Re: [gmx-users] Re: Running Pull Code

2013-05-17 Thread Shima Arasteh
If I skip the pulling code step, how could I generate configurations while 
there are one ion in each window? Am I supposed to save my favorite snapshots 
during MD simulation trajectory?


 
Sincerely,
Shima


- Original Message -
From: Justin Lemkul 
To: Shima Arasteh ; Discussion list for GROMACS 
users 
Cc: 
Sent: Friday, May 17, 2013 4:02 PM
Subject: Re: [gmx-users] Re: Running Pull Code



On 5/17/13 7:16 AM, Shima Arasteh wrote:
> Thanks for your reply.
> It' s around 5 nano seconds that I ran equilibration time on the system, and 
> the average pressure I see as a result, seems sensible. However I am not sure 
> if this criteria is sufficient? Others suggest to evaluate the box-dimension 
> changes using g_energy code to judge of sufficient equilibration time.
>

The box vectors won't tell you anything more than the pressure will since 
they're related quantities.

The better question is, "What is a suitable starting structure for the system 
of 
interest?"  The umbrella sampling tutorial (which everyone seems to take at 
literal face value as the only way to do things, which it is decidedly not) 
presents a simple, easy-to-understand method.  In the paper I did (upon which I 
based the tutorial), I simulated the protofibril structures for 100 ns before I 
was confident they were suitably stable and representative of viable structures 
for doing SMD and US.  Your mileage will vary and depends on the quality of the 
starting structure and what it is that you hope to determine.  There is no 
magic 
recipe that is universal.

-Justin

> I appreciate your suggestion.
>
>
> Sincerely,
> Shima
>
>
> - Original Message -
> From: Thomas Schlesier 
> To: gmx-users@gromacs.org
> Cc:
> Sent: Friday, May 17, 2013 3:30 PM
> Subject: [gmx-users] Re: Running Pull Code
>
> The three steps (EM, NVT and NPT) are to equilibrate the system. How
> much time these steps need depends on the system. But i would assume a
> ouple of nanosecounds are sufficient for most systems. You could look
> into the literature, how long other people equilibrate systems which are
> similar to ours.
> If the system is equilibrated, you an start to perform the pulling
> simulation to obtain the individual structure for the later umbrella
> sampling.
>
> Greetings
> Thomas
>
> Am 17.05.2013 07:46, schrieb gmx-users-requ...@gromacs.org:
>> Hi,
>>
>> I have a system composed of POPC/peptide/water/ions. I aim to study ion 
>> conduction through the peptide using umbrella sampling.
>> I built the system and ran EM, NVT, NPT successfully, but have not run md 
>> yet. I' d like to know if the system is required of passing a few 
>> nanoseconds md? Or I might be able to go to Umbrella Sampling straight after 
>> NPT?
>> As I studied in Justin's tutorial, running pull code is done after some 
>> typical steps of every simulation ( EM, NVT, NPT). But I dont know if is 
>> correct generally for other systems as well?
>>
>> Would you please give me any suggestions?
>>
>>
>> Thanks in advance.
>> Sincerely,
>> Shima?
>

-- 


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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Re: [gmx-users] Inconsistent results in different clusters and cores

2013-05-17 Thread tarak karmakar
@ Justin and Mark,

Do you have any idea about the rlist used by Bjelkmar et. al.
'Implementation of charmm in gromacs'? I see, they have performed
their simulations in gromacs-4.1 version. I'm not sure about whether
in that version the problem persisted or not.

I'm sorry if this mail went to you twice. Facing lot of problems,
here, in mail delivery failure.

Thanks,
Tarak


On Fri, May 17, 2013 at 6:22 PM, tarak karmakar  wrote:
> @ Justin and Mark,
>
> Do you have any idea about the rlist used by Bjelkmar et. al.
> 'Implementation of charmm in gromacs'? I see, they have performed
> their simulations in gromacs-4.1 version. I'm not sure about whether
> in that version the problem persisted or not.
>
> Tarak
>
> On Fri, May 17, 2013 at 5:42 PM, tarak karmakar  wrote:
>> I am extremely sorry for spaming the mail box. It was quite
>> unintentionally. Believe me I was getting the following error every
>> time while sending the mail.
>>
>> Final-Recipient: rfc822; jaanus.k...@eesti.ee
>> Action: failed
>> Status: 5.0.0
>> Diagnostic-Code: X-Postfix; mail forwarding loop for jaanus.k...@eesti.ee
>>
>> Tarak
>>
>>
>> -- Forwarded message --
>> From: tarak karmakar 
>> To: Discussion list for GROMACS users 
>> Cc:
>> Date: Fri, 17 May 2013 15:50:25 +0530
>> Subject: Re: [gmx-users] Inconsistent results in different clusters and cores
>>
>> On Fri, May 17, 2013 at 5:36 PM, Mark Abraham  
>> wrote:
>>> On Fri, May 17, 2013 at 1:23 PM, Justin Lemkul  wrote:
>>>


 On 5/17/13 6:20 AM, tarak karmakar wrote:

> I have read the 'implementation of charmm in gromacs' by bjelkmar,
> JCTC. There they have used following cut-offs
> coulombtype=PME
> rcoulomb=1.2
> vdwtype=switch
> rvdw=1.2
> rvdw-switch=1.0
>
> I am not sure about rlist.
>
>
 It's really unnecessary to spam the list with a dozen requests that ask
 the same question.

 By definition, with PME, rlist = rcoulomb.  For CHARMM, use rlistlong =
 1.4; the message that is printed below is an error that has been fixed in
 newer versions.
>>>
>>>
>>> Are you sure? Looking at the logic in src/mdlib/read_ir.c, I could not see
>>> how Tarak's input could have led (correctly) to that note from grompp. I am
>>> thinking that
>>> https://github.com/gromacs/gromacs/blob/release-4-5-patches/src/kernel/readir.c#L170
>>> is
>>> setting rlistlong = rlist, and so
>>> https://github.com/gromacs/gromacs/blob/release-4-5-patches/src/kernel/readir.c#L586
>>> gets
>>> double-crossed.
>>>
>>> (Note that http://redmine.gromacs.org/issues/1164 pertained to a slightly
>>> different issue.)
>>>
>>> Mark
>>> --
>>> gmx-users mailing listgmx-users@gromacs.org
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Re: [gmx-users] Tryptophan rings are not connected in visualization

2013-05-17 Thread Justin Lemkul



On 5/17/13 10:08 PM, Shima Arasteh wrote:


Hi,
I am simulating a system composed if POPC , peptide, waters and ions.
I used the InflateGRO methodology to construct the system.
There
  are 2 Tryptophan residues in my peptide. Each Tryptophan has 2rings
connected from one side. After inflategro one of the Tryptophan rings is
normal, but the other is not because  What I see them in vmd, there are
2rings remain close to eachother but the expected bonds between them are
  not visible.
The top file shows the correct bonds and angles and ... .
I ran EM, NVT, NPT, and thought this problem would be solved but it is still as 
well as before.
The EM was also ok and did not show high enegy or crash.
Does this problem relate to the vmd and its algorithms? Or there is a problem 
with my system.


http://www.gromacs.org/Downloads/Related_Software/Visualization_Software#Topology_bonds_vs_Rendered_bonds

The topology is definitive.  VMD is not.


How would the rings look usual? How could I solve it?



Run EM.  InflateGRO should not have messed with the coordinates though.  If the 
bad geometry is a result of EM, that means you have really nasty forces 
somewhere in the system.


-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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Re: [gmx-users] Re: Running Pull Code

2013-05-17 Thread Justin Lemkul



On 5/17/13 8:25 AM, Shima Arasteh wrote:

Thanks for your reply.
In fact, I plan to study ion conduction through the peptide inserted in lipid 
membrane and acting as an ion channel. According to the literature, an ion 
across the membrane in less than 20 ns.
Can I decide upon this information to apply pull code?

You simulated the protofibril structures for 100 ns, in another article 25 ns.
  Ok, if there is not any universal recipe for it, what do you suggest me? Try 
and error?



Assess the literature thoroughly.  Basing your plan on only one paper may not be 
the most productive way to go.  See what many do, and base what you try off of 
what you find.


-Justin



Sincerely,
Shima


- Original Message -
From: Justin Lemkul 
To: Shima Arasteh ; Discussion list for GROMACS users 

Cc:
Sent: Friday, May 17, 2013 4:02 PM
Subject: Re: [gmx-users] Re: Running Pull Code



On 5/17/13 7:16 AM, Shima Arasteh wrote:

Thanks for your reply.
It' s around 5 nano seconds that I ran equilibration time on the system, and 
the average pressure I see as a result, seems sensible. However I am not sure 
if this criteria is sufficient? Others suggest to evaluate the box-dimension 
changes using g_energy code to judge of sufficient equilibration time.



The box vectors won't tell you anything more than the pressure will since
they're related quantities.

The better question is, "What is a suitable starting structure for the system of
interest?"  The umbrella sampling tutorial (which everyone seems to take at
literal face value as the only way to do things, which it is decidedly not)
presents a simple, easy-to-understand method.  In the paper I did (upon which I
based the tutorial), I simulated the protofibril structures for 100 ns before I
was confident they were suitably stable and representative of viable structures
for doing SMD and US.  Your mileage will vary and depends on the quality of the
starting structure and what it is that you hope to determine.  There is no magic
recipe that is universal.

-Justin


I appreciate your suggestion.


Sincerely,
Shima


- Original Message -
From: Thomas Schlesier 
To: gmx-users@gromacs.org
Cc:
Sent: Friday, May 17, 2013 3:30 PM
Subject: [gmx-users] Re: Running Pull Code

The three steps (EM, NVT and NPT) are to equilibrate the system. How
much time these steps need depends on the system. But i would assume a
ouple of nanosecounds are sufficient for most systems. You could look
into the literature, how long other people equilibrate systems which are
similar to ours.
If the system is equilibrated, you an start to perform the pulling
simulation to obtain the individual structure for the later umbrella
sampling.

Greetings
Thomas

Am 17.05.2013 07:46, schrieb gmx-users-requ...@gromacs.org:

Hi,

I have a system composed of POPC/peptide/water/ions. I aim to study ion 
conduction through the peptide using umbrella sampling.
I built the system and ran EM, NVT, NPT successfully, but have not run md yet. 
I' d like to know if the system is required of passing a few nanoseconds md? Or 
I might be able to go to Umbrella Sampling straight after NPT?
As I studied in Justin's tutorial, running pull code is done after some typical 
steps of every simulation ( EM, NVT, NPT). But I dont know if is correct 
generally for other systems as well?

Would you please give me any suggestions?


Thanks in advance.
Sincerely,
Shima?






--


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] Tryptophan rings are not connected in visualization

2013-05-17 Thread Shima Arasteh

Hi,
I am simulating a system composed if POPC , peptide, waters and ions.
I used the InflateGRO methodology to construct the system.
There
 are 2 Tryptophan residues in my peptide. Each Tryptophan has 2rings 
connected from one side. After inflategro one of the Tryptophan rings is 
normal, but the other is not because  What I see them in vmd, there are 
2rings remain close to eachother but the expected bonds between them are
 not visible.
The top file shows the correct bonds and angles and ... .
I ran EM, NVT, NPT, and thought this problem would be solved but it is still as 
well as before.
The EM was also ok and did not show high enegy or crash.
Does this problem relate to the vmd and its algorithms? Or there is a problem 
with my system.
How would the rings look usual? How could I solve it?

Thanks in advance.
 
Sincerely,
Shima
--
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Re: [gmx-users] compile Gromacs using Cray compilers

2013-05-17 Thread Mark Abraham
Cray's compiler is largely/wholly untested. I'd suggest you use the version
of gcc that you know works.

For use on a big cluster, you probably don't want Thread MPI anyway. Does
cmake -DGMX_MPI work?

Mark


On Sat, May 18, 2013 at 12:01 AM, Humayun Arafat  wrote:

> Hi,
>
>
> I need some help for the compilation of gromacs using Cray compilers(CCE).
>
> I can compile gromacs using GNU compilers but not using CCE.
>
> I am using gromacs 4.6 and cmake 2.8.4 on Cray XE6
>
>
>
> After doing cmake, when I try to do make, I am getting this error.
>
>
>
> CC-20 craycc: ERROR File =
> /home/users/me/gromacs/include/thread_mpi/atomic.h, Line = 202
>
> The identifier "tMPI_Thread_mutex_t" is undefined.
>
> static tMPI_Thread_mutex_t tMPI_Atomic_mutex =
> TMPI_THREAD_MUTEX_INITIALIZER;
>
> ^
>
>
>
> Then I checked that the cmake  configuration had errors for this atomic.h
> header file.
>
> It does not find any atomic operations for cray compilers.
>
> Inside this header file, I see that there is nothing for Cray compilers.
>
> It has GNU,Intel, xlc….
>
> My guess is that probably it is not adding any atomic header file for CCE.
>
>
>
>
> Please suggest me some ways to fix this.
>
> Thank you for your help.
>
>
> Thanks
>
> Humayun
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[gmx-users] compile Gromacs using Cray compilers

2013-05-17 Thread Humayun Arafat
Hi,


I need some help for the compilation of gromacs using Cray compilers(CCE).

I can compile gromacs using GNU compilers but not using CCE.

I am using gromacs 4.6 and cmake 2.8.4 on Cray XE6



After doing cmake, when I try to do make, I am getting this error.



CC-20 craycc: ERROR File =
/home/users/me/gromacs/include/thread_mpi/atomic.h, Line = 202

The identifier "tMPI_Thread_mutex_t" is undefined.

static tMPI_Thread_mutex_t tMPI_Atomic_mutex =
TMPI_THREAD_MUTEX_INITIALIZER;

^



Then I checked that the cmake  configuration had errors for this atomic.h
header file.

It does not find any atomic operations for cray compilers.

Inside this header file, I see that there is nothing for Cray compilers.

It has GNU,Intel, xlc….

My guess is that probably it is not adding any atomic header file for CCE.




Please suggest me some ways to fix this.

Thank you for your help.


Thanks

Humayun
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Re: [gmx-users] visualizing the system

2013-05-17 Thread Mark Abraham
On Fri, May 17, 2013 at 10:21 PM, Shima Arasteh  wrote:

>
> Hi,
> I am simulating a system composed if POPC , peptide, waters and ions.
> I used the InflateGRO methodology to construct the system.
> There are 2 phenylalanine residues in my peptide. Each phenyl has 2rings
> connected from one side.


I don't understand. Phenylalanine has a single aromatic ring.


> After inflategro one of the phenyl rings is normal, but the other is not
> because  What I see them in vmd, there are 2rings remain close to eachother
> but the expected bonds between them are not visible.
>

Two phenylalanine residues are not expected to bond.


> The top file shows the correct bonds and angles and ... .
> I ran EM, NVT, NPT, and thought this problem would be solved but it is
> still as well as before.
> The EM was also ok and did not show high enegy or crash.
> Does this problem relate to the vmd and its algorithms? Or there is a
> problem with my system.
> How would the rings look usual? How could I solve it?
>

Your description of your expectations of phenylalanine do not seem to make
sense. :-)

Mark
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[gmx-users] visualizing the system

2013-05-17 Thread Shima Arasteh

Hi,
I am simulating a system composed if POPC , peptide, waters and ions.
I used the InflateGRO methodology to construct the system.
There are 2 phenylalanine residues in my peptide. Each phenyl has 2rings 
connected from one side. After inflategro one of the phenyl rings is normal, 
but the other is not because  What I see them in vmd, there are 2rings remain 
close to eachother but the expected bonds between them are not visible.
The top file shows the correct bonds and angles and ... .
I ran EM, NVT, NPT, and thought this problem would be solved but it is still as 
well as before.
The EM was also ok and did not show high enegy or crash.
Does this problem relate to the vmd and its algorithms? Or there is a problem 
with my system.
How would the rings look usual? How could I solve it?

Thanks in advance.
Sincerely,
Shima

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Re: [gmx-users] Expanding a .top file to have all connection information

2013-05-17 Thread Mark Abraham
On Fri, May 17, 2013 at 4:28 PM, David Rosenman wrote:

> This is a good idea, but it doesn't work. It produces a more detailed .top
> file with force field parameters, but still, only the connectivities of the
> protein are provided.


What "connectivities" are missing?


> top2psf has no idea what to do with this file, by the
> way.
>
> Would it help for me to provide the pre-processed and post-processed top
> files?
>

Sure, but attachments will generally be rejected. Use a file sharing
service.

Mark


>
> Cheers,
> David
>
>
> On Fri, May 17, 2013 at 10:17 AM, Mark Abraham  >wrote:
>
> > How does grompp -pp look?
> >
> > Mark
> >
> >
> > On Fri, May 17, 2013 at 3:40 PM, davidjrosenman <
> davidjrosen...@gmail.com
> > >wrote:
> >
> > > Hello everyone,
> > >
> > > This may be a bit out of the purview of this list, but it can't hurt to
> > > ask.
> > >
> > > Let me start from the beginning: I'm trying to take a
> structure/topology
> > > that I generated with GROMACS tools and convert it to run with NAMD.
> The
> > > problem is that this is a huge simulation box with many different atom
> > > types
> > > (homodimeric protein, water, lipids, ions), and I am having a lot of
> > > trouble
> > > generating a .psf file from the information I have.
> > >
> > > The current strategy I'm pursuing to accomplish this task is to use the
> > > top2psf script:
> > > http://www.ks.uiuc.edu/Research/vmd/script_library/scripts/top2psf/
> > >
> > > The issue is that this script will only read what is explicitly written
> > in
> > > the top file. All of the include records will be ignored, as will
> > multiple
> > > molecules. So, the output is a psf suitable ONLY for the first chain of
> > my
> > > dimer. I want a psf that will include all components of my structure,
> > > including the lipids, waters, etc.
> > >
> > > So, I ask, is there a way to expand a topology to explicitly get all of
> > the
> > > connectivities in a structure? I figure this information must be
> > contained
> > > in the .tpr file, but that's neither human readable nor compatible with
> > > top2psf.
> > >
> > > If you have any advice for that, or for the larger problem at hand, I
> > would
> > > appreciate it. Thank you very much!
> > >
> > > Cheers,
> > > David Rosenman
> > > Grad Student, Rensselaer Polytechnic Institute
> > >
> > >
> > >
> > >
> > > --
> > > View this message in context:
> > >
> >
> http://gromacs.5086.x6.nabble.com/Expanding-a-top-file-to-have-all-connection-information-tp5008345.html
> > > Sent from the GROMACS Users Forum mailing list archive at Nabble.com.
> > > --
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> > >
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Re: [gmx-users] Re: REMD analysis

2013-05-17 Thread Mark Abraham
On Fri, May 17, 2013 at 4:26 PM, bharat gupta wrote:

> Dear Sir,
>
> The the default bin width is 0.1 which I used for plotting the graphs.
>

That's nice. You need to decide what you need to do about it if you want
graphs that look like those you see reported :-)


> Another question is about your last reply to my thread "exchange acceptance
> is a poor proxy for sampling efficiency". Sorry to ask this, but how to
> check whether the sampling efficiency is optimal or not (what should be
> optimal sampling efficiency) ??
>

Ah, now here's the real question :-) Spacing the replicas for optimal
*flow* is a difficult problem, even for toy peptides, see e.g. papers by
Nadler and Hansmann. Merely accepting exchanges does not imply flow. The
belief is that getting flow enhances sampling, but the latter is hard to
demonstrate without showing that "simulation time to converged sampling"
actually reduces. I'm not aware of anybody who's actually done that - but
it would certainly be an advantage if your application is interested in
data at a range of temperatures.

Mark

On Fri, May 17, 2013 at 11:10 PM, Mark Abraham  >wrote:
>
> > Histograms 101: The smaller your bin width, the more variations you see.
> > The more samples you have, the fewer variations you see. A histogram that
> > does not mention either of this is a work of fiction.
> >
> > The number of degrees of freedom in the potential energy distribution is
> > also a factor in whether the distribution will look smooth for a given
> bin
> > width and number of samples.
> >
> > Mark
> >
> > On Fri, May 17, 2013 at 3:51 PM, bharat gupta  > >wrote:
> >
> > > Dear Sir,
> > >
> > > I tried plotting the PE overlap using the following way :-
> > >
> > > 1. extract PE of each replica using g_energy
> > > 2. get the PE distribution using g_analyze -f potential_0.xvg -dist
> > > pot0.xvg
> > > 3. used xmgrace to plot all the PE distribution graphs together.
> > >
> > > The same thing I did for temperature distribution for each replica.
> > >
> > > Here's the file for both PE overlap (
> > > https://www.dropbox.com/s/895f1bi0hkuy884/pe_dist.png)
> > > temp distribution (
> > https://www.dropbox.com/s/ed66uop16blgqwa/temp_dist.png
> > > )
> > > Is this the correct way ??
> > >
> > >
> > > But the plot doesnot look like this (
> > > https://www.dropbox.com/s/fsuabkl7zrydnib/sample%20PE%20overlap.jpg).
> > Do i
> > > have to normalize the data and then plot in order to get a smooth plot
> > like
> > > this one??
> > >
> > > 
> > > Bharat
> > > --
> > > gmx-users mailing listgmx-users@gromacs.org
> > > http://lists.gromacs.org/mailman/listinfo/gmx-users
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Re: [gmx-users] Expanding a .top file to have all connection information

2013-05-17 Thread David Rosenman
This is a good idea, but it doesn't work. It produces a more detailed .top
file with force field parameters, but still, only the connectivities of the
protein are provided. top2psf has no idea what to do with this file, by the
way.

Would it help for me to provide the pre-processed and post-processed top
files?

Cheers,
David


On Fri, May 17, 2013 at 10:17 AM, Mark Abraham wrote:

> How does grompp -pp look?
>
> Mark
>
>
> On Fri, May 17, 2013 at 3:40 PM, davidjrosenman  >wrote:
>
> > Hello everyone,
> >
> > This may be a bit out of the purview of this list, but it can't hurt to
> > ask.
> >
> > Let me start from the beginning: I'm trying to take a structure/topology
> > that I generated with GROMACS tools and convert it to run with NAMD. The
> > problem is that this is a huge simulation box with many different atom
> > types
> > (homodimeric protein, water, lipids, ions), and I am having a lot of
> > trouble
> > generating a .psf file from the information I have.
> >
> > The current strategy I'm pursuing to accomplish this task is to use the
> > top2psf script:
> > http://www.ks.uiuc.edu/Research/vmd/script_library/scripts/top2psf/
> >
> > The issue is that this script will only read what is explicitly written
> in
> > the top file. All of the include records will be ignored, as will
> multiple
> > molecules. So, the output is a psf suitable ONLY for the first chain of
> my
> > dimer. I want a psf that will include all components of my structure,
> > including the lipids, waters, etc.
> >
> > So, I ask, is there a way to expand a topology to explicitly get all of
> the
> > connectivities in a structure? I figure this information must be
> contained
> > in the .tpr file, but that's neither human readable nor compatible with
> > top2psf.
> >
> > If you have any advice for that, or for the larger problem at hand, I
> would
> > appreciate it. Thank you very much!
> >
> > Cheers,
> > David Rosenman
> > Grad Student, Rensselaer Polytechnic Institute
> >
> >
> >
> >
> > --
> > View this message in context:
> >
> http://gromacs.5086.x6.nabble.com/Expanding-a-top-file-to-have-all-connection-information-tp5008345.html
> > Sent from the GROMACS Users Forum mailing list archive at Nabble.com.
> > --
> > gmx-users mailing listgmx-users@gromacs.org
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Re: [gmx-users] Re: REMD analysis

2013-05-17 Thread bharat gupta
Dear Sir,

The the default bin width is 0.1 which I used for plotting the graphs.
Another question is about your last reply to my thread "exchange acceptance
is a poor proxy for sampling efficiency". Sorry to ask this, but how to
check whether the sampling efficiency is optimal or not (what should be
optimal sampling efficiency) ??

On Fri, May 17, 2013 at 11:10 PM, Mark Abraham wrote:

> Histograms 101: The smaller your bin width, the more variations you see.
> The more samples you have, the fewer variations you see. A histogram that
> does not mention either of this is a work of fiction.
>
> The number of degrees of freedom in the potential energy distribution is
> also a factor in whether the distribution will look smooth for a given bin
> width and number of samples.
>
> Mark
>
> On Fri, May 17, 2013 at 3:51 PM, bharat gupta  >wrote:
>
> > Dear Sir,
> >
> > I tried plotting the PE overlap using the following way :-
> >
> > 1. extract PE of each replica using g_energy
> > 2. get the PE distribution using g_analyze -f potential_0.xvg -dist
> > pot0.xvg
> > 3. used xmgrace to plot all the PE distribution graphs together.
> >
> > The same thing I did for temperature distribution for each replica.
> >
> > Here's the file for both PE overlap (
> > https://www.dropbox.com/s/895f1bi0hkuy884/pe_dist.png)
> > temp distribution (
> https://www.dropbox.com/s/ed66uop16blgqwa/temp_dist.png
> > )
> > Is this the correct way ??
> >
> >
> > But the plot doesnot look like this (
> > https://www.dropbox.com/s/fsuabkl7zrydnib/sample%20PE%20overlap.jpg).
> Do i
> > have to normalize the data and then plot in order to get a smooth plot
> like
> > this one??
> >
> > 
> > Bharat
> > --
> > gmx-users mailing listgmx-users@gromacs.org
> > http://lists.gromacs.org/mailman/listinfo/gmx-users
> > * Please search the archive at
> > http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
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> >
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Re: [gmx-users] Expanding a .top file to have all connection information

2013-05-17 Thread Mark Abraham
How does grompp -pp look?

Mark


On Fri, May 17, 2013 at 3:40 PM, davidjrosenman wrote:

> Hello everyone,
>
> This may be a bit out of the purview of this list, but it can't hurt to
> ask.
>
> Let me start from the beginning: I'm trying to take a structure/topology
> that I generated with GROMACS tools and convert it to run with NAMD. The
> problem is that this is a huge simulation box with many different atom
> types
> (homodimeric protein, water, lipids, ions), and I am having a lot of
> trouble
> generating a .psf file from the information I have.
>
> The current strategy I'm pursuing to accomplish this task is to use the
> top2psf script:
> http://www.ks.uiuc.edu/Research/vmd/script_library/scripts/top2psf/
>
> The issue is that this script will only read what is explicitly written in
> the top file. All of the include records will be ignored, as will multiple
> molecules. So, the output is a psf suitable ONLY for the first chain of my
> dimer. I want a psf that will include all components of my structure,
> including the lipids, waters, etc.
>
> So, I ask, is there a way to expand a topology to explicitly get all of the
> connectivities in a structure? I figure this information must be contained
> in the .tpr file, but that's neither human readable nor compatible with
> top2psf.
>
> If you have any advice for that, or for the larger problem at hand, I would
> appreciate it. Thank you very much!
>
> Cheers,
> David Rosenman
> Grad Student, Rensselaer Polytechnic Institute
>
>
>
>
> --
> View this message in context:
> http://gromacs.5086.x6.nabble.com/Expanding-a-top-file-to-have-all-connection-information-tp5008345.html
> Sent from the GROMACS Users Forum mailing list archive at Nabble.com.
> --
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Re: [gmx-users] Re: REMD analysis

2013-05-17 Thread Mark Abraham
Histograms 101: The smaller your bin width, the more variations you see.
The more samples you have, the fewer variations you see. A histogram that
does not mention either of this is a work of fiction.

The number of degrees of freedom in the potential energy distribution is
also a factor in whether the distribution will look smooth for a given bin
width and number of samples.

Mark

On Fri, May 17, 2013 at 3:51 PM, bharat gupta wrote:

> Dear Sir,
>
> I tried plotting the PE overlap using the following way :-
>
> 1. extract PE of each replica using g_energy
> 2. get the PE distribution using g_analyze -f potential_0.xvg -dist
> pot0.xvg
> 3. used xmgrace to plot all the PE distribution graphs together.
>
> The same thing I did for temperature distribution for each replica.
>
> Here's the file for both PE overlap (
> https://www.dropbox.com/s/895f1bi0hkuy884/pe_dist.png)
> temp distribution (https://www.dropbox.com/s/ed66uop16blgqwa/temp_dist.png
> )
> Is this the correct way ??
>
>
> But the plot doesnot look like this (
> https://www.dropbox.com/s/fsuabkl7zrydnib/sample%20PE%20overlap.jpg). Do i
> have to normalize the data and then plot in order to get a smooth plot like
> this one??
>
> 
> Bharat
> --
> gmx-users mailing listgmx-users@gromacs.org
> http://lists.gromacs.org/mailman/listinfo/gmx-users
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Re: [gmx-users] Re: REMD analysis

2013-05-17 Thread XAvier Periole

What do you not like in your distributions? What are your looking for in these 
distributions? 

I am not sure what you are expecting from the list here … your distributions 
are fine, but, as Mark noted, it does not mean your simulation and sampling 
will be optimal … 

On May 17, 2013, at 3:51 PM, bharat gupta  wrote:

> Dear Sir,
> 
> I tried plotting the PE overlap using the following way :-
> 
> 1. extract PE of each replica using g_energy
> 2. get the PE distribution using g_analyze -f potential_0.xvg -dist pot0.xvg
> 3. used xmgrace to plot all the PE distribution graphs together.
> 
> The same thing I did for temperature distribution for each replica.
> 
> Here's the file for both PE overlap (
> https://www.dropbox.com/s/895f1bi0hkuy884/pe_dist.png)
> temp distribution (https://www.dropbox.com/s/ed66uop16blgqwa/temp_dist.png)
> Is this the correct way ??
> 
> 
> But the plot doesnot look like this (
> https://www.dropbox.com/s/fsuabkl7zrydnib/sample%20PE%20overlap.jpg). Do i
> have to normalize the data and then plot in order to get a smooth plot like
> this one??
> 
> 
> Bharat
> -- 
> gmx-users mailing listgmx-users@gromacs.org
> http://lists.gromacs.org/mailman/listinfo/gmx-users
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Re: [gmx-users] Comparing Gromacs versions

2013-05-17 Thread Szilárd Páll
On Fri, May 17, 2013 at 2:48 PM, Djurre de Jong-Bruinink
 wrote:
>
>
>>The answer is in the log files, in particular the performance summary
>>should indicate where is the performance difference. If you post your
>>log files somewhere we can probably give further tips on optimizing
>>your run configurations.
>
>
> I put the log files for 72 CPUs, using GMX455, GMX461+group and GMX461+verlet 
> here:
> http://md.chem.rug.nl/~djurre/logs/N6_gmx455.log
> http://md.chem.rug.nl/~djurre/logs/N6_gmx461_group.log
> http://md.chem.rug.nl/~djurre/logs/N6_gmx461_verlet.log

That tells much more.

> It would be great if you could point out some  possible optimizations.

Here you go:
- You seem to be using 2 fs time-steps so you don't need to constrain
all bonds, constraining only h-bonds is enough. This will reduce the
cell size requirement posed by LINCS and will allow further
decomposition. Additionally, you can also tweak the LINCS order and
iteration.
- With the Verlet scheme you can use OpenMP parallelization to reduce
the pressure on domain-decomposition, e.g. by using 2 OpenMP threads
(at least for PP) you'd need only 24 domains instead of 48. OpenMP
parallelization is not very efficient on the old-ish AMD processors
you are using, but 2 threads/MPI ranks should still help at very high
parallelization (<200 atoms/core).
- On the AMD Istambul (K10) processors that you are using gcc
generates rather poor non-bonded kernel code. icc will make the
non-bondeds run 10-20% faster.
- With Verlet scheme you can safely increase nstlist to higher values
so already at 72 cores and especially at higher core count 12,15, or
even 20 might give better performance.
- Your 4.6 group scheme run shows large PP-PME imbalance, try
increasing the number of PME ranks!

>
>
>>Note that with such a small system the scaling with the group scheme
>>surely becomes limited by imbalance and probably it won't scale much
>>further than 72 cores. At the same time, simulations with the verlet
>>scheme have shown scaling to below 100 atoms/core.
>
> I tried running on 84 cpus (56PP cores=400 atoms/PP core), but I did get an 
> domain decomposition error. Maybe I could optimize -rcon and -dds further, 
> however although the scaling to more CPUs is better with the verlet scheme, I 
> think you will never win:  with 72 CPUs Verlet is almost as fast as with 
> group at 60 CPUs, however compared to 24 cpus the scaling per CPU is already 
> down to 60%.
>
> But as Mark Abraham mentioned, it might be that my system is just to small to 
> get the advantage of scaling that will be there in larger systems.

As I mentioned before, you *should* be able to use 2x more cores (or
perhaps even more), but of course the parallel efficiency will
decrease.

Cheers,
--
Szilard

>
>
> Groetnis,
> Djurre
>
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[gmx-users] Re: REMD analysis

2013-05-17 Thread bharat gupta
Dear Sir,

I tried plotting the PE overlap using the following way :-

1. extract PE of each replica using g_energy
2. get the PE distribution using g_analyze -f potential_0.xvg -dist pot0.xvg
3. used xmgrace to plot all the PE distribution graphs together.

The same thing I did for temperature distribution for each replica.

Here's the file for both PE overlap (
https://www.dropbox.com/s/895f1bi0hkuy884/pe_dist.png)
temp distribution (https://www.dropbox.com/s/ed66uop16blgqwa/temp_dist.png)
Is this the correct way ??


But the plot doesnot look like this (
https://www.dropbox.com/s/fsuabkl7zrydnib/sample%20PE%20overlap.jpg). Do i
have to normalize the data and then plot in order to get a smooth plot like
this one??


Bharat
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[gmx-users] Expanding a .top file to have all connection information

2013-05-17 Thread davidjrosenman
Hello everyone, 

This may be a bit out of the purview of this list, but it can't hurt to ask. 

Let me start from the beginning: I'm trying to take a structure/topology
that I generated with GROMACS tools and convert it to run with NAMD. The
problem is that this is a huge simulation box with many different atom types
(homodimeric protein, water, lipids, ions), and I am having a lot of trouble
generating a .psf file from the information I have. 

The current strategy I'm pursuing to accomplish this task is to use the
top2psf script: 
http://www.ks.uiuc.edu/Research/vmd/script_library/scripts/top2psf/

The issue is that this script will only read what is explicitly written in
the top file. All of the include records will be ignored, as will multiple
molecules. So, the output is a psf suitable ONLY for the first chain of my
dimer. I want a psf that will include all components of my structure,
including the lipids, waters, etc. 

So, I ask, is there a way to expand a topology to explicitly get all of the
connectivities in a structure? I figure this information must be contained
in the .tpr file, but that's neither human readable nor compatible with
top2psf. 

If you have any advice for that, or for the larger problem at hand, I would
appreciate it. Thank you very much! 

Cheers, 
David Rosenman 
Grad Student, Rensselaer Polytechnic Institute




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Re: [gmx-users] Inconsistent results in different clusters and cores

2013-05-17 Thread tarak karmakar
@ Justin and Mark,

Do you have any idea about the rlist used by Bjelkmar et. al.
'Implementation of charmm in gromacs'? I see, they have performed
their simulations in gromacs-4.1 version. I'm not sure about whether
in that version the problem persisted or not.

Tarak

On Fri, May 17, 2013 at 5:42 PM, tarak karmakar  wrote:
> I am extremely sorry for spaming the mail box. It was quite
> unintentionally. Believe me I was getting the following error every
> time while sending the mail.
>
> Final-Recipient: rfc822; jaanus.k...@eesti.ee
> Action: failed
> Status: 5.0.0
> Diagnostic-Code: X-Postfix; mail forwarding loop for jaanus.k...@eesti.ee
>
> Tarak
>
>
> -- Forwarded message --
> From: tarak karmakar 
> To: Discussion list for GROMACS users 
> Cc:
> Date: Fri, 17 May 2013 15:50:25 +0530
> Subject: Re: [gmx-users] Inconsistent results in different clusters and cores
>
> On Fri, May 17, 2013 at 5:36 PM, Mark Abraham  
> wrote:
>> On Fri, May 17, 2013 at 1:23 PM, Justin Lemkul  wrote:
>>
>>>
>>>
>>> On 5/17/13 6:20 AM, tarak karmakar wrote:
>>>
 I have read the 'implementation of charmm in gromacs' by bjelkmar,
 JCTC. There they have used following cut-offs
 coulombtype=PME
 rcoulomb=1.2
 vdwtype=switch
 rvdw=1.2
 rvdw-switch=1.0

 I am not sure about rlist.


>>> It's really unnecessary to spam the list with a dozen requests that ask
>>> the same question.
>>>
>>> By definition, with PME, rlist = rcoulomb.  For CHARMM, use rlistlong =
>>> 1.4; the message that is printed below is an error that has been fixed in
>>> newer versions.
>>
>>
>> Are you sure? Looking at the logic in src/mdlib/read_ir.c, I could not see
>> how Tarak's input could have led (correctly) to that note from grompp. I am
>> thinking that
>> https://github.com/gromacs/gromacs/blob/release-4-5-patches/src/kernel/readir.c#L170
>> is
>> setting rlistlong = rlist, and so
>> https://github.com/gromacs/gromacs/blob/release-4-5-patches/src/kernel/readir.c#L586
>> gets
>> double-crossed.
>>
>> (Note that http://redmine.gromacs.org/issues/1164 pertained to a slightly
>> different issue.)
>>
>> Mark
>> --
>> gmx-users mailing listgmx-users@gromacs.org
>> http://lists.gromacs.org/mailman/listinfo/gmx-users
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Re: [gmx-users] Comparing Gromacs versions

2013-05-17 Thread Djurre de Jong-Bruinink


>The answer is in the log files, in particular the performance summary
>should indicate where is the performance difference. If you post your
>log files somewhere we can probably give further tips on optimizing
>your run configurations.


I put the log files for 72 CPUs, using GMX455, GMX461+group and GMX461+verlet 
here:
http://md.chem.rug.nl/~djurre/logs/N6_gmx455.log
http://md.chem.rug.nl/~djurre/logs/N6_gmx461_group.log
http://md.chem.rug.nl/~djurre/logs/N6_gmx461_verlet.log

It would be great if you could point out some  possible optimizations.


>Note that with such a small system the scaling with the group scheme
>surely becomes limited by imbalance and probably it won't scale much
>further than 72 cores. At the same time, simulations with the verlet
>scheme have shown scaling to below 100 atoms/core.

I tried running on 84 cpus (56PP cores=400 atoms/PP core), but I did get an 
domain decomposition error. Maybe I could optimize -rcon and -dds further, 
however although the scaling to more CPUs is better with the verlet scheme, I 
think you will never win:  with 72 CPUs Verlet is almost as fast as with group 
at 60 CPUs, however compared to 24 cpus the scaling per CPU is already down to 
60%.

But as Mark Abraham mentioned, it might be that my system is just to small to 
get the advantage of scaling that will be there in larger systems.


Groetnis,
Djurre

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Re: [gmx-users] Re: Running Pull Code

2013-05-17 Thread Shima Arasteh


Thanks for your reply.
In fact, I plan to study ion conduction through the peptide inserted in lipid 
membrane and acting as an ion channel. According to the literature, an ion 
across the membrane in less than 20 ns. 
Can I decide upon this information to apply pull code?

You simulated the protofibril structures for 100 ns, in another article 25 ns.
 Ok, if there is not any universal recipe for it, what do you suggest me? Try 
and error? 

 
Sincerely,
Shima


- Original Message -
From: Justin Lemkul 
To: Shima Arasteh ; Discussion list for GROMACS 
users 
Cc: 
Sent: Friday, May 17, 2013 4:02 PM
Subject: Re: [gmx-users] Re: Running Pull Code



On 5/17/13 7:16 AM, Shima Arasteh wrote:
> Thanks for your reply.
> It' s around 5 nano seconds that I ran equilibration time on the system, and 
> the average pressure I see as a result, seems sensible. However I am not sure 
> if this criteria is sufficient? Others suggest to evaluate the box-dimension 
> changes using g_energy code to judge of sufficient equilibration time.
>

The box vectors won't tell you anything more than the pressure will since 
they're related quantities.

The better question is, "What is a suitable starting structure for the system 
of 
interest?"  The umbrella sampling tutorial (which everyone seems to take at 
literal face value as the only way to do things, which it is decidedly not) 
presents a simple, easy-to-understand method.  In the paper I did (upon which I 
based the tutorial), I simulated the protofibril structures for 100 ns before I 
was confident they were suitably stable and representative of viable structures 
for doing SMD and US.  Your mileage will vary and depends on the quality of the 
starting structure and what it is that you hope to determine.  There is no 
magic 
recipe that is universal.

-Justin

> I appreciate your suggestion.
>
>
> Sincerely,
> Shima
>
>
> - Original Message -
> From: Thomas Schlesier 
> To: gmx-users@gromacs.org
> Cc:
> Sent: Friday, May 17, 2013 3:30 PM
> Subject: [gmx-users] Re: Running Pull Code
>
> The three steps (EM, NVT and NPT) are to equilibrate the system. How
> much time these steps need depends on the system. But i would assume a
> ouple of nanosecounds are sufficient for most systems. You could look
> into the literature, how long other people equilibrate systems which are
> similar to ours.
> If the system is equilibrated, you an start to perform the pulling
> simulation to obtain the individual structure for the later umbrella
> sampling.
>
> Greetings
> Thomas
>
> Am 17.05.2013 07:46, schrieb gmx-users-requ...@gromacs.org:
>> Hi,
>>
>> I have a system composed of POPC/peptide/water/ions. I aim to study ion 
>> conduction through the peptide using umbrella sampling.
>> I built the system and ran EM, NVT, NPT successfully, but have not run md 
>> yet. I' d like to know if the system is required of passing a few 
>> nanoseconds md? Or I might be able to go to Umbrella Sampling straight after 
>> NPT?
>> As I studied in Justin's tutorial, running pull code is done after some 
>> typical steps of every simulation ( EM, NVT, NPT). But I dont know if is 
>> correct generally for other systems as well?
>>
>> Would you please give me any suggestions?
>>
>>
>> Thanks in advance.
>> Sincerely,
>> Shima?
>

-- 


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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Re: [gmx-users] Comparing Gromacs versions

2013-05-17 Thread Mark Abraham
On Fri, May 17, 2013 at 2:21 PM, Djurre de Jong-Bruinink <
djurredej...@yahoo.com> wrote:

> >You are doing simulations with a lot of water (and perhaps with charge
> groups),
>
> >and that is the case where an unbuffered group scheme has the best
> performance.
>
> >How much you like the physics is another story.
>
>
> Thank you for your answer. I didn't realize a system like this is already
> in the "lot of water"-regime (it makes sense though, ~95% of the particles
> is water). I could lower the water content a bit by reducing the solute to
> box distance (eg from 1.5 to 1.2/1.0nm), but that only saves a few percent.
> In practice it will mean that for any system containing soluble proteins,
> the group scheme will still be faster? Right?
>

This was what the group kernels were built for. But after a certain number
of cores (as Szilard said), by construction, the group scheme will stop
scaling, and the group and verlet performance curves will certainly cross.
The PME performance also starts to die at large MPI process counts because
of the global inter-PME-node communication, which you can see in the .log
file timing breakdowns. I expect you are not being fair to the Verlet
scheme at high core counts by requiring high MPI process counts by turning
off OpenMP.

Mark


> Groetnis,
> Djurre de Jong
> --
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Re: [gmx-users] Re: Running Pull Code

2013-05-17 Thread Shima Arasteh
Thanks for your reply.
In fact, I plan to study ion conduction through the peptide inserted in lipid 
membrane and acting as an ion channel. According to the literature, an ion 
across the membrane in less than 20 ns. 
Can I decide upon this information to apply pull code?

You simulated the protofibril structures for 100 ns, in another article 25 ns.
 Ok, if there is not any universal recipe for it, what do you suggest me? Try 
and error? 

 
Sincerely,
Shima


- Original Message -
From: Justin Lemkul 
To: Shima Arasteh ; Discussion list for GROMACS 
users 
Cc: 
Sent: Friday, May 17, 2013 4:02 PM
Subject: Re: [gmx-users] Re: Running Pull Code



On 5/17/13 7:16 AM, Shima Arasteh wrote:
> Thanks for your reply.
> It' s around 5 nano seconds that I ran equilibration time on the system, and 
> the average pressure I see as a result, seems sensible. However I am not sure 
> if this criteria is sufficient? Others suggest to evaluate the box-dimension 
> changes using g_energy code to judge of sufficient equilibration time.
>

The box vectors won't tell you anything more than the pressure will since 
they're related quantities.

The better question is, "What is a suitable starting structure for the system 
of 
interest?"  The umbrella sampling tutorial (which everyone seems to take at 
literal face value as the only way to do things, which it is decidedly not) 
presents a simple, easy-to-understand method.  In the paper I did (upon which I 
based the tutorial), I simulated the protofibril structures for 100 ns before I 
was confident they were suitably stable and representative of viable structures 
for doing SMD and US.  Your mileage will vary and depends on the quality of the 
starting structure and what it is that you hope to determine.  There is no 
magic 
recipe that is universal.

-Justin

> I appreciate your suggestion.
>
>
> Sincerely,
> Shima
>
>
> - Original Message -
> From: Thomas Schlesier 
> To: gmx-users@gromacs.org
> Cc:
> Sent: Friday, May 17, 2013 3:30 PM
> Subject: [gmx-users] Re: Running Pull Code
>
> The three steps (EM, NVT and NPT) are to equilibrate the system. How
> much time these steps need depends on the system. But i would assume a
> ouple of nanosecounds are sufficient for most systems. You could look
> into the literature, how long other people equilibrate systems which are
> similar to ours.
> If the system is equilibrated, you an start to perform the pulling
> simulation to obtain the individual structure for the later umbrella
> sampling.
>
> Greetings
> Thomas
>
> Am 17.05.2013 07:46, schrieb gmx-users-requ...@gromacs.org:
>> Hi,
>>
>> I have a system composed of POPC/peptide/water/ions. I aim to study ion 
>> conduction through the peptide using umbrella sampling.
>> I built the system and ran EM, NVT, NPT successfully, but have not run md 
>> yet. I' d like to know if the system is required of passing a few 
>> nanoseconds md? Or I might be able to go to Umbrella Sampling straight after 
>> NPT?
>> As I studied in Justin's tutorial, running pull code is done after some 
>> typical steps of every simulation ( EM, NVT, NPT). But I dont know if is 
>> correct generally for other systems as well?
>>
>> Would you please give me any suggestions?
>>
>>
>> Thanks in advance.
>> Sincerely,
>> Shima?
>

-- 


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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Re: [gmx-users] Comparing Gromacs versions

2013-05-17 Thread Djurre de Jong-Bruinink
>You are doing simulations with a lot of water (and perhaps with charge 
>groups), 

>and that is the case where an unbuffered group scheme has the best 
>performance. 

>How much you like the physics is another story. 


Thank you for your answer. I didn't realize a system like this is already in 
the "lot of water"-regime (it makes sense though, ~95% of the particles is 
water). I could lower the water content a bit by reducing the solute to box 
distance (eg from 1.5 to 1.2/1.0nm), but that only saves a few percent. In 
practice it will mean that for any system containing soluble proteins, the 
group scheme will still be faster? Right?

Groetnis,
Djurre de Jong
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Re: [gmx-users] Inconsistent results in different clusters and cores

2013-05-17 Thread tarak karmakar
I am extremely sorry for spaming the mail box. It was quite
unintentionally. Believe me I was getting the following error every
time while sending the mail.

Final-Recipient: rfc822; jaanus.k...@eesti.ee
Action: failed
Status: 5.0.0
Diagnostic-Code: X-Postfix; mail forwarding loop for jaanus.k...@eesti.ee

Tarak


-- Forwarded message --
From: tarak karmakar 
To: Discussion list for GROMACS users 
Cc:
Date: Fri, 17 May 2013 15:50:25 +0530
Subject: Re: [gmx-users] Inconsistent results in different clusters and cores

On Fri, May 17, 2013 at 5:36 PM, Mark Abraham  wrote:
> On Fri, May 17, 2013 at 1:23 PM, Justin Lemkul  wrote:
>
>>
>>
>> On 5/17/13 6:20 AM, tarak karmakar wrote:
>>
>>> I have read the 'implementation of charmm in gromacs' by bjelkmar,
>>> JCTC. There they have used following cut-offs
>>> coulombtype=PME
>>> rcoulomb=1.2
>>> vdwtype=switch
>>> rvdw=1.2
>>> rvdw-switch=1.0
>>>
>>> I am not sure about rlist.
>>>
>>>
>> It's really unnecessary to spam the list with a dozen requests that ask
>> the same question.
>>
>> By definition, with PME, rlist = rcoulomb.  For CHARMM, use rlistlong =
>> 1.4; the message that is printed below is an error that has been fixed in
>> newer versions.
>
>
> Are you sure? Looking at the logic in src/mdlib/read_ir.c, I could not see
> how Tarak's input could have led (correctly) to that note from grompp. I am
> thinking that
> https://github.com/gromacs/gromacs/blob/release-4-5-patches/src/kernel/readir.c#L170
> is
> setting rlistlong = rlist, and so
> https://github.com/gromacs/gromacs/blob/release-4-5-patches/src/kernel/readir.c#L586
> gets
> double-crossed.
>
> (Note that http://redmine.gromacs.org/issues/1164 pertained to a slightly
> different issue.)
>
> Mark
> --
> gmx-users mailing listgmx-users@gromacs.org
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Re: [gmx-users] Comparing Gromacs versions

2013-05-17 Thread Szilárd Páll
The answer is in the log files, in particular the performance summary
should indicate where is the performance difference. If you post your
log files somewhere we can probably give further tips on optimizing
your run configurations.

Note that with such a small system the scaling with the group scheme
surely becomes limited by imbalance and probably it won't scale much
further than 72 cores. At the same time, simulations with the verlet
scheme have shown scaling to below 100 atoms/core.

Cheers,
--
Szilárd


On Fri, May 17, 2013 at 11:07 AM, Djurre de Jong-Bruinink
 wrote:
> Dear all,
>
> We recently did some comparisons of gmx 4.5.5, 4.6.1+group and 4.6.1+verlet 
> cutoff scheme. The system was a protein (amber99) in water (tip3p) in a 
> triclinic box (23k atoms total). We're using pme with a realspace 
> cutoff=0.9nm, gridspacing=0.12nm, npme=-1, which based on g_tune_pme gives 
> (close to) best performance. Below some performance measure (ns/day) from 
> 100,000 step runs:
>
> CPUs G455G461+group   G461+verlet
> 2434.9  43.1   35.3
> 3647.6  57.8   49.7
> 4850.8  65.9   60.4
> 6059.9  81.8   71.1
> 7257.7  78.7   78.2
>
> The scaling to more CPUs in 4.6.1 is much better (thank you developers for 
> putting up all the hard work!), however I would have expected more 
> improvements from the verlet scheme. Note that both 455 and 461 have been 
> compiled with MPI only (no OMP, GPU), and 461 was compiled with gcc (4.7.2). 
> I did change the nstlist from 5 to 10 for the verlet scheme only.
>
>
> Are these results expected given the setup? Is there anything I'm doing wrong?
>
> Thanks in advance,
> Djurre de Jong
> --
> gmx-users mailing listgmx-users@gromacs.org
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Re: [gmx-users] Inconsistent results in different clusters and cores

2013-05-17 Thread Mark Abraham
On Fri, May 17, 2013 at 1:23 PM, Justin Lemkul  wrote:

>
>
> On 5/17/13 6:20 AM, tarak karmakar wrote:
>
>> I have read the 'implementation of charmm in gromacs' by bjelkmar,
>> JCTC. There they have used following cut-offs
>> coulombtype=PME
>> rcoulomb=1.2
>> vdwtype=switch
>> rvdw=1.2
>> rvdw-switch=1.0
>>
>> I am not sure about rlist.
>>
>>
> It's really unnecessary to spam the list with a dozen requests that ask
> the same question.
>
> By definition, with PME, rlist = rcoulomb.  For CHARMM, use rlistlong =
> 1.4; the message that is printed below is an error that has been fixed in
> newer versions.


Are you sure? Looking at the logic in src/mdlib/read_ir.c, I could not see
how Tarak's input could have led (correctly) to that note from grompp. I am
thinking that
https://github.com/gromacs/gromacs/blob/release-4-5-patches/src/kernel/readir.c#L170
is
setting rlistlong = rlist, and so
https://github.com/gromacs/gromacs/blob/release-4-5-patches/src/kernel/readir.c#L586
gets
double-crossed.

(Note that http://redmine.gromacs.org/issues/1164 pertained to a slightly
different issue.)

Mark
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Re: [gmx-users] Re: REMD analysis

2013-05-17 Thread XAvier Periole

Well use a regular plotting software and look at it or do some more elaborated 
operation in or out the software to estimate the overlap :))

On May 17, 2013, at 1:14 PM, bharat gupta  wrote:

> Dear Sir,
> 
> I ran the REMD simulation with temp. distribution discussed in my last
> thread. Each replica was run for 50 ns
> 
> Replica exchange statistics
> Repl  24999 attempts, 12500 odd, 12499 even
> Repl  average probabilities:
> Repl 0123456789   10   11   12
> Repl  .22  .19  .18  .16  .19  .21  .23  .25  .26  .29  .28  .28
> Repl  number of exchanges:
> Repl 0123456789   10   11   12
> Repl 2661 2369 2296 2008 2360 2668 2866 3119 3234 3549 3469 3475
> Repl  average number of exchanges:
> Repl 0123456789   10   11   12
> Repl  .21  .19  .18  .16  .19  .21  .23  .25  .26  .28  .28  .28
> 
> Now, how to find the potential energy overlap for each replica??.. I have
> obtained the pot. energy for each replica separately..
> 
> -- 
> Bharat
> -- 
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Re: [gmx-users] Re: Running Pull Code

2013-05-17 Thread Justin Lemkul



On 5/17/13 7:16 AM, Shima Arasteh wrote:

Thanks for your reply.
It' s around 5 nano seconds that I ran equilibration time on the system, and 
the average pressure I see as a result, seems sensible. However I am not sure 
if this criteria is sufficient? Others suggest to evaluate the box-dimension 
changes using g_energy code to judge of sufficient equilibration time.



The box vectors won't tell you anything more than the pressure will since 
they're related quantities.


The better question is, "What is a suitable starting structure for the system of 
interest?"  The umbrella sampling tutorial (which everyone seems to take at 
literal face value as the only way to do things, which it is decidedly not) 
presents a simple, easy-to-understand method.  In the paper I did (upon which I 
based the tutorial), I simulated the protofibril structures for 100 ns before I 
was confident they were suitably stable and representative of viable structures 
for doing SMD and US.  Your mileage will vary and depends on the quality of the 
starting structure and what it is that you hope to determine.  There is no magic 
recipe that is universal.


-Justin


I appreciate your suggestion.


Sincerely,
Shima


- Original Message -
From: Thomas Schlesier 
To: gmx-users@gromacs.org
Cc:
Sent: Friday, May 17, 2013 3:30 PM
Subject: [gmx-users] Re: Running Pull Code

The three steps (EM, NVT and NPT) are to equilibrate the system. How
much time these steps need depends on the system. But i would assume a
ouple of nanosecounds are sufficient for most systems. You could look
into the literature, how long other people equilibrate systems which are
similar to ours.
If the system is equilibrated, you an start to perform the pulling
simulation to obtain the individual structure for the later umbrella
sampling.

Greetings
Thomas

Am 17.05.2013 07:46, schrieb gmx-users-requ...@gromacs.org:

Hi,

I have a system composed of POPC/peptide/water/ions. I aim to study ion 
conduction through the peptide using umbrella sampling.
I built the system and ran EM, NVT, NPT successfully, but have not run md yet. 
I' d like to know if the system is required of passing a few nanoseconds md? Or 
I might be able to go to Umbrella Sampling straight after NPT?
As I studied in Justin's tutorial, running pull code is done after some typical 
steps of every simulation ( EM, NVT, NPT). But I dont know if is correct 
generally for other systems as well?

Would you please give me any suggestions?


Thanks in advance.
Sincerely,
Shima?




--


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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Re: [gmx-users] Inconsistent results in different clusters and cores

2013-05-17 Thread Justin Lemkul



On 5/17/13 6:20 AM, tarak karmakar wrote:

I have read the 'implementation of charmm in gromacs' by bjelkmar,
JCTC. There they have used following cut-offs
coulombtype=PME
rcoulomb=1.2
vdwtype=switch
rvdw=1.2
rvdw-switch=1.0

I am not sure about rlist.



It's really unnecessary to spam the list with a dozen requests that ask the same 
question.


By definition, with PME, rlist = rcoulomb.  For CHARMM, use rlistlong = 1.4; the 
message that is printed below is an error that has been fixed in newer versions.


-Justin


On Fri, May 17, 2013 at 1:46 PM, tarak karmakar  wrote:

Now if I increase the rlist it is showing that

With coulombtype = PME, rcoulomb must be equal to rlist
   If you want optimal energy conservation or exact integration
   use PME-Switch

I don't know exactly what will be the best set up with charmm force field.

Any suggestion please!!

Thanks,

Tarak




On Fri, May 17, 2013 at 1:34 PM, tarak karmakar 
wrote:


What about Dispersion Correction ?
But if I use this set of informations

; 7.3.3 Run Control
integrator  = md; md integrator
tinit   = 0 ; [ps] starting time for
run
dt  = 0.001 ; [ps] time step for
integration
nsteps  = 500   ; maximum number of steps
to integrate, 0.001 * 50,00,000 =5 ns
nstcomm = 1 ; [steps] frequency of
mass motion removal
comm_grps   = system; group(s) for center of
mass motion removal

comm_mode   = linear


; 7.3.8 Output Control
nstxout = 5000   ; [steps] freq to write coordinates
to trajectory
nstvout = 5000   ; [steps] freq to write velocities to
trajectory
nstfout = 5000   ; [steps] freq to write forces to
trajectory
nstlog  = 1000  ; [steps] freq to write energies
to log file
nstenergy   = 1000  ; [steps] freq to write energies
to energy file
nstxtcout   = 1000  ; [steps] freq to write
coordinates to xtc trajectory
xtc_precision   = 1000 ; [real] precision to write xtc
trajectory
xtc_grps= System; group(s) to write to xtc
trajectory
energygrps  = protein ligand

; 7.3.9 Neighbor Searching
nstlist = 10; [steps] freq to update neighbor
list
ns_type = grid  ; method of updating neighbor list
pbc = xyz   ; periodic boundary conditions in
all directions
rlist   = 1.2   ; [nm] cut-off distance for the
short-range neighbor list
rlistlong   = 1.4

; 7.3.10 Electrostatics
coulombtype = PME   ; Particle-Mesh Ewald
electrostatics
rcoulomb= 1.2   ; [nm] distance for Coulomb
cut-off
fourierspacing  = 0.16  ; [nm] grid spacing for FFT grid
when using PME
pme_order   = 4 ; interpolation order for PME, 4 =
cubic
ewald_rtol  = 1e-5  ; relative strength of
Ewald-shifted potential at rcoulomb

; 7.3.11 VdW
vdwtype = switch; twin-range cut-off with rlist
where rvdw >= rlist
rvdw= 1.2   ; [nm] distance for LJ cut-off
rvdw-switch = 1.0

DispCorr= Ener  ; apply long range dispersion
corrections for energy


; 7.3.14 Temperature Coupling
tcoupl  = nose-hoover   ; temperature coupling
tc_grps = system; groups to couple seperately to
temperature bath
tau_t   = 1.0   ; [ps] time constant for coupling
ref_t   = 300   ; [K] reference temperature for
coupling

; 7.3.15 Pressure Coupling
pcoupl  = parrinello-rahman ; pressure coupling where
box vectors are variable
pcoupltype  = isotropic ; pressure coupling in
x-y-z directions
tau_p   = 1.0   ; [ps] time constant for
coupling
compressibility = 4.5e-5; [bar^-1] compressibility
ref_p   = 1.0   ; [bar] reference pressure
for coupling

gen_vel = yes ; velocity generation

gen_temp= 300
gen_seed= 8877691

; 7.3.18 Bonds
constraints = h-bonds   ; covalent h-bonds constraints
constraint_algorithm= LINCS ; LINear Constraint Solver
continuation= yes   ; apply constraints to the start
configuration
lincs_order = 4 ; highest order in the expansion
of the contraint coupling matrix
lincs_iter  = 1 ; number of iterations to correct
for rotational lengthening
lincs_warnangle = 30; [degrees] maximum angle that a
bond can rotate before LINCS will complain


It is showing

[gmx-users] Re: REMD analysis

2013-05-17 Thread bharat gupta
Dear Sir,

I ran the REMD simulation with temp. distribution discussed in my last
thread. Each replica was run for 50 ns

Replica exchange statistics
Repl  24999 attempts, 12500 odd, 12499 even
Repl  average probabilities:
Repl 0123456789   10   11   12
Repl  .22  .19  .18  .16  .19  .21  .23  .25  .26  .29  .28  .28
Repl  number of exchanges:
Repl 0123456789   10   11   12
Repl 2661 2369 2296 2008 2360 2668 2866 3119 3234 3549 3469 3475
Repl  average number of exchanges:
Repl 0123456789   10   11   12
Repl  .21  .19  .18  .16  .19  .21  .23  .25  .26  .28  .28  .28

Now, how to find the potential energy overlap for each replica??.. I have
obtained the pot. energy for each replica separately..

-- 
Bharat
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Re: [gmx-users] Re: Running Pull Code

2013-05-17 Thread Shima Arasteh
Thanks for your reply.
It' s around 5 nano seconds that I ran equilibration time on the system, and 
the average pressure I see as a result, seems sensible. However I am not sure 
if this criteria is sufficient? Others suggest to evaluate the box-dimension 
changes using g_energy code to judge of sufficient equilibration time. 

I appreciate your suggestion.


Sincerely,
Shima


- Original Message -
From: Thomas Schlesier 
To: gmx-users@gromacs.org
Cc: 
Sent: Friday, May 17, 2013 3:30 PM
Subject: [gmx-users] Re: Running Pull Code

The three steps (EM, NVT and NPT) are to equilibrate the system. How 
much time these steps need depends on the system. But i would assume a 
ouple of nanosecounds are sufficient for most systems. You could look 
into the literature, how long other people equilibrate systems which are 
similar to ours.
If the system is equilibrated, you an start to perform the pulling 
simulation to obtain the individual structure for the later umbrella 
sampling.

Greetings
Thomas

Am 17.05.2013 07:46, schrieb gmx-users-requ...@gromacs.org:
> Hi,
>
> I have a system composed of POPC/peptide/water/ions. I aim to study ion 
> conduction through the peptide using umbrella sampling.
> I built the system and ran EM, NVT, NPT successfully, but have not run md 
> yet. I' d like to know if the system is required of passing a few nanoseconds 
> md? Or I might be able to go to Umbrella Sampling straight after NPT?
> As I studied in Justin's tutorial, running pull code is done after some 
> typical steps of every simulation ( EM, NVT, NPT). But I dont know if is 
> correct generally for other systems as well?
>
> Would you please give me any suggestions?
>
>
> Thanks in advance.
> Sincerely,
> Shima?

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Re: [gmx-users] Comparing Gromacs versions

2013-05-17 Thread Mark Abraham
On Fri, May 17, 2013 at 11:07 AM, Djurre de Jong-Bruinink <
djurredej...@yahoo.com> wrote:

> Dear all,
>
> We recently did some comparisons of gmx 4.5.5, 4.6.1+group and
> 4.6.1+verlet cutoff scheme. The system was a protein (amber99) in water
> (tip3p) in a triclinic box (23k atoms total). We're using pme with a
> realspace cutoff=0.9nm, gridspacing=0.12nm, npme=-1, which based on
> g_tune_pme gives (close to) best performance. Below some performance
> measure (ns/day) from 100,000 step runs:
>
> CPUs G455G461+group   G461+verlet
> 2434.9  43.1   35.3
> 3647.6  57.8   49.7
> 4850.8  65.9   60.4
> 6059.9  81.8   71.1
> 7257.7  78.7   78.2
>
> The scaling to more CPUs in 4.6.1 is much better (thank you developers for
> putting up all the hard work!), however I would have expected more
> improvements from the verlet scheme.


You are doing simulations with a lot of water (and perhaps with charge
groups), and that is the case where an unbuffered group scheme has the best
performance. How much you like the physics is another story. See
http://www.gromacs.org/Documentation/Acceleration_and_parallelization and
http://www.gromacs.org/Documentation/Cut-off_schemes

Note that both 455 and 461 have been compiled with MPI only (no OMP, GPU),
> and 461 was compiled with gcc (4.7.2). I did change the nstlist from 5 to
> 10 for the verlet scheme only.
>
>
> Are these results expected given the setup? Is there anything I'm doing
> wrong?
>

I am not aware of a case where compiling without OpenMP is
necessary/desirable for maximum performance. Whether you should use it (and
how many OpenMP threads to use) depends on lots of things, particularly
including what hardware you use and the atoms/core. You should experiment
if you want maximum performance.

Mark


> Thanks in advance,
> Djurre de Jong
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[gmx-users] Re: Running Pull Code

2013-05-17 Thread Thomas Schlesier
The three steps (EM, NVT and NPT) are to equilibrate the system. How 
much time these steps need depends on the system. But i would assume a 
ouple of nanosecounds are sufficient for most systems. You could look 
into the literature, how long other people equilibrate systems which are 
similar to ours.
If the system is equilibrated, you an start to perform the pulling 
simulation to obtain the individual structure for the later umbrella 
sampling.


Greetings
Thomas

Am 17.05.2013 07:46, schrieb gmx-users-requ...@gromacs.org:

Hi,

I have a system composed of POPC/peptide/water/ions. I aim to study ion 
conduction through the peptide using umbrella sampling.
I built the system and ran EM, NVT, NPT successfully, but have not run md yet. 
I' d like to know if the system is required of passing a few nanoseconds md? Or 
I might be able to go to Umbrella Sampling straight after NPT?
As I studied in Justin's tutorial, running pull code is done after some typical 
steps of every simulation ( EM, NVT, NPT). But I dont know if is correct 
generally for other systems as well?

Would you please give me any suggestions?


Thanks in advance.
Sincerely,
Shima?


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Re: [gmx-users] Inconsistent results in different clusters and cores

2013-05-17 Thread tarak karmakar
I have read the 'implementation of charmm in gromacs' by bjelkmar,
JCTC. There they have used following cut-offs
coulombtype=PME
rcoulomb=1.2
vdwtype=switch
rvdw=1.2
rvdw-switch=1.0

I am not sure about rlist.

Regards,
Tarak


On Fri, May 17, 2013 at 1:46 PM, tarak karmakar  wrote:
> Now if I increase the rlist it is showing that
>
> With coulombtype = PME, rcoulomb must be equal to rlist
>   If you want optimal energy conservation or exact integration
>   use PME-Switch
>
> I don't know exactly what will be the best set up with charmm force field.
>
> Any suggestion please!!
>
> Thanks,
>
> Tarak
>
>
>
>
> On Fri, May 17, 2013 at 1:34 PM, tarak karmakar 
> wrote:
>>
>> What about Dispersion Correction ?
>> But if I use this set of informations
>>
>> ; 7.3.3 Run Control
>> integrator  = md; md integrator
>> tinit   = 0 ; [ps] starting time for
>> run
>> dt  = 0.001 ; [ps] time step for
>> integration
>> nsteps  = 500   ; maximum number of steps
>> to integrate, 0.001 * 50,00,000 =5 ns
>> nstcomm = 1 ; [steps] frequency of
>> mass motion removal
>> comm_grps   = system; group(s) for center of
>> mass motion removal
>>
>> comm_mode   = linear
>>
>>
>> ; 7.3.8 Output Control
>> nstxout = 5000   ; [steps] freq to write coordinates
>> to trajectory
>> nstvout = 5000   ; [steps] freq to write velocities to
>> trajectory
>> nstfout = 5000   ; [steps] freq to write forces to
>> trajectory
>> nstlog  = 1000  ; [steps] freq to write energies
>> to log file
>> nstenergy   = 1000  ; [steps] freq to write energies
>> to energy file
>> nstxtcout   = 1000  ; [steps] freq to write
>> coordinates to xtc trajectory
>> xtc_precision   = 1000 ; [real] precision to write xtc
>> trajectory
>> xtc_grps= System; group(s) to write to xtc
>> trajectory
>> energygrps  = protein ligand
>>
>> ; 7.3.9 Neighbor Searching
>> nstlist = 10; [steps] freq to update neighbor
>> list
>> ns_type = grid  ; method of updating neighbor list
>> pbc = xyz   ; periodic boundary conditions in
>> all directions
>> rlist   = 1.2   ; [nm] cut-off distance for the
>> short-range neighbor list
>> rlistlong   = 1.4
>>
>> ; 7.3.10 Electrostatics
>> coulombtype = PME   ; Particle-Mesh Ewald
>> electrostatics
>> rcoulomb= 1.2   ; [nm] distance for Coulomb
>> cut-off
>> fourierspacing  = 0.16  ; [nm] grid spacing for FFT grid
>> when using PME
>> pme_order   = 4 ; interpolation order for PME, 4 =
>> cubic
>> ewald_rtol  = 1e-5  ; relative strength of
>> Ewald-shifted potential at rcoulomb
>>
>> ; 7.3.11 VdW
>> vdwtype = switch; twin-range cut-off with rlist
>> where rvdw >= rlist
>> rvdw= 1.2   ; [nm] distance for LJ cut-off
>> rvdw-switch = 1.0
>>
>> DispCorr= Ener  ; apply long range dispersion
>> corrections for energy
>>
>>
>> ; 7.3.14 Temperature Coupling
>> tcoupl  = nose-hoover   ; temperature coupling
>> tc_grps = system; groups to couple seperately to
>> temperature bath
>> tau_t   = 1.0   ; [ps] time constant for coupling
>> ref_t   = 300   ; [K] reference temperature for
>> coupling
>>
>> ; 7.3.15 Pressure Coupling
>> pcoupl  = parrinello-rahman ; pressure coupling where
>> box vectors are variable
>> pcoupltype  = isotropic ; pressure coupling in
>> x-y-z directions
>> tau_p   = 1.0   ; [ps] time constant for
>> coupling
>> compressibility = 4.5e-5; [bar^-1] compressibility
>> ref_p   = 1.0   ; [bar] reference pressure
>> for coupling
>>
>> gen_vel = yes ; velocity generation
>>
>> gen_temp= 300
>> gen_seed= 8877691
>>
>> ; 7.3.18 Bonds
>> constraints = h-bonds   ; covalent h-bonds constraints
>> constraint_algorithm= LINCS ; LINear Constraint Solver
>> continuation= yes   ; apply constraints to the start
>> configuration
>> lincs_order = 4 ; highest order in the expansion
>> of the contraint coupling matrix
>> lincs_iter  = 1 ; number of iterations to correct
>> for rotational lengthening
>> lincs_warnangle = 30; [degrees] maximum angle that a
>> bond can rotate before LINCS w

[gmx-users] cut-offs

2013-05-17 Thread tarak karmakar
Dear All,

I have read the 'implementation of charmm in gromacs' by bjelkmar,
JCTC. There they have used following cut-offs
coulombtype=PME
rcoulomb=1.2
vdwtype=switch
rvdw=1.2
rvdw-switch=1.0

If I use the same numbers with rlist=1.2 it is showing warning saying
rlist should be at lear 0.1 - 0.3 nm larger to get proper conservation
of energy. Now, changing the rlist enforces to change the rcoulomb.
Can anyone please suggest the best possible combination of these numbers?

Thanks,
Tarak
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[gmx-users] CHARMM lipid parameters

2013-05-17 Thread Venkat Reddy
Dear all,
How can I generate a particular lipid itp file compatible with CHARMM27
(say Cholesteryl oleate). The link for CHARMM compatible cholesterol
parameters in  the lipidbook website is
also dead.

Thanks a lot

-- 
With Best Wishes
Venkat Reddy Chirasani
PhD student
Laboratory of Computational Biophysics
Department of Biotechnology
IIT Madras
Chennai
INDIA-600036
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[gmx-users] (no subject)

2013-05-17 Thread Sathish Kumar
Sir,
   I want to do pulling simulations for membrane protein and gold
nanoparticles. Can you please suggest me some tutorials for calculating
youngs modules ,stress and strain.
  Thank You

-- 
regards
M.SathishKumar
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[gmx-users] pulling simulations

2013-05-17 Thread Sathish Kumar
Sir,
   I want to do pulling simulations for membrane protein and gold
nanoparticles. Can you please suggest me some tutorials.
  Thank You
-- 
regards
M.SathishKumar
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Re: [gmx-users] puuling simulations

2013-05-17 Thread Shima Arasteh
http://www.gromacs.org/Documentation/Tutorials

 
Sincerely,
Shima


- Original Message -
From: Sathish Kumar 
To: Discussion list for GROMACS users 
Cc: 
Sent: Friday, May 17, 2013 2:08 PM
Subject: [gmx-users] puuling simulations

Sir,
       I want to do pulling simulations for membrane protein and gold
nanoparticles. Can you please suggest me some tutorials.
                      Thank You
-- 
regards
M.SathishKumar
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[gmx-users] Fwd: puuling simulations

2013-05-17 Thread Sathish Kumar
Sir,
   I want to do pulling simulations for membrane protein and gold
nanoparticles. Can you please suggest me some tutorials.
  Thank You
-- 
regards
M.SathishKumar



-- 
regards
M.SathishKumar
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[gmx-users] puuling simulations

2013-05-17 Thread Sathish Kumar
Sir,
   I want to do pulling simulations for membrane protein and gold
nanoparticles. Can you please suggest me some tutorials.
  Thank You
-- 
regards
M.SathishKumar
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[gmx-users] charmm in gromacs cut-offs

2013-05-17 Thread tarak karmakar
Dear All,

I'm using charmm force field for simulation of a protein ligand system.
I have read the paper "implementation of charmm in gromacs by Bjelkmar,
JCTC'
They have used the following set up

coulombtype = PME
rcoulomb= 1.2


vdwtype = switch
rvdw= 1.2
rvdw-switch = 1.0

Now, with this same set up if I use

rlist = 1.2
rlistlong =1.4

It is showing the following warning


  "For energy conservation with switch/shift potentials, rlist should be 0.1
  to 0.3 nm larger than rvdw."


Now, if I try to increase the rlist as rlist =1.3
Coulomb part is showing warning as

"With coulombtype = PME, rcoulomb must
be equal to rlist**   If you want optimal energy conservation or exact
integration use** PME-Switch*"

I read few posts in this issue
But the point, if I use rlist=rvdw then the dynamics will not be proper as
in the neighbor list updating and energy calculations. Now, the any kind of
change in the rlist essentially enforcing to change the coul cut-off. So,
rlist and coul-cut-off are not independent of each other.

Can any one suggest me the best possible use of these parameters?
I am using gromacs-4.5.5 for simulations.

Thanks,
Tarak
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[gmx-users] Cholesteryl oleate parameters for CHARMM27 ff in Gromacs

2013-05-17 Thread Venkat Reddy
Dear all,
How can I generate a particular lipid itp file compatible with CHARMM27
(say Cholesteryl oleate). The link for CHARMM compatible cholesterol
parameters in  *lipidbook *website is
also dead.

Thanks a lot
-- 
With Best Wishes
Venkat Reddy Chirasani
PhD student
Laboratory of Computational Biophysics
Department of Biotechnology
IIT Madras
Chennai
INDIA-600036
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[gmx-users] charmm in gromacs cut-offs

2013-05-17 Thread tarak karmakar
Dear All,

I'm using charmm force field for simulation of a protein ligand system.
I have read the paper "implementation of charmm in gromacs by Bjelkmar,
JCTC'
They have used the following set up

coulombtype = PME
rcoulomb= 1.2


vdwtype = switch
rvdw= 1.2
rvdw-switch = 1.0

Now, with this same set up if I use

rlist = 1.2
rlistlong =1.4

It is showing the following warning


  "For energy conservation with switch/shift potentials, rlist should be 0.1
  to 0.3 nm larger than rvdw."


Now, if I try to increase the rlist as rlist =1.3
Coulomb part is showing warning as

"With coulombtype = PME, rcoulomb must
be equal to rlist**   If you want optimal energy conservation or exact
integration use** PME-Switch*"

I read few posts in this issue
But the point, if I use rlist=rvdw then the dynamics will not be proper as
in the neighbor list updating and energy calculations. Now, the any kind of
change in the rlist essentially enforcing to change the coul cut-off. So,
rlist and coul-cut-off are not independent of each other.

Can any one suggest me the best possible use of these parameters?
I am using gromacs-4.5.5 for simulations.

Thanks,
Tarak
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[gmx-users] charmm in gromacs cut-offs

2013-05-17 Thread tarak karmakar
Dear All,

I'm using charmm force field for simulation of a protein ligand system.
I have read the paper "implementation of charmm in gromacs by Bjelkmar,
JCTC'
They have used the following set up

coulombtype = PME
rcoulomb= 1.2


vdwtype = switch
rvdw= 1.2
rvdw-switch = 1.0

Now, with this same set up if I use

rlist = 1.2
rlistlong =1.4

It is showing the following warning


  "For energy conservation with switch/shift potentials, rlist should be 0.1
  to 0.3 nm larger than rvdw."


Now, if I try to increase the rlist as rlist =1.3
Coulomb part is showing warning as

"With coulombtype = PME, rcoulomb must
be equal to rlist**   If you want optimal energy conservation or exact
integration use** PME-Switch*"


I came across this post in the mailing list
http://lists.gromacs.org/pipermail/gmx-users/2013-February/079037.html

But the point, if I use rlist=rvdw then the dynamics will not be proper as
in the neighbor list updating and energy calculations.

Can any one suggest me the best possible use of these parameters?
I am using gromacs-4.5.5 for simulations.

Thanks,
Tarak
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[gmx-users] charmm in gromacs cut-offs

2013-05-17 Thread tarak karmakar
Dear All,

I'm using charmm force field for simulation of a protein ligand system.
I have read the paper "implementation of charmm in gromacs by Bjelkmar,
JCTC'
They have used the following set up

coulombtype = PME
rcoulomb= 1.2


vdwtype = switch
rvdw= 1.2
rvdw-switch = 1.0

Now, with this same set up if I use

rlist = 1.2
rlistlong =1.4

It is showing the following warning


  "For energy conservation with switch/shift potentials, rlist should be 0.1
  to 0.3 nm larger than rvdw."


Now, if I try to increase the rlist as rlist =1.3
Coulomb part is showing warning as

"With coulombtype = PME, rcoulomb must
be equal to rlist**   If you want optimal energy conservation or exact
integration use** PME-Switch*"


I came across this post in the mailing list
http://lists.gromacs.org/pipermail/gmx-users/2013-February/079037.html

But the point, if I use rlist=rvdw then the dynamics will not be proper as
in the neighbor list updating and energy calculations.

Can any one suggest me the best possible use of these parameters?
I am using gromacs-4.5.5 for simulations.

Thanks,
Tarak
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[gmx-users] Comparing Gromacs versions

2013-05-17 Thread Djurre de Jong-Bruinink
Dear all,

We recently did some comparisons of gmx 4.5.5, 4.6.1+group and 4.6.1+verlet 
cutoff scheme. The system was a protein (amber99) in water (tip3p) in a 
triclinic box (23k atoms total). We're using pme with a realspace cutoff=0.9nm, 
gridspacing=0.12nm, npme=-1, which based on g_tune_pme gives (close to) best 
performance. Below some performance measure (ns/day) from 100,000 step runs:

CPUs     G455    G461+group   G461+verlet
24    34.9  43.1   35.3
36    47.6  57.8   49.7
48    50.8  65.9   60.4
60    59.9  81.8   71.1
72    57.7  78.7   78.2

The scaling to more CPUs in 4.6.1 is much better (thank you developers for 
putting up all the hard work!), however I would have expected more improvements 
from the verlet scheme. Note that both 455 and 461 have been compiled with MPI 
only (no OMP, GPU), and 461 was compiled with gcc (4.7.2). I did change the 
nstlist from 5 to 10 for the verlet scheme only.


Are these results expected given the setup? Is there anything I'm doing wrong?

Thanks in advance,
Djurre de Jong
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[gmx-users] charmm in gromacs cut-offs

2013-05-17 Thread tarak karmakar
Dear All,

I'm using charmm force field for simulation of a protein ligand system.
I have read the paper "implementation of charmm in gromacs by Bjelkmar,
JCTC'
They have used the following set up

coulombtype = PME
rcoulomb= 1.2


vdwtype = switch
rvdw= 1.2
rvdw-switch = 1.0

Now, with this same set up if I use

rlist = 1.2
rlistlong =1.4

It is showing the following warning

NOTE 1 [file 02md.mdp]:
  For energy conservation with switch/shift potentials, rlist should be 0.1
  to 0.3 nm larger than rvdw.


Now, if I try to increase the rlist as rlist =1.3
Coulomb part is showing warning as

*ERROR 1 [file 02md.mdp]:**With coulombtype = PME, rcoulomb must
be equal to rlist**   If you want optimal energy conservation or exact
integration use** PME-Switch*


I came across this post in the mailing list
http://lists.gromacs.org/pipermail/gmx-users/2013-February/079037.html

But the point, if I use rlist=rvdw then the dynamics will not be proper as
in the neighbor list updating and energy calculations.

Can any one suggest me the best possible use of these parameters?
I am using gromacs-4.5.5 for simulations.

Thanks,
Tarak
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[gmx-users] charmm in gromacs cut-offs

2013-05-17 Thread tarak karmakar
Dear All,

I'm using charmm force field for simulation of a protein ligand system.
I have read the paper "implementation of charmm in gromacs by Bjelkmar,
JCTC'
They have used the following set up

coulombtype = PME
rcoulomb= 1.2


vdwtype = switch
rvdw= 1.2
rvdw-switch = 1.0

Now, with this same set up if I use

rlist = 1.2
rlistlong =1.4

It is showing the following warning

NOTE 1 [file 02md.mdp]:
  For energy conservation with switch/shift potentials, rlist should be 0.1
  to 0.3 nm larger than rvdw.


Now, if I try to increase the rlist as rlist =1.3
Coulomb part is showing warning as

*ERROR 1 [file 02md.mdp]:**With coulombtype = PME, rcoulomb must
be equal to rlist**   If you want optimal energy conservation or exact
integration use** PME-Switch*


I came across this post in the mailing list
http://lists.gromacs.org/pipermail/gmx-users/2013-February/079037.html

But the point, if I use rlist=rvdw then the dynamics will not be proper as
in the neighbor list updating and energy calculations.

Can any one suggest me the best possible use of these parameters?
I am using gromacs-4.5.5 for simulations.

Thanks,
Tarak
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Re: [gmx-users] 1-4 scaling factor

2013-05-17 Thread Mark Abraham
See chapter 5

Mark
On May 17, 2013 8:25 AM, "tarak karmakar"  wrote:

> Dear All,
>
> How do I incorporate the 1-4 scaling factor ( e.g., 1.0 for CHARMM and
> 0.833 in AMBER) in gromacs? Or, is it internally taken care of by gromacs
> while specifying the -ff flag?
>
> NAMD input file uses the following keyword
>
> 1-4scaling  1.0 (for charmm force field)
>
>
> Thanks,
> Tarak
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Re: [gmx-users] Reduced Units

2013-05-17 Thread Mark Abraham
I don't understand what you are asking for.

Mark
On May 17, 2013 7:59 AM, "Rasoul Nasiri"  wrote:

> Are you sure lattice cell set up in f.c.c structure has been explained
> there for the positions of molecules?
>
>
>
>
> On Thu, May 16, 2013 at 3:28 PM, Mark Abraham  >wrote:
>
> > Does manual 2.3 help?
> >
> >
> > On Thu, May 16, 2013 at 2:51 PM, Rasoul Nasiri 
> > wrote:
> >
> > > Hi All,
> > >
> > > Has anyone performed MD simulation on fluids in reduced units with
> > GROMACS?
> > > I just wandering how the obtained density values through the box should
> > be
> > > converted in the SI unit (Kg/m3).
> > >
> > > Thanks
> > > Rasoul
> > > --
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> > >
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Re: [gmx-users] Inconsistent results in different clusters and cores

2013-05-17 Thread tarak karmakar
Now if I increase the rlist it is showing that

With coulombtype = PME, rcoulomb must be equal to rlist
  If you want optimal energy conservation or exact integration
  use PME-Switch

I don't know exactly what will be the best set up with charmm force field.

Any suggestion please!!

Thanks,

Tarak




On Fri, May 17, 2013 at 1:34 PM, tarak karmakar wrote:

> What about Dispersion Correction ?
> But if I use this set of informations
>
> ; 7.3.3 Run Control
> integrator  = md; md integrator
> tinit   = 0 ; [ps] starting time for
> run
> dt  = 0.001 ; [ps] time step for
> integration
> nsteps  = 500   ; maximum number of steps
> to integrate, 0.001 * 50,00,000 =5 ns
> nstcomm = 1 ; [steps] frequency of
> mass motion removal
> comm_grps   = system; group(s) for center of
> mass motion removal
>
> comm_mode   = linear
>
>
> ; 7.3.8 Output Control
> nstxout = 5000   ; [steps] freq to write coordinates
> to trajectory
> nstvout = 5000   ; [steps] freq to write velocities to
> trajectory
> nstfout = 5000   ; [steps] freq to write forces to
> trajectory
> nstlog  = 1000  ; [steps] freq to write energies
> to log file
> nstenergy   = 1000  ; [steps] freq to write energies
> to energy file
> nstxtcout   = 1000  ; [steps] freq to write
> coordinates to xtc trajectory
> xtc_precision   = 1000 ; [real] precision to write xtc
> trajectory
> xtc_grps= System; group(s) to write to xtc
> trajectory
> energygrps  = protein ligand
>
> ; 7.3.9 Neighbor Searching
> nstlist = 10; [steps] freq to update neighbor
> list
> ns_type = grid  ; method of updating neighbor list
> pbc = xyz   ; periodic boundary conditions in
> all directions
> rlist   = 1.2   ; [nm] cut-off distance for the
> short-range neighbor list
> rlistlong   = 1.4
>
> ; 7.3.10 Electrostatics
> coulombtype = PME   ; Particle-Mesh Ewald
> electrostatics
> rcoulomb= 1.2   ; [nm] distance for Coulomb cut-off
> fourierspacing  = 0.16  ; [nm] grid spacing for FFT grid
> when using PME
> pme_order   = 4 ; interpolation order for PME, 4 =
> cubic
> ewald_rtol  = 1e-5  ; relative strength of
> Ewald-shifted potential at rcoulomb
>
> ; 7.3.11 VdW
> vdwtype = switch; twin-range cut-off with rlist
> where rvdw >= rlist
> rvdw= 1.2   ; [nm] distance for LJ cut-off
> rvdw-switch = 1.0
>
> DispCorr= Ener  ; apply long range dispersion
> corrections for energy
>
>
> ; 7.3.14 Temperature Coupling
> tcoupl  = nose-hoover   ; temperature coupling
> tc_grps = system; groups to couple seperately to
> temperature bath
> tau_t   = 1.0   ; [ps] time constant for coupling
> ref_t   = 300   ; [K] reference temperature for
> coupling
>
> ; 7.3.15 Pressure Coupling
> pcoupl  = parrinello-rahman ; pressure coupling where
> box vectors are variable
> pcoupltype  = isotropic ; pressure coupling in
> x-y-z directions
> tau_p   = 1.0   ; [ps] time constant for
> coupling
> compressibility = 4.5e-5; [bar^-1] compressibility
> ref_p   = 1.0   ; [bar] reference pressure
> for coupling
>
> gen_vel = yes ; velocity generation
>
> gen_temp= 300
> gen_seed= 8877691
>
> ; 7.3.18 Bonds
> constraints = h-bonds   ; covalent h-bonds constraints
> constraint_algorithm= LINCS ; LINear Constraint Solver
> continuation= yes   ; apply constraints to the start
> configuration
> lincs_order = 4 ; highest order in the expansion
> of the contraint coupling matrix
> lincs_iter  = 1 ; number of iterations to correct
> for rotational lengthening
> lincs_warnangle = 30; [degrees] maximum angle that a
> bond can rotate before LINCS will complain
>
>
> It is showing the following warning
>
> "For energy conservation with switch/shift potentials, rlist should be 0.1
>   to 0.3 nm larger than rvdw."
>
>
>
>
>
>
> On Sun, May 12, 2013 at 11:57 PM, tarak karmakar wrote:
>
>> Oh !
>> Thanks a lot Justin. I'll rerun all my jobs with this corrected mdp.
>> Restrains things I didn't follow properly, anyway I'll read about this.
>>
>>
>> On Sun, May 12, 2013

Re: [gmx-users] Inconsistent results in different clusters and cores

2013-05-17 Thread tarak karmakar
What about Dispersion Correction ?
But if I use this set of informations

; 7.3.3 Run Control
integrator  = md; md integrator
tinit   = 0 ; [ps] starting time for run
dt  = 0.001 ; [ps] time step for
integration
nsteps  = 500   ; maximum number of steps
to integrate, 0.001 * 50,00,000 =5 ns
nstcomm = 1 ; [steps] frequency of mass
motion removal
comm_grps   = system; group(s) for center of
mass motion removal
comm_mode   = linear


; 7.3.8 Output Control
nstxout = 5000   ; [steps] freq to write coordinates to
trajectory
nstvout = 5000   ; [steps] freq to write velocities to
trajectory
nstfout = 5000   ; [steps] freq to write forces to
trajectory
nstlog  = 1000  ; [steps] freq to write energies to
log file
nstenergy   = 1000  ; [steps] freq to write energies to
energy file
nstxtcout   = 1000  ; [steps] freq to write coordinates
to xtc trajectory
xtc_precision   = 1000 ; [real] precision to write xtc
trajectory
xtc_grps= System; group(s) to write to xtc
trajectory
energygrps  = protein ligand

; 7.3.9 Neighbor Searching
nstlist = 10; [steps] freq to update neighbor
list
ns_type = grid  ; method of updating neighbor list
pbc = xyz   ; periodic boundary conditions in
all directions
rlist   = 1.2   ; [nm] cut-off distance for the
short-range neighbor list
rlistlong   = 1.4

; 7.3.10 Electrostatics
coulombtype = PME   ; Particle-Mesh Ewald electrostatics
rcoulomb= 1.2   ; [nm] distance for Coulomb cut-off
fourierspacing  = 0.16  ; [nm] grid spacing for FFT grid
when using PME
pme_order   = 4 ; interpolation order for PME, 4 =
cubic
ewald_rtol  = 1e-5  ; relative strength of
Ewald-shifted potential at rcoulomb

; 7.3.11 VdW
vdwtype = switch; twin-range cut-off with rlist
where rvdw >= rlist
rvdw= 1.2   ; [nm] distance for LJ cut-off
rvdw-switch = 1.0

DispCorr= Ener  ; apply long range dispersion
corrections for energy


; 7.3.14 Temperature Coupling
tcoupl  = nose-hoover   ; temperature coupling
tc_grps = system; groups to couple seperately to
temperature bath
tau_t   = 1.0   ; [ps] time constant for coupling
ref_t   = 300   ; [K] reference temperature for
coupling

; 7.3.15 Pressure Coupling
pcoupl  = parrinello-rahman ; pressure coupling where
box vectors are variable
pcoupltype  = isotropic ; pressure coupling in
x-y-z directions
tau_p   = 1.0   ; [ps] time constant for
coupling
compressibility = 4.5e-5; [bar^-1] compressibility
ref_p   = 1.0   ; [bar] reference pressure
for coupling

gen_vel = yes ; velocity generation
gen_temp= 300
gen_seed= 8877691

; 7.3.18 Bonds
constraints = h-bonds   ; covalent h-bonds constraints
constraint_algorithm= LINCS ; LINear Constraint Solver
continuation= yes   ; apply constraints to the start
configuration
lincs_order = 4 ; highest order in the expansion of
the contraint coupling matrix
lincs_iter  = 1 ; number of iterations to correct
for rotational lengthening
lincs_warnangle = 30; [degrees] maximum angle that a
bond can rotate before LINCS will complain


It is showing the following warning

"For energy conservation with switch/shift potentials, rlist should be 0.1
  to 0.3 nm larger than rvdw."






On Sun, May 12, 2013 at 11:57 PM, tarak karmakar wrote:

> Oh !
> Thanks a lot Justin. I'll rerun all my jobs with this corrected mdp.
> Restrains things I didn't follow properly, anyway I'll read about this.
>
>
> On Sun, May 12, 2013 at 11:27 PM, Justin Lemkul  wrote:
>
>>
>>
>> On 5/12/13 1:53 PM, tarak karmakar wrote:
>>
>>> Thanks,
>>>
>>> I have used CGENFF force field parameters for the ligand generated from
>>> PARMCHEM with 0 penalties. For protein I have used CHARMM36 force field.
>>> my npt.mdp file is as follows,
>>>
>>> ; 7.3.3 Run Control
>>> integrator  = md
>>>
>>
>> Bug 1021 was only relevant with md-vv, so it is not your problem here.
>>
>>
>>  tinit   = 0
>>> dt  = 0.001
>>> nsteps  = 500
>>> nstcomm = 1

Re: [gmx-users] Hydrogen Bond analysis using Gromacs

2013-05-17 Thread Erik Marklund
HI,

s0, s1,… is (xm)grace codes that refer to the different datasets in the file. 
Gromacs prints the datasets as different columns. I suggest opening the file 
with xmgrace -nxy yourxvgfile.xvg. As for the -life option, the results are 
based on a too wimple kinetic model for most applications.

Erik

On 17 May 2013, at 08:21, Keerthana S.P Periasamy  
wrote:

> 
> 
> Hai
> In Hydrogen Bonding Analysis, I  want to know about the the 
> interpretation of   option -life and  -ac (autocorrelation) I cannot 
> understand what the columns P(t) and t p(t)  describe and how to interpret 
> this. Similarly after tagging -ac option in .xvg file I am getting@ s0 
> legend "Ac\sfin sys\v{}\z{}(t)"
>  @ s1 legend "Ac(t)"
>  @ s2 legend "Cc\scontact,hb\v{}\z{}(t)"   @ s3 legend "-dAc\sfs\v{}\z{}/dt"  
>   i also want to know what these s0 to s3 specify and how to interpret 
> this.Please help me to get cleared of my doubts so that I can continue 
> further.   Thanks in Advance
> with regardsKeerthanaPeriasamy
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