSE
Will do PME sum in reciprocal space.
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
U. Essman, L. Perela, M. L. Berkowitz, T. Darden, H. Lee and L. G. Pedersen
A smooth particle mesh Ewald method
J. Chem. Phys. 103 (1995) pp. 8577-8592
-------- -------- --- Thank You --- -------- --------
Will do ordinary reciprocal space Ewald sum.
Using a Gaussian width (1/beta) of 0.384195 nm for Ewald
Cut-off's: NS: 1.2 Coulomb: 1.2 LJ: 1.2
Long Range LJ corr.: <C6> 3.3273e-04
System total charge: -0.000
Generated table with 1100 data points for Ewald.
Tabscale = 500 points/nm
Generated table with 1100 data points for LJ6.
Tabscale = 500 points/nm
Generated table with 1100 data points for LJ12.
Tabscale = 500 points/nm
Generated table with 1100 data points for 1-4 COUL.
Tabscale = 500 points/nm
Generated table with 1100 data points for 1-4 LJ6.
Tabscale = 500 points/nm
Generated table with 1100 data points for 1-4 LJ12.
Tabscale = 500 points/nm
Enabling SPC-like water optimization for 1359 molecules.
Configuring nonbonded kernels...
Configuring standard C nonbonded kernels...
Testing x86_64 SSE2 support... present.
Removing pbc first time
Initializing LINear Constraint Solver
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
B. Hess and H. Bekker and H. J. C. Berendsen and J. G. E. M. Fraaije
LINCS: A Linear Constraint Solver for molecular simulations
J. Comp. Chem. 18 (1997) pp. 1463-1472
-------- -------- --- Thank You --- -------- --------
The number of constraints is 900
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
S. Miyamoto and P. A. Kollman
SETTLE: An Analytical Version of the SHAKE and RATTLE Algorithms for Rigid
Water Models
J. Comp. Chem. 13 (1992) pp. 952-962
-------- -------- --- Thank You --- -------- --------
Center of mass motion removal mode is Linear
We have the following groups for center of mass motion removal:
0: rest
++++ PLEASE READ AND CITE THE FOLLOWING REFERENCE ++++
G. Bussi, D. Donadio and M. Parrinello
Canonical sampling through velocity rescaling
J. Chem. Phys. 126 (2007) pp. 014101
-------- -------- --- Thank You --- -------- --------
SIMULATION RECAP
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