[gmx-users] Gromacs on GPU: GTX or Tesla?

2011-08-04 Thread Efrat Exlrod
Hi,



We want to start using Gromacs on GPU and we are debating whether to purchase 
GeForce GTX card or Tesla platform. Looking at the published data it seems 
GTX580 has much impressive performance compared to Tesla C2050, and of course 
it is much cheaper. Is there a reason to prefer Tesla over GTX for running 
Gromacs in the short or long term?



Thanks, Efrat
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[gmx-users] RE: Gromacs on GPU: GTX or Tesla?

2011-08-04 Thread Jagdish S. Varma
Hi,
In the long term the Tesla is much more preferable as the GTX would not support 
certain high end functions. Pls verify these before you purchase one. Also the 
Tesla C-2070 is the newer one available and with 6.0GB RAM it really gives out 
great performance. The price is the same.

Rgds
JSV

From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org] On Behalf 
Of Efrat Exlrod [efrat.exl...@biu.ac.il]
Sent: Thursday, August 04, 2011 12:13 PM
To: gmx-users@gromacs.org
Subject: [gmx-users] Gromacs on GPU: GTX or Tesla?


Hi,



We want to start using Gromacs on GPU and we are debating whether to purchase 
GeForce GTX card or Tesla platform. Looking at the published data it seems 
GTX580 has much impressive performance compared to Tesla C2050, and of course 
it is much cheaper. Is there a reason to prefer Tesla over GTX for running 
Gromacs in the short or long term?



Thanks, Efrat


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[gmx-users] Regarding Segmentation fault during mdrun_d

2011-08-04 Thread Ravi Kumar Venkatraman
Dear All,
 I was trying to run NVT equilibration for cyclohexane. When I
started running it shows following error

Reading file nvt.tpr, VERSION 4.5.4 (double precision)
Starting 2 threads
Making 1D domain decomposition 2 x 1 x 1
starting mdrun 'Cyclohexane box'
5 steps,100.0 ps.
Segmentation fault.

Please suggest me something to overcome this.
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Re: [gmx-users] Regarding Segmentation fault during mdrun_d

2011-08-04 Thread lina
On Thu, Aug 4, 2011 at 3:03 PM, Ravi Kumar Venkatraman
ravikumarvenkatra...@gmail.com wrote:
 Dear All,
  I was trying to run NVT equilibration for cyclohexane. When I
 started running it shows following error

 Reading file nvt.tpr, VERSION 4.5.4 (double precision)
 Starting 2 threads
 Making 1D domain decomposition 2 x 1 x 1
 starting mdrun 'Cyclohexane box'
 5 steps,    100.0 ps.
 Segmentation fault.

 Please suggest me something to overcome this.

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try mdrun -pd

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Best Regards,

lina
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Re: [gmx-users] Regarding Segmentation fault during mdrun_d

2011-08-04 Thread Mark Abraham

On 4/08/2011 5:03 PM, Ravi Kumar Venkatraman wrote:

Dear All,
 I was trying to run NVT equilibration for cyclohexane. 
When I started running it shows following error


Reading file nvt.tpr, VERSION 4.5.4 (double precision)
Starting 2 threads
Making 1D domain decomposition 2 x 1 x 1
starting mdrun 'Cyclohexane box'
5 steps,100.0 ps.
Segmentation fault.

Please suggest me something to overcome this.


Depends what is going wrong. Consult the .log file.

Mark
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[gmx-users] g_dipoles - averaging

2011-08-04 Thread Kukol, Andreas
Hello, 

Is there any way to output the dipole moment averaged over all molecules or for 
each molecule separately (and not the total dipole moment of the simulation 
box) ?

Apparently the dipole autocorrelation function can be obtained as an average 
over all molecules with the '-corr mol' option, but from the help info it is 
not clear, how and if the total dipole moment can be obtained in this way (and 
in which file Mtot.xvg or aver.xvg ?).

Many thanks
Andreas

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[gmx-users] the density does not stablize

2011-08-04 Thread xiaowu759
Dear gmxers,
 I try to perform NPT MD to obtain the density of system. But the value of 
density does not stablize even after over 40 ns. The content of mdp file can be 
seen below. How to deal with it? Please give me some hints. Thanks a lot for 
any replies.
  
 .mdp file: 
 title= 
 cpp= /lib/cpp
include= -I../top
define= ;{-DFLEXIBLE,-DPOSRES} 
integrator   = md
dt= 0.001
comm_mode   = Linear   ;{Linear,Angular,No}
nstcomm   = 10
nstcalcenergy   = 1
nsttcouple   = 1
nstpcouple   = 1
comm_grps   = 
nsteps = 2500
nstxout= 1000
nstvout= 1000
nstlog = 1000
nstenergy   = 1000
nstxtcout   = 1000
nstlist= 10
ns_type= grid;{simple,grid}
rlist= 1.0
coulombtype   = pme
fourierspacing  = 0.12; [0.12 nm]
optimize_fft   = yes;{no,yes}
rcoulomb   = 1.0
rvdw= 1.0
DispCorr   = EnerPres   ;{no,EnerPres,Ener}
pbc= xyz; Periodic Boundary Conditions {xyz,no,xy}
tcoupl = berendsen  ;no,berendsen,nose-hoover,v-rescale
tc-grps= Other 
tau_t= 0.1 
ref_t= 600  
Pcoupl = berendsen  ;{no,berendsen,Parrinello-Rahman}
Pcoupltype  = isotropic   ;{isotropic,semiisotropic;anisotropic;surface-tension}
tau_p= 0.1
compressibility   = 4.5e-5
ref_p= 1.0;the unit is bar(1 bar =10^5 Pa)
gen_vel= no 
gen_temp   = 600
gen_seed   = 173529
constraints   = none;{none,hbonds,all-bonds,h-angles,all-angles}
constraint_algorithm  = LINCS   ;{LINCS,SHAKE}
periodic_molecules  = no;{no,yes}
 annealing   = no ;{no,single,periodic}
annealing_npoints  = 11
annealing_time  = 0  100  200  300  400  500  600  700  800  900  1000
annealing_temp  = 600  580  560  540  520  500  520  540  560  580  600

 Best regards,
 Dr. Chaofu Wu
  --
  Department of Chemistry and Materials Science
 Hunan University of Humanities, Science and Technology, 
 Loudi 417000, the People's Republic of China (P.R. China)-- 
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Re: [gmx-users] the density does not stablize

2011-08-04 Thread Mark Abraham


On 04/08/11, xiaowu759  xiaowu...@qq.com wrote:
 Dear gmxers,
 
 I try to perform NPT MD to obtain the density of system. But the value of 
 density does not stablize even after over 40 ns. The content of mdp file can 
 be seen below. How to deal with it? Please give me some hints. Thanks a lot 
 for any replies.
 
 

We have no idea whether your judgement that density is not stabilized after 
40ns is sound, because you provided no data. Your temperature coupling is to 
group Other, which may or may not be reasonable. Your integration time step 
is possibly too large for a simulation using no bond constraints. Your initial 
density could be so far from correct that reaching equilibrium is infeasible. 
You'll need to provide a lot more information to get useful help.

Mark


 
 
  
 
 .mdp file: 
 
 title    = 
 
 cpp    = /lib/cpp
 include    = -I../top
 define    = ;{-DFLEXIBLE,-DPOSRES} 
 integrator   = md
 dt    = 0.001
 comm_mode   = Linear   ;{Linear,Angular,No}
 nstcomm   = 10
 nstcalcenergy   = 1
 nsttcouple   = 1
 nstpcouple   = 1
 comm_grps   = 
 nsteps     = 2500
 nstxout    = 1000
 nstvout    = 1000
 nstlog     = 1000
 nstenergy   = 1000
 nstxtcout   = 1000
 nstlist    = 10
 ns_type    = grid;{simple,grid}
 rlist    = 1.0
 coulombtype   = pme
 fourierspacing  = 0.12; [0.12 nm]
 optimize_fft   = yes;{no,yes}
 rcoulomb   = 1.0
 rvdw    = 1.0
 DispCorr   = EnerPres   ;{no,EnerPres,Ener}
 pbc    = xyz; Periodic Boundary Conditions {xyz,no,xy}
 tcoupl     = berendsen  ;no,berendsen,nose-hoover,v-rescale
 tc-grps    = Other 
 tau_t    = 0.1     
 ref_t    = 600  
 Pcoupl     = berendsen  ;{no,berendsen,Parrinello-Rahman}
 Pcoupltype  = 
 isotropic   ;{isotropic,semiisotropic;anisotropic;surface-tension}
 tau_p    = 0.1
 compressibility   = 4.5e-5
 ref_p    = 1.0;the unit is bar(1 bar =10^5 Pa)
 gen_vel    = no 
 gen_temp   = 600
 gen_seed   = 173529
 constraints   = none;{none,hbonds,all-bonds,h-angles,all-angles}
 constraint_algorithm  = LINCS   ;{LINCS,SHAKE}
 periodic_molecules  = no;{no,yes}
 
 annealing   = no ;{no,single,periodic}
 annealing_npoints  = 11
 annealing_time  = 0  100  200  300  400  500  600  700  800  900  1000
 annealing_temp  = 600  580  560  540  520  500  520  540  560  580  600
 
 
 Best regards,
 
 Dr. Chaofu Wu
 
 
 --
 
 
 Department of Chemistry and Materials Science
 
 Hunan University of Humanities, Science and Technology, 
 
 Loudi 417000, the People's Republic of China (P.R. China)
 
 
 
  
 

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Re: [gmx-users] setting vdw cutoff with specific force-filed?

2011-08-04 Thread Justin A. Lemkul



Yun Shi wrote:

Hi all,

I am working with GROMOS 53a6 ff in GROMACS 4.5, and I assume a 
Lennard-Jones interaction function was used for short-range vdw 
interactions.


 From the reference paper /A Biomolecular Force Field Based on the Free 
Enthalpy of Hydration and Solvation: The GROMOS Force-Field Parameter 
Sets 53A5 and 53A6/, I found that for example,


when rvdw = 1.5nm, the repulsion term of the interaction between two CH1 
type atoms (C12ij = 9.85^2) can be calculated as 9.850*9.850 / (1.5^12) 
= 0.747786 kJ/mol. So I wonder if this value is considered to be small 
enough to be ignored.


In addition, it seems not until 5 nm does the dispersion term become 
larger than the repulsion term in this case, so would turning on 
Dispersion Correction between, say 1.5 to 5 nm introduce more errors 
than turning it off?




You should use the cutoff described the authors of the force field, in this case 
rvdw=1.4.  Unless you can demonstrate that by using a different value you can 
achieve superior results, stick with the specifics of parameterization.  I have 
never seen ill effects of setting rvdw=1.4 and using dispersion correction with 
this force field.


-Justin

--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu | (540) 231-9080
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin


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[gmx-users] g_membed stops after only one iteration

2011-08-04 Thread maria goranovic
Hi

I am trying to use g_membed to insert a protein into a bilayer. I made some
changes to the sample.mdp file downloaded from the authors' homepage. The
changes were:

- reduced time step to 0.001 ps (instead of 0.002)
- changed constraints to hbonds instead of all-bonds.

g_membed runs fine, but stops only after one iteration after which the
protein is of course shrunk. The command used is:

echo 20 16 | g_membed -f membed.tpr  -n membed.ndx -xyinit 0.1 -xyend 1.0
-nxy 1000 -maxwarn 10

I am wondering what is going on ?

Also, is there a way to parallelize g_membed?



-- 
Maria G.
Technical University of Denmark
Copenhagen
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[gmx-users] Fwd: Regarding segmentation fault

2011-08-04 Thread Mark Abraham
 Please leave discussion on the mailing list so that the archives are available 
for posterity and that you might get input from more than one person.

Apparently your .log file has been truncated abnormally, but the energy values 
reported are clearly indicative of 
http://www.gromacs.org/Documentation/Terminology/Blowing_Up See that link for 
dealing with it.

Mark
---BeginMessage---
This is what I got from .log file please help me find the error.

---

Input Parameters:
   integrator   = md
   nsteps   = 5
   init_step= 0
   ns_type  = Grid
   nstlist  = 5
   ndelta   = 2
   nstcomm  = 10
   comm_mode= Linear
   nstlog   = 100
   nstxout  = 100
   nstvout  = 100
   nstfout  = 0
   nstcalcenergy= 5
   nstenergy= 100
   nstxtcout= 0
   init_t   = 0
   delta_t  = 0.002
   xtcprec  = 1000
   nkx  = 21
   nky  = 21
   nkz  = 21
   pme_order= 4
   ewald_rtol   = 1e-05
   ewald_geometry   = 0
   epsilon_surface  = 0
   optimize_fft = FALSE
   ePBC = xyz
   bPeriodicMols= FALSE
   bContinuation= FALSE
   bShakeSOR= FALSE
   etc  = Berendsen
   nsttcouple   = 5
   epc  = No
   epctype  = Isotropic
   nstpcouple   = -1
   tau_p= 1
   ref_p (3x3):
  ref_p[0]={ 0.0e+00,  0.0e+00,  0.0e+00}
  ref_p[1]={ 0.0e+00,  0.0e+00,  0.0e+00}
  ref_p[2]={ 0.0e+00,  0.0e+00,  0.0e+00}
   compress (3x3):
  compress[0]={ 0.0e+00,  0.0e+00,  0.0e+00}
  compress[1]={ 0.0e+00,  0.0e+00,  0.0e+00}
  compress[2]={ 0.0e+00,  0.0e+00,  0.0e+00}
   refcoord_scaling = No
   posres_com (3):
  posres_com[0]= 0.0e+00
  posres_com[1]= 0.0e+00
  posres_com[2]= 0.0e+00
   posres_comB (3):
  posres_comB[0]= 0.0e+00
  posres_comB[1]= 0.0e+00
  posres_comB[2]= 0.0e+00
   andersen_seed= 815131
   rlist= 1.6
   rlistlong= 1.6
   rtpi = 0.05
   coulombtype  = PME
   rcoulomb_switch  = 0
   rcoulomb = 1.6
   vdwtype  = Cut-off
   rvdw_switch  = 0
   rvdw = 1.6
   epsilon_r= 1
   epsilon_rf   = 1
   tabext   = 1
   implicit_solvent = No
   gb_algorithm = Still
   gb_epsilon_solvent   = 80
   nstgbradii   = 1
   rgbradii = 1
   gb_saltconc  = 0
   gb_obc_alpha = 1
   gb_obc_beta  = 0.8
   gb_obc_gamma = 4.85
gb_dielectric_offset = 0.009
   sa_algorithm = Ace-approximation
   sa_surface_tension   = 2.05016
   DispCorr = EnerPres
   free_energy  = no
   init_lambda  = 0
   delta_lambda = 0
   n_foreign_lambda = 0
   sc_alpha = 0
   sc_power = 0
   sc_sigma = 0.3
   sc_sigma_min = 0.3
   nstdhdl  = 10
   separate_dhdl_file   = yes
   dhdl_derivatives = yes
   dh_hist_size = 1
   dh_hist_spacing  = 0.1
   nwall= 0
   wall_type= 9-3
   wall_atomtype[0] = -1
   wall_atomtype[1] = -1
   wall_density[0]  = 0
   wall_density[1]  = 0
   wall_ewald_zfac  = 3
   pull = no
   disre= No
   disre_weighting  = Conservative
   disre_mixed  = FALSE
   dr_fc= 1000
   dr_tau   = 0
   nstdisreout  = 100
   orires_fc= 0
   orires_tau   = 0
   nstorireout  = 100
   dihre-fc = 1000
   em_stepsize  = 0.01
   em_tol   = 10
   niter= 20
   fc_stepsize  = 0
   nstcgsteep   = 1000
   em_stepsize  = 0.01
   em_tol   = 10
   niter= 20
   fc_stepsize  = 0
   nstcgsteep   = 1000
   nbfgscorr= 10
   ConstAlg = Lincs
   shake_tol= 0.0001
   lincs_order  = 4
   lincs_warnangle  = 30
   lincs_iter   = 1
   bd_fric  = 0
   ld_seed  = 1993
   cos_accel= 0
   deform (3x3):
  deform[0]={ 0.0e+00,  0.0e+00,  0.0e+00}
  deform[1]={ 0.0e+00,  0.0e+00,  0.0e+00}
  deform[2]={ 0.0e+00,  0.0e+00,  0.0e+00}
   userint1 = 0
   userint2 = 0
   userint3 = 0
   userint4 = 0
   userreal1= 0
   userreal2= 0
   userreal3= 0
   userreal4= 0

[gmx-users] Hydrogen atoms type

2011-08-04 Thread Amir Abbasi
Hi Dear Users!
I'm Using MMB to produce initial structures for my simulations.
This program creating a .pdb file in output.
The output file containing Hydrogen atoms that are not recognized by gromos53a5.
I want to edit my pdb file but I can't find anything about hydrogen types in 
gromos!
any suggestion?
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Re: [gmx-users] Hydrogen atoms type

2011-08-04 Thread Justin A. Lemkul



Amir Abbasi wrote:

Hi Dear Users!
I'm Using MMB to produce initial structures for my simulations.
This program creating a .pdb file in output.
The output file containing Hydrogen atoms that are not recognized by 
gromos53a5.
I want to edit my pdb file but I can't find anything about hydrogen 
types in gromos!

any suggestion?



The Gromos force fields are united-atom, so most H atoms are not used.  Aromatic 
hydrogens are type HC and polar hydrogens are type H.


If you're trying to run your structure through pdb2gmx and it's complaining, use 
-ignh and only necessary hydrogens will be built back on.


-Justin

--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu | (540) 231-9080
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin


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Re: [gmx-users] setting vdw cutoff with specific force-filed?

2011-08-04 Thread Mark Abraham


On 04/08/11, Justin A. Lemkul  jalem...@vt.edu wrote:
 
 
 Yun Shi wrote:
 Hi all,
 
 I am working with GROMOS 53a6 ff in GROMACS 4.5, and I assume a 
 Lennard-Jones interaction function was used for short-range vdw interactions.
 
  From the reference paper /A Biomolecular Force Field Based on the Free 
  Enthalpy of Hydration and Solvation: The GROMOS Force-Field Parameter Sets 
  53A5 and 53A6/, I found that for example,
 
 when rvdw = 1.5nm, the repulsion term of the interaction between two CH1 
 type atoms (C12ij = 9.85^2) can be calculated as 9.850*9.850 / (1.5^12) = 
 0.747786 kJ/mol. So I wonder if this value is considered to be small enough 
 to be ignored.
 

You should pay attention to the column headings in table 7 so that you can 
compute the contribution correctly. However, the magnitude of the energy of any 
particular interaction is not really of any concern. The evolution of the 
system depends on the *forces*, and it is likely that the sum of the forces on 
any atom from all its repulsion interactions from atoms that are (say) 1.4nm to 
1.5nm away is very close to zero, except in highly non-homogeneous spatial 
distributions of particles. In any case, the sum of that contribution will be 
much smaller than the other contributions.

Mark

 
 
 In addition, it seems not until 5 nm does the dispersion term become larger 
 than the repulsion term in this case, so would turning on Dispersion 
 Correction between, say 1.5 to 5 nm introduce more errors than turning it 
 off?
 
 
 You should use the cutoff described the authors of the force field, in this 
 case rvdw=1.4.  Unless you can demonstrate that by using a different value 
 you can achieve superior results, stick with the specifics of 
 parameterization.  I have never seen ill effects of setting rvdw=1.4 and 
 using dispersion correction with this force field.
 
 -Justin
 
 -- 
 
 
 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 MILES-IGERT Trainee
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
 
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[gmx-users] add Argon to a force field?

2011-08-04 Thread Amir Abbasi
   Hi!
I want to simulate an RNA molecule.
I have the .pdb file of that.
I want to create an Argon wall and make a hole on it to pull my molecule 
through it.
Argon defined in OPLS/AA force field. but it has not nucleic acids.
how can i define the argon in other force fields?
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Re: [gmx-users] add Argon to a force field?

2011-08-04 Thread Justin A. Lemkul



Amir Abbasi wrote:

   Hi!
I want to simulate an RNA molecule.
I have the .pdb file of that.
I want to create an Argon wall and make a hole on it to pull my molecule 
through it.

Argon defined in OPLS/AA force field. but it has not nucleic acids.
how can i define the argon in other force fields?



http://www.gromacs.org/Documentation/How-tos/Parameterization
http://www.gromacs.org/Documentation/How-tos/Adding_a_Residue_to_a_Force_Field

Simulations of argon have been done for many years.  You may be able to find 
suitable parameters by doing a literature search.


-Justin

--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu | (540) 231-9080
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin


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RE: [gmx-users] g_dipoles - averaging

2011-08-04 Thread Kukol, Andreas
Florian,

I am not sure, which of the output files of g_current contains the dipole 
moment for each molecule. Applying g_current to a trajectory of four molecules 
of asparagin in water gives the following output:

g_current -s tpr_200ps.tpr -f xtcIRWhole_100-200ps.xtc -eps 80 -o current.xvg
(selecting 4 molecules of asparagin from the index group)

md.xvg
@title Averaged rotational part of M
@xaxis  label Time (ps)
@yaxis  label  M\sD\N  (enm)
@TYPE xy
# time   x   y   z   average of M_D^2std.dev
0.000   -0.10261 0.12324 0.27085 0.09908 0.31477
0.001   -0.10421 0.12287 0.27297 0.09977 0.31587
0.002   -0.09766 0.12637 0.27104 0.09951 0.31543
...

dsp.xvg
@title MSD of the squared translational dipole moment M
@xaxis  label Time (ps)
@yaxis  label |M\sJ\N(t)-M\sJ\N(0)|\S2\N  / 6.0*V*k\sB\N*T / 
Sm\S-1\Nps\S-1\N
@TYPE xy
#Prefactor fit E-H: 1 / 6.0*V*k_B*T: 3.15249e-11
0.0000
0.001   8.70985e-30
0.002   1.9936e-29
...

mj.xvg
@title Averaged translational part of M
@xaxis  label Time (ps)
@yaxis  label  M\sJ\N  (enm)
@TYPE xy
# time   x   y   z   average of M_J^2std.dev
0.0000.1 0.0 0.0 0.0 0.1
0.0010.1 0.0 0.0 0.0 0.1
...

current.xvg was not produced due to:
...
...
Average volume V=32.764893 nm^3 at T=300.00 K
and corresponding refactor 1.0 / 3.0*V*k_B*T*EPSILON_0: 7.120911 
Too less points for a fit.verage volume V=32.764893 nm^3 at T=300.00 K
and corresponding refactor 1.0 / 3.0*V*k_B*T*EPSILON_0: 7.120911 
Too less points for a fit.

I am not sure, where to find the dipole moment for each of the four molecules.

Many thanks
Andreas


 -Original Message-
 From: gmx-users-boun...@gromacs.org [mailto:gmx-users-boun...@gromacs.org]
 On Behalf Of Dommert Florian
 Sent: 04 August 2011 12:31
 To: Discussion list for GROMACS users
 Subject: Re: [gmx-users] g_dipoles - averaging
 
 On Thu, 2011-08-04 at 09:08 +0100, Kukol, Andreas wrote:
  Hello,
 
  Is there any way to output the dipole moment averaged over all molecules
 or for each molecule separately (and not the total dipole moment of the
 simulation box) ?
 
 
 Yes, the tool g_current decomposes the total dipole moment into a component
 in respect to the center of mass of the molecules and a translational term,
 which is present, if you are dealing with charged species. So, if you
 prepare a corresponding index file you can derive the average molecular
 dipole moment for every molecule and finally average the results.
 
 /Flo
 
  Apparently the dipole autocorrelation function can be obtained as an
 average over all molecules with the '-corr mol' option, but from the help
 info it is not clear, how and if the total dipole moment can be obtained in
 this way (and in which file Mtot.xvg or aver.xvg ?).
 
  Many thanks
  Andreas
 
 
 
 
 --
 Florian Dommert
 Dipl. - Phys.
 
 Institute for Computational Physics
 University Stuttgart
 
 Pfaffenwaldring 27
 70569 Stuttgart
 
 EMail: domm...@icp.uni-stuttgart.de
 Homepage: http://www.icp.uni-stuttgart.de/~icp/Florian_Dommert
 
 Tel.: +49 - (0)711 - 68563613
 Fax.: +49 - (0)711 - 68563658
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[gmx-users] PRODRG topology

2011-08-04 Thread Marzinek, Jan
Dear Gromacs Users,



I used PRODRG server in order to obtain the topology file for my molecule (52 
atoms with all hydrogens). However, server generated Gromacs topology which 
involves 47 atoms (for PDB file with polar/aromatic hydrogens). Whether I will 
use the pdb file with missing 4 hydrogen that wont be a good apporximation. How 
to overcome this?



Thank you in advance,



Jan
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Re: [gmx-users] PRODRG topology

2011-08-04 Thread Justin A. Lemkul



Marzinek, Jan wrote:

Dear Gromacs Users,

 

I used PRODRG server in order to obtain the topology file for my 
molecule (52 atoms with all hydrogens). However, server generated 
Gromacs topology which involves 47 atoms (for PDB file with 
polar/aromatic hydrogens). Whether I will use the pdb file with missing 
4 hydrogen that wont be a good apporximation. How to overcome this?


 


The Gromos96 force fields are united-atom force fields and may not use all the H 
atoms your input coordinates did.  If you suspect some issue with protonation 
state, PRODRG can be forced into certain protonation with the ADDHYD or DELHYD 
keywords.  Be advised, of course, of the usual caveats regarding the quality of 
PRODRG topologies:


http://www.gromacs.org/Downloads/Related_Software/PRODRG#Tips

-Justin

--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu | (540) 231-9080
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin


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Re: [gmx-users] setting vdw cutoff with specific force-filed?

2011-08-04 Thread Yun Shi
Hi Justin and Mark,

Thank you very much for the reply.

I was using table 7 (Normal van der Waals Parameters) to calculate
non-bonded vdw interactions that are not between third neighbors, such as
CH1 carbons between different chains in a biomolecular system. Anything
wrong here?

I understand that it is the force that dictates the MD evolution, and I
calculated in this case as F = 12 * 9.85^2 / 1.5^13 = 5.98 kJ/mol/nm for the
repulsion term. The force from different directions on a atom in a
homogeneous system would cancel each other to some extend, but what about
the energy arises from this interaction? Would this considerably affect the
calculation of, say, binding energy of a ligand to a receptor from
thermodynamic integration or pulling simulation?

Besides, the GROMOS 53a6 paper used triple range scheme for calculations of
nonbonded interactions, and I guess it was rlist = 0.8 nm while rvdw =
rcoulomb = 1.4 nm. So is this considered to be accurate enough in
calculating free enthalpies of solvation since we know the interactions
between 0.8 and 1.4 nm were calculated every 5 steps?

The paper also used reaction-field instead PME to account for long-range
electrostatic interactions. I heard some people argue that PME would be more
accurate and it seemed to be utilized more often even in gromacs tutorials.
So does this mean certain accuracy could be achieved by using triple range
scheme and reaction-field together because the errors they incur
respectively somehow cancel out each other?

Thanks a lot,

Yun Shi


On 04/08/11, Justin A. Lemkul  jalem...@vt.edu wrote:


 Yun Shi wrote:
 Hi all,
 
 I am working with GROMOS 53a6 ff in GROMACS 4.5, and I assume a
Lennard-Jones interaction function was used for short-range vdw
interactions.
 
  From the reference paper /A Biomolecular Force Field Based on the Free
Enthalpy of Hydration and Solvation: The GROMOS Force-Field Parameter Sets
53A5 and 53A6/, I found that for example,
 
 when rvdw = 1.5nm, the repulsion term of the interaction between two CH1
type atoms (C12ij = 9.85^2) can be calculated as 9.850*9.850 / (1.5^12) =
0.747786 kJ/mol. So I wonder if this value is considered to be small enough
to be ignored.


You should pay attention to the column headings in table 7 so that you can
compute the contribution correctly. However, the magnitude of the energy of
any particular interaction is not really of any concern. The evolution of
the system depends on the *forces*, and it is likely that the sum of the
forces on any atom from all its repulsion interactions from atoms that are
(say) 1.4nm to 1.5nm away is very close to zero, except in highly
non-homogeneous spatial distributions of particles. In any case, the sum of
that contribution will be much smaller than the other contributions.

Mark


 
 In addition, it seems not until 5 nm does the dispersion term become
larger than the repulsion term in this case, so would turning on Dispersion
Correction between, say 1.5 to 5 nm introduce more errors than turning it
off?
 

 You should use the cutoff described the authors of the force field, in
this case rvdw=1.4.  Unless you can demonstrate that by using a different
value you can achieve superior results, stick with the specifics of
parameterization.  I have never seen ill effects of setting rvdw=1.4 and
using dispersion correction with this force field.

 -Justin

 --
 ==
==

 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 MILES-IGERT Trainee
 Department of Biochemistry
 Virginia Tech
 Blacksburg, VA
 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin

 
 --
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 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at
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 Please don't post (un)subscribe requests to the list. Use the www
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Re: [gmx-users] setting vdw cutoff with specific force-filed?

2011-08-04 Thread Justin A. Lemkul



Yun Shi wrote:

Hi Justin and Mark,

Thank you very much for the reply.

I was using table 7 (Normal van der Waals Parameters) to calculate 
non-bonded vdw interactions that are not between third neighbors, such 
as CH1 carbons between different chains in a biomolecular system. 
Anything wrong here?


I understand that it is the force that dictates the MD evolution, and I 
calculated in this case as F = 12 * 9.85^2 / 1.5^13 = 5.98 kJ/mol/nm for 
the repulsion term. The force from different directions on a atom in a 
homogeneous system would cancel each other to some extend, but what 
about the energy arises from this interaction? Would this considerably 
affect the calculation of, say, binding energy of a ligand to a receptor 
from thermodynamic integration or pulling simulation?




Check your units and the column headings of Table 7.  Plugging in 9.85 as the 
energy will give you a wildly inflated result.  The C12 parameters listed are 
actually square roots and listed as 10^-3.  I think you will find the resulting 
energies and forces are vastly smaller for a simple interaction between two atoms.


Besides, the GROMOS 53a6 paper used triple range scheme for calculations 
of nonbonded interactions, and I guess it was rlist = 0.8 nm while rvdw 
= rcoulomb = 1.4 nm. So is this considered to be accurate enough in 
calculating free enthalpies of solvation since we know the interactions 
between 0.8 and 1.4 nm were calculated every 5 steps?




There is no need to update the neighbor list every single step.  Typically, 
water is the fastest-diffusing molecule in the system, but it will generally not 
have a dramatic displacement on the scale of 10 fs or so.


The paper also used reaction-field instead PME to account for long-range 
electrostatic interactions. I heard some people argue that PME would be 
more accurate and it seemed to be utilized more often even in gromacs 
tutorials. So does this mean certain accuracy could be achieved by using 
triple range scheme and reaction-field together because the errors they 
incur respectively somehow cancel out each other?




PME is substantially more accurate.  Using it also requires rlist=rcoulomb, so 
the exact details of the Gromos96 derivation may be somewhat outdated.  Typical 
settings for Gromos96 would be something like:


rlist = 0.9
rcoulomb = 0.9
rvdw = 1.4
nstlist = 5
coulombtype = PME

Note that the value of rcoulomb and rlist can vary a bit as a consequence of 
PME.

-Justin


Thanks a lot,

Yun Shi


On 04/08/11, Justin A. Lemkul  jalem...@vt.edu 
mailto:jalem...@vt.edu wrote:

 
 
  Yun Shi wrote:
  Hi all,
  
  I am working with GROMOS 53a6 ff in GROMACS 4.5, and I assume a 
Lennard-Jones interaction function was used for short-range vdw 
interactions.

  
   From the reference paper /A Biomolecular Force Field Based on the 
Free Enthalpy of Hydration and Solvation: The GROMOS Force-Field 
Parameter Sets 53A5 and 53A6/, I found that for example,

  
  when rvdw = 1.5nm, the repulsion term of the interaction between two 
CH1 type atoms (C12ij = 9.85^2) can be calculated as 9.850*9.850 / 
(1.5^12) = 0.747786 kJ/mol. So I wonder if this value is considered to 
be small enough to be ignored.

 

You should pay attention to the column headings in table 7 so that you 
can compute the contribution correctly. However, the magnitude of the 
energy of any particular interaction is not really of any concern. The 
evolution of the system depends on the *forces*, and it is likely that 
the sum of the forces on any atom from all its repulsion interactions 
from atoms that are (say) 1.4nm to 1.5nm away is very close to zero, 
except in highly non-homogeneous spatial distributions of particles. In 
any case, the sum of that contribution will be much smaller than the 
other contributions.


Mark

 
  
  In addition, it seems not until 5 nm does the dispersion term become 
larger than the repulsion term in this case, so would turning on 
Dispersion Correction between, say 1.5 to 5 nm introduce more errors 
than turning it off?

  
 
  You should use the cutoff described the authors of the force field, 
in this case rvdw=1.4.  Unless you can demonstrate that by using a 
different value you can achieve superior results, stick with the 
specifics of parameterization.  I have never seen ill effects of setting 
rvdw=1.4 and using dispersion correction with this force field.

 
  -Justin
 
  --
  ==
==
 
  Justin A. Lemkul
  Ph.D. Candidate
  ICTAS Doctoral Scholar
  MILES-IGERT Trainee
  Department of Biochemistry
  Virginia Tech
  Blacksburg, VA
  jalemkul[at]vt.edu http://vt.edu/ | (540) 231-9080 
tel:%28540%29%20231-9080

  http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
 
  
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mailto:gmx-users@gromacs.org

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  Please search the archive at 

RE: [gmx-users] g_dipoles - averaging

2011-08-04 Thread Dommert Florian
On Thu, 2011-08-04 at 15:49 +0100, Kukol, Andreas wrote: 
 Florian,
 
 I am not sure, which of the output files of g_current contains the dipole 
 moment for each molecule. Applying g_current to a trajectory of four 
 molecules of asparagin in water gives the following output:
 

To obtain the dipole moment for every single molecule you have to create
index groups for every single molecule, and the output you are looking
for is the rotational part of M contained in md.xvg
the -eps flag is also not necessary and only required for the
calculation of the dielectric constant. 

/Flo

 g_current -s tpr_200ps.tpr -f xtcIRWhole_100-200ps.xtc -eps 80 -o current.xvg
 (selecting 4 molecules of asparagin from the index group)
 
 md.xvg
 @title Averaged rotational part of M
 @xaxis  label Time (ps)
 @yaxis  label  M\sD\N  (enm)
 @TYPE xy
 # time x   y   z   average of M_D^2std.dev
 0.000 -0.10261 0.12324 0.27085 0.09908 0.31477
 0.001 -0.10421 0.12287 0.27297 0.09977 0.31587
 0.002 -0.09766 0.12637 0.27104 0.09951 0.31543
 ...
 
 dsp.xvg
 @title MSD of the squared translational dipole moment M
 @xaxis  label Time (ps)
 @yaxis  label |M\sJ\N(t)-M\sJ\N(0)|\S2\N  / 6.0*V*k\sB\N*T / 
 Sm\S-1\Nps\S-1\N
 @TYPE xy
 #Prefactor fit E-H: 1 / 6.0*V*k_B*T: 3.15249e-11
 0.000  0
 0.001 8.70985e-30
 0.002 1.9936e-29
 ...
 
 mj.xvg
 @title Averaged translational part of M
 @xaxis  label Time (ps)
 @yaxis  label  M\sJ\N  (enm)
 @TYPE xy
 # time x   y   z   average of M_J^2std.dev
 0.000  0.1 0.0 0.0 0.0 0.1
 0.001  0.1 0.0 0.0 0.0 0.1
 ...
 
 current.xvg was not produced due to:
 ...
 ...
 Average volume V=32.764893 nm^3 at T=300.00 K
 and corresponding refactor 1.0 / 3.0*V*k_B*T*EPSILON_0: 7.120911 
 Too less points for a fit.verage volume V=32.764893 nm^3 at T=300.00 K
 and corresponding refactor 1.0 / 3.0*V*k_B*T*EPSILON_0: 7.120911 
 Too less points for a fit.
 
 I am not sure, where to find the dipole moment for each of the four molecules.
 
 Many thanks
 Andreas
 
 
  -Original Message-
  From: gmx-users-boun...@gromacs.org [mailto:gmx-users-boun...@gromacs.org]
  On Behalf Of Dommert Florian
  Sent: 04 August 2011 12:31
  To: Discussion list for GROMACS users
  Subject: Re: [gmx-users] g_dipoles - averaging
  
  On Thu, 2011-08-04 at 09:08 +0100, Kukol, Andreas wrote:
   Hello,
  
   Is there any way to output the dipole moment averaged over all molecules
  or for each molecule separately (and not the total dipole moment of the
  simulation box) ?
  
  
  Yes, the tool g_current decomposes the total dipole moment into a component
  in respect to the center of mass of the molecules and a translational term,
  which is present, if you are dealing with charged species. So, if you
  prepare a corresponding index file you can derive the average molecular
  dipole moment for every molecule and finally average the results.
  
  /Flo
  
   Apparently the dipole autocorrelation function can be obtained as an
  average over all molecules with the '-corr mol' option, but from the help
  info it is not clear, how and if the total dipole moment can be obtained in
  this way (and in which file Mtot.xvg or aver.xvg ?).
  
   Many thanks
   Andreas
  
  
  
  
  --
  Florian Dommert
  Dipl. - Phys.
  
  Institute for Computational Physics
  University Stuttgart
  
  Pfaffenwaldring 27
  70569 Stuttgart
  
  EMail: domm...@icp.uni-stuttgart.de
  Homepage: http://www.icp.uni-stuttgart.de/~icp/Florian_Dommert
  
  Tel.: +49 - (0)711 - 68563613
  Fax.: +49 - (0)711 - 68563658
 -- 
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-- 
Florian Dommert
Dipl. - Phys.

Institute for Computational Physics
University Stuttgart

Pfaffenwaldring 27
70569 Stuttgart

EMail: domm...@icp.uni-stuttgart.de
Homepage: http://www.icp.uni-stuttgart.de/~icp/Florian_Dommert

Tel.: +49 - (0)711 - 68563613
Fax.: +49 - (0)711 - 68563658


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Re: [gmx-users] RE: Gromacs on GPU: GTX or Tesla?

2011-08-04 Thread Szilárd Páll
Hi,

Tesla cards won't give you much benefit when it comes to running the
current Gromacs. Additionally, I can tell you so much that this won't
change in the future either. The only advantage of the C20x0-s is ECC
and double precision - which is ATM anyway not supported in Gromacs on
GPUs.

Gromacs in general doesn't use much memory so unless you will want to
run gigantic systems with a single card, C2070 will not give you any
added benefit at all, in fact 1-1.5GB/card should be more than enough.

What kind of machine are you planning to buy/how many GPUs?

--
Szilárd



On Thu, Aug 4, 2011 at 8:59 AM, Jagdish S. Varma jsva...@connoiseur.com wrote:
 Hi,
 In the long term the Tesla is much more preferable as the GTX would not
 support certain high end functions. Pls verify these before you purchase
 one. Also the Tesla C-2070 is the newer one available and with 6.0GB RAM it
 really gives out great performance. The price is the same.

 Rgds
 JSV
 
 From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org] On
 Behalf Of Efrat Exlrod [efrat.exl...@biu.ac.il]
 Sent: Thursday, August 04, 2011 12:13 PM
 To: gmx-users@gromacs.org
 Subject: [gmx-users] Gromacs on GPU: GTX or Tesla?

 Hi,



 We want to start using Gromacs on GPU and we are debating whether
 to purchase GeForce GTX card or Tesla platform. Looking at the published
 data it seems GTX580 has much impressive performance compared to Tesla
 C2050, and of course it is much cheaper. Is there a reason to prefer Tesla
 over GTX for running Gromacs in the short or long term?



 Thanks, Efrat

 
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[gmx-users] angular velocities in gromacs?

2011-08-04 Thread Tom
Dear Gromacs User,

Gromacs *trr file has the velocities. They are for translational motions.
But how can we get the angular velocities?

Thanks for the information!

Tom
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[gmx-users] Re: setting vdw cutoff with specific force-filed?

2011-08-04 Thread Yun Shi
Hi Justin,

I got it now. During the 10fs, even water molecules with a speed of 500 m/s
only have a 0.005 nm displacement, which is far less than than 0.9 nm or 1.4
nm.

Thanks again!

Yun


Yun Shi wrote:
 Hi Justin and Mark,

 Thank you very much for the reply.

 I was using table 7 (Normal van der Waals Parameters) to calculate
 non-bonded vdw interactions that are not between third neighbors, such
 as CH1 carbons between different chains in a biomolecular system.
 Anything wrong here?

 I understand that it is the force that dictates the MD evolution, and I
 calculated in this case as F = 12 * 9.85^2 / 1.5^13 = 5.98 kJ/mol/nm for
 the repulsion term. The force from different directions on a atom in a
 homogeneous system would cancel each other to some extend, but what
 about the energy arises from this interaction? Would this considerably
 affect the calculation of, say, binding energy of a ligand to a receptor
 from thermodynamic integration or pulling simulation?


Check your units and the column headings of Table 7.  Plugging in 9.85 as
the
energy will give you a wildly inflated result.  The C12 parameters listed
are
actually square roots and listed as 10^-3.  I think you will find the
resulting
energies and forces are vastly smaller for a simple interaction between two
atoms.

 Besides, the GROMOS 53a6 paper used triple range scheme for calculations
 of nonbonded interactions, and I guess it was rlist = 0.8 nm while rvdw
 = rcoulomb = 1.4 nm. So is this considered to be accurate enough in
 calculating free enthalpies of solvation since we know the interactions
 between 0.8 and 1.4 nm were calculated every 5 steps?


There is no need to update the neighbor list every single step.  Typically,
water is the fastest-diffusing molecule in the system, but it will generally
not
have a dramatic displacement on the scale of 10 fs or so.

 The paper also used reaction-field instead PME to account for long-range
 electrostatic interactions. I heard some people argue that PME would be
 more accurate and it seemed to be utilized more often even in gromacs
 tutorials. So does this mean certain accuracy could be achieved by using
 triple range scheme and reaction-field together because the errors they
 incur respectively somehow cancel out each other?


PME is substantially more accurate.  Using it also requires rlist=rcoulomb,
so
the exact details of the Gromos96 derivation may be somewhat outdated.
 Typical
settings for Gromos96 would be something like:

rlist = 0.9
rcoulomb = 0.9
rvdw = 1.4
nstlist = 5
coulombtype = PME

Note that the value of rcoulomb and rlist can vary a bit as a consequence of
PME.

-Justin

 Thanks a lot,

 Yun Shi


 On 04/08/11, Justin A. Lemkul  jalem...@vt.edu
 mailto:jalem...@vt.edu wrote:
  
  
   Yun Shi wrote:
   Hi all,
   
   I am working with GROMOS 53a6 ff in GROMACS 4.5, and I assume a
 Lennard-Jones interaction function was used for short-range vdw
 interactions.
   
From the reference paper /A Biomolecular Force Field Based on the
 Free Enthalpy of Hydration and Solvation: The GROMOS Force-Field
 Parameter Sets 53A5 and 53A6/, I found that for example,
   
   when rvdw = 1.5nm, the repulsion term of the interaction between two
 CH1 type atoms (C12ij = 9.85^2) can be calculated as 9.850*9.850 /
 (1.5^12) = 0.747786 kJ/mol. So I wonder if this value is considered to
 be small enough to be ignored.
  

 You should pay attention to the column headings in table 7 so that you
 can compute the contribution correctly. However, the magnitude of the
 energy of any particular interaction is not really of any concern. The
 evolution of the system depends on the *forces*, and it is likely that
 the sum of the forces on any atom from all its repulsion interactions
 from atoms that are (say) 1.4nm to 1.5nm away is very close to zero,
 except in highly non-homogeneous spatial distributions of particles. In
 any case, the sum of that contribution will be much smaller than the
 other contributions.

 Mark

  
   
   In addition, it seems not until 5 nm does the dispersion term become
 larger than the repulsion term in this case, so would turning on
 Dispersion Correction between, say 1.5 to 5 nm introduce more errors
 than turning it off?
   
  
   You should use the cutoff described the authors of the force field,
 in this case rvdw=1.4.  Unless you can demonstrate that by using a
 different value you can achieve superior results, stick with the
 specifics of parameterization.  I have never seen ill effects of setting
 rvdw=1.4 and using dispersion correction with this force field.
  
   -Justin
  
   --
   ==
 ==
  
   Justin A. Lemkul
   Ph.D. Candidate
   ICTAS Doctoral Scholar
   MILES-IGERT Trainee
   Department of Biochemistry
   Virginia Tech
   Blacksburg, VA
   jalemkul[at]vt.edu http://vt.edu/ | (540) 231-9080
 tel:%28540%29%20231-9080
   http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
  
   ==
==
 

Re: [gmx-users] Problem of Kinetic Energy

2011-08-04 Thread Mark Abraham

On 4/08/2011 7:17 AM, Size Zheng wrote:

Hi Mark,

When I used the g_traj with options of -ekt and -ekr, i made a selection as 
follow

Group 0 ( System) has  6400 elements
Group 1 (TP4) has  6400 elements
Select a group: 1
Selected 1: 'TP4'

So according to you that g_traj uses the whole 1600-molecules' COM to report the
value of translational and rotational kinetics energy, rather than the sum of 
all 1600 rigid molecules?


That is my understanding, based purely on reading g_traj -h.



Is there any other command or options can operate ekrot and ektrans on atoms or 
molecules?


I don't know, but I would start by looking in Chapter 8 of the manual.

Mark
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Re: [gmx-users] angular velocities in gromacs?

2011-08-04 Thread Mark Abraham

On 5/08/2011 6:08 AM, Tom wrote:

Dear Gromacs User,

Gromacs *trr file has the velocities. They are for translational motions.
But how can we get the angular velocities?


Angular velocities with respect to what?

Mark
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[gmx-users] How to exclude the interactions between molecule A and B in Gromacs?

2011-08-04 Thread DeChang Li
Dear all,


   I want to use Gromacs to run an enhanced sampling molecular dynamics
(ESMD) proposed by Karplus’s group (J. Am. Chem. Soc. (1990) 112, 9161-9175.
 J. Mol. Biol. (1999) 291, 101-115). In the ESMD simulation, we need to
exclude the interactions (especially the Coulomb interactions) between some
small molecules (e.g. ligand A and its replica). How can Gromacs to do this?
Any suggestion will be very appreciated.




Best regards,

=
Dechang Li, Ph.D
Biomechanics and Biomaterials Laboratory
Department of Applied Mechanics
School of Aerospace Engineering
Beijing Institute of Technology
Beijing 100081, P. R. China
=
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Re: [gmx-users] angular velocities in gromacs?

2011-08-04 Thread Matthew Zwier
Hi Tom,

TRR files contain velocities for individual atoms as a function of
time, which is all the velocity information there is in an MD
simulation.  You can reduce that information to rotation about a
principle molecular axis, or rotation with respect to the simulation
box, or whatever you need.

MZ

On Thu, Aug 4, 2011 at 4:08 PM, Tom dna...@gmail.com wrote:
 Dear Gromacs User,

 Gromacs *trr file has the velocities. They are for translational motions.
 But how can we get the angular velocities?

 Thanks for the information!

 Tom

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Re: [gmx-users] How to exclude the interactions between molecule A and B in Gromacs?

2011-08-04 Thread Mark Abraham

On 5/08/2011 1:17 PM, DeChang Li wrote:


Dear all,

I want to use Gromacs to run an enhanced sampling molecular dynamics 
(ESMD) proposed by Karplus's group (J. Am. Chem. Soc. (1990) 112, 
9161-9175.  J. Mol. Biol. (1999) 291, 101-115). In the ESMD 
simulation, we need to exclude the interactions (especially the 
Coulomb interactions) between some small molecules (e.g. ligand A and 
its replica). How can Gromacs to do this? Any suggestion will be very 
appreciated.


See energy groups and energy group exclusions in 3.3 and 7.3.19 of the 
manual.


Mark
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