[gmx-users] Drift in Conserved-Energy with Nose-Hoover thermostat
Bernhard
b.reuter at uni-kassel.de
Wed Jul 15 17:01:01 CEST 2015
Dear Gromacs Users and Developers,
I have a problem regarding energy conservation in my 10ns NVT
protein+water+ions (22765 atoms) production (minimization and
equilibration for more than 15ns was carried out in NPT before)
simulations using a Nose-Hoover thermostat (tau=2.5ps).
On first glance everything looks fine - the potential, kinetic and total
energy are nearly perfectly constant (with normal fluctuations) - but
when I checked the "Conserved-Energy" quantity that g_energy outputs I
had to recognize a significant (nearly perfectly) linear downward drift
of this "to-be-conserved" quantity of around 1.7 kJ/mol/ps (7.48*10^-5
kJ/mol/ps per atom).
This appears somehow disturbing to me since I would expect that this
Conserved-Energy is the conserved energy of the extended Nose-Hoover
Hamiltonian - which should by definition be conserved.
If it would be a drift caused by normal round-off error due to single
precision I would expect it to grow with Sqrt(N) and not with N (linear)
(N=number of steps).
So I would like to know if this is a normal behaviour and also what
could cause this (buffer size, precision, constraints etc)?
Also I would like to know, if I am correct with my guess that the
"Conserved-Energy" quantity is in this case the energy of the extended
Nose-Hoover Hamiltonian?
The .mdp file is atatched (don't be confused about rlist=1 - since Im
using the Verlet-scheme the verlet-buffer-drift option should be by
default active and determine the rlist value (Verlet buffer-size)
automatically).
Best regards,
Bernhard
; Run parameters
integrator = md ; leap-frog integrator
nsteps = 10000000 ; 10000 ps = 10 ns
dt = 0.001 ; 1 fs
; Output control
nstxout = 5000 ; save coordinates every ps
nstvout = 5000 ; save velocities every ps
nstxtcout = 1000 ; xtc compressed trajectory output every ps
nstenergy = 1000 ; save energies every ps
nstlog = 5000 ; update log file every ps
; Bond parameters
continuation = yes ; continue from NPT
constraint_algorithm = lincs ; holonomic constraints
constraints = h-bonds ; all bonds (even heavy atom-H bonds)
constrained
lincs_iter = 1 ; accuracy of LINCS
lincs_order = 4 ; also related to accuracy
; Neighborsearching
cutoff-scheme = Verlet ; Verlet cutoff-scheme instead of
group-scheme (no charge-groups used)
ns_type = grid ; search neighboring grid cells
nstlist = 10 ; 10 fs
rlist = 1.0 ; short-range neighborlist cutoff (in nm)
rcoulomb = 1.0 ; short-range electrostatic cutoff (in nm)
rvdw = 1.0 ; short-range van der Waals cutoff (in nm)
; Electrostatics
coulombtype = PME ; Particle Mesh Ewald for long-range
electrostatics
pme_order = 4 ; cubic interpolation
fourierspacing = 0.12 ; grid spacing for FFT
; Temperature coupling is on
tcoupl = nose-hoover ; modified Berendsen thermostat
tc-grps = Protein Non-Protein ; two coupling groups - more
accurate
tau_t = 2.5 2.5 ; time constant, in ps
ref_t = 300 300 ; reference temperature, one for each
group, in K
; Pressure coupling is off
pcoupl = no ; no pressure coupling in NVT
; Periodic boundary conditions
pbc = xyz ; 3-D PBC
; Dispersion correction
DispCorr = EnerPres ; account for cut-off vdW scheme
; Velocity generation
gen_vel = no ; don’t assign velocities from Maxwell
distribution
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