<div dir="ltr"><br><br><div class="gmail_quote">2008/8/5 Justin A. Lemkul <span dir="ltr"><<a href="mailto:jalemkul@vt.edu">jalemkul@vt.edu</a>></span><br><blockquote class="gmail_quote" style="margin:0 0 0 .8ex;border-left:1px #ccc solid;padding-left:1ex;">
<div class="Ih2E3d"><br>
<blockquote class="gmail_quote" style="margin:0 0 0 .8ex;border-left:1px #ccc solid;padding-left:1ex">
Yes I done energy minimization, and mdrun output here:<br>
Steepest Descents converged to machine precision in 17 steps,<br>
but did not reach the requested Fmax < 10.<br>
Potential Energy = -1.6686725e+06<br>
Maximum force = 2.4212272e+07 on atom 5<br>
Norm of force = 3.4130568e+07<br>
</blockquote>
<br></div>
This would concern me a bit. You've got an enormous force on atom 5! That's probably causing the explosion. So even though the potential energy seems reasonable, you've got something pushing very hard against that particle, and it may be ripping your system apart.<br>
<br>
You were aiming for an Fmax < 10, and got nowhere close (by a factor of a million!) so I would check that initial configuration and examine your parameters closely.<br><font color="#888888">
<br>
-Justin<br>
<br>
</font><blockquote class="gmail_quote" style="margin:0 0 0 .8ex;border-left:1px #ccc solid;padding-left:1ex"><div><div class="Wj3C7c">
other files from my system here too. It is chain cosist 5 coarse-grained units, in initial conformation there are two parallel chains on distance nm.<br>
==============ffgmx.itp======================== [ defaults ]<br>
; nbfunc comb-rule gen-pairs fudgeLJ fudgeQQ<br>
1 1 no 1.0 1.0<br>
<br>
[ atomtypes ]<br>
<br>
B 337.000 0.000 A 4.275 2.14<br>
[ bondtypes ]<br>
; i j func b0 kb<br>
B B 1 1.3 1105.7 ; gaussian<br>
[ angletypes ]<br>
B B B 1 170.7 33.4<br>
[ dihedraltypes ]<br>
B B B B 1 164.9 0.87 1<br>
[ nonbond_params ]<br>
;i j C6 C12<br>
B B 1 4.275 2.14<br>
<br>
[ pairtypes ]<br>
;i j C6 C12<br>
B B 1 4.275 2.14<br>
<br>
=====================table.xvg===============================<br>
<br>
0 0.0 0.0 5.31525e-317 0.0 0.0 0.0<br>
0.0505051 0.0 0.0 2.72297e 0.0 0.0 0.0<br>
0.10101 0.0 0.0 6.64787e 0.0 0.0 0.0<br>
0.151515 0.0 0.0 5.12363e 0.0 0.0 0.0<br>
0.20202 0.0 0.0 1.6228e 0.0 0.0 0.0<br>
0.252525 0.0 0.0 1.11475e 0.0 0.0 0.0<br>
0.30303 0.0 0.0 1.24898e 0.0 0.0 0.0<br>
0.353535 0.0 0.0 195960 0.0 0.0 0.0<br>
0.40404 0.0 0.0 39279.7 0.0 0.0 0.0<br>
0.454545 0.0 0.0 9471.18 0.0 0.0 0.0<br>
0.505051 0.0 0.0 2632.59 0.0 0.0 0.0<br>
0.555556 0.0 0.0 816.605 0.0 0.0 0.0<br>
0.606061 0.0 0.0 275.131 0.0 0.0 0.0<br>
0.656566 0.0 0.0 98.1504 0.0 0.0 0.0<br>
0.707071 0.0 0.0 36.0257 0.0 0.0 0.0<br>
0.757576 0.0 0.0 13.0521 0.0 0.0 0.0<br>
0.808081 0.0 0.0 4.28676 0.0 0.0 0.0<br>
0.858586 0.0 0.0 0.929196 0.0 0.0 0.0<br>
0.909091 0.0 0.0 -0.30352 0.0 0.0 0.0<br>
0.959596 0.0 0.0 -0.690878 0.0 0.0 0.0<br>
1.0101 0.0 0.0 -0.747432 0.0 0.0 0.0<br>
1.06061 0.0 0.0 -0.683641 0.0 0.0 0.0<br>
1.11111 0.0 0.0 -0.585339 0.0 0.0 0.0<br>
1.16162 0.0 0.0 -0.486288 0.0 0.0 0.0<br>
1.21212 0.0 0.0 -0.398389 0.0 0.0 0.0<br>
1.26263 0.0 0.0 -0.324521 0.0 0.0 0.0<br>
1.31313 0.0 0.0 -0.264044 0.0 0.0 0.0<br>
1.36364 0.0 0.0 -0.21515 0.0 0.0 0.0<br>
1.41414 0.0 0.0 -0.175831 0.0 0.0 0.0<br>
1.46465 0.0 0.0 -0.144252 0.0 0.0 0.0<br>
1.51515 0.0 0.0 -0.118857 0.0 0.0 0.0<br>
1.56566 0.0 0.0 -0.0983815 0.0 0.0 0.0<br>
1.61616 0.0 0.0 -0.0818131 0.0 0.0 0.0<br>
1.66667 0.0 0.0 -0.0683514 0.0 0.0 0.0<br>
1.71717 0.0 0.0 -0.0573661 0.0 0.0 0.0<br>
1.76768 0.0 0.0 -0.0483612 0.0 0.0 0.0<br>
1.81818 0.0 0.0 -0.0409463 0.0 0.0 0.0<br>
1.86869 0.0 0.0 -0.0348131 0.0 0.0 0.0<br>
1.91919 0.0 0.0 -0.0297176 0.0 0.0 0.0<br>
1.9697 0.0 0.0 -0.025466 0.0 0.0 0.0<br>
2.0202 0.0 0.0 -0.0219036 0.0 0.0 0.0<br>
2.07071 0.0 0.0 -0.0189067 0.0 0.0 0.0<br>
2.12121 0.0 0.0 -0.0163756 0.0 0.0 0.0<br>
2.17172 0.0 0.0 -0.0142297 0.0 0.0 0.0<br>
2.22222 0.0 0.0 -0.0124039 0.0 0.0 0.0<br>
2.27273 0.0 0.0 -0.010845 0.0 0.0 0.0<br>
2.32323 0.0 0.0 -0.00950938 0.0 0.0 0.0<br>
2.37374 0.0 0.0 -0.00836141 0.0 0.0 0.0<br>
2.42424 0.0 0.0 -0.00737164 0.0 0.0 0.0<br>
2.47475 0.0 0.0 -0.00651568 0.0 0.0 0.0<br>
2.52525 0.0 0.0 -0.0057733 0.0 0.0 0.0<br>
2.57576 0.0 0.0 -0.00512764 0.0 0.0 0.0<br>
2.62626 0.0 0.0 -0.00456457 0.0 0.0 0.0<br>
2.67677 0.0 0.0 -0.00407227 0.0 0.0 0.0<br>
2.72727 0.0 0.0 -0.00364076 0.0 0.0 0.0<br>
2.77778 0.0 0.0 -0.00326162 0.0 0.0 0.0<br>
2.82828 0.0 0.0 -0.00292772 0.0 0.0 0.0<br>
2.87879 0.0 0.0 -0.002633 0.0 0.0 0.0<br>
2.92929 0.0 0.0 -0.00237231 0.0 0.0 0.0<br>
2.9798 0.0 0.0 -0.00214121 0.0 0.0 0.0<br>
3.0303 0.0 0.0 -0.00193595 0.0 0.0 0.0<br>
3.08081 0.0 0.0 -0.00175327 0.0 0.0 0.0<br>
3.13131 0.0 0.0 -0.00159038 0.0 0.0 0.0<br>
3.18182 0.0 0.0 -0.00144487 0.0 0.0 0.0<br>
3.23232 0.0 0.0 -0.00131466 0.0 0.0 0.0<br>
3.28283 0.0 0.0 -0.00119792 0.0 0.0 0.0<br>
3.33333 0.0 0.0 -0.0010931 0.0 0.0 0.0<br>
3.38384 0.0 0.0 -0.000998824 0.0 0.0 0.0<br>
3.43434 0.0 0.0 -0.000913896 0.0 0.0 0.0<br>
3.48485 0.0 0.0 -0.000837272 0.0 0.0 0.0<br>
3.53535 0.0 0.0 -0.000768038 0.0 0.0 0.0<br>
3.58586 0.0 0.0 -0.000705391 0.0 0.0 0.0<br>
3.63636 0.0 0.0 -0.000648625 0.0 0.0 0.0<br>
3.68687 0.0 0.0 -0.000597116 0.0 0.0 0.0<br>
3.73737 0.0 0.0 -0.000550316 0.0 0.0 0.0<br>
3.78788 0.0 0.0 -0.00050774 0.0 0.0 0.0<br>
3.83838 0.0 0.0 -0.000468957 0.0 0.0 0.0<br>
3.88889 0.0 0.0 -0.000433586 0.0 0.0 0.0<br>
3.93939 0.0 0.0 -0.000401288 0.0 0.0 0.0<br>
3.9899 0.0 0.0 -0.000371763 0.0 0.0 0.0<br>
4.0404 0.0 0.0 -0.000344741 0.0 0.0 0.0<br>
4.09091 0.0 0.0 -0.000319982 0.0 0.0 0.0<br>
4.14141 0.0 0.0 -0.000297274 0.0 0.0 0.0<br>
4.19192 0.0 0.0 -0.000276423 0.0 0.0 0.0<br>
4.24242 0.0 0.0 -0.000257258 0.0 0.0 0.0<br>
4.29293 0.0 0.0 -0.000239626 0.0 0.0 0.0<br>
4.34343 0.0 0.0 -0.000223388 0.0 0.0 0.0<br>
4.39394 0.0 0.0 -0.000208419 0.0 0.0 0.0<br>
4.44444 0.0 0.0 -0.000194607 0.0 0.0 0.0<br>
4.49495 0.0 0.0 -0.000181851 0.0 0.0 0.0<br>
4.54545 0.0 0.0 -0.00017006 0.0 0.0 0.0<br>
4.59596 0.0 0.0 -0.000159152 0.0 0.0 0.0<br>
4.64646 0.0 0.0 -0.000149051 0.0 0.0 0.0<br>
4.69697 0.0 0.0 -0.00013969 0.0 0.0 0.0<br>
4.74747 0.0 0.0 -0.000131008 0.0 0.0 0.0<br>
4.79798 0.0 0.0 -0.000122948 0.0 0.0 0.0<br>
4.84848 0.0 0.0 -0.000115462 0.0 0.0 0.0<br>
4.89899 0.0 0.0 -0.000108502 0.0 0.0 0.0<br>
4.94949 0.0 0.0 -0.000102026 0.0 0.0 0.0<br>
5 0.0 0.0 -9.59969e-05 0.0 0.0 0.0<br>
<br>
=================================grompp.mdp====================<br>
<br>
<br>
; File 'mdout.mdp' was generated<br>
; By user: spoel (291)<br>
; On host: chagall<br>
; At date: Mon Dec 15 13:52:23 2003<br>
;<br>
<br>
; VARIOUS PREPROCESSING OPTIONS<br>
title = Perylene<br>
;cpp = xlc -E<br>
cpp = cpp<br>
include =<br>
define =<br>
<br>
; RUN CONTROL PARAMETERS<br>
integrator = steep<br>
; Start time and timestep in ps<br>
tinit = 0<br>
dt = 0.002<br>
nsteps = 10000 ; For exact run continuation or redoing part of a run<br>
init_step = 0<br>
; mode for center of mass motion removal<br>
;comm-mode = None<br>
comm-mode = Linear<br>
;comm-mode = Angular<br>
; number of steps for center of mass motion removal<br>
nstcomm = 1<br>
; group(s) for center of mass motion removal<br>
comm-grps =<br>
<br>
; LANGEVIN DYNAMICS OPTIONS<br>
; Temperature, friction coefficient (amu/ps) and random seed<br>
bd-fric = 0.5<br>
ld-seed = 1993<br>
<br>
; ENERGY MINIMIZATION OPTIONS<br>
; Force tolerance and initial step-size<br>
emtol = 10<br>
emstep = 0.01<br>
; Max number of iterations in relax_shells<br>
niter = 2000<br>
; Step size (1/ps^2) for minimization of flexible constraints<br>
fcstep = 0<br>
; Frequency of steepest descents steps when doing CG<br>
nstcgsteep = 1000<br>
nbfgscorr = 10<br>
<br>
; OUTPUT CONTROL OPTIONS<br>
; Output frequency for coords (x), velocities (v) and forces (f)<br>
nstxout = 10000<br>
nstvout = 0<br>
nstfout = 0<br>
; Checkpointing helps you continue after crashes<br>
nstcheckpoint = 10000<br>
; Output frequency for energies to log file and energy file<br>
nstlog = 10000<br>
nstenergy = 10000<br>
; Output frequency and precision for xtc file<br>
nstxtcout = 100<br>
xtc-precision = 1000<br>
; This selects the subset of atoms for the xtc file. You can<br>
; select multiple groups. By default all atoms will be written.<br>
xtc-grps =<br>
; Selection of energy groups<br>
energygrps =<br>
<br>
; NEIGHBORSEARCHING PARAMETERS<br>
; nblist update frequency<br>
nstlist = 5<br>
; ns algorithm (simple or grid)<br>
ns_type = grid<br>
; Periodic boundary conditions: xyz (default), no (vacuum)<br>
; or full (infinite systems only)<br>
;pbc = no<br>
pbc = xyz<br>
; nblist cut-off<br>
rlist = 1.0<br>
domain-decomposition = no<br>
<br>
; OPTIONS FOR ELECTROSTATICS AND VDW<br>
; Method for doing electrostatics<br>
coulombtype = Cut-off rcoulomb-switch = 0<br>
rcoulomb = 1.0<br>
; Dielectric constant (DC) for cut-off or DC of reaction field<br>
epsilon-r = 1<br>
; Method for doing Van der Waals<br>
vdw-type = User<br>
; cut-off lengths<br>
rvdw-switch = 0<br>
rvdw = 1.0<br>
; Apply long range dispersion corrections for Energy and Pressure<br>
DispCorr = EnerPres<br>
; Extension of the potential lookup tables beyond the cut-off<br>
table-extension = 1<br>
; Spacing for the PME/PPPM FFT grid<br>
fourierspacing = 0.12<br>
; FFT grid size, when a value is 0 fourierspacing will be used<br>
fourier_nx = 0<br>
fourier_ny = 0<br>
fourier_nz = 0<br>
; EWALD/PME/PPPM parameters<br>
pme_order = 4<br>
ewald_rtol = 1e-05<br>
ewald_geometry = 3d<br>
epsilon_surface = 0<br>
optimize_fft = no<br>
<br>
; GENERALIZED BORN ELECTROSTATICS<br>
; Algorithm for calculating Born radii<br>
gb_algorithm = Still<br>
; Frequency of calculating the Born radii inside rlist<br>
nstgbradii = 1<br>
; Cutoff for Born radii calculation; the contribution from atoms<br>
; between rlist and rgbradii is updated every nstlist steps<br>
rgbradii = 2<br>
; Salt concentration in M for Generalized Born models<br>
gb_saltconc = 0<br>
<br>
; IMPLICIT SOLVENT (for use with Generalized Born electrostatics)<br>
implicit_solvent = No<br>
<br>
; OPTIONS FOR WEAK COUPLING ALGORITHMS<br>
; Temperature coupling<br>
;Tcoupl = yes<br>
Tcoupl = Berendsen<br>
; Groups to couple separately<br>
tc-grps = System<br>
; Time constant (ps) and reference temperature (K)<br>
tau_t = 0.01<br>
ref_t = 300<br>
; Pressure coupling<br>
;Pcoupl = Berendsen<br>
Pcoupl = no<br>
;Pcoupltype = isotropic<br>
; Time constant (ps), compressibility (1/bar) and reference P (bar)<br>
tau_p = 5.0<br>
compressibility = 4.5e-5<br>
ref_p = 1.0<br>
; Random seed for Andersen thermostat<br>
andersen_seed = 815131<br>
<br>
; SIMULATED ANNEALING<br>
; Type of annealing for each temperature group (no/single/periodic)<br>
annealing = no<br>
; Number of time points to use for specifying annealing in each group<br>
annealing_npoints =<br>
; List of times at the annealing points for each group<br>
ANnealing_time =<br>
; Temp. at each annealing point, for each group.<br>
annealing_temp =<br>
<br>
; GENERATE VELOCITIES FOR STARTUP RUN<br>
gen_vel = yes<br>
gen_temp = 300<br>
gen_seed = 1993<br>
<br>
; OPTIONS FOR BONDS<br>
constraints = none<br>
;constraints = all-bonds<br>
; Type of constraint algorithm<br>
constraint-algorithm = Lincs<br>
; Do not constrain the start configuration<br>
unconstrained-start = no<br>
; Use successive overrelaxation to reduce the number of shake iterations<br>
Shake-SOR = no<br>
; Relative tolerance of shake<br>
shake-tol = 1e-04<br>
; Highest order in the expansion of the constraint coupling matrix<br>
lincs-order = 4<br>
; Number of iterations in the final step of LINCS. 1 is fine for<br>
; normal simulations, but use 2 to conserve energy in NVE runs.<br>
; For energy minimization with constraints it should be 4 to 8.<br>
lincs-iter = 1<br>
; Lincs will write a warning to the stderr if in one step a bond<br>
; rotates over more degrees than<br>
lincs-warnangle = 30<br>
; Convert harmonic bonds to morse potentials<br>
morse = no<br>
<br>
; ENERGY GROUP EXCLUSIONS<br>
; Pairs of energy groups for which all non-bonded interactions are excluded<br>
energygrp_excl =<br>
<br>
; NMR refinement stuff<br>
; Distance restraints type: No, Simple or Ensemble<br>
disre = No<br>
; Force weighting of pairs in one distance restraint: Conservative or Equal<br>
disre-weighting = Conservative<br>
; Use sqrt of the time averaged times the instantaneous violation<br>
disre-mixed = no<br>
disre-fc = 1000<br>
disre-tau = 0<br>
; Output frequency for pair distances to energy file<br>
nstdisreout = 100<br>
; Orientation restraints: No or Yes<br>
orire = no<br>
; Orientation restraints force constant and tau for time averaging<br>
orire-fc = 0<br>
orire-tau = 0<br>
orire-fitgrp =<br>
; Output frequency for trace(SD) to energy file<br>
nstorireout = 100<br>
; Dihedral angle restraints: No, Simple or Ensemble<br>
dihre = No<br>
dihre-fc = 1000<br>
dihre-tau = 0<br>
; Output frequency for dihedral values to energy file<br>
nstdihreout = 100<br>
<br>
; Free energy control stuff<br>
free-energy = no<br>
init-lambda = 0<br>
delta-lambda = 0<br>
sc-alpha = 0<br>
sc-sigma = 0.3<br>
<br>
; Non-equilibrium MD stuff<br>
acc-grps =<br>
accelerate =<br>
freezegrps =<br>
freezedim =<br>
cos-acceleration = 0<br>
<br>
; Electric fields<br>
; Format is number of terms (int) and for all terms an amplitude (real)<br>
; and a phase angle (real)<br>
E-x =<br>
E-xt =<br>
E-y =<br>
E-yt =<br>
E-z =<br>
E-zt =<br>
<br>
; User defined thingies<br>
user1-grps =<br>
user2-grps =<br>
userint1 = 0<br>
userint2 = 0<br>
userint3 = 0<br>
userint4 = 0<br>
userreal1 = 0<br>
userreal2 = 0<br>
userreal3 = 0<br>
userreal4 = 0<br>
<br>
<br>
<br>
<br></div></div><div class="Ih2E3d">
------------------------------------------------------------------------<br>
<br>
_______________________________________________<br>
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</div></blockquote><div><div class="Wj3C7c">
<br>
-- <br>
========================================<br>
<br>
Justin A. Lemkul<br>
Graduate Research Assistant<br>
Department of Biochemistry<br>
Virginia Tech<br>
Blacksburg, VA<br>
jalemkul[at]<a href="http://vt.edu" target="_blank">vt.edu</a> | (540) 231-9080<br>
<a href="http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin" target="_blank">http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin</a><br>
<br>
========================================<br>
_______________________________________________<br>
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</div></div></blockquote></div>Ok, Thank you very much, I will wait you reply.<br></div>