mpirun -np 5 mdrun_plumed-hrex -v -plumed plumed.dat -multi 5 -replex 100 -s start.tpr -deffnm prod -hrex
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Repl 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23
Repl 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23
Repl 1.0 1.0 1.0 1.0 1.0 1.0 .99 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0
for 30ps single precision with gpu ( nstlist is 20 , exchange freq 500 ):
several different values for dplumed term including 0.00 (kT)
Repl average number of exchanges:
Repl 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23
Repl .98 .98 .98 .98 .98 .97 .95 .98 .98 .99 .97 .99 .98 .96 .96 .99 .96 .99 .99 .96 .97 .98 .96
Single precision is not giving the expected exchange rate of 1.0 for all replicas. I am wondering if gromacs is calculating the energy term in single precision and plumed in double precision ( PLUMED 2.0 always uses double precision ; https://groups.google.com/forum/#!topic/plumed-users/l11d83yvXUs, https://groups.google.com/forum/#!topic/plumed-users/MxCY_-tFLS4, https://groups.google.com/forum/#!msg/plumed-users/ey9eAWE3-tw/Xl7t5R860tMJ) , this gives slight deviation in the dplumed term which is affecting the exchange probability.
Does that mean with large systems we can only use plumed patched with gromacs double precision ? Is there a way for using plumed in single precision as well ? If not, would you consider this deviation significant?
Gromacs double precision is 50% slower than single precision for my system.
Thanks
Ruchi
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Repl 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23
Repl 1.0 1.0 .90 .71 .62 .90 1.0 .62 .90 .71 1.0 1.0 1.0 .95 1.0 .95 .95 1.0 1.0 .86 .95 .71 .95
Thanks
Ruchi
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;title = Replica exchange simulation from appropriate starting structure (all 24 replicas have different starting structure with same box size )
; Run parameters
integrator = sd ; stochastic-dynamics integrator
ld-seed = -1
nsteps = 500000000 ; the amount of time for the system to be simulated, 1us
dt = 0.002 ; 2 fs
nstcomm = 100
; Output control
nstxout = 0 ; save coordinates at last step only
nstvout = 0 ; save velocity at the last step only
nstcalcenergy = 100 ; should be a multiple of nstlist, every 1.0 ps
nstenergy = 25000 ; save energies every 50.0 ps
nstlog = 25000 ; update log file every 50.0 ps
nstxtcout = 25000 ; save xtc files cooordinates every 50.0 ps
xtc-grps = System ; saves the coordinates for the entire system
; Bond parameters
continuation = yes ; first dynamics run
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 ; Using group scheme
ns_type = grid ; search neighboring grid cells
nstlist = 20 ; 10 fs
rlist = 1.0 ; short-range neighborlist cutoff (in nm)
; Electrostatics
rcoulomb = 1.0 ; short-range electrostatic cutoff (in nm)
rvdw = 1.0 ; short-range van der Waals cutoff (in nm)
coulombtype = PME ; Particle Mesh Ewald for long-range electrostatics
pme_order = 4 ; cubic interpolation
fourierspacing = 0.12 ; grid spacing for FFT
optimize_fft = yes
; Temperature coupling is on with sd
tc-grps = Protein Non-Protein ; two coupling groups - more accurate
tau_t = 1.5 1.5 ; 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 ; give new velocities
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Repl 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23
Repl 1.0 1.0 1.0 1.0 1.0 1.0 .99 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0
replex 500
nstlist 20
total time 34.32000 ps
dplumed term includes non zero values
Repl 34 attempts, 17 odd, 17 even
Repl average number of exchanges:
Repl 0 1 2 3 4 5 6 7 8 9 10 11 12 13 14 15 16 17 18 19 20 21 22 23
Repl 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0 1.0
Thanks
Ruchi
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