[gmx-users] NVE Temperature Drift
Johnny Lu
johnny.lu128 at gmail.com
Mon Aug 25 21:18:41 CEST 2014
Hi. I'm trying to run NVE on a
~170 amino acid protein
with a harmonic dihedral angle restraint of 4184 kJ/mol rad^2,
in a rhombic dodecahedron water box that is 15 angstroms away from the
protein
using single precision gromacs,
and 0.5 fs time step.
Since I only want to get many short stretches of NVE simulations, I
alternate npt and nve:
0. Steepest descent minimization with emtol = 1000.0.
1. [NVT equilibration, 2fs timestep 100,000 frames]
2. [NPT equilibration, 2fs timestep, 100,000 frames]
3. [NPT equilibration, 2fs timestep, 5,000 frames, Berendsen thermostat at
300K, position restraint?]
4. [NVE md,0.5 fs timestep, 35,000 frames, no thermostat]
5. go to step 3.
(all of these steps have the dihedral angle restraint)
In the NVE step, I get about 0.1% total energy decrease from start to
end(figure). (the total energy keep dropping).
But, the temperature still fluctuate in a range of ~ 5 Kelvin (figure
<http://oi60.tinypic.com/sni5at.jpg>). Is that normal? Does that happen in
real world? Where does this temperature fluctuation come from? How to
reduce that? Does the restraint have anything to do with this?
[image: Inline image 2]
[image: Inline image 1]
Below is the mdp file that I was using:
; Amber99SB MD
; Run parameters
integrator = md ; leap-frog integrator
nsteps = 32768 ; 2 * 100000 = 200 ps, 1 ns
dt = 0.0005 ; 1 fs
; Output control
nstfout = 2
nstxtcout = 2 ; xtc compressed trajectory output every 2 fs
nstlog = 1000 ; update log file every 2 ps
xtc-grps=protein;
continuation = yes ; Restarting after NPT
constraint_algorithm = Lincs ; holonomic constraints
constraints = h-bonds ; all bonds (even heavy atom-H bonds)
constrained
lincs_iter = 2 ; accuracy of LINCS
lincs_order = 4 ; also related to accuracy
; Neighborsearching
ns_type = grid ; search neighboring grid cells
nstlist = 10 ; 10 fs
rlist = 1.8 ; short-range neighborlist cutoff (in nm)
rcoulomb = 1.5 ; short-range electrostatic cutoff (in nm)
rvdw = 1.5 ; short-range van der Waals cutoff (in nm)
; Electrostatics
coulombtype = PME ; Particle Mesh Ewald for long-range
electrostatics
pme_order = 6 ; cubic interpolation
fourierspacing = 0.12 ; grid spacing for FFT
optimize_fft = yes
tcoupl = no
pcoupl = no
compressibility = 4.5e-5 ; isothermal compressibility of water, bar^-1
; Periodic boundary conditions
pbc = xyz ; 3-D PBC
; Dispersion correction
DispCorr = EnerPres ; account for cut-off vdW scheme
; Velocity generation
gen_vel = no ; Velocity generation is off
verlet-buffer-drift=-1
cutoff-scheme = Verlet;
Thanks again.
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