[gmx-users] Re: CHARMM36 force field available for GROMACS

2013-10-09 Thread ABEL Stephane 175950
Hello Justin, 

Two quick questions, here 

- Since the lipid charmm36 parameters for lipids are already available in the 
gromacs format on the GROMACS website  (charmm36.ff_4.5.4_ref.tgz) from thomas 
Piggot. Does it means that these files are considered as deprecated and all the 
users are invited to use in their simulations the CHARMM -GROMACS official 
release from you ?

- Did you compare the results for the common molecules, to see if some 
errors/typos in charmm36.ff_4.5.4_ref.tgz were presents ?

Stephane   

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[gmx-users] RE : gmx-users Digest, Vol 114, Issue 21

2013-10-09 Thread ABEL Stephane 175950
OK thank you four kind response. And also thank you and the CHARMM team for 
this geat job. 

Stephane
---

On 10/9/13 11:28 AM, ABEL Stephane 175950 wrote:
 Hello Justin,

 Two quick questions, here

 - Since the lipid charmm36 parameters for lipids are already available in the 
 gromacs format on the GROMACS website  (charmm36.ff_4.5.4_ref.tgz) from 
 thomas Piggot. Does it means that these files are considered as deprecated 
 and all the users are invited to use in their simulations the CHARMM -GROMACS 
 official release from you ?


AFAIK, the charmm36.ff_4.5.4_ref.tgz only contains updated CHARMM36 lipids and
nothing else.  Someone please correct me if I am wrong here, but a quick scan
through that archive indicated to me that the force fields for other molecules
(proteins, nucleic acids, etc) were outdated.

Thus, I feel that our new distribution supersedes the available files because
what is contained there is not what we consider the CHARMM36 force field in its
entirety.  Users are welcome to use whatever they like, but our distribution is
the only one (to our knowledge) that is equivalent to the current force field
set distributed with CHARMM and does contain an important reparametrization of
the CMAP terms that go along with what we call the CHARMM36 protein force field,
which is probably of particular interest to this community.

 - Did you compare the results for the common molecules, to see if some 
 errors/typos in charmm36.ff_4.5.4_ref.tgz were presents ?


We did not look into any errors or typos in other distributions.  We created our
files completely on our own directly from existing CHARMM force field files, not
based on anything found in charmm36.ff_4.5.4_ref.tgz.

-Justin

--
==

Justin A. Lemkul, Ph.D.
Postdoctoral Fellow

Department of Pharmaceutical Sciences
School of Pharmacy
Health Sciences Facility II, Room 601
University of Maryland, Baltimore
20 Penn St.
Baltimore, MD 21201

jalem...@outerbanks.umaryland.edu | (410) 706-7441

==

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[gmx-users] script to convert the TIP3P water model into TIP4P

2013-09-23 Thread ABEL Stephane 175950
Hello all, 

It is not a gromacs problem per se, but I hope that some gromacs users can 
help me. I would to do simulations of phospholipid bilayers with the TIP4P/2005 
water model. I have downloaded in the Klauda's website several bilayer starting 
conformations. However, since CHARMM uses the TIP3 water model, I am confused 
to convert the water coordinates into a water four sites. Does somebody has a 
little script to share with me that can help me?

Thank you for kindly help 

Stephane
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[gmx-users] script to convert the TIP3P water model into TIP4

2013-09-23 Thread ABEL Stephane 175950
Hello,

Because I want to compare the simulation results (essentially water dynamic) 
with previous simulations of reverse micelles, micelles carried out with the 
same water model. 

Stephane


--

Message: 8
Date: Mon, 23 Sep 2013 10:45:56 +0200
From: Dr. Vitaly Chaban vvcha...@gmail.com
Subject: Re: [gmx-users] script to convert the TIP3P water model into
TIP4P
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID:
capxdd+alyfc4g+wnzj7bk0+rj3eexj_js7stjtdwymayt5t...@mail.gmail.com
Content-Type: text/plain; charset=ISO-8859-1

I am confused. Why do you want 4-sites water?


Dr. Vitaly V. Chaban


On Mon, Sep 23, 2013 at 10:36 AM, ABEL Stephane 175950
stephane.a...@cea.fr wrote:
 Hello all,

 It is not a gromacs problem per se, but I hope that some gromacs users can 
 help me. I would to do simulations of phospholipid bilayers with the 
 TIP4P/2005 water model. I have downloaded in the Klauda's website several 
 bilayer starting conformations. However, since CHARMM uses the TIP3 water 
 model, I am confused to convert the water coordinates into a water four 
 sites. Does somebody has a little script to share with me that can help me?

 Thank you for kindly help

 Stephane
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[gmx-users] script to convert the TIP3P water model into TIP4(P)/2005

2013-09-23 Thread ABEL Stephane 175950
Hello Justin,

Thank you for your response and your interest for my simulations ;) I am of 
course aware that the primary water model for the CHARMM is the TIP3(S)P 
model. 

Since, I am mainly interested to the water dynamic around DOPC molecules in the 
context of the different water/DOPC mesophases (not data available, I currently 
doing the tests ;)) and that it is known that the TIP4P/2005 water model (it is 
the model, I want to use) reproduces better the water dynamic and structure 
than the TIP3P water model, I would like to test if the TIP4P/2005 water can be 
used in simulation of membranes. I am not aware that somebody have already done 
the test. 

Finally, Justin, you are probably right here, the results will be probably not 
good as it is suggested by Pastor and MacKerell in their paper for TIP4P-EW 
water model [1], but I think that it is worth a test to confirm this in case of 
the TIP4P/2005. I am not the first one to ask this question in the context of 
simulations with the CHARMM force field (for protein, here [2]).

[1] www.ncbi.nlm.nih.gov/pmc/articles/PMC3133452/
[2]  Nutt, D. R.; Smith, J. C. Molecular Dynamics Simulations of Proteins: Can 
the Explicit Water Model Be Varied? J. Chem. Theory Comput. 2007, 3, 1550–1560.

Stephane


On 9/23/13 5:02 AM, ABEL Stephane 175950 wrote:
 Hello,

 Because I want to compare the simulation results (essentially water dynamic) 
 with previous simulations of reverse micelles, micelles carried out with the 
 same water model.


The math for producing the virtual site in TIP4P is described in tip4p.itp, so
you can use that.  What's more curious is that if a paper claims to use TIP4P
but the provided files use TIP3P, then either there has been a mix-up in the
files or an error in the paper.  In either case, I find it odd to use TIP4P with
CHARMM, especially given the sensitivity of lipid parameters to the water model.
  Without knowing the paper you're talking about, I will not criticize the
choice as it may have been justified.  It's probably a good question to ask of
the corresponding author of the study you are trying to reproduce.

-Justin

--
==

Justin A. Lemkul, Ph.D.
Postdoctoral Fellow

Department of Pharmaceutical Sciences
School of Pharmacy
Health Sciences Facility II, Room 601
University of Maryland, Baltimore
20 Penn St.
Baltimore, MD 21201

jalem...@outerbanks.umaryland.edu | (410) 706-7441

==

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[gmx-users] RE : gmx-users Digest, Vol 113, Issue 106

2013-09-23 Thread ABEL Stephane 175950
Finally, I have resolved my (little) problem: I used CHARMM-GUI to constructed 
the membrane, removed the TIP3 water molecules and then resolvate the bilayer 
with TIP4P/2005 water molecules. The simulation seems to work.

Stephane


 
On 9/23/13 10:23 AM, ABEL Stephane 175950 wrote:
 Hello Justin,

 Thank you for your response and your interest for my simulations ;) I am of 
 course aware that the primary water model for the CHARMM is the TIP3(S)P 
 model.

 Since, I am mainly interested to the water dynamic around DOPC molecules in 
 the context of the different water/DOPC mesophases (not data available, I 
 currently doing the tests ;)) and that it is known that the TIP4P/2005 water 
 model (it is the model, I want to use) reproduces better the water dynamic 
 and structure than the TIP3P water model, I would like to test if the 
 TIP4P/2005 water can be used in simulation of membranes. I am not aware that 
 somebody have already done the test.

 Finally, Justin, you are probably right here, the results will be probably 
 not good as it is suggested by Pastor and MacKerell in their paper for 
 TIP4P-EW water model [1], but I think that it is worth a test to confirm this 
 in case of the TIP4P/2005. I am not the first one to ask this question in the 
 context of simulations with the CHARMM force field (for protein, here [2]).

 [1] www.ncbi.nlm.nih.gov/pmc/articles/PMC3133452/
 [2]  Nutt, D. R.; Smith, J. C. Molecular Dynamics Simulations of Proteins: 
 Can the Explicit Water Model Be Varied? J. Chem. Theory Comput. 2007, 3, 
 1550?1560.


It sounds like you're on the right track, at least knowing that a considerable
amount of work has to be done to prove that the force field + water model
combination is sound.  Given that you're going to have to re-equilibrate the
water anyway, I don't see why you have to start with TIP3P and try to hack it
into becoming TIP4P; I would just strip the water and re-solvate.

-Justin

--
==

Justin A. Lemkul, Ph.D.
Postdoctoral Fellow

Department of Pharmaceutical Sciences
School of Pharmacy
Health Sciences Facility II, Room 601
University of Maryland, Baltimore
20 Penn St.
Baltimore, MD 21201

jalem...@outerbanks.umaryland.edu | (410) 706-7441

==

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[gmx-users] Select atoms in a residue

2013-09-03 Thread ABEL Stephane 175950
Hello all, 

A Quick question below: 

My peptide contains one trp, and i want to select only the atoms that form the 
the indol ring. I would like a portable script for others systems that contain 
also a peptide with one Trp residue. So I am not interesting to select the 
corresponding atoms by their numbers in the pdb/gro files 

The atom name in the indol group are  aCG | aCD1 | aHD1 | aCD2 | aCE3 | aHE3 | 
aCZ3 | aHZ3 | aCH2 | aHH2 | aCZ2 | aHZ2 | aCE2 | aNE1 | aHE1

Can you help me ? 

Best,

Stephane   --
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[gmx-users] Re: Select atoms in a residue

2013-09-03 Thread ABEL Stephane 175950
Hello Justin, 

My question was  How to select the following atoms CG, CD1, HD1, CD2, CE3, 
HE3, CZ3, HZ3, CH2, etc.. present ONLY in the trp residue with a single line 
command with make_ndx. Indeed some of them can be also present in other 
residues. 

Stephane

--

Message: 4
Date: Tue, 3 Sep 2013 12:57:25 +
From: ABEL Stephane 175950 stephane.a...@cea.fr
Subject: [gmx-users] Select atoms in a residue
To: gmx-users@gromacs.org gmx-users@gromacs.org
Message-ID:
3e39b768bb199548ab18f7289e7534af1a880...@exdag0-b0.intra.cea.fr
Content-Type: text/plain; charset=us-ascii

Hello all,

A Quick question below:

My peptide contains one trp, and i want to select only the atoms that form the 
the indol ring. I would like a portable script for others systems that contain 
also a peptide with one Trp residue. So I am not interesting to select the 
corresponding atoms by their numbers in the pdb/gro files

The atom name in the indol group are  aCG | aCD1 | aHD1 | aCD2 | aCE3 | aHE3 | 
aCZ3 | aHZ3 | aCH2 | aHH2 | aCZ2 | aHZ2 | aCE2 | aNE1 | aHE1

Can you help me ?

Best,

Stephane
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[gmx-users] How do I make an AOT reverse micelle, which package I should use

2013-07-13 Thread ABEL Stephane 175950
Hello, 

I have a done a lot of simulations of reverse micelles. For me to construct the 
best model of preformed RM you can indeed use Packmol. But after that, you will 
carry out out different equilibration stages to obtain stable reverse micelles.
 I want to arrange charge, LJ parameter, hydrogen bond length? protonation 
 state of the water molecules, and the proper orientation like angles as 
 well. 
About what ? Sorry I do not not understand your questions. Moreover, since you 
will do classical MD, water state will not change at all during the simulation

Stéphane

--

Message: 5
Date: Fri, 12 Jul 2013 18:36:03 -0700 (PDT)
From: Hari Pandey hariche...@yahoo.com
Subject: [gmx-users] How do I make an AOT reverse micell,   which
package I should use
To: gmx-users@gromacs.org gmx-users@gromacs.org
Message-ID:
1373679363.26833.yahoomail...@web163003.mail.bf1.yahoo.com
Content-Type: text/plain; charset=iso-8859-1

Hi all GROMACS users,

I need to make a pdb file of AOT reverse micell . Please some body tell me how 
do I build it and which package would best for this work. Now I am using 
PACKMOL but it seems just a geometrical mathematical manipulation. I want to 
arrange charge, LJ parameter, hydrogen bond length? protonation state of the 
water molecules, and the proper orientation like angles as well. I don't know 
how do I use all these parameters in PACKMOL. So please advice me which package 
could be good for this purpose.
I appreciate your help.

Thank you very much
Hari

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[gmx-users] probability from COM of micelle

2013-05-10 Thread ABEL Stephane 175950
Hi,

You indeed could use  the g_rdf command like this (in the script)

g_rdf_mpi -f $pathXTC -s $pathTPR -n bOG_Micelle_RDF.ndx -norm -com -b 
$timeBegin1 -e $timeEnd1 -o $name1_$name2_$name3_$i_original.xvg  
RadDensFunc_$i.txt

Where in the  RadDensFunc.txt file, i choose as the first group the micelle 
group (for the micelle COM) and as the second group  the micelle atom you want 
to plot the rdf (i.e. surfactant headgroup, alkyl tail, etc?)

Do not forget to take into account the (average) volume of the simulation cell 
and the mass of the atom group to obtain the rho(r) (g.cm-3) as function of the 
Micelle COM otherwise, you will obtain the N(r) as function of Micelle COM (in 
nm-1)

HTH




On 5/9/13 10:15 AM, mohammad agha wrote:


 Dear GROMACS Specialist,

 I want to plot probability (nm^-1) distribution of micelle selected atoms 
 with respect to COM of the micelle (nm).
 with respect to this definition, Probability was defined as the number of 
 instances the selected atom was found within a spherical shell of width 0.02 
 nm at a distance r from the micelle COM divided by r, may I ask you to give 
 me one formula to plot of this probability, Please?
 for example, to plot of density(nm^-3) with respect to COM of micelle (nm), I 
 do as following:
 density = g(r) * (N/V)


It sounds like all you need to do is create a histogram from data produced by
g_dist.  You can make the histogram with g_analyze or any number of other 
programs.

-Justin

--


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




--

Message: 2
Date: Thu, 09 May 2013 21:03:44 +0200
From: David van der Spoel sp...@xray.bmc.uu.se
Subject: Re: [gmx-users] Fw: probability from COM of micelle
To: gmx-users@gromacs.org
Message-ID: 518bf310.6020...@xray.bmc.uu.se
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

On 2013-05-09 20:15, Justin Lemkul wrote:


 On 5/9/13 10:15 AM, mohammad agha wrote:


 Dear GROMACS Specialist,

 I want to plot probability (nm^-1) distribution of micelle selected
 atoms with respect to COM of the micelle (nm).
 with respect to this definition, Probability was defined as the
 number of instances the selected atom was found within a spherical
 shell of width 0.02 nm at a distance r from the micelle COM divided by
 r, may I ask you to give me one formula to plot of this probability,
 Please?
 for example, to plot of density(nm^-3) with respect to COM of micelle
 (nm), I do as following:
 density = g(r) * (N/V)


 It sounds like all you need to do is create a histogram from data
 produced by g_dist.  You can make the histogram with g_analyze or any
 number of other programs.

 -Justin

How about g_rdf?


--
David van der Spoel, Ph.D., Professor of Biology
Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
sp...@xray.bmc.uu.sehttp://folding.bmc.uu.se


--

Message: 3
Date: Thu, 9 May 2013 13:33:54 -0700
From: Eric Stokes es...@uw.edu
Subject: [gmx-users] Charmm27 potential energies.
To: gmx-users@gromacs.org
Message-ID:
capsvvmtorup3gnxthy6gkouevenstp1qydhgr7yweq-r8vg...@mail.gmail.com
Content-Type: text/plain; charset=ISO-8859-1

Hello,

I am attempting to generate force-field parameters for a fatty acid
molecule that contains a carboxilic acid head group. I decided to use the
parameters for stearic acid as the base for my molecule, since they contain
similar structures with the only major change being a shorter hydrophobic
tail. I noticed that the charge on stearic acid, and other molecules that
have a carboxilic head group, is spread out with -0.9 residing on the head
group and -0.1 on the second carbon. I need to use the protonated from of
my molecule for my simulation, as well as the deprotonated form. I looked
into the parameters for the COOH replacement in the Charmm27 force-field
and used that to form the head group of the protonated form of my molecule.
The problem that I am facing is that this left behind a charge of -0.1 that
resides on the second carbon. Is there any way to find acceptable partial
charges without doing the full Gaussian calculations? I would also
appreciate it if someone could explain why the charges were split onto the
second carbon in the first place.

Thanks in advance,
Eric Stokes


--

Message: 4
Date: Thu, 09 May 2013 16:39:41 -0400
From: Justin Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] Charmm27 potential energies.
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 518c098d.2080...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



On 5/9/13 4:33 PM, Eric Stokes wrote:
 Hello,

 I am attempting to generate force-field parameters for a fatty acid
 

[gmx-users] RE: Martini with PME, temp two low

2013-04-26 Thread ABEL Stephane 175950
Hi Xavier, 

I used a dt of 10 ps with nstlist of 2. In that case the Temp of the system is 
stable and the energy well conserved (400 ns of run). I do know if it is 
optimal but it works for my system. 

Stephane



--

Message: 1
Date: Fri, 26 Apr 2013 07:58:12 +0200
From: XAvier Periole x.peri...@rug.nl
Subject: Re: [gmx-users] Re: Martini with PME,  temp two low (ABEL
Stephane 175950)
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 6d1fd74e-91bb-4c0c-95ce-e863924dd...@rug.nl
Content-Type: text/plain;   charset=us-ascii


Good. Note however that we do get the right temperature with a dt=20fs with 
Martini so you energy leak might be in the cutoff scheme or the system is 
really badly equilibrated.

On Apr 25, 2013, at 18:23, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Xavier

 I have followed your suggestion and did a longer NPT equilibration with 
 smaller dt and ntlist values and It works. The Energy and Temp  reach to 
 stables values as i want.

 thank you again  for your help

 Stephane

 --

 Message: 2
 Date: Thu, 25 Apr 2013 14:17:00 +
 From: ABEL Stephane 175950 stephane.a...@cea.fr
 Subject: [gmx-users] Re: Martini with PME, temp two low
 To: gmx-users@gromacs.org gmx-users@gromacs.org
 Message-ID:
3e39b768bb199548ab18f7289e7534af1a818...@exdag0-b0.intra.cea.fr
 Content-Type: text/plain; charset=us-ascii

 @ Vitaly
 of course. I know that. My system is neutral  but with charged particles (AOT 
 and Na+).

 @Xavier
 I will try your suggestion and equilibrate my system for a longer period

 Thanks again

 Stephane



 --

 Message: 1
 Date: Thu, 25 Apr 2013 15:52:09 +0200
 From: XAvier Periole x.peri...@rug.nl
 Subject: Re: [gmx-users] Martini with PME, temp two low
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 0a7b7d0a-b419-4d3d-826b-e6d61de6d...@rug.nl
 Content-Type: text/plain; charset=windows-1252


 Well ? 400 ps is rather small and you can expect deviations from so short 
 simulations if you start from an non-equilibrated system. I am not sure what 
 the void is but this indicates that your system might not be equilibrated ?

 You can try to decrease the time step and nstlist to see if you the drop of 
 temperature is due a flow of energy.

 On Apr 25, 2013, at 3:26 PM, ABEL Stephane 175950 stephane.a...@cea.fr 
 wrote:

 Hello Xavier,

 Thank you for your response.

 nstlist = 10 and the rlist = 1.0
 My mistake, i did not changes these values when i switched to PME,

 I have rerun the simulations for 400 ps in NPT with these changes and 
 plotted Epot and Temp vs Time The Epot and Temp values are not stables. The 
 average Temp of the system  is better than previously but fluctuate around 
 (294 K) instead of 298 K . Note i use gmx4.5.5 to do my calculations.

 I have also visualized my  system at the end of the NPT run, the  na+, 
 water, surfactant, octane molecules  form a slab with void

 What's wrong ?

 Stephane

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[gmx-users] RE: Martini with PME, temp two low

2013-04-26 Thread ABEL Stephane 175950
Xavier, 

as i said in my message, this nstlist value is not optimal, but it works !!! if 
wlll try a higher nstlist value, if I have same problem in futur simulations 

Thanks again for you help 

Stephane




--

Message: 1
Date: Fri, 26 Apr 2013 07:58:12 +0200
From: XAvier Periole x.peri...@rug.nl
Subject: Re: [gmx-users] Re: Martini with PME,  temp two low (ABEL
Stephane 175950)
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 6d1fd74e-91bb-4c0c-95ce-e863924dd...@rug.nl
Content-Type: text/plain;   charset=us-ascii


Good. Note however that we do get the right temperature with a dt=20fs with 
Martini so you energy leak might be in the cutoff scheme or the system is 
really badly equilibrated.

On Apr 25, 2013, at 18:23, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Xavier

 I have followed your suggestion and did a longer NPT equilibration with 
 smaller dt and ntlist values and It works. The Energy and Temp  reach to 
 stables values as i want.

 thank you again  for your help

 Stephane

 --

 Message: 2
 Date: Thu, 25 Apr 2013 14:17:00 +
 From: ABEL Stephane 175950 stephane.a...@cea.fr
 Subject: [gmx-users] Re: Martini with PME, temp two low
 To: gmx-users@gromacs.org gmx-users@gromacs.org
 Message-ID:
3e39b768bb199548ab18f7289e7534af1a818...@exdag0-b0.intra.cea.fr
 Content-Type: text/plain; charset=us-ascii

 @ Vitaly
 of course. I know that. My system is neutral  but with charged particles (AOT 
 and Na+).

 @Xavier
 I will try your suggestion and equilibrate my system for a longer period

 Thanks again

 Stephane



 --

 Message: 1
 Date: Thu, 25 Apr 2013 15:52:09 +0200
 From: XAvier Periole x.peri...@rug.nl
 Subject: Re: [gmx-users] Martini with PME, temp two low
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 0a7b7d0a-b419-4d3d-826b-e6d61de6d...@rug.nl
 Content-Type: text/plain; charset=windows-1252


 Well ? 400 ps is rather small and you can expect deviations from so short 
 simulations if you start from an non-equilibrated system. I am not sure what 
 the void is but this indicates that your system might not be equilibrated ?

 You can try to decrease the time step and nstlist to see if you the drop of 
 temperature is due a flow of energy.

 On Apr 25, 2013, at 3:26 PM, ABEL Stephane 175950 stephane.a...@cea.fr 
 wrote:

 Hello Xavier,

 Thank you for your response.

 nstlist = 10 and the rlist = 1.0
 My mistake, i did not changes these values when i switched to PME,

 I have rerun the simulations for 400 ps in NPT with these changes and 
 plotted Epot and Temp vs Time The Epot and Temp values are not stables. The 
 average Temp of the system  is better than previously but fluctuate around 
 (294 K) instead of 298 K . Note i use gmx4.5.5 to do my calculations.

 I have also visualized my  system at the end of the NPT run, the  na+, 
 water, surfactant, octane molecules  form a slab with void

 What's wrong ?

 Stephane

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[gmx-users] Martini with PME, temp two low

2013-04-25 Thread ABEL Stephane 175950
Hello all, 

I am trying to test the martini force field with PME for a charged system that 
contains na+, water, surfactant, octane molecules at 298K and P=0.1MPa. My 
system works well, if i use the standard shift parameters (correct temp, and 
pressure). But for for the simulation with PME , the temp of the system 
decrease to  290 K. Below my *.mdp parameters for a NPT equil at 298K 


integrator   = md
dt   = 0.020
nsteps   = 1 ; 200ps
nstcomm  = 10
comm-grps=
;refcoord_scaling = com

nstxout  = 0
nstvout  = 0
nstfout  = 0
nstlog   = 1000
nstenergy= 100
;nstxtcout= 1000
xtc_precision= 100
;xtc-grps =
energygrps   = AOT W ION OCT

nstlist  = 10
ns_type  = grid
pbc  = xyz
rlist= 1.

; PME parameters
coulombtype  = PME
rcoulomb = 1.2
rvdw = 1.2
fourierspacing   = 0.12
fourier_nx   = 0
fourier_ny   = 0
fourier_nz   = 0
pme_order= 4

tcoupl   = v-rescale
tc-grps  = AOT_W_ION OCT
tau_t= 1.0 1.0
ref_t= 298 298
Pcoupl   = berendsen
Pcoupltype   = isotropic
tau_p= 1.0
compressibility  = 4.5e-5
ref_p= 1.0

;gen_vel  = no
;gen_temp = 0
;gen_seed = 473529


; MARTINI and CONSTRAINTS
; for ring systems and stiff bonds constraints are defined
; which are best handled using Lincs.

constraints  = none
constraint_algorithm = Lincs
unconstrained_start  = no
lincs_order  = 4
lincs_warnangle  = 3


Results obtained with W/ PME 

   Statistics over 10001 steps using 1001 frames

   Energies (kJ/mol)
   Bond   G96AngleLJ (SR)   Coulomb (SR)   Coul. recip.
1.63789e+041.25195e+03   -4.02093e+05   -8.22079e+03   -4.86843e+04
  PotentialKinetic En.   Total EnergyTemperature Pressure (bar)
   -4.41367e+057.81801e+04   -3.63187e+052.90373e+02   -1.76470e+01
T-AOT_W_ION  T-OCT
2.90629e+022.90357e+02

Results W:o PME

   Energies (kJ/mol)
   Bond   G96AngleLJ (SR)   Coulomb (SR)  Potential
1.60482e+041.24820e+03   -3.34608e+05   -7.33665e+02   -3.18046e+05
Kinetic En.   Total EnergyTemperature Pressure (bar)
8.02685e+04   -2.3e+052.98129e+02   -3.07123e+01

  Box-X  Box-Y  Box-Z
1.52926e+011.52926e+011.52926e+01


T-AOT_W_ION  T-OCT
2.98141e+022.98129e+02


Did I miss something ?


Note that for the moment i do not use the polarizable water model.

Thanks for your help 

Stephane




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[gmx-users] RE : gmx-users Digest, Vol 108, Issue 154

2013-04-25 Thread ABEL Stephane 175950
Hello Xavier, 

Thank you for your response. 

 nstlist = 10 and the rlist = 1.0 
My mistake, i did not changes these values when i switched to PME,

I have rerun the simulations for 400 ps in NPT with these changes and plotted 
Epot and Temp vs Time The Epot and Temp values are not stables. The average 
Temp of the system  is better than previously but fluctuate around (294 K) 
instead of 298 K . Note i use gmx4.5.5 to do my calculations.

 I have also visualized my  system at the end of the NPT run, the  na+, water, 
surfactant, octane molecules  form a slab with void

What's wrong ?

Stephane 



--

Message: 5
Date: Thu, 25 Apr 2013 13:34:21 +0200
From: XAvier Periole x.peri...@rug.nl
Subject: Re: [gmx-users] Martini with PME, temp two low
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4632c83b-cd6f-4c92-b887-a1c39dff4...@rug.nl
Content-Type: text/plain; charset=us-ascii


Did you visualise the system? T in function of time? Epot in function of time?

As a side note (not relevant for PME) the mix of nstlist = 10 and the rlist = 
1.0 is pretty bad! You want at least rlist=1.2 when nstlist=5 and rlist=1.4 if 
nstlist =10.

On Apr 25, 2013, at 1:10 PM, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Hello all,

 I am trying to test the martini force field with PME for a charged system 
 that contains na+, water, surfactant, octane molecules at 298K and P=0.1MPa. 
 My system works well, if i use the standard shift parameters (correct temp, 
 and pressure). But for for the simulation with PME , the temp of the system 
 decrease to  290 K. Below my *.mdp parameters for a NPT equil at 298K


 integrator   = md
 dt   = 0.020
 nsteps   = 1 ; 200ps
 nstcomm  = 10
 comm-grps=
 ;refcoord_scaling = com

 nstxout  = 0
 nstvout  = 0
 nstfout  = 0
 nstlog   = 1000
 nstenergy= 100
 ;nstxtcout= 1000
 xtc_precision= 100
 ;xtc-grps =
 energygrps   = AOT W ION OCT

 nstlist  = 10
 ns_type  = grid
 pbc  = xyz
 rlist= 1.

 ; PME parameters
 coulombtype  = PME
 rcoulomb = 1.2
 rvdw = 1.2
 fourierspacing   = 0.12
 fourier_nx   = 0
 fourier_ny   = 0
 fourier_nz   = 0
 pme_order= 4

 tcoupl   = v-rescale
 tc-grps  = AOT_W_ION OCT
 tau_t= 1.0 1.0
 ref_t= 298 298
 Pcoupl   = berendsen
 Pcoupltype   = isotropic
 tau_p= 1.0
 compressibility  = 4.5e-5
 ref_p= 1.0

 ;gen_vel  = no
 ;gen_temp = 0
 ;gen_seed = 473529


 ; MARTINI and CONSTRAINTS
 ; for ring systems and stiff bonds constraints are defined
 ; which are best handled using Lincs.

 constraints  = none
 constraint_algorithm = Lincs
 unconstrained_start  = no
 lincs_order  = 4
 lincs_warnangle  = 3


 Results obtained with W/ PME

   Statistics over 10001 steps using 1001 frames

   Energies (kJ/mol)
   Bond   G96AngleLJ (SR)   Coulomb (SR)   Coul. recip.
1.63789e+041.25195e+03   -4.02093e+05   -8.22079e+03   -4.86843e+04
  PotentialKinetic En.   Total EnergyTemperature Pressure (bar)
   -4.41367e+057.81801e+04   -3.63187e+052.90373e+02   -1.76470e+01
T-AOT_W_ION  T-OCT
2.90629e+022.90357e+02

 Results W:o PME

   Energies (kJ/mol)
   Bond   G96AngleLJ (SR)   Coulomb (SR)  Potential
1.60482e+041.24820e+03   -3.34608e+05   -7.33665e+02   -3.18046e+05
Kinetic En.   Total EnergyTemperature Pressure (bar)
8.02685e+04   -2.3e+052.98129e+02   -3.07123e+01

  Box-X  Box-Y  Box-Z
1.52926e+011.52926e+011.52926e+01


T-AOT_W_ION  T-OCT
2.98141e+022.98129e+02


 Did I miss something ?


 Note that for the moment i do not use the polarizable water model.

 Thanks for your help

 Stephane




 --
 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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--

Message: 6
Date: Thu, 25 Apr 2013 14:05:51 +0200
From: Berk Hess g...@hotmail.com
Subject: RE: [gmx-users] Differences between 4.5.5 and 4.6.2-dev?
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID

Re: [gmx-users] Martini with PME, temp two low

2013-04-25 Thread ABEL Stephane 175950
Sorry for the double post, but i forgot to remove the others message. I have 
also added the average values obtained for this run 

Statistics over 20001 steps using 4001 frames

   Energies (kJ/mol)
   Bond   G96AngleLJ (SR)   Coulomb (SR)   Coul. recip.
1.65683e+041.26644e+03   -4.02287e+05   -8.47260e+03   -4.90494e+04
  PotentialKinetic En.   Total EnergyTemperature Pressure (bar)
   -4.41974e+057.91982e+04   -3.62776e+052.94154e+02   -1.80237e+01

  Box-X  Box-Y  Box-Z
1.51316e+011.51316e+011.51316e+01

   Total Virial (kJ/mol)
2.90936e+04   -4.68005e+01   -2.46005e+01
   -4.68005e+012.92687e+04   -2.56235e+01
   -2.46006e+01   -2.56236e+012.64822e+04

   Pressure (bar)
   -2.57341e+015.58858e-011.46893e-01
5.58858e-01   -2.74443e+012.21040e-01
1.46893e-012.21041e-01   -8.92609e-01

   Total Dipole (D)
4.16699e+021.92049e+026.43137e+02

  Epot (kJ/mol)Coul-SR  LJ-SR
AOT-AOT5.26697e+02   -4.94208e+03
  AOT-W0.0e+00   -2.35002e+03
AOT-ION   -9.54002e+03   -1.89339e+03
AOT-OCT0.0e+00   -2.04448e+04
W-W0.0e+00   -3.88078e+02

Stephane

--

Message: 4
Date: Thu, 25 Apr 2013 13:26:32 +
From: ABEL Stephane 175950 stephane.a...@cea.fr
Subject: [gmx-users] RE : gmx-users Digest, Vol 108, Issue 154
To: gmx-users@gromacs.org gmx-users@gromacs.org
Message-ID:
3e39b768bb199548ab18f7289e7534af1a818...@exdag0-b0.intra.cea.fr
Content-Type: text/plain; charset=us-ascii

Hello Xavier,

Thank you for your response.

 nstlist = 10 and the rlist = 1.0
My mistake, i did not changes these values when i switched to PME,

I have rerun the simulations for 400 ps in NPT with these changes and plotted 
Epot and Temp vs Time The Epot and Temp values are not stables. The average 
Temp of the system  is better than previously but fluctuate around (294 K) 
instead of 298 K . Note i use gmx4.5.5 to do my calculations.

 I have also visualized my  system at the end of the NPT run, the  na+, water, 
surfactant, octane molecules  form a slab with void

What's wrong ?

Stephane



--

Message: 5
Date: Thu, 25 Apr 2013 13:34:21 +0200
From: XAvier Periole x.peri...@rug.nl
Subject: Re: [gmx-users] Martini with PME, temp two low
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4632c83b-cd6f-4c92-b887-a1c39dff4...@rug.nl
Content-Type: text/plain; charset=us-ascii


Did you visualise the system? T in function of time? Epot in function of time?

As a side note (not relevant for PME) the mix of nstlist = 10 and the rlist = 
1.0 is pretty bad! You want at least rlist=1.2 when nstlist=5 and rlist=1.4 if 
nstlist =10.

On Apr 25, 2013, at 1:10 PM, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Hello all,

 I am trying to test the martini force field with PME for a charged system 
 that contains na+, water, surfactant, octane molecules at 298K and P=0.1MPa. 
 My system works well, if i use the standard shift parameters (correct temp, 
 and pressure). But for for the simulation with PME , the temp of the system 
 decrease to  290 K. Below my *.mdp parameters for a NPT equil at 298K


 integrator   = md
 dt   = 0.020
 nsteps   = 1 ; 200ps
 nstcomm  = 10
 comm-grps=
 ;refcoord_scaling = com

 nstxout  = 0
 nstvout  = 0
 nstfout  = 0
 nstlog   = 1000
 nstenergy= 100
 ;nstxtcout= 1000
 xtc_precision= 100
 ;xtc-grps =
 energygrps   = AOT W ION OCT

 nstlist  = 10
 ns_type  = grid
 pbc  = xyz
 rlist= 1.

 ; PME parameters
 coulombtype  = PME
 rcoulomb = 1.2
 rvdw = 1.2
 fourierspacing   = 0.12
 fourier_nx   = 0
 fourier_ny   = 0
 fourier_nz   = 0
 pme_order= 4

 tcoupl   = v-rescale
 tc-grps  = AOT_W_ION OCT
 tau_t= 1.0 1.0
 ref_t= 298 298
 Pcoupl   = berendsen
 Pcoupltype   = isotropic
 tau_p= 1.0
 compressibility  = 4.5e-5
 ref_p= 1.0

 ;gen_vel  = no
 ;gen_temp = 0
 ;gen_seed = 473529


 ; MARTINI and CONSTRAINTS
 ; for ring systems and stiff bonds constraints are defined
 ; which are best handled using Lincs.

 constraints  = none
 constraint_algorithm = Lincs
 unconstrained_start  = no
 lincs_order  = 4
 lincs_warnangle  = 3


 Results obtained with W/ PME

   Statistics over 10001 steps using 1001 frames

[gmx-users] Martini with PME, temp two low

2013-04-25 Thread ABEL Stephane 175950
And ? sorry but i do not understand...

Stephane

--

Message: 2
Date: Thu, 25 Apr 2013 15:39:12 +0200
From: Dr. Vitaly Chaban vvcha...@gmail.com
Subject: Re: [gmx-users] Martini with PME, temp two low
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID:
CAPXdD+bDiuQWG_3eWZ_0yb=aynlaaf08vt46usel4wk_bjg...@mail.gmail.com
Content-Type: text/plain; charset=ISO-8859-1

Hmmm

Aren't the keywords here charged system + PME?


Dr. Vitaly Chaban



On Thu, Apr 25, 2013 at 1:34 PM, XAvier Periole x.peri...@rug.nl wrote:


 Did you visualise the system? T in function of time? Epot in function of
 time?

 As a side note (not relevant for PME) the mix of nstlist = 10 and the
 rlist = 1.0 is pretty bad! You want at least rlist=1.2 when nstlist=5 and
 rlist=1.4 if nstlist =10.

 On Apr 25, 2013, at 1:10 PM, ABEL Stephane 175950 stephane.a...@cea.fr
 wrote:

  Hello all,
 
  I am trying to test the martini force field with PME for a charged
 system that contains na+, water, surfactant, octane molecules at 298K and
 P=0.1MPa. My system works well, if i use the standard shift parameters
 (correct temp, and pressure). But for for the simulation with PME , the
 temp of the system decrease to  290 K. Below my *.mdp parameters for a NPT
 equil at 298K
 
 
  integrator   = md
  dt   = 0.020
  nsteps   = 1 ; 200ps
  nstcomm  = 10
  comm-grps=
  ;refcoord_scaling = com
 
  nstxout  = 0
  nstvout  = 0
  nstfout  = 0
  nstlog   = 1000
  nstenergy= 100
  ;nstxtcout= 1000
  xtc_precision= 100
  ;xtc-grps =
  energygrps   = AOT W ION OCT
 
  nstlist  = 10
  ns_type  = grid
  pbc  = xyz
  rlist= 1.
 
  ; PME parameters
  coulombtype  = PME
  rcoulomb = 1.2
  rvdw = 1.2
  fourierspacing   = 0.12
  fourier_nx   = 0
  fourier_ny   = 0
  fourier_nz   = 0
  pme_order= 4
 
  tcoupl   = v-rescale
  tc-grps  = AOT_W_ION OCT
  tau_t= 1.0 1.0
  ref_t= 298 298
  Pcoupl   = berendsen
  Pcoupltype   = isotropic
  tau_p= 1.0
  compressibility  = 4.5e-5
  ref_p= 1.0
 
  ;gen_vel  = no
  ;gen_temp = 0
  ;gen_seed = 473529
 
 
  ; MARTINI and CONSTRAINTS
  ; for ring systems and stiff bonds constraints are defined
  ; which are best handled using Lincs.
 
  constraints  = none
  constraint_algorithm = Lincs
  unconstrained_start  = no
  lincs_order  = 4
  lincs_warnangle  = 3
 
 
  Results obtained with W/ PME
 
Statistics over 10001 steps using 1001 frames
 
Energies (kJ/mol)
Bond   G96AngleLJ (SR)   Coulomb (SR)   Coul.
 recip.
 1.63789e+041.25195e+03   -4.02093e+05   -8.22079e+03
 -4.86843e+04
   PotentialKinetic En.   Total EnergyTemperature Pressure
 (bar)
-4.41367e+057.81801e+04   -3.63187e+052.90373e+02
 -1.76470e+01
 T-AOT_W_ION  T-OCT
 2.90629e+022.90357e+02
 
  Results W:o PME
 
Energies (kJ/mol)
Bond   G96AngleLJ (SR)   Coulomb (SR)
  Potential
 1.60482e+041.24820e+03   -3.34608e+05   -7.33665e+02
 -3.18046e+05
 Kinetic En.   Total EnergyTemperature Pressure (bar)
 8.02685e+04   -2.3e+052.98129e+02   -3.07123e+01
 
   Box-X  Box-Y  Box-Z
 1.52926e+011.52926e+011.52926e+01
 
 
 T-AOT_W_ION  T-OCT
 2.98141e+022.98129e+02
 
 
  Did I miss something ?
 
 
  Note that for the moment i do not use the polarizable water model.
 
  Thanks for your help
 
  Stephane
 
 
 

--
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[gmx-users] Re: Martini with PME, temp two low

2013-04-25 Thread ABEL Stephane 175950
@ Vitaly
of course. I know that. My system is neutral  but with charged particles (AOT 
and Na+).  

@Xavier 
I will try your suggestion and equilibrate my system for a longer period

Thanks again

Stephane



--

Message: 1
Date: Thu, 25 Apr 2013 15:52:09 +0200
From: XAvier Periole x.peri...@rug.nl
Subject: Re: [gmx-users] Martini with PME, temp two low
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 0a7b7d0a-b419-4d3d-826b-e6d61de6d...@rug.nl
Content-Type: text/plain; charset=windows-1252


Well ? 400 ps is rather small and you can expect deviations from so short 
simulations if you start from an non-equilibrated system. I am not sure what 
the void is but this indicates that your system might not be equilibrated ?

You can try to decrease the time step and nstlist to see if you the drop of 
temperature is due a flow of energy.

On Apr 25, 2013, at 3:26 PM, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Hello Xavier,

 Thank you for your response.

 nstlist = 10 and the rlist = 1.0
 My mistake, i did not changes these values when i switched to PME,

 I have rerun the simulations for 400 ps in NPT with these changes and plotted 
 Epot and Temp vs Time The Epot and Temp values are not stables. The average 
 Temp of the system  is better than previously but fluctuate around (294 K) 
 instead of 298 K . Note i use gmx4.5.5 to do my calculations.

 I have also visualized my  system at the end of the NPT run, the  na+, water, 
 surfactant, octane molecules  form a slab with void

 What's wrong ?

 Stephane



 --

 Message: 5
 Date: Thu, 25 Apr 2013 13:34:21 +0200
 From: XAvier Periole x.peri...@rug.nl
 Subject: Re: [gmx-users] Martini with PME, temp two low
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 4632c83b-cd6f-4c92-b887-a1c39dff4...@rug.nl
 Content-Type: text/plain; charset=us-ascii


 Did you visualise the system? T in function of time? Epot in function of time?

 As a side note (not relevant for PME) the mix of nstlist = 10 and the rlist = 
 1.0 is pretty bad! You want at least rlist=1.2 when nstlist=5 and rlist=1.4 
 if nstlist =10.

 On Apr 25, 2013, at 1:10 PM, ABEL Stephane 175950 stephane.a...@cea.fr 
 wrote:

 Hello all,

 I am trying to test the martini force field with PME for a charged system 
 that contains na+, water, surfactant, octane molecules at 298K and P=0.1MPa. 
 My system works well, if i use the standard shift parameters (correct temp, 
 and pressure). But for for the simulation with PME , the temp of the system 
 decrease to  290 K. Below my *.mdp parameters for a NPT equil at 298K


 integrator   = md
 dt   = 0.020
 nsteps   = 1 ; 200ps
 nstcomm  = 10
 comm-grps=
 ;refcoord_scaling = com

 nstxout  = 0
 nstvout  = 0
 nstfout  = 0
 nstlog   = 1000
 nstenergy= 100
 ;nstxtcout= 1000
 xtc_precision= 100
 ;xtc-grps =
 energygrps   = AOT W ION OCT

 nstlist  = 10
 ns_type  = grid
 pbc  = xyz
 rlist= 1.

 ; PME parameters
 coulombtype  = PME
 rcoulomb = 1.2
 rvdw = 1.2
 fourierspacing   = 0.12
 fourier_nx   = 0
 fourier_ny   = 0
 fourier_nz   = 0
 pme_order= 4

 tcoupl   = v-rescale
 tc-grps  = AOT_W_ION OCT
 tau_t= 1.0 1.0
 ref_t= 298 298
 Pcoupl   = berendsen
 Pcoupltype   = isotropic
 tau_p= 1.0
 compressibility  = 4.5e-5
 ref_p= 1.0

 ;gen_vel  = no
 ;gen_temp = 0
 ;gen_seed = 473529


 ; MARTINI and CONSTRAINTS
 ; for ring systems and stiff bonds constraints are defined
 ; which are best handled using Lincs.

 constraints  = none
 constraint_algorithm = Lincs
 unconstrained_start  = no
 lincs_order  = 4
 lincs_warnangle  = 3


 Results obtained with W/ PME

  Statistics over 10001 steps using 1001 frames

  Energies (kJ/mol)
  Bond   G96AngleLJ (SR)   Coulomb (SR)   Coul. recip.
   1.63789e+041.25195e+03   -4.02093e+05   -8.22079e+03   -4.86843e+04
 PotentialKinetic En.   Total EnergyTemperature Pressure (bar)
  -4.41367e+057.81801e+04   -3.63187e+052.90373e+02   -1.76470e+01
   T-AOT_W_ION  T-OCT
   2.90629e+022.90357e+02

 Results W:o PME

  Energies (kJ/mol)
  Bond   G96AngleLJ (SR)   Coulomb (SR)  Potential
   1.60482e+041.24820e+03   -3.34608e+05   -7.33665e+02   -3.18046e+05
   Kinetic En.   Total EnergyTemperature

[gmx-users] Re: Martini with PME, temp two low (ABEL Stephane 175950)

2013-04-25 Thread ABEL Stephane 175950
Xavier 

I have followed your suggestion and did a longer NPT equilibration with smaller 
dt and ntlist values and It works. The Energy and Temp  reach to stables values 
as i want. 

 thank you again  for your help

Stephane

--

Message: 2
Date: Thu, 25 Apr 2013 14:17:00 +
From: ABEL Stephane 175950 stephane.a...@cea.fr
Subject: [gmx-users] Re: Martini with PME, temp two low
To: gmx-users@gromacs.org gmx-users@gromacs.org
Message-ID:
3e39b768bb199548ab18f7289e7534af1a818...@exdag0-b0.intra.cea.fr
Content-Type: text/plain; charset=us-ascii

@ Vitaly
of course. I know that. My system is neutral  but with charged particles (AOT 
and Na+).

@Xavier
I will try your suggestion and equilibrate my system for a longer period

Thanks again

Stephane



--

Message: 1
Date: Thu, 25 Apr 2013 15:52:09 +0200
From: XAvier Periole x.peri...@rug.nl
Subject: Re: [gmx-users] Martini with PME, temp two low
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 0a7b7d0a-b419-4d3d-826b-e6d61de6d...@rug.nl
Content-Type: text/plain; charset=windows-1252


Well ? 400 ps is rather small and you can expect deviations from so short 
simulations if you start from an non-equilibrated system. I am not sure what 
the void is but this indicates that your system might not be equilibrated ?

You can try to decrease the time step and nstlist to see if you the drop of 
temperature is due a flow of energy.

On Apr 25, 2013, at 3:26 PM, ABEL Stephane 175950 stephane.a...@cea.fr wrote:

 Hello Xavier,

 Thank you for your response.

 nstlist = 10 and the rlist = 1.0
 My mistake, i did not changes these values when i switched to PME,

 I have rerun the simulations for 400 ps in NPT with these changes and plotted 
 Epot and Temp vs Time The Epot and Temp values are not stables. The average 
 Temp of the system  is better than previously but fluctuate around (294 K) 
 instead of 298 K . Note i use gmx4.5.5 to do my calculations.

 I have also visualized my  system at the end of the NPT run, the  na+, water, 
 surfactant, octane molecules  form a slab with void

 What's wrong ?

 Stephane

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[gmx-users] Re: GROMOS54A8 parameters in GROMACS format

2013-02-14 Thread ABEL Stephane 175950
Hello, 

Yeap, I  have seen the links on ATB. Indeed, the conversion  of  the bonded 
terms (in this file 54a8.ifp ?) will be not too hard, but it is not the case 
for the AA  topology  where several changes were done. 

So any help will be appreciate..

Stephane 

--

Message: 5
Date: Thu, 14 Feb 2013 11:18:17 +0100
From: lloyd riggs lloyd.ri...@gmx.ch
Subject: Re: [gmx-users] GROMOS54A8 parameters in GROMACS format
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 20130214101817.72...@gmx.net
Content-Type: text/plain; charset=utf-8

Dear Stephane Abel,

Theres a link I on the gromacs web site to ATB, or you can google it.  If it is 
not in Gromacs format you can just write a couple 6 liner scripts to re-format 
it by parsing into the gromacs format,

Stephan Watkins

 Original-Nachricht 
 Datum: Wed, 13 Feb 2013 21:25:33 +
 Von: ABEL Stephane 175950 stephane.a...@cea.fr
 An: gmx-users@gromacs.org gmx-users@gromacs.org
 Betreff: [gmx-users] GROMOS54A8 parameters in GROMACS format

 Hello all,

 Does somebody know where i can find  the latest GROMOS force field (i.e.
 GROMOS54A8) described in [1]  in the GROMACS format (gromos54a7.ff) ?

 [1] Reif et al. J. Chem. Theory Comput. 2013, 9, 1247???1264 doi:
 http://pubs.acs.org/doi/citedby/10.1021/ct300156h

 Thank you

 Stephane


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[gmx-users] GROMOS54A8 parameters in GROMACS format

2013-02-14 Thread ABEL Stephane 175950
Thanks Berk, 

I have found the script, I will try them

Best

Stephane

Message: 4
Date: Thu, 14 Feb 2013 13:53:56 +0100
From: Berk Hess g...@hotmail.com
Subject: RE: [gmx-users] Re: GROMOS54A8 parameters in GROMACS format
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: dub124-w200b8c2eb085c78933a9418e...@phx.gbl
Content-Type: text/plain; charset=iso-8859-1


Hi,

There are two scripts make_gromos_rtp in the scripts directory which were used 
to convert Gromos AA topologies to rtp entries.

Cheers,

Berk


 From: stephane.a...@cea.fr
 To: gmx-users@gromacs.org
 Date: Thu, 14 Feb 2013 11:34:59 +
 Subject: [gmx-users] Re: GROMOS54A8 parameters in GROMACS format

 Hello,

 Yeap, I have seen the links on ATB. Indeed, the conversion of the bonded 
 terms (in this file 54a8.ifp ?) will be not too hard, but it is not the case 
 for the AA topology where several changes were done.

 So any help will be appreciate..

 Stephane

 --

 Message: 5
 Date: Thu, 14 Feb 2013 11:18:17 +0100
 From: lloyd riggs lloyd.ri...@gmx.ch
 Subject: Re: [gmx-users] GROMOS54A8 parameters in GROMACS format
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 20130214101817.72...@gmx.net
 Content-Type: text/plain; charset=utf-8

 Dear Stephane Abel,

 Theres a link I on the gromacs web site to ATB, or you can google it. If it 
 is not in Gromacs format you can just write a couple 6 liner scripts to 
 re-format it by parsing into the gromacs format,

 Stephan Watkins

  Original-Nachricht 
  Datum: Wed, 13 Feb 2013 21:25:33 +
  Von: ABEL Stephane 175950 stephane.a...@cea.fr
  An: gmx-users@gromacs.org gmx-users@gromacs.org
  Betreff: [gmx-users] GROMOS54A8 parameters in GROMACS format

  Hello all,
 
  Does somebody know where i can find the latest GROMOS force field (i.e.
  GROMOS54A8) described in [1] in the GROMACS format (gromos54a7.ff) ?
 
  [1] Reif et al. J. Chem. Theory Comput. 2013, 9, 1247???1264 doi:
  http://pubs.acs.org/doi/citedby/10.1021/ct300156h
 
  Thank you
 
  Stephane


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Message: 5
Date: Thu, 14 Feb 2013 08:01:43 -0500
From: Justin Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] different springs - WHAM
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 511ce037.5020...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



On 2/13/13 5:23 PM, Steven Neumann wrote:
 On Tue, Feb 12, 2013 at 5:01 PM, Justin Lemkul jalem...@vt.edu wrote:


 On 2/12/13 9:57 AM, Steven Neumann wrote:

 On Tue, Feb 12, 2013 at 2:53 PM, Justin Lemkul jalem...@vt.edu wrote:



 On 2/12/13 9:40 AM, Steven Neumann wrote:


 Dear Gmx Users,

 I know it is possible to combine windows with different spring
 constants into the one PMF curve using g_wham.

 Do I have to somehow tell g_wham that one or two windows have
 different spring constants?


 No, they are read from the .tpr files.


 For instance - I got the better histogram overlap with lower force
 constant in one window. When I replace this window into the window
 with the sring constant like all windwos (worse overlap) both PMF
 curves differ app. 2kcal/mol which is around 30% of the overall
 deltaG.

 Is there any error I should inroduce when one window differ in terms of
 k1?


 What does g_wham's error analysis suggest?

 -Justin


 In both PMF error estimate with bayesian bootstraping is app. 0.2 kcal/mol


 Seems like a good result, so what's the problem?

 -Justin

 That the better overlap of histograms produce worse deltaG comparing
 to experiment. With all the same spring constants I get the
 experimental value of deltaG but there is a poor overlap. There must
 be (somehow) a correction added to deltaG when introdcuing windows
 with different spring constants.


The code and/or g_wham paper should address this.  In principle, WHAM can be
conducted with any assortment of spring constants you like.  If you track down a
bug or something, please report it on redmine.gromacs.org.

A workaround of course would be to simply add another window (or windows) with
the same original force constant that gives adequate sampling.

-Justin

[gmx-users] GROMOS54A8 parameters in GROMACS format

2013-02-13 Thread ABEL Stephane 175950
Hello all, 

Does somebody know where i can find  the latest GROMOS force field (i.e. 
GROMOS54A8) described in [1]  in the GROMACS format (gromos54a7.ff) ? 

[1] Reif et al. J. Chem. Theory Comput. 2013, 9, 1247−1264 doi: 
http://pubs.acs.org/doi/citedby/10.1021/ct300156h

Thank you

Stephane-- 
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[gmx-users] Re:united atom

2013-02-07 Thread ABEL Stephane 175950
Hello, 

Is it correct for you that in your topolgy file, some atoms have wrong  mass 
(i.e. C7 and C9 have a mass of 15.035 instead of 14.027) in your DECAN  
molecule ? Are they at the end ? 

Stephane 


--

Message: 3
Date: Thu, 7 Feb 2013 19:13:11 +0330
From: Ali Alizadeh ali.alizadehmoja...@gmail.com
Subject: [gmx-users] Re:united atom
To: gmx-users gmx-users@gromacs.org
Message-ID:
capfuhmvnbu3v0verko_faxuvkk0qtg7hgazatjp16-a1rsh...@mail.gmail.com
Content-Type: text/plain; charset=UTF-8

Dear Justin

Thank you for your reply,

I want to use Nose-Hoover thermostat and MTTK barostat and shake
algorithm and md-vv integrator,

but I got this error:

---
Fatal error:
SHAKE is not supported with domain decomposition and constraint that
cross charge group boundaries, use LINCS
--

A part of my topology file:
--
[ moleculetype ]
; Namenrexcl
DECANE  9

[ atoms ]
;   nr   type  resnr residue  atom   cgnr charge   mass
typeBchargeB  massB
; residue   0 LI  rtp LI   q  0.0
 1   opls_071  0 LI C1  1  0 14.027   ; qtot 0
 2   opls_071  0 LI C2  2  0 14.027   ; qtot 0
 3   opls_071  0 LI C3  3  0 14.027   ; qtot 0
 4   opls_071  0 LI C4  4  0 14.027   ; qtot 0
 5   opls_071  0 LI C5  5  0 14.027   ; qtot 0
 6   opls_071  0 LI C6  6  0 14.027   ; qtot 0
 7   opls_068  0 LI C7  7  0 15.035   ; qtot 0
 8   opls_071  0 LI C8  8  0 14.027   ; qtot 0
 9   opls_068  0 LI C9  9  0 15.035   ; qtot 0
10   opls_071  0 LIC10  10  0 14.027   ; qtot 0

---


On 2/7/13 9:46 AM, Ali Alizadeh wrote:
 Dear All user

 There are 350 decane molecules in my simulation box,

 I like doing a simulation(npt ensemble) by a united atom force field,
 Can I use the opls (nonbonded: L-J 6-12 and coloumb) that is in
 gromacs?

 Beside, How can I neglect  coloumb interaction(non-bonded) and
 dihedrals(bonded)?


The OPLS force field in Gromacs contains both OPLS-AA (all-atom) and OPLS-UA
(united-atom) types, so you could in theory use OPLS-UA, but that's a fairly
ancient force field.  In that case, there are no Coulombic interactions 
anyway,
because the united-atom carbons should not have any charge.  If you want to
neglect dihedrals, I think you're hacking the force field in a way that makes 
no
sense.

-Justin

--
Sincerely

Ali Alizadeh
University of Tehran
College of engineering(Fanni)
Department of chemical engineering
IPE (Institute of Petroleum Engineering)
M.Sc Candidate, class of 2013
B.Sc Graduate 2011(University of Tehran,Fanni)

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[gmx-users] Compute the end to end distance distribution for surfactant

2013-01-10 Thread ABEL Stephane 175950
Dear All, 

I would like to compute the end to end distribution for different parts (i.e.  
hydrophobic and the polar) of several detergent molecules. I know that 
g_polystat can do the job and indeed i can obtain the end-to-end distance of 
the whole  molecule (at least for  the distance vs. time). But it is not clear 
to me how to obtain the end to end distance values for the different parts of 
my molecule with g_polystat. 

Can you help me ?

Stephane

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[gmx-users] Re: pressure_coupling

2012-11-22 Thread ABEL Stephane 175950
Hello,

This is a very nice and interesting work, Michael. Thank you for the efforts 
you made in writing this paper. I hope you will publish it. 

Best 

Stephane




Hi, all-

There are some issues with MTTK + constraints that are being worked
out for 4.6.  The good thing is, I have developed some sensitive tests
of the correct volume distribution (see
http://arxiv.org/abs/1208.0910) and the errors in PR are very, very
small. I would recommend using md + PR for projects with code before
4.6.

On Thu, Nov 22, 2012 at 4:27 AM, Florian Dommert
domm...@icp.uni-stuttgart.de wrote:
 -Urspr?ngliche Nachricht-
 Von: gmx-users-boun...@gromacs.org [mailto:gmx-users-
 boun...@gromacs.org] Im Auftrag von tarak karmakar
 Gesendet: Donnerstag, 22. November 2012 10:15
 An: Discussion list for GROMACS users
 Betreff: Re: [gmx-users] pressure_coupling

 U r right FLorian
 I have also tried playing around the tau_p but in vain.
 Even in absence of any constraints, it is giving almost same result.
 Em thinking to move again to Leap-Frog, NH , PR.  I see people generally
 use this
 combination a lot.
 Thanks

 Tarak

 Yes, that is right. The reason might be, that it is stable, working with
 Leap-Frog and implemented in Gromacs. However actually PR does not produce
 an NpT but an isoenthalpic ensemble. It also does not conform to both
 pressure virial theorems (see appendix of the Nose paper cited in the
 Gromacs manual). For this reason it would be very very good, if MTTK would
 work in Gromacs, because it fulfills all requirements for an NpT ensemble.
 On the other hand side the deviations vanish in the thermodynamic limit, so
 if your system is large enough, there should be no significant difference.

 /Flo


 On Wed, Nov 21, 2012 at 8:08 PM, Florian Dommert domm...@icp.uni-
 stuttgart.de wrote:
 
 
  ---
  Florian Dommert
  Dipl. Phys.
 
  Institut f?r Computerphysik
  Universit?t Stuttgart
  Allmandring 3
  D-70569 Stuttgart
 
  Tel.: 0711-68563613
  Fax: 0711-68563658
 
 
  -Urspr?ngliche Nachricht-
  Von: gmx-users-boun...@gromacs.org [mailto:gmx-users-
  boun...@gromacs.org] Im Auftrag von tarak karmakar
  Gesendet: Mittwoch, 21. November 2012 15:03
  An: Discussion list for GROMACS users
  Betreff: Re: [gmx-users] pressure_coupling
 
  Thanks for the information Flo.
  Before doing NPT I have already equilibrated my system by heating it
  from
  0K to
  300K in 300 ps, then the pressure has reached to 1 bar. Now while
  doing
  NPT I'm
  getting the excess pressure.
  Is there any problem with the coupling constant ? I am checking it by
  taking
  different tau_p values. Let's see.
 
 
  I don't think that playing around with the coupling constant will help
 you.
  You can set it to extreme values, but you won't see any difference.
  The coupling constant determines, how fast the system pressure should
  relax to the reference pressure. I would see a better possibility to
  play around by simulating for a longer time. Then observing the
  variation of the pressure in time, the size of the fluctuation and the
  excess pressure. Perhaps something will change, but I don't think so.
  I play around with the coupling constants but observed no change.
 
  Maybe, but this is really speculation, there is a problem with the
  combination of constraints and MTTK. Please check the archives of the
  user and developer list to obtain more information.
 
  /Flo
 
 
  On Wed, Nov 21, 2012 at 1:16 AM, Florian Dommert domm...@icp.uni-
  stuttgart.de wrote:
   -Urspr?ngliche Nachricht-
   Von: gmx-users-boun...@gromacs.org [mailto:gmx-users-
   boun...@gromacs.org] Im Auftrag von Justin Lemkul
   Gesendet: Dienstag, 20. November 2012 18:33
   An: Discussion list for GROMACS users
   Betreff: Re: [gmx-users] pressure_coupling
  
  
  
   On 11/20/12 12:29 PM, tarak karmakar wrote:
Thanks Justin for the quick reply.
Is there any problem with the algorithms ??
   
I have used Velocity Verlet , Nose-Hoover and MTTK combination.
SHAKE has been used to constrains the H-covalent bonds.
tau_t = 1 ps
tau_P = 1 ps
I got the mean pressure at ~130 bar.
   
Previously with the same initial coordinates I have used
Leap-Frog, NH, Parinello-Rehman with LINCS to constrain H-covalent
 bonds.
tau_t was 0.1 ps
and tau P was 2 ps.
The I have seen the pressure fluctuating around 1 bar( as
expected) So can you please inform me from where this problem is
coming - algorithms and/ tau_t and tau_P parameters ?
   
  
   I have no personal experience with the md-vv/MTTK combination.
   The way to test if there is a bug or something is to take an
   equilibrated system (as
   suggested
   before) and continue it with the desired parameters.  If they
   deviate or incorrectly report pressure, then there's probably a
   bug.  I'm not ready
   to
   conclude that until it is tested though.
  
   -Justin
  
  
   I once tried to use the same 

[gmx-users] which version it is

2012-11-19 Thread ABEL Stephane 175950
Hi, 

Probably the CHARMM27_protein+Charmm36_lipids version. AFAIK, the second 
version was not already converted in GROMACS format. 

Stephane

---

hello:

  I found a charmm36.tar.gz in Gromacs website


  GROMACS 4.5.4 version of the CHARMM36 force field files. These updated 
CHARMM lipids allow the all-atom simulations of membrane and 
membrane-protein systems without the use of surface tension. Check out 
the forcefield.doc for more information regarding these files
 71.65 kB15:42, 25 Sep 2012TomPiggot


I am just wondering, is the the one with 
CHARMM27_protein+Charmm36_lipids or it is CHARMM36_protein+CHARMM36_lipids?

thank you very much
best
Albert
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[gmx-users] which version it is

2012-11-19 Thread ABEL Stephane 175950
Hi Thomas and Justin, 

I agree with you, but I think that Albert asked if the GROMACS 4.5.4 version of 
the CHARMM36 force field files contain the newly  developed parameters for 
protein (also called CHARMM36) and described in 

Best, R. B., Zhu, X., Shim, J., Lopes, P. E. M., Mittal, J., Feig, M.,  
MacKerell, A. D. (2012). Optimization of the additive CHARMM all-atom protein 
force field targeting improved sampling of the backbone φ, ψ and side-chain χ1 
and χ2 dihedral angles. Journal of Chemical Theory and Computation, 
120718184839007. doi:10.1021/ct300400x

I said no

Sorry if it was not clear in my previous message

Stephane


--

Message: 1
Date: Mon, 19 Nov 2012 16:14:48 +
From: ABEL Stephane 175950 stephane.a...@cea.fr
Subject: [gmx-users] which version it is
To: gmx-users@gromacs.org gmx-users@gromacs.org
Message-ID:
3e39b768bb199548ab18f7289e7534af02d1c...@exdag0-b0.intra.cea.fr
Content-Type: text/plain; charset=us-ascii

Hi,

Probably the CHARMM27_protein+Charmm36_lipids version. AFAIK, the second 
version was not already converted in GROMACS format.

Stephane

---

hello:

  I found a charmm36.tar.gz in Gromacs website


  GROMACS 4.5.4 version of the CHARMM36 force field files. These updated
CHARMM lipids allow the all-atom simulations of membrane and
membrane-protein systems without the use of surface tension. Check out
the forcefield.doc for more information regarding these files
 71.65 kB15:42, 25 Sep 2012TomPiggot


I am just wondering, is the the one with
CHARMM27_protein+Charmm36_lipids or it is CHARMM36_protein+CHARMM36_lipids?

thank you very much
best
Albert


--

Message: 3
Date: Mon, 19 Nov 2012 16:28:28 +
From: Thomas Piggot t.pig...@soton.ac.uk
Subject: Re: [gmx-users] which version it is
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 50aa5e2c.4000...@soton.ac.uk
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

Hi,

As I understand it, the current and most up to date CHARMM protein force
field (as included in both the charmm27 and charmm36 force field
directories) is the CHARMM22 protein force field with the CMAP
correction. In other words there would be no difference between the two
options originally mentioned.

Cheers

Tom

ABEL Stephane 175950 wrote:
 Hi,

 Probably the CHARMM27_protein+Charmm36_lipids version. AFAIK, the second 
 version was not already converted in GROMACS format.

 Stephane

 ---

 hello:

   I found a charmm36.tar.gz in Gromacs website


   GROMACS 4.5.4 version of the CHARMM36 force field files. These updated
 CHARMM lipids allow the all-atom simulations of membrane and
 membrane-protein systems without the use of surface tension. Check out
 the forcefield.doc for more information regarding these files
  71.65 kB15:42, 25 Sep 2012TomPiggot


 I am just wondering, is the the one with
 CHARMM27_protein+Charmm36_lipids or it is CHARMM36_protein+CHARMM36_lipids?

 thank you very much
 best
 Albert

--
Dr Thomas Piggot
University of Southampton, UK.


--

Message: 4
Date: Mon, 19 Nov 2012 11:34:28 -0500
From: Justin Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] which version it is
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 50aa5f94.6090...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



On 11/19/12 11:28 AM, Thomas Piggot wrote:
 Hi,

 As I understand it, the current and most up to date CHARMM protein force field
 (as included in both the charmm27 and charmm36 force field directories) is the
 CHARMM22 protein force field with the CMAP correction. In other words there
 would be no difference between the two options originally mentioned.


There is indeed a CHARMM36 protein force field that is distinct from the one
included in CHARMM27 (which is, as you say, CHARMM22 + CMAP).

http://www.charmm.org/ubbthreads/ubbthreads.php?ubb=showflatNumber=30472

-Justin

--


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




--

Message: 5
Date: Mon, 19 Nov 2012 16:48:27 +
From: Thomas Piggot t.pig...@soton.ac.uk
Subject: Re: [gmx-users] which version it is
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 50aa62db.8010...@soton.ac.uk
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

I must have missed that one, thanks for the link!

So, to confirm, the protein force field in the CHARMM36 force field
contribution is the CHARMM22 protein force field with the CMAP
correction. The contribution is just for the updated CHARMM36 lipids.

Cheers

[gmx-users] Ryckeat-Bellemans Potential in Charmm forcefield

2012-11-15 Thread ABEL Stephane 175950
Hi,

CHARMM22star FF is a fork of CHARMM27 ff for proteins with several changes in 
some diedral parameters. It should be compatible with the others CHARMM 
parameters for biomolecules.

Stephane --
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[gmx-users] Ryckeat-Bellemans Potential in Charmm forcefield (XUEMING TANG)

2012-11-14 Thread ABEL Stephane 175950
Hello, 

Can you explain why you want to use/convert the RB form for your alkane 
dihedral angles instead of the usual CHARMM dihedral potential form available 
in charmm force field library available in the GROMACS distribution ?

Stephane
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[gmx-users] charge calculation........

2012-09-17 Thread ABEL Stephane 175950
Hi 

Since you want to use the AMBER force for your calculations, you will need to 
compute the RESP charges for your new residue (unprotoned TYR) and add the 
charges in your *rtp file. To compute the charges, you can use the RED.Server  
(http://q4md-forcefieldtools.org/REDS/).

It is not easy, so read the tutorials.

HTH 

Stephane


--

Dear All,

 I want to have one of tyrosine residues in my protein to
be unprotonated. I am using amber force field for the simulation. But
in aminoacid.rtp there is no entry for the unprotonated one. So I am
adding it by myself in to the .rtp file. Now I am bit confused with
the charge of the unprotonated one. How can I calculate the partial
charges for each and every atoms in  unprotonated tyrosine? Would
Gaussian/SCF be a good one to deal with this matter? Should I take the
tyrosine amino acid alone to calculate the charge in Gaussian ?
Please suggest me the proper method(s) to calculate the charge.

Thanks,

Tarak


--

Message: 6
Date: Mon, 17 Sep 2012 08:08:22 -0400
From: Justin Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] visualize trajectory
To: Shima Arasteh shima_arasteh2...@yahoo.com,Discussion list for
GROMACS users gmx-users@gromacs.org
Message-ID: 505712b6.3030...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



On 9/17/12 6:57 AM, Shima Arasteh wrote:
 Hi ,

 Which software is used to visualize a large mdrun output? For example 60 GB 
 trajectory file.


I think you should probably have a look at
http://www.gromacs.org/Documentation/How-tos/Reducing_Trajectory_Storage_Volume
before proceeding.  There are several programs that will work, provided you
don't exhaust the memory available on your workstation.

-Justin

--


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




--

Message: 7
Date: Mon, 17 Sep 2012 08:10:27 -0400
From: Justin Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] Regarding RMSD graph nalysis
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 50571333.1060...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



On 9/17/12 7:02 AM, naga sundar wrote:
 Dear gromacs users

 I run  20 ns MD simulation for protein mutant complexes. In RMSD analysis
 at ~9 ns sudden increase in the deviation was observed from 0.2 nm to 1.7
 nm and immediate fall was observed.

 I rerun the 20 ns simulation for the same molecule with same procedure.
 While analyzing the RMSD sudden increase in the deviation was observed (0.2
 nm to 1.7 nm) at the simulation period of ~12 ns.

 So i want to know  the reason

 For sudden rise and fall in RMSD values.

 Next, in first MD run this deviation was observed at ~9 ns (0.2 nm to 1.7
 nm) but while rerun the molecule with same procedure this deviation was
 observed at ~12 ns.


It sounds to me like your trajectories haven't correctly accounted for
periodicity.  g_rms does not elegantly handle sudden jumps across the box.  You
will need to work with trjconv.  Usually a simple trjconv -pbc mol -ur compact
-center does the trick for a simple protein, but for complexes it is often more
difficult.

http://www.gromacs.org/Documentation/Terminology/Periodic_Boundary_Conditions#Suggested_trjconv_workflow

-Justin

--


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




--

Message: 8
Date: Mon, 17 Sep 2012 21:48:23 +0900
From: Rajiv Gandhi graji...@gmail.com
Subject: Re: [gmx-users] Resuming of calculation from last *.cpt
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID:
capen9rxbkuf7mzjt8usbzreshwd9amrixh7xbp97ogtdzsb...@mail.gmail.com
Content-Type: text/plain; charset=ISO-8859-1

Dear all,

I have read few papers regarding the photo dissociation event such
as Myoglobin heme-ligand bond deletion to induce the photodissociation in
MD simulation.

Could you please tell me the procedure how can i perform the
photodissociation mechanism in Gormacs and which force field have to use,

 Also I want to study Upon the photo dissociation their structural changes
in MD. Thanks in advance,



Regards

Rajiv


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[gmx-users] Problems with Dihedral transition times for dodecane

2012-06-28 Thread ABEL Stephane 175950
Daer all, 

I am trying to compute the transition times (TT) for all the  angles in 
dodecane in the bulk (216) with gromacs 4.5.5

 I have constructed an index file with all  angles 
(C1C2C3C4C9C10C11C12) and for all the nine  angles (C*C*C*C*) and use 
the following command for each angle. 

### C1C2C3C4

 g_angle_mpi -f 216_Dodecane_run_1.xtc -of 
216_Dodecane_GRO54A7-Angle_9_Frac_Dihed.xvg -ot  
216_Dodecane_GRO54A7_1_Trans_Dihed.xvg -ov 216_Dodecane_GRO54A7_1_Avg_Dihed.xvg 
-b 3000 -e 1 -n 216_Dodecane_.ndx -type dihedral -noperiodic  Dih_1.txt

up to .

### C9C10C11C12 

 g_angle_mpi -f 216_Dodecane_run_1.xtc -of 
216_Dodecane_GRO54A7-Angle_8_Frac_Dihed.xvg -ot  
216_Dodecane_GRO54A7_8_Trans_Dihed.xvg -ov 216_Dodecane_GRO54A7_8_Avg_Dihed.xvg 
-b 3000 -e 1 -n216_Dodecane_.ndx -type dihedral -noperiodic  Dih_8.txt

And for the last one for all  angles

###  

g_angle_mpi -f 216_Dodecane_run_1.xtc -of 
216_Dodecane_GRO54A7-Angle_9_Frac_Dihed.xvg -ot  
216_Dodecane_GRO54A7_9_Trans_Dihed.xvg -ov 216_Dodecane_GRO54A7_9_Avg_Dihed.xvg 
-b 3000 -e 1 -n 216_Dodecane_.ndx -type dihedral -noperiodic  Dih_9.txt

I obtain the following results for all the dihedral 

### C1C2C3C4

Now calculating transitions...
Total number of transitions:  28828
Time between transitions:52.464 ps

### C2C3C4C5

Total number of transitions:  29821
Time between transitions:50.717 ps

### C3C4C5C6

Now calculating transitions...
Total number of transitions:  33654
Time between transitions:44.941 ps

### C4C5C6C7

Now calculating transitions...
Total number of transitions:  32206
Time between transitions:46.961 ps

### C5C6C7C8

Now calculating transitions...
Total number of transitions:  31356
Time between transitions:48.234 ps

### C6C7C8C9

Now calculating transitions...
Total number of transitions:  34014
Time between transitions:44.465 ps

### C7C8C9C10

Total number of transitions:  31840
Time between transitions:47.501 ps

### C8C9C10C11

Total number of transitions:  31885
Time between transitions:47.434 ps

### C9C10C11C12C13

Total number of transitions:  30362
Time between transitions:49.813 ps

And for all the  angles in the dodecane 

Total number of transitions:  90546
Time between transitions:50.110 ps
 
I am confused with these last values, where did they come from ? Why the Total 
number of transitions (90546): is not the sum of all the previous values. How 
these values are obtained. Note i have generated the index file for  as 
following: aC* | aC* |  aC* | aC* 

Your advices are welcome. 

Stephane





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[gmx-users] number of gauche - trans transitions with CHARMM36 and AMBER force fields

2012-06-26 Thread ABEL Stephane 175950
Dear all, 

I would like to compute the number of  gauche -- trans transitions (per 
ns) for for several alkanes. I know that I can use g_angle with -ot flag. But 
in the manual it is stated that this command works only for dihedrals with 
multiplicity 3. 

In CHARMM36 force field, for example,  the  dihedrals parameters have the 
following form:  

CTL2CTL2CTL2CTL39   0.000.6778082   ; New
CTL2CTL2CTL2CTL39   180.00  0.1966483   ; New
CTL2CTL2CTL2CTL39   0.000.43932 4   ; New
CTL2CTL2CTL2CTL39   0.000.7405685   ; New
CTL2CTL2CTL2CTL29   0.000.4225842   ; New
CTL2CTL2CTL2CTL29   180.00  0.5941283   ; New
CTL2CTL2CTL2CTL29   0.000.3096164   ; New
CTL2CTL2CTL2CTL29   0.000.4058485   ; New

So it is possible to use the g_angle functionality with this force field ? 
Probably I can comment the lines where the angle multiplicity is not equal tp 3 
and regenerate a  tpr file and use it with g_angle, right ?  

Stephane 

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[gmx-users] Re : How GROMACS calculate the energy of hydrogen bond

2012-05-31 Thread ABEL Stephane 175950
Hi, 

Here, my 2 cents worth. You can also estimate (roughly !!) the HB energy 
between two groups (say NH---CO) by using the Kabsch and Sander function  
described  in Kabsch, W.; Sander, C.  Biopolymers 1983, 22, 2577−2637).

Quoting: E = qlq2(1/r(0N) + l/r(CH) - l/r(OH) - l/r(CN))*f with q1 = 0.42e and 
q 2 = 0.20e, e being the unit electron charge and r(AB) the interatomic 
distance from A to B. In chemical units, r is in angstroms,
the dimensional factor f = 332, and E is in kcal/mol. A good H bond has about 
-3 kcal/mol binding energy. We choose a generous cutoff to allow for bifurcated 
H bonds and errors in coordinates and assign an H bond
between C=O of residue i and N-H of residue j if E is less than the cutoff, 
i.e., “Hbond(ij)=: [E  -0.5kcal/mole].”

To obtain  HB energy value E, you need only the distance between the donnor and 
acceptor groups. 

HTH 

Stephane 




--

Message: 2
Date: Thu, 31 May 2012 15:00:05 +0200
From: lloyd riggs lloyd.ri...@gmx.ch
Subject: Re: [gmx-users] How GROMACS calculate the energy of hydrogen
bond
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 20120531130005.302...@gmx.net
Content-Type: text/plain; charset=utf-8

Dear All,

I have no clue what specifically you are trying, but I feal bad for all the 
physicist and quantum chemist whom have provided the software and continued to 
develop it.

Scanning in my free time, it seems a large amount of confusion on what people 
are trying to do stems from differences in what is taught textbook wise for 
things.

For instance a hydrogen bond to a physicist is an integration over space in 3 
dimensions including time and probabilities of occupied spaces (atom position 
variabilities reflected even more in proteins, ie the necessity of multiple MD 
runs with different starting conformations), Vs.  an organic chemist whom has 
cut offs, ie angles between two points and set distances between two atoms 
which generally reflect the means of calculated chemical energies within a 
range (say 80-90% which represent means, but usually from raw small molecules 
as determinants), Vs. Biologist whom have tables which either use a set 
distance and angle and little account of variability over time (ie a hydrogen 
bond equals 1.4 kCal/mol reflecting the absolute mean), conformations in amino 
acids, etc...

I think with gromacs it is very precise, as even the smallest energies between 
two interacting atoms is taken into account with accuracy reflected by the 
force fields used, and how they were derived.

Good luck, your going to start seeing more and more a flood of biologist.

Stephan Watkins

 Original-Nachricht 
 Datum: Thu, 31 May 2012 19:54:04 +1000
 Von: Mark Abraham mark.abra...@anu.edu.au
 An: Discussion list for GROMACS users gmx-users@gromacs.org
 Betreff: Re: [gmx-users] How GROMACS calculate the energy of hydrogen bond

 On 31/05/2012 7:46 PM, Acoot Brett wrote:
  Hi Mark,
 
  It is confusing. As you know, for the same hydrogen bond in a protein,
  the related hydrogen bond angle and bond length can vary within a
  scope during the whole simulation process, however this small
  vibration of the hydrogen bond angle and length can lead to
  significant energy change, and correspondingly the energy of a
  hydrogen bond in simulation can be varied significantly. In comparison
  with hydrophobic effect, it would be too much is the energy of the
  hydrogen bond would be  not calculated  continuously.

 It isn't, if the model physics isn't paramtrized to include it
 explicitly - which is the case for all the force fields in GROMACS.

 
  Could you give some further clarification?

 What are trying to do? Measuring the strength of a hydrogen bond
 requires you identify a state with and without it and a path between
 them over which you can integrate.

 Mark

 
  Cheers,
 
  Acoot
 
  
  *From:* Mark Abraham mark.abra...@anu.edu.au
  *To:* Discussion list for GROMACS users gmx-users@gromacs.org
  *Sent:* Thursday, 31 May 2012 4:48 PM
  *Subject:* Re: [gmx-users] How GROMACS calculate the energy of
  hydrogen bond
 
  On 31/05/2012 4:42 PM, Acoot Brett wrote:
  Dear All,
  The value of the energy of the hydrogen bond has relation with
  distance and angle of the hydrogen bond related atoms. As for in the
  simulation process, the distance and angle of the hydrogen bond
  related atoms may change continuously. Will you please let me know
  based on which formula GROMACS calculated the value of the energy of
  the hydrogen bonds?
 
  There is no such formula used in MD force fields implemented in
  GROMACS. The only non-bonded interactions are the ones you already
  know about: electrostatics and VDW.
  Observables like hydrogen bonds and the hydrophobic effect arise from
  them.
 
  Mark
 
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[gmx-users] Re: What is the autocorrelation time

2012-05-18 Thread ABEL Stephane 175950
Hi Patrick, 

Your response  is indeed more useful  that my previous answer and with 
interesting links

thank for the pointers

Stephane

--

Message: 4
Date: Fri, 18 May 2012 10:51:35 +0200
From: Patrick Fuchs patrick.fu...@univ-paris-diderot.fr
Subject: Re: [gmx-users] What is the autocorrelation time
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4fb60d97.3010...@univ-paris-diderot.fr
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

Hi Chris,
I understand your question, this autocorrelation time puzzled me for a
long time as well. Not far from the interpretation you give, Scott
Feller defines it (http://dx.doi.org/10.1007/978-1-59745-519-0_7) as the
time a given observable takes to lose the memory of its previous state,
or in other words the time it takes to relax (that's why it's sometimes
called relaxation time). He also discusses it as a tool to choose the
block size for calculating an error estimate of an observable (one
single simulation can be used as independant samples if each block size
is  autocorrelation time).
We also had a nice discussion some years ago on the mailing list on free
energy calculation and error estimate:
http://lists.gromacs.org/pipermail/gmx-users/2007-May/027281.html. John
Chodera pointed me to a useful article from Wolfhard Janke (the link in
the discussion is broken, here's the new one:
http://www2.fz-juelich.de/nic-series/volume10/janke2.pdf). There you'll
find a rigorous mathematical definition of autocorrelation time. Quoting
this paper This shows more clearly that only every 2 tau_int
iterations the measurements are approximately uncorrelated and gives a
better idea of the relevant effective size of the statistical sample
(tau_int is the integrated autocorrelation time; as you said the
autocorrelation function is usually a single exponential, but sometimes
it's more complex and one needs to evaluate it by integration of the
autocorrelation function).
After all these considerations, the autocorrelation time can be seen as
a tool to assess the time that is needed to have a good estimate of an
observable: the simulation must be many many times longer than the
autocorrelation time. And sometimes it's directly related to
experimental observables (i.e. NMR relaxation experiments).
Hope it's useful,

Patrick

Le 16/05/2012 23:39, Christopher Neale a ?crit :
 Thank you Stephane.

 Unfortunately, neither of those links contains the information that I am
 seeking. Those links contain some example plots of autocorrelation
 functions including a discussion of time-spans over which the example
 time-series is autocorrelated and when it is not, but neither link
 defines the (exponential or integral) autocorrelation time except to
 show a plot and indicate when it is non-zero and when it fluctuates
 about zero.

 For example, I already know that the autocorrelation time describes the
 exponential decay of the correlation and that two values drawn from the
 same simulation are statistically independent if they are separated by a
 sufficient number of (accurate) autocorrelation times, but this
 information is not exactly a definition of the autocorrelation time.

 I am hoping to find a definition of the autocorrelation time in terms of
 the probability of drawing uncorrelated samples, although any complete
 definition will do.

 If anybody else has the time, I would appreciate it.

 Thank you,
 Chris.

 -- original message --

 Probably these links give you simple and clear response for your
 question
 http://idlastro.gsfc.nasa.gov/idl_html_help/Time-Series_Analysis.html
 and http://www.statsoft.com/textbook/time-series-analysis/ HTH Stephane



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___
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Dynamique des Structures et Interactions des Macromol?cules Biologiques
INTS, INSERM UMR-S665, Universit? Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-43-06-50-19
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[gmx-users] What is the autocorrelation time

2012-05-16 Thread ABEL Stephane 175950
Hi Chris, 

Probably these links give you simple and clear response for your question 

http://idlastro.gsfc.nasa.gov/idl_html_help/Time-Series_Analysis.html

and 

http://www.statsoft.com/textbook/time-series-analysis/

HTH 

Stephane 

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[gmx-users] amber-lipid

2012-02-06 Thread ABEL Stephane 175950
Hi, 

In my  opinion use Amber ff to simulate phospholipids is a bad idea. An 
alternative is to use GAFF with the good RESP charges. 

See these papers where several phospholipids are simulated with the GAFF ff.

(1) Siu, S. W. I.; Vácha, R.; Jungwirth, P.; Böckmann, R. A.; Shirley, S. W. 
I.; Robert, V.; Pavel, J.; Rainer, A. B. The Journal of chemical physics 2008, 
128, 125103.
(2) Rosso, L.; Gould, I. R. J. Comput. Chem. 2008, 29, 24-37.

HTH

Stephane

-

Message: 7
Date: Mon, 6 Feb 2012 14:04:21 +0200
From: ???  rayevsk...@gmail.com
Subject: [gmx-users] amber-lipid
To: gmx-users@gromacs.org
Message-ID:
cab6cz-kcannphwurmpho_zqdcafknhxej1aa0tjadk+0cek...@mail.gmail.com
Content-Type: text/plain; charset=ISO-8859-1

Hi
Is it possible to use amber forcefield with lipid parameters like it
was done with gmx in KALP-15 in DPPC tutorial?
I have to use amber forcefield as it is neccessary for parametrization
of my ligand and its stecking interactions.

Thank you very much

--



Nemo me impune lacessit


--

Message: 8
Date: Mon, 6 Feb 2012 17:39:54 +0530
From: Anushree Tripathi anushritripa...@gmail.com
Subject: Re: [gmx-users] problem with nvt equilibration
To: jalem...@vt.edu, Discussion list for GROMACS users
gmx-users@gromacs.org
Message-ID:
CAAx43BzE=yB3FK=2lcktmul9+tmpj_hb6wqrx6ibmd60p8q...@mail.gmail.com
Content-Type: text/plain; charset=iso-8859-1

Will you please send me the basic tutorial in which I can find how to use
-n option in  grompp -f nvt.mdp -c em.gro -p topol.top -o nvt.tpr command.

On Mon, Feb 6, 2012 at 5:17 PM, Justin A. Lemkul jalem...@vt.edu wrote:



 Anushree Tripathi wrote:

 where should I use -n option in the command (i.e., grompp -f nvt.mdp -c
 em.gro -p topol.top -o nvt.tpr).Please tell me.


 I would suggest you refer to grompp -h and/or go through some basic
 tutorial material so that you can get a feel for command line options and
 how to apply them.

 -Justin

  On Mon, Feb 6, 2012 at 4:58 PM, Mark Abraham mark.abra...@anu.edu.aumailto:
 mark.abra...@anu.edu.**au mark.abra...@anu.edu.au wrote:

On 6/02/2012 8:28 PM, Anushree Tripathi wrote:

Inspite of having DPPC in index file,when I run the command (
i.e., grompp -f nvt.mdp -c em.gro -p topol.top -o nvt.tpr ),I am
getting the error:

Group DPPC not found in indexfile.
Maybe you have non-default goups in your .mdp file, while not
using the '-n' option of grompp.
In that case use the '-n' option.

Now, what to do? Please guide me.


You seem not to have used the -n option. You could try using it. :)

Mark
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 Department of Biochemistry
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 jalemkul[at]vt.edu | (540) 231-9080
 http://www.bevanlab.biochem.**vt.edu/Pages/Personal/justinhttp://www.bevanlab.biochem.vt.edu/Pages/Personal/justin

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[gmx-users] Half double pair list method in GROMACS [update]

2011-12-03 Thread ABEL Stephane 175950
Hi Sai

I am also agree with Christ, your approach seems also correct to me. But don't 
to forget to test your change to be sure, by doing a single point energy test 
as it is said in the Christ's message.

Good luck

Stephane



--

Message: 1
Date: Fri, 02 Dec 2011 16:07:19 -0500
From: Chris Neale chris.ne...@utoronto.ca
Subject: [gmx-users] Half double pair list method in GROMACS [update]
To: gmx-users@gromacs.org
Message-ID: 4ed93e07.5070...@utoronto.ca
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

What you have done seems alright. I didn't look closely enough to be
sure though. One of the good things about this method is that you can
easily test it yourself. To do this, create two different .gro files,
one containing the atoms from one ff and the other containing the other
atoms. For each, do separate zero-step mdrun evaluations of their
energies under (a) their original ff, and (b) the combined HEDP ff that
you have constructed. The energy evaluations should be the same once you
account for rounding errors. Then all that is left is for you to be
certain that you didn't cause any problems for nonbonded interactions.
Note that you'll need to return to the original atomtypes for the first
half of this test.

Note that the only thing that the HEDP method is intended to perturb is
the 1-4 interactions (and by perturb I mean that they will now be correct).

Chris.

  -- original message --

Hi Stephane  Chris,
I followed all the threads posted by you two.
I have a protein using ff99SB and GLYCAM for sugars. I have a disaccharide
bound to protein. In xleap of AMBERTOOLS, I use the GLYCAM and ff99SB to
generate the topology and coordinate files. I did the tests as Chris'
original posts and by Stephane.
The 1-4 interaction terms match for sugar alone and protein alone with HEDP
method.
When I generate topology and coordinate files with xleap of AMBER, there
are three atom types that are common to protein and sugar. The atom types
for my case are H1, OH and HO.
Since for protein pairtypes using ff99SB, the epsilon has to be divided by
10 and pairs section be replicated five times and for sugar the epsilon in
the pairtypes be divided by six and replicated six times, I am a little
concerned about the three atomtypes that are common.
So what I did was to change the atomtypes of sugar as H1S, OHS HOS for
sugar and H1, OH and HO for protein and I made the changes accordingly in
the pairtypes section for protein and sugar.
Is this a valid approach?
Any suggestion will be helpful.

To make things little more clear:
H1H10.  0.  A   2.47135e-01  6.56888e-02
;originally obtained using amb2gmx.pl
H1S  H1S  0.  0.  A   2.47135e-01  6.56888e-02 ;Glycam
Hydrogen of Sugar ( I changed this so that the common atom types be
separated)

In the ffnonbonded_complex_mod.itp:
;;using combination rule of 2
[ pairtypes ]
;;for protein
H1  H1  1   0.247135000 0.006568880 ;the epsilon is divided
by 10

;;for sugar

  H1S   H1S 1   0.24713500  0.010948133 ;the epsilon is divided
by 6


Thanks for your time,


Regards
Sai


On Mon, Sep 5, 2011 at 11:33 AM, ABEL Stephane 175950
Stephane.ABEL at cea.frwrote:

  Dear All,
 
  Below a little update and results about the application of half double
  pair list method to scale properly the Coulombic 1-4 interactions in case
  of a system where the AMBER99SB (fudgeLJ=0.5 and fudgeLJ=0.8333) and
  GLYCAM06 (fudgeLJ=1.0 and fudgeLJ=1.0) force fields are combined.
 
  I have followed the 4 steps described in [1] and used the following
values
  in my forcefield.itp file
 
  [ defaults ]
  ; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
  1   2   yes 1.0 0.16
  #include ffnonbonded_mod.itp
  ;#include ffnonbonded.itp
  #include ffbonded.itp
 
  I used two different topology files for the glycolipid (bDM) and the
  peptide. One with (*_mod.itp) with pair list parameters duplicated 6
times
  (bDM) and 5 times (peptide) and with single pair list (*_no_mod.itp) as
  decribed in [1].
 
  TESTING:
 
  Three 3 different systems were examined:
 
  A. A first system containing 1 glycolipid (bDM)  in water cubic box
  B. A second system with 1 peptide in TIP3P water
  C. And a third system with 1 peptide and 1 glycolipid in water cubic box
 
  To obtain the glycolipid and peptide energy pairs, I did one step of
MD in
  NVT ensemble with the *.mdp file given in [2] with different
energygrps and
  tc_grps.
  For 1. energygrps and tc_grps = bDM SOL
  For 2. energygrps and tc_grps = Protein SOL
  For 3. energygrps and = Protein bDM SOL
 
  bDM/water system
 
  Test_A1
 
  ## Control with GLYCAM force field fudgeLJ fudgeQQ parameters and  the
  *_no_mod.itp file :
  ##; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
  ##  1   2   yes 1.0

[gmx-users] diffusion of the water at the micelle surface

2011-11-27 Thread ABEL Stephane 175950
Hi Chris,  Druz

Thank you very much for your reply. Indeed I have read several papers where the 
diffusion of water at the membrane surface have been computed. Since the 
diffusion of the interfacial water is an useful properties to examine the 
micelle/surface irregularities, I would hope that this option exist in gromacs. 
Unfortunately, it is not the case, so i will try your suggestions .

Stephane


--

Message: 6
Date: Sat, 26 Nov 2011 10:17:10 -0500
From: chris.ne...@utoronto.ca
Subject: [gmx-users] diffusion of the water at the micelle surface
To: gmx-users@gromacs.org
Message-ID: 2026101710.bbl5wl376s04c...@webmail.utoronto.ca
Content-Type: text/plain;   charset=ISO-8859-1; DelSp=Yes;
format=flowed

When people do this for lipid bilayers, they compute depth-dependent
diffusion profiles (often diffusion is computed separately for lateral
diffusion and diffusion along the bilayer normal). Sounds like you
might do something similar. I doubt that the standard gromacs tools
will do this for you. If you don't hear from anybody about how to do
this, then I'd suggest that you simply use g_dist to get the
time-dependent distance for each water molecule and then use g_traj to
output the coordinates of each water molecule and then script it
yourself after reading one of the papers where people compute
depth-dependent diffusion profiles for a lipid bilayer.

Chris.

-- original message --

I would like to compute the translational diffusion around the micelle
surface. I know that I can select the water molecules at x distance of the
micelle surface with g_select (right ?) but how to use this file generated
by g_select to compute de diffusion, since the index and/or the number of
water will change with the simulation time .



Thank you for your response



Stephane



--

Message: 7
Date: Sat, 26 Nov 2011 23:22:59 +0800
From: lina lina.lastn...@gmail.com
Subject: Re: [gmx-users] diffusion of the water at the micelle surface
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID:
cag9cjmnxasa7nj+8cgkhavodvobluvzqqruqrcsxzs37m6z...@mail.gmail.com
Content-Type: text/plain; charset=ISO-8859-1

On Sat, Nov 26, 2011 at 11:17 PM,  chris.ne...@utoronto.ca wrote:
 When people do this for lipid bilayers, they compute depth-dependent
 diffusion profiles (often diffusion is computed separately for lateral
 diffusion and diffusion along the bilayer normal). Sounds like you might do
 something similar. I doubt that the standard gromacs tools will do this for
 you. If you don't hear from anybody about how to do this, then I'd suggest
 that you simply use g_dist to get the time-dependent distance for each water
 molecule and then use g_traj to output the coordinates of each water
 molecule and then script it yourself after reading one of the papers where
 people compute depth-dependent diffusion profiles for a lipid bilayer.

 Chris.

 -- original message --

 I would like to compute the translational diffusion around the micelle
 surface. I know that I can select the water molecules at x distance of the
 micelle surface with g_select (right ?) but how to use this file generated
 by g_select to compute de diffusion, since the index and/or the number of
 water will change with the simulation time .

You may try g_density, choose different time interval.




 Thank you for your response



 Stephane

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[gmx-users] Calculation of the isothermal compressibility with g_energy for a box with different components.

2011-09-22 Thread ABEL Stephane 175950
Hi GMXusers,

I know that the g_energy can be used to compute/estimate the adiabatic and 
isothermal compressibility values of the simulation box when the TEMP, volume 
and nmol values are given. nmol can be easily given for a pure solvent but when 
I have a two (or more) different species in the my system how to choose the 
nmol value to obtain the compressibility of the system. 

I know that I can also manually obtained the isothermal compressibility value 
at T manually from the simulation box volume  but i would like to use g_energy 
to verify my results

Thanks in advance for your help.

Stephane--
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[gmx-users] Half double pair list method in GROMACS [update]

2011-09-05 Thread ABEL Stephane 175950
Dear All,

Below a little update and results about the application of half double pair 
list method to scale properly the Coulombic 1-4 interactions in case of a 
system where the AMBER99SB (fudgeLJ=0.5 and fudgeLJ=0.8333) and GLYCAM06 
(fudgeLJ=1.0 and fudgeLJ=1.0) force fields are combined.

I have followed the 4 steps described in [1] and used the following values in 
my forcefield.itp file

[ defaults ]
; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
1   2   yes 1.0 0.16
#include ffnonbonded_mod.itp
;#include ffnonbonded.itp
#include ffbonded.itp

I used two different topology files for the glycolipid (bDM) and the peptide. 
One with (*_mod.itp) with pair list parameters duplicated 6 times (bDM) and 5 
times (peptide) and with single pair list (*_no_mod.itp) as decribed in [1].

TESTING:

Three 3 different systems were examined:

A. A first system containing 1 glycolipid (bDM)  in water cubic box
B. A second system with 1 peptide in TIP3P water
C. And a third system with 1 peptide and 1 glycolipid in water cubic box

To obtain the glycolipid and peptide energy pairs, I did one step of MD in NVT 
ensemble with the *.mdp file given in [2] with different energygrps and tc_grps.
For 1. energygrps and tc_grps = bDM SOL
For 2. energygrps and tc_grps = Protein SOL
For 3. energygrps and = Protein bDM SOL

bDM/water system

Test_A1

## Control with GLYCAM force field fudgeLJ fudgeQQ parameters and  the 
*_no_mod.itp file :
##; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
##  1   2   yes 1.0 1.0
Epot (kJ/mol)Coul-SR  LJ-SRCoul-14  LJ-14
bDM-bDM   -4.00855e+02   -3.71401e+012.03406e+032.79234e+02

Test_A2

 with the topology *_mod.itp file and the directive
##; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
##  1   2   yes 1.0 0.16
Epot (kJ/mol)Coul-SR  LJ-SRCoul-14  LJ-14
bDM-bDM   -4.00855e+02   -3.71401e+012.03406e+032.79234e+02

Test_A3

 with the topology *_no_mod.itp file and the directive
##; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
##  1   2   yes 1.0 0.16
Epot (kJ/mol)Coul-SR  LJ-SRCoul-14  LJ-14
bDM-bDM   -4.00855e+02   -3.71401e+013.39010e+022.79234e+02

Coul-14 energy for bDM-bDM in Test_A1 = Coul-14 energy in Test_A2 -- OK !
Coul-14 energy for bDM-bDM Test_A3 is 6 smaller than Coul-14 energy in Test_A1 
and Test 2 --- OK !

peptide/water system

Test_B1

 Control with AMBER force field fudgeLJ fudgeQQ parameters, the 
*_no_mod.itp file
##; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
##  1   2   yes 0.5  0.8333
Epot (kJ/mol)Coul-SR  LJ-SRCoul-14  LJ-14
Protein-Protein   -1.49026e+03   -4.12114e+023.80551e+036.55321e+02

Test_B2

 Control with the peptide *_no_mod.itp file and the directive
##; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
##  1   2   yes 1.0 0.166
Epot (kJ/mol)Coul-SR  LJ-SRCoul-14  LJ-14
Protein-Protein   -1.49026e+03   -4.12114e+027.61132e+021.31064e+03

Test_B3

 With the peptide *_mod.itp file and the directive
##; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
##  1   2   yes 1.0 0.16
Epot (kJ/mol)Coul-SR  LJ-SRCoul-14  LJ-14
Protein-Protein   -1.49026e+03   -4.12114e+023.80566e+036.55320e+02

Coul-14 and LJ-14 energies for Protein-Protein in Test_B3 are 5 times Coul-14 
and 2 times LJ-14 energies, respectively, than in Test_B1 --- OK !
Coul-14 and LJ-14 energies for Protein-Protein in Test_B3 = Coul-14 and LJ-14 
energies in Test_B1 --- OK !

peptide/bDM/water system

Test_C1

## Control with the peptide and the bDM *_mod.itp topology files and the 
directive
##; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ
## 1   2   yes 1.0 0.16
Epot (kJ/mol)Coul-SR  LJ-SRCoul-14  LJ-14
Protein-Protein   -1.48386e+03   -3.99146e+023.79532e+036.53553e+02
bDM-bDM   -3.69788e+02   -3.51804e+012.00228e+032.25026e+02

Test_C2

## Control with the peptide and the bDM *no_mod.itp topology files and  the 
directive
Epot (kJ/mol)Coul-SR  LJ-SRCoul-14  LJ-14
Protein-Protein   -1.48386e+03   -3.99146e+027.59063e+021.30711e+03
bDM-bDM   -3.69788e+02   -3.51804e+013.33713e+022.25026e+02

bDM-bDM Coul-14 energy in Test_C2 is 6 times smaller, respectively, than in the 
Test_C1  --- OK !
Protein-Protein Coul-14 and LJ1-4 energies 

[gmx-users] Half double pair list method in GROMACS

2011-09-01 Thread ABEL Stephane 175950
Chris,

Thank you for your confirmation. I did the changes. I am currently doing some 
tests, I will send you a feedback about the results off-list (if you want) 
shortly.

A bientôt 

Stéphane




Message: 1
Date: Thu, 01 Sep 2011 14:38:53 -0400
From: chris.ne...@utoronto.ca
Subject: [gmx-users] Half double pair list method in GROMACS
To: gmx-users@gromacs.org
Message-ID: 20110901143853.537ln0dj94w4w...@webmail.utoronto.ca
Content-Type: text/plain;   charset=ISO-8859-1; DelSp=Yes;
format=flowed

It's a typo, but it's in the discussion and not in the do this part
of the method so I decided not to mention it. I don't see another
question in this post, so I hope that you have figured things out.
Note that I have never tested the exact implementation that I
suggested in that April email. It seems like it should work just fine,
but it is numerically different than the OPLS/Berger combination so
there is no way to be sure until you check the energies as I
suggested. I'd be interested to have you report back on the energy
matching once you have done the tests.

Good luck,
Chris.

-- original message --

Hi Chris,

Sorry to repost the same question, but I have really tested your method the
last few weeks. My question about the gen-pairs directive come from the fact
that I have read a message from you

http://lists.gromacs.org/pipermail/gmx-users/2006-September/023761.html

Where you detailed how to use the Berger and OPLS force fields together in
the same system. By reading carefully the meaning of the gen-pairs
directive, I found several errors in my force field.

BYW in your previous message

http://lists.gromacs.org/pipermail/gmx-users/2011-April/060839.html

In the step 3, I think there is a typo, it is values/10 instead of
values/12. Am I right?

Thank you again

Stephane



Dear Stephane:

We discussed this in April:

http://lists.gromacs.org/pipermail/gmx-users/2011-April/060839.html

At that time I also provided a method for you to verify your files
(and the method in general).

It is possible for you to answer your gen-pairs question by looking
into the manual and reading about pairs, gen-pairs, and pairtypes. I
think that this is one case where you would benefit more from fully
understanding how these parts work than from a direct answer to your
question.

If you are having problems, please provide a whole bunch more
information on the problems that you are seeing. If, on the other
hand, you are just looking for somebody other than me to comment on
the accuracy of the April post, then that is perfectly fine with me,
but you should state that.

Chris.


-- original message --

Dear All,



I try to apply the half double pair list method for a system containing a
glycolipid surfactant and a peptide modeled with the GLYCAM and AMBER99SB
force field. Briefly what I did :



1- I have changed the  forcefield.itp like this



[ defaults ]

; gen_pairs set explicitly --- gen-pairs = no

; nbfunccomb-rule   gen-pairs   fudgeLJ fudgeQQ

;1   2   yes 0.5 0.8333 --- for
AMBER99SB only

1   2no 1.0 0.16 ---
 for both GLYCAM et AMBER99SB

;1   2yes  1.0 1.0 -- for
GLYCAM only



#include ffnonbonded_mod.itp

#include ffbonded.itp



2- For the surfactant, I have calculated the pair-types interactions
manually with the comb-rule = 2 and divided the values /6 and added these
values in [pairtypes] section in the ffnonbonded_mod.itp files



3- For the peptide, I have calculated the pair-types interactions manually
comb-rule = 2 and divided the values /10 and added these values in
[pairtypes] section in the ffnonbonded_mod.itp files.



4- In the surfactant topology file I have repeated 6 times the [pairs]
directives 0.16*6 ~=10



5 - In the peptide topology file I have repeated 5 times the [pairs]
directives 0.16*5 ~= 0.8333



Is it correct ?



However I have a little doubt about gen-pairs directive should I have set
it to no or yes. in a previous message with a similar problem, the gen
directive was set yes



http://lists.gromacs.org/pipermail/gmx-users/2006-September/023761.html



Thank you for your help



Stephane




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[gmx-users] GROMOS45ACARBO force fields in the GROMACS format.

2011-04-06 Thread ABEL Stephane 175950
Dear All,  

I would like to perform some MD of disaccharides in water using GROMACS and the 
new ff for sugars GROMOS45ACARBO from Hansen and unenberger(JCC, 32, 6, 2011). 
Does somebody have these parameters in the GROMACS format (e.g. the *.itp 
files) and want to share them with me. 

Thank you in advance.

Stéphane

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[gmx-users] solvation box for say 50mM chaps solution

2011-01-18 Thread ABEL Stephane 175950
HI shahid,
 
you can also use the following formula
 
((N_chaps/(Nw*Vw))/6.02214179)*1=density you want in (Mol) 
Where 
- N_chaps is the number of  chaps mol. 614.88 g (from wikipedia)
- Nw : number of water mol. 
- Vw : volume of water (30 A3 in ambiant condition) ~
- 6.02214179 Avogadro number 
- 1 : correction factor 
 
I hope this will help
 
S

On 18/01/2011 10:33 PM, shahid nayeem wrote:
 Dear Gmx User
 I want to prepare a solvation box for say 50mM chaps solution. The
 density is not known.

An aqueous solution has density close to 1g/mL. That's enough to make an
estimate of the number of molecules, which you can refine if you don't
like the resulting equilibrated size/density/concentration/whatever.

Mark

 How should I start calculating the number of chaps molecule and number
 of water molecule required for say 6X6X6 size box, which after
 equilibriation should give the exact strength of the solution. For
 Urea and guanidinium I know the references and mail archive has many
 suggestion but how I should proceed with this new solvation box.

 msnayeem



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[gmx-users] perfluorohexane pdb

2011-01-10 Thread ABEL Stephane 175950
Re hi Marcelo,
 
Below the perfluorohexane molecule in the pdb format construct with the 
Discovery Studio Visualizer v2.5
 
REMARK   Accelrys Discovery Studio PDB file
REMARK   Created:  Mon Jan 10 20:52:13 Paris, Madrid 2011
HETATM1  C1  0 -11.336  -0.581   0.212  1.00  0.00   C  
HETATM2  C2  0 -10.035  -0.174  -0.542  1.00  0.00   C  
HETATM3  C3  0  -8.771  -0.197   0.410  1.00  0.00   C  
HETATM4  C4  0  -7.458   0.219  -0.369  1.00  0.00   C  
HETATM5  C5  0  -6.194   0.196   0.583  1.00  0.00   C  
HETATM6  C6  0  -4.893   0.603  -0.171  1.00  0.00   C  
HETATM7  F7  0 -11.590   0.293   1.248  1.00  0.00   F  
HETATM8  F8  0 -11.226  -1.862   0.712  1.00  0.00   F  
HETATM9  F9  0 -12.391  -0.539  -0.675  1.00  0.00   F  
HETATM   10  F10 0 -10.216   1.097  -1.046  1.00  0.00   F  
HETATM   11  F11 0  -9.852  -1.059  -1.582  1.00  0.00   F  
HETATM   12  F12 0  -8.977   0.685   1.449  1.00  0.00   F  
HETATM   13  F13 0  -8.613  -1.470   0.913  1.00  0.00   F  
HETATM   14  F14 0  -7.617   1.493  -0.871  1.00  0.00   F  
HETATM   15  F15 0  -7.252  -0.663  -1.408  1.00  0.00   F  
HETATM   16  F16 0  -6.377   1.082   1.623  1.00  0.00   F  
HETATM   17  F17 0  -6.013  -1.074   1.087  1.00  0.00   F  
HETATM   18  F18 0  -5.004   1.884  -0.671  1.00  0.00   F  
HETATM   19  F19 0  -4.639  -0.271  -1.207  1.00  0.00   F  
HETATM   20  F20 0  -3.839   0.561   0.716  1.00  0.00   F  
END
 
The structure needs some changes (atom names ?) and minimization steps to relax 
the structure. 
 
hope this helps 
 
Stephane
 
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[gmx-users] RE : gmx-users Digest, Vol 81 , Issue 58

2011-01-10 Thread ABEL Stephane 175950
Hi Marcelo,  
 
I can send you a pdb file of this molecule construct with Discovery visualizer 
2.5 if you are interested. You will need only to change the atom names and a do 
several minimzation steps. 
 
Stephane
 
On Mon, 2011-01-10 at 17:59 +, Marcelo Silva wrote:

 Hi everybody,

 I was looking for the structure of perfluorohexane to create the pdb
 file to use with gromacs but I can't find anywhere. I have also looked
 in pdb databases. Do you know any paper where the structure is
 reported? Is it possible to use gromacs to do the geometry
 optimization?

 Thank you

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[gmx-users] perfluorohexane pdb... again

2011-01-10 Thread ABEL Stephane 175950
Hi Justin 
 
As i have said in the message the pdb file needs probably some (small) changes. 
emacs (or vi) and vmd or rasmol are our friends ;) 
 
 
Below the pdb file in the correct format (tested with rasmol and vmd)
 
REMARK   Accelrys Discovery Studio PDB file
REMARK   Created:  Mon Jan 10 20:52:13 Paris, Madrid 2011
ATOM  1  C1  HEF 0 -11.336  -0.581   0.212  1.00  0.00   C  
ATOM  2  C2  HEF 0 -10.035  -0.174  -0.542  1.00  0.00   C  
ATOM  3  C3  HEF 0  -8.771  -0.197   0.410  1.00  0.00   C  
ATOM  4  C4  HEF 0  -7.458   0.219  -0.369  1.00  0.00   C  
ATOM  5  C5  HEF 0  -6.194   0.196   0.583  1.00  0.00   C  
ATOM  6  C6  HEF 0  -4.893   0.603  -0.171  1.00  0.00   C  
ATOM  7  F7  HEF 0 -11.590   0.293   1.248  1.00  0.00   F  
ATOM  8  F8  HEF 0 -11.226  -1.862   0.712  1.00  0.00   F  
ATOM  9  F9  HEF 0 -12.391  -0.539  -0.675  1.00  0.00   F  
ATOM 10  F10 HEF 0 -10.216   1.097  -1.046  1.00  0.00   F  
ATOM 11  F11 HEF 0  -9.852  -1.059  -1.582  1.00  0.00   F  
ATOM 12  F12 HEF 0  -8.977   0.685   1.449  1.00  0.00   F  
ATOM 13  F13 HEF 0  -8.613  -1.470   0.913  1.00  0.00   F  
ATOM 14  F14 HEF 0  -7.617   1.493  -0.871  1.00  0.00   F  
ATOM 15  F15 HEF 0  -7.252  -0.663  -1.408  1.00  0.00   F  
ATOM 16  F16 HEF 0  -6.377   1.082   1.623  1.00  0.00   F  
ATOM 17  F17 HEF 0  -6.013  -1.074   1.087  1.00  0.00   F  
ATOM 18  F18 HEF 0  -5.004   1.884  -0.671  1.00  0.00   F  
ATOM 19  F19 HEF 0  -4.639  -0.271  -1.207  1.00  0.00   F  
ATOM 20  F20 HEF 0  -3.839   0.561   0.716  1.00  0.00   F  
END
 
Stephane

 Re hi Marcelo,

 Below the perfluorohexane molecule in the pdb format construct with 
 the Discovery Studio Visualizer v2.5

 REMARK   Accelrys Discovery Studio PDB file
 REMARK   Created:  Mon Jan 10 20:52:13 Paris, Madrid 2011
 HETATM1  C1  0 -11.336  -0.581   0.212  1.00  0.00   
 C
 HETATM2  C2  0 -10.035  -0.174  -0.542  1.00  0.00   
 C
 HETATM3  C3  0  -8.771  -0.197   0.410  1.00  0.00   
 C
 HETATM4  C4  0  -7.458   0.219  -0.369  1.00  0.00   
 C
 HETATM5  C5  0  -6.194   0.196   0.583  1.00  0.00   
 C
 HETATM6  C6  0  -4.893   0.603  -0.171  1.00  0.00   
 C
 HETATM7  F7  0 -11.590   0.293   1.248  1.00  0.00   
 F
 HETATM8  F8  0 -11.226  -1.862   0.712  1.00  0.00   
 F
 HETATM9  F9  0 -12.391  -0.539  -0.675  1.00  0.00   
 F
 HETATM   10  F10 0 -10.216   1.097  -1.046  1.00  0.00   
 F
 HETATM   11  F11 0  -9.852  -1.059  -1.582  1.00  0.00   
 F
 HETATM   12  F12 0  -8.977   0.685   1.449  1.00  0.00   
 F
 HETATM   13  F13 0  -8.613  -1.470   0.913  1.00  0.00   
 F
 HETATM   14  F14 0  -7.617   1.493  -0.871  1.00  0.00   
 F
 HETATM   15  F15 0  -7.252  -0.663  -1.408  1.00  0.00   
 F
 HETATM   16  F16 0  -6.377   1.082   1.623  1.00  0.00   
 F
 HETATM   17  F17 0  -6.013  -1.074   1.087  1.00  0.00   
 F
 HETATM   18  F18 0  -5.004   1.884  -0.671  1.00  0.00   
 F
 HETATM   19  F19 0  -4.639  -0.271  -1.207  1.00  0.00   
 F
 HETATM   20  F20 0  -3.839   0.561   0.716  1.00  0.00   
 F
 END

 The structure needs some changes (atom names ?) and minimization 
 steps to relax the structure.


If you want Gromacs to read this file, it also needs residue names.  
PDB format is fixed, and this set of coordinates is not correctly 
formatted, so it will undoubtedly cause problems in Gromacs.

-Justin

 hope this helps

 Stephane

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[gmx-users] tfe.gro

2010-11-30 Thread ABEL Stephane 175950
Hi Hengameh
 
Below, my TFE.gro (with the atom names for CHARMM Cgenff) i used it previously 
for md. You can easely translated in others ff you use
 
9
1TFE O11   0.397   1.386   1.484  0.4892 -0.3653 -0.3242
1TFEHO12   0.446   1.346   1.557  0.8382 -0.5070 -0.6322
1TFEH113   0.334   1.332   1.295  1.2033 -0.8553 -0.5343
1TFEH124   0.436   1.209   1.380  2.6521  2.1877  0.2597
1TFE C15   0.355   1.285   1.393  0. -0.4118 -0.0512
1TFEF216   0.186   1.128   1.352  0.1711 -0.0500  0.0270
1TFEF227   0.117   1.302   1.447 -0.1931  0.5088 -0.2066
1TFEF238   0.235   1.159   1.557  0.0214  0.0727 -0.2415
1TFE C29   0.224   1.222   1.439 -0.3522  0.2823 -0.0958
 
and the TFE.pdb file used to obtain the gro file above
 
ATOM  1  O1   TFE 1  1.9123 -0.2235  0.
ATOM  2  HO1  TFE 1  2.7589  0.2000  0.
ATOM  3  H11  TFE 1  0.9282  1.3623 -0.8827
ATOM  4  H12  TFE 1  0.9282  1.3623  0.8827
ATOM  5  C1   TFE 1 -0.4189  0.0062 -0.
ATOM  6  F21  TFE 1 -1.4055  0.8930 -0.
ATOM  7  F22  TFE 1 -0.5650 -0.7556 -1.0660
ATOM  8  F23  TFE 1 -0.5650 -0.7556  1.0660
ATOM  9  C2   TFE 1  0.9031  0.7318 -0. 
 
Hope it helps
 
Stefane
 

 
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[gmx-users] Questions about REMD calculations

2010-10-14 Thread ABEL Stephane 175950
Dear all, 
 
I come back to you for several questions about the futures replica-exchange 
calculations that i would like to perform. The system of interest will contain 
12 peptides (with 7 residues each) and 4 water molecules, it come from a 
previous MD performed in NPT ensemble. With these systems, i would like to 
study the aggregation process between the peptides.
 
After reading several paper about REMD method and playing with the Temperature 
generator for REMD-simulations web server (http://folding.bmc.uu.se/remd/), i 
suspect that this system is too big for REMD. Indeed if use the following 
parameters in the webserver
 
Pdes 0.2
Temperature range 290 - 600
Number of water molecules 41380
Number of protein atoms 1092
Including all H ~ 1656
Number of hydrogens in protein ~ 240
Number of constraints ~ 1092
Number of vsites ~ 0
Number of degrees of freedom ~ 250464
Energy loss due to constraints 520.59 (kJ/mol K)

I obtain 271 replicas (ouch !!) . If i assume that for each replica app. 16 
CPU, The simulations will be too big and will cost a lot CPU time. 
 
So my question is can i reduce safely the number of water in system to reduce 
the number of replicas ? 
 
For example for 1 mol of water the number of replicas will be 135. It is 
not bad. It is a good option to overcome this limitation. 

I have also read the number of replicas can be significantly reduced by using 
variants of REMD for example replica exchange with solute tempering (REST) from 
Berne and co-workers. Is this method is implemented in GROMACS ?
 
Or Can i use the REMD in implicit solvant for example with the coarse grain 
OPEP force field as described in Chebaro, et al. (2008).J. Phys. Chem. B 
113(1): 267-274. or by Wang and Voth in J. Phys. Chem. B 112(41): 13079-13090. 
 
Any advices and comments are welcome 
 
Stefane
 
--
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CEA Saclay DSV/IBITEC-S/SB2SM
91191 Saclay, FRANCE
website: http://www.st-abel.com
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[gmx-users] RE : Questions about REMD calcula tions

2010-10-14 Thread ABEL Stephane 175950
Dear all, 
 
Thank you very much Chris, Xavier and ms (;) for your comments and I will take 
into account your suggestions in my proposal (for GENCI, Chris ;)) . 
 
A bientot
 
Stefane


--

Message: 1
Date: Thu, 14 Oct 2010 17:22:38 +0200
From: Florian Dommert domm...@icp.uni-stuttgart.de
Subject: Re: [gmx-users] Re: g_velacc problem (Florian Dommert)
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4cb7203e.1020...@icp.uni-stuttgart.de
Content-Type: text/plain; charset=ISO-8859-1

-BEGIN PGP SIGNED MESSAGE-
Hash: SHA1

On 10/14/2010 04:41 PM, Eudes Fileti wrote:
 Dear Florian, thanks for the help. I wonder just one more thing.
 Is it possible to obtain the lateral diffusion coefficient in a specific
 plane (say xy)
 using g_velacc? Or it is only possible with g_msd?

I am not sure, but the MSD is nothing else than the integrated VACF, so
if you modify the code correspondingly it should work. The modification
shouldn't be that hard, because you just have to prevent summing up a
certain direction of the velocity.

/Flo

 Bests
 eef
 ___
 Eudes Eterno Fileti
 Física da Matéria Condensada
 Simulação Computacional de Nano-estruturas via Dinâmica Molecular






- --
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Dipl.-Phys.

Institute for Computational Physics

University Stuttgart

Pfaffenwaldring 27
70569 Stuttgart

Phone: +49(0)711/685-6-3613
Fax:   +49-(0)711/685-6-3658

EMail: domm...@icp.uni-stuttgart.de
Home: http://www.icp.uni-stuttgart.de/~icp/Florian_Dommert
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iEYEARECAAYFAky3ID4ACgkQLpNNBb9GiPkK2QCg3gMovcfuJRdOd9+IZ7KrmZ1u
2VgAoIPTQGVxyrmDUXi5PbPPg5tCr7h2
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Message: 2
Date: Thu, 14 Oct 2010 17:54:02 +0200
From: ABEL Stephane 175950 stephane.a...@cea.fr
Subject: [gmx-users] Questions about REMD calculations
To: gmx-users@gromacs.org
Message-ID:
f654b3ee96986e4b8dc6ef0919c88da301038...@loderi.intra.cea.fr
Content-Type: text/plain;   charset=iso-8859-1

Dear all,

I come back to you for several questions about the futures replica-exchange 
calculations that i would like to perform. The system of interest will contain 
12 peptides (with 7 residues each) and 4 water molecules, it come from a 
previous MD performed in NPT ensemble. With these systems, i would like to 
study the aggregation process between the peptides.

After reading several paper about REMD method and playing with the Temperature 
generator for REMD-simulations web server (http://folding.bmc.uu.se/remd/), i 
suspect that this system is too big for REMD. Indeed if use the following 
parameters in the webserver

Pdes 0.2
Temperature range 290 - 600
Number of water molecules 41380
Number of protein atoms 1092
Including all H ~ 1656
Number of hydrogens in protein ~ 240
Number of constraints ~ 1092
Number of vsites ~ 0
Number of degrees of freedom ~ 250464
Energy loss due to constraints 520.59 (kJ/mol K)

I obtain 271 replicas (ouch !!) . If i assume that for each replica app. 16 
CPU, The simulations will be too big and will cost a lot CPU time.

So my question is can i reduce safely the number of water in system to reduce 
the number of replicas ?

For example for 1 mol of water the number of replicas will be 135. It is 
not bad. It is a good option to overcome this limitation.

I have also read the number of replicas can be significantly reduced by using 
variants of REMD for example replica exchange with solute tempering (REST) from 
Berne and co-workers. Is this method is implemented in GROMACS ?

Or Can i use the REMD in implicit solvant for example with the coarse grain 
OPEP force field as described in Chebaro, et al. (2008).J. Phys. Chem. B 
113(1): 267-274. or by Wang and Voth in J. Phys. Chem. B 112(41): 13079-13090.

Any advices and comments are welcome

Stefane

--
Stéphane Abel, PhD
CEA Saclay DSV/IBITEC-S/SB2SM
91191 Saclay, FRANCE
website: http://www.st-abel.com http://www.st-abel.com/ 
--


--

Message: 3
Date: Thu, 14 Oct 2010 12:16:35 -0400
From: chris.ne...@utoronto.ca
Subject: [gmx-users] Questions about REMD calculations
To: gmx-users@gromacs.org
Message-ID: 20101014121635.bg1lkn1bswkks...@webmail.utoronto.ca
Content-Type: text/plain;   charset=ISO-8859-1; DelSp=Yes;
format=flowed

Stefane,

why are you hesitant to reduce the size of your system. If you can 
still address the same questions with a smaller system, then I'd say 
the answer is nearly always to use that smaller system (REMD or not). 
Besides, my gut feeling is that even if you had enough 271*16 cpus 
available, you would not get enough exchanges within a reasonable wall 
clock time to get a converged answer. I say this because you're 
basically

[gmx-users] REMD speed calculation compared to classical MD

2010-10-13 Thread ABEL Stephane 175950
Dear All,
 
For a futur project, I would like to perform the REMD calculations with 
GROMACS4.5.X. To have an estimation of CPU time required, I have a naive 
question: What is the speed of REMD compared to a classic NPT MD ? I am aware 
that the response depends a lot of factor (number of replica, etc.), but since 
i have no idea and experience with this type of MD, I ask the question ;). 
 
The system will have approximatively 25000 atoms. Previously for this system, I 
got 11 ns/day on 32 CPU for a NPT MD with GROMOS53A6 and GMX4.0.5.
 
Thanks you in advance for your response. 
 
Stefane
 
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[gmx-users] REMD speed calculation compared to classical MD

2010-10-13 Thread ABEL Stephane 175950
Thank you all for all your interesting comments. I have now an idea how to 
write my proposal. 
 
A bientôt
 
Stefane
 

Message: 2
Date: Wed, 13 Oct 2010 14:38:54 -0400
From: Chris Neale chris.ne...@utoronto.ca
Subject: [gmx-users] REMD speed calculation compared to classical MD
To: gmx-users@gromacs.org
Message-ID: 4cb5fcbe.2080...@utoronto.ca
Content-Type: text/plain; charset=iso-8859-1

Stefane,

If you are asking for a comparison of simulation time required, then
that is not something that can be answered in the abstract. There are
even cases in which REMD will take more total simulation time to
converge the 300K ensemble than will N simulations all at 300K. The
efficiency of REMD will be highly dependent on the size of the important
energy barriers. REMD becomes more efficient than MD as the barriers get
higher. To take that to an extreme, if you wanted to know the
distribution of x-coordinate values of one specific water molecule in a
box of pure water, REMD with 100 replicas would be 100 times less
efficient than simple MD -- there are no energy barriers and so the 99
replicas at temperatures above 300K are a total waste of time. At the
other extreme, if your energy barrier is 30 Kcal/mol at 300K, then you
will essentially never cross it at 300K and REMD, if it works, will be
infinitely more efficient because the replica at 300K will essentially
never sample the other side of that barrier.

There have been a few comparisons, but I don;t know of any general rule
that you can apply here.

On 10/13/10 7:42 PM, XAvier Periole wrote:

/
//  Well the exchanges do not cost time ... so basically each replica runs
//  at the speed it would run it was a regular simulation on the number of
//  cpu you give each replica.
//
//  I do not think there any significant difference in NPT/NVT simulations.
//  Note NVT is often used for REMD
/It us, but that gives high pressure at high T, which is typically not
what you want.

If you use NPT REMD than the run time between exchanges is in general
equal to that of the coldest replica, since that will be at the highest
density (unless you go below the density maximum of water :)).


/
//  XAvier.
//
//  On Oct 13, 2010, at 11:36 AM, ABEL Stephane 175950 wrote:
//
//  Dear All,
//
//  For a futur project, I would like to perform the REMD calculations
//  with GROMACS4.5.X. To have an estimation of CPU time required, I have
//  a naive question: What is the speed of REMD compared to a classic NPT
//  MD ? I am aware that the response depends a lot of factor (number of
//  replica, etc.), but since i have no idea and experience with this type
//  of MD, I ask the question ;).
//
//  The system will have approximatively 25000 atoms. Previously for this
//  system, I got 11 ns/day on 32 CPU for a NPT MD with GROMOS53A6 and
//  GMX4.0.5.
//
//  Thanks you in advance for your response.
//
//  Stefane
//
//  --
//  gmx-users mailing listgmx-users at gromacs.org  
http://lists.gromacs.org/mailman/listinfo/gmx-users
//  http://lists.gromacs.org/mailman/listinfo/gmx-users
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/

--
David.

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[gmx-users] Error : There is no domain decomposition for 4 nodes that compatible with the given box

2010-09-30 Thread ABEL Stephane 175950
Dear All,

I am trying to do a MD of a system containing TIP3P water, a peptide, some 
glycolipids molecule and ions in a cubic box. The forcefield used is CHARMM and 
are taken from previous MD. The bonded and nonbonded parameters was converted 
in GROMACS manually because some parameters are not in present in current GMX 
(v 4.5.1) distribution.

I have minimized successfully the system. see below 

 em.mdp ---

title = bDM+KTM17 in water

; Preprocessor - specify a full path if necessary.

cpp = cpp

include = -I../top

define = -DFLEXIBLE

integrator = steep

nstcgsteep = 5000

emstep = 0.01

emtol = 500.0

;dt = 0.002

pbc = xyz

nsteps = 5000

nstlist = 5

ns_type = grid

rlist = 1.2

coulombtype = PME

rcoulomb = 1.2

rvdw = 1.2

fourierspacing = 0.12

pme_order = 4

ewald_rtol = 1e-05

optimize_fft = yes

---

 Final results of energy minimization process

Energies (kJ/mol)

Bond Angle U-B Proper Dih. Improper Dih.

3.58212e+04 1.88051e+04 6.00353e+03 3.58404e+04 7.30187e+00

CMAP Dih. LJ-14 Coulomb-14 LJ (SR) Coulomb (SR)

-1.39601e+02 1.11718e+04 1.76772e+05 1.66576e+05 -1.30112e+06

Coul. recip. Potential Pressure (bar)

-1.17090e+05 -9.67347e+05 0.0e+00

Steepest Descents converged to Fmax  500 in 107 steps

Potential Energy = -9.67347283476003e+05

Maximum force = 4.75153618041724e+02 on atom 313

Norm of force = 9.37591893853129e+00

But when i try to equilibrate this system in NVT ensemble for 100 ps with the 
md.mdp below 

 nvt.mdp ---

title = KTM17-bDM MD

;define = -DPOSRES ; position restrain the protein

; Run parameters

integrator = md ; leap-frog integrator

nsteps = 5 ; 2 * 5 = 100 ps

dt = 0.002 ; 2 fs

; Output control

nstxout = 100 ; save coordinates every 0.2 ps

nstvout = 100 ; save velocities every 0.2 ps

nstenergy = 100 ; save energies every 0.2 ps

nstlog = 100 ; update log file every 0.2 ps

; Bond parameters

continuation = no ; first dynamics run

constraint_algorithm = lincs ; holonomic constraints

constraints = all-bonds ; all bonds (even heavy atom-H bonds) constrained

lincs_iter = 1 ; accuracy of LINCS

lincs_order = 4 ; also related to accuracy

; Neighborsearching

vdw-type = cut-off

ns_type = grid ; search neighboring grid cels

nstlist = 5 ; 10 fs

rlist = 1.2 ; short-range neighborlist cutoff (in nm)

rcoulomb = 1.2 ; short-range electrostatic cutoff (in nm)

rvdw = 1.2 ; short-range van der Waals cutoff (in nm)

; Electrostatics

coulombtype = PME ; Particle Mesh Ewald for long-range electrostatics

pme_order = 4 ; cubic interpolation

fourierspacing = 0.12 ; grid spacing for FFT

; Temperature coupling is on

tcoupl = V-rescale ; modified Berendsen thermostat

tc-grps = System ; one coupling groups - more accurate

tau_t = 0.1 ; time constant, in ps

ref_t = 300 ; reference temperature, one for each group, in K

; Pressure coupling is off

pcoupl = no ; no pressure coupling in NVT

; Periodic boundary conditions

pbc = xyz ; 3-D PBC

; Dispersion correction

DispCorr = EnerPres ; account for cut-off vdW scheme

; Velocity generation

gen_vel = yes ; assign velocities from Maxwell distribution

gen_temp = 300 ; temperature for Maxwell distribution

gen_seed = -1 ; generate a random seed

-

I obtain the following error with mdrun_mpi command

/usr/pbs/bin/mpiexec mdrun_mpi -s hMRP1_K-TM17_md.tpr -o hMRP1_K-TM17_md.trr -c 
hMRP1_K-TM17_md.gro -e hMRP1_K-TM17_bDM_h2o_Cl_md.edr -g 
hMRP1_K-TM17_bDM_h2o_Cl_md.log

-- error 

Initializing Domain Decomposition on 4 nodes

Dynamic load balancing: auto

Will sort the charge groups at every domain (re)decomposition

Initial maximum inter charge-group distances:

two-body bonded interactions: 6.729 nm, LJ-14, atoms 11100 11107

multi-body bonded interactions: 6.729 nm, U-B, atoms 11100 11106

Minimum cell size due to bonded interactions: 7.402 nm

Maximum distance for 5 constraints, at 120 deg. angles, all-trans: 0.819 nm

Estimated maximum distance required for P-LINCS: 0.819 nm

Using 0 separate PME nodes

Scaling the initial minimum size with 1/0.8 (option -dds) = 1.25

Optimizing the DD grid for 4 cells with a minimum initial size of 9.252 nm

The maximum allowed number of cells is: X 0 Y 0 Z 0

---

Program mdrun_mpi, VERSION 4.5.1

Source code file: domdec.c, line: 6428

Fatal error:

There is no domain decomposition for 4 nodes that is compatible with the given 
box and a minimum cell size of 9.25216 nm

Change the number of nodes or mdrun option -rdd or -dds

Look in the log file for details on the domain decomposition

For more information and tips for troubleshooting, please check the GROMACS

website at http://www.gromacs.org/Documentation/Errors

---

Player Sleeps With the Fishes (Ein Bekanntes Spiel Von ID Software)

I have also checked the mimized structure at different minimization step, and I 
saw no 

[gmx-users] Error : There is no domain decomposition for

2010-09-30 Thread ABEL Stephane 175950
Yeah Justin, I have already read the comments related to the link before to 
post in the mailing list. But I don't know how to correct this ? 
 
Increase/decrease the number of node or CPU ? 
 
Thank you again for your help
 
Stephane  

ABEL Stephane 175950 wrote:
 Dear All,

 I am trying to do a MD of a system containing TIP3P water, a peptide, some 
 glycolipids molecule and ions in a cubic box. The forcefield used is CHARMM 
 and are taken from previous MD. The bonded and nonbonded parameters was 
 converted in GROMACS manually because some parameters are not in present in 
 current GMX (v 4.5.1) distribution.

 I have minimized successfully the system. see below

  em.mdp ---

 title = bDM+KTM17 in water

 ; Preprocessor - specify a full path if necessary.

 cpp = cpp

 include = -I../top

 define = -DFLEXIBLE

 integrator = steep

 nstcgsteep = 5000

 emstep = 0.01

 emtol = 500.0

 ;dt = 0.002

 pbc = xyz

 nsteps = 5000

 nstlist = 5

 ns_type = grid

 rlist = 1.2

 coulombtype = PME

 rcoulomb = 1.2

 rvdw = 1.2

 fourierspacing = 0.12

 pme_order = 4

 ewald_rtol = 1e-05

 optimize_fft = yes

 ---

  Final results of energy minimization process

 Energies (kJ/mol)

 Bond Angle U-B Proper Dih. Improper Dih.

 3.58212e+04 1.88051e+04 6.00353e+03 3.58404e+04 7.30187e+00

 CMAP Dih. LJ-14 Coulomb-14 LJ (SR) Coulomb (SR)

 -1.39601e+02 1.11718e+04 1.76772e+05 1.66576e+05 -1.30112e+06

 Coul. recip. Potential Pressure (bar)

 -1.17090e+05 -9.67347e+05 0.0e+00

 Steepest Descents converged to Fmax  500 in 107 steps

 Potential Energy = -9.67347283476003e+05

 Maximum force = 4.75153618041724e+02 on atom 313

 Norm of force = 9.37591893853129e+00

 But when i try to equilibrate this system in NVT ensemble for 100 ps with the 
 md.mdp below

  nvt.mdp ---

 title = KTM17-bDM MD

 ;define = -DPOSRES ; position restrain the protein

 ; Run parameters

 integrator = md ; leap-frog integrator

 nsteps = 5 ; 2 * 5 = 100 ps

 dt = 0.002 ; 2 fs

 ; Output control

 nstxout = 100 ; save coordinates every 0.2 ps

 nstvout = 100 ; save velocities every 0.2 ps

 nstenergy = 100 ; save energies every 0.2 ps

 nstlog = 100 ; update log file every 0.2 ps

 ; Bond parameters

 continuation = no ; first dynamics run

 constraint_algorithm = lincs ; holonomic constraints

 constraints = all-bonds ; all bonds (even heavy atom-H bonds) constrained

 lincs_iter = 1 ; accuracy of LINCS

 lincs_order = 4 ; also related to accuracy

 ; Neighborsearching

 vdw-type = cut-off

 ns_type = grid ; search neighboring grid cels

 nstlist = 5 ; 10 fs

 rlist = 1.2 ; short-range neighborlist cutoff (in nm)

 rcoulomb = 1.2 ; short-range electrostatic cutoff (in nm)

 rvdw = 1.2 ; short-range van der Waals cutoff (in nm)

 ; Electrostatics

 coulombtype = PME ; Particle Mesh Ewald for long-range electrostatics

 pme_order = 4 ; cubic interpolation

 fourierspacing = 0.12 ; grid spacing for FFT

 ; Temperature coupling is on

 tcoupl = V-rescale ; modified Berendsen thermostat

 tc-grps = System ; one coupling groups - more accurate

 tau_t = 0.1 ; time constant, in ps

 ref_t = 300 ; reference temperature, one for each group, in K

 ; Pressure coupling is off

 pcoupl = no ; no pressure coupling in NVT

 ; Periodic boundary conditions

 pbc = xyz ; 3-D PBC

 ; Dispersion correction

 DispCorr = EnerPres ; account for cut-off vdW scheme

 ; Velocity generation

 gen_vel = yes ; assign velocities from Maxwell distribution

 gen_temp = 300 ; temperature for Maxwell distribution

 gen_seed = -1 ; generate a random seed

 -

 I obtain the following error with mdrun_mpi command

 /usr/pbs/bin/mpiexec mdrun_mpi -s hMRP1_K-TM17_md.tpr -o hMRP1_K-TM17_md.trr 
 -c hMRP1_K-TM17_md.gro -e hMRP1_K-TM17_bDM_h2o_Cl_md.edr -g 
 hMRP1_K-TM17_bDM_h2o_Cl_md.log

 -- error

 Initializing Domain Decomposition on 4 nodes

 Dynamic load balancing: auto

 Will sort the charge groups at every domain (re)decomposition

 Initial maximum inter charge-group distances:

 two-body bonded interactions: 6.729 nm, LJ-14, atoms 11100 11107

 multi-body bonded interactions: 6.729 nm, U-B, atoms 11100 11106

 Minimum cell size due to bonded interactions: 7.402 nm

 Maximum distance for 5 constraints, at 120 deg. angles, all-trans: 0.819 nm

 Estimated maximum distance required for P-LINCS: 0.819 nm

 Using 0 separate PME nodes

 Scaling the initial minimum size with 1/0.8 (option -dds) = 1.25

 Optimizing the DD grid for 4 cells with a minimum initial size of 9.252 nm

 The maximum allowed number of cells is: X 0 Y 0 Z 0

 ---

 Program mdrun_mpi, VERSION 4.5.1

 Source code file: domdec.c, line: 6428

 Fatal error:

 There is no domain decomposition for 4 nodes that is compatible with the 
 given box and a minimum cell size of 9.25216 nm

 Change the number of nodes or mdrun option -rdd or -dds

 Look in the log file for details

[gmx-users] Re: Error : There is no domain decomposition for ....

2010-09-30 Thread ABEL Stephane 175950
Mark, 
 
These long range parameters have been used by Bjelkmar et al.  in their recent 
paper [1]for simulations of CHARMM ff in GROMACS. So I use it ! 
 
[1] Bjelkmar, P., P. Larsson, et al. (2010). Implementation of the CHARMM 
Force Field in GROMACS: Analysis of Protein Stability Effects from Correction 
Maps, Virtual Interaction Sites, and Water Models. J. Chem. Theory Comput. 
6(2): 459-466.
 

 Yeah Justin, I have already read the comments related to the link before to 
 post in the  mailing list. But I don't know how to correct this ?

 Increase/decrease the number of node or CPU ?

 Thank you again for your help

 Stephane 

ABEL Stephane 175950 wrote:
 Dear All,

 I am trying to do a MD of a system containing TIP3P water, a peptide, some 
 glycolipids molecule and ions in a cubic box. The forcefield used is CHARMM 
 and are taken from previous MD. The bonded and nonbonded parameters was 
 converted in GROMACS manually because some parameters are not in present in 
 current GMX (v 4.5.1) distribution.

 I have minimized successfully the system. see below

  em.mdp ---

 title = bDM+KTM17 in water

 ; Preprocessor - specify a full path if necessary.

 cpp = cpp

 include = -I../top

 define = -DFLEXIBLE

 integrator = steep

 nstcgsteep = 5000

 emstep = 0.01

 emtol = 500.0

 ;dt = 0.002

 pbc = xyz

 nsteps = 5000

 nstlist = 5

 ns_type = grid

 rlist = 1.2

 coulombtype = PME

 rcoulomb = 1.2

 rvdw = 1.2

 fourierspacing = 0.12

 pme_order = 4

 ewald_rtol = 1e-05

 optimize_fft = yes

 ---

  Final results of energy minimization process

 Energies (kJ/mol)

 Bond Angle U-B Proper Dih. Improper Dih.

 3.58212e+04 1.88051e+04 6.00353e+03 3.58404e+04 7.30187e+00

 CMAP Dih. LJ-14 Coulomb-14 LJ (SR) Coulomb (SR)

 -1.39601e+02 1.11718e+04 1.76772e+05 1.66576e+05 -1.30112e+06

 Coul. recip. Potential Pressure (bar)

 -1.17090e+05 -9.67347e+05 0.0e+00

 Steepest Descents converged to Fmax  500 in 107 steps

 Potential Energy = -9.67347283476003e+05

 Maximum force = 4.75153618041724e+02 on atom 313

 Norm of force = 9.37591893853129e+00

 But when i try to equilibrate this system in NVT ensemble for 100 ps with the 
 md.mdp below

  nvt.mdp ---

 title = KTM17-bDM MD

 ;define = -DPOSRES ; position restrain the protein

 ; Run parameters

 integrator = md ; leap-frog integrator

 nsteps = 5 ; 2 * 5 = 100 ps

 dt = 0.002 ; 2 fs

 ; Output control

 nstxout = 100 ; save coordinates every 0.2 ps

 nstvout = 100 ; save velocities every 0.2 ps

 nstenergy = 100 ; save energies every 0.2 ps

 nstlog = 100 ; update log file every 0.2 ps

 ; Bond parameters

 continuation = no ; first dynamics run

 constraint_algorithm = lincs ; holonomic constraints

 constraints = all-bonds ; all bonds (even heavy atom-H bonds) constrained

 lincs_iter = 1 ; accuracy of LINCS

 lincs_order = 4 ; also related to accuracy

 ; Neighborsearching

 vdw-type = cut-off

 ns_type = grid ; search neighboring grid cels

 nstlist = 5 ; 10 fs

 rlist = 1.2 ; short-range neighborlist cutoff (in nm)

 rcoulomb = 1.2 ; short-range electrostatic cutoff (in nm)

 rvdw = 1.2 ; short-range van der Waals cutoff (in nm)

 ; Electrostatics

 coulombtype = PME ; Particle Mesh Ewald for long-range electrostatics

 pme_order = 4 ; cubic interpolation

 fourierspacing = 0.12 ; grid spacing for FFT

 ; Temperature coupling is on

 tcoupl = V-rescale ; modified Berendsen thermostat

 tc-grps = System ; one coupling groups - more accurate

 tau_t = 0.1 ; time constant, in ps

 ref_t = 300 ; reference temperature, one for each group, in K

 ; Pressure coupling is off

 pcoupl = no ; no pressure coupling in NVT

 ; Periodic boundary conditions

 pbc = xyz ; 3-D PBC

 ; Dispersion correction

 DispCorr = EnerPres ; account for cut-off vdW scheme

 ; Velocity generation

 gen_vel = yes ; assign velocities from Maxwell distribution

 gen_temp = 300 ; temperature for Maxwell distribution

 gen_seed = -1 ; generate a random seed

 -

 I obtain the following error with mdrun_mpi command

 /usr/pbs/bin/mpiexec mdrun_mpi -s hMRP1_K-TM17_md.tpr -o hMRP1_K-TM17_md.trr 
 -c hMRP1_K-TM17_md.gro -e hMRP1_K-TM17_bDM_h2o_Cl_md.edr -g 
 hMRP1_K-TM17_bDM_h2o_Cl_md.log

 -- error

 Initializing Domain Decomposition on 4 nodes

 Dynamic load balancing: auto

 Will sort the charge groups at every domain (re)decomposition

 Initial maximum inter charge-group distances:

 two-body bonded interactions: 6.729 nm, LJ-14, atoms 11100 11107

 multi-body bonded interactions: 6.729 nm, U-B, atoms 11100 11106

 Minimum cell size due to bonded interactions: 7.402 nm

 Maximum distance for 5 constraints, at 120 deg. angles, all-trans: 0.819 nm

 Estimated maximum distance required for P-LINCS: 0.819 nm

 Using 0 separate PME nodes

 Scaling the initial minimum size with 1/0.8 (option -dds) = 1.25

 Optimizing the DD grid for 4 cells with a minimum initial size of 9.252 nm

 The maximum allowed

[gmx-users] RE : gmx-users Digest, Vol 77 , Issue 201

2010-09-30 Thread ABEL Stephane 175950
OK Mark and Justin, thank you for the pointer
 
I will take a look about it
 
A bientot
 
Stephane
 
--
Stéphane Abel, PhD
CEA Saclay DSV/IBITEC-S/SB2SM
91191 Saclay, FRANCE
website: http://www.st-abel.com
--



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Date: jeu. 30/09/2010 13:56
À: gmx-users@gromacs.org
Objet : gmx-users Digest, Vol 77, Issue 201



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Today's Topics:

   1. Re: Re: Error : There is no domain decomposition for 
  (Mark Abraham)
   2. Re: NAMD simulation in Gromacs (Mark Abraham)


--

Message: 1
Date: Thu, 30 Sep 2010 21:48:05 +1000
From: Mark Abraham mark.abra...@anu.edu.au
Subject: Re: [gmx-users] Re: Error : There is no domain decomposition
for 
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: fbd7dfad5f039.4ca50...@anu.edu.au
Content-Type: text/plain; charset=us-ascii



- Original Message -
From: ABEL Stephane 175950 stephane.a...@cea.fr
Date: Thursday, September 30, 2010 21:43
Subject: [gmx-users] Re: Error : There is no domain decomposition for 
To: gmx-users@gromacs.org

 Mark,
 
 These long range parameters have been used by Bjelkmar et
 al.  in their recent paper [1]for simulations of CHARMM ff
 in GROMACS. So I use it !
 
 [1] Bjelkmar, P., P. Larsson, et al. (2010). Implementation of
 the CHARMM Force Field in GROMACS: Analysis of Protein Stability
 Effects from Correction Maps, Virtual Interaction Sites, and
 Water Models. J. Chem. Theory Comput. 6(2): 459-466.

I'm not questioning any .mdp file settings. However the combination of topology 
and initial coordinates contains some kind of bonded interaction between atoms 
that are much further apart than you would normally suppose. You should explore 
what is going on there.

Mark

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Message: 2
Date: Thu, 30 Sep 2010 21:55:04 +1000
From: Mark Abraham mark.abra...@anu.edu.au
Subject: Re: [gmx-users] NAMD simulation in Gromacs
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: fbb29fd25ceae.4ca50...@anu.edu.au
Content-Type: text/plain; charset=us-ascii



- Original Message -
From: oguz gurbulak gurbulako...@yahoo.com
Date: Thursday, September 30, 2010 21:38
Subject: [gmx-users] NAMD simulation in Gromacs
To: gmx-users@gromacs.org

---
|Dear All,
  
   I performed a 50 ns md simulation using NAMD and want to continue this 
simulation for 10 ns in Gromacs. Is it possible to continue a NAMD simulation 
in Gromacs ? If so, could you please give me the information about this process 
?



Not really. You would need to generate a .top in the normal way, and this 
process cannot use any topology information that NAMD was using. You could 
start the GROMACS simulation from the endpoint of the NAMD simulation, but it 
would not be continuous in any sense.

  
  Secondly can I convert NAMD output files into gromacs output files and use 
gromacs analysis tools ? Could you please also give me the information about 
this issue ?
  
If you have VMD installed then GROMACS is supposed to be able to link to its 
libraries to enable GROMACS tools to read any file format that VMD can read, 
which will include all NAMD formats. I'm unaware that anybody has written any 
documentation about this, however. That's probably the path of least resistance.


Mark

 |
---

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[gmx-users] Re: A common error Atom O11 in residue bDM 1 was

2010-09-27 Thread ABEL Stephane 175950
OK you thank Justin for your explanation. Accordingly, I have changed the C* 
and O* atom names in the pdb and now it works. 
 
A bientôt 
 
Stefane


ABEL Stephane 175950 wrote:
 You are right Justin,

 The 1O1 atoms and (others 1O2, etc.) are changed to O11, O21, etc. (?). Why
 this problem happens ? Should I change the name of these atoms in the rtp and
 pdb files ? Is a trick is available to avoid this bad translation ?


The only option is to not use digits as the first characters in an atom name.
The code in pdb2gmx.c calls a function rename_atoms in xlate.c, which (since a
value of TRUE is passed to the function for bReorderNum), shifts the position of
all digits in the first position:

 if (bReorderNum)
 {
 if (isdigit(atombuf[0]))
 {
 c = atombuf[0];
 for (i=0; ((size_t)istrlen(atombuf)-1); i++)
 {
 atombuf[i] = atombuf[i+1];
 }
 atombuf[i] = c;
 bReorderedNum = TRUE;
 }
 }

I think the purpose is really to deal with hydrogens (i.e. 1HG1, etc) but
affects all atoms, as written.  A check could probably be implemented to
determine if the atom is H or not, but really might not be worth the effort,
since the vast majority of all structures that will be passed to pdb2gmx will
follow the normal route of: character first, then digits.

-Justin

 Stefane


 ABEL Stephane 175950 wrote:
 Dear all,

 I have a very common problem when I try to convert a pdb file to a gro
 file with the following command.

 I use charmm27ff and gmx4.5.1.

 pdb2gmx_mpi -f 1-bDM.pdb -o 1-bDM.gro -p 1-bDM.top -chargegrp

 I obtain the following commun error :

 Atom O11 in residue bDM 1 was not found in rtp entry bDM with 80 atoms
 while sorting atoms.

 I am surprised to have this message, since after verification in the
 1-bDM.pdb, I have not found an atom with this name. I have also checked the
 format of the pdb and all the fields are in right place.


 Probably atom 1O1 is being translated as O11.  I have had similar problems
 with translated atom names.  If you add -debug 1 to your pdb2gmx command
 line, you will get output .pdb files containing the structure as pdb2gmx is
 interpreting it.  That's how I've identified some spurious translations
 before.

 -Justin

 Below my PDB file ATOM  1 1C1  bDM 1 -28.807  -8.973  -4.361
 0.30  0.00 ATOM  2 H1A  bDM 1 -28.976  -9.551  -3.427  0.10
 0.00 ATOM  3 1O1  bDM 1 -27.541  -9.232  -4.796 -0.40  0.00
 ATOM  4 1C2  bDM 1 -29.836  -9.352  -5.325  0.14  0.00 ATOM
 5 H2A  bDM 1 -30.783  -9.324  -4.746  0.09  0.00 ATOM  6 1O2
 bDM 1 -29.680 -10.694  -5.733 -0.66  0.00 ATOM  7 H2OA bDM
 1 -28.731 -10.800  -5.827  0.43  0.00 ATOM  8 1C3  bDM 1
 -29.990  -8.385  -6.493  0.14  0.00 ATOM  9 H3A  bDM 1 -29.086
 -8.411  -7.139  0.09  0.00 ATOM 10 1O3  bDM 1 -31.239  -8.585
 -7.237 -0.66  0.00 ATOM 11 H3OA bDM 1 -31.193  -8.053  -8.035
 0.43  0.00 ATOM 12 1C4  bDM 1 -29.957  -6.922  -6.018  0.14
 0.00 ATOM 13 H4A  bDM 1 -30.923  -6.772  -5.490  0.09  0.00
 ATOM 14 1O4  bDM 1 -29.963  -6.003  -7.122 -0.66  0.00 ATOM
 15 H4OA bDM 1 -29.993  -5.118  -6.751  0.43  0.00 ATOM 16 1C5
 bDM 1 -28.865  -6.650  -5.081  0.10  0.00 ATOM 17 H5A  bDM
 1 -27.963  -7.009  -5.622  0.10  0.00 ATOM 18 1C6  bDM 1
 -28.730  -5.254  -4.552  0.05  0.00 ATOM 19 H61A bDM 1 -29.694
 -5.009  -4.056  0.09  0.00 ATOM 20 H61B bDM 1 -28.509  -4.622
 -5.438  0.09  0.00 ATOM 21 1O6  bDM 1 -27.593  -5.254  -3.684
 -0.66  0.00 ATOM 22 H6OA bDM 1 -27.699  -5.900  -2.982  0.43
 0.00 ATOM 23 1O5  bDM 1 -28.979  -7.582  -3.963 -0.40  0.00
 ATOM 24 2C1  bDM 1 -23.620  -9.286  -3.000  0.20  0.00 ATOM
 25 H1B  bDM 1 -23.440 -10.274  -3.475  0.09  0.00 ATOM 26 2C2
 bDM 1 -24.806  -9.283  -2.026  0.14  0.00 ATOM 27 H2B  bDM
 1 -24.867  -8.235  -1.662  0.09  0.00 ATOM 28 2O2  bDM 1
 -24.477 -10.097  -0.884 -0.66  0.00 ATOM 29 H2OB bDM 1 -23.792
 -9.775  -0.294  0.43  0.00 ATOM 30 2C3  bDM 1 -26.163  -9.642
 -2.661  0.14  0.00 ATOM 31 H3B  bDM 1 -26.142 -10.663  -3.098
 0.09  0.00 ATOM 32 2O3  bDM 1 -27.232  -9.397  -1.722 -0.66
 0.00 ATOM 33 H3OB bDM 1 -27.384 -10.156  -1.155  0.43  0.00
 ATOM 34 2C4  bDM 1 -26.364  -8.872  -3.987  0.10  0.00 ATOM
 35 H4B  bDM 1 -26.533  -7.835  -3.626  0.10  0.00 ATOM 36 2C5
 bDM 1 -25.089  -8.936  -4.892  0.25  0.00 ATOM 37 H5B  bDM
 1 -24.906  -9.942  -5.326  0.09  0.00 ATOM 38 2C6  bDM 1
 -25.225  -7.980  -6.074  0.05  0.00 ATOM 39 H62A bDM 1 -25.159
 -6.910  -5.780  0.09  0.00 ATOM 40 H62B bDM 1

[gmx-users] A common error Atom O11 in residue bDM 1 was

2010-09-26 Thread ABEL Stephane 175950
You are right Justin, 
 
The 1O1 atoms and (others 1O2, etc.) are changed to O11, O21, etc. (?). Why 
this problem happens ? Should I change the name of these atoms in the rtp and 
pdb files ? Is a trick is available to avoid this bad translation ?
 
Stefane


ABEL Stephane 175950 wrote:
 Dear all,
 
 I have a very common problem when I try to convert a pdb file to a gro file 
 with the following command.
 
 I use charmm27ff and gmx4.5.1.
 
 pdb2gmx_mpi -f 1-bDM.pdb -o 1-bDM.gro -p 1-bDM.top -chargegrp
 
 I obtain the following commun error :
 
 Atom O11 in residue bDM 1 was not found in rtp entry bDM with 80 atoms while 
 sorting atoms.
 
 I am surprised to have this message, since after verification in the 
 1-bDM.pdb, I have not found an atom with this name. I have also checked the 
 format of the pdb and all the fields are in right place.
 

Probably atom 1O1 is being translated as O11.  I have had similar problems with
translated atom names.  If you add -debug 1 to your pdb2gmx command line, you
will get output .pdb files containing the structure as pdb2gmx is interpreting
it.  That's how I've identified some spurious translations before.

-Justin

 Below my PDB file
 ATOM  1 1C1  bDM 1 -28.807  -8.973  -4.361  0.30  0.00
 ATOM  2 H1A  bDM 1 -28.976  -9.551  -3.427  0.10  0.00
 ATOM  3 1O1  bDM 1 -27.541  -9.232  -4.796 -0.40  0.00
 ATOM  4 1C2  bDM 1 -29.836  -9.352  -5.325  0.14  0.00
 ATOM  5 H2A  bDM 1 -30.783  -9.324  -4.746  0.09  0.00
 ATOM  6 1O2  bDM 1 -29.680 -10.694  -5.733 -0.66  0.00
 ATOM  7 H2OA bDM 1 -28.731 -10.800  -5.827  0.43  0.00
 ATOM  8 1C3  bDM 1 -29.990  -8.385  -6.493  0.14  0.00
 ATOM  9 H3A  bDM 1 -29.086  -8.411  -7.139  0.09  0.00
 ATOM 10 1O3  bDM 1 -31.239  -8.585  -7.237 -0.66  0.00
 ATOM 11 H3OA bDM 1 -31.193  -8.053  -8.035  0.43  0.00
 ATOM 12 1C4  bDM 1 -29.957  -6.922  -6.018  0.14  0.00
 ATOM 13 H4A  bDM 1 -30.923  -6.772  -5.490  0.09  0.00
 ATOM 14 1O4  bDM 1 -29.963  -6.003  -7.122 -0.66  0.00
 ATOM 15 H4OA bDM 1 -29.993  -5.118  -6.751  0.43  0.00
 ATOM 16 1C5  bDM 1 -28.865  -6.650  -5.081  0.10  0.00
 ATOM 17 H5A  bDM 1 -27.963  -7.009  -5.622  0.10  0.00
 ATOM 18 1C6  bDM 1 -28.730  -5.254  -4.552  0.05  0.00
 ATOM 19 H61A bDM 1 -29.694  -5.009  -4.056  0.09  0.00
 ATOM 20 H61B bDM 1 -28.509  -4.622  -5.438  0.09  0.00
 ATOM 21 1O6  bDM 1 -27.593  -5.254  -3.684 -0.66  0.00
 ATOM 22 H6OA bDM 1 -27.699  -5.900  -2.982  0.43  0.00
 ATOM 23 1O5  bDM 1 -28.979  -7.582  -3.963 -0.40  0.00
 ATOM 24 2C1  bDM 1 -23.620  -9.286  -3.000  0.20  0.00
 ATOM 25 H1B  bDM 1 -23.440 -10.274  -3.475  0.09  0.00
 ATOM 26 2C2  bDM 1 -24.806  -9.283  -2.026  0.14  0.00
 ATOM 27 H2B  bDM 1 -24.867  -8.235  -1.662  0.09  0.00
 ATOM 28 2O2  bDM 1 -24.477 -10.097  -0.884 -0.66  0.00
 ATOM 29 H2OB bDM 1 -23.792  -9.775  -0.294  0.43  0.00
 ATOM 30 2C3  bDM 1 -26.163  -9.642  -2.661  0.14  0.00
 ATOM 31 H3B  bDM 1 -26.142 -10.663  -3.098  0.09  0.00
 ATOM 32 2O3  bDM 1 -27.232  -9.397  -1.722 -0.66  0.00
 ATOM 33 H3OB bDM 1 -27.384 -10.156  -1.155  0.43  0.00
 ATOM 34 2C4  bDM 1 -26.364  -8.872  -3.987  0.10  0.00
 ATOM 35 H4B  bDM 1 -26.533  -7.835  -3.626  0.10  0.00
 ATOM 36 2C5  bDM 1 -25.089  -8.936  -4.892  0.25  0.00
 ATOM 37 H5B  bDM 1 -24.906  -9.942  -5.326  0.09  0.00
 ATOM 38 2C6  bDM 1 -25.225  -7.980  -6.074  0.05  0.00
 ATOM 39 H62A bDM 1 -25.159  -6.910  -5.780  0.09  0.00
 ATOM 40 H62B bDM 1 -26.236  -8.045  -6.532  0.09  0.00
 ATOM 41 2O5  bDM 1 -24.218  -8.289  -7.105 -0.66  0.00
 ATOM 42 H5OB bDM 1 -24.661  -8.895  -7.704  0.43  0.00
 ATOM 43 2O4  bDM 1 -24.011  -8.432  -4.077 -0.40  0.00
 ATOM 44 2O1  bDM 1 -22.364  -8.895  -2.386 -0.30  0.00
 ATOM 45 C7   bDM 1 -21.159  -9.105  -3.148 -0.11  0.00
 ATOM 46 H7A  bDM 1 -20.922 -10.188  -3.228  0.09  0.00
 ATOM 47 H7B  bDM 1 -21.320  -8.848  -4.217  0.09  0.00
 ATOM 48 C8   bDM 1 -19.961  -8.389  -2.410 -0.18  0.00
 ATOM 49 H8A  bDM 1 -19.829  -8.778  -1.378  0.09  0.00
 ATOM 50 H8B  bDM 1 -20.171  -7.300  -2.464  0.09  0.00
 ATOM 51 C9   bDM 1 -18.547  -8.641  -3.005 -0.18  0.00
 ATOM 52 H9A  bDM 1 -18.718  -8.465  -4.089  0.09  0.00
 ATOM 53 H9B  bDM 1 -18.415  -9.744  -3.010  0.09  0.00
 ATOM 54 C10  bDM 1 -17.452  -7.785  -2.397 -0.18  0.00
 ATOM 55 H10A bDM 1 -16.675  -7.915  -3.180  0.09  0.00
 ATOM 56 H10B bDM 1 -17.700  -6.702  -2.407  0.09  0.00

[gmx-users] CHARMM - gromacs epsilon and sigma conversiion

2010-09-25 Thread ABEL Stephane 175950
Thank you !!! Jianhui
 
Stefane

--

Message: 5
Date: Fri, 24 Sep 2010 14:18:25 -0600
From: Jianhui Tian jianhuit...@gmail.com
Subject: [gmx-users] CHARMM - gromacs epsilon and sigma conversiion
To: gmx-users@gromacs.org
Message-ID:
aanlktik8xpfhf66l78uxshh7tv6xfhretc8hhbwja...@mail.gmail.com
Content-Type: text/plain; charset=iso-8859-1

eps(charmm)*4.184=epsilon(Gromacs)
0.15*4.184=0.6276

Rmin/2(Charmm)*2/(2^1/6)=sigma(Gromacs)
2.27*2/(2^(1/6))=0.404468(nm)

Cheers,
Jianhui

Date: Fri, 24 Sep 2010 15:55:44 +0200
From: ABEL Stephane 175950 stephane.a...@cea.fr
Subject: [gmx-users] CHARMM - gromacs epsilon and sigma conversiion
   factors
To: gmx-users@gromacs.org
Message-ID:
   f654b3ee96986e4b8dc6ef0919c88da301038...@loderi.intra.cea.fr
Content-Type: text/plain;   charset=iso-8859-1

Hi all,

I would like to add new  atom types in the charmm27.ff for futures
simulations of glyolipids in water with gmx 4.5.1. I have finished to
convert the bonded in GROMACS format. However, I am little puzzled with the
vdW paramaters. I would like to know how to convert them (i.e. what are the
conversion factors used to convert the CHARMM sigma and epsilon parameters
to gromacs sigma and epsilon values ?).

For example for the chloride atom CLA

CHARMM 27

; atom  ignoredepsilon  Rmin/2   ignored   eps,1-4   Rmin/2,1-4
CLA  0.0   -0.150 2.27  ! chloride

GROMACS ffcharmmnb.itp

;name at.num mass charge ptype sigma epsilon
CLA 17 35.45 -1.00 A 0.404468018036 0.6276

Thanks in advance for your help

Stefane
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[gmx-users] A common error Atom O11 in residue bDM 1 was not found in rtp entry

2010-09-25 Thread ABEL Stephane 175950
Dear all, 
 
I have a very common problem when I try to convert a pdb file to a gro file 
with the following command.
 
I use charmm27ff and gmx4.5.1.
 
pdb2gmx_mpi -f 1-bDM.pdb -o 1-bDM.gro -p 1-bDM.top -chargegrp
 
I obtain the following commun error :
 
Atom O11 in residue bDM 1 was not found in rtp entry bDM with 80 atoms while 
sorting atoms. 
 
I am surprised to have this message, since after verification in the 1-bDM.pdb, 
I have not found an atom with this name. I have also checked the format of the 
pdb and all the fields are in right place. 
 
Below my PDB file
ATOM  1 1C1  bDM 1 -28.807  -8.973  -4.361  0.30  0.00
ATOM  2 H1A  bDM 1 -28.976  -9.551  -3.427  0.10  0.00
ATOM  3 1O1  bDM 1 -27.541  -9.232  -4.796 -0.40  0.00
ATOM  4 1C2  bDM 1 -29.836  -9.352  -5.325  0.14  0.00
ATOM  5 H2A  bDM 1 -30.783  -9.324  -4.746  0.09  0.00
ATOM  6 1O2  bDM 1 -29.680 -10.694  -5.733 -0.66  0.00
ATOM  7 H2OA bDM 1 -28.731 -10.800  -5.827  0.43  0.00
ATOM  8 1C3  bDM 1 -29.990  -8.385  -6.493  0.14  0.00
ATOM  9 H3A  bDM 1 -29.086  -8.411  -7.139  0.09  0.00
ATOM 10 1O3  bDM 1 -31.239  -8.585  -7.237 -0.66  0.00
ATOM 11 H3OA bDM 1 -31.193  -8.053  -8.035  0.43  0.00
ATOM 12 1C4  bDM 1 -29.957  -6.922  -6.018  0.14  0.00
ATOM 13 H4A  bDM 1 -30.923  -6.772  -5.490  0.09  0.00
ATOM 14 1O4  bDM 1 -29.963  -6.003  -7.122 -0.66  0.00
ATOM 15 H4OA bDM 1 -29.993  -5.118  -6.751  0.43  0.00
ATOM 16 1C5  bDM 1 -28.865  -6.650  -5.081  0.10  0.00
ATOM 17 H5A  bDM 1 -27.963  -7.009  -5.622  0.10  0.00
ATOM 18 1C6  bDM 1 -28.730  -5.254  -4.552  0.05  0.00
ATOM 19 H61A bDM 1 -29.694  -5.009  -4.056  0.09  0.00
ATOM 20 H61B bDM 1 -28.509  -4.622  -5.438  0.09  0.00
ATOM 21 1O6  bDM 1 -27.593  -5.254  -3.684 -0.66  0.00
ATOM 22 H6OA bDM 1 -27.699  -5.900  -2.982  0.43  0.00
ATOM 23 1O5  bDM 1 -28.979  -7.582  -3.963 -0.40  0.00
ATOM 24 2C1  bDM 1 -23.620  -9.286  -3.000  0.20  0.00
ATOM 25 H1B  bDM 1 -23.440 -10.274  -3.475  0.09  0.00
ATOM 26 2C2  bDM 1 -24.806  -9.283  -2.026  0.14  0.00
ATOM 27 H2B  bDM 1 -24.867  -8.235  -1.662  0.09  0.00
ATOM 28 2O2  bDM 1 -24.477 -10.097  -0.884 -0.66  0.00
ATOM 29 H2OB bDM 1 -23.792  -9.775  -0.294  0.43  0.00
ATOM 30 2C3  bDM 1 -26.163  -9.642  -2.661  0.14  0.00
ATOM 31 H3B  bDM 1 -26.142 -10.663  -3.098  0.09  0.00
ATOM 32 2O3  bDM 1 -27.232  -9.397  -1.722 -0.66  0.00
ATOM 33 H3OB bDM 1 -27.384 -10.156  -1.155  0.43  0.00
ATOM 34 2C4  bDM 1 -26.364  -8.872  -3.987  0.10  0.00
ATOM 35 H4B  bDM 1 -26.533  -7.835  -3.626  0.10  0.00
ATOM 36 2C5  bDM 1 -25.089  -8.936  -4.892  0.25  0.00
ATOM 37 H5B  bDM 1 -24.906  -9.942  -5.326  0.09  0.00
ATOM 38 2C6  bDM 1 -25.225  -7.980  -6.074  0.05  0.00
ATOM 39 H62A bDM 1 -25.159  -6.910  -5.780  0.09  0.00
ATOM 40 H62B bDM 1 -26.236  -8.045  -6.532  0.09  0.00
ATOM 41 2O5  bDM 1 -24.218  -8.289  -7.105 -0.66  0.00
ATOM 42 H5OB bDM 1 -24.661  -8.895  -7.704  0.43  0.00
ATOM 43 2O4  bDM 1 -24.011  -8.432  -4.077 -0.40  0.00
ATOM 44 2O1  bDM 1 -22.364  -8.895  -2.386 -0.30  0.00
ATOM 45 C7   bDM 1 -21.159  -9.105  -3.148 -0.11  0.00
ATOM 46 H7A  bDM 1 -20.922 -10.188  -3.228  0.09  0.00
ATOM 47 H7B  bDM 1 -21.320  -8.848  -4.217  0.09  0.00
ATOM 48 C8   bDM 1 -19.961  -8.389  -2.410 -0.18  0.00
ATOM 49 H8A  bDM 1 -19.829  -8.778  -1.378  0.09  0.00
ATOM 50 H8B  bDM 1 -20.171  -7.300  -2.464  0.09  0.00
ATOM 51 C9   bDM 1 -18.547  -8.641  -3.005 -0.18  0.00
ATOM 52 H9A  bDM 1 -18.718  -8.465  -4.089  0.09  0.00
ATOM 53 H9B  bDM 1 -18.415  -9.744  -3.010  0.09  0.00
ATOM 54 C10  bDM 1 -17.452  -7.785  -2.397 -0.18  0.00
ATOM 55 H10A bDM 1 -16.675  -7.915  -3.180  0.09  0.00
ATOM 56 H10B bDM 1 -17.700  -6.702  -2.407  0.09  0.00
ATOM 57 C11  bDM 1 -16.987  -8.238  -1.043 -0.18  0.00
ATOM 58 H11A bDM 1 -16.658  -9.299  -1.039  0.09  0.00
ATOM 59 H11B bDM 1 -17.874  -8.295  -0.376  0.09  0.00
ATOM 60 C12  bDM 1 -15.798  -7.399  -0.595 -0.18  0.00
ATOM 61 H12A bDM 1 -16.131  -6.343  -0.678  0.09  0.00
ATOM 62 H12B bDM 1 -14.966  -7.559  -1.314  0.09  0.00
ATOM 63 C13  bDM 1 -15.271  -7.639   0.808 -0.18  0.00
ATOM 64 H13A bDM 1 -15.139  -8.740   0.874  0.09  0.00
ATOM 65 H13B bDM 1 -15.946  -7.348   1.641  0.09  0.00
ATOM 66 C14  bDM 1 -13.783  -7.068   1.047 -0.18  

[gmx-users] CHARMM - gromacs epsilon and sigma conversiion factors

2010-09-24 Thread ABEL Stephane 175950
Hi all,
 
I would like to add new  atom types in the charmm27.ff for futures simulations 
of glyolipids in water with gmx 4.5.1. I have finished to convert the bonded in 
GROMACS format. However, I am little puzzled with the vdW paramaters. I would 
like to know how to convert them (i.e. what are the conversion factors used to 
convert the CHARMM sigma and epsilon parameters to gromacs sigma and epsilon 
values ?).
 
For example for the chloride atom CLA
 
CHARMM 27 
 
; atom  ignoredepsilon  Rmin/2   ignored   eps,1-4   Rmin/2,1-4
CLA  0.0   -0.150 2.27  ! chloride
 
GROMACS ffcharmmnb.itp
 
;name at.num mass charge ptype sigma epsilon
CLA 17 35.45 -1.00 A 0.404468018036 0.6276 
 
Thanks in advance for your help
 
Stefane 
 
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[gmx-users] charmm to gromacs nonbonded parameters after conversion

2010-09-12 Thread ABEL Stephane 175950
Hi GMX users,
 
I would like to perform MD with new developped CHARMM parameters in GROMACS. 
Since these parameters are new, they are not presents in the ffcharm*.itp files 
 given in the of charmm27.ff in the latest GMX distribution. So I have already 
made the conversions for the bonded parameters. In case of the nonbonded 
parameters, I have added the LJ values for the new atom types at the end of the 
 NONBONDED section of a par_all_27_lipid.prm file downloaded from the CHARMM 
website. To convert the LJ values in GROMACS format, I used the perl script of 
M. Abraham :  convert_charmm_to_gromacs.pl (v.1.3) as follow : 
 
perl convert_charmm_to_gromacs.pl  par_all27_lipid.prm
 
I obtain the ffcharmm.itp and ffcharmmnb.itp files as expected. In the 
ffcharmmnb.itp the [ atomtypes ] section is present but not the [ pairtypes ] 
section. Moreover the values in the  [ atomtypes ]  are different compared to 
same file given in latest GMX distrib (see below). Why these differences ?
- My ffcharmmnb.itp file 
[ atomtypes ]
;name mass charge ptype c6   c12

 CTL1 12.011000   0.0 A -0.001485 -6.588e-06 ; -0.000252 -3.793e-07
 CTL2 12.011000   0.0 A -0.001978 -4.173e-06 ; -0.000252 -3.793e-07
 CTL3 12.011000   0.0 A -0.003011 -6.944e-06 ; -0.000252 -3.793e-07
 CTL5 12.011000   0.0 A -0.003274 -8.007e-06 ; -0.000252 -3.793e-07
 CEL1 12.011000   0.0 A -0.003035 -8.095e-06

-- GROMACS 4.5.1  ffcharmmnb.itp

[ atomtypes ]
;name at.num mass charge ptype sigma epsilon

CTL1 6 12.01100 0.14 A 0.405358916754 0.08368 
CTL2 6 12.01100 0.05 A 0.358141284692 0.234304
CTL3 6 12.01100 -0.27 A 0.363486677001 0.326352 
CTL5 6 12.01100 -0.35 A 0.367050271874 0.33472
CEL1 6 12.01100 -0.15 A 0.372395664183 0.284512 
.
Thank in advance for your halp 
 
Stefane
 

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[gmx-users] How to center molecules in the box with trjconv ?

2010-08-21 Thread ABEL Stephane 175950
It works !!!
 
Thank you Justin
 
A bientôt 

Stefane


ABEL Stephane 175950 wrote:
 Hi all,

 I have simulated a system containing 55 DPC molecules, a peptide some ions
 and water in a cubic box. Initially all molecules were placed randomly in the
 box. As expected during the simulation all the DPC molecules aggregate to
 form a stable micelle with the peptide located at the micelle interface.

 Now I would like to plot some MD configs in a PDB format some configs where
 the micelle and the peptide are placed in the center of the box. To take into
 account the PBC and to obtain the PDB, for the last frame at 150 ns as I used
 trjconv with the following commands:

 1-  trjconv_mpi -f traj_KTM17_DPC_all.xtc -s hMRP1_K-TM17_DPC.tpr -pbc nojump
 -b 15 -e 15 -o traj_KTM17_DPC_0ns_noJump.pdb

 With non-SOL (DPC and peptide) as a group for output and where
 traj_KTM17_DPC_all.xtc is the trajectory with *no* PBC transformation

 2-  trjconv_mpi -f traj_KTM17_DPC_0ns_noJump.pdb -s hMRP1_K-TM17_dpc.gro
 -center -o traj_KTM17_DPC_0ns_noJump_center.pdb

 With DPC as a group for centering and System (DPC and peptide) as a group
 for output. the *.gro file contains only the DPC and peptide.

 Unfortunately, these commands do not work since the micelle (and the peptide)
 are not in the box center. I have tried many others commands with -pbc as
 mol, res with no success.


I have never had much success using multi-molecule groups for centering or other
correction using trjconv.  Centering on the peptide, i.e. trjconv -pbc mol -ur
compact -center, should do the trick.  I have never found -pbc nojump to work
very well, for a reason that is still unknown to me.

-Justin

 I used GMX version 4.0.7

 Any advices would be helpful.

 Stefane



--


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




--

Message: 6
Date: Fri, 20 Aug 2010 13:19:54 -0400
From: Justin A. Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] intersting problem
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4c6eb93a.6010...@vt.edu
Content-Type: text/plain; charset=UTF-8; format=flowed



babu gokul wrote:
 dear all
 I want to calculate the how many water molecule are their with in 3.5 A
 of a particular atom. could anyone help me in this regard

g_dist -dist

-Justin

 E R Azhagiya singam



--


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




--

Message: 7
Date: Fri, 20 Aug 2010 21:55:40 +0200
From: XAvier Periole x.peri...@rug.nl
Subject: Re: [gmx-users] force constants for umbrellla histograms
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: daae7e83-e389-4dc8-9e38-517ab08d5...@rug.nl
Content-Type: text/plain; charset=US-ASCII; format=flowed; delsp=yes


The most important is that you have to put in trajectories that
are equilibrated! You can mix as much force constant values
you like but always equilibrated ...

Then the lower the force constant the longer the simulation needs
to be to reach equilibrium: larger conformational space accessible.
I can also imagine that a too strong force constant might deform
your molecules in a manner you should not.


 Then does it matter how many times you vary it, and how large ?
 In my
 sampling I have very good histograms up to 2 nm (force constant = 1000
 kj/mol), above 2nm they are not. I feel I may have to use a force
 constant of 500 for the next 3 or 4 windows, and even less again 
 (ca~ 50
 kj/mol) beyond that.

 Cheers

 Gavin


 XAvier Periole wrote:

 On Aug 20, 2010, at 5:12 PM, Gavin Melaugh wrote:

 Hi all

 Is is O.K to use different force constants for different sampling
 windows for the generation of the potential of mean force curves?
 Yes.

 Many Thanks

 Gavin
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[gmx-users] How to center molecules in the box with trjconj ?

2010-08-20 Thread ABEL Stephane 175950
Hi all,
 
I have simulated a system containing 55 DPC molecules, a peptide some ions and 
water in a cubic box. Initially all molecules were placed randomly in the box. 
As expected during the simulation all the DPC molecules aggregate to form a 
stable micelle with the peptide located at the micelle interface. 
 
Now I would like to plot some MD configs in a PDB format some configs where the 
micelle and the peptide are placed in the center of the box. To take into 
account the PBC and to obtain the PDB, for the last frame at 150 ns as I used 
trjconv with the following commands: 
 
1-  trjconv_mpi -f traj_KTM17_DPC_all.xtc -s hMRP1_K-TM17_DPC.tpr -pbc nojump 
-b 15 -e 15 -o traj_KTM17_DPC_0ns_noJump.pdb
 
With non-SOL (DPC and peptide) as a group for output and where 
traj_KTM17_DPC_all.xtc is the trajectory with *no* PBC transformation 
 
2-  trjconv_mpi -f traj_KTM17_DPC_0ns_noJump.pdb -s hMRP1_K-TM17_dpc.gro 
-center -o traj_KTM17_DPC_0ns_noJump_center.pdb 
 
With DPC as a group for centering and System (DPC and peptide) as a group for 
output. the *.gro file contains only the DPC and peptide.
 
Unfortunately, these commands do not work since the micelle (and the peptide) 
are not in the box center. I have tried many others commands with -pbc as mol, 
res with no success. 
 
I used GMX version 4.0.7 
 
Any advices would be helpful.
 
Stefane 
 
 
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[gmx-users] intrapeptide hbond existence map

2010-02-11 Thread ABEL Stephane 175950
Hi everybody, 

I am doing some analysis of the interpeptidique hbonds (INTRHB) during the 
aggregation in beta fuof 4 heptapeptides in water 

I have defined in a index file the Acceptor-Donor-Hydrogen atoms list for the 
28 INTRHB like this 

NH--CO


[intra_hbds]
4 17 5
18 26 19
27 43 28
44 52 45
53 60 54


to obtain the INTRHB existence map i used the command with gmx4.05

g_hbond_mpi -n 4_Peptide_53A6_hbonds.ndx -s 4_Peptide_53A6.tpr -f 
./XTC/Whole_Traj_53A6Center.xtc -b 40 -e 50 -hbn 
4_Peptide_53A6_hbonds_400_500ns_index -hbm 4_Peptide_53A6_hbonds_400_500ns_Map

The map show in the x and y axis the time and residue (up to 84). I have no 
idea what the figure means. The olot is stored here 
http://www.st-abel.com/Hbond_occupency.jpg

I want only to know if, for example, the Hbond_occupency for the group NH or CO 
of the residu 1 

Thank you in advance for your help

Stephane






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[gmx-users] intrapeptide hbond existence map

2010-02-11 Thread ABEL Stephane 175950
Ok thank you all for your suggestions

A bientot



 ABEL Stephane 175950 wrote:
 Hi everybody,
 I am doing some analysis of the interpeptidique hbonds (INTRHB) 
 during the aggregation in beta fuof 4 heptapeptides in water
 I have defined in a index file the Acceptor-Donor-Hydrogen atoms list 
 for the 28 INTRHB like this
 NH--CO


 [intra_hbds]
 4 17 5
 18 26 19
 27 43 28
 44 52 45
 53 60 54
 

 to obtain the INTRHB existence map i used the command with gmx4.05

 g_hbond_mpi -n 4_Peptide_53A6_hbonds.ndx -s 4_Peptide_53A6.tpr -f 
 ./XTC/Whole_Traj_53A6Center.xtc -b 40 -e 50 -hbn 
 4_Peptide_53A6_hbonds_400_500ns_index -hbm 
 4_Peptide_53A6_hbonds_400_500ns_Map

 The map show in the x and y axis the time and residue (up to 84). I 
 have no idea what the figure means. The olot is stored here 
 http://www.st-abel.com/Hbond_occupency.jpg

 I want only to know if, for example, the Hbond_occupency for the 
 group NH or CO of the residu 1

 The output file -hbn 4_Peptide_53A6_hbonds_400_500ns_index maps the 
 donor-acceptor pairs to the plot. Find within that index file a 
 directive that starts with hbonds that corresponds to all of the 
 H-bonds that were found, and thus plotted. Red indicates the H-bond 
 exists, white means it doesn't. As for occupancy, you'd probably have 
 to script that to parse the .xpm file and calculate a percentage of 
 frames for when the particular H-bond exists, or get lifetimes from 
 g_hbond.

 -Justin
.or to define smaller index groups, e.g. the NH- or CO-group of res 1, 
and get the number of hydrogen bonds as function of time from the -num 
output (default is hbnum.xvg). You would have to repeat this for all 
(reasonable combinations of) hbonding groups that you're interested in, 
which can result in maaany g_hbond executions. But if the number of 
groups are small, then it's certainly doable. It seems from your plot 
though, that scripted processing of the -hbm and -hbn output, as Justin 
suggests, is the way to go here. Make sure you're matching the index 
file to the xpm file in the right way! I've made mistakes in that area 
myself.

Erik


 Thank you in advance for your help

 Stephane










-- 
---
Erik Marklund, PhD student
Laboratory of Molecular Biophysics,
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://xray.bmc.uu.se/molbiophys



--

Message: 5
Date: Thu, 11 Feb 2010 09:49:42 -0800
From: Lum Nforbi lumngwe...@gmail.com
Subject: [gmx-users] Working with Reduced Units
To: gmx-users@gromacs.org
Message-ID:
f7e1d8851002110949w126829c5y3f5f2859cef45...@mail.gmail.com
Content-Type: text/plain; charset=iso-8859-1

Hi all,

   Please, can someone shed more light on how to set up reduced units in
an .mdp file? I have tried to this but it does not work. I set epsilon,
sigma and mass to 1 in my force field file as stated in section 2.3 of the
manual. I multiplied 300K temperature by 0.00831451 and divided by epsilon
to get a temperature in reduced units with value 2.5. I also calculated the
pressure of 1bar in reduced units as shown on Table 2.4 of the manual to get
a value of 0.0431 and included all of these in the .mdp file but this did
not work for me in the mdrun.
  Is this the right way to set up reduced units in gromacs? Please, help
me out.

Thanks,
Lum
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Message: 6
Date: Thu, 11 Feb 2010 18:40:10 +
From: Rebeca Garc?a Fandi?o rega...@hotmail.com
Subject: [gmx-users] different results in different machines
To: gmx-users@gromacs.org
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End of gmx-users Digest, Vol 70, Issue 75
*

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[gmx-users] perl scripts to convert CHARMM ff in GROMACS

2010-02-01 Thread ABEL Stephane 175950
Hi GMXusers

I am testing the parameters of CHARMM, it works fine for lipids and protein. 
This is a great job, thanks to the devellopers But i would like to add some new 
molecule for solvent (e.g. for TFE) The atom types of TFE are present in the 
ffcharmm27bon.itp available in latest port (c32b1_release_1.1.zip, dowloaded 
http://www.dbb.su.se/User:Bjelkmar/Ffcharmm), unfortunately several bonded 
parameters (for example  F3-CF3, CF3-CT2x, etc..) are missing in 
ffcharmm27bon.itp file. So I need to convert the missing parameters into 
gromacs format. In website 
(URL:http://www.gromacs.org/@api/deki/files/76/=charmm_to_gromacs.tgz), I have 
found that several perl scripts exist for the conversion charmm-- gromacs. The 
archive is corrupted so, I cannot unpacked the directory to obtain the files.

Where I can find these scripts

Thanks in advance for your help

Stephane

  
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[gmx-users] amidated C-terminus in the charmm ff port for gromacs

2010-01-28 Thread ABEL Stephane 175950
Hi everybody

I am currently testing the CHARMM port for GROMACS pre4.1. I have downloaded 
the c32b1_release_1.1.zip file http://www.dbb.su.se/User:Bjelkmar/Ffcharmm 
(11:59, 23 Oct 2009). My protein protein have an acetylated N-terminus and 
amidated C-terminus. According to the CHARMM force field, these groups are 
considered as two residus named ACE and CT2, respectively. In the 
ffcharmm27.rtp, only the statement ACE, NMA are presents, where is the CT2 
group in the file?

Thank you in advance for your help.

Stephane

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[gmx-users] RE : gmx-users Digest, Vol 69 , Issue 132

2010-01-26 Thread ABEL Stephane 175950
Thanks Justin

Indeed, It worked !!!

In french, one says: je ne dormirai pas idiot ce soir. 

Stéphane



Thank you Roland for your response

I have effectively downloaded from the 
http://repo.or.cz/w/gromacs.git/snapshot/HEAD.tar.gz, the HEAD version 
of gmx Unfortunately, the unpacked directory does not contain a 
configure file, I have only an configure.ac.

So my question is: how to obtain a fully fonctional version of 4.1 
without using git

Thank you for your response

 Hi,

 there is currently no web-interface on the official git server. Thus
 repo.or.wz is probably the best solution.
 I checked that http://repo.or.cz/w/gromacs.git/snapshot/HEAD.tar.gz is
 up-to-date.

 Roland

 On Tue, Feb 23, 2010 at 8:31 AM, intra\sa175950 stephane.a...@cea.frwrote:

   
  Hi all,



 For a future project, I would like to use gromacs for simulations with the
 CHARMM force field. I am aware that the CHARMM ff is not yet officially
 supported by gromacs, even if a paper about this port will be published
 soon. By reading the mailing list, I understand that a beta version of
 gmx4.1 is available for testing from the git depositary. I have tried to use
 git, but since I am behind a firewall, I cannot easily access to the
 depositary. I have tried to obtain a previous from
 http://repo.or.cz/w/gromacs.git through the master branch but I am not
 sure that the file downloaded was the latest version. Therefore, my question
 is how to obtain the latest version of pre gmx4.1 without using git ?



 Thank you for your help



 Stéphane

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--

Message: 3
Date: Tue, 26 Jan 2010 14:00:00 -0500
From: Justin A. Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] Re: Obtain a pre-version of gromacs 4.1
without git
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4b5f3bb0.1000...@vt.edu
Content-Type: text/plain; charset=windows-1252; format=flowed



Stephane Abel wrote:
 Thank you Roland for your response
 
 I have effectively downloaded from the 
 http://repo.or.cz/w/gromacs.git/snapshot/HEAD.tar.gz, the HEAD version 
 of gmx Unfortunately, the unpacked directory does not contain a 
 configure file, I have only an configure.ac.
 
 So my question is: how to obtain a fully fonctional version of 4.1 
 without using git
 

In the code you downloaded, there should be a script called bootstrap which 
you can execute to generate the configure file.

-Justin

 Thank you for your response

 Hi,

 there is currently no web-interface on the official git server. Thus
 repo.or.wz is probably the best solution.
 I checked that http://repo.or.cz/w/gromacs.git/snapshot/HEAD.tar.gz is
 up-to-date.

 Roland

 On Tue, Feb 23, 2010 at 8:31 AM, intra\sa175950 
 stephane.a...@cea.frwrote:

  
  Hi all,



 For a future project, I would like to use gromacs for simulations 
 with the
 CHARMM force field. I am aware that the CHARMM ff is not yet 
 officially
 supported by gromacs, even if a paper about this port will be published
 soon. By reading the mailing list, I understand that a beta version of
 gmx4.1 is available for testing from the git depositary. I have tried 
 to use
 git, but since I am behind a firewall, I cannot easily access to the
 depositary. I have tried to obtain a previous from
 http://repo.or.cz/w/gromacs.git through the master branch but I am not
 sure that the file downloaded was the latest version. Therefore, my 
 question
 is how to obtain the latest version of pre gmx4.1 without using git ?



 Thank you for your help



 Stéphane

 -- 
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at http://www.gromacs.org/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.
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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




--

Message: 4
Date: Wed, 27 Jan 2010 08:09:47 +1100
From: Dallas B. Warren dallas.war...@pharm.monash.edu.au
Subject: RE: [gmx-users] Ligand coming out while trying Drug-enzyme
tutorial
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID:
89907ea1dcfb7548a431c13a270f9dd508fd8...@prk-exch-01.vcp.local

[gmx-users] Making Commands Non-Interactive

2009-10-04 Thread ABEL Stephane 175950
Dear GMX Users,

I ask this question in this mailing list since probably a user have already 
encountered this similar problem. I would like to  post-process my trajectory 
with the command trjconv (in mpi mode). For this I use the following shell 
command: 

echo 0 | /usr/pbs/bin/mpiexec /scratch/name/gromacs-4.0.5/bin/trjconv_mpi -s 
Peptide_43A1_topol.tpr -f ./XTC/Whole_Traj_43A1.xtc -o 
./XTC/Whole_Traj_43A1noPBC.xtc -pbc mol -ur compact. With the selection 0 
(System) 

It works but since my simulations is very long ( 300ns) the command stops in 
the middle of the trajectory before to finish the process ( i suspect a time 
limit for using the interactive mode). So i would like to use a script to do 
the task. How to pass the choice 0 in the script (i.e. equivalent to the echo 
0). I use a bash shell and the command qsub to launch a mpi job. 

I have tried to adapt the examples available in the GMX website with a text 
file as suggested by the author in GROMACS site with no success. 

Thank you again for your help 

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[gmx-users] good Atom type in gromacs with the AMBER ff port

2009-09-30 Thread ABEL Stephane 175950
Hi gromacs users

I have a newbie question about the atom type in gromacs. I would like to 
simulate a peptide with AMBER ff (ffamber03) in gromacs v.4.05 , so I have 
downloaded the ffamber files and followed the explanation given in Sorin's lab 
homepage. To neutralize my system i have added one CL- ion in the simulation 
box, but i am not sure it was good ion (in a other word the CL- ion compatible 
with the AMBER ff and not the default ion parameters). Here what i did 

- Added ions.itp file the following directive:
 
#ifdef _FF_AMBER99
[ moleculetype ]
; molname   nrexcl
Cl-  1

[ atoms ]
; idat type res nr  residu name at name  cg nr  charge   mass
1 amber99_301   CL- CL   1  -1   35.4530
#endif

- Use the following command with genion 

genion_mpi -s ions.tpr -o beta-I-Ac-NH2_slv_AMBER_ions.gro -p topol.top -pname 
NA+ -nname CL- -nn 1 - genion passes correctly

It is correct ? If not what is wrong ?

Thanks in advance for your help. 

Stéphane
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Re: [gmx-users] Large fluctuation of protein temperature with nose hoover thermostat

2009-09-17 Thread ABEL Stephane 175950
OK thank you Omer, for you response



The group PROTEIN isn't very large as the group NONPROTEIN, therefore its
total kinetic energy fluctuates more.
--Omer.

On Wed, Sep 16, 2009 at 12:10, Stephane Abel stephane.a...@cea.fr wrote:

 tc-grps = Protein Non-Protein ; two coupling groups - more accurate
 tau_t = 0.4 0.4 ; time constant, in ps
 ref_t = 310 310 ; reference temperature, one for each group, in K

Energy Average RMSD Fluct. Drift Tot-Drift

 ---
 Temperature 310 2.46886 2.46886 6.12135e-07 0.0171398
 T-Protein 310 32.1134 32.1117 -4.10352e-05 -1.14898
 T-Non-Protein 310 2.47549 2.47548 8.55869e-07 0.0239643

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Message: 4
Date: Thu, 17 Sep 2009 01:39:15 -0700
From: Darrell Koskinen darre...@ece.ubc.ca
Subject: [gmx-users] Periodic Boundary Conditions  Location of Atoms
NearBox Edges
To: gmx-users@gromacs.org
Message-ID: 4ab1f5b3.5060...@ece.ubc.ca
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

Dear GROMACS Gurus,
In order to correctly model an infinite graphene sheet using periodic 
boundary conditions, should the box edges be located at the midpoints 
between the atomic bonds?

Thanks.

Darrell


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[gmx-users] .pdb to .gro = the atoms are not conneced with VMD

2008-10-05 Thread ABEL Stephane 175950
Hi,

VMD uses a heuristic method to know if some atoms are connected. Sometimes the 
method fails. To be sure (and see) the atoms are well connected in VMD, you 
need to provided a psf file with your pdb/gro in VMD. So in your case you gro 
files is correct (since you indicated that your system are correct). An 
alternative see you gro in other software in pymol to confirm. 


I hope it helps 


Stefane

--

Stéphane Abel, PhD
CEA Saclay DSV/IBITEC-S/SB2SM
91191 Saclay, FRANCE
website: http://www.st-abel.com

--



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Date: dim. 05/10/2008 12:00
À: gmx-users@gromacs.org
Objet : gmx-users Digest, Vol 54, Issue 18
 
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Today's Topics:

   1. PR after minimisation and PR of missing residues? (minnale )
   2. .pdb to .gro = the atoms are not conneced with VMD
  (Chih-Ying Lin)


--

Message: 1
Date: 5 Oct 2008 05:26:52 -
From: minnale  [EMAIL PROTECTED]
Subject: [gmx-users] PR after minimisation and PR of missing residues?
To: gmx-users1 gmx-users@gromacs.org
Message-ID: [EMAIL PROTECTED]
Content-Type: text/plain; charset=iso-8859-1


Hi all,
  I have two doubts on PR, may be these are trivial to you.

1.According to Gromacs procedure(from Gromacs tutorial) the sequential steps 
are (a)Energy minimisation (b)Position restrain with force constant descendant 
manner and finally (c)production. Here my doubt that, is it require to do 
energy minimisation between PR and production? because after PR the system 
equilibrating properly if do one minimisation the structure looses bad contacts 
with low energy, am I right?  

2.If my desire protein contain some missing residues(from PDB)rectified those 
residues by using INSIGHT-II. Later start simulations particularly at PR, is it 
require to keep restrain specifically on added missing residues or whole 
protein residues in .itp file?  

Any suggestions would be appreciated

Thanks in advance.
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Message: 2
Date: Sun, 5 Oct 2008 01:53:36 -0700
From: Chih-Ying Lin [EMAIL PROTECTED]
Subject: [gmx-users] .pdb to .gro = the atoms are not conneced with
VMD
To: gmx-users@gromacs.org
Message-ID:
[EMAIL PROTECTED]
Content-Type: text/plain; charset=ISO-8859-1

Hi
I make .pdb file to .gro file.

With the VMD, the atoms are seen NOT conneced.

Why?
Is there any possible errors in my .gro file?

Lin


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[gmx-users] do_dssp file format, Resolved !!!

2008-01-17 Thread ABEL Stephane 175950
Hi Gromacs Users 

My Problem with do_dssp is resolved : my do_dssp was strangely corrupted. After 
recompilation it works well. Thank you for all people who helped me. See U soon 
on this mailing list

Stefane
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[gmx-users] fit the secondary structure time serie graph in page

2008-01-17 Thread ABEL Stephane 175950
Hi gromacs users 

When I use the xpm2ps utility to made a ps graphic of the secondary structure 
with my xpm file, the graph obtained is show in portrait orientation and by 
consequence trucated because the page width is to small. How to change the 
orientation of graph with xpm2ps (for example a landscape orientation) to fit 
the graph in one page ? 

Thanks for your response 

Stefane
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[gmx-users] RE : gmx-users Digest, Vol 45, Issue 36

2008-01-11 Thread ABEL Stephane 175950
Thanks Justin for your reply

So I used the choice 5(MainChain), 6(MainChain+Cb) and 7(MainChain+H)to test. I 
obtained always the same error. 

Opening library file /applications/gromacs-3.2.1/share/top/ss.map
Reading frame   0 time   -1.000
Back Off! I just backed up ddjapK9A to ./#ddjapK9A.1#

Note that the pdb seems correct because the secondary structure can be obtained 
with Stride available in VMD. And my trajectory was made CHARMM ffield. is this 
a problem in this case

Thank a lot 

My story with do_dssp 

As suggested David and others i rename my pdb file with the extension .pdb

i used the following command 

./do_dssp -s RM106-Cytc-CH22-SecStruc.pdb -f RM106-Cytc-CH22-SecStruc.pdb

A menu appears, I choose the group 1 (protein) and i obtained the error message 

Opening library file /applications/gromacs-3.2.1/share/top/ss.map
Reading frame   0 time   -1.000
Back Off! I just backed up ddjapK9A to ./#ddjapK9A.1#

What iis the problem. I give below a part of my pdb file

ATOM  1 CAY  ACE 1   6.421  -7.877 -11.574 -0.27  0.00
ATOM  2 HA1  ACE 1   6.050  -8.804 -12.062  0.09  0.00
ATOM  3 HA2  ACE 1   6.728  -7.203 -12.402  0.09  0.00
ATOM  4 HA3  ACE 1   5.529  -7.417 -11.098  0.09  0.00
ATOM  5 CACE 1   7.470  -8.140 -10.510  0.51  0.00
ATOM  6 OACE 1   7.594  -9.280 -10.074 -0.51  0.00
ATOM  7 NGLY 2   8.125  -7.096 -10.030 -0.47  0.00
ATOM  8 HN   GLY 2   7.927  -6.156 -10.295  0.31  0.00
ATOM  9 CA   GLY 2   8.970  -7.131  -8.819 -0.02  0.00
ATOM 10 HA1  GLY 2   8.889  -8.007  -8.193  0.09  0.00
ATOM 11 HA2  GLY 2   8.638  -6.265  -8.265  0.09  0.00
ATOM 12 CGLY 2  10.408  -6.734  -9.033  0.51  0.00
ATOM 13 OGLY 2  11.313  -7.365  -8.492 -0.51  0.00
ATOM 14 NASP 3  10.647  -5.532  -9.599 -0.47  0.00
ATOM 15 HN   ASP 3   9.863  -5.073 -10.011  0.31  0.00
ATOM 16 CA   ASP 3  11.864  -4.806  -9.831  0.07  0.00
ATOM 17 HA   ASP 3  12.713  -5.321  -9.406  0.09  0.00
ATOM 18 CB   ASP 3  12.026  -4.347 -11.282 -0.28  0.00
ATOM 19 HB1  ASP 3  11.065  -4.008 -11.725  0.09  0.00
ATOM 20 HB2  ASP 3  12.877  -3.652 -11.448  0.09  0.00
ATOM 21 CG   ASP 3  12.414  -5.579 -12.163  0.62  0.00
ATOM 22 OD1  ASP 3  11.641  -5.923 -13.130 -0.76  0.00
ATOM 23 OD2  ASP 3  13.571  -5.997 -12.137 -0.76  0.00

Thank you again for your kindly help

Stefane

ABEL Stephane 175950 wrote:
 I used the following command 
  
 ./do_dssp -s test.SecStruc.tpr with test.SecStruc.tpr is a pdb file with a 
 part is show below. I obtained a segmentation fault. 
  
 Maybe it is not a the good command. Remember that my trajectories are not 
 made/compatible with GROMACS and i have only a pdb coordinates of my MD.
  
don't rename the .pdb file to .tpr. Just use .pdb

-- 
David van der Spoel, Ph.D.
Molec. Biophys. group, Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205. Fax: +4618511755.
[EMAIL PROTECTED]   [EMAIL PROTECTED]   http://folding.bmc.uu.se


--

Message: 2
Date: Fri, 11 Jan 2008 09:30:47 +1100
From: Mark Abraham [EMAIL PROTECTED]
Subject: Re: [gmx-users] Re: Targeted MD
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: [EMAIL PROTECTED]
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

Steven Kirk wrote:
 Mark Abraham [EMAIL PROTECTED] wrote

 Non-Protein serves well here. So a usual tc-grps line has Protein 
 Non-Protein for a protein simulation.

 Mark
 
 A supplementary question.
 
 The tc-grps line can take predefined standard group names such as 
 'System', 'Protein' and 'Non-Protein'.
 
 Does the 'Protein' group need to actually BE a protein, or are 'Protein' 
 and 'Non-Protein' really synonyms for 
 'PresumablyBigMoleculeOfInterestProteinOrNot' and 'EverythingElse' ?

I haven't read the code or found any mention in the manual, but I expect 
that src/share/top/aminoacids.dat contains the names of any amino acids, 
and thus implicitly defines these groups.

Mark


--

Message: 3
Date: Fri, 11 Jan 2008 09:24:40 +0800
From: xuji[EMAIL PROTECTED]
Subject: [gmx-users] Asking help about PME
To: gmx-users@gromacs.org gmx-users@gromacs.org
Message-ID: [EMAIL PROTECTED]
Content-Type: text/plain; charset=gb2312

Hi all gromacs users:

I am digging into the PME method in gromacs. Can someone tell
me what files have something to do with PME and the corresponding
method FFT? 
 
Thanks!



Best wishes!

Ji Xu
Institute of Process Engineering
Chinese Academy of Sciences
P.O.Box 353, Beijing, 100080, China
Tel: +86-10-82627076
Fax:+86-10-62558065
[EMAIL PROTECTED]

2008-01-11

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[gmx-users] do_dssp file format

2008-01-11 Thread ABEL Stephane 175950
My story with do_dssp 
continues...https://webmail.cea.fr/Exchange/Stephane.ABEL/Bo%C3%AEte%20de%20r%C3%A9ception/?Cmd=contentsPage=1
 Boîte de réception 

As suggested David and others i rename my pdb file with the extension .pdb

i used the following command 

./do_dssp -s RM106-Cytc-CH22-SecStruc.pdb -f RM106-Cytc-CH22-SecStruc.pdb

A menu appears, I choose the group 1 (protein) and i obtained the error message 

Opening library file /applications/gromacs-3.2.1/share/top/ss.map
Reading frame   0 time   -1.000
Back Off! I just backed up ddjapK9A to ./#ddjapK9A.1#

What iis the problem. I give below a part of my pdb file

ATOM  1 CAY  ACE 1   6.421  -7.877 -11.574 -0.27  0.00
ATOM  2 HA1  ACE 1   6.050  -8.804 -12.062  0.09  0.00
ATOM  3 HA2  ACE 1   6.728  -7.203 -12.402  0.09  0.00
ATOM  4 HA3  ACE 1   5.529  -7.417 -11.098  0.09  0.00
ATOM  5 CACE 1   7.470  -8.140 -10.510  0.51  0.00
ATOM  6 OACE 1   7.594  -9.280 -10.074 -0.51  0.00
ATOM  7 NGLY 2   8.125  -7.096 -10.030 -0.47  0.00
ATOM  8 HN   GLY 2   7.927  -6.156 -10.295  0.31  0.00
ATOM  9 CA   GLY 2   8.970  -7.131  -8.819 -0.02  0.00
ATOM 10 HA1  GLY 2   8.889  -8.007  -8.193  0.09  0.00
ATOM 11 HA2  GLY 2   8.638  -6.265  -8.265  0.09  0.00
ATOM 12 CGLY 2  10.408  -6.734  -9.033  0.51  0.00
ATOM 13 OGLY 2  11.313  -7.365  -8.492 -0.51  0.00
ATOM 14 NASP 3  10.647  -5.532  -9.599 -0.47  0.00
ATOM 15 HN   ASP 3   9.863  -5.073 -10.011  0.31  0.00
ATOM 16 CA   ASP 3  11.864  -4.806  -9.831  0.07  0.00
ATOM 17 HA   ASP 3  12.713  -5.321  -9.406  0.09  0.00
ATOM 18 CB   ASP 3  12.026  -4.347 -11.282 -0.28  0.00
ATOM 19 HB1  ASP 3  11.065  -4.008 -11.725  0.09  0.00
ATOM 20 HB2  ASP 3  12.877  -3.652 -11.448  0.09  0.00
ATOM 21 CG   ASP 3  12.414  -5.579 -12.163  0.62  0.00
ATOM 22 OD1  ASP 3  11.641  -5.923 -13.130 -0.76  0.00
ATOM 23 OD2  ASP 3  13.571  -5.997 -12.137 -0.76  0.00

Thank you again for your kindly help

Stefane

ABEL Stephane 175950 wrote:
 I used the following command 
  
 ./do_dssp -s test.SecStruc.tpr with test.SecStruc.tpr is a pdb file with a 
 part is show below. I obtained a segmentation fault. 
  
 Maybe it is not a the good command. Remember that my trajectories are not 
 made/compatible with GROMACS and i have only a pdb coordinates of my MD.
  
don't rename the .pdb file to .tpr. Just use .pdb

-- 
David van der Spoel, Ph.D.
Molec. Biophys. group, Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205. Fax: +4618511755.
[EMAIL PROTECTED]   [EMAIL PROTECTED]   http://folding.bmc.uu.se


--

Message: 2
Date: Fri, 11 Jan 2008 09:30:47 +1100
From: Mark Abraham [EMAIL PROTECTED]
Subject: Re: [gmx-users] Re: Targeted MD
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: [EMAIL PROTECTED]
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

Steven Kirk wrote:
 Mark Abraham [EMAIL PROTECTED] wrote

 Non-Protein serves well here. So a usual tc-grps line has Protein 
 Non-Protein for a protein simulation.

 Mark
 
 A supplementary question.
 
 The tc-grps line can take predefined standard group names such as 
 'System', 'Protein' and 'Non-Protein'.
 
 Does the 'Protein' group need to actually BE a protein, or are 'Protein' 
 and 'Non-Protein' really synonyms for 
 'PresumablyBigMoleculeOfInterestProteinOrNot' and 'EverythingElse' ?

I haven't read the code or found any mention in the manual, but I expect 
that src/share/top/aminoacids.dat contains the names of any amino acids, 
and thus implicitly defines these groups.

Mark


--

Message: 3
Date: Fri, 11 Jan 2008 09:24:40 +0800
From: xuji[EMAIL PROTECTED]
Subject: [gmx-users] Asking help about PME
To: gmx-users@gromacs.org gmx-users@gromacs.org
Message-ID: [EMAIL PROTECTED]
Content-Type: text/plain; charset=gb2312

Hi all gromacs users:

I am digging into the PME method in gromacs. Can someone tell
me what files have something to do with PME and the corresponding
method FFT? 
 
Thanks!



Best wishes!

Ji Xu
Institute of Process Engineering
Chinese Academy of Sciences
P.O.Box 353, Beijing, 100080, China
Tel: +86-10-82627076
Fax:+86-10-62558065
[EMAIL PROTECTED]

2008-01-11

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Message: 4
Date: Fri, 11 Jan 2008 13:10:11 +1100
From: Mark Abraham [EMAIL PROTECTED]
Subject: Re: [gmx-users] Asking help about PME
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: [EMAIL PROTECTED]
Content-Type: text

[gmx-users] do_dssp file format

2008-01-11 Thread ABEL Stephane 175950
 -11.574 -0.27  0.00
 ATOM  2 HA1  ACE 1   6.050  -8.804 -12.062  0.09  0.00
 ATOM  3 HA2  ACE 1   6.728  -7.203 -12.402  0.09  0.00
 ATOM  4 HA3  ACE 1   5.529  -7.417 -11.098  0.09  0.00
 ATOM  5 CACE 1   7.470  -8.140 -10.510  0.51  0.00
 ATOM  6 OACE 1   7.594  -9.280 -10.074 -0.51  0.00
 ATOM  7 NGLY 2   8.125  -7.096 -10.030 -0.47  0.00
 ATOM  8 HN   GLY 2   7.927  -6.156 -10.295  0.31  0.00
 ATOM  9 CA   GLY 2   8.970  -7.131  -8.819 -0.02  0.00
 ATOM 10 HA1  GLY 2   8.889  -8.007  -8.193  0.09  0.00
 ATOM 11 HA2  GLY 2   8.638  -6.265  -8.265  0.09  0.00
 ATOM 12 CGLY 2  10.408  -6.734  -9.033  0.51  0.00
 ATOM 13 OGLY 2  11.313  -7.365  -8.492 -0.51  0.00
 ATOM 14 NASP 3  10.647  -5.532  -9.599 -0.47  0.00
 ATOM 15 HN   ASP 3   9.863  -5.073 -10.011  0.31  0.00
 ATOM 16 CA   ASP 3  11.864  -4.806  -9.831  0.07  0.00
 ATOM 17 HA   ASP 3  12.713  -5.321  -9.406  0.09  0.00
 ATOM 18 CB   ASP 3  12.026  -4.347 -11.282 -0.28  0.00
 ATOM 19 HB1  ASP 3  11.065  -4.008 -11.725  0.09  0.00
 ATOM 20 HB2  ASP 3  12.877  -3.652 -11.448  0.09  0.00
 ATOM 21 CG   ASP 3  12.414  -5.579 -12.163  0.62  0.00
 ATOM 22 OD1  ASP 3  11.641  -5.923 -13.130 -0.76  0.00
 ATOM 23 OD2  ASP 3  13.571  -5.997 -12.137 -0.76  0.00

 Thank you again for your kindly help

 Stefane

 ABEL Stephane 175950 wrote:
  I used the following command
 
  ./do_dssp -s test.SecStruc.tpr with test.SecStruc.tpr is a pdb file with a
 part is show below. I obtained a segmentation fault.
 
  Maybe it is not a the good command. Remember that my trajectories are not
 made/compatible with GROMACS and i have only a pdb coordinates of my MD.
 
 don't rename the .pdb file to .tpr. Just use .pdb

 --
 David van der Spoel, Ph.D.
 Molec. Biophys. group, Dept. of Cell  Molec. Biol., Uppsala University.
 Box 596, 75124 Uppsala, Sweden. Phone:+46184714205. Fax: +4618511755.
 [EMAIL PROTECTED] [EMAIL PROTECTED]   http://folding.bmc.uu.se


 --

 Message: 2
 Date: Fri, 11 Jan 2008 09:30:47 +1100
 From: Mark Abraham [EMAIL PROTECTED]
 Subject: Re: [gmx-users] Re: Targeted MD
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: [EMAIL PROTECTED]
 Content-Type: text/plain; charset=ISO-8859-1; format=flowed

 Steven Kirk wrote:
  Mark Abraham [EMAIL PROTECTED] wrote

  Non-Protein serves well here. So a usual tc-grps line has Protein
  Non-Protein for a protein simulation.
 
  Mark
 
  A supplementary question.
 
  The tc-grps line can take predefined standard group names such as
  'System', 'Protein' and 'Non-Protein'.
 
  Does the 'Protein' group need to actually BE a protein, or are 'Protein'
  and 'Non-Protein' really synonyms for
  'PresumablyBigMoleculeOfInterestProteinOrNot' and 'EverythingElse' ?

 I haven't read the code or found any mention in the manual, but I expect
 that src/share/top/aminoacids.dat contains the names of any amino acids,
 and thus implicitly defines these groups.

 Mark


 --

 Message: 3
 Date: Fri, 11 Jan 2008 09:24:40 +0800
 From: xuji[EMAIL PROTECTED]
 Subject: [gmx-users] Asking help about PME
 To: gmx-users@gromacs.org gmx-users@gromacs.org
 Message-ID: [EMAIL PROTECTED]
 Content-Type: text/plain; charset=gb2312

 Hi all gromacs users:

 I am digging into the PME method in gromacs. Can someone tell
 me what files have something to do with PME and the corresponding
 method FFT?

 Thanks!
 


 Best wishes!

 Ji Xu
 Institute of Process Engineering
 Chinese Academy of Sciences
 P.O.Box 353, Beijing, 100080, China
 Tel: +86-10-82627076
 Fax:+86-10-62558065
 [EMAIL PROTECTED]

 2008-01-11
 
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 Message: 4
 Date: Fri, 11 Jan 2008 13:10:11 +1100
 From: Mark Abraham [EMAIL PROTECTED]
 Subject: Re: [gmx-users] Asking help about PME
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: [EMAIL PROTECTED]
 Content-Type: text/plain; charset=GB2312

 xuji wrote:
 
  Hi all gromacs users:
 
  I am digging into the PME method in gromacs. Can someone tell
  me what files have something to do with PME and the corresponding
  method FFT?

 From the gromacs source directory, try

 find * -name *pme*

 and

 grep -i pme src/*/*.c include/*.h include/*/*.h | grep -v -i development

 Mark


 --

 Message: 5
 Date: Fri, 11 Jan 2008 10:44:05 +0800
 From: Yang Ye [EMAIL PROTECTED]
 Subject: Re: [gmx-users] Asking help about PME
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: [EMAIL

[gmx-users] do_dssp file format

2008-01-10 Thread ABEL Stephane 175950
 Hi gromacs users

 For my work I have performed some simulations of a protein in water with an 
 other MD software not compatible with GROMACS. And I would like to compute 
 the time evolution of the secondary structure of my protein, I know that the 
 with the xpm2ps tool give in gromacs. Is it possible to have an (small) 
 exemple of an .xpm file generated by the do_dssp tools

Just run a 10-step MD simulation and generate one yourself. Or convert
your other trajectories into .pdb format and use that as input to
do_dssp. You do not necessarily need a .tpr file for do_dssp, see man
do_dssp under the -s flag.

Mark

Thanks Mark for your suggestions but it is not working for me So i have tested 
an other approach with VMD to obtain the secondary structure time series for my 
protein. The ouput graph obtained is not pretty, so i would like to make for a 
paper a same graph that i found in some gromacs papers. For this i need to 
convert the output datas file of VMD to gromacs xpm file obtained with do_dssp 
with a script and convert it to ps with the xpm2ps tool. In gromacs 
documentation i can not find an exemple of xpm file generated with do_dssp. So 
it is possible to obtain from the gromacs users a small exemple of this file to 
see how the datas are arranged

Thank you very much

Stefane
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[gmx-users] do_dssp file format

2008-01-10 Thread ABEL Stephane 175950
I used the following command 
 
./do_dssp -s test.SecStruc.tpr with test.SecStruc.tpr is a pdb file with a part 
is show below. I obtained a segmentation fault. 
 
Maybe it is not a the good command. Remember that my trajectories are not 
made/compatible with GROMACS and i have only a pdb coordinates of my MD.
 
 
Any help will be appreciate
 
Stefane
 
 
ATOM  1 CAY  ACE 1   6.421  -7.877 -11.574 -0.27  0.00
ATOM  2 HA1  ACE 1   6.050  -8.804 -12.062  0.09  0.00
ATOM  3 HA2  ACE 1   6.728  -7.203 -12.402  0.09  0.00
ATOM  4 HA3  ACE 1   5.529  -7.417 -11.098  0.09  0.00
ATOM  5 CACE 1   7.470  -8.140 -10.510  0.51  0.00
ATOM  6 OACE 1   7.594  -9.280 -10.074 -0.51  0.00
ATOM  7 NGLY 2   8.125  -7.096 -10.030 -0.47  0.00
ATOM  8 HN   GLY 2   7.927  -6.156 -10.295  0.31  0.00
ATOM  9 CA   GLY 2   8.970  -7.131  -8.819 -0.02  0.00
ATOM 10 HA1  GLY 2   8.889  -8.007  -8.193  0.09  0.00
ATOM 11 HA2  GLY 2   8.638  -6.265  -8.265  0.09  0.00
ATOM 12 CGLY 2  10.408  -6.734  -9.033  0.51  0.00
ATOM 13 OGLY 2  11.313  -7.365  -8.492 -0.51  0.00
ATOM 14 NASP 3  10.647  -5.532  -9.599 -0.47  0.00
ATOM 15 HN   ASP 3   9.863  -5.073 -10.011  0.31  0.00
ATOM 16 CA   ASP 3  11.864  -4.806  -9.831  0.07  0.00
ATOM 17 HA   ASP 3  12.713  -5.321  -9.406  0.09  0.00
ATOM 18 CB   ASP 3  12.026  -4.347 -11.282 -0.28  0.00
ATOM 19 HB1  ASP 3  11.065  -4.008 -11.725  0.09  0.00
ATOM 20 HB2  ASP 3  12.877  -3.652 -11.448  0.09  0.00
ATOM 21 CG   ASP 3  12.414  -5.579 -12.163  0.62  0.00
ATOM 22 OD1  ASP 3  11.641  -5.923 -13.130 -0.76  0.00
ATOM 23 OD2  ASP 3  13.571  -5.997 -12.137 -0.76  0.00

 
 
 
 
 
 
 



--

Message: 3
Date: Thu, 10 Jan 2008 13:03:30 -0500
From: Justin A. Lemkul [EMAIL PROTECTED]
Subject: Re: [gmx-users] do_dssp file format
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: [EMAIL PROTECTED]
Content-Type: text/plain; charset=ISO-8859-1

Quoting ABEL Stephane 175950 [EMAIL PROTECTED]:

  Hi gromacs users
 
  For my work I have performed some simulations of a protein in water with an
 other MD software not compatible with GROMACS. And I would like to compute
 the time evolution of the secondary structure of my protein, I know that the
 with the xpm2ps tool give in gromacs. Is it possible to have an (small)
 exemple of an .xpm file generated by the do_dssp tools

 Just run a 10-step MD simulation and generate one yourself. Or convert
 your other trajectories into .pdb format and use that as input to
 do_dssp. You do not necessarily need a .tpr file for do_dssp, see man
 do_dssp under the -s flag.

 Mark

 Thanks Mark for your suggestions but it is not working for me So i have
 tested an other approach with VMD to obtain the secondary structure time
 series for my protein. The ouput graph obtained is not pretty, so i would
 like to make for a paper a same graph that i found in some gromacs papers.
 For this i need to convert the output datas file of VMD to gromacs xpm file
 obtained with do_dssp with a script and convert it to ps with the xpm2ps
 tool. In gromacs documentation i can not find an exemple of xpm file
 generated with do_dssp. So it is possible to obtain from the gromacs users a
 small exemple of this file to see how the datas are arranged

What exactly is not working?  As in, what commands are you issuing?  Did the
MD fail, or the analysis of the trajectory?  If you provide this type of
information, we may be able to help you better.

-Justin


 Thank you very much

 Stefane
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Justin A. Lemkul
Graduate Research Assistant
Department of Biochemistry
Virginia Tech
Blacksburg, VA
[EMAIL PROTECTED] | (540) 231-9080
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin/




--

Message: 4
Date: Thu, 10 Jan 2008 19:27:38 +0100
From: David van der Spoel [EMAIL PROTECTED]
Subject: Re: [gmx-users] Dihedral with parameters set to zero
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: [EMAIL PROTECTED]
Content-Type: text/plain; charset=ISO-8859-1; format=flowed

van Bemmelen wrote:
 OK. Now I'm confused. What did you mean by the second part?

 Of course, when doing FEP with the B state different, you would
 gradually introduce a dihedral

[gmx-users] do_dssp file format

2008-01-08 Thread ABEL Stephane 175950
Hi gromacs users

For my work I have performed some simulations of a protein in water with an 
other MD software not compatible with GROMACS. And I would like to compute the 
time evolution of the secondary structure of my protein, I know that the 
do_dssp tool in GROMACS is made for this. This tools also plot the results in 
.xpm matrix file which can be convert with the xpm2ps tool give in gromacs. Is 
it possible to have an (small) exemple of an .xpm file generated by the do_dssp 
tools

Thank you very much in advance for you help

Stefane


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