[gmx-users] compressing the system

Moeed lecielll at googlemail.com
Thu Jul 29 05:41:05 CEST 2010


Dear Dr.Chaban,

I tried to get the same results as you got for density and total energy
starting from the 8 chains is the box. I used the revised mdp file and since
PME option takes much time I used shift instead for a moment to verify if I
can get the density you obtained. Also I used constraints for bonds. density
I get after 1800ps is 850 kg/m3 while what you got is a slightly different
(after 1000ps density varies around 880!). Also the total energy you have is
bout 2300 whereas I get somethong around 12000!. I dont know why they are so
different..

In the second trial I used "constraints         =  none" just the "shift"
for electrostatics is not the same as the mdp file you suggested. again
results are not the same for total energy (20000 Kj/mol). Below is the
average values...also simulation crashes at 1550 ps and the last density I
am getting is 834! still less than what you got. dont really know why
results are not the same. The reason simulation crashes could be due to
dt=0.002 while removing constraints?

I have two more inquiries:

1- What I see is that the system is getting compressed to a size of around 3
3 3 nm is the first 20ps abruptly and in the remainder of time system
reaches equilibrium... This is very different approach than what I was
trying doing before. I used berendsen scheme for pressure coupling and box
reduced is size slowly but I had difficulty reaching the size I want and
most of the simulations crashed. Does this mean berenden is not suitable for
compressing system for all systems?

2- You said I dont need NVT at all. But if I want to study the system I get
from NPT giving the density I want, can I not do NVT for a fixed system size
and calcualte energies or other quantities I am after?

Thanks for your attention
Moeed


Energy                      Average       RMSD     Fluct.      Drift
Tot-Drift
-------------------------------------------------------------------------------
Bond                        3885.23    141.365    139.725  0.0478427
74.3668
Angle                       5864.23    149.886    149.885 -0.00114897
-1.78597
Ryckaert-Bell.              2243.62    144.068    134.737  -0.113664
-176.679
LJ-14                        1167.5    30.8742    30.6402 -0.00845667
-13.1451
Coulomb-14                 -553.954    31.3413    30.7865 -0.0130831
-20.3364
LJ (SR)                    -4898.73    405.434    386.584  -0.272304
-423.27
Coulomb (SR)                1250.22    56.2361    56.1252  0.0078672
12.2288
Potential                   8958.11    379.038    344.366  -0.352947
-548.621
Kinetic En.                 10834.2    156.085    156.066 -0.00535835
-8.32903
Total Energy                19792.3    414.016    381.523  -0.358305
-556.95
Temperature                 300.069    4.32299    4.32248 -0.000148407
-0.230684
Pressure (bar)              29.5896    1263.17    1263.16  0.0112876
17.5454
Box-X                       3.67408    1.72247    1.70558 -0.000536305
-0.833634
Box-Y                       3.44445    1.61482    1.59898 -0.000502786
-0.781532
Box-Z                       2.45126    1.66735    1.64995 -0.000535423
-0.832263
Density (SI)                815.504    72.8491    70.7123  0.0390324
60.6721
pV                          54.9014     2111.1    2111.07 -0.0208174
-32.3586
Vir-XX                      3606.98    1466.95    1466.92  0.0213665
33.2121
Box-Vel-XX               -0.0182685   0.234428   0.232397 6.8633e-05
0.106683
Mu-Y                       0.102393   0.966426   0.966077 -5.79406e-05
-0.0900631
Heat Capacity Cv:      12.4757 J/mol K (factor = 0.000207551)


;        Run control
integrator          =  md                 ; type of dynamics algorithm. Here
md uses a leap-frog algorithm for integrating Newtons's eq of motion
dt                  =  0.002                 ; in ps !
nsteps              =  900000                  ; length of simulation=
nsteps*dt
nstcomm             =  1                 ; frequency for center of mass
motion removal

;        Output control
nstenergy           =  100                  ; frequency to write energies to
energy file. i.e., energies and other statistical data are stored every 10
steps
nstxout             =  100                 ; frequency to write
coordinates/velocity/force to output trajectory file. how often snapshots
are collected= nstxout*dt
nstvout             =  0
nstfout             =  0
nstlog              =  1000                 ; frequency to write energies to
log file
nstxtcout          =  0                 ; frequency to write coordinates to
xtc trajectory

;        Neighbor searching
nstlist             =  10                 ; frequency to update neighbor
list. Neighborlist will be updated at least every 10 steps. Manual p80
ns_type             =  grid                 ; make a grid in the box and
only check atoms in neighboring grid cells when constructing a new neighbor
list every nstlist steps

;        Electrostatics/VdW
coulombtype         =  Shift      ;PME rev     ; tells gromacs how to model
electrostatics. Shift: Coulomb/LJ potential is decreased over the whole
range and forces decay smoothly to zero between
vdw-type            =  Shift               ; rcoulomb-switch/rvw-switch &
rcoulomb/rvdw
rcoulomb-switch    =   0.9    ;0              ; where to start switching the
Coulomb potential
rvdw-switch         =  0.9 ;0                 ; where to start switching the
LJ potential

;        Cut-offs
rlist               =  1.1                 ; in nm. Cut-off distance for
short-range neighbor list
rcoulomb            =  1.1 ;1.0             ; distance for coulomb cut-off
rvdw                =  1.0                 ; distance for coulomb cut-off

;        Temperature coupling
Tcoupl              =  v-rescale             ;berendsen
tc-grps             =  System  ;HEX             ; groups to couple to
thermostat; Berendsen temperature coupling is on in these groups
tau_t               =  0.1     ;0.1             ; time constant for T
coupling
ref_t               =  300     ;300             ; reference T for coupling.
When you alter the T, don't forget to change the gen_temp for velocity
generation

;        Pressure coupling
Pcoupl              =  Parrinello-Rahman           ;berendsen
Pcoupltype          =  semiisotropic ;isotropic  ; isotropic: means the box
expands and contracts in all directions(x,y,z)in order to maintain the
proper pressure; semiisotropic: isotropic in x & y directions
tau_p               =  1       1        ;0.5        ; time constant for
coupling in ps
compressibility     =  4.5e-5     4.5e-5         ; compressibility of
solvent used in simulation in 1/bar
ref_p               =  30.0     30.0             ; reference P for coupling
in bar

;        Velocity generation               Generate velocites is on at 300
K. Manual p155
gen_vel             =  yes                 ; generate velocites according to
Maxwell distribution at T: gen_temp with random gen seed gen_seed
gen_temp            =  300.0                 ; T for Maxwell distribution
gen_seed            =  173529                 ; used to initialize random
generator for random velocities

;        Bonds
constraints         =  none     ;all-bonds              ; sets the LINCS
constraint for all bonds
constraint-algorithm = lincs
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