[gmx-users] NVE Energy drop in Mixed Precision 4.6.7
Guillaume Chevrot
guillaume.chevrot at gmail.com
Tue Oct 7 10:07:48 CEST 2014
Hi,
You should maybe show us a plot of the energy for more than just a few
picoseconds.
Nevertheless, from my experience the only way to obtain constant energy
in the NVE ensemblewas to use double precision.
Guillaume
On 10/06/2014 09:34 PM, Johnny Lu wrote:
> The run was on 12 Xeon CPU with a GPU.
>
> On Mon, Oct 6, 2014 at 3:03 PM, Johnny Lu <johnny.lu128 at gmail.com> wrote:
>
>> here is the energy from nve1.edr
>> http://oi62.tinypic.com/2pqw70l.jpg
>>
>> On Mon, Oct 6, 2014 at 3:01 PM, Johnny Lu <johnny.lu128 at gmail.com> wrote:
>>
>>> Hi.
>>>
>>> The system has 9000 water and a ~160 aa amino acid and uses
>>> amber99SB-ildn.
>>>
>>> After extensive NPT (300ns, 2ns ts), and then NVT equilibrium (300 ns,
>>> 2ns ts), the NVE simulation still has energy drop, despite of the very
>>> small time step.
>>>
>>> Is double precision gromacs the only solution?
>>>
>>> The mdp file is:
>>>
>>> title = NVT equilibration
>>> ; Run parameters
>>> integrator = md ; leap-frog integrator
>>> nsteps = 29500000 ; 1 ns
>>> dt = 0.0002 ; 0.5 fs
>>>
>>> ;NVE
>>> ;nstcomm = 500 ; remove center of mass motion to reduce energy
>>> and temp. drift.
>>> shake-tol = 0.0000001 ; shake tolerance.
>>> verlet-buffer-drift = -1
>>>
>>>
>>> - Output control
>>> ;nstxout = 20 ; save coordinates every 1.0 ps
>>> ;nstvout = 4 ; save velocities every 1.0 ps
>>> ;nstfout = 20
>>> nstenergy = 20 ; save energies every 1.0 ps
>>>
>>> nstlog = 1000 ; update log file every 0.2 ps
>>> ; Bond parameters
>>> continuation = yes ; Restarting after NVT
>>> constraint_algorithm = lincs ; holonomic constraints
>>> constraints = all-bonds ; all bonds (even heavy atom-H bonds)
>>> constrained
>>> lincs_iter = 4 ; accuracy of LINCS
>>> lincs_order = 4 ; also related to accuracy
>>> ; Neighborsearching
>>> ns_type = grid ; search neighboring grid cells
>>> nstlist = 40 ; 10 fs
>>> rlist = 1.3 ; 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 = 6 ; cubic interpolation
>>> fourierspacing = 0.1 ; grid spacing for FFT
>>>
>>> ; Temperature coupling is off
>>> tcoupl = no ; modified Berendsen thermostat
>>> ; Pressure coupling is off
>>> pcoupl = no
>>>
>>> refcoord_scaling = com
>>> ; 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
>>> cutoff-scheme = Verlet
>>>
>>> Thank you in advance.
>>>
>>
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