[gmx-users] Re:problem with simulation of freezing of water

2012-11-11 Thread ran friedman
Hi,

Also note that it is difficult to simulate the right structure of ice (Ih).
You didn't write what you want to study, but search the literature
carefully. You may need to use an ab-initio model.

Ran

Message: 7
Date: Sun, 11 Nov 2012 11:26:19 -0500
From: Justin Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] Re:problem with simulation of freezing of
water
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 509fd1ab.50...@vt.edu
Content-Type: text/plain; charset=UTF-8; format=flowed



On 11/11/12 11:22 AM, Ali Alizadeh wrote:
 Dear Justin

 Thank you for reply,

 I want to simulation of water freezing, my condition:

 pressure=300 bar and T=240 k , number 1656, run time= 100ns,

 I can not see regular structure of ice by MD simulation or by gromacs?

 In your opinion, if i want this structure of ice for my simulation,
 What can i do?


Start by searching the literature for a suitable protocol.  Ice simulations
have
been done before.  As I said before, each water model has a different
melting
point, and hardly any of them correspond to the actual experimental value.
 See
if you can produce a suitable simulation with a pressure of 1 bar (proof of
concept) and then change conditions.

What you have to keep in mind is that most water models were designed to
work at
ambient conditions for normal simulations.  They do not necessarily work
under
extremes or produce useful results under those conditions.

-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




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[gmx-users] Re: genion problem with divalent ions

2012-09-09 Thread ran friedman
Hi,
As a side note, you should be careful when using Mg (and probably all other
multiply charged ions, as well as large polarisable ions like I-). It's
very difficult to correctly represent the interactions of such ions in the
bulk correctly using non-polarisable force fields.
Ran

Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
http://lnu.se/ccbg



On 9 September 2012 16:10, gmx-users-requ...@gromacs.org wrote:



 Message: 2
 Date: Sun, 9 Sep 2012 13:53:35 +0200
 From: Matthias Ernst un...@student.kit.edu
 Subject: [gmx-users] genion problem with divalent ions
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 504c833f.2050...@student.kit.edu
 Content-Type: text/plain; charset=ISO-8859-15; format=flowed

 Hi,

 I just encountered (another) strange thing with genion.
 I wanted to neutralized a system by adding Mg-Ions (charge in ions.itp:
 2, forcefield amber99sb), so I expected half of the system charge (-52)
 to be added as ions. BUT it added the same amount, i.e. 52 Mg ions
 instead of 26 which would be needed for neutralization. The same holds
 for Zn or Ca ions, which also are divalent in ions.itp

 Could it be that the routines of genion to determine the number of ions
 are not working properly? I mean, the -neutral option also does work
 only if the -conc flag is also there and provides a value  0.0 (which
 in fact is not what I want when I just want do neutralize my system by
 adding ions...)

 Does anyone of you also had similar problems?

 Thank you,
 Matthias


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[gmx-users] RE: quasi-harmonic entropy calculation

2012-03-22 Thread Ran Friedman
Hi,
IIRC I tested g_anaeig when David wrote it and the results were the same as 
calc_entropies.pl, so it sounds strange. Are you sure you use the same input in 
both cases? Did you use the eigenvectors that correspond to the same 
eigenvalues? Also, how may eigenvalues are close to zero?
Ran

Message: 4
Date: Thu, 22 Mar 2012 10:27:36 -0400
From: wmira...@estudiantes.fbio.uh.cu
Subject: [gmx-users] Re: quasi-harmonic entropy calculation
To: gmx-users@gromacs.org
Message-ID: 5e667c140e0c268c9e87681be3535b89.squir...@est.fbio.uh.cu
Content-Type: text/plain;charset=iso-8859-1

My name is Williams. I am a Biochemistry student. I have done QH entropy
calculation using g_anaeig, but I found an old perl script at GROMACS web
site to do the same. The problem is that when I calculate entropy for the
loops of my protein the results are the same using g_anaeig or the old
perl script, but when I compare the entropy calculated through both
methods for my entire protein the results diverges in one order of
magnitud and I give to the script the same eigenvalues obtained by g_covar
(g_anaeig uses the eigenvectors). Please, help me.
Thanks

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[gmx-users] RE: g_clustsize

2011-07-28 Thread Ran Friedman
Dear Stefano,

I forward your question to the gromacs-users mailing list. Please send further 
inquiries there - there may be people more qualified than me to reply (unless 
you refer to my modified version or to one of my papers)

I'm not sure if the .xpm files give the information you're interested at but 
using g_clustsize -av and -hc is useful to get the average size and 
distribution. You can further use -mcn and extract the index group of the 
largest cluster. By a combination of scripting and other Gromacs tools you can 
get more info on the largest cluster per frame if you need it.

g_clustsize doesn't give you the radius of gyration of the cluster. My modified 
version does, but only for the largest cluster - not for all as you need I 
guess.

Good luck,
Ran


Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/ccbg



From: Stefano [boro...@unitus.it]
Sent: 26 July 2011 15:49
To: Ran Friedman
Subject:

Dear Prof Friedman
I am Stefano Borocci, a GROMACS user.
I am currently studying, through molecular dynamics simulations, the
self-assembly of Gemini surfactants.
I have some problems to use the g_clustsize of GROMACS and  I don't
understand the results obtained with this tool.

I have analyzed the xtc file of my trajectory

g_clustsize -f trj.xtc -s top.tpr -mol (and without) -cut 0.35

and the cluster size and cluster distributions predicted by g_clustsize
does not match with what I see by a visual analysis of trajectory (using
VMD).
I also tried to remove the periodic boundary (-pbc mol) without result.
I have two questions:
How to calculate the cluster (micelle) size and cluster distribution of
my sistem?
How to calculate the radius of gyration of the aggregates if in my box
there are more clusters (3 or 4)?

I would be very grateful if you could help me
Thanks in advance.

Best regards



  
Stefano Borocci

--
---
Dr Stefano Borocci
Laboratorio di Chimica e Chimica Computazionale
Dipartimento per la Innovazione nei Sistemi Biologici,
Agroalimentari e Forestali (DIBAF)
Università degli Studi della Tuscia
Largo dell'Università, snc 01100 Viterbo
Tel. +39-0761-357127
  +39-0761-357193
Fax  +39 0761-357179
e-mail: boro...@unitus.it
---

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[gmx-users] RE: Including quadrupole-charge interaction in GROMACS (WU Yanbin)

2011-06-16 Thread Ran Friedman
Hi,
Not implemented in Gromacs AFAIK.
Note that (1) even the definition of a quadruple isn't straightforwards and 
depends on the orientation and (2) common FF parameters were not developed with 
higher ordered multiple taken into account.

@Article{Plattner2009,
author = Plattner, N and Meuwly, M,
title = {Higher order multipole moments for molecular dynamics simulations},
journal = J Mol Model,
year = 2009,
volume = 15,
pages = 687-694
}

Ran

Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/ccbg



From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org] On Behalf 
Of gmx-users-requ...@gromacs.org [gmx-users-requ...@gromacs.org]
Sent: 16 June 2011 09:00
To: gmx-users@gromacs.org
Subject: gmx-users Digest, Vol 86, Issue 96

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Today's Topics:

   1. Re: CHARMM forcefield (Justin A. Lemkul)
   2. Re: local pressure calcuation for Gromacs-4.5 (Justin A. Lemkul)
   3. Including quadrupole-charge interaction in GROMACS (WU Yanbin)
   4. g_density (chris.ne...@utoronto.ca)
   5. Position restraints (Tom Dupree)
   6. Re: Position restraints (Mark Abraham)


--

Message: 1
Date: Wed, 15 Jun 2011 17:11:08 -0400
From: Justin A. Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] CHARMM forcefield
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4df91fec.8080...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



simon sham wrote:
 Hi,
 I have two questions about using the charmm force field.
 1. Do we still need to use the two perl scripts, convert_charmm_
 to_gromacs.pl and fix_top_for_charmm.pl?

No.

 2. I got the following note when I tried to do energy minim. with grompp:

 NOTE 1 [file topol.top]:
   The largest charge group contains 12 atoms.
   Since atoms only see each other when the centers of geometry of the charge
   groups they belong to are within the cut-off distance, too large charge
   groups can lead to serious cut-off artifacts.
   For efficiency and accuracy, charge group should consist of a few atoms.
   For all-atom force fields use: CH3, CH2, CH, NH2, NH, OH, CO2, CO, etc.

 Is this a problem?


Yes.  CHARMM topologies should not use charge groups.  You should invoke pdb2gmx
with the -nochargegrp option to create a proper topology.

-Justin

 Thanks for your insight!

 Simon


--


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: 2
Date: Wed, 15 Jun 2011 17:17:53 -0400
From: Justin A. Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] local pressure calcuation for Gromacs-4.5
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4df92181.2090...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



Amit Choubey wrote:
 Dear all,

 Could anyone direct me to the manual for local pressure calculation or a
 place where everything is mentioned about it ? I have been only able to
 collect bits and pieces from the mailing lists.


That's probably all there is to be found.  There's no manual linked from the git
web interface or the ftp site.

-Justin

 Thank you
 Amit

 On Wed, Jun 15, 2011 at 5:35 AM, Mark Abraham mark.abra...@anu.edu.au
 mailto:mark.abra...@anu.edu.au wrote:

 On 15/06/2011 9:09 PM, Jianguo Li wrote:
 Dear all,

 I have made a test calculation of local pressure using version 4.5
 for my membrane simulation using CHARMM FF. When rerun the
 simulation, mdrun gives the localpressure data. Howeve, instead of
 giving an anveraged data of the local pressure, mdrun gives a
 separate file for each frame, so I got many files:
 localpressure.dat0, localpressure.dat1, localpressure.dat2,
 localpressure.dat3 ..
 Then I need to calculate the pressure tensor for each frame and
 make average. but these localpressure.dat files are very big (each
 file is about 30 Mb), occupying large space of the hard disk. Can

[gmx-users] RE: Essential dynamics - concepts (Kavyashree M)

2011-06-06 Thread Ran Friedman
From: Tsjerk Wassenaar tsje...@gmail.com
Subject: Re: [gmx-users] Essential dynamics - concepts
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: BANLkTim7wkRbvJZiJJbuHg=mkp5dgfu...@mail.gmail.com
Content-Type: text/plain; charset=ISO-8859-1

Hi Kavya,

 Its g_covar contributed by Dr. Rossen apostolov if I am right.? Here it
 states that those which are having correlation coefficient better than 0.5
 will be reported, so covariance gives those which have correlation
 coefficient
 less than 0.5?

I don't know the modified version. But I presume that the components
with eigenvalues higher than 0.5 are written out, which is not quite
the same as having a correlation coefficient of 0.5.

 It's the correlation coefficient indeed. the version is available from the 
 Gromacs user contributions site.
 Ran
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[gmx-users] RE: Metal surfaces (Sergio Manzetti)

2011-04-28 Thread Ran Friedman
Hi,

That's unlikely, but maybe the following publications can help you to build the 
surface:


@Article{Iori2008,
author = Iori, F and Corni, S,
title = {Including image charge effects in the molecular dynamics simulations 
of molecules on metal surfaces},
journal = J Comput Chem,
year = 2008,
volume = 29,
pages = 1656-1666
}

@Article{Iori2009,
author = Iori, F and Di Felice, R and Molinari, E and Corni, S,
title = {{G}ol{P}: {A}n atomistic force-field to describe the interaction of 
proteins with {A}u(111) surfaces in water},
journal = J Comput Chem,
year = 2009,
volume = 30,
pages = 1465-1476
}

@article{Kalcher2009,
Author = {Kalcher, I. and Horinek, D. and Netz, R. R. and Dzubiella, J.},
Title = {{Ion specific correlations in bulk and at biointerfaces}},
Journal = {JOURNAL OF PHYSICS-CONDENSED MATTER},
Year = {{2009}},
Volume = {{21}},
Article-Number = {{424108}}
}


Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/ccbg


Hello, does anybody have an idea if there are availbale PDB files which
represent metal surfaces for transition state metals, to be used for MD?

BW

S
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[gmx-users] RE: micelles and trjconv -pbc cluste

2011-04-15 Thread Ran Friedman
Hi,
I've sent the program off list. I hope to have a version compatible with the 
current or future version of Gromacs and will then upload it to the user 
contributions.
Ran
--

Message: 2
Date: Thu, 14 Apr 2011 13:29:42 -0700 (PDT)
From: jim jack blhaw...@yahoo.com
Subject: [gmx-users] Re: micelles and trjconv -pbc cluster
To: gmx-users@gromacs.org
Message-ID: 401162.89007...@web35301.mail.mud.yahoo.com
Content-Type: text/plain; charset=iso-8859-1

Dear Ran Friedman and Tsjerk Wassennaar,
? ?First of all, thanks to all responses to my problem. As far as the modified 
versions of g_clustsize and trjconv, I really want to try them.??Best regards?

George Koros
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[gmx-users] RE: micelles and trjconv -pbc cluster

2011-04-14 Thread Ran Friedman
Hi,

Likewise, I have a modified version of g_clustsize that calculates the radius 
of gyration for the largest structure and can send you the code. 

Ran

Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/ccbg


Message: 4
Date: Thu, 14 Apr 2011 17:44:07 +0200
From: Tsjerk Wassenaar tsje...@gmail.com
Subject: Re: [gmx-users] micelles and trjconv -pbc cluster
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: BANLkTin-YV43F=s1r-ng8xnzj9ejeqr...@mail.gmail.com
Content-Type: text/plain; charset=iso-8859-1

Hi George,

Recently I wrote an alternative, non-iterative clustering routine, that does
not suffer from convergence failures. If you want, I can send you the
modified trjconv source code. Note that it does not bother about the center
of mass of the cluster, but just builds a network of neighbours, until there
are no more. If you're clusters are not periodic, it won't matter.

Let me know...

Cheers,

Tsjerk

On Thu, Apr 14, 2011 at 4:48 PM, Erik Marklund er...@xray.bmc.uu.se wrote:

  jim jack skrev 2011-04-14 16.42:

   Dear GROMACS users,

I am trying to simulate an SDS micelle in water. As simulation time goes
 by, the micelle approaches the edge of the box and consequently some of
 these molecules get in from the other side. This leads to incorrect radius
 of gyration, eccentricity, etc. A solution to this problem is the option 
 trjconv
 -pbc cluster as described in the page
 http://www.gromacs.org/Documentation/How-tos/Micelle_Clustering. In this
 case, the problem is that it takes a lot of time and a huge file (several
 GB) is created due to this procedure. Is there any other alternative?

 Thanks in advance

 George Koros

I don't think that the cluster option always converges. You could, if
 your micelle is intact at frame 0, first do trjconv -pbc nojump, then
 optionally trjconv -center. That should give a trajectory from which you
 could calculate the radius of gyration. If SDS molecules occationally leave
 the micelle and recombine with a priodic, then you might have a problem with
 the suggested approach.

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


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--
Tsjerk A. Wassenaar, Ph.D.

post-doctoral researcher
Molecular Dynamics Group
* Groningen Institute for Biomolecular Research and Biotechnology
* Zernike Institute for Advanced Materials
University of Groningen
The Netherlands
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[gmx-users] RE: Regarding DCCM analysis with g_covar available in user contributed section

2011-03-12 Thread Ran Friedman
Hi,
As stated below the upper half of the triangle shows correlations having r0.5 
or r-0.5, that is |r|0.5
Ran


From: bipin singh [bipinel...@gmail.com]
Sent: 12 March 2011 12:27
To: Discussion list for GROMACS users
Cc: r.fried...@bioc.uzh.ch
Subject: Regarding DCCM analysis with g_covar available in user contributed 
section

Hello,
I am using g_covar vailable in user contributed section (by Ran Friedman) the 
description available for the package is as follows:

This package contains a modified version of g_covar, which can print a matrix
of atomic correlation coefficients (with -xpmc) and write all pairs with a
correlation  0.5 to a log file (with -clog). Otherwise it is the same as the
original program.
The xpm correlation matrix shows only cross-correlations larger than 0.5
(absolute values) on the upper triangle and all values on the lower
triangle. Thus, the upper triangle displays only the most correlated motions.

As stated that the upper triangle only shows the cross-correlation greater than
0.5, but I am also getting some negative correlation values(blue regions) in 
above triangle.
I don't know what is the region behind this.
Plz help me to understand this behaviour.
I have attached my xpm matrix file generated using g_covar.
--
-
Thanks and regards
Bipin Singh


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[gmx-users] Re: RE: simulation of a metal binding sites (bharat gupta)

2011-02-18 Thread Ran Friedman
Hi,

If you know the structure of the zinc binding domain and assume that the zinc 
ion stays in place it may be all right to use the bonded representation. 

Recent publications:

@article{Lin2010,
author = {Lin, F and Wang, R},
title = {Systematic Derivation of {AMBER} Force Field Parameters Applicable to 
Zinc-Containing Systems},
journal = {J Chem Theory Comput},
volume = {6},
pages = {1852-1870},
year = {2010}
}


@Article{Peters2010,
author = Peters, M B and Yang, Y and Wang, B and F{\u}sti-Moln{\'a}r, L and 
Weaver, M N and Merz, K M,
title = {Structural Survey of Zinc Containing Proteins and the Development of 
the Zinc {AMBER} Force Field ({ZAFF})},
journal = J Chem Theory Comput,
year = 2010,
volume = 6,
pages = 2935-2947
}

You have to know quite a lot on the structure to use this approach.

Good luck,
Ran.


Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/ccbg


Message: 6
Date: Thu, 17 Feb 2011 23:46:02 -0800
From: bharat gupta bharat.85.m...@gmail.com
Subject: Re: [gmx-users] RE: simulation of a metal binding sites
To: Discussion list for GROMACS users gmx-users@gromacs.org,
baa...@smplinux.de
Message-ID:
AANLkTi=7rJZLS6B+hQvjNH5Su=qf3y9ay75ebm9fh...@mail.gmail.com
Content-Type: text/plain; charset=iso-8859-1

Thanks for these two references ... I am trying to simulate a zinc ion
(Zn++) binding domains .. Actually the study involves grafting the Zinc ion
domain onto some other protein to check whether it binds to ions or not and
what will be the effect of ion binding onto the topology of  the other
protein to which the zinc ion binding domain is attached .

On Thu, Feb 17, 2011 at 11:15 PM, Marc Baaden baa...@smplinux.de wrote:


 Hi,

 As mentioned by others, there's really lots of literature out there. I
 thought I mention a recent study we carried out, because it actually
 helped discover some new ion binding sites based on MD. By re-examining
 crystal structures based on these results, we could even find
 experimental evidence for those ions being there. [1]

 But actually you didn't tell us which ions you want to simulate?
 Monovalent ions should be sort of ok, although there are differences
 among the forcefields (some original KCl used to crystallize).
 Di-valent ions, in particular Ca2+, are much more tricky. Higher
 charged ones are a nightmare. The higher the charge, the more likely
 you might want things like polarization in your simulation.

 There are also some specific forcefields finely parameterized for ions
 based on quantum mechanics. I suggest you check out SIBFA [2] by Gresh
 and Piquemal.

 Good luck,
  Marc

 [1] How Cations Can Assist DNase I in DNA Binding and Hydrolysis

 http://www.ploscompbiol.org/article/info%3Adoi%2F10.1371%2Fjournal.pcbi.1001000

 [2] SIBFA (Sum of Interactions Between Fragments Ab initio computed)
 http://www.lct.jussieu.fr/pagesperso/jpp/SIBFA.html


 bharat.85.m...@gmail.com said:
  Thankx for the reply ...
  Can you refer some papers which can be helpful for me to do MD
  simulation of proteins with ions ... It will be of great help.. I
  searched the gromacs user list but couldn't get much material..



 --
  Dr. Marc Baaden  - Institut de Biologie Physico-Chimique, Paris
  mailto:baa...@smplinux.de  -  http://www.baaden.ibpc.fr
  FAX: +33 15841 5026  -  Tel: +33 15841 5176  ou  +33 609 843217


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[gmx-users] RE: simulation of a metal binding sites

2011-02-17 Thread Ran Friedman
Hi,

There are methodological difficulties in simulating multivalent ions together 
with proteins. Check the mailing list for a discussion and reference. This is 
not an
issue of Gromacs but of dealing with protein-ion interactions using a classical 
non-polarisable force field. Check the literature.

Ran.

Message: 3
Date: Wed, 16 Feb 2011 20:14:07 -0800
From: bharat gupta bharat.85.m...@gmail.com
Subject: [gmx-users] RE: simulation of a metal binding sites
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID:
aanlktin06ut6+wrfpz4a79fq9g-galmk35uxecph+...@mail.gmail.com
Content-Type: text/plain; charset=iso-8859-1

Hi,

I have incorporated some metal binding sites(zinc ion) in my protein. Now I
want to see whether that region binds to zinc ions or not and what is the
effect of ion binding to the topology of the protein .. Can this be done
using gromacs and how ??

Regards

--
Bharat
Ph.D. Candidate
Room No. : 7202A, 2nd Floor
Biomolecular Engineering Laboratory
Division of Chemical Engineering and Polymer Science
Pusan National University
Busan -609735
South Korea
Lab phone no. - +82-51-510-3680, +82-51-583-8343
Mobile no. - 010-5818-3680
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Re: [gmx-users] Simulation using Martini force field

2011-02-14 Thread Ran Friedman
Hi Regina,

Most CG force fields for proteins are less versatile than all-atom force fields 
and are simply not adequate for every application. As the secondary structure 
is determined a priori, you cannot model secondary structure changes, as 
probably happen during aggregation - even if the definition of the unordered 
protein was correct. You probably need to choose another FF or method. The 
UNRES FF from the Scheraga group doesn't suffer from this limitation, but isn't 
implemented in Gromacs and may have other caveats.

You can take a look at the MARTINI web page and paper (on the protein FF) about 
the definition of secondary structure.

Best regards,
Ran

Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/ccbg

--

Message: 1
Date: Tue, 15 Feb 2011 00:43:51 +0200
From: pol...@fh.huji.ac.il
Subject: Re: [gmx-users] Simulation using Martini force field
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 20110215004351.13575htmiyeiz...@webmail.huji.ac.il
Content-Type: text/plain;   charset=UTF-8;  DelSp=Yes;format=flowed

Thank you very much for you reply. Can you please explain me why do i
need secondary structure file at all and why secondary structure is
pre-defined and thus static throughout a simulation? I didn't see
that something like this defined for lipids. How do I use do_dssp to
build the needed file? I saw that I need a topology file in rder to
use do_dssp. Where can I find this topology file? I hope this is ok
that I'm asking so many questions. Thank you very much for your help.
Regina
Quoting XAvier Periole x.peri...@rug.nl:


 Dear Regina,

 You have two problems:
 1- the parameterization of phosphorylated serine should be done
 following the same philosophy of Martini. Check the Martini papers
 to see how this is done. In short partitioning is of primary importance.
 2- you want to simulate unfolded protein ... indeed there is evidently
 no persistent structure in such system and therefore the choice for
 secondary structure would be coil in the Martini force field.
 However the definition of coil for Martini has not been parameterize
 to reproduce anything even close to what an unfolded protein, assuming
 that we know what it looks like :)) The Martini coil is simply something
 flexible.

 I am afraid Martini is just not ready for simulating unfolded proteins.
 Any outcome of a simulation would have to be interpreted with CARE!

 XAvier.

 On Feb 14, 2011, at 2:09 PM, pol...@fh.huji.ac.il wrote:

 Dear Gromacs users and developers,
 I'm interested to run simulation of natively unstructured protein
 (casein), that can self assembly and create micelles, using Martini
 force field. The initial structure of the monomer was created and
 minimized using Sybyl. This protein includes also 4 phosporylated
 serines. I'm trying to understand how should I set my system. I
 started from the tutorial
 (http://md.chem.rug.nl/cgmartini/index.php/tutorial/ubiquitin-in-water) but
 I found that have no idea how to create a phosphorylated serine
 inCG structure (I have it in my initial pdb). In addition, I found
 that I need a secondary structure of the protein and I don't have
 something like this. Moreover, this protein doesn't have one. I
 will appreciated very much if somebody can help me and guide me a
 little.
 Thank you very much in advance.
 Regina

 
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RE: [gmx-users] .psf and .dcd files

2010-12-19 Thread Ran Friedman
Hi,

You can use wordom to convert .xtc files to .dcd.
As for the .psf AFAIK you'll have to work on it yourself using CHARMM or psfgen.

Ran


Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/research-groups/computational-chemistry-and-biochemistry-group?l=en


From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org] On Behalf 
Of atila petrosian [atila.petros...@gmail.com]
Sent: 19 December 2010 11:04
To: gmx-users@gromacs.org
Subject: [gmx-users] .psf and .dcd files

Dear gromacs users

I did simulation of protein-ligand by gromacs 4.0.7 with amber 03 forcefield.

I need to .psf and .dcd files. can I convert/obtain them?

any help will highly appreciated.
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RE: [gmx-users] .psf and .dcd files

2010-12-19 Thread Ran Friedman
Hi,

psfgen is a part of VMD but maybe you can also use it separately.

Note that you have to give it the right input and parameters, and I don't know 
if it works with AMBER-FF.

Good luck
Ran

From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org] On Behalf 
Of atila petrosian [atila.petros...@gmail.com]
Sent: 19 December 2010 12:36
To: gmx-users@gromacs.org
Subject: [gmx-users] .psf and .dcd files

Dear Ran

thanks for your reply.

Is psfgen a separately program?
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RE: [gmx-users] proton proton transfer

2010-12-02 Thread Ran Friedman
Hi Olga,

It's not straightforward in CHARMM as well. One method is to use conjugate peak 
refinement, but this will only get you the potential energy surface, but 
there's also a force field made by Meuwly for dealing with proton transfer 
IIRC. Depending on the system size, you may want to use QM/MM (implemented in 
Gromacs) or simulate your system with a DFT-based 'on semi-empricial code. 

Ran 


Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/research-groups/computational-chemistry-and-biochemistry-group?l=en


From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org] On Behalf 
Of Olga Ivchenko [olga.ivche...@gmail.com]
Sent: 02 December 2010 14:59
To: jalem...@vt.edu; Discussion list for GROMACS users
Subject: Re: [gmx-users] proton proton transfer

Thnaks, Justin.
Probably CHARMM is suitable for this.

2010/12/2 Justin A. Lemkul jalem...@vt.edumailto:jalem...@vt.edu


Olga Ivchenko wrote:
Dear gromacs users,

I want to simulate proton transfer between water and another small molecule in 
gromacs. In the end I should have the velosity of proton proton exchange. 
Please can you advice me which method is better to use for this in gromacs.
I read about umbrella sampling, but may be there is other techniques?


You can't do this with standard MD.  Bonds cannot break and re-form in a 
classical force field.  You might be able to do accomplish it with QM, however, 
but in that case you need to be looking outside of Gromacs.

-Justin

Yours sincerely,
Olga


--


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


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RE: [gmx-users] proton proton transfer

2010-12-02 Thread Ran Friedman
Sorry for the typo below. DFT based *or* semi empirical code.

From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org] On Behalf 
Of Ran Friedman
Sent: 02 December 2010 15:01
To: Discussion list for GROMACS users
Subject: RE: [gmx-users] proton proton transfer

Hi Olga,

It's not straightforward in CHARMM as well. One method is to use conjugate peak 
refinement, but this will only get you the potential energy surface, but 
there's also a force field made by Meuwly for dealing with proton transfer 
IIRC. Depending on the system size, you may want to use QM/MM (implemented in 
Gromacs) or simulate your system with a DFT-based 'on semi-empricial code.

Ran


Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

Norrgård, room 328d
+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/research-groups/computational-chemistry-and-biochemistry-group?l=en


From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org] On Behalf 
Of Olga Ivchenko [olga.ivche...@gmail.com]
Sent: 02 December 2010 14:59
To: jalem...@vt.edu; Discussion list for GROMACS users
Subject: Re: [gmx-users] proton proton transfer

Thnaks, Justin.
Probably CHARMM is suitable for this.

2010/12/2 Justin A. Lemkul jalem...@vt.edumailto:jalem...@vt.edu


Olga Ivchenko wrote:
Dear gromacs users,

I want to simulate proton transfer between water and another small molecule in 
gromacs. In the end I should have the velosity of proton proton exchange. 
Please can you advice me which method is better to use for this in gromacs.
I read about umbrella sampling, but may be there is other techniques?


You can't do this with standard MD.  Bonds cannot break and re-form in a 
classical force field.  You might be able to do accomplish it with QM, however, 
but in that case you need to be looking outside of Gromacs.

-Justin

Yours sincerely,
Olga


--


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


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RE: [gmx-users] Claculating Equilibrium constants

2010-11-30 Thread Ran Friedman
Hi Gideon,

If the binding is relatively weak and the force field parameters are good 
enough that should be feasible. See e.g., Biophys J. 2005 August; 89(2): 
768–781.
However, in other cases this is more challenging. This is discussed in details 
for simulations of a Zinc binding protein in Phys Chem Chem Phys. 2009 Feb 14; 
11(6): 975-83 

Good luck,
Ran


Ran Friedman
Biträdande Lektor (Assistant Professor)

Linnaeus University
School of Natural Sciences
391 82 Kalmar, Sweden

+46 480 446 290 Telephone
+46 76 207 8763 Mobile
ran.fried...@lnu.se
http://lnu.se/research-groups/computational-chemistry-and-biochemistry-group?l=en


From: gmx-users-boun...@gromacs.org [gmx-users-boun...@gromacs.org] On Behalf 
Of גדעון לפידות [glapid...@gmail.com]
Sent: 30 November 2010 10:45
To: gmx-users@gromacs.org
Subject: [gmx-users] Claculating Equilibrium constants

Hello all,
I have a protein bound to ions. is there a way to calculate the Kd of the bound 
ion in Gromaces so I can compare it to experimental Kd?
Thanks,
Gideon
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Re: [gmx-users] RE: Targeted MD

2010-08-20 Thread Ran Friedman
Hi,

-r and -rb are for FEP.

If you want to bias your simulation's sampling, you can use the pull
code, essential dynamics sampling or flooding, all of which are
described in the manual and literature.

Ran

Nimesh Jain wrote:
 Hello,

 I realize that this topic has been discussed before, but I just need
 to ascertain a few things: I have a system of about 1400 atoms with
 implicit solvent and I want to do a targeted MD. While doing the
 pre-processing, if I just specify grompp -r in.gro -rb out.gro, is
 this sufficient or are there any other things that I need to consider.
 Also, I have tabulated potentials.

 If any one knows how to do this, or if you need more info on my
 system, please let me know.

 Thanks,
 Nimesh

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Re: [gmx-users] Is there a way to calculate the hydrodynamic radius using GROMACS?

2010-08-19 Thread Ran Friedman
Hi Art,

For a globular protein, it should correlate with the gyration radius.
You can have a look at Dashevskaya et al., PROTOPLASMA 234: 13-23 for
some discussion about the relation of the radius of gyration and Stokes
radius.

Ran

Berk Hess wrote:
 Hi,

 There might be a way to do this with Gromacs.
 But I would think a protein is simply a volume (maybe with one
 attached water layer)
 for which there is a simple approximation for the hydrodynamic radius
 in hydrodynamics.

 Berk

  From: aroberts99...@yahoo.com
  To: gmx-users@gromacs.org
  Date: Wed, 18 Aug 2010 14:25:26 -0700
  Subject: [gmx-users] Is there a way to calculate the hydrodynamic
 radius using GROMACS?
 
  Hi, all,
 
  I was curious, if there is a way to calculate the hydrodynamic radius
  of a protein using GROMACS?
 
  Much appreciated,
  Art
 
  Dr. Arthur Roberts, Ph.D.
  University of California, San Diego
  Skaggs School of Pharmacy and Pharmaceutical Sciences
  9500 Gilman Drive #0703
  La Jolla, CA 92093-0703
 
  email: aroberts99...@yahoo.com
  cell: 206-850-7468
  skype=aroberts92122
 
 
 
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-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.uzh.ch
Skype: ran.friedman
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Re: [gmx-users] Entropy from NMA

2010-07-28 Thread Ran Friedman
Hi,

Can you post the exact commands you used for EM and NMA?

Ran

nahren manuel wrote:
 Dear Gromacs Users,

 I am trying to calculate Entropy from Normal Mode Analysis.
 I minimized the structure to
 8.41750710592449e-09

 Then I calculated the normal mode (the mdp file is given below).

 But when i try to calculate the Eigenvalues, I get the following warning


 One of the lowest 6 eigenvalues has a non-zero value.
 This could mean that the reference structure was not
 properly energy minimized.
 Writing eigenvalues...

 I get only negative eigenvalues.

 Let me also add that I used the same mdp file for minimization
 changing the integrator to steep, cg and finally to l-bfgs.

 Best,
 nahren

 ---
 integrator= nm 
 constraints = none
 define = -DFLEXIBLE
 emtol= 0.0001
 emstep  = 0.0001 
 nsteps= 5   
 nstlist= 1  
 ns_type= grid
 rlist= 1.5 
 coulombtype= shift 
 rcoulomb-switch= 1.0
 rvdw-switch= 1.0  
 vdwtype = shift
 rcoulomb = 1.3
 rvdw = 1.3




-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.uzh.ch
Skype: ran.friedman
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Re: [gmx-users] Entropy from NMA

2010-07-28 Thread Ran Friedman
p.s. How big is this negative value?

Ran Friedman wrote:
 Hi,

 Can you post the exact commands you used for EM and NMA?

 Ran

 nahren manuel wrote:
 Dear Gromacs Users,

 I am trying to calculate Entropy from Normal Mode Analysis.
 I minimized the structure to
 8.41750710592449e-09

 Then I calculated the normal mode (the mdp file is given below).

 But when i try to calculate the Eigenvalues, I get the following warning


 One of the lowest 6 eigenvalues has a non-zero value.
 This could mean that the reference structure was not
 properly energy minimized.
 Writing eigenvalues...

 I get only negative eigenvalues.

 Let me also add that I used the same mdp file for minimization
 changing the integrator to steep, cg and finally to l-bfgs.

 Best,
 nahren

 ---
 integrator= nm 
 constraints = none
 define = -DFLEXIBLE
 emtol= 0.0001
 emstep  = 0.0001 
 nsteps= 5   
 nstlist= 1  
 ns_type= grid
 rlist= 1.5 
 coulombtype= shift 
 rcoulomb-switch= 1.0
 rvdw-switch= 1.0  
 vdwtype = shift
 rcoulomb = 1.3
 rvdw = 1.3




 -- 
 --
 Ran Friedman
 Postdoctoral Fellow
 Computational Structural Biology Group (A. Caflisch)
 Department of Biochemistry
 University of Zurich
 Winterthurerstrasse 190
 CH-8057 Zurich, Switzerland
 Tel. +41-44-639
 Email: r.fried...@bioc.uzh.ch
 Skype: ran.friedman
 --
   


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Re: [gmx-users] Entropy from NMA

2010-07-28 Thread Ran Friedman
Dear Rui,

Thanks for the info - maybe it's better to submit a bugzilla for the NMA
in parallel then, do I'm not sure if this can be checked on run-time
with mdrun. From Nahren's description I understood that multiples files
were generated and assumed that they were backups (as if you run
identical MD multiple times with the same input and files).

Ran

J. Rui Rodrigues wrote:
 Dear Ran and Nahren,

 I run into a similar problem a couple of weeks ago:
 http://lists.gromacs.org/pipermail/gmx-users/2010-July/052377.html

 In short,
 integrator =  steep  can be run in parallel. Output from parallel and 
 single-node are equal.

 integrator =  l-bfgs runs only in single-node, as advertised in the 
 manual. mdrun dies with a fatal error if one tries to run in parallel:
 Fatal error: Cannot do parallel L-BFGS Minimization - yet.

 integrator = nm runs in parallel without any error. However, output 
 is wrong: mdrun write multiple hessian.mtx files, each with small size.
 mdrun seems to get in to some kind of race condition, because sometimes
 only one  .mtx is produced (still, with small size). Running g_nmeig in these
 parallel  mtx results in huge all-negative eigenvalues.
 The same input in single-node goes just fine, with first 6 eigenvalues close
 to zero.

  
 Rui Rodrigues




 On Wed, 28 Jul 2010 12:55:44 +0200, Ran Friedman wrote
   
 Your NMA seem to run on one processor four times. I'm not sure if the EM
 part can be run in parallel. This doesn't seem to be the reason for the
 negative eigenvalue. What was the g_anaeig command (with flags)?

 nahren manuel wrote:
 
 Dear Ran,

 I ran the whole NMA again and I found where I go wrong. I hope it will
 help others as well.
 (sorry for a big email)


 In steps 1  2 (of minimization) I kept the C-alpha frozen.

 1. doublegrompp -f em1.mdp -c r1dodecapdb.pdb -p r1top.top -o em1tpr.tpr
 mpirun -np 8 ~/gmxdpr/bin/doublemdrun -v -deffnm em1tpr

 Steepest Descents converged to Fmax  100 in 2569 steps
 Potential Energy  = -6.21296128286120e+03
 Maximum force =  9.87358378592302e+01 on atom 701
 Norm of force =  1.04875323563923e+01

 2. doublegrompp -f em2.mdp -c em1tpr.gro -p r1top.top -o em2tpr.tpr -t
 em1tpr.trr
 mpirun -np 8 ~/gmxdpr/bin/doublemdrun -v -deffnm em2tpr

 Polak-Ribiere Conjugate Gradients converged to Fmax  1 in 6596 steps
 Potential Energy  = -7.56682084795001e+03
 Maximum force =  9.92719787231560e-01 on atom 1320
 Norm of force =  6.47772253797808e-02

 3. doublegrompp -f em3.mdp -c em2tpr.gro -p r1top.top -o em3tpr.tpr -t
 em2tpr.trr
 mpirun -np 8 ~/gmxdpr/bin/doublemdrun -v -deffnm em3tpr

 Stepsize too small, or no change in energy.
 Converged to machine precision,
 but not to the requested precision Fmax  10

 writing lowest energy coordinates.

 Steepest Descents converged to machine precision in 3018 steps,
 but did not reach the requested Fmax  10.
 Potential Energy  = -8.49398064549505e+03
 Maximum force =  6.86336687926682e+01 on atom 935
 Norm of force =  7.15798864024085e+00


 4. doublegrompp -f em4.mdp -c em3tpr.gro -p r1top.top -o em4tpr.tpr -t
 em3tpr.trr
 mpirun -np 8 ~/gmxdpr/bin/doublemdrun -v -deffnm em4tpr

 Stepsize too small, or no change in energy.
 Converged to machine precision,
 but not to the requested precision Fmax  0.01

 writing lowest energy coordinates.


 Polak-Ribiere Conjugate Gradients converged to machine precision in
 21674 steps,
 but did not reach the requested Fmax  0.01.
 Potential Energy  = -9.66058047638671e+03
 Maximum force =  1.49342602818840e+00 on atom 590
 Norm of force =  1.86576579430541e-01


 5.doublegrompp -f em5.mdp -c em4tpr.gro -p r1top.top -o em5tpr.tpr -t
 em4tpr.trr
  ~/gmxdpr/bin/doublemdrun -v -deffnm em5tpr

 Low-Memory BFGS Minimizer converged to machine precision in 10346 steps,
 but did not reach the requested Fmax  0.0001.
 Potential Energy  = -9.66337416273684e+03
 Maximum force =  6.48625019025464e-04 on atom 581
 Norm of force =  6.35632681200205e-05

 6.doublegrompp -f em6.mdp -c em5tpr.gro -p r1top.top -o em6tpr.tpr -t
 em5tpr.trr

 Low-Memory BFGS Minimizer converged to machine precision in 3316 steps,
 but did not reach the requested Fmax  1e-08.
 Potential Energy  = -9.66337416275038e+03
 Maximum force =  6.48788529801368e-05 on atom 8
 Norm of force =  6.56362137550289e-06

 7. doublegrompp -f em7.mdp -c em6tpr.gro -p r1top.top -o em7tpr.tpr -t
 em6tpr.trr

 Low-Memory BFGS Minimizer converged to machine precision in 7530 steps,
 but did not reach the requested Fmax  1e-08.
 Potential Energy  = -9.66337416275071e+03
 Maximum force =  4.07762128402886e-07 on atom 10
 Norm of force =  5.79534451487287e-08

 8. doublegrompp -f em8.mdp -c em7tpr.gro -p r1top.top -o em8tpr.tpr -t
 em7tpr.trr
 Low-Memory BFGS Minimizer converged to Fmax  1e-08 in 5840 steps
 Potential Energy  = -9.66337416275070e+03
 Maximum force =  8.41750710592449e-09 on atom 521
 Norm of force =  1.2888919393e-09


 NMA

 9

Re: [gmx-users] NPH Simulations

2010-07-15 Thread Ran Friedman
Hi,

You can run a simulation with a barostat but with no temperature
coupling. It's probably a good idea to make sure that the system is
equilibrated in terms of the temperature first (with NPT). Also, I'd use
a small timestep and double precision. Search the literature for
protocols from researchers who have already employed NPH, though that's
not too common.

Ran

sapna sarupria wrote:
 Hi All,

 I was wondering if there is a way to run simulations in the NPH
 ensemble in Gromacs. Does any one have experience doing this?

 Thank you
 Sapna
-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.uzh.ch
Skype: ran.friedman
--

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Re: [gmx-users] g_cluster Jarvis-Patrick

2010-07-14 Thread Ran Friedman
Hi,

The nearest neighbours are defined according to RMSD between the
structures. If M=10, a new conformation x is added to a given cluster
when a conformation y in the cluster exists such that:
(1) x and y are neighbours, i.e., x has y among the 10 conformations
with minimal RMSD to x and vice versa for y.
(2) x any y have at least P (default: 3) neighbours in common.

You may want to prepare a diagram to graphically illustrate this.

Ran

Marc Charendoff wrote:
 Hello,
  
  In the Jarvis-Patrick method g_cluster shows that when M=0, the
 cutoff is used to determine nearest neighbors (those within X.X nm).
 In the absence of cutoff - e.g. M is defaulted to 10, how are nearest
 neighbors determined? What does M=10 (or anyother number) mean?
  
 Thanks, Marc

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Re: [gmx-users] Re: g_cluster settings

2010-07-12 Thread Ran Friedman
Marc - Note that you used the linkage method which maps a structure to a
cluster if its distance to any structure already in the cluster is is
less than the cutoff. If you think it's not representative of your
system try another clustering method, but note that you may need a
longer trajectory as well.

Vitali - g_clustersize is for clustering molecules (can be useful e.g.,
for the formation of micelles) whereas g_cluster is for clustering the
trajectories.

Ran

Vitaly Chaban wrote:
 Dear Marc:

 Please look towards g_clustzise (instead of g_cluster). We tried to
 use g_cluster some years ago and eventually switched to g_clustzise -
 I do not remember why but the latter was more successful. If you want
 to monitor the number of clusters in the system, g_clustzise can
 certainly do it.

 Dr. Vitaly Chaban



   
 I am trying to perform a cluster analysis on a 4 ns trajectory (4000 
 frame
 trajectory), but I am not getting any more than 1 cluster until I get down 
 to a
 cutoff of 0.05 nm. This seems like an awfully small number, so I checked my 
 rmsd
 distribution and found that 44% of my rmsds are at 0.1 nm or greater. My
 distribution looks like the following:

 And my command line is as follows:

 g_cluster -f md.trr -s md.tpr -n index.ndx -sz clustersize1.xvg -clid
 clusterid1.xvg -cutoff .10   -cl clusters1.pdb -b 1 -e 4001

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Re: [gmx-users] Electric field, potential, dielectric constant

2010-06-17 Thread Ran Friedman
Hi,
You may want to use a Poisson-Boltzmann solver, e.g., APBS for this purpose.
Ran

Vladimir Lankevich wrote:
 Dear Gromacs Users,

 I have several questions about electrostatics in Gromacs.
 I am simulating two proteins in water, separated by certain distance,
 and was interested in their electrostatic interactions.

 I was wondering if Gromacs can calculate and show me values of
 electric field or electric potential at any point within the volume.
 If yes, how can this be done?

 I looked through the manual and did not find much. I tried using
 g_potential, but it only gives me ten values for electric field (if I
 use 10 slices, and particular direction).
 This confused me, because I thought that in the system each coordinate
 would have different electric field.
 How should I interpret the results of g_potential?

 Also, can I use Gromacs to compute dielectric constant of a particular
 region within the volume? How can I do that?

 Thank you very much!!

 Cheers,
 Vladimir

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Re: [gmx-users] large forces and monstrous water molecules in energy minimization step

2010-06-17 Thread Ran Friedman
Hi,

For the dynamics to work you indeed need smaller forces (on the order of
10^3 in GMX units).
Using flexible water molecules I was able to get this for your NaCl model. 
Just add:
define  =  -DFLEXIBLE
To your input.

This should work also to fill in the voids I guess.

Ran

-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.uzh.ch
Skype: ran.friedman
--

Justin A. Lemkul wrote:

 Use a different box size.  I replicated your problem, but your run
 completes successfully with a box set up with editconf -d 1 instead of
 -d 3.3.

 If you set nstxout = 1 during the EM process, you'll see the
 problematic water molecule become unstable.  It looks as if there is a
 small void in the solvent (due to the way genbox tries to stack
 solvent configurations) and your water molecule simply can't find a
 good orientation within that void.

 -Justin

 Ehud Schreiber wrote:
 Dear GROMACS users,

  

 When trying to simulate a pair of interacting proteins in water, I
 have encountered problems that ultimately resulted in the simulation
 crashing. I then tried to simplify the system as far as possible
 while retaining the problem; I now believe the problem (or at least a
 part of it) lies in the energy minimization step (the first molecular
 dynamics one). Specifically, the forces encountered during this step
 are very large, and some water molecules (which are supposed to be
 rigid) become giant and misshapen.

  

 In more details:

 1) I use GROMACS version 4.0.7, single precision, on a server with
 two Intel x86-64 processors and the redhat 5.4 linux OS.

 2) I created a PDB file, called NaCl.pdb, with only two “atoms”,
 actually Na+ and Cl- ions separated by their distance in the lattice
 of salt:

  

 HET NA  A   1   1

 HET CL  A   1   1

 HETNAM  NA SODIUM ION

 HETNAM  CL CHLORIDE ION

 FORMUL   1   NANA 1+

 FORMUL   2   CLCL 1-

 HETATM1 NANA A   1  -1.410.0   0.01.00 
 0.0  NA

 HETATM2 CLCL A   1  +1.410.0   0.01.00 
 0.0  CL

  

 3) I use the tip3p water model:

  

 pdb2gmx -f NaCl.pdb -water tip3p

  

 4) I create the box:

  

 editconf -f conf.gro -bt dodecahedron -d 3.3 -o box.gro

  

 5) I add water using spc216, creating the saltwater.gro file (which
 seems O.K. by inspection):

  

 genbox -cp box.gro -cs spc216.gro -p topol.top -o saltwater.gro

  

 6) I create the energy minimization parameter file em.mdp:

  

 --em.mdp--

 integrator  = steep

 nsteps  = 200

 nstlist = 10

 rlist   = 1.0

 coulombtype = pme

 rcoulomb= 1.0

 vdwtype = Cut-off

 rvdw= 1.0

 nstenergy   = 10

 --

  

 7) I prepare the em.tpr file for the energy minimization run:

  

 grompp -f em.mdp -p topol.top -c saltwater.gro -o em.tpr

  

 8) I run the energy minimization step:

  

 mdrun -v -deffnm em

  

 9) Looking at the em.log file I see that this step converged to
 machine precision but did not have maximal force  10:

  

 …

 Enabling SPC water optimization for 7561 molecules.

 …

 Max number of connections per atom is 2

 Total number of connections is 30244

 Max number of graph edges per atom is 2

 Total number of graph edges is 30244

 Going to use C-settle (7561 waters)

 wo = 0.33, wh =0.33, wohh = 3, rc = 0.075695, ra = 0.0390588

 rb = 0.0195294, rc2 = 0.15139, rone = 1, dHH = 0.15139, dOH = 0.09572

 …

 Stepsize too small, or no change in energy.

 Converged to machine precision,

 but not to the requested precision Fmax  10

 …

 Steepest Descents converged to machine precision in 36 steps,

 but did not reach the requested Fmax  10.

 Potential Energy  = -3.4678925e+05

 Maximum force =  6.4623531e+05 on atom 11052

 Norm of force =  5.4643726e+03

  

 10) Looking at the em.gro file I see one monstrous water molecule
 (no. 3686); e.g., it has |HW2-OW| = 3.384876 nm, while the normal
 distance is about 0.1 nm. Its HW2 atom (no. 11054) is close to
 another water molecule (no. 5849), e.g., 0.047 nm from the latter’s
 HW2 atom (no. 17543):

  

 …

 3686SOL OW11052   4.348   3.778  -0.629

 3686SOLHW111053   5.360   2.601   0.505

 3686SOLHW211054   6.518   1.650   0.861 
 …

 5849SOL OW17541   6.525   1.698   0.900

 5849SOLHW117542   6.606   1.649   0.918

 5849SOLHW217543   6.481   1.648   0.832

 …

  

 11) During the simulation, several files called stepnnl.pdb were
 produced for problematic steps, where nn=11,15,19 and l=b,c. For
 example, the file step19c.pdb indeed shows a problematic water
 molecule no. 3686, while step19b.pdb does not. Likewise, the earlier
 step11c.pdb shows

Re: [gmx-users] Re: Simulation with CsCl

2010-06-09 Thread Ran Friedman
Dear Sonali,

Unfortunately development of force-field parameters is difficult, and
even more so for bivalent ions and transition metals. This is certainly
not suitable as a project to begin with.

Having said that, a careful search in the literature will reveal that
many sets of parameters for metal ions do exist. Try to find a set that
works best with the water model that you're using or your particular
model, and carry out some simulations to validate that the results are
correct, reproducible and robust. The following references discuss some
aspects of simulations of ions and proteins:

@article{Project2006,
   Author = {Project, E. and Friedman, R. and Nachliel, E. and Gutman, M.},
   Title = {A Molecular Dynamics Study of the Effect of Ca{2+} Removal
on Calmodulin Structure},
   Journal = {Biophys. J.},
   Volume= {90},
   Pages = {3842-3850},
   Year = {2006}
}


@Article{Fyta2010,
author = Fyta, M and Kalcher, I and Dzubiella, J and Vrbka, L and Netz,
R R,
title = {Ionic force field optimization based on single-ion and ion-pair
solvation properties},
journal = J Chem Phys,
year = 2010,
volume = 132,
pages = 024911-024911
}

Ran.

sonali dhindwal wrote:
 Hello All ,
 I am also trying to simulate my protein with Mn ion present in it.
 So can I create the topology entry for Mn ion similar  to MG2+ ion ?
 and how can I get the values of C6 and C12 leonard jones potential in
 [atom type] entry and will it be required to add [nonbond_params] also
 ? how can I get them ?

 Also I want to use Fe2+ also, but it  is also not included in gromos
 force field. This problem of adding other ions and molecule in the
 system always remains. And being new to this field, can someone
 suggest in simple terms how to include these considering the person is
 not an expert in this field.
 Please help.

 --
 Sonali Dhindwal


 --- On *Tue, 8/6/10, Vitaly Chaban /vvcha...@gmail.com/* wrote:


 From: Vitaly Chaban vvcha...@gmail.com
 Subject: [gmx-users] Re: Simulation with CsCl
 To: gmx-users@gromacs.org
 Date: Tuesday, 8 June, 2010, 9:03 PM

  Hi all:
  I am trying to simulate a polysaccharide in solution of water
 and CsCl, but
  cesium is not parametrized in the gromacs 4. I am using the force
  field GROMOS 96.
  I have looked for the parameters of Cs+ in the OPLS Force field
 and I have
  created 4 files: Cs.atp, Cs.itp, Csnb.itp and Cs.rtp. Also I
 have include
  the parameters for Cs+ in the ions.itp file, but it didn't
 work, Can
  someone help me?
  Thanks in advance.
  Cecilia.

 Cecilia -

 You do not need so many files so cesium. Just copy your parameters to
 the force field used and create the topology entry for cesium similar
 to

 [ moleculetype ]
 Ar 1

 [ atoms ]
 1   Ar1Ar  Ar0  0.0

 Do not forget, cesium+ is an ion...

 -- 
 Dr. Vitaly Chaban
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-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.uzh.ch
Skype: ran.friedman
--

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Re: [gmx-users] How to increase the tolerance for conjugate gradient minimization

2010-06-08 Thread Ran Friedman
Hi Arthur,

The most useful option from my experience is to run Gromacs in double
precision.
You also can try to make emstep smaller (after an initial minimisation
of the crude structure) and use l-bfgs.

Good luck,
Ran

-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.uzh.ch
Skype: ran.friedman
--

Arthur Roberts wrote:
 I agree the code is fine.  Is there a parameter that I need to change
 to increase the tolerance?  I have issues energy minimizing a small
 molecule in the presence of a macromolecule.  One work around is to
 increase the energy of the small molecule, so that the macromolecule
 no longer dominates the energetics.  I would appreciate your input.

 Art

 On Jun 4, 2010, at 5:45 PM, Mark Abraham wrote:



 - Original Message -
 From: Arthur Roberts aroberts99...@yahoo.com
 Date: Saturday, June 5, 2010 4:57
 Subject: [gmx-users] How to increase the tolerance for conjugate
 gradient minimization
 To: gmx users gmx-users@gromacs.org

  Hi, all,
 
  Is there a way to increase the tolerance for Conjugate Gradient
  energy minimization?
 
  It seems that I can only get a Tolerance (Fmax) = 1e-4
 
  emtol doesn't seem to do the trick.  I tried several values.

 The code's fine in 4.0.7. Does your .mdp value match that reported in
 the .log file? Ditto in gmxcheck on the .tpr?

 Mark --
 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!
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 Art Roberts
 7254 Shoreline Dr. #130
 San Diego, CA 92122
 cell: 206-850-7468
 email: aroberts99...@yahoo.com
 skype=aroberts92122

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Re: [gmx-users] g_cluster, RMSD distribution

2010-05-19 Thread Ran Friedman
Hi,

The distribution is calculated as follows:
101 bins are formed between zero and maximum rmsd in equal separation
(by calculating the largest value by 100 to create the separation). Each
rmsd value is put into the right bin and the counter for that bin is
increased by 1. The total number of counts is the size of half a matrix.

Example:
If the maximal rmsd is 10.0 and a certain comparison yield rmsd=0.13 the
value of the second bin in increased by 1.

Ran.

Michał Koliński wrote:
 Dear All

 I’m trying to obtain RMSD distribution of  a ligand in the binding site of 
 the receptor protein during 40 ns MD simulation.
 Could you please explain:

 - what is exactly the yaxis unit  of the plot obtained using g_cluster with 
 –dist option
 -  how is this distribution calculated?

 Thank you in advance,

 All best,
 Michal
   

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Re: [gmx-users] about SHAKE, SETTLE, LINCS and double x single precision

2010-05-14 Thread Ran Friedman
Hi Alan,
I don't think using single precision is much of a problem when using
thermostats, regardless of the constraint on the water.

See also Berks' comments:
http://oldwww.gromacs.org/pipermail/gmx-users/2010-March/049137.html
http://oldwww.gromacs.org/pipermail/gmx-users/2010-March/049152.html

Ran.

Alan wrote:
 Hi there,

 From what I've read and known, here in the list as well, one of the
 main reasons why Gromacs run in single precision is because it has
 LINCS, besides SHAKE, which I believe requires double precision for
 accuracy.

 I am drawing such conclusion (that can be wrong) partially based on 

 Lippert, R. A., Bowers, K. J., Dror, R. O., Eastwood, M. P.,
 Gregersen, B. A., Klepeis, J. L., Kolossvary, I., and Shaw, D. E. A
 common, avoidable source of error in molecular dynamics integrators.
 Journal of Chemical Physics 126, 4 (Jan. 2007), 046101–1–046101–2

 However, in this letter article they didn't test with LINCS. I would
 love to hear some comments from Gromacs developers.

 When I started in MD, developing our own MD software, all was done in
 double precision, then came Gromacs blowing up this paradigm. (I am
 aware that even in Gromacs, there are routines that really requires
 double precision, e.g. normal mode analysis).

 Essentially I would like to understand better this double x single
 approach in MD re accuracy.

 Thanks,

 Alan

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Re: [gmx-users] protein Aggregation using Gromacs

2010-05-12 Thread Ran Friedman
Hi,

There's no recipie to locate aggregation hot spots based on MD
simulations. There are many papers on simulations of protein and peptide
aggregation from which you can draw some ideas, but bear in mind that
aggregation of more than very few and very small peptides is typically
much slower than what one can simulate using atomistic MD.

For a quick approach you can use sequence analysis tools, e.g., TANGO
http://tango.crg.es/

Good luck,
Ran

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Department of Biochemistry
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Winterthurerstrasse 190
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Tel. +41-44-639
Email: r.fried...@bioc.uzh.ch
Skype: ran.friedman
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shahid nayeem wrote:
 Dear all
 What are the analysis tools which should be used on MD trajectory file
 in order to find potential aggregation sites of a protein. Anyone can
 tell me about specific resource material on use of Gromacs to predict
 protein aggregation hot spots from MD trajectory anlysis.
 Shahid Nayeem

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Re: [gmx-users] protein Aggregation using Gromacs

2010-05-12 Thread Ran Friedman
Hello again -

IMHO the best approach for any simulation study is to plan how the
simulation will be used to solve a specific scientific problem before
running the simulations, rather then the other way around. To clarify
what I wrote below, there's no algorithm I'm aware of where the input is
an MD simulation of a certain protein and the output is an aggregation
propensity of certain residues.

Having said that, simulations can be a useful tool to study amyloid
aggregation and even tendency of specific residues to aggregate first. A
useful approach was developed in the group where I work now, based on
the aggregation propensity of peptide sequences decomposed from the
whole protein:
http://dx.doi.org/10.1016/j.jmb.2006.01.009

Using your simulations, you can check if some residues are more prone to
lose their secondary structure as the temperature increases, which 
suggests that they are more likely to unfold. Do bear in mind though
that aggregation is a complex process which involves multimers. Unless
you show some correlation with experimental findings it will be
difficult to defend your conclusions.

Ran

shahid nayeem wrote:
 Hi
  I have used TANGO Aggrescan, Zyggregator and other online tools but I
 am unable to find and pinpoint residue responsible for aggregation.
 Then I did MD simulation of the proteins with gromacs at different
 temperature. Now in this background I need  suggestion to analyse my
 MD trajectory.
 shahid Nayeem

  
 On 5/12/10, *Ran Friedman* r.fried...@bioc.uzh.ch
 mailto:r.fried...@bioc.uzh.ch wrote:

 Hi,

 There's no recipie to locate aggregation hot spots based on MD
 simulations. There are many papers on simulations of protein and
 peptide
 aggregation from which you can draw some ideas, but bear in mind that
 aggregation of more than very few and very small peptides is typically
 much slower than what one can simulate using atomistic MD.

 For a quick approach you can use sequence analysis tools, e.g., TANGO
 http://tango.crg.es/

 Good luck,
 Ran

 --
 --
 Ran Friedman
 Postdoctoral Fellow
 Computational Structural Biology Group (A. Caflisch)
 Department of Biochemistry
 University of Zurich
 Winterthurerstrasse 190
 CH-8057 Zurich, Switzerland
 Tel. +41-44-639
 Email: r.fried...@bioc.uzh.ch mailto:r.fried...@bioc.uzh.ch
 Skype: ran.friedman
 --

 shahid nayeem wrote:
  Dear all
  What are the analysis tools which should be used on MD
 trajectory file
  in order to find potential aggregation sites of a protein.
 Anyone can
  tell me about specific resource material on use of Gromacs to
 predict
  protein aggregation hot spots from MD trajectory anlysis.
  Shahid Nayeem


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Re: [gmx-users] Normal Mode Analysis

2010-04-27 Thread Ran Friedman
Hi,

NMA is not MD - for one thing you don't run an NMA simulation for a
certain time. I suggest you read about NMA and make sure you understand
what the method does and what it can achieve before continuing. There is
some data on the manual, a lot of data on the web and even more in
books. When you have a good idea on what is NMA and why you're
interested in running it, you can try to run things and come back to the
list with more specific questions if such arise. In parallel, it may be
a good idea to read some papers where NMA was applied. I have in mind
papers of Lindahl and Levitt from the recent years, but you should be
able to come with an elaborate list.

Good luck,
Ran

Anirban Ghosh wrote:

 Hi ALL,

 This may sound like a very basic question, but I am still pondering
 over it. I have simulated a membrane protein system for 30 ns after
 Steepest Descent minimization and now I want to perform NMA. From the
 help pages what I understand is that I need a very well minimized
 system (using l-bfgs) and then generate a Hessian matrix. My question
 is that after my 30 ns run, should I again go for another run of
 minimization with l-bfgs and the should I run MD using nm as the
 integrator? For how long should I run this MD with nm integrator? Is
 a 1 ns run enough? Or am I required to run it for 30 ns (for which I
 have run the normal MD)?
 Any suggestion is welcome. Thanks a lot in advance.

 Regards,

 Anirban

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Re: [gmx-users] Dynamics cross correlation map

2010-03-24 Thread Ran Friedman, Biochemisches Inst.

Hi Sukesh,

I once put a version of g_covar that can calculate the correlations in the 
user contributions. Check if it's there or reply to me privately if you 
can't find it (though I'm on the road till Friday).


Good luck,
Ran

On Wed, 24 Mar 2010 11:46:42 +0530
 sukesh chandra gain suk...@atc.tcs.com wrote:

Hi Tsjerk,

Thank you for your reply. May be I was not very clear with my previous 
post.
I am not looking for covariance / atomic covariances map (ie., 
covar.xpm/covara.xpm) which are generated by g_covar tool in GROMACS. I am 
particularly trying to get correlation map (example: 
http://www.pnas.org/content/102/4/994/F2.large.jpg, 
http://www.pnas.org/content/99/26/16597/F3.small.gif). I hope there is a 
difference between covariance matrix and correlation matrix.
The correlated motions between two atoms is calculated as the magnitude of 
the co-relation coefficient between the atoms.  In case of a system it can 
be assessed by examining the magnitude of all pairwise cross-correlation 
coefficients. The cross-correlation coefficient, C(i,j) for each pair of 
atoms i and j is calculated as:
C(i,j) =  delta r(i) * delta r(j)  / sqrt  sqr(delta r(i) )  . sqrt  
sqr(delta r(j) )  , where delta r(i) is the displacement from mean 
position of the ith atom and   symbol represents the time average.
This function returns a matrix of all atom-wise cross-correlations whose 
elements, C(i,j), may be displayed in a graphical representation frequently 
termed a dynamical cross-correlation map, or DCCM. If C(i,j) = 1 the 
fluctuations of atoms i and j are completely correlated, if C(i,j) = -1 the 
fluctuations of atoms i and j are completely anticorrelated and if C(i,j) = 
0 the fluctuations of i and j are not correlated.
Now my query is there any tool like g_correlation 
(http://www.mpibpc.mpg.de/home/grubmueller/projects/MethodAdvancements/GeneralizedCorrelations/index.html) 
by which I can get the cross-correlation matrix from covariance matrix or 
directly from trajectory file.


Ref:1. Hünenberger PH, Mark AE, van Gunsteren WF; Fluctuation and 
cross-correlation analysis of protein motions observed in nanosecond 
molecular dynamics simulations; JMB 1995; 252:492-503
2. Oliver F. Lange, H. Grubmüller; Generalized Correlation for 
Biomolecular Dynamics; Proteins  2006; 62:1053-1061



Thank You,
Regards,
Sukesh

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TCS Innovation Labs
Tata Consultancy Services Ltd.
'Deccan Park', Madhapur
Hyderabad 500081
Phone:  +91 40 6667 3572

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Tel. +41-44-639
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Re: [gmx-users] Turn-off water optimisation

2010-03-05 Thread Ran Friedman
Hi,

Can you also post your .mdp?

Ran

Berk Hess wrote:
 Hi,

 I have never heard about problems like this before.
 It seems highly unlikely to me that the innerloops are causing this.

 Are your running exacly the same tpr file on your local machine
 and the cluster?

 You probably want to update to version 4.0.7 to be sure you have
 all the latest bugfixes.

 Please keep us updated on this issue, since things like this should
 never happen (unless there is a compiler bug).

 Berk

  Date: Fri, 5 Mar 2010 14:41:02 +0100
  From: schl...@uni-mainz.de
  To: gmx-users@gromacs.org
  Subject: Re: [gmx-users] Turn-off water optimisation
 
  Hi,
  i have the following problem: (GROMACS 4.0.5)
 
  when i simulated water in serial on our cluster with the brendsen or
  v-rescale thermostat i get to high temperatures (300 K goes in very
  short time up to around 425 K). If i simulate in parallel or at my
 local
  machine i get no problems. Also if i change water to another molecule
  there are no such problems. (I use the same mdp file for all the
  simulations).
 
  Because the problem appears with water (spc and tip4p) but not with
  mesitylene i thought probably the special things for water (settle, and
  so on) could be the problem. So i wanted to simulate water without that
  fancy stuff.
  Thanks for the info with the enviroment variable, but where can i
 set it?
 
  For the other problems (why it works on the cluster in parallel, but
 not
  in serial, but works on the local-pc in serial) i have so far no idea,
  where to look. But first i'm happy to know if the problem comes from
 the
  special water-loops.
 
  Thomas
 
 
 
  Hi,
  
  You don't want to mess with the topology, you will be simulating a
  quit different
  system when you turn off constraints. Also Gromacs does not optimize
  based
  on names, since the name might not say anything about the molecule.
  I don't know what effect of what optimizations you want to test,
  but setting the environment variable GMX_NO_SOLV_OPT will turn off
  the special inner-loops for water.
  
  Berk
 
   Date: Fri, 5 Mar 2010 11:31:50 +0100
   From: schlesi at uni-mainz.de
   To: gmx-users at gromacs.org
   Subject: [gmx-users] Turn-off water optimisation
  
   Dear all,
   I simulated water (spc) with the ffG53a5 force field. For testing
   propose i want to turn of the water optimisation. How do i do this?
   So far i have tried:
   * contraints = none
   * define = -DFLEXIBLE
   * took the spc.itp file and deleted all the stuff for settle and the
   other force fields, changed resname from SOL to WAT (also spc.itp -
   wat.itp)
  
   But all the time i the log file there is this line:
   Enabling SPC water optimization for 1184 molecules.
  
   Espically with the last option (change of the spc.itp) i don't how
   GROMACS recorgnises that i simulate SPC water, because i has a
 different
   name and so.
  
   Thanks for your help in advance.
   Greetings
   Thomas
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Re: [gmx-users] NVE of water

2010-03-01 Thread Ran Friedman
Hi Andrea,
Did you use double precision? Also, I'd try a lower dt (say 1fs) and
shake tolerance (maybe 1E-8).
Good luck,
Ran

Andrea wrote:
 Dear users,
  
 for test purposes in order to set up a bigger system, I try to run NVE
 simulations of SPC water, but the energy increases very rapidely. My
 guess is that the cutoffs I use are not good for water. I that the
 case ( I would be grateful for a good reference for suitable SPC water
 parameters) or do I miss something else?
 My parameter file for the NVE is:
  
 title= NVE
 cpp  = /lib/cpp
 integrator   = md
 dt   = 0.002   ; ps ! = 2 fs
 nsteps   = 5   ; total 100 ps
 nstxout  = 5000
 nstvout  = 5000
 nstxtcout= 0
 nstlog   = 5000
 nstenergy= 5000
 nstlist  = 10
 ns_type  = grid
 rlist= 1.1

 unconstrained-start  = yes
 constraints  = all-bonds
 constraint_algorithm = shake
 shake_tol= 0.0001
 ;VdW
 vdwtype  = Switch
 rvdw = 1.0  ; rvdw+ (0.1:0.3)=  rlist
 rvdw_switch  = 0.9
 gen_vel  = no   ; yes
 gen_temp = 300
 gen_seed = -1
 ;Temperature coupling
 tc_grps  = system
 tcoupl   = no   ;nose-hoover
 tau_t= 0.1
 ref_t= 300
 ;Pressure coupling
 pcoupl   = no
 optimize_fft = yes
  
 Any suggesions are really welcome.
  
 Thank you.
  
 Regards,
 Andrea Muntean


-- 
--
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Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.uzh.ch
Skype: ran.friedman
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Re: [gmx-users] NVE of water

2010-03-01 Thread Ran Friedman
Hi,

I would still argue that double precision is important.
My comment on SHAKE was based on CHARMM - in Gromacs it indeed doesn't
matter for water.

Ran

Justin A. Lemkul wrote:


 Berk Hess wrote:
 Hi,

 Shake is not relevant for water and also a time step of 2 fs should
 be fine.
 The cut-off's are the problem. You have a buffer size of 0.1 nm,
 which is already smaller than 2 times the distance from the center of
 geometry
 of a water molecule to a hydrogen. You need some additional distance
 for water diffusion. I would use a buffer of 0.25 to 0.3 nm.
 You don't list you coulombtype setting. Use pme (or if you want
 perfect energy
 conservation: pme-switch), you can also use reaction-field-zero if
 you really don't
 want to use PME.
 Then use nstlist=-1, run a short simulation and check in at the end
 of your log file
 that the neighbor list lifetime is somewhere between 5 and 20 steps.

 We should have a wiki entry for such details. Maybe there is one, but
 I was too lazy
 to check or make one.

 There was a basic NVE page; I have updated it based on your notes above:

 http://www.gromacs.org/Documentation/Terminology/NVE

 -Justin


 Berk

   Date: Mon, 1 Mar 2010 09:16:36 +0100
   From: r.fried...@bioc.uzh.ch
   To: gmx-users@gromacs.org
   Subject: Re: [gmx-users] NVE of water
  
   Hi Andrea,
   Did you use double precision? Also, I'd try a lower dt (say 1fs) and
   shake tolerance (maybe 1E-8).
   Good luck,
   Ran
  
   Andrea wrote:
Dear users,
   
for test purposes in order to set up a bigger system, I try to
 run NVE
simulations of SPC water, but the energy increases very
 rapidely. My
guess is that the cutoffs I use are not good for water. I that the
case ( I would be grateful for a good reference for suitable SPC
 water
parameters) or do I miss something else?
My parameter file for the NVE is:
   
title = NVE
cpp = /lib/cpp
integrator = md
dt = 0.002 ; ps ! = 2 fs
nsteps = 5 ; total 100 ps
nstxout = 5000
nstvout = 5000
nstxtcout = 0
nstlog = 5000
nstenergy = 5000
nstlist = 10
ns_type = grid
rlist = 1.1
   
unconstrained-start = yes
constraints = all-bonds
constraint_algorithm = shake
shake_tol = 0.0001
;VdW
vdwtype = Switch
rvdw = 1.0 ; rvdw+ (0.1:0.3)= rlist
rvdw_switch = 0.9
gen_vel = no ; yes
gen_temp = 300
gen_seed = -1
;Temperature coupling
tc_grps = system
tcoupl = no ;nose-hoover
tau_t = 0.1
ref_t = 300
;Pressure coupling
pcoupl = no
optimize_fft = yes
   
Any suggesions are really welcome.
   
Thank you.
   
Regards,
Andrea Muntean
  
  
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   Postdoctoral Fellow
   Computational Structural Biology Group (A. Caflisch)
   Department of Biochemistry
   University of Zurich
   Winterthurerstrasse 190
   CH-8057 Zurich, Switzerland
   Tel. +41-44-639
   Email: r.fried...@bioc.uzh.ch
   Skype: ran.friedman
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Re: [gmx-users] NVE of water

2010-03-01 Thread Ran Friedman
Berk Hess wrote:


  Date: Mon, 1 Mar 2010 15:44:28 +0100
  From: r.fried...@bioc.uzh.ch
  To: gmx-users@gromacs.org
  Subject: Re: [gmx-users] NVE of water
 
  Mark Abraham wrote:
   On 2/03/2010 12:39 AM, Ran Friedman wrote:
   Hi,
  
   I would still argue that double precision is important.
  
   Oh? The discussion of Table 4 of
   http://pubs.acs.org/doi/abs/10.1021/ct700301q (2008 GROMACS 4 JCTC
   paper) suggested to me that single-precision NVE could be done well in
   GROMACS. Am I missing something?
  
   Mark
  The presented benchmarks were performed in the NVT ensemble
 (section IX).
  Or am I missing something?

 No, but everything that affects energy conservation in NVE also
 affects it in NVT,
 in addition the thermostat affect the integration accuracy in NVT (and
 in NVT
 you do not measure energy conservation from the total energy, but from the
 conserved energy quantity).

 Double precision can be important for energy conservation, but often other
 factors deteriorate the energy conservation orders of magnitude from what
 can be reached in single precision already. Double precision is only
 required
 for testing or when you really need to generate an NVE ensemble.

 Berk
Thanks for clarifying Berk - I was referring to the latter (i.e., when
you really need to generate an NVE ensemble). I guess this is the main
reason to run with NVE. Since most people are not running NVE with large
systems or for production simulations, the added accuracy often
justifies the use of double precision.

Best,
Ran

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Re: [gmx-users] Assembling a good simulation starting point

2010-02-19 Thread Ran Friedman, Biochemisches Inst.

Hello John,

How large was the force after EM? Large forces often results in systems that 
explode during the simulation. Also, did you minimise with or without 
solvent? You assessment seems correct - the initial structure wasn't 
minimised and the tools of the trade are trying different conformations, 
minimising in vacuo at first and using other modelling tools before Gromacs. 
Also, read a bit in the mailing list and search the literature for similar 
studies.


Good luck,
Ran

On Thu, 18 Feb 2010 19:08:11 -0800 (PST)
 John Ladasky blind.watchma...@yahoo.com wrote:

Hello everyone,

I'm a fairly new GROMACS user.  I'm running GROMACS 4.0.5 on top of Ubuntu 
Linux 9.10.  I am still learning a lot.

 
I just tried to set up my first fairly complex simulation, and it failed.  
I have a protein of interest, a beta barrel with a hydrophobic, 
ligand-binding interior.  I am interested in making mutations to this 
protein, with the goal of getting it to bind to a rather different ligand 
than the one it normally binds.

 
The way that I propose to go about studying this problem is to construct a 
partially-unfolded version of the protein structure, add my ligand of 
interest, and then run an energy minimization.

 
My first naive attempt to construct the partially-unfolded protein was not 
successful.  I knew that it might have problems, but I tried it anyway.  
Using Biopython, I rotated the atomic coordinates so that the beta barrel 
was parallel to an axis.  Then I simply pulled all of the atoms 3 Angstroms 
away from the axis.  Finally, I inserted my ligand.  Visually, inspecting 
the starting structure with PyMol, I didn't see anything egregious.  
However, I could have some unwanted close contacts.


I got a few long bond warnings from pdb2gmx, but I persisted.  I got 
through genbox, editconf, and my first grompp sucessfully. But then when I 
tried the first, position-restrained energy minimization, it aborted with 
too many LINCS warnings.   I blew the system up.


These LINCS warnings could come from close contacts, or from large forces 
in over-stretched bonds which resulted from my crude approach to expanding 
the protein structure.  Whatever the cause, I need a smarter way to start.  
I am open to ANY suggestions!

 
What I THINK I might want to do is to manipulate the starting structure in 
a more natural way.  For example, selecting some peptide bonds in the beta 
turns, and changing their angles.  A program which allows me to manipulate 
structures, and not just simulate natural forces, is what I think I need.  
 
Surely, people who have used GROMACS will have faced problems simliar to 
mine.  Thanks for your advice!

 
John Ladasky




 


--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Institute of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Skype: ran.friedman
--

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Re: [gmx-users] problem normal mode analysis

2010-02-14 Thread Ran Friedman
Hi,
I guess posting the whole set of commands you used and mdp file for NMA
can help.
Best,
Ran

sarbani chattopadhyay wrote:
 hi,
 I want to do a normal mode analysis on a small peptide.
 I had complied gromacs in double precision and energy minimized the
 structure in vacuum,
 using steepest descent followed by conjugate gradient method. the log
 file of conjugate
 gradient method reads
 Polak-Ribiere Conjugate Gradients converged to Fmax  0.0001 in 1023 steps
 Potential Energy = -1.95899271351756e+02
 Maximum force = 9.50250289517625e-05 on atom 48
 Norm of force = 3.82317661305055e-05

 but when i try to run mdrun_d ( for normal mode analysis) , it shows
 Maximum force: 2.05241e+02
 Maximum force probably not small enough to ensure that you are in an
 energy well. Be aware that negative eigenvalues may occur when the
 resulting matrix is diagonalized

 I had made grompp_d read the trajectory file of cg energy
 minimization by using the -t
 flag.
 where have i gone wrong?
 Any suggestion will be of great help.
 Thanks in advance.
 Sarbani Chattopadhyay
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Re: [gmx-users] Problem with OPLS Benzene and Bond Constraints

2010-02-11 Thread Ran Friedman
Dear Mike,

It's hard to know what's going on from your input. Did you check the
thermodynamic components with g_energy (especially the pressure bond, LJ
and Coulomb energies)? This may give you a hint. Also, I would do a test
run with PME - you're anyway not following the parametrisation of
Jorgensen and co-workers exactly. As a final note - the correct phase is
something that's very difficult to reproduce exactly with classical MD,
and while a single molecule interacting with a protein may work just
fine, a bulk of such molecules does not always reproduce the correct
phase at a given temperature. This is one reason why lipid models are
still being developed.

Hope that helps a bit,
Ran

Mike Wykes wrote:
 Dear All

 I would like to perform MD simulations with benzene as a solvent and
 am observing some strange behaviour when I use Lincs to constrain all
 the bonds. When I run a fully flexible NPT MD of a box of 320 benzene
 molecules simulation at 298K and 1bar, the density comes out at  841
 g/l, not too far away from the experimental value of 876 g/l. However
 when I constrain all bonds using Lincs, the system expands rapidly,
 stabilising at a density of  2.62 g/l ! Both simulations started from
 NVT equilibrated simulations fixed to the experimental density. In the
 papers describing OPLS parametrisation, the MC simulations were indeed
 performed with fully flexible molecules, but it surprises me that the
 bond constraints would affect the density so strongly. Does anyone
 have any ideas why this is occurring? I am using a cutoff of 1.5 nm
 for VDW and Coulomb interactions without EWALD/PME but this is
 consistent with how OPLS was parametrised. There are no Lincs warnings
 in the log file of the constrained simulation.

 Please find my mdp and Benzene itp files below, the only difference
 between the flexible and constrained runs being dt = 0.001/0.002 and
 constraints = none/all-bonds respectively.

 Many thanks for your ideas/explanations as to what could be going on,

 Mike

 ;
 ;   File 'mdout.mdp' was generated
 ;   By user: mwykes (7017)
 ;   On host: node168
 ;   At date: Thu Feb  4 20:05:46 2010
 ;

 ; VARIOUS PREPROCESSING OPTIONS
 ; Preprocessor information: use cpp syntax.
 ; e.g.: -I/home/joe/doe -I/home/mary/hoe
 include  =
 ; e.g.: -DI_Want_Cookies -DMe_Too
 define   = -DFLEX_SPC

 ; RUN CONTROL PARAMETERS
 integrator   = md
 ; Start time and timestep in ps
 tinit= 0
 dt   = 0.002
 nsteps   = 500
 ; For exact run continuation or redoing part of a run
 ; Part index is updated automatically on checkpointing (keeps files separate)
 simulation_part  = 1
 init_step= 0
 ; mode for center of mass motion removal
 comm-mode= LINEAR
 ; number of steps for center of mass motion removal
 nstcomm  = 1
 ; group(s) for center of mass motion removal
 comm-grps=

 ; LANGEVIN DYNAMICS OPTIONS
 ; Friction coefficient (amu/ps) and random seed
 bd-fric  = 0
 ld-seed  = 1993

 ; ENERGY MINIMIZATION OPTIONS
 ; Force tolerance and initial step-size
 emtol= 1.0
 emstep   = 0.1
 ; Max number of iterations in relax_shells
 niter= 20
 ; Step size (ps^2) for minimization of flexible constraints
 fcstep   = 0
 ; Frequency of steepest descents steps when doing CG
 nstcgsteep   = 1000
 nbfgscorr= 10

 ; TEST PARTICLE INSERTION OPTIONS
 rtpi = 0.05

 ; OUTPUT CONTROL OPTIONS
 ; Output frequency for coords (x), velocities (v) and forces (f)
 nstxout  = 0
 nstvout  = 0
 nstfout  = 0
 ; Output frequency for energies to log file and energy file
 nstlog   = 500
 nstenergy= 500
 ; Output frequency and precision for xtc file
 nstxtcout= 500
 xtc-precision= 1000
 ; This selects the subset of atoms for the xtc file. You can
 ; select multiple groups. By default all atoms will be written.
 xtc-grps = BNZ
 ; Selection of energy groups
 energygrps   = BNZ

 ; NEIGHBORSEARCHING PARAMETERS
 ; nblist update frequency
 nstlist  = 10
 ; ns algorithm (simple or grid)
 nstype   = grid
 ; Periodic boundary conditions: xyz, no, xy
 pbc  = xyz
 periodic_molecules   = no
 ; nblist cut-off
 rlist= 1.5

 ; OPTIONS FOR ELECTROSTATICS AND VDW
 ; Method for doing electrostatics
 coulombtype  = Cut-off
 rcoulomb-switch  = 0
 rcoulomb = 1.5
 ; Relative dielectric constant for the medium and the reaction field
 epsilon_r= 1
 epsilon_rf   = 1
 ; Method for doing Van der Waals
 vdw-type = Cut-off
 ; cut-off lengths
 

Re: [gmx-users] intrapeptide hbond existence map

2010-02-11 Thread Ran Friedman
Hi Stephane,

The map shows weather a certain hydrogen bond exists at a certain time.
In principle you can get the information by integrating this data, but
I'm not sure it can be done without changing the code. A possible
solution is to use a script and run g_hbond -num 28 times with two
relevant groups (N-H  donor and oxygen acceptor), and calculate the
occupancy based on this (I guess you mean the fraction of time that this
h_bond existed.

Ran.

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 

 Thank you in advance for your help

 Stephane
   

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Re: [gmx-users] ice.pdbice.itp

2010-02-04 Thread Ran Friedman

 fairuz zulkifli wrote:
 Hello everybody,
 I'm Fairuz from Malaysia.
 I just want to ask if there is someone that have information about
 PDB of ice and itp file of ice.
 I only had PDB of the ice and trying to convert it into itp file
 using GAMESS software.

 You can't.  A .pdb file is a coordinate file, while an .itp is a
 parameter file (topology).  The two are not interchangeable.  I
 presume that you can use the parameters for water and simulate at a
 suitable temperature, though.

 -Justin
Not always - that depends on what you want to study.
It's very difficult to get realistic presentations of ice in MD, and the
freezing temperature of water models is usually not 273K. There are some
works on the subject, using an initial model prepared according to
geometric specifications. I remember something from Victoria Buch but
there may be newer studies around.

Ran.

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Re: [gmx-users] Re: Locally Enhanced Sampling with Gromacs

2010-01-27 Thread Ran Friedman
Hi,
LES as developed by Elber is available in CHARMM and MOIL.
Ran.

Massimiliano Bonomi wrote:
 Hi!
 You may want to try PLUMED, which is the evolution of grometa

 http://merlino.mi.infn.it/~plumed/PLUMED/Home.html

 and can do also steered MD and umbrella sampling.

 Massimiliano

 On Jan 27, 2010, at 8:48 AM, David van der Spoel wrote:

   
 On 1/27/10 7:49 AM, swa...@ncbs.res.in wrote:
 
 Dear Dr. Spoel,

 I am garduate student in National Centre for Biological
 Sciences(NCBS-TIFR), India. I am willing to do Locally Enhanced
 Sampling(LES) in one my research project.I saw few webpages on LES using
 GROMACS but not able to find any proper documentation/tutorial on that.
 Would you please help me regarding the same??

 Thanks,

 Regards,


   
 Please keep questions on the list.
 Gromacs implements Flooding and Replica Exchange, both are well documented. 
 In addition you can use metadynamics (similar to flooding) with gromacs if 
 you install grometa.

 -- 
 David van der Spoel, Ph.D., Professor of Biology
 Dept. of Cell  Molec. Biol., Uppsala University.
 Box 596, 75124 Uppsala, Sweden. Phone:   +46184714205. Fax: +4618511755.
 sp...@xray.bmc.uu.se sp...@gromacs.org   http://folding.bmc.uu.se
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Re: [gmx-users] Problems with g_hbond

2010-01-04 Thread Ran Friedman
Hi Rolf,
Try renaming the atom names to something that starts with O and H for
oxygen and hydrogen.
Good luck,
Ran.

Rolf Erwin Isele-Holder wrote:
 Dear users,

 I'm running a simulation which uses ethanol as solvent. When using g_hbond 
 the programm is able to recognize the solute's donors and acceptors, however 
 it does not recognize any acceptors or donors of ethanol. Here is a part of 
 my topology:

 [ atoms ]
 ;   nr   type  resnr residue  atom   cgnr charge   mass  typeB
 chargeB  massB
  1 HO  1   ETHH EH  1  0.398  1.008   ; qtot 
 0.398
  2 OA  1   ETHH EO  1 -0.54815.9994   ; qtot 
 -0.15
  3CH2  1   ETHHEC1  1   0.15 14.027   ; qtot 0
  4CH3  1   ETHHEC2  2  0 15.035   ; qtot 0

 [ bonds ]
 ;  aiaj functc0c1c2c3
 1 2 1 
 2 3 1 
 3 4 1 

 Why doesn't g_hbond recognize any donors or acceptors?

 Regards,

 Rolf
   

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Re: [gmx-users] g_mindist -or inconsistencies with atom-pairs

2009-12-22 Thread Ran Friedman
Dear Shay,

What do you get when -or is present? Do the atoms always belong to the
same residues?
I suspect that since the calculation of the minimal distance is made for
all residues, what you get at the end is the atoms at minimal distance
between the last two residues. This seems like a bug and I suggest you
submit a bugzilla.

As a side note I think that the output will be given only for the last
two groups in case there are more than two. You may want to check this
as well if you submit a bug report.

It should be too difficult to fix, but would involve changes in a few
places in the code.

Best regards,
Ran.

shaya...@post.tau.ac.il wrote:
 Dear Gromacs users,

 We used g_mindist analysis as follows:
 g_mindist -f *.xtc -s *.tpr -o atom-pairs.out -od mindist.xvg -or
 res_mindist.xvg

 and surprisingly in the atom-pairs.out only several atoms in one
 residue (from group 1) were at minimum distance from group 2
 throughout the entire simulation. Checking this output manually showed
 it to be incorrect.
 res_mindist.xvg seems to hold the correct data.

 When running the same analysis, only omitting the -or flag, we get a
 *correct* atom-pairs.out.
 g_mindist -f *.xtc -s *.tpr -o atom-pairs.out -od mindist.xvg

 Comparing mindist.xvg from both scenarios shows no difference (files
 are identical).

 Is the -or flag supposed to affect the other output files of the
 g_mindist function?

 Supplementary details:
 1. The same thing happened when g_mindist -s was supplied with either
 .gro, .pdb or .tpr files.
 2. Index-groups 1 and 2 consisted upon full molecules with no
 ommisions (full protein and not only C-alpha).
 3. We ruled out PBC by using -nopi
 4. This is common with the following Gromacs versions: 3.3.3., 4.0.5,
 4.0.7.

 Regards,
 -Shay

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Re: [gmx-users] reference for make_edi -linacc

2009-12-18 Thread Ran Friedman
Hi Chris,

Maybe in this paper:
http://www.ncbi.nlm.nih.gov/pmc/articles/PMC1303567/

Daidone et al., Molecular Dynamics Simulation of Protein Folding by
Essential Dynamics Sampling: Folding Landscape of Horse Heart Cytochrome c

Ran.

chris.ne...@utoronto.ca wrote:
 Hello,

 does anybody have a reference for the -linacc method applied by
 make_edi/mdrun? I have checked the references mentioned in make_edi -h
 as well as the manual, but didn't find anything that matches -linacc
 exactly.

 For example, gromacs suggests that entire MD steps will be accepted or
 rejected if they do or do not move in the desired direction along the
 selected eigenvectors, respectively:

 -linacc: perform acceptance linear expansion along selected eigenvectors.
 (steps in the desired directions will be accepted, others will be
 rejected).

 While the published version appears to be more complex:

 B.L. de Groot, A.Amadei, R.M. Scheek, N.A.J. van Nuland and H.J.C.
 Berendsen;
 An extended sampling of the configurational space of HPr from E. coli
 PROTEINS: Struct. Funct. Gen. 26: 314-322 (1996)

 Briefly, the algorithm consists of the following steps: a starting
 position is defined as the set of essential coordinates of the
 starting conformation; a number of regular MD steps is preformed; for
 each step, a new starting position is accepted only if it is not
 closer to the starting position than the previous position, in the
 subspace defined by the first three eigenvectors (i.e., if the
 distance from the starting position in this subspace does not
 decrease). If the new position is closet to the starting position, a
 correctio is applied only in the subspace defied by the first three
 eigenvectors with least perturbation.

 Thank you,
 Chris.

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Re: [gmx-users] using trjconv to get a 2x2x2 unit cell for traj.xtc

2009-12-08 Thread Ran Friedman
Dear Jenny,

You can do this directly in VMD, using the Periodic tab under
Graphics-Representations.

Ran

Jennifer Williams wrote:


 Hello,

 I am trying to find a way around a visualisation problem I am having
 in VMD. Some of my molecules go over periodic boundary conditions
 meaning that bonds sometimes appear missing when looking at movies (I
 am trying to fix this using wrap, unwrap and join in VMD but as yet no
 luck).

 I was wondering if there is a way in gromacs to multiply the number of
 unit cells shown in a trajectory. i.e instead of a 1x1x1 I want the
 new unit cell to be 2x2x2. This would mean the section of the
 structure I want to zoom in doesn't go over the pbc.

 For the confout.gro file I have done this using

 genconf -nbox 2 2 2 -f confout.gro -o confbig.out

 and this enables me to at least see a static image where all bonds are
 present.

 but in order to view a movie, I need to carry out something similar on
 the traj.xtc file. I have seen that with trjconv there is the option

 -box  Size for new cubic box

 but my unit cell is not cubic, it is a parallelepiped. The cell
 dimensions are :

 4.64210   3.77847   1.89596   0.0   0.0  -2.18150   0.0  
 0.0   0.0

 I tried using this anyway with the following command:

 trjconv -box 9.28414 8.72598 3.79192 -f traj.xtc -o trajbig.xtc

 but the resulting .xtc file wouldn't load into VMD so I assume that
 the .xtc file and the .gro file didn't match.

 Any ideas?,

 Thanks

 Jenny







 --The University of Edinburgh is a charitable body, registered in
 Scotland, with registration number SC005336.


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Re: [gmx-users] Docking with PyMol and using Gromacs

2009-11-12 Thread Ran Friedman
With VMD it's even simpler: use dynamic bonds.

Ran.

Nicolas Sapay wrote:


 Dallas B. Warren a écrit :

 Coordinate files like pdb and gro aren’t used by GROMACS to provide
 any bonding information. That is what the topology files are for. So
 their “presence” in your pdb isn’t an issue.

 Actually, what is probably happening is that PyMol is guessing the
 bonds presence, based on the distance between atoms, and displaying
 it (which is what VMD does as well). So the bonds aren’t actually
 there at all in the pdb file.

 VMD can read/write CHARMM/NAMD topology files (namely psf files). If
 your problem is *just* a visualization artefact, you can load your
 structure in VMD, write a psf file and delete the unwanted bonds (this
 does not require a specific forcefield). You can also combine 2 psf
 files (1 for your protein and 1 for your ligand), that require some
 basic knowledge of TCL though. After that, you just have to load the
 topology abd the coordinates:

vmd -psf topology.psf -pdb coordinate.pdb

 You won't see any weird bonds.

 Nicolas

 Catch ya,

 Dr. Dallas Warren
 Drug Delivery, Disposition and Dynamics
 Monash Institute of Pharmaceutical Sciences, Monash University
 381 Royal Parade, Parkville VIC 3010
 dallas.war...@pharm.monash.edu.au
 +61 3 9903 9167
 -
 When the only tool you own is a hammer, every problem begins to
 resemble a nail.

 *From:* gmx-users-boun...@gromacs.org
 [mailto:gmx-users-boun...@gromacs.org] *On Behalf Of *Gunnar
 Widtfeldt Reginsson
 *Sent:* Thursday, 12 November 2009 10:13 AM
 *To:* gmx-users@gromacs.org
 *Subject:* [gmx-users] Docking with PyMol and using Gromacs

 Hi.

 I am a new user of Gromacs.

 My question is both PyMol and Gromacs related.

 I tried the PyMol users mailing list but couldn't find anything.

 I have a small organic molecule that I am inserting into DNA in pymol.

 I have the DNA as one pdb file and the organic molecule as another
 pdb file. I open the DNA file in pymol and then load the organic
 molecule. After docking the organic molecule I write save name.pdb

 When viewing the name.pdb file in pymol there are some bonds between
 the organic molecule and the DNA that I don't want. Somehow pymol
 creates them and I don't see those bonds in the name.pdb file when I
 open it in a text reader.

 I then create a .gro file with pdb2gmx of the DNA.pdb and a .gro file
 of the organic molecule with topolbuilder 1.2 , and unite those .gro
 files and convert into a .pdb with editconf

 The newly created pdb file still has those unwanted bonds.

 My question is:

 Can I ignore those bonds?

 If not, how can I prevent pymol making those bonds?

 Thanks.


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Re: [gmx-users] Constraints Restraints

2009-11-12 Thread Ran Friedman
Erik Marklund wrote:
 Mark Abraham skrev:
 Darrell Koskinen wrote:
 Hi Tsjerk,
 So then, if I understand correctly, setting constraints =
 all-bonds is not as realistic as setting constraints = none,
 since the latter will allow for flexible (e.g. harmonic) behavoir
 which is more realistic than fixing the bond to a certain distance,
 correct?

 Actually not. It would be a better model of a harmonic potential
 (duh), but it has been shown that the use of constraints can lead to
 a (more?) acceptable model of a real system, and they allow a larger
 integration time to boot. Check out the papers for the constraint
 algorithms (refs in GROMACS manual).

 Mark

 Agreed. And this is especially true for hydrogen atoms as I understand
 it, since their behaviour as quantum particles deviate more from a
 classical treatment than is the case for heavier nuclei. This is
 mentioned in the gromacs manual.

 /Erik
This depends on the system you study. In some cases it is necessary not
to constrain the hydrogen atoms to get a better agreement with the
experiment. Also,  if one needs to deal with vibrational spectra
involving hydrogens, they must be mobile.

Ran.
 Date: Wed, 11 Nov 2009 21:45:44 +0100
 From: Tsjerk Wassenaar tsje...@gmail.com
 Subject: Re: [gmx-users] Constraints  Restraints
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID:
 8ff89815091245u63c6aa65sa839f24634352...@mail.gmail.com
 Content-Type: text/plain; charset=ISO-8859-1

 Hi Darrell,

 Constraints and restraints also apply to relative positions. A bond
 constraint fixes the bond to a certain distance. constraints =
 all-bonds means that all bonds are to be converted to constraints,
 rather than have them flexible, e.g. harmonic. Harmonic bonds are
 actually more like restraints, penalizing deviations from the
 equilibrium values. These equilibrium values and the 'penalty
 function' are described in the force field.

 Hope it helps,

 Tsjerk

 On Wed, Nov 11, 2009 at 9:32 PM,  darre...@ece.ubc.ca wrote:
  
 Hi,
 I just have a quick question on contraints and restraints. My
 understanding is that constraints fix the position of an atom in
 space and restraints restrain the deviation of the atom's position
 from its equilibrium point. Is that correct? If so, then I am a
 little
 confused by the purpose of constraints = all-bonds or constraints
 = none in an mdp file, since by selection of a force field, which
 has
 bond/angle/dihedral stretching/bending/torsion constants, we are
 specifying the constraints applied to the simulation. So then what is
 the purpose of constraints = all-bonds and constraints = none?

 Thanks.

 Darrell
 




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--
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Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.unizh.ch
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Re: [gmx-users] Hydrogen bond occupancy for the dimer of Acetic Acid

2009-11-12 Thread Ran Friedman
Hi Rasmus,

A simple solution would be to run g_hbond twice, with two separate
groups for acetate 1 as donor and acetate 2 as acceptor or vice versa,
check the existence an hydrogen bond with g_hbond -num and write a
script to check when the two hydrogen bonds co-exist.

Hope that helps,
Ran.

Rasmus Termo Lundsgaard wrote:
 Hi All.

 I'm trying to calculate the Hydrogen bond occupancy when there is two
 hydrogen bonds between same two acetic acid molecules at the same time.

 With g_hbond I can get the hbond.ndx giving me all ocuring hydrogen
 bonds group and the hbmap.xpm gives me the matrix of when these
 hydrogen bonds exist for each timeframe...

 How can I calculate the occupancy of when two hydrogen bonds exist
 between the same two molecules??


 Best regards
 Rasmus

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Re: [gmx-users] Hydrogen bond occupancy for the dimer of Acetic Acid

2009-11-12 Thread Ran Friedman
Hi Rasmus,

From your previous email I understood that you have only two molecules
(you didn't write that you're using 500 and nothing on the rest of the
system). Apparently, this is not the case. I don't think you can get
what you want from g_hbond without modifying the source code.  If you
don't mind 500 runs you can use g_dist -dist, where group 1 is a single
hydrogen bond donor oxygen and group two all potential acceptors, find
the molecules which satisfy your criterion and then run g_hbond on them
if you want to be sure that you have a hydrogen bond that satisfy angle
criteria as well. Tedious, but can work with some scripting and patience.

Ran.

Rasmus Termo Lundsgaard wrote:
 Hi Ran.

 If I understand you right, then you suggest to have one molecule as
 acceptor, and the rest (499) as donors, and then look in the hbnum.xvg
 to see how often there is two hydrogen bonds...

 1. is that I have to do this check for every molecule.

 2. there is no guaranty that the two hydrogen bonds are to the same
 other molecule - it could very well be as a part of a chain...

 3. If possible I would like to do measurement of distance between
 molecules when they are bonded as a dimer...

 Best regards
 Rasmus


 Ran Friedman wrote:
 Hi Rasmus,

 A simple solution would be to run g_hbond twice, with two separate
 groups for acetate 1 as donor and acetate 2 as acceptor or vice versa,
 check the existence an hydrogen bond with g_hbond -num and write a
 script to check when the two hydrogen bonds co-exist.

 Hope that helps,
 Ran.

 Rasmus Termo Lundsgaard wrote:
   
 Hi All.

 I'm trying to calculate the Hydrogen bond occupancy when there is two
 hydrogen bonds between same two acetic acid molecules at the same time.

 With g_hbond I can get the hbond.ndx giving me all ocuring hydrogen
 bonds group and the hbmap.xpm gives me the matrix of when these
 hydrogen bonds exist for each timeframe...

 How can I calculate the occupancy of when two hydrogen bonds exist
 between the same two molecules??


 Best regards
 Rasmus
 


   



-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.unizh.ch
Skype: ran.friedman
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Re: [gmx-users] Martini simulation problem in recentering trajectory so that the bilayer is at the center

2009-11-06 Thread Ran Friedman
For quite a long time I had the feeling that trjconv doesn't resolve all
situations. Following the very recent discussion between Roland Schutz
and Tsjerk, I'm not sure there is an immediate solution. Ad hoc
approaches such as preparation of tpr files from intermediate snapshots
were useful for me in some cases, so you can try these. For calculations
of distances you can sometimes calculate the shift and apply an a
posteriori fix, but that won't work for visualisation and isn't a robust
solution. I don't think it has anything to do with the MARTINI FF.

Ran.

maria goranovic wrote:
 So lets say that I delete the first frame from the trajectory in which
 some atoms might have been outside the box. Everything should be
 within the box once the simulation starts (from the second frame
 onwards)? So the procedure should work if the reference structure is
 the second frame? I have tried that, and it fails as well.

 On Thu, Nov 5, 2009 at 4:40 PM, XAvier Periole x.peri...@rug.nl
 mailto:x.peri...@rug.nl wrote:


 The nojump option will not apply the pbc when an atom is crossing the 
 box boundaries ... in your case your bilayer should definitely be
 in the 
 center of your box and all the atoms in  If not ot course it
 does not work!

 On Nov 5, 2009, at 4:33 PM, maria goranovic wrote:

 my starting structure looks quite all right to me. everything is
 in the box (except the tails of some lipids) .. wonder whats
 wrong. thank you verymuch for helping

 On Thu, Nov 5, 2009 at 4:04 PM, XAvier Periole x.peri...@rug.nl
 mailto:x.peri...@rug.nl wrote:


 On Nov 5, 2009, at 4:00 PM, maria goranovic wrote:

 Hi Xavier,

 Thanks for the clear instructions. The bilayer is not in one
 piece in the z direction after the -pbc nojump  for some
 reason.
 the problem might be from your starting structure, everything
 should be in the box! 
 Or you may be facing strange/funny/incomprehensible behavior
 ... 


 after the third step, the water is in the right place, but
 the bilayer has expanded to periodic boxes in the xy plane.
 so the center of mass of the lipid molecules is not really
 being centered in the box ?


 On Thu, Nov 5, 2009 at 3:34 PM, XAvier Periole
 x.peri...@rug.nl mailto:x.peri...@rug.nl wrote:


 you need to do:

 1- trjconv -pbc nojump; this keeps your bilayer in one
 piece on the z direction
 2- trjconv -center; using the bilayer to center and the
 system as output; this will 
 translate your bilayer on the z axis and normally not
 modify it on the xy plan. 
 3- trjconv -pbc mol; will put your lipids in one piece
 in the box; I believe this 
 step cn be coupled to the previous quite safely.

 On Nov 5, 2009, at 3:23 PM, maria goranovic wrote:

 One more note about -pbc nojump. I typically use -pbc
 mol. Using pbc nojump succeeds in keeping the center of
 the bilayer at 0 0 0, but the atoms have moved way out
 of the simulation box resulting in a dilute system

 On Thu, Nov 5, 2009 at 2:31 PM, maria goranovic
 mariagorano...@gmail.com
 mailto:mariagorano...@gmail.com wrote:

 Centering on one atom has a problem that the lipid
 diffuses in the plane of the membrane, and as a
 result, the entire system starts to center around
 the lipid resulting in a simulation box which
 translates a lot in the bilayer plane.

 The splitting is not a problem, yes. But during the
 simulation period when the bilayer is not split, it
 diffuses quite a bit along the bilayer normal
 (after use of -pbc mol, and centering around the
 lipid center of mass). a plot of the lipid center
 of mass shows the bilayer diffusing along z, when
 its not split.


 On Thu, Nov 5, 2009 at 2:25 PM, XAvier Periole
 x.peri...@rug.nl mailto:x.peri...@rug.nl wrote:


 On Nov 5, 2009, at 2:02 PM, Justin A. Lemkul wrote:



 maria goranovic wrote:

 I did use -pbc nojump, but that does
 not help


 What about entering on a central lipid tail
 atom, I suggested some time ago? The
 bilayer probably just splits across
 periodic boundaries, so this is not really
 a problem; just a visualization artefact.

 The splitting is not a problem and I think that
 centering using one lipid (tail) won't change
 

Re: [gmx-users] Is anyone also using lammps?s

2009-11-04 Thread Ran Friedman
Dear Peng,

Did you also try to run GMX in double precision at some point?

Ran

Peng Yi wrote:

 I turned off the torsion interaction.  The difference between Lammps
 and Gromacs at integration time step 2fs was reduced.  Details below:

 A melt of 240 n-octane (united-atom model), NVT, T=300K, V=55.46nm^3.
 Both Lammps and Gromacs use berendsen thermostat with tau_t=1ps.

 Integration time step 1fs:
  LammpsGromacsStd. Err. (for both)
 Ebond(kJ/mol):2092  2109   100
 Eangle:   1778  175480
 Elj+corr:   -10501-10553   100
 T(K):  300   299 5
 P(atm):   3188  3016   700

 integration time step 2fs:
  LammpsGromacsStd.Err. (for both)
 Ebond:2133  2232   100
 Eangle:   1803  173780
 Elj+corr:   -10501-10623   100
 T: 300   298 5
 P:3133  2955   600

 Lammps results remain almost unchanged when dt increases from 1fs to 2fs,
 and Ebond : Eangle = 7 : 6, which is the ratio between # of bonds and
 # of angles.

 Gromacs results change more significantly when dt goes from 1fs to 2fs.
 and the trend of Ebond and Eangle are opposite.  It is more significant
 when torsion interaction is present.


 On Tue, 3 Nov 2009, David van der Spoel wrote:

 Peng Yi wrote:

 Hi, David,

 I used Berendsen thermostat and a bigger tau_t=1ps to redo the
 simulations.
 The general conclusion is the same.  The std err is the same in both
 packages.  And during each simulation, the integration time does not
 change.  Details below:

 Integration time step 1fs:
 Lammps  GromacsStd.Err. (for both)
 Ebond(kJ/mol):   21122170   100
 Eangle:  17991770   100
 Etors:   25522490   100
 Elj+corr:  -10711  -10777   100
 P(atm):  32503216   500

 Integration time step 2fs:
 Lammps  GromacsStd.Err. (for both)
 Ebond:   21542654   120
 Eangle:  18401645   120
 Etors:   25732236   120
 Elj+corr:  -10711  -11019   100 P(atm): 
 3250 2590   600


 How about the temperature in both systems? Was Lammps also run with
 Berendsen? It could also still be a topology error. Maybe you can
 turn off the torsion potential to test this.

 -Peng

 On Sun, 1 Nov 2009, David van der Spoel wrote:

 Peng Yi wrote:

 Thank for your reply!  I have done some NVT runs per your
 suggestion, and
 the results are similar to NPT runs, i.e., Gromacs results is more
 affected by changing integration timestep than Lammps.  Details
 below:

 A melt of 240 octane chains by united-atom model. T=300K, V=55.46
 nm^3.
 Both Gromacs and Lammps use Nose-Hoover thermostat with tau_t=0.2 ps.

 As some people have note the tau_t is short for Nose Hoover. Are
 you sure this means the same in Lammps and in Gromacs? For one
 thing, there is no tau_t in the NH algorithm as far as I know, and
 Gromacs converts it to an appropriate weight or whatever that is
 called. What does Lammps do with this tau_t. To be a the safe side
 you could run both with Berendsen as well. Is the std err identical
 in both packages? And in the 2 fs run, are both simulation
 equlibrated with this time step as well?

 All other parameters in .top and .mdp files are the same as
 previously
 attached..

 If I use integration time 1fs, Lammps and Gromacs produce
 consistent results:
  Lammps  Gromacs  std. err.
 Ebond(kJ/mol):21332160 100
 Eangle:   17571780  80
 Etors:25312510  80
 Elj+corr:   -10711  -10767  90
 P(atm):   35003250 500

 if I use integration time 2fs, Lammps results remain unchanged, but
 Gromacs results change significantly, particularly bonded energy:

  Lammps  Gromacs  std. err.
 Ebond(kJ/mol):21752710 100
 Eangle:   17991640  70
 Etors:25732230  80
 Elj+corr:   -10711  -11007 100 P(atm):
 3200 2730 700

 Would that be a result of using different integrator between
 Lammps and Gromacs?  Lammps uses Velocity-Verlet, and Gromacs uses
 Leap-frog.
 Thanks,
 -Peng

 On Thu, 29 Oct 2009, David van der Spoel wrote:

 aherz wrote:
 Hey,

 are you running single or double precision gromacs?
 Afaik, depending on the circumstances the energy drift in
 gromacs can be
 rather bad for single precision.

 Please refer to the gromacs 4.0 paper for a discussion of the drift.
 If you want to compare energies you need the same density, which
 you do not have, you may need to run NVT for 

Re: [gmx-users] Is anyone also using lammps?s

2009-11-04 Thread Ran Friedman
Hi Peng,

AFAIK GMX only uses fftw for PME.

If you have no reason to prefer flexible bonds you can use LINCS or
SHAKE to constrain the bond lengths and run with a timestep of 2fs at
room temperature.

You may want to try LAMMPS and GMX with SHAKE and a timestep of 2fs and
see if the results are similar before recompiling GMX. If I understood
you correctly you didn't constrain the bonds.

Ran

Peng Yi wrote:

 Hi, Ran,

 Do you mean the simulation I used here for testing purpose?  That is
 not long, maybe a few hours.  But my research will require simulations
 for days.  If I will not use PME, do I still need a fftw?

 -Peng

 On Wed, 4 Nov 2009, Ran Friedman wrote:

 Hi Peng,

 It would be slower - never made any benchmarks on how much slower. But
 you don't run a very long simulation, do you?
 Installing it isn't a problem. If you use PME you also need fftw in
 double precision though.

 Ran

 Peng Yi wrote:

 Hi, Ran,

 No, I haven't.  I still have to find out how to install in double
 precision.  Would double precision be slower than single?  If so,
 how much?  Or just double the memory used?  Thanks,

 -Peng

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Re: [gmx-users] % of existence of hydrogen bond

2009-10-29 Thread Ran Friedman
Hi,
You can use g_hbond -num and write a small script to calculate the
percentage of h-bond existence per frame by calculating the number of
frames for which a h-bond exists.
Good luck,
Ran.

Moutusi Manna wrote:

 Dear all,

 I am dealing with a POPC+PEPTDE+WATER system. Basic residues
 of the peptide make hydrogen bonds with lipid headgroup (as reflected
 from g_rdf analysis) and the number of hydrogen bonds formed can be
 calculated from g_hbond program. Now, i want to calculate the % of
 trajectory time for which a bond between a particular group (say LYS
 and lipid headgroup po4) exist. -hbm gives a .xpm matrix, on solving
 (using xpm2ps) that i got a .eps file, which is a picture file of
 h_bond existence map, but the data sheet is not given.

 Can any one help me to solve this problem?

 With regards,

  

 Moutusi Manna

  


 
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Re: [gmx-users] Is anyone also using lammps?s

2009-10-29 Thread Ran Friedman
Hi Peng,

Note that you're not using any bond constraints in Gromacs and a
timestep of 2fs may be too long.
Also, tau_t=0.02 seems too short for me.

With 1fs timescale the agreement seem good enough, but you didn't
include estimated errors so it's hard to tell. Also, I assume you run
GMX in single and LAMMPS in double precision. Did you check for convergence?

Ran

Peng Yi wrote:

 On Wed, 28 Oct 2009, Mark Abraham wrote:

 Peng Yi wrote:

 I am trying to simulate alkane melt and found out that gromacs and
 lammps gave different results, particularly the bonded interaction
 energy.
 I wonder if anyone has such experience.  Thanks,

 Even two installations of the same version of GROMACS can give
 different results. The question is whether when using comparable
 model physics you observe the same ensemble averages.

 Mark

 Hi, Mark,

 Thanks for reply!  The difference is statistically significant.  And I am
 wondering if it is caused by the integrator: Leap-frog for Gromacs and
 Velocity-verlet for Lammps.  Detail description of the comparison please
 see below:

 It is an NPT simulation of a melt of 240 n-octane molecules using
 united-atom model, i.e., CHx group is considered as one atom.  There are
 bond, angle, torsion and LJ interactions.  T=300K and P=1atm.

 Lammps uses nose-hoover thermostat and barostat, and Gromacs uses
 nose-hoover thermostat and Parranello-Rahman barostat.  Time constants
 for
 thermostat and barostat are 0.02ps and 2.0ps, respectively.

 If I use integration time 1fs, Lammps and Gromacs gave consistent
 results:
 Lammps   Gromacs
 Ebond(kJ/mol):2092 2146
 Eangle:   1757 1760
 Etors:2510 2500
 Elj+corr:-9238-9350
 Volume(nm^3): 66.7 66.5

 where energy fluctuation is 100 kJ/mol and volume fluctuation is 1 nm^3,
 Elj+corr is the total LJ energy including tail correction.

 However, if I use integration time 2fs, Lammps results do not change
 much, but Gromacs results changed a lot:

 Lammps   Gromacs
 Ebond(kJ/mol):2133 2700 Eangle:  
 1799 1640
 Etors:2552 2200
 Elj+corr:-9292-9886 Volume:  
 66.7 64.0

 The results given by Lammps is more reasonable because the Ebond should
 be equal to the total # of bonds times 1/2k_BT and Eangle should be equal
 to the total # of angles times 1/2k_BT.  At T=300K, 1/2k_BT=1.25 kJ/mol.
 240 n-octanes have total 1680 bonds and 1440 angles.

 The bond and angle interactions are both harmonic functions.  Bond
 interaction constant kl=292880 kJ/mol/nm^2, corresponding to a bond
 ossilation period 16 fs.

 Is there something related to the integrator?

 Here I attached my grompp.mdp and topol.top files.

 ##
 grompp.mdp
 ##

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

 ; RUN CONTROL PARAMETERS
 integrator   = md
 tinit= 0
 dt   = 0.001
 nsteps   = 200
 init_step= 0
 comm-mode= Linear
 nstcomm  = 1
 comm-grps=

 ; OUTPUT CONTROL OPTIONS
 nstxout  = 5000
 nstvout  = 5000
 nstfout  = 5000
 nstcheckpoint= 1
 nstlog   = 1000
 nstenergy= 1000
 nstxtcout= 5000
 xtc-precision= 1000
 xtc-grps = energygrps   =

 ; NEIGHBORSEARCHING PARAMETERS
 nstlist  = 10
 ns_type  = grid
 pbc  = xyz
 rlist= 1.0025
 domain-decomposition = no

 ; OPTIONS FOR ELECTROSTATICS AND VDW
 coulombtype  = Cut-off
 rcoulomb-switch  = 0
 rcoulomb = 1.0025
 epsilon-r= 1
 vdw-type = Cut-off
 rvdw-switch  = 0; default rvdw
 = 1.0025; default 1 nm
 DispCorr = EnerPres
 ;table-extension  = 1.5
 fourierspacing   = 0.12
 fourier_nx   = 0
 fourier_ny   = 0
 fourier_nz   = 0
 pme_order= 4
 ewald_rtol   = 1e-05
 ewald_geometry   = 3d
 epsilon_surface  = 0
 optimize_fft = no


 ; OPTIONS FOR WEAK COUPLING ALGORITHMS
 Tcoupl   = nose-hoover
 tc-grps  = System
 tau_t= 0.02
 ref_t= 300.0
 Pcoupl   = Parrinello-Rahman
 Pcoupltype   = isotropic
 tau_p= 2.0
 compressibility  = 4.5e-5
 ref_p= 1.0
 andersen_seed= 815131

 ; GENERATE 

Re: [gmx-users] Is anyone also using lammps?s

2009-10-29 Thread Ran Friedman
Hi Peng,

The time scale should be much shorter than the fastest vibration. A rule
of thumb from the reference below is a factor of ten, but it would
depend on the precision. Running with double precision is shorter but I
didn't make benchmarks (perhaps other users have).

Appropriate values of tau_t and tau_p have also been discussed in this
list (search for references by Berk). I tend to use something like
tau_t=0.2 and tau_p=1.0.

I advise you to follow David's suggestion as well and run with NVT.

Ran.

Reference:
@book{Becker2001,
   Author = {Becker, O. M. and MacKerell, A. D. Jr. and Roux, B.  and
Watanabe, M.},
   Title = {Computational biochemistry and biophysics},
   Publisher = {Dekker, M.},
   Address = {New York},
 Year = {2001} }

Peng Yi wrote:

 Hi, Ran,

 I didn't use bond restraints.  I checked that the bond length had a
 Gaussian-like distributes, and the length range looked normal.

 I estimated the fastest timescale in the system, which is the bond
 ossilation period, around 16fs.  Would that require as integration
 timestep much smaller than 1fs?

 With the parameters I have, could you recommend a set of tau_t and tau_p?
 I did mention the fluctuation, 100 kJ/mol for energy and 1 nm^3 for
 volume.  And I ran GMX in single.  Not sure about Lammps, should be
 double.  All measured physical quantities converged well.  Would you
 expect differece if I compile GMX in double?  Would that be much slower?
 -Peng

 On Thu, 29 Oct 2009, Ran Friedman wrote:

 Hi Peng,

 Note that you're not using any bond constraints in Gromacs and a
 timestep of 2fs may be too long.
 Also, tau_t=0.02 seems too short for me.

 With 1fs timescale the agreement seem good enough, but you didn't
 include estimated errors so it's hard to tell. Also, I assume you run
 GMX in single and LAMMPS in double precision. Did you check for
 convergence?

 Ran

 Peng Yi wrote:

 On Wed, 28 Oct 2009, Mark Abraham wrote:

 Peng Yi wrote:

 I am trying to simulate alkane melt and found out that gromacs and
 lammps gave different results, particularly the bonded interaction
 energy.
 I wonder if anyone has such experience.  Thanks,

 Even two installations of the same version of GROMACS can give
 different results. The question is whether when using comparable
 model physics you observe the same ensemble averages.

 Mark

 Hi, Mark,

 Thanks for reply!  The difference is statistically significant.  And
 I am
 wondering if it is caused by the integrator: Leap-frog for Gromacs and
 Velocity-verlet for Lammps.  Detail description of the comparison
 please
 see below:

 It is an NPT simulation of a melt of 240 n-octane molecules using
 united-atom model, i.e., CHx group is considered as one atom.  There
 are
 bond, angle, torsion and LJ interactions.  T=300K and P=1atm.

 Lammps uses nose-hoover thermostat and barostat, and Gromacs uses
 nose-hoover thermostat and Parranello-Rahman barostat.  Time constants
 for
 thermostat and barostat are 0.02ps and 2.0ps, respectively.

 If I use integration time 1fs, Lammps and Gromacs gave consistent
 results:
 Lammps   Gromacs
 Ebond(kJ/mol):2092 2146
 Eangle:   1757 1760
 Etors:2510 2500
 Elj+corr:-9238-9350
 Volume(nm^3): 66.7 66.5

 where energy fluctuation is 100 kJ/mol and volume fluctuation is 1
 nm^3,
 Elj+corr is the total LJ energy including tail correction.

 However, if I use integration time 2fs, Lammps results do not change
 much, but Gromacs results changed a lot:

 Lammps   Gromacs
 Ebond(kJ/mol):2133 2700 Eangle:
 1799 1640
 Etors:2552 2200
 Elj+corr:-9292-9886 Volume:
 66.7 64.0

 The results given by Lammps is more reasonable because the Ebond should
 be equal to the total # of bonds times 1/2k_BT and Eangle should be
 equal
 to the total # of angles times 1/2k_BT.  At T=300K, 1/2k_BT=1.25
 kJ/mol.
 240 n-octanes have total 1680 bonds and 1440 angles.

 The bond and angle interactions are both harmonic functions.  Bond
 interaction constant kl=292880 kJ/mol/nm^2, corresponding to a bond
 ossilation period 16 fs.

 Is there something related to the integrator?

 Here I attached my grompp.mdp and topol.top files.

 ##
 grompp.mdp
 ##

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

 ; RUN CONTROL PARAMETERS
 integrator   = md
 tinit= 0
 dt   = 0.001
 nsteps   = 200
 init_step= 0
 comm-mode= Linear
 nstcomm  = 1
 comm-grps=

 ; OUTPUT CONTROL OPTIONS
 nstxout  = 5000
 nstvout  = 5000
 nstfout  = 5000

Re: [gmx-users] g_hbond and fluor

2009-10-13 Thread Ran Friedman
David van der Spoel wrote:
 Alvaro Cortes wrote:
 Hi all.

 I'm new at the list so i don't know if something similar has been
 discussed before.
 I tried to search in the archives, but i can't find something similar.

 I have a doubt about g_hbond and fluor acceptors. As i can see in the
 code, no parsing of F atoms is done in search_acceptors function in
 gmx_hbond.c, so i added || ((*top-atoms.atomname[n])[0] == 'F') ||
 between oxygen and nitrogen parsing. This results in an increase of
 the number of hbonds reported by the program but i dont know if this
 little change  is enough or even correct.

 Someone can bring me light in this stuff?

 I think it should be correct. Obviously it would be good to be more
 flexible without the need for user programming. In some contexts one
 might want to look for C-H ... 0 bonds as well and even N-H ...
 Aromatic interactions.
A bit off topic from the fluor-related issue, but if you modify g_hbond,
maybe it makes sense to disable nitogen atoms from being acceptors per
default. I don't think having nitrogen acceptors is very common.


 Thank you in advance.
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Re: [gmx-users] scalar correlation matrix

2009-09-21 Thread Ran Friedman
Hi,
Check out the modified g_covar version with correlations, which is on
the user contributions.
Ran.

sheerychen wrote:
 Hello, everyone,

 Do anybody knows how to calculate the scalar correlation
 matrix across the alpha carbon atoms, where the correlation function
 is defined as: Cij=delta_ri*delta_rj/squart(delta_ri^2delta_rj^2).
 Is there any direct command can do this in gromacs? Thanks.
 //   
 //
 

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Re: [gmx-users] copper cluster bond to histidines

2009-08-12 Thread Ran Friedman
Dear Andrea,

Which restraints did you use?
I've ran simulations on a similar system (Zn2+ coordinated to
histidines) with NMR restraints as implemented in Gromacs and it worked
fine.

Best regards,
Ran.

andrea spitaleri wrote:
 Dear all,
 I am going to run some MD simulation of a protein bearing a copper cluster (3 
 Cu2+ nominally charge
 2+) coordinates to histidine residues. As far as concerning the importance of 
 this cluster in the
 enzymatic activity (this would require QM/MM), my issue is how to interpret 
 the whole system
 [HIS_{2}-Cu2+]_{3} in term of force field. From literature and from previous 
 posts in this mailing
 list, in MD system similar to mine (aminoacid coordinating ions) are treated 
 as an unique residues
 (i.e. HEME group). My first try was to perform MD without restraints on Cu2+, 
 but unfortunately at
 100K (I am doing an equilibration from 100K to 300K) after few ps one of the 
 Cu2+ left already its
 position (basically it is flying away).
 Second try was to put restraints on the system between the Cu2+ and the 
 N-HIS. However, my doubt is
 how bad is this assumption respect to the possibility to consider the whole 
 system Cu2+-HIS as an
 unique residue in the topology file. I am aware that for the latest 
 hypothesis I should reconsider
 all the properties (i.e. charges, angles, etc ...), so a long way and hard 
 work. Think about that I
 need to put a O2 molecule inside of the Cu2+ cluster in a second study.

 Any suggestion, comments and anything else are very welcome.

 Thanks in advance

 Regards

 andrea

   


-- 
--
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Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.unizh.ch
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Re: [gmx-users] Switch - Shift function electrostatics

2009-07-27 Thread Ran Friedman
David van der Spoel wrote:
 Emanuel Peter wrote:
 Dear Gromacs-users,

 At the moment I have a question which regards the different
 electrostatic algorithms mentioned in the Gromacs-manual.

 I did some simulations and I tried three different electrostatic
 algorithms: Cut-off, Shift and PME.

 It is clear to me what Shift and PME means principally, but I ask myself
  which electrostatic algorithm is used by Cut-off.
 I know that Cut-off means a twin-range-electrostatics calculation with
 rlist as the first range and r_coulomb as the second range. Both are
 calculated within different frequencies. Is that true ?

 In my .log file it is mentioned that when using Cut-off a default value
 r_coulombswitch equal to 0 is set. It is the same in the case of
 r_vdwswitch.

 Does that mean that I use in this special case a switch function which
 switches at 0 nm which represents in this case a shift-function that
 shifts my electrostatic potential in such a way, that it decays to zero
 at r_coulomb?
 I think this means that I used a shift-function which is calculated
 within the twin-range-electrostatics scheme.
 Is this true?

 What disadvantages does the twin-range-electrostatics calculation
 have in comparison to PME?
 Is it true that PME could stabilize my system artificially?

 No, it is the other way around. Cut-offs are bad.
 Check:
 J. Chem. Theor. Comp. 2 pp. 1-11 (2006)


 Now another question:

 Some people who perform molecular-dynamics calculations are stabilizing
 the dihedral angles in the forcefield to avoid 'unrealistical'
 fluctuations of their protein. Is this a reasonable way to simulate a
 protein?
 No, you are changing the force field in that way. I haven't heard of
 this previously.
I guess you mean CMAP in CHARMM.
You can check out the relevant paper, which also includes details about
some other force fields.

Ran.
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Re: [gmx-users] Re: Some questions on Tabulated Dihedral Potential

2009-07-23 Thread Ran Friedman
Hi Johannes,

Thanks for the correction - you're right of course (when deltaX = 1 it's
the same).

To be closer to the gromacs code it's
der = (y[N+1] - y[N-1]) * 0.5 * tabscale

where
tabscale = number of points per nm (or degree for angles/dihedrals).

Ran.

Johannes Kamp wrote:
 Hi Ran,

 are you sure the derivative is calculated as:
 der = (y[N+1] - y[N-1]) * 0.5 * deltaX

 and not as:
 der = (y[N+1] - y[N-1]) * 0.5 / deltaX ?

 The last calculation makes a little more sense to me...

 -Johannes


 Ran Friedman wrote:
 Hi,

 The numerical derivative for the Nth value y[N] is calculated as:
 der = y[N+1] - y[N-1] * 0.5 * deltaX
 Correction:
 der = (y[N+1] - y[N-1]) * 0.5 * deltaX
 where y is the potential deltaX is the difference between two
 successive values in your input (e.g., 1 if you have a table that
 goes from -180 to 180 with 361 values).

 I don't think you can print the number without changing the code,
 but it's not difficult to calculate. You can plot your forces and
 -der and see where they deviate.

 Ran.
 

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Re: [gmx-users] Re: Some questions on Tabulated Dihedral Potential

2009-07-21 Thread Ran Friedman
Hi,

Johannes Kamp wrote:
 Hi Cynthia,

 I'm also working on including some tabulated functions but I don't
 have any simulation yet. Thus I'm not a 'specialist'  in this topic,
 but I hope I can help you a little.

 Dear all, 

 I tried to include 2 tabulated dihedral potential functions into my
 simulation. But it seems to be not able to generate correct results.
 The system just exploded. I defined 3601 points in each table (from
 -180 to 180 with an increment 0.1). After 'mdrun', GOMACS generates
 two warning information:

 WARNING: For the 3598 non-zero entries for table 0 in table_d1.xvg
 the forces deviate on average 193% from minus the numerical
 derivative of the potential
 WARNING: For the 3598 non-zero entries for table 0 in table_d2.xvg
 the forces deviate on average 193% from minus the numerical
 derivative of the potential
  
 Do these two warnings matter very much? I checked the values for
 x,f(x),-f'(x) in the tables and don't think there're mistakes. has
 anyone of you met with such problems?
In the tables you should supply potentials and forces. The forces are
also calculated numerically, and a warning is emitted if the numerical
derivatives deviate too much from the forces supplied by the user. Since
the forces are interpolated, if the numerical derivative is too far from
the input what you'd get will be different then expected. You can
calculate the derivatives yourself and see where there are deviations.

Good luck,
Ran
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Re: 回复: [gmx-users] Re: Some questio ns on Tabulated Dihedral Potential

2009-07-21 Thread Ran Friedman
Hi,

The numerical derivative for the Nth value y[N] is calculated as:
der = y[N+1] - y[N-1] * 0.5 * deltaX
where y is the potential deltaX is the difference between two successive
values in your input (e.g., 1 if you have a table that goes from -180 to
180 with 361 values).

I don't think you can print the number without changing the code, but
it's not difficult to calculate. You can plot your forces and -der and
see where they deviate.

Ran.

hong bingbing wrote:
 Hi, Ran,

 The potential f(x) and force -f'(x) in the table are calculated by
 myself before constructing the table. The potential can be written in
 an analytical form and the force is calculated as the analytical
 negative derivative of the potential at point x. There should not be
 so large deviation betw. the value I supplied and the value calculated
 by GROMACS. Wait. Is there something wrong in my interpretation?
 What's  your method to get the force? Is there a way to see the
 numerical derivative generated by GROMACS?

 Thanks
 CH

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Re: 回复: [gmx-users] Re: Some questio ns on Tabulated Dihedral Potential

2009-07-21 Thread Ran Friedman
Ran Friedman wrote:
 Hi,

 The numerical derivative for the Nth value y[N] is calculated as:
 der = y[N+1] - y[N-1] * 0.5 * deltaX
Correction:
der =  (y[N+1] - y[N-1]) * 0.5 * deltaX
 where y is the potential deltaX is the difference between two
 successive values in your input (e.g., 1 if you have a table that goes
 from -180 to 180 with 361 values).

 I don't think you can print the number without changing the code, but
 it's not difficult to calculate. You can plot your forces and -der and
 see where they deviate.

 Ran.

 hong bingbing wrote:
 Hi, Ran,

 The potential f(x) and force -f'(x) in the table are calculated by
 myself before constructing the table. The potential can be written in
 an analytical form and the force is calculated as the analytical
 negative derivative of the potential at point x. There should not be
 so large deviation betw. the value I supplied and the value
 calculated by GROMACS. Wait. Is there something wrong in my
 interpretation? What's  your method to get the force? Is there a way
 to see the numerical derivative generated by GROMACS?

 Thanks
 CH

 

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-- 
--
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Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.unizh.ch
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Re: 回复: 回复: [gmx-users] Re: So me questions on Tabulated Dihedral Potential

2009-07-21 Thread Ran Friedman
As I wrote it der is the derivative itself, so you should plot (-1)*der.
Ran.

hong bingbing wrote:
 Thanks Ran. Should there also be a minus sign before (y[N+1]-y[N-1])
 because the third column in the table is -f'(x)?
 CH
  




 
 *发件人:* Ran Friedman r.fried...@bioc.uzh.ch
 *收件人:* Discussion list for GROMACS users gmx-users@gromacs.org
 *已发送:* 2009/7/21(周二), 上午9:41:42
 *主题:* Re: 回复: [gmx-users] Re: Some questions on Tabulated
 Dihedral Potential

 Ran Friedman wrote:
 Hi,

 The numerical derivative for the Nth value y[N] is calculated as:
 der = y[N+1] - y[N-1] * 0.5 * deltaX
 Correction:
 der =聽 (y[N+1] - y[N-1]) * 0.5 * deltaX
 where y is the potential deltaX is the difference between two
 successive values in your input (e.g., 1 if you have a table that
 goes from -180 to 180 with 361 values).

 I don't think you can print the number without changing the code, but
 it's not difficult to calculate. You can plot your forces and -der
 and see where they deviate.

 Ran.

 hong bingbing wrote:
 Hi, Ran,

 The potential f(x) and force -f'(x) in the table are calculated by
 myself before constructing the table. The potential can be written
 in an analytical form and the force is calculated as the analytical
 negative derivative of the potential at point x. There should not be
 so large deviation betw. the value I supplied and the value
 calculated by GROMACS. Wait. Is there something wrong in my
 interpretation? What's 聽your method to get the force? Is there a
 way to see the numerical derivative generated by GROMACS?

 Thanks
 CH

 

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 --
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 Computational Structural Biology Group (A. Caflisch)
 Department of Biochemistry
 University of Zurich
 Winterthurerstrasse 190
 CH-8057 Zurich, Switzerland
 Tel. +41-44-639
 Email: r.fried...@bioc.unizh.ch
 Skype: ran.friedman
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Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.unizh.ch
Skype: ran.friedman
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Re: [gmx-users] indexing largest cluster with g_clustsize

2009-07-16 Thread Ran Friedman
Hi Dmitri,
It's the last frame - the file is written after all frames are read and
dealt with.
Best regards,
Ran

Dmitri Dubov wrote:

 Dear gmx'ers!


 One more question on g_clustsize routine:

 It produces an index file with the atom numbers of largest cluster.
 But how it works in an evaporating system where the number of
 clustered molecules reduces greatly through the trajectory? What frame
 the maxclust.ndx file concerns to?

 -- 

 Regards

  Dmitri  mailto:ddu...@ngs.ru

 

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Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-639
Email: r.fried...@bioc.unizh.ch
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Re: [gmx-users] xdr library. Just for an example.

2009-07-07 Thread Ran Friedman
Hi Vitali,

There should be such code with then library itself.

Ran.

Vitaly V. Chaban wrote:
 Hi,

 Can anybody share any working code which uses xdr-1.1 library? - Just
 to consult.

 Thank you very much in advance,
 Vitaly

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Re: [gmx-users] lincs warning

2009-06-03 Thread Ran Friedman
Hi XAvier,
Do you use virtual sites? I've seen this when I used virtual sites,
large time steps and a system that probably wasn't equilibrated enough.
Ran.

XAvier Periole wrote:

 Dears,

 I am experiencing some problems running a few proteins in water
 (GROMOS43a1/SPC)
 with gmx-4.0.4 using 32 CPUs.

 After some ns lincs warnings appear and eventually the simulation
 crashes dues
 to too many lincs warnings.

 When restarting the simulation feeding -cpi md.cpt to mdrun the
 simulation restarts
 fine and no lincs warning are reported on the same portion of the
 simulation. The
 simulation runs again for some ns and the same happens: new lincs
 warning appear
 and eventually the simulation crashes again.

 Any explanation for this? Any solution?

 Best,
 XAvier.

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Re: [gmx-users] oplsaa parametrization

2009-05-25 Thread Ran Friedman
R. A. wrote:
 Dear Users
 I m trying to simulate a structure (not a protein) which is not
 parametrized in oplsaa FF. I created the structure using PRODRG and
 included the results of *.itp from PRODRG to ffoplsaa.rtp file and
 tried to use available oplss_xxx for my atom type near to those ones
 already exists in *.atp. I also optimized my structure at RHF/6-31G*
 level and calculated the charge using resp. Then updated ffoplsaa.rtp
 using this calculated charge. By refering to the mailing list it seems
 that I need to modify bn.itp and nob.itp file as well (?!). I m just
 wonder if anybody use PRODRG how he/she parametrized FF. As I m new in
 GROMACS and any tutorial or procedure to follow will help me so much.
 Thank you in advance for any ideas or comments.
As far as I know PRODRG doesn't produce itp files comparable with OPLS,
so you need to use something else or manual modifications.

Ran.
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Re: [gmx-users] oplsaa parametrization

2009-05-25 Thread Ran Friedman
Hi Rosa,

You can read the paper on PRODRG to study how they parametrise.
There's a topology builder for OPLS-AA:
http://labmm.iq.ufrj.br/mktop/

There're also commercial tools (see some previous posts on the mailing
list) and you can also start with PRODRG and modify the files to have
the right parameters as in GMX.

However, you should verify that your molecules are correctly
parametrised no matter what software you're using - run a simulation
with it and see if things look all right (e.g., if rings are not too
distorted, bonds are correct etc.) and try to get experimental
parameters to compare with.

It has been stressed out a lot in the list that this is an advanced
issue - being familiar with MD and the FF you're using is a
pre-requisite to parametrisation.

Good luck,
Ran.

 Dear Ran

 Thanks for the reply. I think I `ve read some papers using PRODRG and
 opls. However they didnt mention clearly that how they parametrized
 their force field. Just do you know any alternative software. As I
 checked many softwares but I couldnt find any to create .itp file at
 the same time. Thank you.

 Regards
 Rosa

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Re: [gmx-users] Re: MD with RMSD restraint

2009-05-19 Thread Ran Friedman
Hi,
You can also use essential dynamics sampling.
Ran.

David van der Spoel wrote:
 Sam Moors wrote:
 Hi,

 Position restraints do not allow me to do what I want.
 For instance, I want to allow the system to freely explore the
 conformational space within a certain RMSD range, but not evolve
 beyond a specified RMSD cutoff.
 Another application would be to push the system conformation away
 from the reference structure, by using negative force constants.
 Therefore the reference structure should be fitted to the simulation
 structure (or the other way around) before calculating the position
 differences.

 Then you have to derive a force that is the derivative of the RMSD
 with respect to the positions. This may be difficult, since you have
 the superposition step in between.  What you could do straight away is
 move from normal RMSD to distance-based RMSD, in which case the this
 has been implemented using distance restraints. You would use genrestr
 to generate the additional topology input, then determine a suitable
 force constant and Bob's your uncle.

 Cheers.

 Thanks in advance for your help,
 Sam


 Mark Abraham wrote:
 Sam Moors wrote:
 Hi gmx users/developers,

 I would like to do a molecular dynamics simulation with a
 restraint on
 the backbone RMS deviation from a reference structure.
 Does anybody know if this is possible?

 How about position restraints only on the backbone? Same effect.


 Not exactly as you describe, but you should read the section in
 chapter
 4 of the manual and see for yourself.

 If yes, could you explain how to do it?
 If no, what would be the easiest way to implement this in gromacs?

 It could be done, but I'm not sure it's worth the effort.

 Mark
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Re: [gmx-users] different result for entropy with normal mode analysis and schlitter-approximation

2009-04-28 Thread Ran Friedman
Hi Oliver,

I think the eigenvalues in NMA are not the same (there used to be a
factor of 2PI and the mass weighting). Maybe you can try my script from
the user contributions and see if you get something more reasonable (use
to flag -n to indicate that your eigenvalues are from NMA).

Ran.

oliver.k...@uni-duisburg-essen.de wrote:
 Dear Gromacs Users,
 I'm trying to calculate entropies from a md trajectory using g_anaeig.
 There are two ways to go (question at bottom ;-):

 1. NMA and quasi-harmonic approximation: Use a bunch of snapshots (maybe
 5-20), minimize each of them to very low maximum forces, calculate the
 hessian matrix, diagonalize and use g_anaeig to calculate the entropy from
 the resulting eigenvector-matrix assuring that there are no negative
 eigenvalues in the eigenvectors 7 to N (first six eigenvectors will not be
 part of the calculation). - as follows:

 # Energy Minimization
 grompp_d -f em_nma.mdp -t md.fitted.trr -time $t -c md.gro -p protein.top
 -o $t.em.tpr
 mdrun_d -v -deffnm $t.em -table table6-12_4r_doublePrecision.xvg -tablep
 table6-12_4r_doublePrecision.xvg

 # Hessian Matrix
 grompp_d -f nma.mdp -t $t.em.trr -c md.gro -p protein.top -o $t.hessian.tpr
 mdrun_d -v -deffnm $t.hessian -table table6-12_4r_doublePrecision.xvg
 -tablep table6-12_4r_doublePrecision.xvg

 # Diagonalization of the Hessian
 g_nmeig_d -f $t.hessian.mtx -s $t.hessian.tpr -first 1 -last 1 -v
 $t.eigenvec.trr

 # Entropy calculation - vibrational (without first 6 modes)
 g_anaeig_d -v $t.eigenvec.trr -f $t.em.trr -s $t.hessian.tpr -temp 298.15
 -nevskip 6 -entropy 21 | tee out.anaeig.Svib.$t

 grep 'The Entropy due to the Quasi Harmonic approximation is'
 out.anaeig.Svib.$t | awk '{print $10}'  result/Svib.nma

 I use distance-dependent dielectric e=4r, but that doesn't make much
 difference.

 2. Schlitter approximation based on covariance: Use all snapshots of the
 md trajectory, calculate the covariance matrix (g_covar), - diagonalized
 matrix will be returned -, and subsequently calculate the entropy with
 g_anaeig. - as follows:

 # covariance matrix as time average over configurations
 g_covar_d -f md$i.trr -s md.gro -v md$i.eigenvec.trr -mwa -av
 average.$i.pdb -ascii covar.$i -xpm covar.$i -xpma covara.$i -l covar.$i
 -o md$i.eigenval.xvg - EOF
 0
 0
 EOF

 # Analysis of the principal components (and entropy calculation)
 g_anaeig -v md$i.eigenvec.trr -f md$i.trr -s md.gro -first 1 -last -1
 -entropy  out.anaeig.schlitter.$i

 grep 'The Entropy due to the Schlitter formula is' out.anaeig.schlitter.$i
 | awk '{print $9}'  result/Svib.schlitter

 Somebody before mentioned, he would like to have the undiagonalized
 covariance matrix as input for the entropy calculation, I think, that
 doesn't make a difference, am I right?

 So, practically, I tried to reproduce entropy from Schlitter 1993. A
 simulation of a deca-alanine-helix in vacuo in the old gmx force-field
 with vdw-cut-off etc. and I could reproduce the value of ca. 700
 kJoule/mol K with the Schlitter approximation.
 And now the question, why don't I get the same range of values when doing
 normal-mode analysis (as described above)?

 values of the Schlitter-approximation (for different simulation lengths):
 667.365
 685.594
 681.259
 680.269
 values given by the quasi-harmonic approximation when calculating from
 covariance:
 582.731
 596.97
 590.71
 589.07

 values from NMA and quasi-harmonic approximation (for 3 snapshots):
 21662.9
 21674.9
 21662.9

 So, there is a factor of round 30 between hessian- and covariance-based
 entropy!?

 I'm totally stuck with this.
 If anybody has experience with this phenomenon, any help is appreciated.
 Thanx in advance

 Oliver Kuhn







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Department of Biochemistry
University of Zurich
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CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: r.fried...@bioc.unizh.ch
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Re: [gmx-users] HF/6-31G** ESP derived charges to replace PRODRG assigned ones

2009-04-19 Thread Ran Friedman, Biochemisches Inst.

Dear Josmar,

As for the GROMOS FF, I've included a link to the paper describing the most 
recent (AFAIK) version of the FF in one of the recent mailing list massages.


Good luck,
Ran

On Sat, 18 Apr 2009 15:56:11 -0400
 Justin A. Lemkul jalem...@vt.edu wrote:



Josmar R. da Rocha wrote:

Dear Ran,

Thanks for answering and sorry to take so long to reply. After your 
response I went seach for more information about that. What I read here 
in the list is that some people uses antechamber to generate am1-bcc 
charges (or RESP charges using Gaussian program) and convert the output 
files to a .top file (using the amb2gmx.pl script) that can be used in 
gromacs, however, nobody says the kind of ff they intend to use that 
charges with. Do these type of charges can also be used with Gromos96 ff 
( 43a1)? Thanks in advance!




The amb2gmx was created to handle AMBER-to-GROMACS conversion.  It is 
unlikely that it would be useful for ffG43a1.  Since 43a1 is a united-atom 
force field, you have to compensate for the fact that nonpolar hydrogen 
atoms are absent. Furthermore, quantum charge calculation is not a 
necessary component of Gromos96 parameter derivation.  See, for example:


http://wiki.gromacs.org/index.php/Parameterization

-Justin


Regards,

Josmar Rocha

 

--- Em *sex, 27/3/09, Ran Friedman, Biochemisches Inst. 
/r.fried...@bioc.uzh.ch/* escreveu:


De: Ran Friedman, Biochemisches Inst. r.fried...@bioc.uzh.ch
Assunto: Re: [gmx-users] HF/6-31G** ESP derived charges to replace
PRODRG assigned ones
Para: bije...@yahoo.com.br, Discussion list for GROMACS users
gmx-users@gromacs.org
Data: Sexta-feira, 27 de Março de 2009, 17:35

Dear Josmar,

You haven't written which force field you plan to use. For OPLS and 
AMBER
QM-based optimisation should be fine. In Gromos, the FF was developed 
with the
aim of reproducing experimental results and I'm not sure if you can 
find a
better solution than examining other residues with the same chemical 
moieties or
use the same approach as reported in the relevant manuscripts. Some 
software
packages can also be used - these are mostly proprietary and not so 
easy to use.


Once you derive the parameters, it's a good idea to make some test 
runs of
the ligands and see if they behave as expected before you actually run 
a

simulation with the
 protein. For example, if a conjugate ring system isn't
planar something may be wrong in the setting.

There's no easy solution - this is why it's considered an advanced
topic. It is, however, very important. I've encountered a ligand that 
leaves
its binding site during a simulation due to wrong parameters (in this 
case, the
protonation of a protein side chain - FEBS  581, Pages 4120-4124, 
2007).


Hope that helped,
Ran

On Fri, 27 Mar 2009 12:22:01 -0700 (PDT)
 Josmar R. da Rocha bije...@yahoo.com.br wrote:
 Dear users,
 
 I have been reading some posts about using externally computed 
charges to
replace Prodrg charges at ligand topology files. Many users commented 
on the low

trustability given to Prodrg charges (e.g
http://www.mail-archive.com/gmx-users@gromacs.org/msg02360.html ;
http://www.mail-archive.com/gmx-users@gromacs.org/msg17351.html ). Dr. 
Verli

pointed out the
 use of semi-empirical methods such as RM1 in cases not involving
simulations with sulphate or phosphate groups (what is not my case) 
and the use
of QM methods with the 6-31G** basis set, for example, to obtain 
robust charges
(http://www.mail-archive.com/gmx-users@gromacs.org/msg03410.html). On 
the other
hand Dr. Mobley defined as a a bad idea to compute charges for an 
all-atom
case using QM and then try to convert these to a united atom force 
field.
Other users advice that the best charges are that compatible with the 
force

field parametrization
 (http://www.mail-archive.com/gmx-users@gromacs.org/msg10760.html ;
http://www.mail-archive.com/gmx-users@gromacs.org/msg08308.html), 
usually
pointing to http://wiki.gromacs.org/index.php/Parameterization. Dr 
Friedman
suggested that to calculate the electrostatic potential over the 
whole
molecule, and fit the atomic charges so that they reproduce this 
potential

in
 order to make it less sensitive to small changes in the geometry of 
the

molecule may give good results
(http://www.mail-archive.com/gmx-users@gromacs.org/msg08308.html). Dr. 
Lemkul
stressed the need for charges refinement to reproduce 
experimentally-observed

behavior while trying to use QM charges with Gromos ff. since
Parameterization under Gromos usually involves empirical derivation 
of

physical parameters, and free energy calculations using thermodynamic
integration. Few examples of protein-ligand studies using Gromacs and
Gromos96 ff that I have access (from literature) seem to treat it as 
take

Re: [gmx-users] the vdw and electrostatic energy

2009-04-16 Thread Ran Friedman
Hi,

This problem has been discussed for decades in the literature. There are
approaches such as PME and reaction field to deal with the long-range
electrostatics.

Ran.

Dechang Li wrote:
 Dear all, 

  When we do a MD simulation, we always set a cutoff 
 of non-bonded interactions, e.g. r=1.2 nm. When the 
 simulation finished, we can use the command 
 g_energy -f ener.edr -s ... to abtain the non-boned 
 energy of the system. My question is whether the non-bonded 
 energy values dependent on the non-bonded cutoff? If YES,
 there may be no problem of the vdw interaction (LJ-SR), 
 because the vdw interaction vanish in a short distance. But 
 how about the electrostatic term with the distance dependence
  of 1/r^2 ?



 Best regards,



 = 
 Dechang Li, Ph.D Candidate
 Department of Engineering Mechanics
 Tsinghua University
 Beijing 100084
 P.R. China 

 Tel:   +86-10-62773574(O) 
 Email: lidc02 at mails.tsinghua.edu.cn
 =

   

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-- 
--
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Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: r.fried...@bioc.unizh.ch
Skype: ran.friedman
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Re: [gmx-users] Re:Re: the vdw and electrostatic energy (Ran Friedman)

2009-04-16 Thread Ran Friedman
No. SR stands for short-range.
Ran.

   
   I did not mean that. I want to know that when we use g_energy in 
 Gromacs to 
 read the energy from the file ener.edr, does the cutoff affect the values
 of the energy? For example, when the cutoff is set to 1.2 nm and the PME 
 method
 is used, does the energy term Coul-SR read by g_energy contain the long 
 range
 part ?
   

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Re: [gmx-users] Topologies and charges for large organic ligands

2009-04-15 Thread Ran Friedman
Hi,

The answer is (or should be) in:

@article{Oostenbrink2004,
   Author = {Oostenbrink, C. and Villa, A. and Mark, A. E. and Van
Gunsteren, W. F.},
   Title = {A biomolecular force field based on the free enthalpy of
hydration and solvation: The GROMOS force-field parameter sets 53A5 and
53A6},
   Journal = {J. Comput. Chem.},
   Volume = {25},
   Pages = {1656-1676},
   Year = {2004} }

Good luck,
Ran.

Dean Cuebas wrote:
 Dear colleagues,

 In 53a6, the topology and charges for (NAD+) nicotinamide adenine
 dinucleotide are present (listed as NADH, 52 atoms) in polar hydrogen form
 (without aromatic hydrogens).

 Is there anyone who can tell me how such a molecule was charge group
 parameterized? (with sufficient certainty to be included in the ff).

 Please understand that I am not asking how to use the NAD topology that's
 provided.

 I've read that prodrg is a good starting point for parametrizing a ligand,
 but what is the path to improving such a ligand from that starting point?
 (the provided topology for NAD+ in the ff shows 17 charge groups with
 an average of 3-4 atoms per charge group, whereas prodrg gives only 11
 charge groups.)

 I'm not concerned about angles and dihedrals, since that is pretty
 painless... it's the charge groups that I'm concerned about.

 In a nutshell, who and how was the final NAD+ parameters decided upon??
 Does anyone know this??  Is it simply chemical intuition of estimated
 charges that reproduce the dipole of the moiety (like an adenine ring), and
 the charge groups contain the minimum number of atoms that reflect this?

 Is there an algorithm to generating improved charge groups?

 I ask these questions because my ligands are large organics... MW 800 and
 greater.

 Thanks for any and all help in this regard.

   

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Re: [gmx-users] HF/6-31G** ESP derived charges to replace PRODRG assigned ones

2009-04-01 Thread Ran Friedman, Biochemisches Inst.

Hi,

I've recently used OPLS-AA for a similar calculation. It has the advantage 
that many atom types are already defined in Gromacs and that QM-based 
calculations give you reasonable charges.


Note that it may take considerable simulation time (tens of ns) to 
discriminate between similar docked poses of the same molecule, though MD 
can give you a hint. If things were easier docking programs would do a 
better job.


Ran.

On Wed, 01 Apr 2009 00:12:31 -0600
 Lucio Ricardo Montero Valenzuela lucio...@ibt.unam.mx wrote:

So it 's better to switch to the OPLS forcefield if I want to compute the
charges?.
How can I implement the OPLS-UA if my gromacs (version 3.3) only includes 
the

OPLS-AA?
Mensaje citado por Justin A. Lemkul jalem...@vt.edu:




Lucio Montero wrote:
 How about MOPAC to calculate the charges for 3-methyladenine (this
 molecule has a charge +1) for using the G43a1 force field?.



That may not be a bad place to start, but any parameters applied to a 
Gromos

molecule have to reproduce condensed phase thermodynamic observables.
Empirical
fitting of the initial parameters may be required.  Refer to the primary
literature.  The reference for the 53a5 and 53a6 parameter sets are 
published

in
JCC, which may provide you with some useful information.

-Justin

 --
 From: Ran Friedman, Biochemisches Inst. r.fried...@bioc.uzh.ch
 Sent: Friday, March 27, 2009 2:35 PM
 To: bije...@yahoo.com.br; Discussion list for GROMACS users
 gmx-users@gromacs.org
 Subject: Re: [gmx-users] HF/6-31G** ESP derived charges to replace
 PRODRGassignedones

 Dear Josmar,

 You haven't written which force field you plan to use. For OPLS and
 AMBER QM-based optimisation should be fine. In Gromos, the FF was
 developed with the aim of reproducing experimental results and I'm not
 sure if you can find a better solution than examining other residues
 with the same chemical moieties or use the same approach as reported
 in the relevant manuscripts. Some software packages can also be used -
 these are mostly proprietary and not so easy to use.

 Once you derive the parameters, it's a good idea to make some test
 runs of the ligands and see if they behave as expected before you
 actually run a simulation with the protein. For example, if a
 conjugate ring system isn't planar something may be wrong in the 
setting.


 There's no easy solution - this is why it's considered an advanced
 topic. It is, however, very important. I've encountered a ligand that
 leaves its binding site during a simulation due to wrong parameters
 (in this case, the protonation of a protein side chain - FEBS  581,
 Pages 4120-4124, 2007).

 Hope that helped,
 Ran

 On Fri, 27 Mar 2009 12:22:01 -0700 (PDT)
  Josmar R. da Rocha bije...@yahoo.com.br wrote:
 Dear users,

 I have been reading some posts about using externally computed
 charges to replace Prodrg charges at ligand topology files. Many
 users commented on the low trustability given to Prodrg charges (e.g
 http://www.mail-archive.com/gmx-users@gromacs.org/msg02360.html ;
 http://www.mail-archive.com/gmx-users@gromacs.org/msg17351.html ).
 Dr. Verli pointed out the use of semi-empirical methods such as RM1
 in cases not involving simulations with sulphate or phosphate groups
 (what is not my case) and the use of QM methods with the 6-31G**
 basis set, for example, to obtain robust charges
 (http://www.mail-archive.com/gmx-users@gromacs.org/msg03410.html). On
 the other hand Dr. Mobley defined as a a bad idea to compute charges
 for an all-atom case using QM and then try to convert these to a
 united atom force field. Other users advice that the best charges
 are that compatible with the force field parametrization
 (http://www.mail-archive.com/gmx-users@gromacs.org/msg10760.html ;
 http://www.mail-archive.com/gmx-users@gromacs.org/msg08308.html),
 usually pointing to
 http://wiki.gromacs.org/index.php/Parameterization. Dr Friedman
 suggested that to calculate the electrostatic potential over the
 whole molecule, and fit the atomic charges so that they reproduce
 this potential in order to make it less sensitive to small changes
 in the geometry of the molecule may give good results
 (http://www.mail-archive.com/gmx-users@gromacs.org/msg08308.html).
 Dr. Lemkul stressed the need for charges refinement to reproduce
 experimentally-observed behavior while trying to use QM charges with
 Gromos ff. since Parameterization under Gromos usually involves
 empirical derivation of physical parameters, and free energy
 calculations using thermodynamic integration. Few examples of
 protein-ligand studies using Gromacs and Gromos96 ff that I have
 access (from literature) seem to treat it as take it for granted
 issue (any reference with a more detailed description would be
 welcome :-)). Despite reading on this topic I could not compile all
 the information in a clear and objective way (may be because I'm in
 the wrong track). Let ask you some question

Re: [gmx-users] HF/6-31G** ESP derived charges to replace PRODRG assigned ones

2009-03-27 Thread Ran Friedman, Biochemisches Inst.

Dear Josmar,

You haven't written which force field you plan to use. For OPLS and AMBER 
QM-based optimisation should be fine. In Gromos, the FF was developed with 
the aim of reproducing experimental results and I'm not sure if you can find 
a better solution than examining other residues with the same chemical 
moieties or use the same approach as reported in the relevant manuscripts. 
Some software packages can also be used - these are mostly proprietary and 
not so easy to use.


Once you derive the parameters, it's a good idea to make some test runs of 
the ligands and see if they behave as expected before you actually run a 
simulation with the protein. For example, if a conjugate ring system isn't 
planar something may be wrong in the setting.


There's no easy solution - this is why it's considered an advanced topic. It 
is, however, very important. I've encountered a ligand that leaves its 
binding site during a simulation due to wrong parameters (in this case, the 
protonation of a protein side chain - FEBS  581, Pages 4120-4124, 2007).


Hope that helped,
Ran

On Fri, 27 Mar 2009 12:22:01 -0700 (PDT)
 Josmar R. da Rocha bije...@yahoo.com.br wrote:

Dear users,

I have been reading some posts about using externally computed charges to 
replace Prodrg charges at ligand topology files. Many users commented on 
the low trustability given to Prodrg charges (e.g 
http://www.mail-archive.com/gmx-users@gromacs.org/msg02360.html ; 
http://www.mail-archive.com/gmx-users@gromacs.org/msg17351.html ). Dr. 
Verli pointed out the use of semi-empirical methods such as RM1 in cases 
not involving simulations with sulphate or phosphate groups (what is not my 
case) and the use of QM methods with the 6-31G** basis set, for example, to 
obtain robust charges 
(http://www.mail-archive.com/gmx-users@gromacs.org/msg03410.html). On the 
other hand Dr. Mobley defined as a a bad idea to compute charges for an 
all-atom case using QM and then try to convert these to a united atom force 
field. Other users advice that the best charges are that compatible with 
the force field parametrization
(http://www.mail-archive.com/gmx-users@gromacs.org/msg10760.html ; 
http://www.mail-archive.com/gmx-users@gromacs.org/msg08308.html), usually 
pointing to http://wiki.gromacs.org/index.php/Parameterization. Dr Friedman 
suggested that to calculate the electrostatic potential over the whole 
molecule, and fit the atomic charges so that they reproduce this potential 
in order to make it less sensitive to small changes in the geometry of the 
molecule may give good results 
(http://www.mail-archive.com/gmx-users@gromacs.org/msg08308.html). Dr. 
Lemkul stressed the need for charges refinement to reproduce 
experimentally-observed behavior while trying to use QM charges with Gromos 
ff. since Parameterization under Gromos usually involves empirical 
derivation of physical parameters, and free energy calculations using 
thermodynamic integration. 
Few examples of protein-ligand studies using Gromacs and Gromos96 ff that I 
have access (from literature) seem to treat it as take it for granted 
issue (any reference with a more detailed description would be welcome 
:-)). Despite reading on this topic I could not compile all the information 
in a clear and objective way (may be because I'm in the wrong track). Let 
ask you some question that I find would help me to make my ideas more 
clear:



1-am I overestimating the importance of ligand charges in such a simple 
study of protein-small molecule (containg charged Phosphate groups) 
complex? or


1.1-The only way to test for this is doing many different simulation on 
the same system using different type of computed charges to see what 
happen?


2-How could I try to choose a method to obtain reasonable charges based on 
the reproduction of experimentally-observed behavior if I do not have 
experimental data for my system?


3-I also would like to know from users dealing with protein-ligand 
interactions studies what do you consider a good approach to address this 
problem?


Based on what I read I'd have a tendency to use HF/6-31G** ESP derived 
charges (with necessary changes as to make it united-atom charges and 
scaling that to a integer number for each group). Please, let me know if 
that strategy would be as good as a disaster! 


Thank you very much for the attention.


Josmar Rocha



 Veja quais são os assuntos do momento no Yahoo! +Buscados
http://br.maisbuscados.yahoo.com




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Re: [gmx-users] Using R.E.D. charges with OPLS AA

2009-03-26 Thread Ran Friedman
Hi,

HF with 6-31G usually provide a good start for getting OPLS charges:
@article{Jorgensen1996,
   Author = {Jorgensen, W. L.  and Maxwell, D. S. and Tirado-Rives, J.},
   Title = {Development and Testing of the {O}{P}{L}{S} All-Atom Force
Field on
Conformational Energetics and Properties of Organic Liquids.},
   Journal = {J Am Chem Soc},
   Volume = {118},
   Pages = {11225-11236},
 Year = {1996} }

How you assign your charges to the molecule is another issue. I normally
fit the partial charges to the electrostatic potential around the
molecule. RESP was indeed developed with AMBER, but I don't know if the
charges are so different.

Good luck,
Ran

DimitryASuplatov wrote:
 Hello,

 I need to simulate a protein with deprotonated Tyr (HH hydrogen should
 be off). I used R.E.D. approach with PCGAMESS and RESP to calculate the
 charges. 

 1/ The problem is that to my understanding RESP charges apply to AMBER
 only. Am I correct?

 2/ Can I use R.E.D. charges with OPLS AA?

 3/ If not how can I recalculate them to fit the OPLS AA?

 4/ Any Tyr-Deprot topology already available??? 

 Thanks, I appreciate your time.
 SDA

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-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: r.fried...@bioc.unizh.ch
Skype: ran.friedman
--

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[gmx-users] Re: g_covar

2009-03-26 Thread Ran Friedman
Dear Dagoberto,

Choosing the right protein structure (and also which part of the protein
to align) depends a lot of your system. I wouldn't use an average
structure for a system that's changing a lot, because it may not be
representative. It's hard to provide a more elaborate answer without
many details about your system and what you're trying to simulate. It
can be helpful to read both on the methods of covariance analysis and on
some implementation - i.e., papers in which it has been used to
calculate correlated motion.

As to modification of the code, I found it easiest to compile the source
code for various tools within GMX. It's not necessary, but it makes your
life easier.

Since your question doesn't refer to the modified g_covar code directly,
I'm ccing the gromacs mailing list. Please keep future correspondence there.

Good luck,
Ran

darme...@ibt.unam.mx wrote:
 Dear Ran friedman

 I'm actually biochemistry student and I'm using your uploaded version of 
 g_covar
 in order to calculate correlated motion. I have c-alpha trajectory of 50 ns
 simulation that describe the functional movement of my protein, but the
 trajectory are not in the equilibrium. My questions are,  what reference
 structure I must use in order to calculate correlated motion?, could I use the
 average structure as reference?

 In the other hand, Im doing some modifications to the g_covar program and I 
 want
 to know the way to compile it. Is necessary to compile within gromacs?   What 
 is
 the easiest way?

 I would appreciate any help in this matter.

 Dagoberto Armenta Medina



 
 Este mensaje fue enviado desde el servidor Webmail del Instituto de 
 Biotecnologia.

   

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Re: [gmx-users] gromacs 4 mpi weirdness

2009-03-17 Thread Ran Friedman
 shared libraries... yes
 checking whether to build shared libraries... no
 checking whether to build static libraries... yes
 configure: creating libtool
 appending configuration tag CXX to libtool
 appending configuration tag F77 to libtool
 checking for special C compiler options needed for large files... no
 checking for _FILE_OFFSET_BITS value needed for large files... 64
 checking for _LARGEFILE_SOURCE value needed for large files... 1
 checking for sqrt in -lm... yes
 checking for fftw3.h... yes
 checking for main in -lfftw3f... yes
 checking rpc/rpc.h usability... yes
 checking rpc/rpc.h presence... yes
 checking for rpc/rpc.h... yes
 checking for rpc/xdr.h... yes
 checking for xdr_float in -lnsl... yes
 checking for working memcmp... yes
 checking return type of signal handlers... void
 checking for off_t... (cached) yes
 checking for vprintf... yes
 checking for _doprnt... no
 checking if malloc debugging is wanted... no
 checking for strcasecmp... yes
 checking for strdup... yes
 checking for bool... no
 checking for X... libraries , headers
 checking for gethostbyname... yes
 checking for connect... yes
 checking for remove... yes
 checking for shmat... yes
 checking for IceConnectionNumber in -lICE... yes
 checking libxml/parser.h usability... yes
 checking libxml/parser.h presence... yes
 checking for libxml/parser.h... yes
 checking for main in -lxml2... yes
 checking limits.h usability... yes
 checking limits.h presence... yes
 checking for limits.h... yes
 checking for strings.h... (cached) yes
 checking for unistd.h... (cached) yes
 checking for unistd.h... (cached) yes
 checking for an ANSI C-conforming const... yes
 checking for size_t... yes
 checking whether struct tm is in sys/time.h or time.h... time.h
 checking for uid_t in sys/types.h... yes
 checking for inline... inline
 checking whether your compiler can handle assembly files (*.s)... yes
 checking whether as fully supports ia32 SSE... yes
 checking whether as fully supports ia32 3DNow! instructions... yes
 checking whether byte ordering is bigendian... (cached) no
 checking if the compiler supports gcc inline assembly... yes
 checking if the compiler supports MSVC inline assembly... no
 configure: creating ./config.status
 config.status: creating Makefile
 config.status: creating src/Makefile
 config.status: creating src/gmxlib/Makefile
 config.status: creating src/gmxlib/gmx_blas/Makefile
 config.status: creating src/gmxlib/gmx_lapack/Makefile
 config.status: creating src/gmxlib/nonbonded/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel_ia32_3dnow/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel_ia32_sse/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel_ia32_sse2/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel_x86_64_sse/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel_x86_64_sse2/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel_ppc_altivec/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel_ia64_single/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel_ia64_double/Makefile
 config.status: creating src/gmxlib/nonbonded/nb_kernel_bluegene/Makefile
 config.status: creating include/Makefile
 config.status: creating include/types/Makefile
 config.status: creating src/mdlib/Makefile
 config.status: creating src/kernel/Makefile
 config.status: creating src/tools/Makefile
 config.status: creating src/ngmx/Makefile
 config.status: creating src/contrib/Makefile
 config.status: creating scripts/Makefile
 config.status: creating admin/Makefile
 config.status: creating share/Makefile
 config.status: creating share/tutor/Makefile
 config.status: creating share/tutor/gmxdemo/Makefile
 config.status: creating share/tutor/nmr1/Makefile
 config.status: creating share/tutor/nmr2/Makefile
 config.status: creating share/tutor/water/Makefile
 config.status: creating share/tutor/mixed/Makefile
 config.status: creating share/tutor/methanol/Makefile
 config.status: creating share/tutor/speptide/Makefile
 config.status: creating share/template/Makefile
 config.status: creating share/top/Makefile
 config.status: creating share/html/Makefile
 config.status: creating share/html/images/Makefile
 config.status: creating share/html/online/Makefile
 config.status: creating man/Makefile
 config.status: creating man/man1/Makefile
 config.status: creating src/config.h
 config.status: executing depfiles commands

 * On most platforms you can save 10X space with dynamic libraries, although
   the binaries might be less portable. Why not try --enable-shared ?


   


-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: r.fried...@bioc.unizh.ch
Skype: ran.friedman

Re: [gmx-users] initial velocities Langevin dynamics

2009-03-11 Thread Ran Friedman
Hi Loris,

It may be better to have ld_seed=-1. This way, you won't have the same
seed again when you restart.

@Article{Cerutti2008,
author = Cerutti, D S and Duke, R and Freddolino, P L and Fan, H and
Lybrand, T P,
title = {Vulnerability in Popular Molecular Dynamics Packages Concerning
Langevin and Andersen Dynamics},
journal = J Chem Theory Comput,
year = 2008,
volume = 4,
pages = 1669-1680
}

Best regards,
Ran

Loris Moretti wrote:
 Dear Mark and Oscar, 

 Thanks for your help!
 I checked the velocity distribution and the velocity at different simulation 
 frames. As you said the initial velocities are all set to zero and at the 
 next step are already changed, I also guess by the random thermal noise.

 Thus, my idea of simulating the same system with different random generator 
 number for thermal noise (ld_seed) might account for a small variation of the 
 initial conditions? 

 loris...


 In message 8c3f24a40903110611j4f69c75emb0f5eef0484de...@mail.gmail.com 
 Discussion list for GROMACS users gmx-users@gromacs.org writes:
   
 Thus I am a bit confused about it!
   
 I'm confused about the manual comment about only being meaningful with the
 MD integrator, but we 'll have to wait until someone who knows something
 about LD can post!
   
 For LD, the velocities will (should) get rescaled by the random thermal
 noise, that is- by the Langivin thermostat.
 With MD, the thermostat works like friction (positive or negative friction).
 So you see, that for LD, an initial velocity of zero should next be changed
 by the thermostat, while for MD the rescaling shouldn't work for zero.

 --Omer Markovitch.

 Koby Levy research group,
 Weizmann Institute of Science.
 http://www.weizmann.ac.il/sb/faculty_pages/Levy/
 
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-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: r.fried...@bioc.unizh.ch
Skype: ran.friedman
--

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Re: [gmx-users] Conversion of trajectories to netcdf format

2009-02-25 Thread Ran Friedman
I don't know about netcdf, but you can use wordom to convert from xtc to
dcd.
Contact me off list if you don't succeed - I'm not sure whether the
online documentation of wordom is up-to-date.

Ran.

Tobias Unruh wrote:
 Hi,

 I would like to use nMolDyn for the analysis of the GROMACS trajectories.

 I tried VMD and catdcd to convert trr/tpr files to dcd/pdb files. But the
 conversion of the dcd/pdb files to nc (netcdf) files using the dcd_to_nc
 program of the nMolDyn package does not work. Obviously the header of the
 dcd file differs from what is expected by the dcd_to_nc program which
 uses
 MMTK.

 Does anyone know how to convert the GROMACS trajectories such that
 nMolDyn can be used for calculation of correlation and intermediate
 scattering functions?

 I appreciate any suggestion.

 Regards Tobias

 -- 
 Tobias Unruh
 TU Muenchen, FRM-II
 85747 Garching, Germany
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-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: r.fried...@bioc.unizh.ch
Skype: ran.friedman
--

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Re: [gmx-users] gromacs 4.0.3 tests validations

2009-02-12 Thread Ran Friedman
Hi,
I think the tests for pdb2gmx are outdated. Most fail due to warning(s)
while running grompp, which were allowed with older versions.
I'm not sure who maintains this tests - maybe a new version is due.
Ran.

Tru Huynh wrote:
 Hi,

 I am compiling gromacs on CentOS-3 x86_64 both serial and LAM-MPI version
 (7.1.4) and I would like to validate the builds.

 [...@sillage gmxtest]$ rpm -q gcc fftw3 perl
 gcc-3.2.3-59.x86_64
 fftw3-3.0.1-2_centos3.x86_64
 perl-5.8.0-98.EL3.x86_64

 ./configure --prefix=... --with-x --enable-shared
 make  make install

 test validation as stated at http://wiki.gromacs.org/index.php/Test-set
 wget -O - ftp://ftp.gromacs.org/pub/tests/gmxtest-3.3.2.tgz| tar xzvf -
 make tests 
 ...
 All 16 simple tests PASSED
 All 14 complex tests PASSED
 All 63 kernel tests PASSED
 Error not all 45 pdb2gmx tests have been done successfully
 Only 0 energies in the log file

 - The PASSED lines are fine to me, but what about the last 2 lines?

 I also compiled the double precision version with:
 ./configure --prefix=... --with-x --enable-shared --disable-float
 and the tests yields:

 [...@sillage gmxtest]$ ./gmxtest.pl -double all
 All 16 simple tests PASSED
 All 14 complex tests PASSED
 All 63 kernel tests PASSED
 readline() on closed filehandle PIPE at ./gmxtest.pl line 343.
 readline() on closed filehandle PIPE at ./gmxtest.pl line 348.
 ...
 readline() on closed filehandle PIPE at ./gmxtest.pl line 348.
 readline() on closed filehandle PIPE at ./gmxtest.pl line 343.
 readline() on closed filehandle PIPE at ./gmxtest.pl line 348.
 Error not all 45 pdb2gmx tests have been done successfully
 Only 0 energies in the log file

 Should I be worried?

 About the parallel test (grompp -np N for gromacs 3.x) as previoulsy stated 
 on the
 mailing list, one should use:
 grompp -c system.gro -p topology.top -f something.mdp
 mpirun -np N mdrun

 so 
 gmxtest.pl should read:
 system($grompp -maxwarn 10 $ndx  /dev/null  21);
 system(mpirun -$par mdrun -maxwarn 10 $ndx   grompp.out 21);

 instead of:
 system($grompp -maxwarn 10 $ndx $par  grompp.out 21);

 [...@sillage gmxtest]$ ./gmxtest.pl -np 1 all
 Will test on 1 processors
 All 16 simple tests PASSED
 All 14 complex tests PASSED
 All 63 kernel tests PASSED
 Error not all 45 pdb2gmx tests have been done successfully
 Only 0 energies in the log file

 [...@sillage gmxtest]$ ./gmxtest.pl -np 2 all
 Will test on 2 processors
 FAILED. Check files in bham
 1 out of 16 simple tests FAILED
 FAILED. Check files in acetonitrilRF
 FAILED. Check files in aminoacids
 FAILED. Check files in argon
 FAILED. Check files in sw
 FAILED. Check files in tip4p
 FAILED. Check files in urea
 FAILED. Check files in water
 7 out of 14 complex tests FAILED
 All 63 kernel tests PASSED
 Error not all 45 pdb2gmx tests have been done successfully
 Only 0 energies in the log file

 Thanks.

 Tru
   

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Re: [gmx-users] Barostat Density decreasing to zero

2009-02-11 Thread Ran Friedman
Hi Omer,
You use a  dielectric constant is 80, which means that the electrostatic
interactions are screened. Perhaps that's why your density is low.
Ran.

Omer Markovitch wrote:
 Dear All,
 I have simulated a protein inside a box with water and ions. I began
 by minimizing my system (which has a total charge of zero), until the
 maximum gradient was small enough and the potential energy become
 negative.
 Then I heated it, slowly, to 300K at constant volume (using berendsen
 thermostat and tcoupl = 1 ps).
 Then I performed 500 ps NVT simulation to equilibrate the temperature,
 at 300K.
 Then, I tried to equilibrate the pressure and run NPT simulation,
 using Berendsen barostat (p=1, pcoupl=10) and Berendsen thermostat
 (T=300K, tcoupl = 0.1).

 My problem is, that with the barostat  thermostat both active in the
 same MD run, my density drops to a very low value (at the first MD
 steps, the density is 1000, dropping later to 100 kg/m^3). That is- my
 box dimensions increase significantly (from around 6x6x6 to 12x12x12
 nm^3. If I change the pressure coupling constant, the speed of the
 expansion changes but all simulation converged to a small density
 between 50-100 kg/m3.

 Your help is appreciated; Probably, I am not controlling the
 simulation like I should. I will appreciate any advice.
 Thank you, Omer Markovitch.

 I have used gromacs version 3.3.3, Here is my .MDP file for the NPT run:

 integrator   = md
 dt   = 0.001
 nsteps   = 50
 comm_grps= system
 nstxout  = 500
 nstvout  = 500
 nstcheckpoint= 1000
 nstlog   = 500
 nstenergy= 500
 nstlist  = 10
 ns_type  = simple
 pbc  = xyz
 rlist= 1.0
 coulombtype  = PME
 rcoulomb-switch  = 0
 rcoulomb = 1.0
 epsilon_r= 80
 epsilon_rf   = 80
 vdw-type = Cut-off
 rvdw-switch  = 0
 rvdw = 1.0
 table-extension  = 1
 fourierspacing   = 0.12
 pme_order= 4
 ewald_rtol   = 1e-05
 ewald_geometry   = 3d
 optimize_fft = yes
 tcoupl   = berendsen
 tc-grps  = system
 tau_t= 0.1
 ref_t= 300
 Pcoupl   = berendsen
 Pcoupltype   = Isotropic
 tau-p= 10
 compressibility  = 4.5E-5
 ref-p= 1
 andersen_seed= 815131
 constraints  = none

 

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Re: [gmx-users] micelle disaggregated in serial, but not parallel, runs using sd integrator

2009-02-05 Thread Ran Friedman
Hi,
Maybe it's a good idea to have ld-seed=-1 as a default if that's not
already the case.
Ran.

Berk Hess wrote:
 Hi,

 I don't know why I did not add checks for ld-seed before.
 Now grompp gives a note when continutation=yes and ld-seed!=-1.

 tpbconv will now generate a new ld-seed when reading a trajectory
 (but you should not use tpbconv, use a checkpoint file instead).

 But yesterday I forgot to tell that there is a bug in the checkpointing
 of mdrun in 4.0 - 4.0.3. Without domain decomposition the initial box
 size would always be stored in the checkpoint file, which causes problems
 with NPT simulations. NPT simulations with domain decomposition and
 all NVT simulations were fine.

 Gromacs 4.0.4 will all bugs fixed and extra checks should be released
 today.

 Berk

  Date: Wed, 4 Feb 2009 19:30:47 -0500
  From: chris.ne...@utoronto.ca
  To: gmx-users@gromacs.org
  Subject: [gmx-users] micelle disaggregated in serial, but not
 parallel, runs using sd integrator
 
  It appears as if you were correct Berk. I will report on the results
 of my 24h test tomorrow, but I also set up another system
  that used ld_seed=1993 and ran in 20 ps segments instead of the 200
 ps segments that I was previously using. This system shows
  signs of disaggregation on the 200 ps time-scale as opposed to the 2
 ns time-scale that I observed for 200 ps segments.
 
  I don't know how you figured that one out, but I am very grateful.
 
  Now that I see the trajectories, it does make sense that any net
 movement applied to an individual molecule by the noise will
  lead to directed movement over many separate segments.
 
  I think this is probably worth a note in the grompp output for sd
 runs when a user sets ld_seed to something other than -1 and
  utilizes the -t option (or some other indication that this is
 intended as a continuation).
 
  Chris.
 
  -- original message --
 
  Thank you Berk,
 
  I will repeat my runs using the checkpoint file and report my
 findings back to this list. Thank you for this advice.
 
  Chris.
 
  -- original message --
 
  Hi,
 
  In this manner you use the same random seed and thus noise for all
 parts.
  In most cases this will not lead to serious artifacts with SD,
  but you can never be sure.
  When checkpoints are used, you do not repeat random numbers.
  This also gives a difference between serial and parallel in 4.0.
  With serial you get exactly the same noise per atom, in parallel not,
  since atoms migrate from one node to another (with domain decompostion).
 
  If you do not use checkpoints, use ld_seed=-1 and do not use tpbconv.
 
  Berk
 
 
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Re: [gmx-users] micelle disaggregated in serial, but not parallel, runs using sd integrator

2009-02-05 Thread Ran Friedman
Berk Hess wrote:
 Hi,

 That I have thought about and it would avoid a lot of trouble.
 But I have not done that, because that would lead to different run results
 every time you rerun grompp, which can be misleading when you are
 trying to assess the effects of other parameters.

 But maybe the first issue is more important than the second?
That's how I feel. Many users may not be aware of potential artefacts.

Ran.

 Berk

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Re: [gmx-users] Transition difficulties: version 3.3.3 to 4.0.3 regarding pull_geometry=distance

2009-01-27 Thread Ran Friedman
Dear Berk,

I think that g_clustsize has a similar problem. IIRC I fixed it in a
similar way on my own copy.
There are probably other tools that will suffer from this as well, but
for g_clustsize it's important because it may deal with such groups.

Same goes for trjconv, e.g., for a protein and ligand.

Ran.

Berk Hess wrote:
 Hi,

 Just to be sure, the pull code is producing the correct results now?
 The only problems should be in several analysis tools.

 The analysis tools have been written only with analysis of molecules
 or parts of molecules in mind. When you want to analyze groups
 that cover two molecules or more there will be pbc problems.
 These are not simple to fix. If the distances between all the atoms
 in the group are less than half a box length there is a unique COM.
 The procedure should be similar to what trjconv -pbc cluster does.

 I can try to implement this for g_traj and g_dist.
 Are there other tools that cause problems?

 Berk

  Date: Mon, 26 Jan 2009 17:46:26 -0500
  From: fied...@umich.edu
  To: gmx-users@gromacs.org
  Subject: Re: [gmx-users] Transition difficulties: version 3.3.3 to
 4.0.3 regarding pull_geometry=distance
 
  Hi Chris,
 
  Your suggestions were helpful. Due to the nature of this problem, there
  were limitations in the application of the sequence of steps that you
  recommended. Specifically, the difference in the equilibrated structure
  from version 3.3.x to the calculated reference center of mass from
  version 4.0.x causes an unreasonable jump with constraint force
  calculation. Resultant bad contacts prohibit generation of a pull
  output file.
 
  More generally though, I believe I understand your broader point: the
  sensitive nature of the periodic box with respect to the pull code and
  possible discrepancies in the pbc treatment by various utilities, may
  cause confusion with the diagnostic process. The test bilayer system I
  created however, centered distantly from the x and y box edges, may
  effectively remove this set of concerns. For example, this
  configuration is relatively unchanged upon recentering, however it is
  still susceptible to the problem that is the subject of this discussion.
 
  If I can reproduce this phenomenon with a publicly available topology
  file, I can provide the necessary input files for inspection.
 
  Thank you again,
 
  Steve Fiedler
 
 
 
  chris.ne...@utoronto.ca wrote:
   Hi Steve,
  
   what I intended to suggest was actually something different (and much
   easier).
  
   The idea is not that you need some special system to be able to
   utilize the pull code, but that the pull code is correct whereas the
   g_dist and g_traj programs are not as good at treating pbc in the way
   that one desires.
  
   I suggest the following.
  
   1. Take your original system and run the pull code for a very short
   simulation. Use the last line of the output to calculate the relevant
   displacement
  
   2. Now use trjconv -b -e to get the last frame of the .xtc that
   resulted from that short MD run as a .gro file, call it final.gro. I
   suspect that your groups are not entirely in the same simulation box
   in final.gro.
  
   3. Now make a new .ndx file from that .gro and give it a single
   residue that is near your binding pocket, call it R_1
  
   4. Now apply trjconv -center -pbc mol -ur compact while selecting R_1
   for centering, call the new .gro file final_center.gro
  
   5. Visualize final_center.gro and ensure that all of your relevant
   atoms are in the same image in the way that puts the minimum distance
   between them along a path that is entirely contained within the unit
   cell. If not, go back to step 3 and try making a group R_2, etc.
   until this process works. NOTE: you might think that giving trjconv
   -center the relevant groups that you use for pulling will be a good
   idea here, but it is not. The problem there is that the atoms may be
   centered by placing half on the left boundary and half on the right
   boundary. I find using one logically selected residue or atom is the
   best method here.
  
   6. Assuming that you got what you wanted in step 5, now run g_traj
 and
   g_dist on final_center.gro. In my case, I found that g_traj and
 g_dist
   give the same answer as the pull code output when I am using
   final_center.gro, but not always when I am using final.gro.
  
   *** I always laugh when these problems arise because, in an important
   sense, the protein *did* jump out of the simulation box... at
 least as
   far as g_traj and g_dist are concerned. This, we must hope, is
   correctly treated in the pull code even though it is incorrectly (or
   at least unintuitively) treated by g_traj and g_dist.
  
   Chris.
  
   -- original message --
  
   Hi,
  
   Thank you Berk and Chris for the suggestions.
  
   To address the possibility that this issue is related to periodic
   boundaries, I used two approaches:
   1. The pull group of interest (permeant) was centered in 

Re: [gmx-users] g_clustsize

2009-01-19 Thread Ran Friedman
Hi,
Use -n without -mol. Clustering will be atom based.

Good luck,
Ran.

Vitaly Chaban wrote:
 Hi GMX Colleagues,

 I need a little clarification.

 I try to calculate a distribution of clusters of ions in a system with
 several cations and anions and a few solvent molecules. So I just need
 a number of cluster consisting of ions and the size of the each (how many
 ions the cluster includes).

 To do this I use
 g_clustsize(402) -n index.ndx -mol -s topol.tpr
 where index.ndx contains only the number of the atoms of the ions.

 but the programme outputs:
 Back Off! I just backed up temp.xvg to ./#temp.xvg.1#
 Reading frame   0 time0.000   Reading file topol.tpr, VERSION 4.0.2 
 (single precision)
 Reading file topol.tpr, VERSION 4.0.2 (single precision)
 Using molecules rather than atoms. Not reading index file index.ndx

 Why does it not read the index file with the atom number I want to
 cluster?


 When I see for example histo-clust.xvg:

 @title Cluster size distribution
 @xaxis  label Cluster size
 @yaxis  label ()
 @TYPE xy
 0 0.000
 119.531
 2 4.583
 3 1.707
 4 0.647
 5 0.259
 6 0.060
 7 0.140
 8 0.048
 9 0.054
10 0.020
11 0.022
12 0.000
 
 
 
   57731.096
   57833.457
   57936.982
   58028.942
   58131.311
   58234.850
   58338.401
   58430.307


 It looks like all the atoms in the system were used to find clusters.

 And maxclust.xvg:

 @title Max cluster size
 @xaxis  label Time (ps)
 @yaxis  label #molecules
 @TYPE xy
   0.00e+00 577
   1.00e-01 576
   2.00e-01 565
   3.00e-01 550
   4.00e-01 567
   5.00e-01 572
   6.00e-01 566
   7.00e-01 578
   8.00e-01 567
   9.00e-01 565
   1.00e+00 563
   1.10e+00 579
   1.20e+00 566



 Please anybody let me know how to find clusters only among those
 particles I point out in the index file. So I need only the clusters
 consisting of ions but solvent is not of interest in my case.


 Thank you in advance,
 Vitaly



 ===
 Vitaly V. Chaban, Ph.D.(ABD)
 School of Chemistry
 V.N. Karazin Kharkiv National University
 Svoboda sq.,4, Kharkiv 61077, Ukraine
 email: cha...@univer.kharkov.ua,vvcha...@gmail.com
 skype: vvchaban, mob.: +38-097-8259698


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--
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Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: r.fried...@bioc.unizh.ch
Skype: ran.friedman
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Re: [gmx-users] g_clustsize

2009-01-19 Thread Ran Friedman
Vitaly Chaban wrote:
 Hi Ran,

 I will try your advice. And for what purpose should '-mol' be used?
   
To cluster molecules.
In this case, you topology is read from the .tpr file and all of the
molecules there are taken into account for clustering.
 Vitaly


 RF Hi,
 RF Use -n without -mol. Clustering will be atom based.

 RF Good luck,
 RF Ran.

 RF Vitaly Chaban wrote:
   
 Hi GMX Colleagues,

 I need a little clarification.

 I try to calculate a distribution of clusters of ions in a system with
 several cations and anions and a few solvent molecules. So I just need
 a number of cluster consisting of ions and the size of the each (how many
 ions the cluster includes).

 To do this I use
 g_clustsize(402) -n index.ndx -mol -s topol.tpr
 where index.ndx contains only the number of the atoms of the ions.

 but the programme outputs:
 Back Off! I just backed up temp.xvg to ./#temp.xvg.1#
 Reading frame   0 time0.000   Reading file topol.tpr, VERSION 4.0.2 
 (single precision)
 Reading file topol.tpr, VERSION 4.0.2 (single precision)
 Using molecules rather than atoms. Not reading index file index.ndx

 Why does it not read the index file with the atom number I want to
 cluster?


 When I see for example histo-clust.xvg:

 @title Cluster size distribution
 @xaxis  label Cluster size
 @yaxis  label ()
 @TYPE xy
 0 0.000
 119.531
 2 4.583
 3 1.707
 4 0.647
 5 0.259
 6 0.060
 7 0.140
 8 0.048
 9 0.054
10 0.020
11 0.022
12 0.000
 
 
 
   57731.096
   57833.457
   57936.982
   58028.942
   58131.311
   58234.850
   58338.401
   58430.307


 It looks like all the atoms in the system were used to find clusters.

 And maxclust.xvg:

 @title Max cluster size
 @xaxis  label Time (ps)
 @yaxis  label #molecules
 @TYPE xy
   0.00e+00 577
   1.00e-01 576
   2.00e-01 565
   3.00e-01 550
   4.00e-01 567
   5.00e-01 572
   6.00e-01 566
   7.00e-01 578
   8.00e-01 567
   9.00e-01 565
   1.00e+00 563
   1.10e+00 579
   1.20e+00 566



 Please anybody let me know how to find clusters only among those
 particles I point out in the index file. So I need only the clusters
 consisting of ions but solvent is not of interest in my case.


 Thank you in advance,
 Vitaly



 ===
 Vitaly V. Chaban, Ph.D.(ABD)
 School of Chemistry
 V.N. Karazin Kharkiv National University
 Svoboda sq.,4, Kharkiv 61077, Ukraine
 email: cha...@univer.kharkov.ua,vvcha...@gmail.com
 skype: vvchaban, mob.: +38-097-8259698

   


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[gmx-users] Versions of analysis programs

2008-11-12 Thread Ran Friedman
Hi,

I've noticed that the VERSION entry of the analysis programs in GMX
4.0.2 is 3.2.0 or 3.3.2, whereas in GMX 3.3.3 it's 3.3.3.
Is that just a typo?

Thanks,
Ran.

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Re: [gmx-users] rmsd on homologous protein structure

2008-11-06 Thread Ran Friedman
Hi,

For individual structures, you can use g_confrms.
If you want a trajectory you can download do_multiprot from the user
contributions section, and follow the instructions there. Note that
multiprot aligns based on the structure only (no sequence information).

Ran.

Tatsiana Kirys wrote:
 Hi,

 i want to calculate rmsd on homologous protein structures that have different 
 residue numbers. 
 As far as i understood g_rms gives only rmsd of the same structure in 
 different configurations, but it doesn't fit homologous protein structures? 

 In Option -f2 can i provide a trajectory of a homologous protein structure of 
 it also have to be a reserence structure trajectory (which is provided in -s)?

 many many thanks
 Tatsiana 
   
-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: [EMAIL PROTECTED]
Skype: ran.friedman
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Re: [gmx-users] Peptide aggregation

2008-09-20 Thread Ran Friedman, Biochemisches Inst.

Dear Leon,

Note that you can already use g_clustsize to check the aggregates. I'll 
contact you off list next week with the modified version.


Ran

On Fri, 19 Sep 2008 17:13:02 +0100
 Léon Salgado [EMAIL PROTECTED] wrote:

Dear Dr. Ran Friedman

Would you please be so kind to send me your version, to calculate then the 
rgyr of the largest aggregate.
The box was built with a layer of 1.2 nm around the solute (editconf -d 
1.2).


Leon

Ran Friedman wrote:

Dear Leon,

You can try to use g_clustsize to get the aggregates. I have a version
that can calculate the gyration radius of the largest aggregate, but
this would work only if your box is big enough and I haven't tried it
with rhombic dodecahedron boxes.

Ran.

Léon Salgado wrote:
  

Dear gmx users

I did some simulations of multimers (peptides) in rhombic dodecahedron
boxes. In the initial configuration of the system, the peptides are
close of each other in the center of the box.

My aim to see if the peptides do aggregate during the trajectory or if
they tend to stay apart. A rough estimate can be taken from the
gyration radius for all the peptides together.

Already did a trjconv -pbc nojump pre-treatment on the trajectory,
before calculating the Rgyr. The gyration.xvg plots sometimes do show
abrupt jumps, and this is surely due to boundary effects, if I
correctly understood the PBC idea. If a peptide approaches the
boundary, it appears on the opposite side, thus rgyr will show a false
sudden increase. In fact, the peptide could be closer to the rest of
the other peptide molecule(s).

Thus my question is:
how to deal with peptide clusters that span over the periodic boundaries?

A similar question was done by Singh:
http://www.gromacs.org/pipermail/gmx-users/2007-January/025474.html

and it  was suggested by Chris Neale to pre-process the trajectory
(see
http://www.gromacs.org/pipermail/gmx-users/2007-January/025481.html)
with:

trjconv -f a.xtc -o a_cluster.gro -e 0.001 -pbc cluster
grompp -f a.mdp -c a_cluster.gro -o a_cluster.tpr
trjconv -f a.xtc -o a_cluster.xtc -s a_cluster.tpr -pbc nojump

but I'm getting infinite loops on the -pbc cluster treatment, same as
reported by Chris
(http://www.gromacs.org/pipermail/gmx-users/2008-July/035343.html).

Best,
Léon

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--
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Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Institute of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Skype: ran.friedman
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Re: [gmx-users] Peptide aggregation

2008-09-19 Thread Ran Friedman
Dear Leon,

You can try to use g_clustsize to get the aggregates. I have a version
that can calculate the gyration radius of the largest aggregate, but
this would work only if your box is big enough and I haven't tried it
with rhombic dodecahedron boxes.

Ran.

Léon Salgado wrote:
 Dear gmx users

 I did some simulations of multimers (peptides) in rhombic dodecahedron
 boxes. In the initial configuration of the system, the peptides are
 close of each other in the center of the box.

 My aim to see if the peptides do aggregate during the trajectory or if
 they tend to stay apart. A rough estimate can be taken from the
 gyration radius for all the peptides together.

 Already did a trjconv -pbc nojump pre-treatment on the trajectory,
 before calculating the Rgyr. The gyration.xvg plots sometimes do show
 abrupt jumps, and this is surely due to boundary effects, if I
 correctly understood the PBC idea. If a peptide approaches the
 boundary, it appears on the opposite side, thus rgyr will show a false
 sudden increase. In fact, the peptide could be closer to the rest of
 the other peptide molecule(s).

 Thus my question is:
 how to deal with peptide clusters that span over the periodic boundaries?

 A similar question was done by Singh:
 http://www.gromacs.org/pipermail/gmx-users/2007-January/025474.html

 and it  was suggested by Chris Neale to pre-process the trajectory
 (see
 http://www.gromacs.org/pipermail/gmx-users/2007-January/025481.html)
 with:

 trjconv -f a.xtc -o a_cluster.gro -e 0.001 -pbc cluster
 grompp -f a.mdp -c a_cluster.gro -o a_cluster.tpr
 trjconv -f a.xtc -o a_cluster.xtc -s a_cluster.tpr -pbc nojump

 but I'm getting infinite loops on the -pbc cluster treatment, same as
 reported by Chris
 (http://www.gromacs.org/pipermail/gmx-users/2008-July/035343.html).

 Best,
 Léon

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-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: [EMAIL PROTECTED]
Skype: ran.friedman
--

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[gmx-users] About QH entropy, could you please help me?

2008-09-17 Thread Ran Friedman
Dear Li Yang,
I forward your email to the GMX mailing list, which may be better for
you since other users can contribute as well. I'll reply there - I hope
you've subscribed to the list.
Ran.

Li Yang wrote:
 Dear Ran Friedman

 I'm sorry to disturb you, my name is Li Yang, I'm a chinese student.

 I've read some paper about the calculation of QH entropy: 
   (a)Jurgen Schlitter_ChemPhysLett1993_215_617, 
   (b)Ioan Andricioaei_JChemPhys2001_115_6289(quasiharmonic approximation). 
 There is still something confuse me.

 (1) Why the number of the eigenvalues is 3n-6 (the last 6 values are close to 
 zero) but not 3n ?  I practice some small examples by gromacs. (256 argon 
 atoms in a box of 2.3nm^3, you can find this example in paper(b)). For 
 g_covar, when -nofit, the number of eigenvalues is 3n; when -fit the number 
 is 3n-6. It seems there are some freedoms constrainted in the fit process. 

 The paper' conclusion is based on a assumption that hwkT, say, the high 
 frequencies vibrate (both rotation and translations, right?) can be omitted 
 for the entropy calculations, as it were, the contributions of them is too 
 small to be omitted. Are the freedoms mentioned above represent the freedoms 
 of rotations and translations of the molecules. I don't know. Maybe the 
 answer is in those papers, but I cannot catch it.

 While how to use the nofit result and fit result? The eigenv.agr in the 
 attachment includes fit and nofit results for the example: 256 argon 
 atoms in a box of 2.3nm^3. Why there is a big difference between them?


 (2) I split some time-segment to obtain the entropies in each stage to get 
 the convergence variation of the entropy. But I doubt the feasibility of this 
 method. If wrong, how to do?
 eg, time points: 0, 1, 2, 3, 4, 5.  and time stage:0-1, 0-2, 0-3, 0-4, 0-5, 
 right?
 why not 0-1, 1-2, 2-3, 3-4, 4-5.
 In the maillist of gmx, the latter is not wrong because of undersampling, I 
 don't know this meaning. Could you please offer me some suggestions or refs?


 (3) In entropy calculations, a system need to run a long time for entropy 
 convergence, the time seems to be longer than the one which needed for energy 
 convergence. While, for equilibrium thermodynamics simulations, how to 
 justify whether or not the system has achieving a equilibrium stage, based on 
 energy convergence or entropy confvergence?

 (4) For the example mentioned in the paper Ioan 
 Andricioaei_JChemPhys2001_115_6289. I use your perl script for entropy 
 calculation. But I don't reproduce the result. The needed time of entropy 
 convergence is longer than the time mentioned in the paper, and so larger of 
 my entropy. 
 I don't know why, perphas the simulation conditions is not right. My 
 simulation files are included in the attachment. Could you give some 
 suggestions? 
 BTW, in line 77 of your script: $w=$ev*$u*10**(-18), Does 10^-18 mean nm^-2?

 I apologize in advance if I disturb you.
 Thank you very much. Waiting for you reply.


 Best

 Li Yang 


 Li Yang
 [EMAIL PROTECTED]
   2008-09-17
   


-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: [EMAIL PROTECTED]
Skype: ran.friedman
--

___
gmx-users mailing listgmx-users@gromacs.org
http://www.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
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Re: [gmx-users] About QH entropy, could you please help me?

2008-09-17 Thread Ran Friedman
(1) 6 eigenvalues represent rotation and translation. For (very) small
molecules, these can be quite substantial, see Carlsson and Aqvist, /J.
Phys. Chem. B,/ *109* (13), 6448 -6456, 2005. By fitting you remove the
rotation and translation. You can search the literature for papers that
discuss the QH approximation as well. The motions are not really
harmonic - this is why it's an approximation.

I've received very similar results to Carlsson and Aqvist for benzene
and palmatic acid with GMX.

(2) The values you get depend on the sampling and the conversion of the
simulations. To improve sampling, you have to store the coordinates
frequently enough (so you get more samples). In addition, the simulation
should be long enough to give you meaningful results - and both depend
on the system which you study. Checking for convergence can be done by
repeating the calculations on different time windows, as you suggested.

(3) If you want to study the entropy, you have to sure it convergence.
Otherwise, it depends on what you want to calculate.

(4) Try to see if you really simulate the same system, and maybe try
other systems like the ones in the above mentioned paper. There can be
dozens of things that can change and since I didn't run these
simulations I can't be of much help here. As for the units, I don't
really remember what I used for frequencies, only that the final result
should be in J/(mol K) or Cal/(mol K). By following the script, with the
remarks, you should get the right units.

Ran.

Ran Friedman wrote:
 Dear Li Yang,
 I forward your email to the GMX mailing list, which may be better for
 you since other users can contribute as well. I'll reply there - I hope
 you've subscribed to the list.
 Ran.

 Li Yang wrote:
   
 Dear Ran Friedman

 I'm sorry to disturb you, my name is Li Yang, I'm a chinese student.

 I've read some paper about the calculation of QH entropy: 
   (a)Jurgen Schlitter_ChemPhysLett1993_215_617, 
   (b)Ioan Andricioaei_JChemPhys2001_115_6289(quasiharmonic approximation). 
 There is still something confuse me.

 (1) Why the number of the eigenvalues is 3n-6 (the last 6 values are close 
 to zero) but not 3n ?  I practice some small examples by gromacs. (256 argon 
 atoms in a box of 2.3nm^3, you can find this example in paper(b)). For 
 g_covar, when -nofit, the number of eigenvalues is 3n; when -fit the number 
 is 3n-6. It seems there are some freedoms constrainted in the fit process. 

 The paper' conclusion is based on a assumption that hwkT, say, the high 
 frequencies vibrate (both rotation and translations, right?) can be omitted 
 for the entropy calculations, as it were, the contributions of them is too 
 small to be omitted. Are the freedoms mentioned above represent the freedoms 
 of rotations and translations of the molecules. I don't know. Maybe the 
 answer is in those papers, but I cannot catch it.

 While how to use the nofit result and fit result? The eigenv.agr in the 
 attachment includes fit and nofit results for the example: 256 argon 
 atoms in a box of 2.3nm^3. Why there is a big difference between them?


 (2) I split some time-segment to obtain the entropies in each stage to get 
 the convergence variation of the entropy. But I doubt the feasibility of 
 this method. If wrong, how to do?
 eg, time points: 0, 1, 2, 3, 4, 5.  and time stage:0-1, 0-2, 0-3, 0-4, 0-5, 
 right?
 why not 0-1, 1-2, 2-3, 3-4, 4-5.
 In the maillist of gmx, the latter is not wrong because of undersampling, I 
 don't know this meaning. Could you please offer me some suggestions or refs?


 (3) In entropy calculations, a system need to run a long time for entropy 
 convergence, the time seems to be longer than the one which needed for 
 energy convergence. While, for equilibrium thermodynamics simulations, how 
 to justify whether or not the system has achieving a equilibrium stage, 
 based on energy convergence or entropy confvergence?

 (4) For the example mentioned in the paper Ioan 
 Andricioaei_JChemPhys2001_115_6289. I use your perl script for entropy 
 calculation. But I don't reproduce the result. The needed time of entropy 
 convergence is longer than the time mentioned in the paper, and so larger of 
 my entropy. 
 I don't know why, perphas the simulation conditions is not right. My 
 simulation files are included in the attachment. Could you give some 
 suggestions? 
 BTW, in line 77 of your script: $w=$ev*$u*10**(-18), Does 10^-18 mean 
 nm^-2?

 I apologize in advance if I disturb you.
 Thank you very much. Waiting for you reply.


 Best

 Li Yang 


 Li Yang
 [EMAIL PROTECTED]
   2008-09-17
   
 


   


-- 
--
Ran Friedman
Postdoctoral Fellow
Computational Structural Biology Group (A. Caflisch)
Department of Biochemistry
University of Zurich
Winterthurerstrasse 190
CH-8057 Zurich, Switzerland
Tel. +41-44-6355593
Email: [EMAIL PROTECTED]
Skype: ran.friedman

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