[gmx-users] Re:qmmm temp definition + linking atom

2011-05-11 Thread Gerrit Groenhof
 The link atom can be placed anywhere at step 0. These atom are treated 
like virtual sites and will thus be placed at the defined position along 
the QM/MM bond that  needs capping.


Concerning the temperature, one can treat the QM atoms as a separate 
group indeed. But as Mark said, why not expose the whole system to the 
temp-shock?


Gerrit




4. qmmm temp definition (Yao Yao)
5. qmmm linking atom (Yao Yao)
6. Re: qmmm temp definition (Mark Abraham)


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[gmx-users] Running md in different systems

2011-05-11 Thread Kavyashree M
Dear users,

I was running an MD in a system with 8 cores, for some
reasons I had to shift the job to another system with
same OS and gromacs version. After I started runnning
it said

Gromacs binary or parallel settings not identical to previous run.
Continuation is exact, but is not guaranteed to be binary identical.

How does this effect the run and also it gave a warning saying
WARNING: This run will generate roughly 2054591408127343104 Mb of data !!

which generally used to be around 5GB!

What is wrong here?

Thank you
With regards
Kavya
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Re: [gmx-users] g_current and output redirection

2011-05-11 Thread Dommert Florian
Hello Vitaly,

the intention to write out informations to the stdout and the stderr was
that you have the ability to sort it during the analysis. However as
Justin mentionen  will write all open pipes into one file.

Cheers,
Flo

On Tue, 2011-05-10 at 13:16 -0400, Vitaly Chaban wrote: 
 Thanks, Justin! Great solution.
 
 On Tue, May 10, 2011 at 12:57 PM, Justin A. Lemkul jalem...@vt.edu wrote:
 
 
  Vitaly Chaban wrote:
 
  I have a pure linux question. When using g_current and trying to
  redirect its output to the file, e.g.
 
  g_current -temp $TEMPER -b $conduct_b -e $conduct_e  EOF  output
  0
  EOF
 
  only a part of output is written to the file (output)
 
  Here is what is actually written to the file:
 
  Selected 0: 'System'
  Average translational dipole moment M_J [enm] after 25001 frames
  (|M|^2): 5.554790 -5.833042 -0.539783 (68.255722)
  Average molecular dipole moment M_D [enm] after 25001 frames (|M|^2):
  -0.414639 -0.356325 0.148187 (2.359227)
 
  Thus, the relevant data (sigma, dielectric constant) are missed. My
  question is how to redirect all the output of g_current to my file.
 
 
  echo 0 | g_current (options) outfile
 
  -Justin
 
 
  Thanks!
 
  Dr. Vitaly V. Chaban, Department of Chemistry
  University of Rochester, Rochester, New York 14627-0216
 
  --
  
 
  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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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

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[gmx-users] Continuing job in another machine

2011-05-11 Thread Kavyashree M
Dear users,

I was running an MD in a machine with  2 quad core processors
using all 8 cores system cores, for some reasons I had to shift the
 job to another machine with 2 quad cores processors, identical OS
and gromacs version using 8 cores. After I started runnning using check
point
file it said -

 Build time mismatch,
current program: Thu Jan 20 12:00:01 IST 2011
checkpoint file: Thu Jan 20 11:57:38 IST 2011

  Build user mismatch,
current program: kavya@alder
checkpoint file: kavya@yamuna

Gromacs binary or parallel settings not identical to previous run.
Continuation is exact, but is not guaranteed to be binary identical.

How does this effect the run and also it gave a warning saying

WARNING: This run will generate roughly 2054591408127343104 Mb of data !!

which generally used to be around 5GB!

What is wrong here? Kindly reply.

Thank you
With regards
Kavya
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Re: [gmx-users] Continuing job in another machine

2011-05-11 Thread Mark Abraham


On 11/05/11, Kavyashree M  hmkv...@gmail.com wrote:
 Dear users, 
  
     I was running an MD in a machine with  2 quad core processors
 using all 8 cores system cores, for some reasons I had to shift the
  job to another machine with 2 quad cores processors, identical OS 
 
 and gromacs version using 8 cores. After I started runnning using check point
 file it said -
 
  Build time mismatch,
     current program: Thu Jan 20 12:00:01 IST 2011
     checkpoint file: Thu Jan 20 11:57:38 IST 2011
 
 
   Build user mismatch,
     current program: kavya@alder
     checkpoint file: kavya@yamuna
 
 Gromacs binary or parallel settings not identical to previous run.
 
 Continuation is exact, but is not guaranteed to be binary identical.
 
 How does this effect the run and also it gave a warning saying 
 

See http://www.gromacs.org/Documentation/Terminology/Reproducibility. Under 
normal circumstances there is nothing of concern.


 WARNING: This run will generate roughly 2054591408127343104 Mb of data !!
 
 
 
 which generally used to be around 5GB!
 
 What is wrong here? Kindly reply.
 

Some kind of integer datatype is different on the two machines, and some kind 
of overflow is happening in the estimation. Don't worry about it.

Mark
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Re: [gmx-users] Continuing job in another machine

2011-05-11 Thread Kavyashree M
Respected Sir,

  So that number doesnt mean what it says!

Thanking you
With regards
kavya

On Wed, May 11, 2011 at 4:27 PM, Mark Abraham mark.abra...@anu.edu.auwrote:



 On 11/05/11, *Kavyashree M * hmkv...@gmail.com wrote:

 Dear users,

 I was running an MD in a machine with  2 quad core processors
 using all 8 cores system cores, for some reasons I had to shift the
  job to another machine with 2 quad cores processors, identical OS
 and gromacs version using 8 cores. After I started runnning using check
 point
 file it said -

  Build time mismatch,
 current program: Thu Jan 20 12:00:01 IST 2011
 checkpoint file: Thu Jan 20 11:57:38 IST 2011

   Build user mismatch,
 current program: kavya@alder
 checkpoint file: kavya@yamuna

 Gromacs binary or parallel settings not identical to previous run.
 Continuation is exact, but is not guaranteed to be binary identical.

 How does this effect the run and also it gave a warning saying


 See http://www.gromacs.org/Documentation/Terminology/Reproducibility.
 Under normal circumstances there is nothing of concern.


 WARNING: This run will generate roughly 2054591408127343104 Mb of data !!

 which generally used to be around 5GB!

 What is wrong here? Kindly reply.


 Some kind of integer datatype is different on the two machines, and some
 kind of overflow is happening in the estimation. Don't worry about it.

 Mark
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[gmx-users] Surface area calculation

2011-05-11 Thread Laura Leay
Can anyone explain in detail the method that gromacs uses to calculate
surface area? Which surface area is it calculating (e.g., connolley,
accessible)?

I am under the impression that the final result is given in nm^2. Is
this correct?


Carrying out the surface area calculation in gromacs using the OPLS all
atom force field I obtain a value of 4.43 nm^2  for methane (carbon =
opls_138, sigma = 0.35 and hydrogen = opls_140, sigma = 0.25) (CT-HC
ideal bond length = 0.109, e=284512). The command was 

g_sas -f conf.gro -s topol.tpr -oa -or -tv -probe 0.2 -ndots 200 -nopbc

and the result was taken from resarea.xvg


I have written a program to calculate the geometric accessible surface
area using the van der waals radius of the atoms and a probe of a given
size. The surface is defined from the centre of the probe. Using the
above values for sigma I obtain a value for methane of 1.15 nm^2 with a
probe diameter of 0.2 nm.

Obviously the two do not match and I am not sure why. 

The individual atom areas for my molecule are:
C 0.22
H 0.24
H 0.23
H 0.22
H 0.24

Attached are the files used in the gromacs calculation along with the
output and my own program. If any one has any suggestions please let me
know.
# This file was created Wed May 11 13:05:56 2011
# by the following command:
# g_sas -f conf.gro -s topol.tpr -oa -or -tv -probe 0.2 -ndots 200 -nopbc 
#
# g_sas is part of G R O M A C S:
#
# Gravel Rubs Often Many Awfully Cauterized Sores
#
@title Solvent Accessible Surface
@xaxis  label Time (ps)
@yaxis  label Area (nm\S2\N)
@TYPE xy
@ view 0.15, 0.15, 0.75, 0.85
@ legend on
@ legend box on
@ legend loctype view
@ legend 0.78, 0.8
@ legend length 2
@ s0 legend Hydrophobic
@ s1 legend Hydrophilic
@ s2 legend Total
@ s3 legend D Gsolv
 0 4.43467   0 4.43467-11.1328
# This file was created Wed May 11 13:05:56 2011
# by the following command:
# g_sas -f conf.gro -s topol.tpr -oa -or -tv -probe 0.2 -ndots 200 -nopbc 
#
# g_sas is part of G R O M A C S:
#
# Gravel Rubs Often Many Awfully Cauterized Sores
#
@title Area per atom
@xaxis  label Atom #
@yaxis  label Area (nm\S2\N)
@TYPE xy
1 1.53938 0.000291734
2 0.723823 0
3 0.723823 0
4 0.723823 0
5 0.723823 0
methane
   5
1DRGCT1   0.000   0.000   0.000
1DRGHC2   0.000   0.000   1.089
1DRGHC3   1.027   0.000  -0.363
1DRGHC4  -0.513  -0.889  -0.363
1DRGHC5  -0.513   0.889  -0.363
   7.90500   7.90500   7.90500

; VARIOUS PREPROCESSING OPTIONS
title= Yo
cpp  = /usr/bin/cpp
include  = 
define   = 

; RUN CONTROL PARAMETERS
integrator   = steep
; Start time and timestep in ps
tinit= 0
dt   = 0.002
nsteps   = 1000
; For exact run continuation or redoing part of a run
init_step= 0
; mode for center of mass motion removal
comm-mode= Linear
; number of steps for center of mass motion removal
nstcomm  = 1
; group(s) for center of mass motion removal
comm-grps= 

; LANGEVIN DYNAMICS OPTIONS
; Temperature, friction coefficient (amu/ps) and random seed
;bd-temp  = 300
bd-fric  = 0
ld-seed  = 1993

; ENERGY MINIMIZATION OPTIONS
; Force tolerance and initial step-size
emtol= 100
emstep   = 0.01
; Max number of iterations in relax_shells
niter= 20
; Step size (1/ps^2) for minimization of flexible constraints
fcstep   = 0
; Frequency of steepest descents steps when doing CG
nstcgsteep   = 1000
nbfgscorr= 10

; OUTPUT CONTROL OPTIONS
; Output frequency for coords (x), velocities (v) and forces (f)
nstxout  = 0
nstvout  = 0
nstfout  = 0
; Checkpointing helps you continue after crashes
nstcheckpoint= 1000
; Output frequency for energies to log file and energy file
nstlog   = 50
nstenergy= 50
; Output frequency and precision for xtc file
nstxtcout= 50
xtc-precision= 1000
; This selects the subset of atoms for the xtc file. You can
; select multiple groups. By default all atoms will be written.
xtc-grps = 
; Selection of energy groups
energygrps   = 

; NEIGHBORSEARCHING PARAMETERS
; nblist update frequency
nstlist  = 10
; ns algorithm (simple or grid)
ns_type  = grid
; Periodic boundary conditions: xyz (default), no (vacuum)
; or full (infinite systems only)
pbc  = xyz
; nblist cut-off
rlist= 0.9
domain-decomposition = no

; OPTIONS FOR ELECTROSTATICS AND VDW
; Method for doing electrostatics
coulombtype  = Cut-off
rcoulomb-switch  = 0
rcoulomb = 0.9
; Dielectric 

Re: [gmx-users] REMD: after replica exchange breakdown

2011-05-11 Thread SebastianWaltz
On 05/11/2011 05:20 AM, Mark Abraham wrote:
 On 05/11/2011 02:32 AM, SebastianWaltz wrote:
 Dear GROMACS User,

 I'm running a REMD MD of 32 replicas. It worked for the first few
 replica exchanges. After 30ps again two replicas were exchanged and I
 received the Error:
 x particles communicated to PME node y are more than a cell length out
 of the domain decomposition cell of their charge group

 The only rationale I can see is that a velocity was scaled after
 exchange that was now large enough to lead to the normal sort of
 exploding system. Was the exploding replica going up in temperature?
 How did you equilibrate the systems?
I did a NPT equilibration for each replica which leads obviously to
different volumes and looks like to cause some problems. If I use the
same volume for each replica it works fine.  

 I am using NVT assembles for each replica with a exchanging interval of
 5ps. For each replica I use 4 processors. Constraint are only the bonds
 to hydrogens (constraints = hbonds). Using PME for electro static.

 Information like GROMACS version, simulation system dimensions and
 contents would be useful. What replica temperature distribution exists?
I am using version 4.0.7. My system consists of a small peptide soluted
in ~1500 rigid CHCl3 molecules. System equilibrated with NPT and NVT
production run seems to work only if I increase the number of replicas
(32-64) meaning that I also decrease the difference of the volumes. The
temperature is exponentially distributed from 200 to 450K. 

 When running each replica for its own everything is working fine,
 nothing is blowing up like one would expect after getting the above
 Error.

 Good trouble-shooting :) You'd have been told to try this otherwise...

 Mark

Thanks a lot

Sebastian
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Re: [gmx-users] Surface area calculation

2011-05-11 Thread XAvier Periole


reference:
Eisenhaber F, Lijnzaad P, Argos P, Sander C,  Scharf M (1995) J.  
Comput. Chem. 16, 273-284.


On May 11, 2011, at 2:34 PM, Laura Leay wrote:


Can anyone explain in detail the method that gromacs uses to calculate
surface area? Which surface area is it calculating (e.g., connolley,
accessible)?

I am under the impression that the final result is given in nm^2. Is
this correct?


Carrying out the surface area calculation in gromacs using the OPLS  
all

atom force field I obtain a value of 4.43 nm^2  for methane (carbon =
opls_138, sigma = 0.35 and hydrogen = opls_140, sigma = 0.25) (CT-HC
ideal bond length = 0.109, e=284512). The command was

g_sas -f conf.gro -s topol.tpr -oa -or -tv -probe 0.2 -ndots 200 - 
nopbc


and the result was taken from resarea.xvg


I have written a program to calculate the geometric accessible surface
area using the van der waals radius of the atoms and a probe of a  
given

size. The surface is defined from the centre of the probe. Using the
above values for sigma I obtain a value for methane of 1.15 nm^2  
with a

probe diameter of 0.2 nm.

Obviously the two do not match and I am not sure why.

The individual atom areas for my molecule are:
C 0.22
H 0.24
H 0.23
H 0.22
H 0.24

Attached are the files used in the gromacs calculation along with the
output and my own program. If any one has any suggestions please let  
me

know.
 
area 
.xvg 
 
 
atomarea 
.xvg 
 
 
conf 
.gro 
 
grompp.mdpmethane.itpresarea.xvgtopol.topPIsurfaceOPLS.f90--

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Re: [gmx-users] Surface area calculation

2011-05-11 Thread Erik Marklund

Laura Leay skrev 2011-05-11 14.34:

Can anyone explain in detail the method that gromacs uses to calculate
surface area? Which surface area is it calculating (e.g., connolley,
accessible)?

I am under the impression that the final result is given in nm^2. Is
this correct?


Carrying out the surface area calculation in gromacs using the OPLS all
atom force field I obtain a value of 4.43 nm^2  for methane (carbon =
opls_138, sigma = 0.35 and hydrogen = opls_140, sigma = 0.25) (CT-HC
ideal bond length = 0.109, e=284512). The command was

g_sas -f conf.gro -s topol.tpr -oa -or -tv -probe 0.2 -ndots 200 -nopbc

and the result was taken from resarea.xvg


I have written a program to calculate the geometric accessible surface
area using the van der waals radius of the atoms and a probe of a given
size. The surface is defined from the centre of the probe. Using the
above values for sigma I obtain a value for methane of 1.15 nm^2 with a
probe diameter of 0.2 nm.
One difference is that g_sas -probe 0.2 uses a probe with a 0.2 nm 
*radius*, while your code use a 0.2 nm diameter. That doesn't on its own 
explain the difference you report, but you probably want to use the same 
probe when comparing.


Erik

Obviously the two do not match and I am not sure why.

The individual atom areas for my molecule are:
C 0.22
H 0.24
H 0.23
H 0.22
H 0.24

Attached are the files used in the gromacs calculation along with the
output and my own program. If any one has any suggestions please let me
know.



--
---
Erik Marklund, PhD student
Dept. of Cell and Molecular Biology, Uppsala University.
Husargatan 3, Box 596,75124 Uppsala, Sweden
phone:+46 18 471 4537fax: +46 18 511 755
er...@xray.bmc.uu.sehttp://folding.bmc.uu.se/

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[gmx-users] reg pushing rate

2011-05-11 Thread vidhya sankar
Dear justin thank you for your mail
    
to push a mobile group towards reference group  I set the pull_rate in negative 
value (-0.1) as u said My question is 
 when i change the pull rate to less negative value (-0.01) will push rate 
increases or decreases?
 because my doubt is about sign .it means if set pull rate to high negative 
value will push rate decrases or increase sign confuse me  i am expcting  
valuable reply
Thanks in Advance
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Re: [gmx-users] reg pushing rate

2011-05-11 Thread Justin A. Lemkul



vidhya sankar wrote:

Dear justin thank you for your mail
   
to push a mobile group towards reference group  I set the pull_rate in 
negative value (-0.1) as u said My question is
 when i change the pull rate to less negative value (-0.01) will push 
rate increases or decreases?
 because my doubt is about sign .it means if set pull rate to high 
negative value will push rate decrases or increase sign confuse me  i am 


You can answer this question yourself with a simple test.  As stated in the 
manual, pull_rate is the rate of change in the position of the pulled group.


-Justin


expcting  valuable reply
Thanks in Advance



--


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] about g_hbond

2011-05-11 Thread lina
Hi,

For group A, b, C.

It's no doubt can get hb forming number between A-b, b-C. b-(A or C).

But I don't know how to get the number of residues of b forming both
with A and B at the same time. namely b-AC, not with AC group.

Thanks,
--
Best Regards,

lina



-- 
Best Regards,

lina
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Re: [gmx-users] about g_hbond

2011-05-11 Thread Justin A. Lemkul



lina wrote:

Hi,

For group A, b, C.

It's no doubt can get hb forming number between A-b, b-C. b-(A or C).

But I don't know how to get the number of residues of b forming both
with A and B at the same time. namely b-AC, not with AC group.



There's no direct way to do it, but from the output files of g_hbond it can be 
done.  You'd need the .xpm files of A-C and B-C hydrogen bonds, and write some 
script that parses the .xpm files, and whenever there is an entry of A-C in the 
same frame as B-C, then you have a hydrogen bond mediated between the two. 
There's lots of discussion in the list archive about water-mediated hydrogen 
bonds that is likely applicable here.


Note that if you're using g_hbond in version 4.5, there is an important bug that 
was fixed just yesterday:


http://lists.gromacs.org/pipermail/gmx-users/2011-May/061249.html

-Justin


Thanks,
--
Best Regards,

lina





--


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] tabulated potential energy=nan for r=0 nm and charged atoms

2011-05-11 Thread chris . neale

Dear users:

with assistance from Berk on the developers list, I am posting a  
work-around to this issue.


the nonbonded interactions calculate the nonbonded distance, r, using  
the gmx_invsqrt function. Thus, the optimized kernel from 4.5.4 and  
4.0.7 both give nan when two charges occupy the space, even when using  
tables that specify the force and potential energy to be zero.


I had expected that I would need to modify the generic kernel source,  
but that turned out to be unnecessary -- just using it was enough.


For some reason, using export GMX_NOOPTIMIZEDKERNELS=1 prior to  
running mdrun solves the issue for 4.5.4 but not 4.0.7 (on my  
architecture). To solve the problem in v4.0.7 (and this also works for  
v4.5.4) I must export GMX_NB_GENERIC=1; export GMX_NO_SOLV_OPT=1  
prior to running mdrun. Note that the generic nonbonded kernel runs  
1.1x slower then the unoptimized kernel, which itself runs 2.4x slower  
than the optimized kernel (on my architecture for this system).


Thank you,
Chris.

-- original message --

Dear Users:

I am trying to work with tabulated potentials for the first time. I
would like to allow 2 charges to be at the same spot. Imagine taking a
sodium and chloride ion and removing the LJ entirely and I want the
system to evaluate energies correctly and be stable during the
simulation. It was my intention to add a sort-of soft-core to the
charge-charge interactions at very close distances so that the system
did not crash. However, my testing didn't even get that far. I find
that the Coulomb(SR) energy = nan even when using tables that suggest
it should be zero.

I suppose that there is some other place in the code where this
problem develops?

While looking at share/gromacs/top/table6-12.xvg it seems that this
should not lead to energies of nan, but it does.

$ head share/gromacs/top/table6-9.xvg
#
# Table AB1: ndisp=6 nrep=9
#
0.00e+00   0.00e+00 0.00e+00
0.00e+00 0.00e+00   0.00e+00 0.00e+00
2.00e-03   0.00e+00 0.00e+00
0.00e+00 0.00e+00   0.00e+00 0.00e+00
4.00e-03   0.00e+00 0.00e+00
0.00e+00 0.00e+00   0.00e+00 0.00e+00
6.00e-03   0.00e+00 0.00e+00
0.00e+00 0.00e+00   0.00e+00 0.00e+00
8.00e-03   0.00e+00 0.00e+00
0.00e+00 0.00e+00   0.00e+00 0.00e+00
1.00e-02   0.00e+00 0.00e+00
0.00e+00 0.00e+00   0.00e+00 0.00e+00
1.20e-02   0.00e+00 0.00e+00
0.00e+00 0.00e+00   0.00e+00 0.00e+00

and therefore, according to manual 4.5.4 page 151 equation 6.23, the
[(qi*qj)/(4*pi*epsilon)]*f(rij) coulomb SR value should equal zero. I
tried a few things, like modifying the values so that they are
constant from 0 to 0.04 nm in the table.xvg file, but this did not help.

 here is the .top file that I used along with
ffoplsaa to test out this idea:

#include ffoplsaa.itp
#include na.itp

[ system ]
; name
tables

[ molecules ]
; name  number
MOL_A  1
MOL_B  1

 and here is the .itp file that I used along with
ffoplsaa to test out this idea:

[ atomtypes ]
  aaa   AA  8 15.999400.0   A0.0  0.0

[ moleculetype ]
; molname   nrexcl
MOL_A 1

[ atoms ]
; idat type   res nr  residu name at name cg nr   charge
1   aaa   1   MLA AA  11.0

[ moleculetype ]
; molname   nrexcl
MOL_B 1

[ atoms ]
; idat type   res nr  residu name at name cg nr   charge
1   aaa   1   MLB BB  1-1.0

 And the .gro file:

title
 2
 1MLA AA1   0.000   0.000   0.000
 1MLB BB1   0.000   0.000   0.000
   5.0  5.0  5.0

### And my .mdp file is

nsteps = 0
ns_type = grid
rlist = 1
rcoulomb = 1
rvdw = 1
coulombtype = user
tc_grps =  System
tau_t   =  1.0
ld_seed =  -1
ref_t = 300
gen_temp = 300
gen_vel = yes
unconstrained_start = no
gen_seed = -1
Pcoupl = berendsen
pcoupltype = isotropic
tau_p = 4
compressibility = 4.5e-5
ref_p = 1.0



Still, when I run a 0-step mdrun (mdrun -deffnm md1 -table
mod2.table.xvg), I get:

Energies (kJ/mol)
 LJ (SR)   Coulomb (SR)  PotentialKinetic En.   Total Energy
 0.0e+00nannannannan
 Temperature Pressure (bar)
 nannan

# I get the same thing if the two charges are like or dislike...

But if I then modity my topologies to turn the +1 charge to zero, I
get sensible output:

 

[gmx-users] exclusions

2011-05-11 Thread Gavin Melaugh
Hi all

I am cheking the non binary version topol.tpr form grompp and I was
wondering what the following format for the exclusion section signifies?

excls:
 nr=228
 nra=1920
 excls[0][0..12]={0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 15, 16}
 excls[1][13..25]={0, 1, 2, 3, 4, 5, 6, 7, 9, 10, 11, 12, 15}


Also I take it, that this is a result of nrexcl =3

Cheers

Gavin
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[gmx-users] Rigid structure and flexible structure present in sing system

2011-05-11 Thread Luke Goodsell
Hi,

For a while I've been looking for a way to include a rigid
(macromolecular) structure and a flexible (small-protein) structure in
a single system and have not had much success.

I looked for a way to apply a different set of constraints to each
structure, but couldn't find one. I looked into modifying the topology
file, but the only method I could find was to artificially increase
the mass of every atom in the rigid structure and this does not save
any computing time.

Does anyone know how I can fix the relative co-ordinates of one
structure and only calculate the MD of another?

Any constructive criticism (even if to inform me that I'm doing
something ridiculous) is very gratefully received.

Kind regards,
Luke
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Re: [gmx-users] exclusions

2011-05-11 Thread Gavin Melaugh
Regarding my earlier post- If someone could confirm.
Taking into account that atom indices start from zero.
Then excls[0] = exclusions centred around atom 1.
[0..12] = there are 13 exclusions each one labelled form 0-12.
I then assume that you read the exclusions with respect to atom 0
(actual index =1)

In the next set do you read the exclusion with respect to atom 1 (actual
index =2).
and so on 


Many thanks in advance

Gavin
Gavin Melaugh wrote:
 Hi all

 I am cheking the non binary version topol.tpr form grompp and I was
 wondering what the following format for the exclusion section signifies?

 excls:
  nr=228
  nra=1920
  excls[0][0..12]={0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 15, 16}
  excls[1][13..25]={0, 1, 2, 3, 4, 5, 6, 7, 9, 10, 11, 12, 15}


 Also I take it, that this is a result of nrexcl =3

 Cheers

 Gavin
   

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[gmx-users] Rigid structure and flexible structure present in sing system

2011-05-11 Thread chris . neale
If I read between the lines correctly, you know how to do this in  
gromacs, but you wish that you got a big speedup from freezing most of  
the atoms in your system. If that is the case, then I think that  
gromacs can not help you in its current form. Therefore, I suggest  
that you try the Charmm software. It may be slower overall, but it  
gives you the speedup you expect when you freeze 95% of the atoms in  
your system so it may be much faster for your usage. Other software  
may also do this, but I have no experience with it. If you have  
explicit water, this won't be of much use since you're still only  
freezing 10% of the atoms in your system.


If you simply want to know how to freeze one structure, then use  
freeze groups and energy exclusions without pressure coupling, or use  
position restraints and refcoordscaling=com with position restraints,  
or create an elastic network of restraints.


Chris.

-- original message --

Hi,

For a while I've been looking for a way to include a rigid
(macromolecular) structure and a flexible (small-protein) structure in
a single system and have not had much success.

I looked for a way to apply a different set of constraints to each
structure, but couldn't find one. I looked into modifying the topology
file, but the only method I could find was to artificially increase
the mass of every atom in the rigid structure and this does not save
any computing time.

Does anyone know how I can fix the relative co-ordinates of one
structure and only calculate the MD of another?

Any constructive criticism (even if to inform me that I'm doing
something ridiculous) is very gratefully received.

Kind regards,
Luke



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Re: [gmx-users] Rigid structure and flexible structure present in sing system

2011-05-11 Thread Justin A. Lemkul



Luke Goodsell wrote:

Hi,

For a while I've been looking for a way to include a rigid
(macromolecular) structure and a flexible (small-protein) structure in
a single system and have not had much success.

I looked for a way to apply a different set of constraints to each
structure, but couldn't find one. I looked into modifying the topology
file, but the only method I could find was to artificially increase
the mass of every atom in the rigid structure and this does not save
any computing time.



Add a [constraints] directive for the molecule you want to make rigid and use 
constraints = none in the .mdp file.  Thus, only the bonds manually set to be 
constraints will be constrained.


Note that by constraining one molecule but not another, you still can't save any 
computing time, because the timestep of the simulation will still be limited by 
any bonds that are still harmonic (especially X-H).  Your system probably won't 
be stable with dt  1 fs, even with some molecule(s) constrained.



Does anyone know how I can fix the relative co-ordinates of one
structure and only calculate the MD of another?

Any constructive criticism (even if to inform me that I'm doing
something ridiculous) is very gratefully received.


I don't see any value in constraining one molecule but not another.  You can't 
increase the timestep and you lose the ability to have rigid bonds.  The 
argument can be made that a rigid bond is a better representation of reality 
than a harmonic one for most biological applications, or any done at ambient 
temperature, really.


-Justin



Kind regards,
Luke


--


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] selecting groups for full trajectory

2011-05-11 Thread Ravi Bhadauria
Hello,

I wish to select the groups for full precision trajectory (.trr files). Is
there a way to choose which group should be written to trr files (like
xtc-groups for .xtc files). Since I need the forces and velocities, xtc
trajectory won't work.

Thanks in advance,

Ravi Bhadauria
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Re: [gmx-users] selecting groups for full trajectory

2011-05-11 Thread Justin A. Lemkul



Ravi Bhadauria wrote:

Hello,

I wish to select the groups for full precision trajectory (.trr files). 
Is there a way to choose which group should be written to trr files 
(like xtc-groups for .xtc files). Since I need the forces and 
velocities, xtc trajectory won't work.


There is no equivalent option.  You can extract forces and velocities after the 
simulation using g_traj and any index group of your choosing.


-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] CG database for POPC

2011-05-11 Thread Du Jiangfeng (BIOCH)
 have written a program to calculate the geometric accessible surface
 area using the van der waals radius of the atoms and a probe of a
 given
 size. The surface is defined from the centre of the probe. Using the
 above values for sigma I obtain a value for methane of 1.15 nm^2
 with a
 probe diameter of 0.2 nm.

 Obviously the two do not match and I am not sure why.

 The individual atom areas for my molecule are:
 C 0.22
 H 0.24
 H 0.23
 H 0.22
 H 0.24

 Attached are the files used in the gromacs calculation along with the
 output and my own program. If any one has any suggestions please let
 me
 know.
 
 area
 .xvg
 
 
 atomarea
 .xvg
 
 
 conf
 .gro
 
 grompp.mdpmethane.itpresarea.xvgtopol.topPIsurfaceOPLS.f90--
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
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--

Message: 3
Date: Wed, 11 May 2011 15:48:36 +0200
From: Erik Marklund er...@xray.bmc.uu.se
Subject: Re: [gmx-users] Surface area calculation
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4dca93b4.3030...@xray.bmc.uu.se
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

Laura Leay skrev 2011-05-11 14.34:
 Can anyone explain in detail the method that gromacs uses to calculate
 surface area? Which surface area is it calculating (e.g., connolley,
 accessible)?

 I am under the impression that the final result is given in nm^2. Is
 this correct?


 Carrying out the surface area calculation in gromacs using the OPLS all
 atom force field I obtain a value of 4.43 nm^2  for methane (carbon =
 opls_138, sigma = 0.35 and hydrogen = opls_140, sigma = 0.25) (CT-HC
 ideal bond length = 0.109, e=284512). The command was

 g_sas -f conf.gro -s topol.tpr -oa -or -tv -probe 0.2 -ndots 200 -nopbc

 and the result was taken from resarea.xvg


 I have written a program to calculate the geometric accessible surface
 area using the van der waals radius of the atoms and a probe of a given
 size. The surface is defined from the centre of the probe. Using the
 above values for sigma I obtain a value for methane of 1.15 nm^2 with a
 probe diameter of 0.2 nm.
One difference is that g_sas -probe 0.2 uses a probe with a 0.2 nm
*radius*, while your code use a 0.2 nm diameter. That doesn't on its own
explain the difference you report, but you probably want to use the same
probe when comparing.

Erik
 Obviously the two do not match and I am not sure why.

 The individual atom areas for my molecule are:
 C 0.22
 H 0.24
 H 0.23
 H 0.22
 H 0.24

 Attached are the files used in the gromacs calculation along with the
 output and my own program. If any one has any suggestions please let me
 know.


--
---
Erik Marklund, PhD student
Dept. of Cell and Molecular Biology, Uppsala University.
Husargatan 3, Box 596,75124 Uppsala, Sweden
phone:+46 18 471 4537fax: +46 18 511 755
er...@xray.bmc.uu.sehttp://folding.bmc.uu.se/



--

Message: 4
Date: Wed, 11 May 2011 20:15:20 +0530 (IST)
From: vidhya sankar scvsankar_...@yahoo.com
Subject: [gmx-users] reg pushing rate
To: gmx-users@gromacs.org
Message-ID: 214557.84456...@web95502.mail.in.yahoo.com
Content-Type: text/plain; charset=iso-8859-1

Dear justin thank you for your mail
???
to push a mobile group towards reference group? I set the pull_rate in negative 
value (-0.1) as u said My question is
?when i change the pull rate to less negative value (-0.01) will push rate 
increases or decreases?
?because my doubt is about sign .it means if set pull rate to high negative 
value will push rate decrases or increase sign confuse me? i am expcting? 
valuable reply
Thanks in Advance
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Message: 5
Date: Wed, 11 May 2011 10:47:59 -0400
From: Justin A. Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] reg pushing rate
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4dcaa19f.1000...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



vidhya sankar wrote:
 Dear justin thank you for your mail

 to push a mobile group towards reference group  I set the pull_rate in
 negative value (-0.1) as u said My question is
  when i change the pull rate to less negative value (-0.01) will push
 rate increases or decreases?
  because my doubt is about sign .it means if set pull rate to high
 negative value will push rate decrases or increase sign confuse me  i am

You can answer this question yourself with a simple test

Re: [gmx-users] CG database for POPC

2011-05-11 Thread Justin A. Lemkul



Du Jiangfeng (BIOCH) wrote:

Dear All, I require a CG database of POPC for coarse grained simulation. Can
anyone give some suggestions for where to find it or how to make it by
myself? PS: the structure file of POPC was from the Biocomputing, Department
of Biological Sciences, University of Calgary. Thank you in advance.



The MARTINI site has a variety of coordinate and topology files you can likely
make use of:

http://md.chem.rug.nl/cgmartini/index.php/downloads

I don't believe they have a pure POPC membrane, but they do have POPE, which can
easily be converted.

In the future, please do not respond to the entire digest, especially when
starting a new and entirely unrelated thread.  It confuses the archive horribly.
 It's bad enough, let's not make it any worse :)

-Justin

Jiangfeng Du, PhD Student Cardiovascular Research Institute Maastricht 
Department of Biochemistry P.O. Box 616 Mobile: +31-681741859 FAX:
+31-43-3884159 6200 MD Maastricht The Netherlands 



--


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] Genbox question

2011-05-11 Thread Fabian Casteblanco
Hello,

I was wondering if someone can help me with a general genbox question.
 I have been using the command line:

genbox -ci octanol.gro -nmol 1000 -box 5 5 5 -o prop_1000.gro

to fill a box with 1000 molecules of octanol.  With the smaller
n-alcohols, it worked fine but as I started using 1-butanol,
1-pentanol, (longer carbon chains) up to octanol, Gromacs sometimes
ends the command with a 'Killedin-Solvent overlap' line at the very
end.  Sometimes increasing the box size helped, but for 1-pentanol,
even 7 7 7 box size didn't work.  Also, do these killed runs take up
some sort of space.  My memory space decreases a little bit even on
failed runs.

Thanks.

-- 
Best regards,

Fabian F. Casteblanco
Rutgers University --
Chemical Engineering PhD Student
C: +908 917 0723
E:  fabian.castebla...@gmail.com
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Re: [gmx-users] Genbox question

2011-05-11 Thread Justin A. Lemkul



Fabian Casteblanco wrote:

Hello,

I was wondering if someone can help me with a general genbox question.
 I have been using the command line:

genbox -ci octanol.gro -nmol 1000 -box 5 5 5 -o prop_1000.gro

to fill a box with 1000 molecules of octanol.  With the smaller
n-alcohols, it worked fine but as I started using 1-butanol,
1-pentanol, (longer carbon chains) up to octanol, Gromacs sometimes
ends the command with a 'Killedin-Solvent overlap' line at the very
end.  Sometimes increasing the box size helped, but for 1-pentanol,
even 7 7 7 box size didn't work.  Also, do these killed runs take up
some sort of space.  My memory space decreases a little bit even on
failed runs.



Generating random boxes in this way requires lots of memory and is prone to 
failure.  A useful strategy is to overestimate the size of the box so that 
genbox doesn't have to do too many iterations to place all of the molecules, 
then run a nice, long equilibration to get the box vectors (and therefore 
density, etc) correct.


-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] Genbox question

2011-05-11 Thread Justin A. Lemkul



Justin A. Lemkul wrote:



Fabian Casteblanco wrote:

Hello,

I was wondering if someone can help me with a general genbox question.
 I have been using the command line:

genbox -ci octanol.gro -nmol 1000 -box 5 5 5 -o prop_1000.gro

to fill a box with 1000 molecules of octanol.  With the smaller
n-alcohols, it worked fine but as I started using 1-butanol,
1-pentanol, (longer carbon chains) up to octanol, Gromacs sometimes
ends the command with a 'Killedin-Solvent overlap' line at the very
end.  Sometimes increasing the box size helped, but for 1-pentanol,
even 7 7 7 box size didn't work.  Also, do these killed runs take up
some sort of space.  My memory space decreases a little bit even on
failed runs.



Generating random boxes in this way requires lots of memory and is prone 
to failure.  A useful strategy is to overestimate the size of the box so 
that genbox doesn't have to do too many iterations to place all of the 
molecules, then run a nice, long equilibration to get the box vectors 
(and therefore density, etc) correct.


A more reliable method is probably genconf:

genconf -f molecule.gro -nbox 10 10 10 -o box.gro

You'll get 1000 molecules every time and the box size should be sensible.  Then 
proceed with equilibration.


-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_current and output redirection

2011-05-11 Thread Vitaly Chaban
Hi Flo,

Do you imply that conductivity and dielectric constant from g_current
go to the error stream? But why, if these are not errors

Vitaly



On Wed, May 11, 2011 at 5:07 AM, Dommert Florian
domm...@icp.uni-stuttgart.de wrote:
 Hello Vitaly,

 the intention to write out informations to the stdout and the stderr was
 that you have the ability to sort it during the analysis. However as
 Justin mentionen  will write all open pipes into one file.

 Cheers,
 Flo

 On Tue, 2011-05-10 at 13:16 -0400, Vitaly Chaban wrote:
 Thanks, Justin! Great solution.

 On Tue, May 10, 2011 at 12:57 PM, Justin A. Lemkul jalem...@vt.edu wrote:
 
 
  Vitaly Chaban wrote:
 
  I have a pure linux question. When using g_current and trying to
  redirect its output to the file, e.g.
 
  g_current -temp $TEMPER -b $conduct_b -e $conduct_e  EOF  output
  0
  EOF
 
  only a part of output is written to the file (output)
 
  Here is what is actually written to the file:
 
  Selected 0: 'System'
  Average translational dipole moment M_J [enm] after 25001 frames
  (|M|^2): 5.554790 -5.833042 -0.539783 (68.255722)
  Average molecular dipole moment M_D [enm] after 25001 frames (|M|^2):
  -0.414639 -0.356325 0.148187 (2.359227)
 
  Thus, the relevant data (sigma, dielectric constant) are missed. My
  question is how to redirect all the output of g_current to my file.
 
 
  echo 0 | g_current (options) outfile
 
  -Justin
 
 
  Thanks!
 
  Dr. Vitaly V. Chaban, Department of Chemistry
  University of Rochester, Rochester, New York 14627-0216
 
  --
  
 
  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] How to freeze groups

2011-05-11 Thread Elisabeth
Hello,

Can anyone suggest some tutorials or sample top files for simulations
involving freezing of groups? I dont see much info in chapter 5 of manual.

Thanks,
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Re: [gmx-users] How to freeze groups

2011-05-11 Thread Justin A. Lemkul



Elisabeth wrote:

Hello,

Can anyone suggest some tutorials or sample top files for simulations 
involving freezing of groups? I dont see much info in chapter 5 of manual.




You're looking in the wrong place - freezing is not handled in the topology. 
Use the freezegrps .mdp keyword with a group of your choice.  The group may 
require a custom index group if it is one of the non-standard ones.


Try manual section 7.3.24.

-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] Re: [gmx-developers] flexible water model

2011-05-11 Thread Nilesh Dhumal
Hello Justin,

I used 0.5 fs time step and still I got  dielectric constant ~2.

This is the md.mdp file  I used. I checked the temperature it didn't go
more than ~ 320 K.

title   =  cpeptide MD
cpp =  /usr/bin/cpp
integrator  =  md
dt  =  0.001; ps !
nsteps  =  650 ; total 5 ps.
nstcomm =  1000
nstxout =  1000
nstvout =  1000
nstfout =  1
nstlist =  1
ns_type =  grid
rlist   =  0.6
rcoulomb=  0.6
rvdw=  0.7
coulombtype = PME
vdwtype = cut-off
pbc = xyz
fourierspacing  = 0.12
fourier_nx = 0
fourier_ny = 0
fourier_nz = 0
pme_order   = 4
ewald_rtol  = 1e-5
optimize_fft= yes
; Berendsen temperature coupling is on
Tcoupl = v-rescale
tau_t = 0.1
tc-grps  =system
ref_t =   295
; Pressure coupling is  on
Pcoupl  = parrinello-rahman
pcoupltype  = isotropic
tau_p   =  0.5
compressibility =  4.5e-5
ref_p   =  1.0
; Generate velocites is on at 300 K.
gen_vel =  yes
gen_temp=  295.0
gen_seed=  173529


Nilesh


On Tue, May 10, 2011 6:14 pm, Justin A. Lemkul wrote:


 The gmx-developers list is not the forum for these types of questions.  I
 am replying via gmx-users, which is where the discussion should stay.

 I took a few minutes to dig into this.  My conclusion is that your system
 is not stable.  I would encourage you to analyze the temperature and
 pressure of your systems that are giving odd results.  When I used the
 topology you provided, the temperature spiked to over 600 K and the box
 began to oscillate extensively as if the system were about to explode.
 The resulting epsilon value was about 1.6.


 If I reduce the timestep to 0.5 fs, the results are much more reasonable,
 and using the Ka and Kb values in the paper (not halved!) I get a much
 more sensible result, even after just 100 ps.  It looks to me as if the
 combination of these parameters and a 1-fs timestep is not entirely
 stable.  I know the original authors used dt = 1 fs, but the point
 remains.

 -Justin


 Nilesh Dhumal wrote:

 Hello,


 I am using flexible water model for my system. I am referring a paper
 J.
 Chem. Phys. 124, 024503 (2006). Author have used Amber type force field.


 i.e. 1/2 Kbond (r-req)**2 + 1/2 Kangle(theta-thetaeq)**2.

 Kbond = 443153.3808 kJ/mol nm**2


 Kangle= 317.5656 kJ/mol rad**2.


 I am using olss-aa force field parameters in Gromacs  VERSION 4.0.7.


 I checked some papers in which author have used oplsaa force field in
 Gromacs. 1/2 factor is not in opls force field if I compare opls and
 amber.


 I didn’t get the proper dielectric constant for water when I used the
 parameters reported in paper

 (Kbond = 443153.3808 kJ/mol nm**2,Kangle= 317.5656 kJ/mol rad**2)


 I half the value of Kb and get the proper dielectric constant (~80) for
  water reported in paper. If I half Kangle  then I don’t get proper
 value. Below are the results for the dielectric constant of water.
 Bond length is nm.


 Here I have done some analysis.  The original value reported in J.
 Chem.
 Phys. 124, 024503 2006, paper are


 Kbond = 443153.3808 kJ/mol nm**2
 Kangle = 317.5656 kJ/mol rad**2.



 bond lengthKbond   angleKangledielectric constant
 0.1012
 443153.3808113.24  317.5656   ~1.9 : orginal value



 0.1012   221576.6904113.24  317.5656   ~80   : 1/2 (Kbond)



 0.1012   443153.3808113.24  158.7828   ~1.58 : 1/2 (kangle)



 0.1012  221576.6904113.24  317.5656   ~1.9   : 1/2
 (Kbond)(Kangle)



 Here I pasted spc_fw.itp file used for the simulation.


 ; Derived from parsing of runfiles/alat.top.orig
 [ defaults ]
 ; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
 ;1   3   yes 0.5 0.5
 ; comb-rule 3 is square-root sigma, the OPLSAA version


 [ atomtypes ]
 ; full atom descriptions are available in ffoplsaa.atp
 ; name  bond_typemasscharge   ptype  sigma  epsilon
 opls_1001  OW  8 15.99940-0.820   A3.1655e-01
 6.503e-01
 opls_1002  HW  1  1.00800 0.410   A0.00e+00 0.00e+00


 [ bondtypes ]
 ; ij  func   b0  kb
 OWHW  10.1012   443153.3808   ; J. Chem. Phys.
 (2006),124,024503
 [ angletypes ]
 ;  ijk  func   th0   cth
 HW OW HW  1   113.24  317.5656 ; J. Chem. Phys.
 (2006),124,024503


 [ moleculetype ]
 ; Namenrexcl
 WAT 3


 [ atoms ]
 ; nr   type  resnr residue  atom   cgnr charge   mass  typeB
  chargeB  massB 1   opls_1001 1WAT OW  1  -0.82
 15.99940 ;
 2   opls_1002 1WATHW1  1   0.41  1.008   ;
 3   opls_1002 1WATHW2  1   0.41  1.008   ;


 [ bonds ]
 ; i  

Re: [gmx-users] Re: [gmx-developers] flexible water model

2011-05-11 Thread Nilesh Dhumal
I have general question. If this parameters are not giving the proper
results then How come I get the proper results with same parameter if I
use 1/2 value of Kbond with the same parameters.

I checked the temp when I use half value of Kbond and it goes max. ~320.

Nilesh

On Wed, May 11, 2011 4:03 pm, Justin A. Lemkul wrote:



 Nilesh Dhumal wrote:

 Hello Justin,


 I used 0.5 fs time step and still I got  dielectric constant ~2.


 This is the md.mdp file  I used. I checked the temperature it didn't go
  more than ~ 320 K.


 Still, that's unacceptable if your ref_t is 295.  The fact that the
 temperature is still rocketing up suggests the same instability I found.

 title   =  cpeptide MD cpp =  /usr/bin/cpp
 integrator  =  md dt  =  0.001; ps ! nsteps
 =  650 ; total 5 ps.
 nstcomm =  1000 nstxout =  1000 nstvout
 =  1000
 nstfout =  1 nstlist =  1 ns_type =
 grid rlist   =  0.6 rcoulomb=  0.6 rvdw
 =  0.7


 These cutoffs make no sense.  The paper you've cited used 0.9 nm.  If
 you're trying to reproduce previous work, use the same settings.

 coulombtype = PME vdwtype = cut-off

 Similarly here, you haven't applied dispersion correction, which you
 should, per the methods used in the JCP article.

 -Justin


 pbc = xyz fourierspacing  = 0.12 fourier_nx = 0
 fourier_ny = 0 fourier_nz = 0 pme_order   = 4 ewald_rtol
 = 1e-5
 optimize_fft= yes ; Berendsen temperature coupling is on
 Tcoupl = v-rescale
 tau_t = 0.1 tc-grps  =system ref_t =   295 ; Pressure coupling is  on
 Pcoupl  = parrinello-rahman
 pcoupltype  = isotropic tau_p   =  0.5 compressibility
 =  4.5e-5
 ref_p   =  1.0 ; Generate velocites is on at 300 K.
 gen_vel =  yes gen_temp=  295.0 gen_seed
 =  173529



 Nilesh



 On Tue, May 10, 2011 6:14 pm, Justin A. Lemkul wrote:


 The gmx-developers list is not the forum for these types of
 questions.  I am replying via gmx-users, which is where the discussion
 should stay.

 I took a few minutes to dig into this.  My conclusion is that your
 system is not stable.  I would encourage you to analyze the
 temperature and pressure of your systems that are giving odd results.
 When I used the
 topology you provided, the temperature spiked to over 600 K and the
 box began to oscillate extensively as if the system were about to
 explode. The resulting epsilon value was about 1.6.



 If I reduce the timestep to 0.5 fs, the results are much more
 reasonable, and using the Ka and Kb values in the paper (not halved!)
 I get a much
 more sensible result, even after just 100 ps.  It looks to me as if
 the combination of these parameters and a 1-fs timestep is not
 entirely stable.  I know the original authors used dt = 1 fs, but the
 point remains.

 -Justin



 Nilesh Dhumal wrote:


 Hello,



 I am using flexible water model for my system. I am referring a
 paper J.
 Chem. Phys. 124, 024503 (2006). Author have used Amber type force
 field.


 i.e. 1/2 Kbond (r-req)**2 + 1/2 Kangle(theta-thetaeq)**2.

 Kbond = 443153.3808 kJ/mol nm**2



 Kangle= 317.5656 kJ/mol rad**2.



 I am using olss-aa force field parameters in Gromacs  VERSION
 4.0.7.



 I checked some papers in which author have used oplsaa force field
 in Gromacs. 1/2 factor is not in opls force field if I compare opls
 and amber.


 I didn’t get the proper dielectric constant for water when I used
 the parameters reported in paper

 (Kbond = 443153.3808 kJ/mol nm**2,Kangle= 317.5656 kJ/mol rad**2)



 I half the value of Kb and get the proper dielectric constant (~80)
 for water reported in paper. If I half Kangle  then I don’t get
 proper value. Below are the results for the dielectric constant of
 water. Bond length is nm.



 Here I have done some analysis.  The original value reported in J.
 Chem.
 Phys. 124, 024503 2006, paper are



 Kbond = 443153.3808 kJ/mol nm**2
 Kangle = 317.5656 kJ/mol rad**2.




 bond lengthKbond   angleKangledielectric constant
 0.1012
 443153.3808113.24  317.5656   ~1.9 : orginal value




 0.1012   221576.6904113.24  317.5656   ~80   : 1/2
 (Kbond)




 0.1012   443153.3808113.24  158.7828   ~1.58 : 1/2
 (kangle)




 0.1012  221576.6904113.24  317.5656   ~1.9   : 1/2
 (Kbond)(Kangle)




 Here I pasted spc_fw.itp file used for the simulation.



 ; Derived from parsing of runfiles/alat.top.orig
 [ defaults ]
 ; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
 ;1   3   yes 0.5 0.5
 ; comb-rule 3 is square-root sigma, the OPLSAA version



 [ atomtypes ]
 ; full atom descriptions are available in ffoplsaa.atp
 ; name  bond_typemasscharge   ptype  sigma
 epsilon opls_1001  OW  8 15.99940-0.820   A
 

Re: [gmx-users] Re: [gmx-developers] flexible water model

2011-05-11 Thread Justin A. Lemkul



Nilesh Dhumal wrote:

I have general question. If this parameters are not giving the proper
results then How come I get the proper results with same parameter if I
use 1/2 value of Kbond with the same parameters.



Random chance, I imagine.  Your .mdp settings are not correct and the cutoffs 
are unreasonably short for any modern force field.  If you're seeking to 
reproduce others' work, then you have to use the same protocol.  You're not 
doing that.



I checked the temp when I use half value of Kbond and it goes max. ~320.



This would also indicate instability.  You managed to get a correct result for 
one observable from an incorrect simulation wherein the thermodynamic 
observables do not correspond to what you have set.


The way I found all of this out was first and foremost by watching the 
trajectory.  After about 30 ps, the water molecules freeze in place and vibrate 
as if they are about to shear apart.  At this exact time, the value of epsilon 
(from epsilon.xvg, output by g_dipoles) plummets down, after having steadily 
increased for the first 30 ps, as expected.  The temperature spikes and the 
pressure begins to oscillate by +/- 10^5, far higher than what it should for a 
system of a few hundred water molecules.


Watch your trajectories, make sure you're getting the right average temperature 
and pressure, and that all your other energetic terms stabilize, then analyze 
the result of the simulation.  Otherwise, any inferred output is meaningless.


-Justin


Nilesh

On Wed, May 11, 2011 4:03 pm, Justin A. Lemkul wrote:


Nilesh Dhumal wrote:


Hello Justin,


I used 0.5 fs time step and still I got  dielectric constant ~2.


This is the md.mdp file  I used. I checked the temperature it didn't go
 more than ~ 320 K.


Still, that's unacceptable if your ref_t is 295.  The fact that the
temperature is still rocketing up suggests the same instability I found.


title   =  cpeptide MD cpp =  /usr/bin/cpp
integrator  =  md dt  =  0.001; ps ! nsteps
=  650 ; total 5 ps.
nstcomm =  1000 nstxout =  1000 nstvout
=  1000
nstfout =  1 nstlist =  1 ns_type =
grid rlist   =  0.6 rcoulomb=  0.6 rvdw
=  0.7


These cutoffs make no sense.  The paper you've cited used 0.9 nm.  If
you're trying to reproduce previous work, use the same settings.


coulombtype = PME vdwtype = cut-off

Similarly here, you haven't applied dispersion correction, which you
should, per the methods used in the JCP article.

-Justin



pbc = xyz fourierspacing  = 0.12 fourier_nx = 0
fourier_ny = 0 fourier_nz = 0 pme_order   = 4 ewald_rtol
= 1e-5
optimize_fft= yes ; Berendsen temperature coupling is on
Tcoupl = v-rescale
tau_t = 0.1 tc-grps  =system ref_t =   295 ; Pressure coupling is  on
Pcoupl  = parrinello-rahman
pcoupltype  = isotropic tau_p   =  0.5 compressibility
=  4.5e-5
ref_p   =  1.0 ; Generate velocites is on at 300 K.
gen_vel =  yes gen_temp=  295.0 gen_seed
=  173529



Nilesh



On Tue, May 10, 2011 6:14 pm, Justin A. Lemkul wrote:



The gmx-developers list is not the forum for these types of
questions.  I am replying via gmx-users, which is where the discussion
should stay.

I took a few minutes to dig into this.  My conclusion is that your
system is not stable.  I would encourage you to analyze the
temperature and pressure of your systems that are giving odd results.
When I used the
topology you provided, the temperature spiked to over 600 K and the
box began to oscillate extensively as if the system were about to
explode. The resulting epsilon value was about 1.6.



If I reduce the timestep to 0.5 fs, the results are much more
reasonable, and using the Ka and Kb values in the paper (not halved!)
I get a much
more sensible result, even after just 100 ps.  It looks to me as if
the combination of these parameters and a 1-fs timestep is not
entirely stable.  I know the original authors used dt = 1 fs, but the
point remains.

-Justin



Nilesh Dhumal wrote:



Hello,



I am using flexible water model for my system. I am referring a
paper J.
Chem. Phys. 124, 024503 (2006). Author have used Amber type force
field.


i.e. 1/2 Kbond (r-req)**2 + 1/2 Kangle(theta-thetaeq)**2.

Kbond = 443153.3808 kJ/mol nm**2



Kangle= 317.5656 kJ/mol rad**2.



I am using olss-aa force field parameters in Gromacs  VERSION
4.0.7.



I checked some papers in which author have used oplsaa force field
in Gromacs. 1/2 factor is not in opls force field if I compare opls
and amber.


I didn’t get the proper dielectric constant for water when I used
the parameters reported in paper

(Kbond = 443153.3808 kJ/mol nm**2,Kangle= 317.5656 kJ/mol rad**2)



I half the value of Kb and get the proper dielectric constant (~80)
for water reported in paper. If I half Kangle  then I 

[gmx-users] index file

2011-05-11 Thread ahmet yıldırım
Dear users,

I have two ligands. I created a special index group that merges the protein,
LiGA and LİGB.

I have the pr.mdp file as the following:
...
energygrps  = ProteinLİGA_LİGB
tc-grps = Protein_LİGA_LİGBWater_and_ions
...

grompp -f pr.mdp -p topol.top -c em.gro -n index.ndx -o pr.tpr
Fatal error:
Group LİGA_LİGB not found in indexfile.

I get the fatal error since I dont have a special index group that merges
LiGA and LİGB. should I create two different index file?

Thanks in advance
-- 
Ahmet YILDIRIM
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Re: [gmx-users] REMD: after replica exchange breakdown

2011-05-11 Thread Mark Abraham

On 11/05/2011 10:59 PM, SebastianWaltz wrote:

On 05/11/2011 05:20 AM, Mark Abraham wrote:

On 05/11/2011 02:32 AM, SebastianWaltz wrote:

Dear GROMACS User,

I'm running a REMD MD of 32 replicas. It worked for the first few
replica exchanges. After 30ps again two replicas were exchanged and I
received the Error:
x particles communicated to PME node y are more than a cell length out
of the domain decomposition cell of their charge group

The only rationale I can see is that a velocity was scaled after
exchange that was now large enough to lead to the normal sort of
exploding system. Was the exploding replica going up in temperature?
How did you equilibrate the systems?

I did a NPT equilibration for each replica which leads obviously to
different volumes and looks like to cause some problems. If I use the
same volume for each replica it works fine.


Yeah, that'd be it. Do the NPT equilibration at your target temperature, 
and then construct the other replicas to have that volume, before 
equilibrating each replica at its temperature under NVT.



I am using NVT assembles for each replica with a exchanging interval of
5ps. For each replica I use 4 processors. Constraint are only the bonds
to hydrogens (constraints = hbonds). Using PME for electro static.

Information like GROMACS version, simulation system dimensions and
contents would be useful. What replica temperature distribution exists?

I am using version 4.0.7. My system consists of a small peptide soluted
in ~1500 rigid CHCl3 molecules. System equilibrated with NPT and NVT
production run seems to work only if I increase the number of replicas
(32-64) meaning that I also decrease the difference of the volumes. The
temperature is exponentially distributed from 200 to 450K.


Seems OK.

Mark


When running each replica for its own everything is working fine,
nothing is blowing up like one would expect after getting the above
Error.

Good trouble-shooting :) You'd have been told to try this otherwise...

Mark


Thanks a lot

Sebastian


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Re: [gmx-users] index file

2011-05-11 Thread Mark Abraham

On 12/05/2011 8:23 AM, ahmet yıldırım wrote:

Dear users,

I have two ligands. I created a special index group that merges the 
protein, LiGA and LİGB.


I have the pr.mdp file as the following:
...
energygrps  = ProteinLİGA_LİGB
tc-grps = Protein_LİGA_LİGBWater_and_ions
...

grompp -f pr.mdp -p topol.top -c em.gro -n index.ndx -o pr.tpr
Fatal error:
Group LİGA_LİGB not found in indexfile.

I get the fatal error since I dont have a special index group that 
merges LiGA and LİGB. should I create two different index file?


You need to give grompp an index file that defines all the groups you 
use. Yours didn't define LIGA_LIGB, so you need to do so, or to change 
your energygrps


Mark
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Re: [gmx-users] exclusions

2011-05-11 Thread Mark Abraham

On 12/05/2011 2:43 AM, Gavin Melaugh wrote:

Regarding my earlier post- If someone could confirm.
Taking into account that atom indices start from zero.
Then excls[0] = exclusions centred around atom 1.
[0..12] = there are 13 exclusions each one labelled form 0-12.
I then assume that you read the exclusions with respect to atom 0
(actual index =1)


I doubt it. I think each particle excludes itself in the list. Make a 
simple system where you can compute the exclusions by hand and see what 
the data structure is doing. Then vary it until you're happy with your 
deductions.


Mark


In the next set do you read the exclusion with respect to atom 1 (actual
index =2).
and so on 


Many thanks in advance

Gavin
Gavin Melaugh wrote:

Hi all

I am cheking the non binary version topol.tpr form grompp and I was
wondering what the following format for the exclusion section signifies?

excls:
  nr=228
  nra=1920
  excls[0][0..12]={0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 10, 15, 16}
  excls[1][13..25]={0, 1, 2, 3, 4, 5, 6, 7, 9, 10, 11, 12, 15}


Also I take it, that this is a result of nrexcl =3

Cheers

Gavin



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[gmx-users] (no subject)

2011-05-11 Thread X Rules
http://howtofindoutifsomeoneismarried.net/wp-content/themes/twentyten/site.html
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Re: [gmx-users] about g_hbond

2011-05-11 Thread lina
/* y-label: Hydrogen Bond Index */

is it relevant to the total number of hydrogen bonds?

such as
/* XPM */
/* x-label: Time (ps) */
/* y-label: Hydrogen Bond Index */
/* type:Discrete */
static char *gromacs_xpm[] = {

A-b : 51 84   2 1,

b-C : 51 95   2 1,

84, 95?

Thanks,
On Wed, May 11, 2011 at 11:10 PM, Justin A. Lemkul jalem...@vt.edu wrote:


 lina wrote:

 Hi,

 For group A, b, C.

 It's no doubt can get hb forming number between A-b, b-C. b-(A or C).

 But I don't know how to get the number of residues of b forming both
 with A and B at the same time. namely b-AC, not with AC group.


 There's no direct way to do it, but from the output files of g_hbond it can
 be done.  You'd need the .xpm files of A-C and B-C hydrogen bonds, and write
 some script that parses the .xpm files, and whenever there is an entry of
 A-C in the same frame as B-C, then you have a hydrogen bond mediated between
 the two.

 There's lots of discussion in the list archive about water-mediated
 hydrogen bonds that is likely applicable here.

 Note that if you're using g_hbond in version 4.5, there is an important bug
 that was fixed just yesterday:

 http://lists.gromacs.org/pipermail/gmx-users/2011-May/061249.html

 -Justin

 Thanks,
 --
 Best Regards,

 lina




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 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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Best Regards,

lina
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