Re: [gmx-users] removing pbc jumps from trajectory

2011-02-21 Thread XAvier Periole

You have to make sure of two things:

1- use a reference (gro or tpr) where the molecule is whole! The tpr is 
prefered since the molecules are defined. 

2- with such a reference and the option -mol you'll get a trajectory with the 
protein as a whole. 

On that trajectory you may apply more modifications: 
-nojump with generate a trajectory where the pbc are not applied so you can do 
msd analysis. Note that thisnis done by default in g_msd. 
- fitting with only translation removed (equivalent to centering but more 
stable. Centering works strangely)

XAvier.  

On Feb 21, 2011, at 8:52, Evelyne Deplazes depla...@student.uwa.edu.au wrote:

 Hi 
 
 I have a series of trajectories from a coarse grained simulation (Martini 
 force field) that I ran using gromacs 4.0.4. The system consists of a protein 
 embedded in a POPC bilayer solvated with water. During the simulation the 
 protein (most of time its actually *part* of the protein) jumps across the pb 
 into the neighboring box. I use a series of tcl scripts to analyse my 
 trajectories and for that purpose I need to remove that period boundary 
 jump and make the protein whole again. 
 
 I have tried the approach described on the gromacs website 
 http://www.gromacs.org/Documentation/Terminology/Periodic_Boundary_Conditions
 
 I also other combinations of -whole, -center and -pbc nojump of trjconv, 
 without any luck. Can anyone suggest how I can re-center the protein and 
 remove the pb jump ie make the protein whole
 
 Thanks 
 Evelyne 
 
 -- 
 Evelyne Deplazes
 
 PhD student 
 Theoretical Chemistry group
 University of Western Australia 
 
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[gmx-users] Re: gmx-users Digest, Vol 82, Issue 150

2011-02-21 Thread Evelyne Deplazes
I tried a couple of things according to your suggestions, but no luck so far


I used the following commands
1) trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -o trajout_mol.xtc
2) trjconv  -f trajout_mol.xtc -s topol.tpr -pbc nojump trajout_nojump.xtc

no luck...If I use command 1) only the trajout_mol.xtc the protein is still
split into to across 2 boxes ie it looks like it did not do anything to
the trajectory
if I use 1) and 2) the system gets ripped apart. The system is no longer a
box but a flat disk (very funky)


then I tried
trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -fit translation -o
trajout_fit.xtc
again...it looks like the trajectory did not change and the protein is still
jumping out of the box

then I tried
trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -trans -6 6 0 -o
trajout_trans.xtc(the box is about 12 x 12)
now at least this command did something to the trajectory. The entire
protein is now in the center of the box (rather than in the corner) but in
the frames where the pb jump occurs the protein still jumps out of the box!
it now simply jumps from the center to the next box rather than sliding
across the border into the next box

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 Today's Topics:

   1. Re: g_covar to calculate correlation of motion (Tsjerk Wassenaar)
   2. Re: g_covar to calculate correlation of motion (bipin singh)
   3. removing pbc jumps from trajectory (Evelyne Deplazes)
   4. Re: removing pbc jumps from trajectory (XAvier Periole)


 -- Forwarded message --
 From: Tsjerk Wassenaar tsje...@gmail.com
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Date: Mon, 21 Feb 2011 08:14:26 +0100
 Subject: Re: [gmx-users] g_covar to calculate correlation of motion

 Hi Bipin,

 Try using a .gro or .pdb file as reference structure (-s). Only .tpr files
 are version specific.

 Cheers,

 Tsjerk

 On Feb 21, 2011 8:05 AM, bipin singh bipinel...@gmail.com wrote:

 Dear GMX users,
 I want to calculate the correlated motion between atoms during the md 
 simulation

 for that purpose I am using g_covar(the one which is available under 
 http://www.gromacs.org/Downloads/User_contributions/Other_software)


 but it is not compatible with the GROMACS-4.5.3, so please suggest me the 
 alternative way or does anyone have the modified g_covar for
 GROMKACS-4.5.3.

 --
 *
 -
 Thanks and regards
 Bipin Singh
 *
 *
 *


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 -- Forwarded message --
 From: bipin singh bipinel...@gmail.com
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Date: Mon, 21 Feb 2011 13:17:48 +0530
 Subject: Re: [gmx-users] g_covar to calculate correlation of motion
 Hi,
 Thanks for your suggestion.
 While running the g_covar it is showing the error that aminoacids.dat is
 not found, so i have copied the residuetypes.dat(which i seems the new
 modified name for aminoacids.dat in current GROMACS version), then it
 prompts to choose the group for least square fit, which is not usual
 groups(i.e protein or C alpha groups etc.).please suggest where i have
 made mistake.

 Choose a group for the least squares fit
 Opening library file aminoacids.dat
 WARNING 2 [file aminoacids.dat, line 1]:
   File aminoacids.dat is empty
 Group 0 (  System) has 30585 elements
 Group 1 ( GLU) has47 elements
 Group 2 ( HIS) has86 elements
 Group 3 ( ASN) has   224 elements
 Group 4 ( PRO) has56 elements
 Group 5 ( VAL) has   272 elements
 Group 6 ( MET) has68 elements
 Group 7 ( GLY) has   168 elements
 Group 8 ( ILE) has   190 elements
 Group 9 ( ALA) has   110 elements
 Group10 ( SER) has   143 elements
 Group11 ( PHE) has80 elements
 Group12 ( LYS) has   242 elements
 Group13 ( TYR) has   189 elements
 Group14 ( LEU) has   304 elements
 Group15 ( GLN) has   102 elements
 Group16 ( TRP) has48 elements
 Group17 ( 

Re: [gmx-users] configure: error: cannot compute sizeof (off_t)

2011-02-21 Thread Carsten Kutzner

On Feb 20, 2011, at 9:30 PM, Justin Kat wrote:

 Dear experts,
 
 I am still unable to overcome this error during the configuration:
 
 configure: error: cannot compute sizeof (off_t)
 See `config.log' for more details.
So what does config.log say about cannot compute sizeof (off_t) ?

Carsten

 
 I came across this thread with the exact same setup as I have: 
 
 http://lists.gromacs.org/pipermail/gmx-users/2011-February/058369.html
 
 I have tried uninstalling openmpi 1.4.4 and installing the more stable 
 openmpi1.4.3 but I am still experiencing the same error.
 
 ./configure --enable-mpi --program-suffix=_mpi MPICC=/usr/local/bin/mpicc 
 --with-fft=fftw3
 
 I have also tried to explicitly provide the path to mpicc as above but it 
 still gives me the same error.
 
 This may or may not be relevant but at the end of the config.log there is 
 also this line:
 
 configure: exit 77
 
 Does that mean anything?
 
 Any help at all is appreciated!
 
 Thanks,
 Justin--
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 http://lists.gromacs.org/mailman/listinfo/gmx-users
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--
Dr. Carsten Kutzner
Max Planck Institute for Biophysical Chemistry
Theoretical and Computational Biophysics
Am Fassberg 11, 37077 Goettingen, Germany
Tel. +49-551-2012313, Fax: +49-551-2012302
http://www.mpibpc.mpg.de/home/grubmueller/ihp/ckutzne




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Re: [gmx-users] Re: gmx-users Digest, Vol 82, Issue 150

2011-02-21 Thread XAvier Periole


ok this does not make sense! Did you check your tpr file?
the command 1) should give you a trajectory where the molecules
are whole but jumping across the boundaries ... if it does not that
means that the tpr is fucky!

Try to visualize your tpr in vmd ... night give you some insight on  
what is

going on!

You could also make a tpr file ... making sure things a fine :))

On Feb 21, 2011, at 9:45 AM, Evelyne Deplazes wrote:

I tried a couple of things according to your suggestions, but no  
luck so far


I used the following commands
1) trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -o  
trajout_mol.xtc
2) trjconv  -f trajout_mol.xtc -s topol.tpr -pbc nojump  
trajout_nojump.xtc


no luck...If I use command 1) only the trajout_mol.xtc the protein  
is still split into to across 2 boxes ie it looks like it did not  
do anything to the trajectory
if I use 1) and 2) the system gets ripped apart. The system is no  
longer a box but a flat disk (very funky)



then I tried
trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -fit  
translation -o trajout_fit.xtc
again...it looks like the trajectory did not change and the protein  
is still jumping out of the box


then I tried
trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -trans -6 6 0 - 
o trajout_trans.xtc(the box is about 12 x 12)
now at least this command did something to the trajectory. The  
entire protein is now in the center of the box (rather than in the  
corner) but in the frames where the pb jump occurs the protein still  
jumps out of the box! it now simply jumps from the center to the  
next box rather than sliding across the border into the next box


On 21 February 2011 16:02, gmx-users-requ...@gromacs.org wrote:
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than Re: Contents of gmx-users digest...

Today's Topics:

  1. Re: g_covar to calculate correlation of motion (Tsjerk Wassenaar)
  2. Re: g_covar to calculate correlation of motion (bipin singh)
  3. removing pbc jumps from trajectory (Evelyne Deplazes)
  4. Re: removing pbc jumps from trajectory (XAvier Periole)


-- Forwarded message --
From: Tsjerk Wassenaar tsje...@gmail.com
To: Discussion list for GROMACS users gmx-users@gromacs.org
Date: Mon, 21 Feb 2011 08:14:26 +0100
Subject: Re: [gmx-users] g_covar to calculate correlation of motion
Hi Bipin,

Try using a .gro or .pdb file as reference structure (-s). Only .tpr  
files are version specific.


Cheers,

Tsjerk



On Feb 21, 2011 8:05 AM, bipin singh bipinel...@gmail.com wrote:

Dear GMX users,
I want to calculate the correlated motion between atoms during the  
md simulation



for that purpose I am using g_covar(the one which is available  
under http://www.gromacs.org/Downloads/User_contributions/Other_software)




but it is not compatible with the GROMACS-4.5.3, so please suggest  
me the alternative way or does anyone have the modified g_covar for

GROMKACS-4.5.3.

--
-
Thanks and regards
Bipin Singh



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-- Forwarded message --
From: bipin singh bipinel...@gmail.com
To: Discussion list for GROMACS users gmx-users@gromacs.org
Date: Mon, 21 Feb 2011 13:17:48 +0530
Subject: Re: [gmx-users] g_covar to calculate correlation of motion
Hi,
Thanks for your suggestion.
While running the g_covar it is showing the error that  
aminoacids.dat is not found, so i have copied the  
residuetypes.dat(which i seems the new modified name for  
aminoacids.dat in current GROMACS version), then it prompts to  
choose the group for least square fit, which is not usual groups(i.e  
protein or C alpha groups etc.).please suggest where i have made  
mistake.


Choose a group for the least squares fit
Opening library file aminoacids.dat
WARNING 2 [file aminoacids.dat, line 1]:
  File aminoacids.dat is empty
Group 0 (  System) has 30585 elements
Group 1 ( GLU) has47 elements
Group 2 ( HIS) has86 elements
Group 3 ( ASN) has   224 elements
Group 4 ( PRO) has56 elements
Group 5 ( VAL) has   272 elements
Group 6 ( MET) has68 elements
Group 7 ( GLY) has   168 elements
Group 8 ( ILE) has   

Re: [gmx-users] Re: gmx-users Digest, Vol 82, Issue 150

2011-02-21 Thread Tsjerk Wassenaar
Hi Evelyne,

 1) trjconv  -f trajout_dt2000.xtc -s topol.tpr -pbc mol -o trajout_mol.xtc

The option -pbc mol IIRC relates to the option for the unit cell
representation (-ur). To unbreak molecules using trjconv, you need to
have .tpr file and use the option -pbc whole.

 2) trjconv  -f trajout_mol.xtc -s topol.tpr -pbc nojump trajout_nojump.xtc
 if I use 1) and 2) the system gets ripped apart. The system is no longer a
 box but a flat disk (very funky)

This is because the jumps are removed and over time the lipids diffuse
in the plane. They've diffused quite a bit probably, smearing
themselves out over a disk.

Groetjes,

Tsjerk

-- 
Tsjerk A. Wassenaar, Ph.D.

post-doctoral researcher
Molecular Dynamics Group
* Groningen Institute for Biomolecular Research and Biotechnology
* Zernike Institute for Advanced Materials
University of Groningen
The Netherlands
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Re: [gmx-users] g_covar to calculate correlation of motion

2011-02-21 Thread Tsjerk Wassenaar
Hi Bipin,

The file residuetypes.dat is quite different from aminoacids.dat. You
can paste the following into that file (first line is number of
entries, followed by so many residue names):

49
ABU
ACE 
AIB
ALA
ARG
ARGN
ASN
ASN1
ASP
ASP1
ASPH
CYS
CYS1
CYS2
CYSH
DALA
GLN
GLU
GLUH
GLY
HIS
HIS1
HISA
HISB
HISH
HYP
ILE
LEU
LYS
LYSH
MELEU
MET
MEVAL
NAC
NH2
PHE
PHEH
PHEU
PHL
PRO
SER
THR
TRP
TRPH
TRPU
TYR
TYRH
TYRU
VAL


Groetjes,

Tsjerk

On Mon, Feb 21, 2011 at 8:47 AM, bipin singh bipinel...@gmail.com wrote:
 Hi,
 Thanks for your suggestion.
 While running the g_covar it is showing the error that aminoacids.dat is not
 found, so i have copied the residuetypes.dat(which i seems the new modified
 name for aminoacids.dat in current GROMACS version), then it prompts to
 choose the group for least square fit, which is not usual groups(i.e protein
 or C alpha groups etc.).please suggest where i have made mistake.

 Choose a group for the least squares fit
 Opening library file aminoacids.dat
 WARNING 2 [file aminoacids.dat, line 1]:
   File aminoacids.dat is empty
 Group 0 (  System) has 30585 elements
 Group 1 ( GLU) has    47 elements
 Group 2 ( HIS) has    86 elements
 Group 3 ( ASN) has   224 elements
 Group 4 ( PRO) has    56 elements
 Group 5 ( VAL) has   272 elements
 Group 6 ( MET) has    68 elements
 Group 7 ( GLY) has   168 elements
 Group 8 ( ILE) has   190 elements
 Group 9 ( ALA) has   110 elements
 Group    10 ( SER) has   143 elements
 Group    11 ( PHE) has    80 elements
 Group    12 ( LYS) has   242 elements
 Group    13 ( TYR) has   189 elements
 Group    14 ( LEU) has   304 elements
 Group    15 ( GLN) has   102 elements
 Group    16 ( TRP) has    48 elements
 Group    17 ( ARG) has   120 elements
 Group    18 ( ASP) has   108 elements
 Group    19 ( THR) has   141 elements
 Group    20 ( SOL) has 27882 elements
 Group    21 (  CL) has 5 elements


 On Mon, Feb 21, 2011 at 12:44, Tsjerk Wassenaar tsje...@gmail.com wrote:

 Hi Bipin,

 Try using a .gro or .pdb file as reference structure (-s). Only .tpr files
 are version specific.

 Cheers,

 Tsjerk

 On Feb 21, 2011 8:05 AM, bipin singh bipinel...@gmail.com wrote:

 Dear GMX users,

 I want to calculate the correlated motion between atoms during the md
 simulation

 for that purpose I am using g_covar(the one which is available under
 http://www.gromacs.org/Downloads/User_contributions/Other_software)



 but it is not compatible with the GROMACS-4.5.3, so please suggest me the
 alternative way or does anyone have the modified g_covar for
 GROMKACS-4.5.3.

 --
 -
 Thanks and regards
 Bipin Singh


 --
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 --
 -
 Thanks and regards
 Bipin Singh


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-- 
Tsjerk A. Wassenaar, Ph.D.

post-doctoral researcher
Molecular Dynamics Group
* Groningen Institute for Biomolecular Research and Biotechnology
* Zernike Institute for Advanced Materials
University of Groningen
The Netherlands
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Re: [gmx-users] g_covar to calculate correlation of motion

2011-02-21 Thread bipin singh
Thanks a lot Sir.

On Mon, Feb 21, 2011 at 15:26, Tsjerk Wassenaar tsje...@gmail.com wrote:

 Hi Bipin,

 The file residuetypes.dat is quite different from aminoacids.dat. You
 can paste the following into that file (first line is number of
 entries, followed by so many residue names):

 49
 ABU
 ACE
 AIB
 ALA
 ARG
 ARGN
 ASN
 ASN1
 ASP
 ASP1
 ASPH
 CYS
 CYS1
 CYS2
 CYSH
 DALA
 GLN
 GLU
 GLUH
 GLY
 HIS
 HIS1
 HISA
 HISB
 HISH
 HYP
 ILE
 LEU
 LYS
 LYSH
 MELEU
 MET
 MEVAL
 NAC
 NH2
 PHE
 PHEH
 PHEU
 PHL
 PRO
 SER
 THR
 TRP
 TRPH
 TRPU
 TYR
 TYRH
 TYRU
 VAL


 Groetjes,

 Tsjerk

 On Mon, Feb 21, 2011 at 8:47 AM, bipin singh bipinel...@gmail.com wrote:
  Hi,
  Thanks for your suggestion.
  While running the g_covar it is showing the error that aminoacids.dat is
 not
  found, so i have copied the residuetypes.dat(which i seems the new
 modified
  name for aminoacids.dat in current GROMACS version), then it prompts to
  choose the group for least square fit, which is not usual groups(i.e
 protein
  or C alpha groups etc.).please suggest where i have made mistake.
 
  Choose a group for the least squares fit
  Opening library file aminoacids.dat
  WARNING 2 [file aminoacids.dat, line 1]:
File aminoacids.dat is empty
  Group 0 (  System) has 30585 elements
  Group 1 ( GLU) has47 elements
  Group 2 ( HIS) has86 elements
  Group 3 ( ASN) has   224 elements
  Group 4 ( PRO) has56 elements
  Group 5 ( VAL) has   272 elements
  Group 6 ( MET) has68 elements
  Group 7 ( GLY) has   168 elements
  Group 8 ( ILE) has   190 elements
  Group 9 ( ALA) has   110 elements
  Group10 ( SER) has   143 elements
  Group11 ( PHE) has80 elements
  Group12 ( LYS) has   242 elements
  Group13 ( TYR) has   189 elements
  Group14 ( LEU) has   304 elements
  Group15 ( GLN) has   102 elements
  Group16 ( TRP) has48 elements
  Group17 ( ARG) has   120 elements
  Group18 ( ASP) has   108 elements
  Group19 ( THR) has   141 elements
  Group20 ( SOL) has 27882 elements
  Group21 (  CL) has 5 elements
 
 
  On Mon, Feb 21, 2011 at 12:44, Tsjerk Wassenaar tsje...@gmail.com
 wrote:
 
  Hi Bipin,
 
  Try using a .gro or .pdb file as reference structure (-s). Only .tpr
 files
  are version specific.
 
  Cheers,
 
  Tsjerk
 
  On Feb 21, 2011 8:05 AM, bipin singh bipinel...@gmail.com wrote:
 
  Dear GMX users,
 
  I want to calculate the correlated motion between atoms during the md
  simulation
 
  for that purpose I am using g_covar(the one which is available under
  http://www.gromacs.org/Downloads/User_contributions/Other_software)
 
 
 
  but it is not compatible with the GROMACS-4.5.3, so please suggest me
 the
  alternative way or does anyone have the modified g_covar for
  GROMKACS-4.5.3.
 
  --
  -
  Thanks and regards
  Bipin Singh
 
 
  --
  gmx-users mailing listgmx-users@gromacs.org
  http://lists.gromacs.org/mailman/listinfo/gmx-users
  Please search the archive at
  http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
  Please don't post (un)subscribe requests to the list. Use the
  www interface or send it to gmx-users-requ...@gromacs.org.
  Can't post? Read http://www.gromacs.org/Support/Mailing_Lists
 
  --
  gmx-users mailing listgmx-users@gromacs.org
  http://lists.gromacs.org/mailman/listinfo/gmx-users
  Please search the archive at
  http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
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  www interface or send it to gmx-users-requ...@gromacs.org.
  Can't post? Read http://www.gromacs.org/Support/Mailing_Lists
 
 
 
  --
  -
  Thanks and regards
  Bipin Singh
 
 
  --
  gmx-users mailing listgmx-users@gromacs.org
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[gmx-users] how many contacts has a certain atom at MD

2011-02-21 Thread Olga Ivchenko
Dear Gromacs Users,

I would like to know if there is in gromacs an option how to calculate how
many contacts has a certain atom i(n a molecules of interest) with water
during the whole MD simulations (or at each step of MD).
Please could you advice me on this?

best,
Olga
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Re: [gmx-users] how many contacts has a certain atom at MD

2011-02-21 Thread XAvier Periole

g_dist
On Feb 21, 2011, at 11:32 AM, Olga Ivchenko wrote:


Dear Gromacs Users,

I would like to know if there is in gromacs an option how to  
calculate how many contacts has a certain atom i(n a molecules of  
interest) with water during the whole MD simulations (or at each  
step of MD).

Please could you advice me on this?

best,
Olga

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Re: [gmx-users] how many contacts has a certain atom at MD

2011-02-21 Thread Erik Marklund
Or g_hbond -contact. Undfortuntely there are still issues with g_hbond 
at the moment. Version 4.0.x seem to work better.


XAvier Periole skrev 2011-02-21 11.37:

g_dist
On Feb 21, 2011, at 11:32 AM, Olga Ivchenko wrote:


Dear Gromacs Users,

I would like to know if there is in gromacs an option how to 
calculate how many contacts has a certain atom i(n a molecules of 
interest) with water during the whole MD simulations (or at each step 
of MD).

Please could you advice me on this?

best,
Olga

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---
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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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Re: [gmx-users] how many contacts has a certain atom at MD

2011-02-21 Thread Justin A. Lemkul


g_mindist -on (with suitable index groups) should also do the trick.

-Justin

Erik Marklund wrote:
Or g_hbond -contact. Undfortuntely there are still issues with g_hbond 
at the moment. Version 4.0.x seem to work better.


XAvier Periole skrev 2011-02-21 11.37:

g_dist
On Feb 21, 2011, at 11:32 AM, Olga Ivchenko wrote:


Dear Gromacs Users,

I would like to know if there is in gromacs an option how to 
calculate how many contacts has a certain atom i(n a molecules of 
interest) with water during the whole MD simulations (or at each step 
of MD).

Please could you advice me on this?

best,
Olga

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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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Re: [gmx-users] how many contacts has a certain atom at MD

2011-02-21 Thread Olga Ivchenko
Thank you very much.
best,
Olga

2011/2/21 Justin A. Lemkul jalem...@vt.edu


 g_mindist -on (with suitable index groups) should also do the trick.

 -Justin


 Erik Marklund wrote:

 Or g_hbond -contact. Undfortuntely there are still issues with g_hbond at
 the moment. Version 4.0.x seem to work better.

 XAvier Periole skrev 2011-02-21 11.37:

 g_dist
 On Feb 21, 2011, at 11:32 AM, Olga Ivchenko wrote:

  Dear Gromacs Users,

 I would like to know if there is in gromacs an option how to calculate
 how many contacts has a certain atom i(n a molecules of interest) with 
 water
 during the whole MD simulations (or at each step of MD).
 Please could you advice me on this?

 best,
 Olga

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 http://lists.gromacs.org/mailman/listinfo/gmx-users
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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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RE: [gmx-users] Porting Amber parmbsc0 force field to Gromacs

2011-02-21 Thread william Stebbeds

Hello, gods of gromacs,

I have ported the parmbsc0 modifications to a new gromacs force field, based on 
the amber99sb.ff, this involves adding a new carbon atom (CI) to be used in the 
C5' of nucleotides. 

Everything is working perfectly (to my astonishment) and I am confident of all 
of the modifications I have made, except for the func column in 
[diheadraltypes]. The only way I can get the parameters that involve the same 
four atoms to work is to alter this column. I have read chapter 5 but I cannot 
see in what way this will affect the new ff.

These are the original parameters from AMBERparmbsc0:

DIHE
X -CI-OS-X 3   1.150   0.0 3.0
X -CI-OH-X 3   0.500   0.0 3.0
X -CI-CT-X 9   1.400   0.0 3.0
CT-OS-CT-CI1   0.383   0.0-3.0
CT-OS-CT-CI1   0.100 180.0 2.0
H1-CI-CT-OS1   0.250   0.0 1.0
H1-CI-CT-OH1   0.250   0.0 1.0
H1-CT-CI-OS1   0.250   0.0 1.0
H1-CT-CI-OH1   0.250   0.0 1.0
CI-CT-CT-CT1   0.180   0.0-3.0
CI-CT-CT-CT1   0.250 180.0-2.0
CI-CT-CT-CT1   0.200 180.0 1.0
OS-P -OS-CI1   0.185181   31.79508-1.0  alfa
OS-P -OS-CI1   1.256531  351.95960-2.0  alfa
OS-P -OS-CI1   0.354858  357.24748 3.0  alfa
OH-P -OS-CI1   0.185181   31.79508-1.0  alfa
OH-P -OS-CI1   1.256531  351.95960-2.0  alfa
OH-P -OS-CI1   0.354858  357.24748 3.0  alfa
CT-CT-CI-OS1   1.178040  190.97653-1.0  gamma
CT-CT-CI-OS1   0.092102  295.63279-2.0  gamma
CT-CT-CI-OS1   0.962830  348.09535 3.0  gamma
CT-CT-CI-OH1   1.178040  190.97653-1.0  gamma
CT-CT-CI-OH1   0.092102  295.63279-2.0  gamma
CT-CT-CI-OH1   0.962830  348.09535 3.0  gamma

This is from my amberbsc0/ffbonded.itp:
;i  j   k  l func  phase  kd  pn
CT  OS  CT  CI40.00 0.38300-3; parmbsc0  Will 
Stebbeds
CT  OS  CT  CI4  180.00 0.1 2; parmbsc0  Will 
Stebbeds
H1  CI  CT  OS40.00 0.25000 1; parmbsc0  Will 
Stebbeds
H1  CI  CT  OH   40.00 0.25000 1; parmbsc0  Will 
Stebbeds
H1  CT  CI  OH   40.00 0.25000 1; parmbsc0  Will 
Stebbeds
CI  CT  CT  CT40.00 0.18000-3; parmbsc0  Will 
Stebbeds
CI  CT  CT  CT4  180.00 0.25000-2; parmbsc0  Will 
Stebbeds
CI  CT  CT  CT4  180.00 0.2 1; parmbsc0  Will 
Stebbeds
OS   P   OS  CI4   31.79 0.18518-1; parmbsc0  Will 
Stebbeds
OS   P   OS  CI4  351.96 1.25653-2; parmbsc0  Will 
Stebbeds
OS   P   OS  CI4  357.25 0.35486 3; parmbsc0  Will 
Stebbeds
OH  P   OS  CI4   31.79 0.18518-1; parmbsc0  Will 
Stebbeds
OH  P   OS  CI4  351.96 1.25653-2; parmbsc0  Will 
Stebbeds
OH  P   OS  CI4  357.25 0.35486 3; parmbsc0  Will 
Stebbeds
CT  CT  CI  OS4  190.98 1.17804-1; parmbsc0  Will 
Stebbeds
CT  CT  CI  OS4  295.63 0.09210-2; parmbsc0  Will 
Stebbeds
CT  CT  CI  OS4  348.09 0.96283 3; parmbsc0  Will 
Stebbeds
CT  CT  CI  OH   4  190.98 1.17804-1; parmbsc0  Will 
Stebbeds
CT  CT  CI  OH   4  295.63 0.09210-2; parmbsc0  Will 
Stebbeds
CT  CT  CI  OH   4  348.10 0.96283 3; parmbsc0  Will 
Stebbeds

;i   j   k   l   func
 X   CI  OS  X 9   0.0  1.15000 3  ; parmbsc0  Will 
Stebbeds
 X   CI  OH  X 9   0.0  0.5 3  ; parmbsc0  Will 
Stebbeds 
 X   CI  CT  X 9   0.0  1.4 3  ; PARMBSC0 --- Will 
Stebbeds 

As you can see func=1 was changed to func=4 and func=3 was changed to func=9.

This was the only way I could find in which the parameters would work, is it 
valid to make such alterations arbitrarily? The only other way it will work is 
if I comment out the repeated lines for the same 4 atoms.

Any help on this matter would be very much appreciated.

best regards

Will




 Date: Sat, 5 Feb 2011 12:23:32 -0500
 From: jalem...@vt.edu
 To: gmx-users@gromacs.org
 Subject: Re: [gmx-users] Porting Amber parmbsc0 force field to Gromacs
 
 
 
 william Stebbeds wrote:
  Hello,
  
  I would like to use the parmbs0 Amber forcefield to Gromacs, 
  specifically the nucleic acid parameters.
  
  Is this likely to come in a future release?
  
 
 Force fields are only implemented if a developer has a compelling reason to 
 do 
 so, and then take the time to validate it.  As such, new force fields are not 
 often introduced.
 
  I appreciate that this 

Re: [gmx-users] how many contacts has a certain atom at MD

2011-02-21 Thread Olga Ivchenko
So I used mindist for a certain group of molecules which is surrounded by
water. I got plot number of contacts versuc sumulation time. According to
what I see in a distance   0.6nm at certain frame there are on average 150
contacts.

Actually how the programm calculates the number of contacts, if someone
knows what is a creteria that a certain contact is formed?
Is is a certain distance.

best,
Olga

2011/2/21 Olga Ivchenko olga.ivche...@gmail.com

 Thank you very much.
 best,
 Olga

 2011/2/21 Justin A. Lemkul jalem...@vt.edu


 g_mindist -on (with suitable index groups) should also do the trick.

 -Justin


 Erik Marklund wrote:

 Or g_hbond -contact. Undfortuntely there are still issues with g_hbond at
 the moment. Version 4.0.x seem to work better.

 XAvier Periole skrev 2011-02-21 11.37:

 g_dist
 On Feb 21, 2011, at 11:32 AM, Olga Ivchenko wrote:

  Dear Gromacs Users,

 I would like to know if there is in gromacs an option how to calculate
 how many contacts has a certain atom i(n a molecules of interest) with 
 water
 during the whole MD simulations (or at each step of MD).
 Please could you advice me on this?

 best,
 Olga

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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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Re: [gmx-users] how many contacts has a certain atom at MD

2011-02-21 Thread Justin A. Lemkul



Olga Ivchenko wrote:
So I used mindist for a certain group of molecules which is surrounded 
by water. I got plot number of contacts versuc sumulation time. 
According to what I see in a distance   0.6nm at certain frame there 
are on average 150 contacts.


Actually how the programm calculates the number of contacts, if someone 
knows what is a creteria that a certain contact is formed?

Is is a certain distance.



Exactly as the title of the output says, a contact exists if any two atoms of 
the chosen index groups are within 0.6 nm.  You can change the distance with 
g_mindist -d.


-Justin


best,
Olga

2011/2/21 Olga Ivchenko olga.ivche...@gmail.com 
mailto:olga.ivche...@gmail.com


Thank you very much.
best,
Olga

2011/2/21 Justin A. Lemkul jalem...@vt.edu mailto:jalem...@vt.edu


g_mindist -on (with suitable index groups) should also do the trick.

-Justin


Erik Marklund wrote:

Or g_hbond -contact. Undfortuntely there are still issues
with g_hbond at the moment. Version 4.0.x seem to work better.

XAvier Periole skrev 2011-02-21 11.37:

g_dist
On Feb 21, 2011, at 11:32 AM, Olga Ivchenko wrote:

Dear Gromacs Users,

I would like to know if there is in gromacs an
option how to calculate how many contacts has a
certain atom i(n a molecules of interest) with water
during the whole MD simulations (or at each step of MD).
Please could you advice me on this?

best,
Olga

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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 http://vt.edu | (540) 231-9080
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin



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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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Re: [gmx-users] Target implementation date for gb_saltconc?

2011-02-21 Thread Per Larsson


Skickat från min iPhone

18 feb 2011 kl. 21:10 skrev Matthew Zwier mczw...@gmail.com:

 Dear GROMACS developers and users,
 
 Our research group is interested in performing GBSA simulations with
 GROMACS, but we would need to perform them with a nonzero salt
 concentration.  I was wondering if there are plans to implement the
 gb_saltconc parameter, and if so, when it might become available.
 
 Many thanks,
 Matt Zwier
 University of Pittsburgh
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[gmx-users] free energy-couple-intramol options

2011-02-21 Thread Moeed
Hello,

I read through the couple-intramol options (yes and no) good many times but
I can not still realize what is the difference and which option I should
select. I am having a hydrocarbon system (polyethylene in hexane as
solvent). Can anyone help me understand these options please? (in plain
english) option yes, says something about FF of large molecules which is my
case...but I dont see the statement: nb interactions might lead to
kinetically trapped vaccum conformations?!

Also, as with the electrostatics treatment in my hydrocarbon system I am
still unsure if I need to include electrostatics potentials. I digged into
the literature and found the following articles containing nonpolar polymers
where vdw is the only nonbonded term in the FF.

http://pubs.acs.org/doi/abs/10.1021/ma9600419

http://www.sciencedirect.com/science?_ob=ArticleURL_udi=B6TXW-40TY56F-16_user=458507_coverDate=11%2F30%2F2000_rdoc=1_fmt=high_orig=search_origin=search_sort=d_docanchor=view=c_searchStrId=1650178009_rerunOrigin=google_acct=C22002_version=1_urlVersion=0_userid=458507md5=bf0b74cfc76e0dafbadf06396fb63745searchtype=a

Please let me know your comments

Thanks
Moeed
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[gmx-users] diffusion constant

2011-02-21 Thread Rebeca García Fandiño

Hello,
I am trying to calculate the diffusion coefficient of a molecule in water using 
g_msd, and I have a doubt:
I get 3 different values when I use the trajectory directly from the 
simulation, the trajectory using PBC conditions, and the fitted trajectory.
Which would be the correct value for the diffusion coefficient?
Thanks a lot for your help in advance.
Best wishes,

Rebeca Garcia
Organic Chemistry Department
Santiago de Compostela University
Spain
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[gmx-users] PMF from pull code, unexpected results

2011-02-21 Thread Michael Brunsteiner

Dear all,

I would like to calculate the potential of mean force between two molecules 
in aqueous solution using the pull code. For a start i performed a number 
of calulations with a couple of very simple model systems with settings
loosely based on the example in the gmx tutorial section (see mdp file included
at the bottom). My box is 8x8x8 nm**3, pmf is calculated from some r_min up to 
approx 3.8 nm. Performing simulations with two t-buntanol molecules in implicit
solvent, anlyzing the output (x and f*.xvg files) with g_wham, i get rather
unexpected results:

The PMFs look very differnt depending on whether I use pulldim  Y Y Y 
or pulldim  N N Y:
http://www.brunsteiner.net/tbut-pmf.gif
Since we look at two neutral molecules with a permanent dipole
moment one would expect the PMF to be negative up to a distance
at which the two molecules come into contact, but with pulldim  Y Y Y
the PMF is positive, i.e., repulsive, throughout.

With pulldim  N N Y I constrain the two molecules in two
dimensions (by freezing the central atom in the x and y dimensions only,
BTW any ideas how else i could achieve that?)
One could argue that a combination of frozen atoms and pull code might be 
problematic, but i freeze and pull in different dimensions, so this should
be OK, and, more importantly: with pulldim  N N Y i get results that
look much more reasonable than with  pulldim  Y Y Y and NO additional 
constraints.

With pulldim  Y Y Y the RDF (option nolog in g_wahm) looks, in fact, 
like a NON-normalized rdf:
http://www.brunsteiner.net/tbut-rdf.gif
and, interestingly if i normalize it myself (by dividing through z**2 before
taking the logarithm) the resulting PMF looks much more reasonable.

Although what I see suggests that with pulldim  Y Y Y the RDF just doesn't
normalized properly, this issue seems to be more involved: 
Looking at the average forces and positions (the content of the f*xvg and x*xvg 
files)
http://www.brunsteiner.net/tbut-f.gif
http://www.brunsteiner.net/tbut-z.gif
suggests that there's already something wrong in the mdrun output
meaning that the problem is further upstream and not connected to anything
done by g_wham.

I repeated the calculations with an even simpler system (2 single atoms
that only interact via a LJ potential) to get qualitatively the same
results:
http://www.brunsteiner.net/2at-pmf.gif
http://www.brunsteiner.net/2at-rdf.gif
http://www.brunsteiner.net/2at-z.gif
http://www.brunsteiner.net/2at-f.gif

A few more remarks:
1) Convergence does not seem to be an issue here as i extended
some of the calculations to include 35+ windows, 2 ns each, and
the PMF remains the same nearly quantitatively.
2) The length of my reaction coordinates is always shorter
than half the box length.
3) I've compared calculations cut-off vs PME, to get very similar
results.
4) If I use pulldim  Y Y Y with no additional constraints but with
comm_mode = Angular i get results somewhere inbetween the two cases
above.

my specs:
Gromacs version: 4.5.3
Linux 2.6.35-23-generic Ubuntu x86_64
gcc version 4.4.5

I am not sure whether i overlooked something in my input,
or whether there's a problem with code.
I'd be grateful for any ideas/suggestions!

cheers,
Michael



=
mdp file:

integrator  = sd; this is better than md/NHT for systems with very 
few DOFs
tau_t   = 2.0 2.0
ref_t   = 290 290   ; a bit lower than 298 since sd with default 
parameters
; has problems controlling the temperature.
tc_grps = p1 p2 ; also tried System here, no difference
;
dt  = 0.002
tinit   = 0
nsteps  = 10; played with that, results seem to have converged
nstxout = 1000
nstvout = 0
nstfout = 1000
nstenergy   = 100
;
constraint_algorithm = lincs
constraints  = hbonds
continuation = no
;
comm_mode   = Linear
nstcomm = 1
pbc = xyz   ; also tried pbc = no same result
nstlist = 10
ns_type = grid 
rlist   = 4.0
rcoulomb= 4.0
rvdw= 4.0
;
coulombtype = Shift
vdwtype = Shift
epsilon_r   = 80
;
pull= umbrella
pull_geometry   = distance
pull_dim= N N Y   ; or Y Y Y
pull_start  = yes
pull_ngroups= 1
pull_group0 = p1
pull_group1 = p2
pull_rate1  = 0.0
pull_k1 = 500 ; i let this number vary depending on the pull 
distance;
; also played with the numbers, same result
pull_nstxout= 100
pull_nstfout= 100
pull_pbcatom0   = 1   ; my system geometry is so that the molecules 
never leave the box
pull_pbcatom1   = 16  ; or cross a cell boundary.
;
freezegrps  = c1 c2; with pulldim Y Y Y these lines are
freezedim   = Y Y N Y Y N  ; removed or commented out
;
energygrps  = p1 p2


  
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Re: [gmx-users] An argument about long range electrostatics

2011-02-21 Thread Justin A. Lemkul



Hassan Shallal wrote:

Dear Gromacs users,
 
While I was using Gromos force field in simulating a protein in explicit 
solvent, I used the following parameters:
 
*rcoulomb = 1, rlist =1, rvdw = 1.4*

*Electrostatitcs : PME*
*VDW : Twin range cutoff*
 
The above situation will not allow the calculation of any *long-range 
electrostatics (LR-Coul)* while calculating the energy of interaction 
among the specified energy groups of the the studied system.
 


Actually, you're calculating lots of long-range electrostatic interactions, but 
with PME it is the reciprocal space term, Coul-recip.


I am facing the question of to what extent that could affect the 
accuracy of the calculation of the energy of interaction among the 
specified energy groups of the the studied system.
 
I argue that electrostatic interaction is mainly composed of H-bonds and 
salt-bridges, both with distance cutoffs of 0.35 nm and 0.4 nm 
respectively. So there should not be any need for calculating any 
electrostatic interaction beyond 1 nm (rcoulomb).
 


If you maintain that all Coulombic interactions occur within 0.4 nm, why 
arbitrarily set a 1-nm cutoff?  By that logic, anything beyond 0.4 nm is 
unimportant.  Therein lies the flaw.  Electrostatic interactions decay over a 
longer range than do other interactions like van der Waals forces.  If an 
interaction at 1.0 nm is worth calculating, why is one at 1.001 nm completely 
unimportant?  Simple truncation leads to notable artifacts, which have been 
documented in the literature.  The first paragraph of the 1995 PME paper 
describes several.


On the other hand, I came across another argument that calculating the 
long range electrostatics is *complicated by the practical limitations 
of dividing lattice sum energies into energy groups*. I could not find 
any explanation of this point in the Gromacs manual! But I assume this 
kind of argument could be valid if ignoring the long range 
electrostatics would drastically affect the accuracy of interaction 
energy calculations mentioned above.


The manual is not a complete repository of all knowledge, but in conjunction 
with the 140 or so references therein, it comes pretty close ;)  The mesh term 
in the PME calculation cannot be decomposed pairwise, that much is true.  But 
the effects on the dynamics of the system when not calculating long-range 
electrostatics (i.e. plain cutoffs) is what is very troubling.  By all means, if 
you want to use the pinnacle of 1980's methodology, use a plain cutoff :)


In any case, the counterargument to yours played out in the literature long ago. 
 As I said, within the first few lines of the 1995 PME paper, you'll find lots 
of reasons to use a long-range electrostatics method.  There are several recent 
demonstrations that PME is the most accurate for a variety of systems.


-Justin

 
I would appreciate any feedback or comment concerning the above arguments.
 
Thanks a lot

Hassan
 



--


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] An argument about long range electrostatics

2011-02-21 Thread Hassan Shallal
Dear Gromacs users,
 
While I was using Gromos force field in simulating a protein in explicit 
solvent, I used the following parameters:
 
rcoulomb = 1, rlist =1, rvdw = 1.4
Electrostatitcs : PME
VDW : Twin range cutoff
 
The above situation will not allow the calculation of any long-range 
electrostatics (LR-Coul) while calculating the energy of interaction among the 
specified energy groups of the the studied system.
 
I am facing the question of to what extent that could affect the accuracy of 
the calculation of the energy of interaction among the specified energy groups 
of the the studied system.
 
I argue that electrostatic interaction is mainly composed of H-bonds and 
salt-bridges, both with distance cutoffs of 0.35 nm and 0.4 nm respectively. So 
there should not be any need for calculating any electrostatic interaction 
beyond 1 nm (rcoulomb). 
 
On the other hand, I came across another argument that calculating the long 
range electrostatics is complicated by the practical limitations of dividing 
lattice sum energies into energy groups. I could not find any explanation of 
this point in the Gromacs manual! But I assume this kind of argument could be 
valid if ignoring the long range electrostatics would drastically affect the 
accuracy of interaction energy calculations mentioned above.
 
I would appreciate any feedback or comment concerning the above arguments.
 
Thanks a lot
Hassan
 
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Re: [gmx-users] Can g_wham support using different temperature for different windows?

2011-02-21 Thread Justin A. Lemkul



Jianguo Li wrote:

Dear all,

I want to get the PMF of my peptide across the membrane bilayer. First I 
pulled my peptide across the membrane and then did windowed umbrella 
sampling along the reaction coordinates which is the z-distance between 
peptide and membrane. However, I found that sampling is not sufficient 
in some windows(e.g., around the center of the membrane). To enhance the 
sampling, I am thinking to run the simulation in those windows at higher 
temperature (e.g., 500K), but this will introduce a bias. My question 
is: can g_wham remove the bias due to using different temperatures in 
different windows?


If g_wham cannot deal with the bias due to using different T, I may need 
to do REMD in those windows. But that will be very expensive 
computationally. Anybody have an idea of enhancing sampling in those 
windows?


Btw, I am using Martini CG model.

Any suggestions will be highly appreciated, thank you!



A more straightforward approach is to (1) add more sampling windows or (2) 
increase the force constant in regions where there's poor sampling, or perhaps both.


-Justin


Cheers,
Jianguo



--


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] Can g_wham support using different temperature for different windows?

2011-02-21 Thread Jianguo Li
Dear all,

I want to get the PMF of my peptide across the membrane bilayer. First I pulled 
my peptide across the membrane and then did windowed umbrella sampling along 
the 
reaction coordinates which is the z-distance between peptide and membrane. 
However, I found that sampling is not sufficient  in some windows(e.g., around 
the center of the membrane). To enhance the sampling, I am thinking to run the 
simulation in those windows at higher temperature (e.g., 500K), but this will 
introduce a bias. My question is: can g_wham remove the bias due to using 
different temperatures in different windows? 


If g_wham cannot deal with the bias due to using different T, I may need to do 
REMD in those windows. But that will be very expensive computationally. Anybody 
have an idea of enhancing sampling in those windows?

Btw, I am using Martini CG model.

Any suggestions will be highly appreciated, thank you!

Cheers,
Jianguo


-- 
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Re: [gmx-users] Can g_wham support using different temperature for different windows?

2011-02-21 Thread Justin A. Lemkul



Jianguo Li wrote:

Thanks Justin.
I tried your suggestions by either increase more windows and change the 
force constant, but it seems the samplings are still bad in some 
windows. When I did pulling in (0 0 1) direction and a reverse pulling 
in (0 0 -1) direction, I got different configurations at certain 
reaction coordinates. And the windowed umbrella sampling seems depends 
strongly on the initial configurations in that window. Therefore I got 
different PMFs using pulling in (0 0 1) direction and reverse pulling in 
(0 0 -1) direction.




How long are each of the simulations in each window?  Sufficient sampling should 
eliminate any configurational bias and/or hysteresis.  Also, if the pulling that 
sets up the initial configurations is done slowly enough, you won't see these 
problems.  Sounds to me like you're pulling too fast or hard, such that the 
system is not stable.


In my simulation, I exert constraints on phosphate atoms in z direction, 
so there is no lipid flip-flop and the membrane will be stable at high 
temperatures. Then I am thinking of increasing temperature in those bad 
windows to enhance sampling...




I don't know if I can make a convincing argument here, but intuitively, these 
windows would be sampling in a different ensemble, so the free energy landscape 
in these windows would be discontinuous with any adjacent windows that are done 
at different temperatures, and perhaps the forces required to restrain your 
peptide at a given COM distance will still result in a discontinuous PMF.  I 
would also suspect that g_wham can't handle this situation; it has a -temp flag, 
but it only takes one value.  So if you construct your PMF curve using WHAM, but 
supply incorrect or inconsistent information, I certainly wouldn't believe the 
result.


I guess the main point is, there are tons of published demonstrations of 
peptides and other molecules crossing a membrane with SMD and umbrella sampling, 
so it should be possible to generate stable configurations without any funny tricks.


-Justin


best regards,
Jianguo




*From:* Justin A. Lemkul jalem...@vt.edu
*To:* Discussion list for GROMACS users gmx-users@gromacs.org
*Sent:* Tuesday, 22 February 2011 09:35:37
*Subject:* Re: [gmx-users] Can g_wham support using different 
temperature for different windows?




Jianguo Li wrote:
  Dear all,
 
  I want to get the PMF of my peptide across the membrane bilayer. 
First I pulled my peptide across the membrane and then did windowed 
umbrella sampling along the reaction coordinates which is the z-distance 
between peptide and membrane. However, I found that sampling is not 
sufficient in some windows(e.g., around the center of the membrane). To 
enhance the sampling, I am thinking to run the simulation in those 
windows at higher temperature (e.g., 500K), but this will introduce a 
bias. My question is: can g_wham remove the bias due to using different 
temperatures in different windows?

 
  If g_wham cannot deal with the bias due to using different T, I may 
need to do REMD in those windows. But that will be very expensive 
computationally. Anybody have an idea of enhancing sampling in those 
windows?

 
  Btw, I am using Martini CG model.
 
  Any suggestions will be highly appreciated, thank you!
 

A more straightforward approach is to (1) add more sampling windows or 
(2) increase the force constant in regions where there's poor sampling, 
or perhaps both.


-Justin

  Cheers,
  Jianguo
 

-- 

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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--


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] ffamber03 RB dihedrals and amb2gmx.pl problem!

2011-02-21 Thread gromacs564
Hello all
  I obtained a top file after running the amb2gmx.pl script,but I feel some 
errors in this top file.
The functype of the [dihedral] is 3 in this top file,but the [pairs] part aslo 
presence in it. And the
manual is point that with the Ryckaert-Bellemans potential the 1-4 
interactions must be excluded
from the non-bonded list. So I think this top file is incorrect?
  Force field is amber03 in gmx4.5.1,ligand is disaccharide.
Thanks !
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[gmx-users] PMF from pull code, unexpected results

2011-02-21 Thread chris . neale
Looking at http://www.brunsteiner.net/tbut-pmf.gif you seem to be  
getting exactly what I would expect. The difference is the entropy  
term. Note that the spherical shell increases volume as r increases  
for pulldim YYY but this effect is absent for pulldim NNY. This is why  
you can correct as per an RDF.


Please note that I didn;t check everything thoroughly or look at the  
other images so there could still be something weird going on, but I  
disagree that http://www.brunsteiner.net/tbut-pmf.gif shows anything  
strange.


Chris.

-- original message --


Dear all,

I would like to calculate the potential of mean force between two molecules
in aqueous solution using the pull code. For a start i performed a number
of calulations with a couple of very simple model systems with settings
loosely based on the example in the gmx tutorial section (see mdp file  
included

at the bottom). My box is 8x8x8 nm**3, pmf is calculated from some r_min up to
approx 3.8 nm. Performing simulations with two t-buntanol molecules in  
implicit

solvent, anlyzing the output (x and f*.xvg files) with g_wham, i get rather
unexpected results:

The PMFs look very differnt depending on whether I use pulldim  Y Y Y
or pulldim  N N Y:
http://www.brunsteiner.net/tbut-pmf.gif
Since we look at two neutral molecules with a permanent dipole
moment one would expect the PMF to be negative up to a distance
at which the two molecules come into contact, but with pulldim  Y Y Y
the PMF is positive, i.e., repulsive, throughout.

With pulldim  N N Y I constrain the two molecules in two
dimensions (by freezing the central atom in the x and y dimensions only,
BTW any ideas how else i could achieve that?)
One could argue that a combination of frozen atoms and pull code might be
problematic, but i freeze and pull in different dimensions, so this should
be OK, and, more importantly: with pulldim  N N Y i get results that
look much more reasonable than with  pulldim  Y Y Y and NO additional
constraints.

With pulldim  Y Y Y the RDF (option nolog in g_wahm) looks, in fact,
like a NON-normalized rdf:
http://www.brunsteiner.net/tbut-rdf.gif
and, interestingly if i normalize it myself (by dividing through z**2 before
taking the logarithm) the resulting PMF looks much more reasonable.

Although what I see suggests that with pulldim  Y Y Y the RDF just doesn't
normalized properly, this issue seems to be more involved:
Looking at the average forces and positions (the content of the f*xvg  
and x*xvg

files)
http://www.brunsteiner.net/tbut-f.gif
http://www.brunsteiner.net/tbut-z.gif
suggests that there's already something wrong in the mdrun output
meaning that the problem is further upstream and not connected to anything
done by g_wham.

I repeated the calculations with an even simpler system (2 single atoms
that only interact via a LJ potential) to get qualitatively the same
results:
http://www.brunsteiner.net/2at-pmf.gif
http://www.brunsteiner.net/2at-rdf.gif
http://www.brunsteiner.net/2at-z.gif
http://www.brunsteiner.net/2at-f.gif

A few more remarks:
1) Convergence does not seem to be an issue here as i extended
some of the calculations to include 35+ windows, 2 ns each, and
the PMF remains the same nearly quantitatively.
2) The length of my reaction coordinates is always shorter
than half the box length.
3) I've compared calculations cut-off vs PME, to get very similar
results.
4) If I use pulldim  Y Y Y with no additional constraints but with
comm_mode = Angular i get results somewhere inbetween the two cases
above.

my specs:
Gromacs version: 4.5.3
Linux 2.6.35-23-generic Ubuntu x86_64
gcc version 4.4.5

I am not sure whether i overlooked something in my input,
or whether there's a problem with code.
I'd be grateful for any ideas/suggestions!

cheers,
Michael



=
mdp file:

integrator  = sd; this is better than md/NHT for systems with very
few DOFs
tau_t   = 2.0 2.0
ref_t   = 290 290   ; a bit lower than 298 since sd with default
parameters
; has problems controlling the temperature.
tc_grps = p1 p2 ; also tried System here, no difference
;
dt  = 0.002
tinit   = 0
nsteps  = 10; played with that, results seem to have converged
nstxout = 1000
nstvout = 0
nstfout = 1000
nstenergy   = 100
;
constraint_algorithm = lincs
constraints  = hbonds
continuation = no
;
comm_mode   = Linear
nstcomm = 1
pbc = xyz   ; also tried pbc = no same result
nstlist = 10
ns_type = grid
rlist   = 4.0
rcoulomb= 4.0
rvdw= 4.0
;
coulombtype = Shift
vdwtype = Shift
epsilon_r   = 80
;
pull= umbrella
pull_geometry   = distance
pull_dim= N N Y   ; or Y Y Y
pull_start  = yes
pull_ngroups= 1
pull_group0 = p1
pull_group1 = p2
pull_rate1  = 0.0
pull_k1 = 500 ; i let this number 

Re: [gmx-users] Can g_wham support using different temperature for different windows?

2011-02-21 Thread Jianguo Li
Thanks for your comments, Justin.

Using timestep of 20 fs, in each window the simulation runs for 100 ns CG time. 
The pulling rate is 0.001 nm/ps. Is it too fast?

My system is a little different. My peptide is highly positively charged. The 
NMR experiments show that the conformation of the peptide in water is very 
dynamic, so I make it flexible without fixing any secondary structure in 
Martini 
model. 

In the membrane, 25% of the lipids are negatively charged, so there are very 
strong electrostatic attraction between peptides and membrane.


During the peptide approaching the membrane from the top, peptide can take 
different configurations at different reaction coordinates. When pulling the 
peptide into the membrane, the peptide takes relatively compact structure and 
interacts with only the top leaflet until the distance becomes smaller than 
0.45 
nm, after that the peptide becomes extended structure and interacts with both 
leaflets. This extended structure remains until the distance becomes -1.05 nm. 
Further pulling leads to compact structure and interacts only with the lower 
leaflet. So the comformation of the peptide is not symmetric between the center 
of the bilayer, which leads to  Hysteresis. It seems that there is a huge 
energy 
barrier for the peptide to translocate across the membrane because if the 
initial conformation in a certain window is extended (interacting with both 
leaflets), then it remains extended. Similarly, it the initial conformation in 
a 
certain window is compact (interacting with only one leaflet), it will remain 
compact.

Any Suggestions of dealing with the highly charged system?

Cheers,
Jianguo





From: Justin A. Lemkul jalem...@vt.edu
To: Gromacs Users' List gmx-users@gromacs.org
Sent: Tuesday, 22 February 2011 09:58:36
Subject: Re: [gmx-users] Can g_wham support using different temperature for 
different windows?



Jianguo Li wrote:
 Thanks Justin.
 I tried your suggestions by either increase more windows and change the force 
constant, but it seems the samplings are still bad in some windows. When I did 
pulling in (0 0 1) direction and a reverse pulling in (0 0 -1) direction, I 
got 
different configurations at certain reaction coordinates. And the windowed 
umbrella sampling seems depends strongly on the initial configurations in that 
window. Therefore I got different PMFs using pulling in (0 0 1) direction and 
reverse pulling in (0 0 -1) direction.
 

How long are each of the simulations in each window?  Sufficient sampling 
should 
eliminate any configurational bias and/or hysteresis.  Also, if the pulling 
that 
sets up the initial configurations is done slowly enough, you won't see these 
problems.  Sounds to me like you're pulling too fast or hard, such that the 
system is not stable.

 In my simulation, I exert constraints on phosphate atoms in z direction, so 
there is no lipid flip-flop and the membrane will be stable at high 
temperatures. Then I am thinking of increasing temperature in those bad 
windows 
to enhance sampling...
 

I don't know if I can make a convincing argument here, but intuitively, these 
windows would be sampling in a different ensemble, so the free energy landscape 
in these windows would be discontinuous with any adjacent windows that are done 
at different temperatures, and perhaps the forces required to restrain your 
peptide at a given COM distance will still result in a discontinuous PMF.  I 
would also suspect that g_wham can't handle this situation; it has a -temp 
flag, 
but it only takes one value.  So if you construct your PMF curve using WHAM, 
but 
supply incorrect or inconsistent information, I certainly wouldn't believe the 
result.

I guess the main point is, there are tons of published demonstrations of 
peptides and other molecules crossing a membrane with SMD and umbrella 
sampling, 
so it should be possible to generate stable configurations without any funny 
tricks.

-Justin

 best regards,
 Jianguo
 
 
 
 
 *From:* Justin A. Lemkul jalem...@vt.edu
 *To:* Discussion list for GROMACS users gmx-users@gromacs.org
 *Sent:* Tuesday, 22 February 2011 09:35:37
 *Subject:* Re: [gmx-users] Can g_wham support using different temperature for 
different windows?
 
 
 
 Jianguo Li wrote:
   Dear all,
  
   I want to get the PMF of my peptide across the membrane bilayer. First I 
pulled my peptide across the membrane and then did windowed umbrella sampling 
along the reaction coordinates which is the z-distance between peptide and 
membrane. However, I found that sampling is not sufficient in some 
windows(e.g., 
around the center of the membrane). To enhance the sampling, I am thinking to 
run the simulation in those windows at higher temperature (e.g., 500K), but 
this 
will introduce a bias. My question is: can g_wham remove the bias due to using 
different temperatures in different windows?
  
   If 

Re: [gmx-users] Can g_wham support using different temperature for different windows?

2011-02-21 Thread Justin A. Lemkul



Jianguo Li wrote:

Thanks for your comments, Justin.

Using timestep of 20 fs, in each window the simulation runs for 100 ns 
CG time. The pulling rate is 0.001 nm/ps. Is it too fast?




Let me clarify things, since I'm not convinced I understand your procedure.
You generate a series of configurations with 0.001 nm/ps pulling, but then how 
many windows do you generate for independent simulations?  What are your .mdp 
parameters during those windows?  The pull rate should be 0 during the actual 
umbrella sampling, to restrain the peptide within the window.  What force 
constant(s) do you use?


My system is a little different. My peptide is highly positively 
charged. The NMR experiments show that the conformation of the peptide 
in water is very dynamic, so I make it flexible without fixing any 
secondary structure in Martini model.


As was discussed in the last few days, do not interpret changes in structure too 
directly when using MARTINI.  It is not designed to faithfully mimic secondary 
structure changes.


In the membrane, 25% of the lipids are negatively charged, so there are 
very strong electrostatic attraction between peptides and membrane.


During the peptide approaching the membrane from the top, peptide can 
take different configurations at different reaction coordinates. When 
pulling the peptide into the membrane, the peptide takes relatively 
compact structure and interacts with only the top leaflet until the 
distance becomes smaller than 0.45 nm, after that the peptide becomes 
extended structure and interacts with both leaflets. This extended 
structure remains until the distance becomes -1.05 nm. Further pulling 
leads to compact structure and interacts only with the lower leaflet. So 
the comformation of the peptide is not symmetric between the center of 
the bilayer, which leads to  Hysteresis. It seems that there is a huge 


I guess I'm confused here, too.  The peptide is compact when interacting with 
the top leaflet, extended further in the membrane, then compact again when 
interacting with the lower leaflet.  What's strange about that?


energy barrier for the peptide to translocate across the membrane 
because if the initial conformation in a certain window is extended 
(interacting with both leaflets), then it remains extended. Similarly, 
it the initial conformation in a certain window is compact (interacting 
with only one leaflet), it will remain compact.




I don't see how that is necessarily unexpected or problematic.  Peptides will 
change conformation depending on their environment.  If you want a static 
structure to cross the membrane (which may or may not represent reality) you'll 
have to introduce some kind of intramolecular restraints.


-Justin


Any Suggestions of dealing with the highly charged system?

Cheers,
Jianguo



*From:* Justin A. Lemkul jalem...@vt.edu
*To:* Gromacs Users' List gmx-users@gromacs.org
*Sent:* Tuesday, 22 February 2011 09:58:36
*Subject:* Re: [gmx-users] Can g_wham support using different 
temperature for different windows?




Jianguo Li wrote:
  Thanks Justin.
  I tried your suggestions by either increase more windows and change 
the force constant, but it seems the samplings are still bad in some 
windows. When I did pulling in (0 0 1) direction and a reverse pulling 
in (0 0 -1) direction, I got different configurations at certain 
reaction coordinates. And the windowed umbrella sampling seems depends 
strongly on the initial configurations in that window. Therefore I got 
different PMFs using pulling in (0 0 1) direction and reverse pulling in 
(0 0 -1) direction.

 

How long are each of the simulations in each window?  Sufficient 
sampling should eliminate any configurational bias and/or hysteresis.  
Also, if the pulling that sets up the initial configurations is done 
slowly enough, you won't see these problems.  Sounds to me like you're 
pulling too fast or hard, such that the system is not stable.


  In my simulation, I exert constraints on phosphate atoms in z 
direction, so there is no lipid flip-flop and the membrane will be 
stable at high temperatures. Then I am thinking of increasing 
temperature in those bad windows to enhance sampling...

 

I don't know if I can make a convincing argument here, but intuitively, 
these windows would be sampling in a different ensemble, so the free 
energy landscape in these windows would be discontinuous with any 
adjacent windows that are done at different temperatures, and perhaps 
the forces required to restrain your peptide at a given COM distance 
will still result in a discontinuous PMF.  I would also suspect that 
g_wham can't handle this situation; it has a -temp flag, but it only 
takes one value.  So if you construct your PMF curve using WHAM, but 
supply incorrect or inconsistent information, I certainly wouldn't 
believe the result.


I guess the main point is, there are tons of published 

[gmx-users] Can g_wham support using different temperature for different windows?

2011-02-21 Thread chris . neale
Sounds like unconverged sampling. You would be astounded how long  
systems like this can take to converge. An all-atom simulation like  
this can easily require 10 us (microseconds!) per umbrella. I don't  
know about martini, probably a lot less.


Chris.

-- original message --

Thanks Justin.
I tried your suggestions by either increase more windows and change the force
constant, but it seems the samplings are still bad in some windows. When I did
pulling in (0 0 1) direction and a reverse pulling in (0 0 -1)  
direction, I got

different configurations at certain reaction coordinates. And the windowed
umbrella sampling seems depends strongly on the initial configurations in that
window. Therefore I got different PMFs using pulling in (0 0 1) direction and
reverse pulling in ?0 0 -1) direction.


In my simulation, I exert constraints on phosphate atoms in z direction, so
there is no lipid flip-flop and the membrane will be stable at high
temperatures. Then I am thinking of increasing temperature in those  
bad windows

to enhance sampling...

best regards,
Jianguo





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[gmx-users] membrane bilayer simulation by OPLS FF

2011-02-21 Thread mircial

Dear All:

I am using OPLS force field (OPLS FF) to do molecular dynamics  
simulations. My system contains DPPC lipid, protein and a small  
molecule. I have the following questions:


1, where can I get the topology files for the DPPC lipids?

2, How to prepare the topology files for the small molecules? I plan  
to calculate the charges of each atoms by QM method.After I got the  
charges and atom radius, how to prepare the topology files?


3, I am using GROMACS 3 and I found there are three all-atom force  
fields there:

--
 0: GROMOS96 43a1 force field
 1: GROMOS96 43b1 vacuum force field
 2: GROMOS96 43a2 force field (improved alkane dihedrals)
 3: GROMOS96 45a3 force field (Schuler JCC 2001 22 1205)
 4: GROMOS96 53a5 force field (JCC 2004 vol 25 pag 1656)
 5: GROMOS96 53a6 force field (JCC 2004 vol 25 pag 1656)
 6: OPLS-AA/L all-atom force field (2001 aminoacid dihedrals)
 7: Encad all-atom force field, using scaled-down vacuum charges
 8: Encad all-atom force field, using full solvent charges
-

among them, 6, 7, and 8 are all-atom force fields, right? My question  
is are 7 and 8 also OPLS force fields? If so, which one is  
recommendated to use in lipid-protein complex systems MD simulations?  
What are the differences between 6, 7 and 8.


Sincerely Yours

Ruo-Xu Gu


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[gmx-users] %exist hydrogen bond

2011-02-21 Thread leila karami
Dear Justin

My simulation system contains protein, dna and water.
I used your script already for obtaining %exist hydrogen bonds between
protein and dna:

#!/usr/bin/perl

#
# plot_hbmap.pl - plot the probability of finding a particular hydrogen bond
# based on several input files:
#   1. coordinate file (for atom naming) - MUST be a .pdb file with NO CHAIN
#IDENTIFIERS
#   2. hbmap.xpm
#   3. hbond.ndx (modified to contain only the atom numbers in the [hbonds...]
#section, nothing else)
#
use strict;
unless(@ARGV) {
 die Usage: perl $0 -s structure.pdb -map hbmap.xpm -index hbond.ndx\n;
.
.
.
.
It worked good and output file (summary_Hbmap.dat) was as follows:

#DonorAcceptor  % Exist.
 0.000
  NGL1   NDT64  O4   1.195
  NGL1   NDT82  O4   0.797
 ARG57 NH2DA79 O1P  19.920
 ARG57 NH2DA80 O1P   0.797
 ARG57 NH2DA80 O2P  16.335
 ARG57 NH1DA80 O2P  43.426

Now I want to use your script for obtaining %exist hydrogen bonds
between protein and water molecules, but output file
(summary_Hbmap.dat) is as follows:

#DonorAcceptor  % Exist.
  NGL1   N   0.160
 ARG58 NH2   0.400
 ARG58 NH2  43.565
 ARG58 NH1   1.839
 ARG58 NH1   0.080
 ARG58 NH1  21.663


What is problem?
Please guide me about that.






-- 


Leila Karami
Ph.D. student of Physical Chemistry
K.N. Toosi University of Technology
Theoretical Physical Chemistry Group
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RE: [gmx-users] membrane bilayer simulation by OPLS FF

2011-02-21 Thread Dallas Warren
7 and 8 have nothing to do with OPLS-AA.

As the text tells you, it is the Encad forcefield
(http://www.sklogwiki.org/SklogWiki/index.php/ENCAD_%28force_field%29)

So that then leaves you with the OPLS-AA for you to use :-)

Catch ya,

Dr. Dallas Warren
Medicinal Chemistry and Drug Action
Monash Institute of Pharmaceutical Sciences, Monash University
381 Royal Parade, Parkville VIC 3010
dallas.war...@monash.edu
+61 3 9903 9304
-
When the only tool you own is a hammer, every problem begins to resemble
a nail. 


 -Original Message-
 From: gmx-users-boun...@gromacs.org [mailto:gmx-users-
 boun...@gromacs.org] On Behalf Of mirc...@sjtu.edu.cn
 Sent: Tuesday, 22 February 2011 4:18 PM
 To: gmx-users@gromacs.org
 Subject: [gmx-users] membrane bilayer simulation by OPLS FF
 
 Dear All:
 
 I am using OPLS force field (OPLS FF) to do molecular dynamics
 simulations. My system contains DPPC lipid, protein and a small
 molecule. I have the following questions:
 
 1, where can I get the topology files for the DPPC lipids?
 
 2, How to prepare the topology files for the small molecules? I plan
 to calculate the charges of each atoms by QM method.After I got the
 charges and atom radius, how to prepare the topology files?
 
 3, I am using GROMACS 3 and I found there are three all-atom force
 fields there:
 --
   0: GROMOS96 43a1 force field
   1: GROMOS96 43b1 vacuum force field
   2: GROMOS96 43a2 force field (improved alkane dihedrals)
   3: GROMOS96 45a3 force field (Schuler JCC 2001 22 1205)
   4: GROMOS96 53a5 force field (JCC 2004 vol 25 pag 1656)
   5: GROMOS96 53a6 force field (JCC 2004 vol 25 pag 1656)
   6: OPLS-AA/L all-atom force field (2001 aminoacid dihedrals)
   7: Encad all-atom force field, using scaled-down vacuum charges
   8: Encad all-atom force field, using full solvent charges
 -
 
 among them, 6, 7, and 8 are all-atom force fields, right? My question
 is are 7 and 8 also OPLS force fields? If so, which one is
 recommendated to use in lipid-protein complex systems MD simulations?
 What are the differences between 6, 7 and 8.
 
 Sincerely Yours
 
 Ruo-Xu Gu
 
 
 --
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 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at
 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
 Please don't post (un)subscribe requests to the list. Use the
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 Can't post? Read http://www.gromacs.org/Support/Mailing_Lists
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[gmx-users] diffusion coefficients

2011-02-21 Thread Thomas Koller
Hello,

I'm investigating the diffusion coefficient of gases in liquids. Therefore, I 
insert some molecules with the genbox tool in an equilibrated system. After a 
NPT run to adjust the density, I'm running an NVT simulation to calculate the 
diffusion coefficient (g_msd). MSD of the liquids are quite linear, but the gas 
MSDs show sometime fluctuations, even with negative slopes within the run. What 
can be the problem or is this strategy right?

Regards,
Thomas
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Re: [gmx-users] Can g_wham support using different temperature for different windows?

2011-02-21 Thread Jianguo Li
Thanks Justin and Chris and sorry for confusing interpretation.
Let me make it more clear. My peptide is flexible Martini beads, and highly 
positively charged. My membrane is a mixture of negatively charged lipids (25%) 
and zitterionic lipids(75%). So there is strong electrostatic attraction 

between peptide and membrane. To get the PMF, I did the following:

(1) I did pulling simulation along (0 0 -1) direction to pull my peptide across 
the membrane. Then I got different configurations corresponding to different 
windows along the reaction coordinates, which is the z-distance 

between peptide and membrane. This figure 
(http://www.flickr.com/photos/lijg/5467080971/) shows some of the 
configurations 
at certain reaction coordinates.

(2) In each window, I used the corresponding configuration that generated by 
the 
pulling simulation as initial input and run umbrella sampling. The size of each 
window is 0.15 nm, but close to the bilayer cneter (e.g., -0.6d0.6), I have 

increased number of windows so that the width of the window is to be 0.05 or 
0.1 
nm, I also tried to use different force constant in these windows.

From the figure (http://www.flickr.com/photos/lijg/5467080971/) , we can 
classify the peptide conformation to be either extended (interacting with two 
bilayers) or compact (interacting with only one bilayer). Ideally, the peptide 
conformation should be similar for d=x and d=-x. The problem is that the 
configuration of peptide is not symmetric with respect to the bilayer center. 
For example, the peptide configuration is compact at d=0.6 and d=0.9, but the 
peptide is extended at d=-0.6 and d=-0.9. This leads Hysteresis. If I use 
g_wham 
to generate PMF, then the PMF is not symmetric with respect to the bilayer 
center. Using more number of windows and different force constant did not 
remove 
the problem.

In my opinion,  at least in some windows, the peptide should sample both 
compact 
and extended structure. But what I found is that the windowed umbrella 
simulation depends on the initial peptide conformation. If the initial peptide 
conformation is compact, then after 100 ns, it is still compact; if the initial 
peptide in that window is extended, the final configuration is also extended. I 
also tried to run longer equilibrium time (e.g., 200 ns), but the problem still 
exists.

My question is how to increase sampling of the peptide conformation? I just 
think of two choices:
(1) use high temperature (e.g., 500K) at those bad windows. As I mentioned, I 
am 
wondering if g_wham can unbias the effect of using different temperatures in 
different windows.
(2) use REMD in those bad windows. These need a lot of computational resources.

Is there any other method to deal with the insufficient sampling?
Any suggestions are welcome, thanks for your time reading this email!

Cheers,
Jianguo






From: Justin A. Lemkul jalem...@vt.edu
To: Gromacs Users' List gmx-users@gromacs.org
Sent: Tuesday, 22 February 2011 11:13:05
Subject: Re: [gmx-users] Can g_wham support using different temperature for 
different windows?



Jianguo Li wrote:
 Thanks for your comments, Justin.
 
 Using timestep of 20 fs, in each window the simulation runs for 100 ns CG 
 time. 
The pulling rate is 0.001 nm/ps. Is it too fast?
 

Let me clarify things, since I'm not convinced I understand your procedure.
You generate a series of configurations with 0.001 nm/ps pulling, but then how 
many windows do you generate for independent simulations?  What are your .mdp 
parameters during those windows?  The pull rate should be 0 during the actual 
umbrella sampling, to restrain the peptide within the window.  What force 
constant(s) do you use?

 My system is a little different. My peptide is highly positively charged. The 
NMR experiments show that the conformation of the peptide in water is very 
dynamic, so I make it flexible without fixing any secondary structure in 
Martini 
model.

As was discussed in the last few days, do not interpret changes in structure 
too 
directly when using MARTINI.  It is not designed to faithfully mimic secondary 
structure changes.

 In the membrane, 25% of the lipids are negatively charged, so there are very 
strong electrostatic attraction between peptides and membrane.
 
 During the peptide approaching the membrane from the top, peptide can take 
different configurations at different reaction coordinates. When pulling the 
peptide into the membrane, the peptide takes relatively compact structure and 
interacts with only the top leaflet until the distance becomes smaller than 
0.45 
nm, after that the peptide becomes extended structure and interacts with both 
leaflets. This extended structure remains until the distance becomes -1.05 nm. 
Further pulling leads to compact structure and interacts only with the lower 
leaflet. So the comformation of the peptide is not symmetric between the 
center 
of the bilayer, which leads to  Hysteresis. It seems