Re: [gmx-users] Interaction energy

2011-10-18 Thread Steven Neumann
On Mon, Oct 17, 2011 at 6:02 PM, Justin A. Lemkul jalem...@vt.edu wrote:



 Steven Neumann wrote:

 Dear Gmx Users,
  I would like to calculate the interaction energy (LJ and electrostatic)
 between each residue and my ligands (10 ligands in the system). I would like
 to see what is the contribution of electrostatic and vdW interactions
 between ligand and each of my residue. I thought to use g_energy and specify
 each of my residues in index files but it is not possible. Will you suggest
 how to do this?



 For such information, you have to specify these groups as energygrps in the
 .mdp file.  You can rerun the trajectory using mdrun -rerun and a new .tpr
 file specifying these groups, but depending on the output frequency, the
 result may not be as accurate as you'd like.

 -Justin


Thank you Justin. Now I have two groups sepcified in my mdp file:

energygrps = Protein LIG

How can I specify each residue of my protein separately and each ligand? In
my md.gro file I have residues:

 91GLY 92TYR . 161LIG 162LIG...


Will it be correct like this

energygrps = 91GLY 92 TYR ... 161LIG 162LIG...

If yes, will this simulation take longer? Thank you

Steven
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Re: [gmx-users] solvents in gmx

2011-10-18 Thread David van der Spoel

On 2011-10-17 22:58, Justin A. Lemkul wrote:



Yao Yao wrote:

Hi Gmxers,

Is there a way I can check all the kinds of solvents in gromacs? Apart
from water, ethanol, ...,
are there any Glycerol, Treholose, 



There likely aren't many. Anything available would be in the force field
subdirectory for whatever force field you want. Others may be available
on the User Contributions section of the Gromacs website.

-Justin

We have just submitted a paper about organic liquids. We provide boxes 
for 146 liquids and corresponding topologies. The systems have been 
equilibrated using GAFF and OPLS/AA. You can find these boxes at 
http://virtualchemistry.org. Please check back later for information on 
the corresponding paper.


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

2011-10-18 Thread James Starlight
Dear Justin,

Indeed I didnt take into account square degree so all values presented in
the tutorial exactly true so this was exactly my mistake. :(

After some iterations I've obtained value for S per lipid beetween 0.65-0.71
A^2.  This is the example of the system wich I've obtained after solvation
and futher minimization. http://www.sendspace.com/file/h6urhq  It looks
good. :)  By the way I'd like to know about correct value for the S per
protein ? Where I can obtain such information for my protein ? ( e.g for big
proteins such receptors and channels )

The error with GenBox was due to the big vdv R for the carbons. It's
intresting that I couldnt increase this value mush as 1.2. But my finally
system didnt consist of some water within the membrane so I supose that it's
good.

Now my system on the stage of the equilibtation so I have not any questions
yet but I only wounder to know about teqnique of the force fied preparation
for the membrane protein simulation.

In this work I've done this step in accordance with the tutorial. On the
last stage I've copied  gromos53a6_lipid.ff directory in $GMXLIB so now I
can use it in pdb2gmx for instance.
But when I've tried to make gro and top files for my  lipid.pdb via pdb2gmx
I've obtained errors that Residue 'DPP' not found in residue topology
database so I think that in addition to the operations wich I've already
done I should also make some changes in the
/gromos53a6_lipid.ff/aminoacids.hdb
 ./gromos53a6_lipid.ff/aminoacids.n.tdb
 ./gromos53a6_lipid.ff/aminoacids.c.tdb
shouldn't I?

Finally, I've heard that there are already pre-build force fields for the
membrane smulation. E.g  I've heard that there is some modified CHARMM ff
wich gave good results in simulation. Do you know something about this?


Thank you for your help,

James
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[gmx-users] some questions about calculation of dipole ACF

2011-10-18 Thread RuiTing Zhang
I have been performing MD simulation on electrolyte solution recently. And I 
want to calculate the dipoles between cation-anion pairs. But I have no clue 
how to achieve this by gromacs. I also want to know the algorithm for command 
g_dipole about how to cheat a system with both molecules and ions separately. 
Your advisements will be quite helpful
Thank you very much!~






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Re: [gmx-users] High temperature Simulation

2011-10-18 Thread Kavyashree M
Hello,

Thank you. I got the point but I have a doubt,
equilibrate under NPT until the pressure and
temperature are stable, then switch to NVT to
eliminate the boiling issue, how exactly it will
eliminate the boiling issue if we dont use higher
pressure while equlibrating? (as you said that
it is difficult to simulate at high pressure due to
stability reasons.)

Thank you
With Regards
Kavya
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[gmx-users] dihedral restraint violation output

2011-10-18 Thread Markus Weingarth
Dear Gromacs users,I would like to ask how I could vizualise the violations of the dihedral restraints in detail, i.e., a list of all violations.As far as I know, there is nothing like g_disre for dihedrals, or ?Kind regardsMarkusSMS schreiben mit WEB.DE FreeMail - einfach, schnell undkostenguenstig. Jetzt gleich testen! http://f.web.de/?mc=021192

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Re: [gmx-users] Interaction energy

2011-10-18 Thread Justin A. Lemkul



Steven Neumann wrote:



On Mon, Oct 17, 2011 at 6:02 PM, Justin A. Lemkul jalem...@vt.edu 
mailto:jalem...@vt.edu wrote:




Steven Neumann wrote:

Dear Gmx Users,
 I would like to calculate the interaction energy (LJ and
electrostatic) between each residue and my ligands (10 ligands
in the system). I would like to see what is the contribution of
electrostatic and vdW interactions between ligand and each of my
residue. I thought to use g_energy and specify each of my
residues in index files but it is not possible. Will you suggest
how to do this?
 



For such information, you have to specify these groups as energygrps
in the .mdp file.  You can rerun the trajectory using mdrun -rerun
and a new .tpr file specifying these groups, but depending on the
output frequency, the result may not be as accurate as you'd like.

-Justin

 
Thank you Justin. Now I have two groups sepcified in my mdp file:
 
energygrps = Protein LIG


How can I specify each residue of my protein separately and each ligand? 
In my md.gro file I have residues:


91GLY 92TYR . 161LIG 162LIG...

 
Will it be correct like this
 
energygrps = 91GLY 92 TYR ... 161LIG 162LIG...
 


No.  The names must correspond to valid groups in an index file.


If yes, will this simulation take longer? Thank you


Perhaps, but certainly your energy file will be considerably larger.

-Justin

 
Steven


 

 



--


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


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Re: [gmx-users] Simulation of membrane protein

2011-10-18 Thread Justin A. Lemkul



James Starlight wrote:

Dear Justin,

Indeed I didnt take into account square degree so all values presented 
in the tutorial exactly true so this was exactly my mistake. :(


After some iterations I've obtained value for S per lipid beetween 
0.65-0.71 A^2.  This is the example of the system wich I've obtained 
after solvation and futher minimization. 
http://www.sendspace.com/file/h6urhq  It looks good. :)  By the way I'd 
like to know about correct value for the S per protein ? Where I can 
obtain such information for my protein ? ( e.g for big proteins such 
receptors and channels )




Such information depends on whether there is experimental evidence for the 
protein you're looking for.


The error with GenBox was due to the big vdv R for the carbons. It's 
intresting that I couldnt increase this value mush as 1.2. But my 
finally system didnt consist of some water within the membrane so I 
supose that it's good.


Now my system on the stage of the equilibtation so I have not any 
questions yet but I only wounder to know about teqnique of the force 
fied preparation for the membrane protein simulation.


In this work I've done this step in accordance with the tutorial. On the 
last stage I've copied  gromos53a6_lipid.ff directory in $GMXLIB so now 
I can use it in pdb2gmx for instance. 
But when I've tried to make gro and top files for my  lipid.pdb via 
pdb2gmx I've obtained errors that Residue 'DPP' not found in residue 
topology database so I think that in addition to the operations wich 
I've already done I should also make some changes in the

/gromos53a6_lipid.ff/aminoacids.hdb
 ./gromos53a6_lipid.ff/aminoacids.n.tdb
 ./gromos53a6_lipid.ff/aminoacids.c.tdb
shouldn't I?



pdb2gmx is not suited for building topologies of multi-molecule, heterogeneous 
systems like solvated membranes.  You may be able to get a topology, but it will 
be a redundant mess.  Follow the protocol in the tutorial; it avoids these 
issues in the most streamlined way possible.  If you need a topology of a new 
lipid, create an .rtp entry (if one does not exist already) and run pdb2gmx on a 
single lipid molecule.  You can then #include the new .itp file in your system 
topology.


Finally, I've heard that there are already pre-build force fields for 
the membrane smulation. E.g  I've heard that there is some modified 
CHARMM ff wich gave good results in simulation. Do you know something 
about this?




Various CHARMM parameter sets exist.  CHARMM27 is built into the Gromacs 4.5.x 
series, and CHARMM36 is available from the User Contributions section of the 
website.


-Justin



Thank you for your help,

James



--


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


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Re: [gmx-users] High temperature Simulation

2011-10-18 Thread Justin A. Lemkul



Kavyashree M wrote:

Hello,

Thank you. I got the point but I have a doubt,
equilibrate under NPT until the pressure and
temperature are stable, then switch to NVT to
eliminate the boiling issue, how exactly it will
eliminate the boiling issue if we dont use higher
pressure while equlibrating? (as you said that
it is difficult to simulate at high pressure due to
stability reasons.)



You should equilibrate under whatever the necessary conditions are, be it high 
pressure or not.  Once the desired parameters have been achieved, then switch to 
NVT.  Since the box is invariant in NVT, you don't have to worry about anything 
expanding.


Please continue to search in the literature for finer methodology points.  I'm 
certain these issues have been addressed in greater detail elsewhere.


-Justin

--


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


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Re: [gmx-users] Interaction energy

2011-10-18 Thread Steven Neumann
On Tue, Oct 18, 2011 at 11:41 AM, Justin A. Lemkul jalem...@vt.edu wrote:



 Steven Neumann wrote:



 On Mon, Oct 17, 2011 at 6:02 PM, Justin A. Lemkul jalem...@vt.edumailto:
 jalem...@vt.edu wrote:



Steven Neumann wrote:

Dear Gmx Users,
 I would like to calculate the interaction energy (LJ and
electrostatic) between each residue and my ligands (10 ligands
in the system). I would like to see what is the contribution of
electrostatic and vdW interactions between ligand and each of my
residue. I thought to use g_energy and specify each of my
residues in index files but it is not possible. Will you suggest
how to do this?


For such information, you have to specify these groups as energygrps
in the .mdp file.  You can rerun the trajectory using mdrun -rerun
and a new .tpr file specifying these groups, but depending on the
output frequency, the result may not be as accurate as you'd like.

-Justin

  Thank you Justin. Now I have two groups sepcified in my mdp file:
  energygrps = Protein LIG

 How can I specify each residue of my protein separately and each ligand?
 In my md.gro file I have residues:

91GLY 92TYR . 161LIG 162LIG...

  Will it be correct like this
  energygrps = 91GLY 92 TYR ... 161LIG 162LIG...



 No.  The names must correspond to valid groups in an index file.


So do you mean that that I should add my index file with


grompp -f md.mdp -c npt.gro -n *index.ndx* -t npt.cpt -p topol.top -o md.tpr



with specified groups in md.mdp file like they are specified in index file?
:) Then just to



mdrun -rerun -deffnm md2



Please, let me know whether I am correct or not.



Steven


 If yes, will this simulation take longer? Thank you


 Perhaps, but certainly your energy file will be considerably larger.

 -Justin

  Steven





 --
 ==**==

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

 ==**==
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Re: [gmx-users] High temperature Simulation

2011-10-18 Thread Kavyashree M
Ok Thanks.

On Tue, Oct 18, 2011 at 4:41 PM, Justin A. Lemkul jalem...@vt.edu wrote:



 Kavyashree M wrote:

 Hello,

 Thank you. I got the point but I have a doubt,
 equilibrate under NPT until the pressure and
 temperature are stable, then switch to NVT to
 eliminate the boiling issue, how exactly it will
 eliminate the boiling issue if we dont use higher
 pressure while equlibrating? (as you said that
 it is difficult to simulate at high pressure due to
 stability reasons.)


 You should equilibrate under whatever the necessary conditions are, be it
 high pressure or not.  Once the desired parameters have been achieved, then
 switch to NVT.  Since the box is invariant in NVT, you don't have to worry
 about anything expanding.

 Please continue to search in the literature for finer methodology points.
  I'm certain these issues have been addressed in greater detail elsewhere.

 -Justin


 --
 ==**==

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

 ==**==
 --
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 http://lists.gromacs.org/**mailman/listinfo/gmx-usershttp://lists.gromacs.org/mailman/listinfo/gmx-users
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 Support/Mailing_Lists/Searchhttp://www.gromacs.org/Support/Mailing_Lists/Searchbefore
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Re: [gmx-users] Interaction energy

2011-10-18 Thread Justin A. Lemkul



Steven Neumann wrote:



On Tue, Oct 18, 2011 at 11:41 AM, Justin A. Lemkul jalem...@vt.edu 
mailto:jalem...@vt.edu wrote:




Steven Neumann wrote:



On Mon, Oct 17, 2011 at 6:02 PM, Justin A. Lemkul
jalem...@vt.edu mailto:jalem...@vt.edu
mailto:jalem...@vt.edu mailto:jalem...@vt.edu wrote:



   Steven Neumann wrote:

   Dear Gmx Users,
I would like to calculate the interaction energy (LJ and
   electrostatic) between each residue and my ligands (10
ligands
   in the system). I would like to see what is the
contribution of
   electrostatic and vdW interactions between ligand and
each of my
   residue. I thought to use g_energy and specify each of my
   residues in index files but it is not possible. Will you
suggest
   how to do this?
   


   For such information, you have to specify these groups as
energygrps
   in the .mdp file.  You can rerun the trajectory using mdrun
-rerun
   and a new .tpr file specifying these groups, but depending on the
   output frequency, the result may not be as accurate as you'd
like.

   -Justin

 Thank you Justin. Now I have two groups sepcified in my mdp file:
 energygrps = Protein LIG

How can I specify each residue of my protein separately and each
ligand? In my md.gro file I have residues:

   91GLY 92TYR . 161LIG 162LIG...

 Will it be correct like this
 energygrps = 91GLY 92 TYR ... 161LIG 162LIG...
 



No.  The names must correspond to valid groups in an index file.

 
So do you mean that that I should add my index file with
 


grompp -f md.mdp -c npt.gro -n *index.ndx* -t npt.cpt -p topol.top -o md.tpr

 

with specified groups in md.mdp file like they are specified in index 
file? :) Then just to


 


mdrun -rerun -deffnm md2

 


Please, let me know whether I am correct or not.



Yes.

-Justin

 


Steven


If yes, will this simulation take longer? Thank you


Perhaps, but certainly your energy file will be considerably larger.

-Justin

 Steven

 
 



-- 
==__==


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu http://vt.edu/ | (540) 231-9080
tel:%28540%29%20231-9080
http://www.bevanlab.biochem.__vt.edu/Pages/Personal/justin
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin

==__==
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--


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


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[gmx-users] RE:Interaction Energy

2011-10-18 Thread lloyd riggs
Message: 1
Date: Tue, 18 Oct 2011 06:41:55 -0400
From: Justin A. Lemkul jalem...@vt.edu
Subject: Re: [gmx-users] Interaction energy
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4e9d57f3.10...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



Steven Neumann wrote:
 
 
 On Mon, Oct 17, 2011 at 6:02 PM, Justin A. Lemkul jalem...@vt.edu 
 mailto:jalem...@vt.edu wrote:
 
 
 
 Steven Neumann wrote:
 
 Dear Gmx Users,
  I would like to calculate the interaction energy (LJ and
 electrostatic) between each residue and my ligands (10 ligands
 in the system). I would like to see what is the contribution of
 electrostatic and vdW interactions between ligand and each of my
 residue. I thought to use g_energy and specify each of my
 residues in index files but it is not possible. Will you suggest
 how to do this?
  
 
 
 For such information, you have to specify these groups as energygrps
 in the .mdp file.  You can rerun the trajectory using mdrun -rerun
 and a new .tpr file specifying these groups, but depending on the
 output frequency, the result may not be as accurate as you'd like.
 
 -Justin
 
  
 Thank you Justin. Now I have two groups sepcified in my mdp file:
  
 energygrps = Protein LIG
 
 How can I specify each residue of my protein separately and each ligand? 
 In my md.gro file I have residues:
 
 91GLY 92TYR . 161LIG 162LIG...
 
  
 Will it be correct like this
  
 energygrps = 91GLY 92 TYR ... 161LIG 162LIG...
  

No.  The names must correspond to valid groups in an index file.

 If yes, will this simulation take longer? Thank you

Perhaps, but certainly your energy file will be considerably larger.

-Justin

  
 Steven
 
  
 
  
 

-- 


Dear Steven,

I did the following, but like Justin mentioned the files get large.  Basically, 
I made a very complex ndx file from the beggining.  I have the whole proteins 
and peptides involved, then a series of loops, and protein minus loop, and then 
individual amino acids and protein minus the amino acids.  Basically every time 
you make the ndx for a particular amino acid/chain/loop you also have to 
generate the ndx for the rest of your protein minus what you were looking at.  
Otherwise you run out of groups to assign, and will start getting residue or 
atom in multiple groups when it is referenced more than one time.

This might not be necessary in your case, but lets you divie up energy 
contributions easier, although multiple re-runs using varied indexes might be 
necessary, ie for the sum total, then varied parts, etc...

At least that is a suggestion from my experience..

Freundlichen Grüsse

Stephan Watkins
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Re: [gmx-users] RE:Interaction Energy

2011-10-18 Thread Steven Neumann
On Tue, Oct 18, 2011 at 1:36 PM, lloyd riggs lloyd.ri...@gmx.ch wrote:

 Message: 1
 Date: Tue, 18 Oct 2011 06:41:55 -0400
 From: Justin A. Lemkul jalem...@vt.edu
 Subject: Re: [gmx-users] Interaction energy
 To: Discussion list for GROMACS users gmx-users@gromacs.org
 Message-ID: 4e9d57f3.10...@vt.edu
 Content-Type: text/plain; charset=ISO-8859-1; format=flowed



 Steven Neumann wrote:
 
 
  On Mon, Oct 17, 2011 at 6:02 PM, Justin A. Lemkul jalem...@vt.edu
  mailto:jalem...@vt.edu wrote:
 
 
 
  Steven Neumann wrote:
 
  Dear Gmx Users,
   I would like to calculate the interaction energy (LJ and
  electrostatic) between each residue and my ligands (10 ligands
  in the system). I would like to see what is the contribution of
  electrostatic and vdW interactions between ligand and each of my
  residue. I thought to use g_energy and specify each of my
  residues in index files but it is not possible. Will you suggest
  how to do this?
 
 
 
  For such information, you have to specify these groups as energygrps
  in the .mdp file.  You can rerun the trajectory using mdrun -rerun
  and a new .tpr file specifying these groups, but depending on the
  output frequency, the result may not be as accurate as you'd like.
 
  -Justin
 
 
  Thank you Justin. Now I have two groups sepcified in my mdp file:
 
  energygrps = Protein LIG
 
  How can I specify each residue of my protein separately and each ligand?
  In my md.gro file I have residues:
 
  91GLY 92TYR . 161LIG 162LIG...
 
 
  Will it be correct like this
 
  energygrps = 91GLY 92 TYR ... 161LIG 162LIG...
 

 No.  The names must correspond to valid groups in an index file.

  If yes, will this simulation take longer? Thank you

 Perhaps, but certainly your energy file will be considerably larger.

 -Justin

 
  Steven
 
 
 
 
 

 --
 

 Dear Steven,

 I did the following, but like Justin mentioned the files get large.
  Basically, I made a very complex ndx file from the beggining.  I have the
 whole proteins and peptides involved, then a series of loops, and protein
 minus loop, and then individual amino acids and protein minus the amino
 acids.  Basically every time you make the ndx for a particular amino
 acid/chain/loop you also have to generate the ndx for the rest of your
 protein minus what you were looking at.  Otherwise you run out of groups to
 assign, and will start getting residue or atom in multiple groups when it
 is referenced more than one time.

 This might not be necessary in your case, but lets you divie up energy
 contributions easier, although multiple re-runs using varied indexes might
 be necessary, ie for the sum total, then varied parts, etc...

 At least that is a suggestion from my experience..

 Freundlichen Grüsse

 Stephan Watkins
 --
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Thank you Stephan! I have faced the problem you mentioned:

Fatal error: Atom 1 in multiple Energy Mon. groups (1 and 3)

So as I understood what you have written I should specify in my INDEX.ndx:

[r_91] - residue 91
1 2 3 7
[Protein-r91]  - Protein without residue 91
8 9 10 11... 382
[r_92] - resideu 92
8 9 10 11...17
[Protein-r92] - Protein without residue 92
1 2..7 18 19 20...38

etc. etc.

And the same with ligands but substracting from my [System] group?

Then
[Ligand] - all Ligands atoms
[Protein] - all Protein atoms
[Water] - all Water atoms.

Please let me whether I am correct. Did such simulation take much longer? I
run 100ns simulations for 2 days on the cluster with specified energy groups
for Protein and Ligand only. My system consists of app. 4000 atoms only
(water+protein+ligands).
Thank you,

Steven
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Re: [gmx-users] RE:Interaction Energy

2011-10-18 Thread Justin A. Lemkul



Steven Neumann wrote:



On Tue, Oct 18, 2011 at 1:36 PM, lloyd riggs lloyd.ri...@gmx.ch 
mailto:lloyd.ri...@gmx.ch wrote:


Message: 1
Date: Tue, 18 Oct 2011 06:41:55 -0400
From: Justin A. Lemkul jalem...@vt.edu mailto:jalem...@vt.edu
Subject: Re: [gmx-users] Interaction energy
To: Discussion list for GROMACS users gmx-users@gromacs.org
mailto:gmx-users@gromacs.org
Message-ID: 4e9d57f3.10...@vt.edu mailto:4e9d57f3.10...@vt.edu
Content-Type: text/plain; charset=ISO-8859-1; format=flowed



Steven Neumann wrote:
 
 
  On Mon, Oct 17, 2011 at 6:02 PM, Justin A. Lemkul
jalem...@vt.edu mailto:jalem...@vt.edu
  mailto:jalem...@vt.edu mailto:jalem...@vt.edu wrote:
 
 
 
  Steven Neumann wrote:
 
  Dear Gmx Users,
   I would like to calculate the interaction energy (LJ and
  electrostatic) between each residue and my ligands (10
ligands
  in the system). I would like to see what is the
contribution of
  electrostatic and vdW interactions between ligand and
each of my
  residue. I thought to use g_energy and specify each of my
  residues in index files but it is not possible. Will you
suggest
  how to do this?
 
 
 
  For such information, you have to specify these groups as
energygrps
  in the .mdp file.  You can rerun the trajectory using mdrun
-rerun
  and a new .tpr file specifying these groups, but depending on the
  output frequency, the result may not be as accurate as you'd
like.
 
  -Justin
 
 
  Thank you Justin. Now I have two groups sepcified in my mdp file:
 
  energygrps = Protein LIG
 
  How can I specify each residue of my protein separately and each
ligand?
  In my md.gro file I have residues:
 
  91GLY 92TYR . 161LIG 162LIG...
 
 
  Will it be correct like this
 
  energygrps = 91GLY 92 TYR ... 161LIG 162LIG...
 

No.  The names must correspond to valid groups in an index file.

  If yes, will this simulation take longer? Thank you

Perhaps, but certainly your energy file will be considerably larger.

-Justin

 
  Steven
 
 
 
 
 

 --
 

Dear Steven,

I did the following, but like Justin mentioned the files get large.
 Basically, I made a very complex ndx file from the beggining.  I
have the whole proteins and peptides involved, then a series of
loops, and protein minus loop, and then individual amino acids and
protein minus the amino acids.  Basically every time you make the
ndx for a particular amino acid/chain/loop you also have to generate
the ndx for the rest of your protein minus what you were looking at.
 Otherwise you run out of groups to assign, and will start getting
residue or atom in multiple groups when it is referenced more than
one time.

This might not be necessary in your case, but lets you divie up
energy contributions easier, although multiple re-runs using varied
indexes might be necessary, ie for the sum total, then varied parts,
etc...

At least that is a suggestion from my experience..

Freundlichen Grüsse

Stephan Watkins
--
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Thank you Stephan! I have faced the problem you mentioned:
 
Fatal error: Atom 1 in multiple Energy Mon. groups (1 and 3)
 
So as I understood what you have written I should specify in my INDEX.ndx:
 
[r_91] - residue 91

1 2 3 7
[Protein-r91]  - Protein without residue 91
8 9 10 11... 382
[r_92] - resideu 92
8 9 10 11...17
[Protein-r92] - Protein without residue 92
1 2..7 18 19 20...38
 
etc. etc.
 
And the same with ligands but substracting from my [System] group?
 


This is not a correct approach, per the fatal error.  If you want to monitor 
energies involving different residues, the only requirement is that those 
residues be in their own distinct groups, i.e.:


energygrps = r_91 r_92 r_93 ... Ligand

The energy groups cannot be redundant.  What Stephan was suggesting is that you 
cannot, for instance, specify:


energygrps = Protein r_91 r_92 ...

because Protein encompasses residues 91, 92, etc.  You can, however, specify 

[gmx-users] potential energy of one molecule using GAFF: confused regarding Ryckaert-Bellemans and 1-4 potentials

2011-10-18 Thread Vedat Durmaz

hey guys,

i'm a really confused at the moment. reading the gromacs manual 4.5.4 
(GM) and the paper introducing GAFF did not provide insight into this 
issue which drives me crazy! maybe some advanced gromacs user can do so.


up to now, i have simulated very few different systems using amber force 
fields and gromacs (4.0.7). assume you have simulated the global minimum 
conformation of some handsome molecule mol mainly consisting of a 
simple cyclic aliphatic structure (about 13 atoms long) containing a 
double bond resulting in an E-mol and Z-mol isomer.


i know from radicalic interconversion experiments, that Z-mol is about 
100.000 times likelier than E-mol (due to the cyclic structure).


from the simulation, which i've performed in water as well as in vacuum, 
i find that my intramolecular LJ14 and Coul14 energies indeed reflect 
the experimental steady state distribution. LJ-SR and Coul-SR just show 
slight differences only for the isomers. now, in order to see, whether 
the high 14-difference is caused by solvent effects or not, i extracted 
several energies from the vacuum simulation (E-mol left and Z-mol right) 
allowing me additionally to extract the potential energy (as well as 
bonded terms) of the molecule under consideration only:


1  Bond  69.267.3

2  Angle 96.1104.9

3  Proper Dih.3.14.6

4  Ryckaert-Bell.63.9106.3

5  LJ-14 48.446.1

6  Coulomb-14 -1036.6-1065.3

7  LJ (SR)   20.619.1

8  Coulomb (SR) 555.9556.5

9  Potential   -179.4-160.5


the potential energy (line 9) obviously equals the sum of all other 
terms (line 1-8) and reveals, in contrast to the Coulomb-14 (C14) term, 
a completely different steady state distribution of cis- and trans-mol. 
this is mainly due to the Ryckaert-Bellemans (RB) term.


however, as i've understood from the GM, the RB potential for dihedrals 
is not incorporated by every force field because often, the periodic 
type is used instead. and indeed, when comparing the equations from the 
gromacs manual with the Wang-paper in jCompChem-2004 concerning GAFF, it 
seems neither GAFF uses RB.



and here are my lovely questions:

Q1 am i right with my assumption whether GAFF uses RB or not? if not, 
will someone please explain it to me in a few words?


Q2 why does the md.edr file provide two different terms concerning the 
same thing (proper dihedrals): proper dihedrals and RB how can i 
interpret these values?



GM says: With the periodic GROMOS potential a special 1-4 LJ-interaction
must be included; with the Ryckaert-Bellemans potential for alkanes the 
1-4 interactions must be
excluded from the non-bonded list. Note: Ryckaert-Bellemans potentials 
are also used in e.g. the

OPLS force field in combination with 1-4 interactions

Q3 does anyone know, how this is handled in GAFF?

Q4 does this mean i have to exclude 1-4 manually, after having 
parameterized my molecules using acpype (antechamber)?



GM says: For alkanes, the following proper dihedral potential [RB] is 
often used


Q5 what does it depend on, whether RB is used for alkanes or not?


GM says: For third neighbors, the normal Lennard-Jones repulsion is 
sometimes still too strong, ... especially the case for carbon-carbon 
interactions in a cis-conformation ... for some of these interactions, 
the Lennard-Jones repulsion has been reduced in the GROMOS force field, 
which is implemented by keeping a separate list of 1-4 and normal 
Lennard-Jones parameters. In other force fields, such as OPLS [88], the 
standard Lennard-Jones parameters are reduced by a factor of two, ...


Q6 how this is handled with GAFF in gromacs?

Q7 in general, can i still trust the given energies as listed above 
and compare them quantitatively? the simulation should actually result 
in a favorable Z-mol (due to strain) and less favorable E-mol. are the 
force fields and simulation software able to capture these kind of 
differences concerning the steady-state distribution of cis/trans, when 
the respective potentials are modified in such various ways among the 
force fields?


Q8 does anyone have an idea, how to perform the simulation and on which 
energy terms to concentrate in order to get reliable results?


thanks in advance and sorry for the long text ... as i've already told 
you, i'm really confused.


kind regards

vedat durmaz



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[gmx-users] N-terminal PGLU and C-term amidation

2011-10-18 Thread Henry Hocking

Hello,

I am new to gromacs. I am applying the pdb2gmx tool to a peptide that  
has an N-term pyroglutamate and a C-term amidation. The OPLS  
forcefield has an entry for PGLU.


I used the -ter flag of pdb2gmx to define protonation states of the  
termini. While this works fine for the C-term (choosing 3:None) I run  
into trouble with the PGLU at the N-term.


In my input pdb the nitrogen of PGLU is attached to CA, CD and one  
proton.


However when prompted 'Select start terminus type for PGLU-1' there is  
no NH option. If I select 'None' I get Fatal error: There is a  
dangling bond at at least one of the terminal ends. If I chose NH2 I  
end up with too many protons at my N-terminus.


If I leave out the -ter flag altogether I get problems with my C- 
terminus: Fatal error: atom C not found in building block 23NH2 while  
combining tdb and rtp.


How would I solve this?

Regards,

Henry




Henry Hocking, PhD

Utrecht University
Bijvoet Center for Biomolecular Research
Padualaan 8
3584 CH Utrecht, The Netherlands

Phone: +31-30-2532875
Fax: +31-30-253 7623
E-mail: h.g.hock...@uu.nl





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Re: [gmx-users] potential energy of one molecule using GAFF: confused regarding Ryckaert-Bellemans and 1-4 potentials

2011-10-18 Thread Mark Abraham

On 19/10/2011 12:34 AM, Vedat Durmaz wrote:

hey guys,

i'm a really confused at the moment. reading the gromacs manual 4.5.4 
(GM) and the paper introducing GAFF did not provide insight into this 
issue which drives me crazy! maybe some advanced gromacs user can do so.


up to now, i have simulated very few different systems using amber 
force fields and gromacs (4.0.7).


Don't exclusively read documentation that doesn't match the version of 
the software. Things change.


assume you have simulated the global minimum conformation of some 
handsome molecule mol mainly consisting of a simple cyclic aliphatic 
structure (about 13 atoms long) containing a double bond resulting in 
an E-mol and Z-mol isomer.


i know from radicalic interconversion experiments, that Z-mol is about 
100.000 times likelier than E-mol (due to the cyclic structure).


Part of that will be energy-based (E-mol has higher intra-atomic 
repulsion), and part will be entropy-based (Z-mol has fewer available 
configurations), but apparently a 13-atom ring is large enough that we 
should see the former dominate.




from the simulation, which i've performed in water as well as in 
vacuum, i find that my intramolecular LJ14 and Coul14 energies indeed 
reflect the experimental steady state distribution.


Maybe that is just fortuitous. Force fields are not parameterized to 
necessarily be able to be decomposed in ways that correlate numbers with 
chemical intuition. In particular, there is a balance between 1-4 
charge-charge interaction and 1-4 dihedral interaction which depends on 
how everything else is parameterized.


LJ-SR and Coul-SR just show slight differences only for the isomers. 
now, in order to see, whether the high 14-difference is caused by 
solvent effects or not,


Note that you can construct subsets from your water .tpr and .trr with 
tpbconv and trjconv, and then use mdrun -rerun on these existing 
configuration, rather than run a vacuum simulation that samples 
different space.


i extracted several energies from the vacuum simulation (E-mol left 
and Z-mol right) allowing me additionally to extract the potential 
energy (as well as bonded terms) of the molecule under consideration 
only:


I'm assuming these are post-equilibration average values over at least 
several nanoseconds. Otherwise they don't mean anything at all.




1  Bond  69.267.3

2  Angle 96.1104.9

3  Proper Dih.3.14.6

4  Ryckaert-Bell.63.9106.3

5  LJ-14 48.446.1

6  Coulomb-14 -1036.6-1065.3

7  LJ (SR)   20.619.1

8  Coulomb (SR) 555.9556.5

9  Potential   -179.4-160.5


the potential energy (line 9) obviously equals the sum of all other 
terms (line 1-8) and reveals, in contrast to the Coulomb-14 (C14) 
term, a completely different steady state distribution of cis- and 
trans-mol. this is mainly due to the Ryckaert-Bellemans (RB) term.


One could equally observe that the contribution to the wrong relative 
energy is about half due to the angle term and about half due to the sum 
of dihedral and 1-4 terms.


Apparently your experimental results suggest the same relative stability 
trend should be seen with the vacuum and condensed-phase systems, 
however the parameters you are using for the simulation are optimized 
for the condensed phase, so it is far from clear that they will produce 
the correct ensemble.


If you'd done the mdrun -rerun I suggested and produced numbers like the 
above, you'd have the problem that you'd have assumed that the solvent 
potential energy is identical in each case.




however, as i've understood from the GM, the RB potential for 
dihedrals is not incorporated by every force field because often, the 
periodic type is used instead. and indeed, when comparing the 
equations from the gromacs manual with the Wang-paper in 
jCompChem-2004 concerning GAFF, it seems neither GAFF uses RB.



and here are my lovely questions:

Q1 am i right with my assumption whether GAFF uses RB or not? if not, 
will someone please explain it to me in a few words?


Read the GAFF paper for what mathematical function should be used. 
GROMACS would then have the job of implementing that function, but it 
need not do so with one that is named the same way. In particular, 
before GROMACS 4.5, there was no way of implementing multiple periodic 
dihedral types on the same four atoms (as used by CHARMM and AMBER force 
fields), so these had to be combined into one equivalent RB form.




Q2 why does the md.edr file provide two different terms concerning the 
same thing (proper dihedrals): proper dihedrals and RB how can i 
interpret these values?


Your .top file has both types, and it seems the latter result from the 
above-mentioned combining.





GM says: With the periodic GROMOS potential a special 1-4 LJ-interaction
must be included; with the Ryckaert-Bellemans potential for alkanes 
the 1-4 interactions must be
excluded from the 

Re: [gmx-users] RE:Interaction Energy

2011-10-18 Thread Steven Neumann
On Tue, Oct 18, 2011 at 2:50 PM, Justin A. Lemkul jalem...@vt.edu wrote:



 Steven Neumann wrote:



 On Tue, Oct 18, 2011 at 1:36 PM, lloyd riggs lloyd.ri...@gmx.ch mailto:
 lloyd.ri...@gmx.ch wrote:

Message: 1
Date: Tue, 18 Oct 2011 06:41:55 -0400
From: Justin A. Lemkul jalem...@vt.edu mailto:jalem...@vt.edu

Subject: Re: [gmx-users] Interaction energy
To: Discussion list for GROMACS users gmx-users@gromacs.org
mailto:gmx-users@gromacs.org**
Message-ID: 4e9d57f3.10...@vt.edu mailto:4e9d57f3.10...@vt.edu**

Content-Type: text/plain; charset=ISO-8859-1; format=flowed



Steven Neumann wrote:
 
 
  On Mon, Oct 17, 2011 at 6:02 PM, Justin A. Lemkul
jalem...@vt.edu mailto:jalem...@vt.edu
   mailto:jalem...@vt.edu mailto:jalem...@vt.edu wrote:
 
 
 
  Steven Neumann wrote:
 
  Dear Gmx Users,
   I would like to calculate the interaction energy (LJ and
  electrostatic) between each residue and my ligands (10
ligands
  in the system). I would like to see what is the
contribution of
  electrostatic and vdW interactions between ligand and
each of my
  residue. I thought to use g_energy and specify each of my
  residues in index files but it is not possible. Will you
suggest
  how to do this?
 
 
 
  For such information, you have to specify these groups as
energygrps
  in the .mdp file.  You can rerun the trajectory using mdrun
-rerun
  and a new .tpr file specifying these groups, but depending on
 the
  output frequency, the result may not be as accurate as you'd
like.
 
  -Justin
 
 
  Thank you Justin. Now I have two groups sepcified in my mdp file:
 
  energygrps = Protein LIG
 
  How can I specify each residue of my protein separately and each
ligand?
  In my md.gro file I have residues:
 
  91GLY 92TYR . 161LIG 162LIG...
 
 
  Will it be correct like this
 
  energygrps = 91GLY 92 TYR ... 161LIG 162LIG...
 

No.  The names must correspond to valid groups in an index file.

  If yes, will this simulation take longer? Thank you

Perhaps, but certainly your energy file will be considerably larger.

-Justin

 
  Steven
 
 
 
 
 

 --
 =**===

Dear Steven,

I did the following, but like Justin mentioned the files get large.
 Basically, I made a very complex ndx file from the beggining.  I
have the whole proteins and peptides involved, then a series of
loops, and protein minus loop, and then individual amino acids and
protein minus the amino acids.  Basically every time you make the
ndx for a particular amino acid/chain/loop you also have to generate
the ndx for the rest of your protein minus what you were looking at.
 Otherwise you run out of groups to assign, and will start getting
residue or atom in multiple groups when it is referenced more than
one time.

This might not be necessary in your case, but lets you divie up
energy contributions easier, although multiple re-runs using varied
indexes might be necessary, ie for the sum total, then varied parts,
etc...

At least that is a suggestion from my experience..

Freundlichen Grüsse

Stephan Watkins
--
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Jetzt informieren: 
 http://www.gmx.net/de/go/**freephonehttp://www.gmx.net/de/go/freephone
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  posting!
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 http://www.gromacs.org/**Support/Mailing_Listshttp://www.gromacs.org/Support/Mailing_Lists


  Thank you Stephan! I have faced the problem you mentioned:
  Fatal error: Atom 1 in multiple Energy Mon. groups (1 and 3)
  So as I understood what you have written I should specify in my
 INDEX.ndx:
  [r_91] - residue 91
 1 2 3 7
 [Protein-r91]  - Protein without residue 91
 8 9 10 11... 382
 [r_92] - resideu 92
 8 9 10 11...17
 [Protein-r92] - Protein without residue 92
 1 2..7 18 19 20...38
  etc. etc.
  And the same with ligands but substracting from my [System] group?



 This is not a correct approach, per the fatal error.  If you want to
 monitor energies involving different residues, the only requirement is that
 those 

[gmx-users] About pair distribution function

2011-10-18 Thread vidhya sankar
Dear Gromacs user .  Thanks for your previous eply

   I am using plumed gromacs . i would like to 
find out Hydrophobic interaction free energies . As  stated in manual.i used 
COORD keyword which is based on the Switching function . But When i  use the 
COORD option  i need to properly Guess the  Term MM,NN, R_0 D_0 . For that i 
had been advised to look at the pair distribution function of the two groups  
(among Which i want to calculate Hydrophobic energies, plumed 1-2-2 manual)  Is 
ther is any way to calculate pair  Distribution function through gromacs.  
.between two set of groups  .

 Thanks in Advance-- 
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Re: [gmx-users] Link to Intel MKL (fftw) via cmake options

2011-10-18 Thread Mirco Wahab

On 17.10.2011 05:18, Mark Abraham wrote:

On 17/10/2011 7:04 AM, Mirco Wahab wrote:

On 10/16/2011 2:25 PM, Mark Abraham wrote:

On 15/10/2011 9:02 PM, Mirco Wahab wrote:

On 10/15/2011 1:15 AM, Mark Abraham wrote:

I use
...

...

...

OK, I can understand that. But if the options (-mtune ***, -msse2)
are not longer available with the actual free Intel Compiler suites,
shouldn't the cmake definitions be adapted to this fact in order
to avoid loads of compiler warnings?


If someone can identify a way to detect old and new, free and non-free compiler 
suites then we might consider it. Reality is that GROMACS spends a heavy 
majority of its time in loops written mostly in assembly code (using SSE or 
SSE2 if applicable), or in
the FFT library. Compiler performance makes a negligible contribution to 
performance of the rest, so it is really not worth while maintaining complex 
compiler tweaks.


OK,


I'll attach the error messages err.msg, 5.9 KB).
- cmake version 2.8.3
- gcc 4.5.1 x64 (Linux) (20101208)


With cmake 2.8.2 and icc 12.1.0 20110811 using the aforementioned flags, I get 
smooth installation of the git version of 4.5.5. Moreover, I don't even get
.../build/src/gmxlib/CMakeFiles/CMakeRelink.dir
being created. So I think there is something idiosyncratic about your tool 
chain that is at the root of this.


I replicated the error on another machine and already answered this
as a response to Szilárd. I really don't know what the reason is, maybe
I'm doing something really wrong. The only ray of hope: w/autoconf,
everything works fine, even giving one the subjective impression of
'closely controlling' the build process ;-)

Thanks  regards

M.
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[gmx-users] calculation time

2011-10-18 Thread ahmet yıldırım
Dear users,

Sometimes, in the end ( in production simulation), Gromacs doesn't show
calculation/finish time on screen, why? How can we show it?

Thanks in advance

-- 
Ahmet YILDIRIM
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[gmx-users] Charmm27 ff for membrane protein simulation

2011-10-18 Thread James Starlight
Greetings!


Recently I've found that Charmm27 ff is widely used for the simulation of
the membrane proteins. I've tried to work with pure DPPC bilayer in  pdb2grx
and obtain that charm27 ff included in the Gromacs is lack for the
parametries for the lipids.

Could you tell me where I could obtain those parametries ( and tutorial of
how it might be included in processing of lipids) or full functional
charmm27 ff that already has pre-built those parametries?


Thank you for help


James
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Re: [gmx-users] Charmm27 ff for membrane protein simulation

2011-10-18 Thread Justin A. Lemkul



James Starlight wrote:

Greetings!


Recently I've found that Charmm27 ff is widely used for the simulation 
of the membrane proteins. I've tried to work with pure DPPC bilayer in  
pdb2grx and obtain that charm27 ff included in the Gromacs is lack for 
the parametries for the lipids.


Could you tell me where I could obtain those parametries ( and tutorial 
of how it might be included in processing of lipids) or full functional 
charmm27 ff that already has pre-built those parametries?




Most of the common lipids are already present in lipids.rtp in charmm27.ff in 
Gromacs 4.5.x; if you are looking for lipids not present there, please be more 
specific as to what you need.


The only membrane protein tutorial to my knowledge is my own.  Dealing with 
CHARMM should be significantly easier, however, as no modification of the force 
field is necessary.  Run pdb2gmx on a single lipid molecule, convert the .top to 
.itp (see the wiki) and #include it in the .top for your protein, just like in 
my tutorial.


-Justin



Thank you for help


James



--


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


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Re: [gmx-users] Charmm27 ff for membrane protein simulation

2011-10-18 Thread Thomas Piggot
By default in the CHARMM27 force field files there is no DPPC, as this 
is made up from a combination of other entries in the rtp file (because 
this is the way it is done in the CHARMM program's files). If you wish 
to use DPPC you can construct yourself a complete DPPC rtp entry. To do 
this you it is probably easiest to duplicate the DMPC entry and add the 
corresponding atoms and bonds for two extra carbons in each tail.


Alternatively you could use the CHARMM36 force field (available to 
download from the contributions section of the website), there should 
already be an entry for DPPC.


Cheers

Tom

On 18/10/11 19:45, Justin A. Lemkul wrote:


James Starlight wrote:

Greetings!


Recently I've found that Charmm27 ff is widely used for the simulation
of the membrane proteins. I've tried to work with pure DPPC bilayer in
pdb2grx and obtain that charm27 ff included in the Gromacs is lack for
the parametries for the lipids.

Could you tell me where I could obtain those parametries ( and tutorial
of how it might be included in processing of lipids) or full functional
charmm27 ff that already has pre-built those parametries?


Most of the common lipids are already present in lipids.rtp in charmm27.ff in
Gromacs 4.5.x; if you are looking for lipids not present there, please be more
specific as to what you need.

The only membrane protein tutorial to my knowledge is my own.  Dealing with
CHARMM should be significantly easier, however, as no modification of the force
field is necessary.  Run pdb2gmx on a single lipid molecule, convert the .top to
.itp (see the wiki) and #include it in the .top for your protein, just like in
my tutorial.

-Justin


Thank you for help


James



--
Dr Thomas Piggot
University of Southampton, UK.

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[gmx-users] Energy Drift

2011-10-18 Thread Ben Reynwar
I posted to the list a few days ago with an energy drift problem.
Mark Abraham helpfully suggested using all-bonds rather than h-bonds
which solved the problem.  I'm now trying to understand quite why that
helped so much.

The simulation is a protein of about 5000 atoms using GBSA, a time
step of 2 fs, and a cut-off of 1.6 for VdW, coulomb and GB.

I've run energy drift simulations using the md integrator, with no
thermostat, and using the ld integrator with a tau_t of 100.
Simulations were run changing various parameters.  The changes were:
 - dt reduced to 1.5
 - dt reduced to 1.0
 - cutoff increased to 2.0
 - constraint changed from h-bonds to all-bonds

Plot of the energy drifts can be seen at
http://www.reynwar.net/ben/gromacs/energy_drift.png.

Noticeable features are:
 - changing the time step makes no difference (in my last post I
claimed it did, which is why you should make plots rather than
eyeballing log files).
 - increasing the cut-off helps a lot.
 - changing constraint to all-bonds make a dramatic difference
 - using ld there is a downwards drift in the energy when using
all-bonds constraint.  The temperature is roughly 300 K and the set
point is 400 K so this downwards drift seems unlikely to be due to
coupling to the langevin thermostat.

My questions are:
 - why does the all-bonds constraint help so much?
 - why doesn't moving to a smaller time step help with this?
 - what is the cause of the downwards drift when using ld with all-bonds?

Cheers,
Ben
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Re: [gmx-users] Energy Drift

2011-10-18 Thread Justin A. Lemkul



Ben Reynwar wrote:

I posted to the list a few days ago with an energy drift problem.
Mark Abraham helpfully suggested using all-bonds rather than h-bonds
which solved the problem.  I'm now trying to understand quite why that
helped so much.

The simulation is a protein of about 5000 atoms using GBSA, a time
step of 2 fs, and a cut-off of 1.6 for VdW, coulomb and GB.

I've run energy drift simulations using the md integrator, with no
thermostat, and using the ld integrator with a tau_t of 100.
Simulations were run changing various parameters.  The changes were:
 - dt reduced to 1.5
 - dt reduced to 1.0
 - cutoff increased to 2.0
 - constraint changed from h-bonds to all-bonds

Plot of the energy drifts can be seen at
http://www.reynwar.net/ben/gromacs/energy_drift.png.

Noticeable features are:
 - changing the time step makes no difference (in my last post I
claimed it did, which is why you should make plots rather than
eyeballing log files).
 - increasing the cut-off helps a lot.
 - changing constraint to all-bonds make a dramatic difference
 - using ld there is a downwards drift in the energy when using
all-bonds constraint.  The temperature is roughly 300 K and the set
point is 400 K so this downwards drift seems unlikely to be due to
coupling to the langevin thermostat.

My questions are:
 - why does the all-bonds constraint help so much?
 - why doesn't moving to a smaller time step help with this?
 - what is the cause of the downwards drift when using ld with all-bonds?



I can offer a bit of general advice here, but no specific answers.  Hopefully it 
helps.  To get at the root cause of all of this, you should be analyzing 
individual energy components, not just the total energy.  These will tell you 
which terms are systematically changing.


In my experience with GB simulations, using anything other than infinite cutoffs 
(i.e. all-vs-all kernel) has resulted in unstable simulations.  I don't mean 
that the simulations crash or anything, but the results are clearly incorrect. 
Stably folded proteins have drastically increased RMSD and lose their structure 
very easily.  The effect is independent of the chosen force field.  I would 
recommend always using infinite cutoffs for GB simulations.  It may improve your 
situation.


-Justin

--


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


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[gmx-users] Gromacs versions 4.0.5 and 4.5.4

2011-10-18 Thread Sapna Sarupria
Dear All,

I have a simulation set up for a mixture of carbon dioxide and water system
which runs perfectly on Gromacs 4.0.5 version. I have run these simulations
at different temperatures and pressures, from the same starting
configuration and the simulation proceeds smoothly in the 4.0.5 version.
However, when I use exactly the same files to run the simulation in 4.5.4
version, the system crashes and writes out several pdb files. I was
wondering if there is anything specific that has been changed between the
two versions. I have pasted the mdp file of the simulations below. Any input
will be much appreciated.

MDP File

title   =  100% occupancy CO2 hydrate ; a string
cpp   =  /lib/cpp ; c-preprocessor
dt  =  0.002; time step
nsteps  =  1500 ; number of steps
nstcomm  =  10   ; reset c.o.m. motion
nstxout  =  ; write coords
nstvout  =  ; write velocities
nstlog =  25000; print to logfile
nstenergy   =  500  ; print energies
xtc_grps  =  OW_HW1_HW2_CO2
nstxtcout =  1000
nstlist   =  10   ; update pairlist
ns_type=  grid ; pairlist method
coulombtype=  PME
rvdw  =  1.2  ; cut-off for vdw
rcoulomb  =  1.2  ; cut-off for coulomb
rlist=  1.2  ; cut-off for coulomb
DispCorr  =  EnerPres
Tcoupl  =  Nose-Hoover
ref_t  = 270
tc-grps  =  System
tau_t =  0.5
Pcoupl =  Parrinello-Rahman
Pcoupltype  =  semiisotropic; pressure geometry
tau_p=  1.0   1.0; p-coupoling time
compressibility   =  4.5e-5  4.5e-5   ; compressibility
ref_p =  30.5  30.5   ; ref pressure
gen_vel   =  yes  ; generate initial vel
gen_temp =  260  ; initial temperature
gen_seed =  372340   ; random seed
constraint_algorithm = shake
constraints =  all-bonds

---


Thank you,

Sincerely,
Sapna
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[gmx-users] reg g_rdf

2011-10-18 Thread vidhya sankar
Dear justin, 

   Thanks for your replies.
   i am doing Steered MD .. i would like to 
calculate radial Distribution function. of  Moving  group  with respect to 
Fixed   group . I am pulling only in Z direction then  is it possible to 
calculate RDF along Z-direction. only . it means Is there is any option in 
g_rdf  tools of gromacs Available?
Thanks in advance-- 
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Re: [gmx-users] Gromacs versions 4.0.5 and 4.5.4

2011-10-18 Thread Itamar Kass
HiSapna,I had the same problem few weeks ago.Apparently, some parameters are different (eg.nstpcouple).Cheers,ItamarPSI found out that I prefer to stick to 4.0.7.---BeginMessage---
That seems possible Mark. I had actually assumed that Itamar extracted  
a .gro from the 4.0.7 simulations and created a new .tpr with 4.5.4  
grompp. If that was the case, then I would still be surprised that it  
had instability problems. One sees a lot of charmm papers where people  
do slow heating, but my experience with gromacs is that not too many  
people worry about maintaining the velocities from their NVT  
simulations for their NPT simulations (or restrained - unrestrained)  
and that it works out just fine. On the other hand, I don't see too  
many gromacs reaction field studies either, so perhaps it all makes  
sense to those who use these methods.


Thanks again,
Chris.

On 2/09/2011 12:59 AM, chris.neale at utoronto.ca wrote:

That all makes sense Tsjerk.

I wonder if mdrun terminations based on LINCS warnings should come  
with an additional message to explain that one may try running for a  
while with nstpcouple=1.


That tip might be a good thing for the wiki page on that.



Also, I'm still a little curious about a question that Itamar asked  
a few posts ago:


If this is the case, why 5 ns simulations done with 4.0.7 crashed  
when extended it using 4.5.4?


Mark provided a good explanation about how this could be possible,  
but I've never seen lincs warnings or systems blowing up after 5 ns  
of equilibration. I fully realize that it may take even us of  
simulation to properly equilibrate statistical properties, but in my  
experience it is far outside of ordinary to require 5 ns of  
equilibration to avoid systems blowing up.


It's hard to say without more detail of how the extension occurred, and
knowing how much ensemble data got lost. It's still conceivable some
horrible mismatch occurred (e.g. virial over-written by some other
data), but not really worth exploring properly. I'd just expect to have
to re-equilibrate upon changing code version, and just not attempt such
an extension.

Mark



Chris.

-- original message --

Hi Chris,

I can imagine that the pressure scaling has a more profound effect on
the 'visible' surroundings if a cut-off is used, while this will not
be the case when using PME. So the shock for an atom when the
coordinates are adjusted can be expected to be greater with cut-off
based methods, rendering such simulations less stable. As for SD,
probably that causes sufficient damping of jitter introduced due to
pressure coupling for it not to propagate and cause problems.
But those are just my two cents (about 2.8 dollar cents with current  
rates :p).


Cheers,

Tsjerk

On Thu, Sep 1, 2011 at 2:41 PM, chris.neale at utoronto.ca wrote:

I am glad that the pressure coupling intervals have been identified as a
source of instability for poorly equilibrated systems as I was unaware of
that. Still, the fact that the SD integrator also solves the problem also
suggests that this is simply a poorly equilibrated system. I am not sure why
PME would run fine and reaction field would give lincs warnings, but then
again I have no experience with using a reaction field.

Chris.

On 1/09/2011 6:32 PM, Itamar Kass wrote:


Hi Tsjerk,

Thanks for the help, it actually worked. When nstpcouple is set to 1m the
system can be equilibrated (NPT) without LINCS error. I hadn't  
thought about

it as I never use NVT (unless doing FE calculations).


Equilibrating with NVT before NPT can be wise when the system starts far
from equilibrium.




Is this mean the 4.5.4 is more sensitive the 4.0.7? Is this effect the
data collected till now? If this is the case, why 5 ns simulations  
done with

4.0.7 crashed when extended it using 4.5.4?


IIRC 4.0.x and 4.5.x have different mechanisms for deciding how often to
do global communication for things like T and P coupling. Mostly you can
get away with the same kind of approximation one uses with twin-range
neighbour lists, periodic neighbour list updates, RESPA, etc. where
slowly-varying quantities don't have to be recalculated every step.
However during equilibration (and that includes the transition from
4.0.x to 4.5.x) those assumptions need not be valid. So tuning the
update frequency to be high during transitions is a good idea. Then
relax them and see how you go.

Mark



Also, is this mean I can do my productive run using 4.5.4 with the default
value of nstpcouple, it seems that setting it to 1 greatly increases the
computational time. To the best of my knowledge, in prior version  
nstpcouple

was set to 1 by default.

Cheers,
Itamar


On 01/09/2011, at 4:47 PM, Tsjerk Wassenaar wrote:


Hi Itamar,

I haven't really followed the discussion and I'm a bit too lazy to
look it all up now ;) But have you tried setting the nst parameters to
1  (except for output). Especially nstpcouple. Note that nstpcouple=1
requires nstlist=1 and nstcalcenergy=1. If that 

Re: [gmx-users] reg g_rdf

2011-10-18 Thread Justin A. Lemkul



vidhya sankar wrote:

Dear justin,
   Thanks for your replies.
   i am doing Steered MD .. i would like 
to calculate radial Distribution function. of  Moving  group  with 
respect to Fixed   group . I am pulling only in Z direction then  is it 
possible to calculate RDF along Z-direction. only . it means Is there is 
any option in g_rdf  tools of gromacs Available?


Not that I'm aware of, no.  g_rdf works in three dimensions (default) or in the 
x-y plane (for membranes and interfacial systems).


-Justin

--


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


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[gmx-users] reg g_rdf

2011-10-18 Thread vidhya sankar
Dear justin,
    Thanks for you Immediate  reply but When i surf  the 
following site  

http://www.linux-support.com/cms/en/component/content/article/12-man-pages/31116-g-rdf-calculates-radial-distribution-functions-man1
I got he following information 

g_rdf calculates radial distribution functions in different ways. The normal 
method is around a (set of) particle(s), the other method is around the center 
of mass of a set of particles. With both methods rdf’s can also be calculated 
around axes parallel to the z-axis with option -xy
 it represents what?  i need clarity
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Re: [gmx-users] Gromacs versions 4.0.5 and 4.5.4

2011-10-18 Thread Sapna Sarupria
Dear Itamar,

Thank you for your response. Why did you prefer to stick to 4.0.7? Is there
something particularly difficult to transfer from 4.0.7 version to 4.5
version?

Sapna

On Tue, Oct 18, 2011 at 9:36 PM, Itamar Kass itamar.k...@monash.edu wrote:

 Hi Sapna,

 I had the same problem few weeks ago.

 Apparently, some parameters are different (eg. nstpcouple).

 Cheers,
 Itamar

 PS I found out that I prefer to stick to 4.0.7.




 On 19/10/2011, at 12:08 PM, Sapna Sarupria wrote:

 Dear All,

 I have a simulation set up for a mixture of carbon dioxide and water system
 which runs perfectly on Gromacs 4.0.5 version. I have run these simulations
 at different temperatures and pressures, from the same starting
 configuration and the simulation proceeds smoothly in the 4.0.5 version.
 However, when I use exactly the same files to run the simulation in 4.5.4
 version, the system crashes and writes out several pdb files. I was
 wondering if there is anything specific that has been changed between the
 two versions. I have pasted the mdp file of the simulations below. Any input
 will be much appreciated.

 MDP File

 title   =  100% occupancy CO2 hydrate ; a string
 cpp   =  /lib/cpp ; c-preprocessor
 dt  =  0.002; time step
 nsteps  =  1500 ; number of steps
 nstcomm  =  10   ; reset c.o.m. motion
 nstxout  =  ; write coords
 nstvout  =  ; write velocities
 nstlog =  25000; print to logfile
 nstenergy   =  500  ; print energies
 xtc_grps  =  OW_HW1_HW2_CO2
 nstxtcout =  1000
 nstlist   =  10   ; update pairlist
 ns_type=  grid ; pairlist method
 coulombtype=  PME
 rvdw  =  1.2  ; cut-off for vdw
 rcoulomb  =  1.2  ; cut-off for coulomb
 rlist=  1.2  ; cut-off for coulomb
 DispCorr  =  EnerPres
 Tcoupl  =  Nose-Hoover
 ref_t  = 270
 tc-grps  =  System
 tau_t =  0.5
 Pcoupl =  Parrinello-Rahman
 Pcoupltype  =  semiisotropic; pressure geometry
 tau_p=  1.0   1.0; p-coupoling time
 compressibility   =  4.5e-5  4.5e-5   ; compressibility
 ref_p =  30.5  30.5   ; ref pressure
 gen_vel   =  yes  ; generate initial vel
 gen_temp =  260  ; initial temperature
 gen_seed =  372340   ; random seed
 constraint_algorithm = shake
 constraints =  all-bonds

 ---


 Thank you,

 Sincerely,
 Sapna
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 ===
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 |
 | Department of Biochemistry and Molecular Biology
 | Building 77 Clayton Campus
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 | Victoria 3800
 | Australia
 |
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 | Fax: +61 3 9902 9500
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Re: [gmx-users] reg g_rdf

2011-10-18 Thread Justin A. Lemkul



vidhya sankar wrote:

Dear justin,
Thanks for you Immediate  reply but When i surf  the 
following site 
http://www.linux-support.com/cms/en/component/content/article/12-man-pages/31116-g-rdf-calculates-radial-distribution-functions-man1

I got he following information
g_rdf calculates radial distribution functions in different ways. The 
normal method is around a (set of) particle(s), the other method is 
around the center of mass of a set of particles. With both methods rdf’s 
can also be calculated around axes parallel to the z-axis with option -xy

 it represents what?  i need clarity


I explained this previously.  With the -xy option, only the x- and y-dimensions 
are considered relative to the reference, which makes sense for systems like 
proteins in membranes.


-Justin

--


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


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Re: [gmx-users] Gromacs versions 4.0.5 and 4.5.4

2011-10-18 Thread Itamar Kass
Hi Sapna,

It is a good question, but such of personal preferences.  I found out that my 
simulations tend to crash more often when I am using 4.5.5. It might be the 
General-reaction -field I use or something else, I am not sure. Also, it seems 
I will not gain much from upgrading, so I stick to 4.0.7.

All this is not to say that 4.5.5 is not a good simulation package. It is a 
good and useful MD package, and I highly appreciate all the time and effort put 
into it.

Best,
Itamat

PS, there are still people around using 3.3.3 or even 3.2.1, so I am not that 
behind. 

On 19/10/2011, at 1:14 PM, Sapna Sarupria wrote:

 Dear Itamar,
 
 Thank you for your response. Why did you prefer to stick to 4.0.7? Is there 
 something particularly difficult to transfer from 4.0.7 version to 4.5 
 version?
 
 Sapna
 
 On Tue, Oct 18, 2011 at 9:36 PM, Itamar Kass itamar.k...@monash.edu wrote:
 Hi Sapna,
 
 I had the same problem few weeks ago.
 
 Apparently, some parameters are different (eg. nstpcouple).
 
 Cheers,
 Itamar
 
 PS I found out that I prefer to stick to 4.0.7.
 
 
 
 
 On 19/10/2011, at 12:08 PM, Sapna Sarupria wrote:
 
 Dear All,
 
 I have a simulation set up for a mixture of carbon dioxide and water system 
 which runs perfectly on Gromacs 4.0.5 version. I have run these simulations 
 at different temperatures and pressures, from the same starting 
 configuration and the simulation proceeds smoothly in the 4.0.5 version. 
 However, when I use exactly the same files to run the simulation in 4.5.4 
 version, the system crashes and writes out several pdb files. I was 
 wondering if there is anything specific that has been changed between the 
 two versions. I have pasted the mdp file of the simulations below. Any input 
 will be much appreciated.
 
 MDP File 
 
 title   =  100% occupancy CO2 hydrate ; a string
 cpp   =  /lib/cpp ; c-preprocessor
 dt  =  0.002; time step
 nsteps  =  1500 ; number of steps
 nstcomm  =  10   ; reset c.o.m. motion
 nstxout  =  ; write coords
 nstvout  =  ; write velocities
 nstlog =  25000; print to logfile
 nstenergy   =  500  ; print energies
 xtc_grps  =  OW_HW1_HW2_CO2 
 nstxtcout =  1000
 nstlist   =  10   ; update pairlist
 ns_type=  grid ; pairlist method
 coulombtype=  PME
 rvdw  =  1.2  ; cut-off for vdw
 rcoulomb  =  1.2  ; cut-off for coulomb
 rlist=  1.2  ; cut-off for coulomb
 DispCorr  =  EnerPres
 Tcoupl  =  Nose-Hoover
 ref_t  = 270 
 tc-grps  =  System
 tau_t =  0.5 
 Pcoupl =  Parrinello-Rahman
 Pcoupltype  =  semiisotropic; pressure geometry
 tau_p=  1.0   1.0; p-coupoling time
 compressibility   =  4.5e-5  4.5e-5   ; compressibility
 ref_p =  30.5  30.5   ; ref pressure
 gen_vel   =  yes  ; generate initial vel
 gen_temp =  260  ; initial temperature
 gen_seed =  372340   ; random seed
 constraint_algorithm = shake
 constraints =  all-bonds 
 
 ---
 
 
 Thank you,
 
 Sincerely,
 Sapna
 -- 
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at 
 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
 Please don't post (un)subscribe requests to the list. Use the 
 www interface or send it to gmx-users-requ...@gromacs.org.
 Can't post? Read http://www.gromacs.org/Support/Mailing_Lists
 
 -
 In theory, there is no difference between theory and practice. But, in 
 practice, there is. - Jan L.A. van de Snepscheut
 
 ===
 | Itamar Kass, Ph.D.
 | Postdoctoral Research Fellow
 |
 | Department of Biochemistry and Molecular Biology
 | Building 77 Clayton Campus
 | Wellington Road
 | Monash University,
 | Victoria 3800
 | Australia
 |
 | Tel: +61 3 9902 9376
 | Fax: +61 3 9902 9500
 | E-mail: itamar.k...@monash.edu
 
 
 
 --
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at 
 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
 Please don't post (un)subscribe requests to the list. Use the
 www interface or send it to gmx-users-requ...@gromacs.org.
 Can't post? Read http://www.gromacs.org/Support/Mailing_Lists
 
 
 
 -- 
 gmx-users mailing listgmx-users@gromacs.org
 

Re: [gmx-users] Gromacs versions 4.0.5 and 4.5.4

2011-10-18 Thread Justin A. Lemkul



Itamar Kass wrote:

Hi Sapna,

It is a good question, but such of personal preferences.  I found out 
that my simulations tend to crash more often when I am using 4.5.5. It 
might be the General-reaction -field I use or something else, I am not 
sure. Also, it seems I will not gain much from upgrading, so I stick to 
4.0.7.




The general instabilities result from tweaks to the handling of temperature and 
pressure coupling.  Simply setting nsttcouple and nstpcouple to 1 during the 
initial equilibration seems to give stable systems.


I'd say there are many reasons for upgrading.  Tons of new features, bug fixes, 
etc.  But then too, that's my personal preference ;)


-Justin

All this is not to say that 4.5.5 is not a good simulation package. It 
is a good and useful MD package, and I highly appreciate all the time 
and effort put into it.


Best,
Itamat

PS, there are still people around using 3.3.3 or even 3.2.1, so I am not 
that behind. 


On 19/10/2011, at 1:14 PM, Sapna Sarupria wrote:


Dear Itamar,

Thank you for your response. Why did you prefer to stick to 4.0.7? Is 
there something particularly difficult to transfer from 4.0.7 version 
to 4.5 version?


Sapna

On Tue, Oct 18, 2011 at 9:36 PM, Itamar Kass itamar.k...@monash.edu 
mailto:itamar.k...@monash.edu wrote:


Hi Sapna,

I had the same problem few weeks ago.

Apparently, some parameters are different (eg. nstpcouple).

Cheers,
Itamar

PS I found out that I prefer to stick to 4.0.7.




On 19/10/2011, at 12:08 PM, Sapna Sarupria wrote:


Dear All,

I have a simulation set up for a mixture of carbon dioxide and
water system which runs perfectly on Gromacs 4.0.5 version. I
have run these simulations at different temperatures and
pressures, from the same starting configuration and the
simulation proceeds smoothly in the 4.0.5 version. However, when
I use exactly the same files to run the simulation in 4.5.4
version, the system crashes and writes out several pdb files. I
was wondering if there is anything specific that has been changed
between the two versions. I have pasted the mdp file of the
simulations below. Any input will be much appreciated.

MDP File 


title   =  100% occupancy CO2 hydrate ; a string
cpp   =  /lib/cpp ; c-preprocessor
dt  =  0.002; time step
nsteps  =  1500 ; number of steps
nstcomm  =  10   ; reset c.o.m. motion
nstxout  =  ; write coords
nstvout  =  ; write velocities
nstlog =  25000; print to logfile
nstenergy   =  500  ; print energies
xtc_grps  =  OW_HW1_HW2_CO2 
nstxtcout =  1000

nstlist   =  10   ; update pairlist
ns_type=  grid ; pairlist method
coulombtype=  PME
rvdw  =  1.2  ; cut-off for vdw
rcoulomb  =  1.2  ; cut-off for coulomb
rlist=  1.2  ; cut-off
for coulomb
DispCorr  =  EnerPres
Tcoupl  =  Nose-Hoover
ref_t  = 270 
tc-grps  =  System
tau_t =  0.5 
Pcoupl =  Parrinello-Rahman

Pcoupltype  =  semiisotropic; pressure geometry
tau_p=  1.0   1.0; p-coupoling time
compressibility   =  4.5e-5  4.5e-5   ; compressibility
ref_p =  30.5  30.5   ; ref pressure
gen_vel   =  yes  ; generate
initial vel
gen_temp =  260  ; initial
temperature
gen_seed =  372340   ; random seed
constraint_algorithm = shake
constraints =  all-bonds 


---


Thank you,

Sincerely,
Sapna
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-
In theory, there is no difference between theory and practice.
But, in practice, there is. - Jan L.A. van de Snepscheut

===
| Itamar Kass, Ph.D.
| Postdoctoral Research Fellow
|
| Department of Biochemistry and Molecular Biology
| Building 77 Clayton Campus

[gmx-users] Using CHARMM force fields in Gromacs

2011-10-18 Thread Jernej Zidar
Dear all,
  I would like to do MD simulations of polymer binding to lipid bilayers.

  To that end I have generated the following components:
- CgenFF-based force field for the polymers' monomeric units (tested
in NAMD/CHARMM)
- CHARMM36 lipid force field for the lipid bilayers with some added
lipids (tested in NAMD/CHARMM)

  On the internet
(http://www.gromacs.org/Downloads/User_contributions/Force_fields) I
found the appropriate force fields (CgenFF and CHARMM36 for lipids).
How do I combine those with the monomeric residues I have generated
with ParamChem? I'm very familiar with Charmm, where all the necessary
force field can be easily combined, but I have no idea how to do it
Gromacs.

  Also worth mentioning: I will generate the initial structures of the
lipid bilayers and of the polymers in Charmm for Charmm is the only
package that can generate structures using just the internal
coordinates in the force field.

Thanks in advance for any help and tips,
Jernej Zidar
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Re: [gmx-users] calculation time

2011-10-18 Thread Mark Abraham

On 19/10/2011 5:26 AM, ahmet yıldırım wrote:

Dear users,

Sometimes, in the end ( in production simulation), Gromacs doesn't 
show calculation/finish time on screen, why? How can we show it?


I don't know what you mean.

Mark
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RE: [gmx-users] calculation time

2011-10-18 Thread Emanuel Birru
You can get them in the log file. (At the bottom)

Cheers,







=
Emanuel Birru
PhD Candidate

Faculty of Pharmacy and Pharmaceutical Sciences
Monash University (Parkville Campus)
381 Royal Parade, Parkville
Victoria 3052, Australia

Tel: Int + 61 3 9903 9187
E-mail: emanuel.bi...@monash.edu 
www.pharm.monash.edu.au

-Original Message-
From: gmx-users-boun...@gromacs.org [mailto:gmx-users-boun...@gromacs.org] On 
Behalf Of Mark Abraham
Sent: Wednesday, 19 October 2011 3:08 PM
To: Discussion list for GROMACS users
Subject: Re: [gmx-users] calculation time

On 19/10/2011 5:26 AM, ahmet yıldırım wrote:
 Dear users,

 Sometimes, in the end ( in production simulation), Gromacs doesn't 
 show calculation/finish time on screen, why? How can we show it?

I don't know what you mean.

Mark
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[gmx-users] atom names in ffbonded.itp (oplsaa.ff)

2011-10-18 Thread mu xiaojia
Dear gmx-users,

Does anyone know where can I find any explanations about the atom names in
ffbonded.itp file in oplsaa.ff? I am trying to compare the amino acids'
parameters in gromacs 4.5.4 with in tinker. Or where to find the default
parameters gromacs takes for amino acids in its aminoacids.rtp file?

For example, it is hard to guess what are C*, C_2  and C= in ffbonded.itp
file:

 C*HC  10.10800   284512.0   ;
  C C3  10.15220   265265.6   ; END
  C_2   C3  10.15220   265265.6   ; END
...
C= C= HC  1   120.000292.880   ; wlj
  C  C= HC  1   119.700292.880   ;

Thanks!

jia
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Re: [gmx-users] atom names in ffbonded.itp (oplsaa.ff)

2011-10-18 Thread Mark Abraham

On 19/10/2011 3:50 PM, mu xiaojia wrote:

Dear gmx-users,

Does anyone know where can I find any explanations about the atom 
names in ffbonded.itp file in oplsaa.ff? I am trying to compare the 
amino acids' parameters in gromacs 4.5.4 with in tinker. Or where to 
find the default parameters gromacs takes for amino acids in its 
aminoacids.rtp file?


For example, it is hard to guess what are C*, C_2  and C= in 
ffbonded.itp file:


 C*HC  10.10800   284512.0   ;
  C C3  10.15220   265265.6   ; END
  C_2   C3  10.15220   265265.6   ; END
...
C= C= HC  1   120.000292.880   ; wlj
  C  C= HC  1   119.700292.880   ;

Thanks!



You need to cross-reference the OPLS atom types (full description in 
their literature, partial description in atomtypes.atp) with the atom 
names in ffnonbonded.itp to make ffbonded.itp more clear.


Mark
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