RE: [gmx-users] Setting up an infinitely hard wall

2009-10-23 Thread Berk Hess

Hi,

I have obtained distributions with in infinite wall by simulating with an 
softer wall
and unbiasing with configurations with the wall potential.
But if you need the dynamics, or you want less hassle during the simulation,
you will have to do a bit more effort in coding an infinitely hard wall.

You will not only have to inverse the velocity, but also mirror the position
of the particle in the wall. This should on require a few lines of code in 
do_update_md
in src/mdlib/update.c.

Note that this will only work easily when you do not have constraints present.
With constraints things get much more complicated.

Berk

Date: Thu, 22 Oct 2009 14:34:06 -0700
From: kgp.a...@gmail.com
To: gmx-users@gromacs.org
Subject: [gmx-users] Setting up an infinitely hard wall

Hi everyone,
I am sending this email again hoping for any quick input for my question.



I have been trying to set up an infinitely hard potential wall. 
I tried to use the available wall options and could not really get it to do 
what i needed. I wanted a steep repulsive potential but when i created that, 
the system was blowing up, reason being that it requires smaller time step and 
i cant afford to have smaller time step. 


My idea to overcome this issue is to just reverse the velocity of the particle 
whenever it hits the wall. I am not sure if there is any thing in GROMACS which 
does this but any suggestions will be very helpful.


If there is nothing set up for something like above, i would like to play 
around with the code to figure it out. If this is the case, could somebody 
direct me to a starting point.


Thank you Amit

  
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Re: [gmx-users] Setting up an infinitely hard wall

2009-10-23 Thread Amit Choubey
Hi Berk,
Thank you for the response.

I have obtained distributions with in infinite wall by simulating with an
 softer wall
 and unbiasing with configurations with the wall potential.


Could you explain the above ? I am not sure if i get your point.


 But if you need the dynamics, or you want less hassle during the
 simulation,
 you will have to do a bit more effort in coding an infinitely hard wall.

 You will not only have to inverse the velocity, but also mirror the
 position
 of the particle in the wall.


That's true. I am sorry i didnt mention that.


 This should on require a few lines of code in do_update_md
 in src/mdlib/update.c.


Great, I will try this as soon as possible.


 Note that this will only work easily when you do not have constraints
 present.
 With constraints things get much more complicated.


I do have constraints present. Thank you for pointing this. I am working
with SPC water and I should, in principle be able to figure out the
co-ordinates of all atoms in the molecule if I am given one of the water's
atom's co-ordinate. Does that sound ok?

Thanks for the input again,
Amit



 Berk

 --
 Date: Thu, 22 Oct 2009 14:34:06 -0700
 From: kgp.a...@gmail.com
 To: gmx-users@gromacs.org
 Subject: [gmx-users] Setting up an infinitely hard wall


 Hi everyone,

 I am sending this email again hoping for any quick input for my question.



 I have been trying to set up an infinitely hard potential wall.

 I tried to use the available wall options and could not really get it to do
 what i needed. I wanted a steep repulsive potential but when i created that,
 the system was blowing up, reason being that it requires smaller time step
 and i cant afford to have smaller time step.

 My idea to overcome this issue is to just reverse the velocity of the
 particle whenever it hits the wall. I am not sure if there is any thing in
 GROMACS which does this but any suggestions will be very helpful.

 If there is nothing set up for something like above, i would like to play
 around with the code to figure it out. If this is the case, could somebody
 direct me to a starting point.

  Thank you
 Amit


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 New Windows 7: Find the right PC for you. Learn 
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Re: [gmx-users] POPG-Martini Force Field

2009-10-23 Thread XAvier Periole


On Oct 22, 2009, at 11:28 PM, Amit Choubey wrote:




On Thu, Oct 22, 2009 at 9:53 AM, S hv sola...@hotmail.com wrote:
Hi,

I am currently working with peptide/lipids interactions using the  
martini force field. I want to built a bacterial membrane, so I  
trying to find the

topology of the POPG lipid but until now without success.


In the martini_v2.0_lipids.itp file, the PG lipids are no included.  
I have seen some works using the martini force field and POPG  
lipids, e.g.,  The molecular mechanism monolayer PNAS 105,  
10803-10808, but they don't specify the topology of POPG lipids.


You can do this on your own just pull out the atomic structure of  
DPPC and POPG from any website. Compare atomistic DPPC with the  
Coarse Grained DPPC and it wont be hard to figure out the POPG CG  
topology.
That is certainly not that easy. A lot of parameterizations efforts  
have to be

involved.


BTW, the paper does give a short description about the topology of  
POPG
The best is probably to ask the authors of that paper to share their  
topology,

which they should.



I also tried in the martini web page, but I just found the  
martini_v2.0_lipids.itp file.


Could anyone help me to find such topology?

Thanks a lot for your time,

Salvador

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Re: [gmx-users] POPG-Martini Force Field

2009-10-23 Thread Amit Choubey
On Fri, Oct 23, 2009 at 12:33 AM, XAvier Periole x.peri...@rug.nl wrote:


 On Oct 22, 2009, at 11:28 PM, Amit Choubey wrote:



 On Thu, Oct 22, 2009 at 9:53 AM, S hv sola...@hotmail.com wrote:

  Hi,

 I am currently working with peptide/lipids interactions using the martini
 force field. I want to built a bacterial membrane, so I trying to find the
 topology of the POPG lipid but until now without success.




 In the martini_v2.0_lipids.itp file, the PG lipids are no included. I have
 seen some works using the martini force field and POPG lipids, e.g.,  The
 molecular mechanism monolayer PNAS 105, 10803-10808, but they don't specify
 the topology of POPG lipids.



 You can do this on your own just pull out the atomic structure of DPPC and 
 POPG from any website. Compare atomistic DPPC with the Coarse Grained DPPC 
 and it wont be hard to figure out the POPG CG topology.

 That is certainly not that easy. A lot of parameterizations efforts have to
 be
 involved.


No, thats easy because you are working with a coarse grained model. There
are are only few types of particles possible. The only tricky ones are the
head groups which the paper does mention.



 BTW, the paper does give a short description about the topology of POPG

 The best is probably to ask the authors of that paper to share their
 topology,
 which they should.



 I also tried in the martini web page, but I just found the
 martini_v2.0_lipids.itp file.

 Could anyone help me to find such topology?

 Thanks a lot for your time,

 Salvador

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RE: [gmx-users] Setting up an infinitely hard wall

2009-10-23 Thread Berk Hess

Hi,

If you have a wall potential, you can reweight the configurations
with weight 0 if one or more particles are beyond the wall
and exp(Vwall/kT) if no particles are beyond the wall.
This will only work efficiently if you choose the wall potential in a smart way.
I managed to get an efficiency of 70%.

If you have constraints, an atom that goes beyond the wall is directly
coupled to the atoms it is constrained to. You will have to work out
the equations for such a situation. It might be as simple that you can
just correct x and v for the atom that went beyond the wall and then
apply the constraints as normal.

Berk

Date: Fri, 23 Oct 2009 00:26:08 -0700
Subject: Re: [gmx-users] Setting up an infinitely hard wall
From: kgp.a...@gmail.com
To: gmx-users@gromacs.org

Hi Berk,
Thank you for the response.

I have obtained distributions with in infinite wall by simulating with an 
softer wall

and unbiasing with configurations with the wall potential.

Could you explain the above ? I am not sure if i get your point. 
But if you need the dynamics, or you want less hassle during the simulation,
you will have to do a bit more effort in coding an infinitely hard wall.

You will not only have to inverse the velocity, but also mirror the position

of the particle in the wall. 
That's true. I am sorry i didnt mention that. 
This should on require a few lines of code in do_update_md
in src/mdlib/update.c.

Great, I will try this as soon as possible. 

Note that this will only work easily when you do not have constraints present.
With constraints things get much more complicated.

I do have constraints present. Thank you for pointing this. I am working with 
SPC water and I should, in principle be able to figure out the co-ordinates of 
all atoms in the molecule if I am given one of the water's atom's co-ordinate. 
Does that sound ok?

Thanks for the input again,Amit 
Berk

Date: Thu, 22 Oct 2009 14:34:06 -0700

From: kgp.a...@gmail.com
To: gmx-users@gromacs.org
Subject: [gmx-users] Setting up an infinitely hard wall


Hi everyone,
I am sending this email again hoping for any quick input for my question.



I have been trying to set up an infinitely hard potential wall. 
I tried to use the available wall options and could not really get it to do 
what i needed. I wanted a steep repulsive potential but when i created that, 
the system was blowing up, reason being that it requires smaller time step and 
i cant afford to have smaller time step. 



My idea to overcome this issue is to just reverse the velocity of the particle 
whenever it hits the wall. I am not sure if there is any thing in GROMACS which 
does this but any suggestions will be very helpful.



If there is nothing set up for something like above, i would like to play 
around with the code to figure it out. If this is the case, could somebody 
direct me to a starting point.



Thank you Amit

  
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Re: [gmx-users] POPG-Martini Force Field

2009-10-23 Thread XAvier Periole


On Oct 23, 2009, at 9:45 AM, Amit Choubey wrote:




On Fri, Oct 23, 2009 at 12:33 AM, XAvier Periole x.peri...@rug.nl  
wrote:


On Oct 22, 2009, at 11:28 PM, Amit Choubey wrote:




On Thu, Oct 22, 2009 at 9:53 AM, S hv sola...@hotmail.com wrote:
Hi,

I am currently working with peptide/lipids interactions using the  
martini force field. I want to built a bacterial membrane, so I  
trying to find the

topology of the POPG lipid but until now without success.


In the martini_v2.0_lipids.itp file, the PG lipids are no included.  
I have seen some works using the martini force field and POPG  
lipids, e.g.,  The molecular mechanism monolayer PNAS 105,  
10803-10808, but they don't specify the topology of POPG lipids.


You can do this on your own just pull out the atomic structure of  
DPPC and POPG from any website. Compare atomistic DPPC with the  
Coarse Grained DPPC and it wont be hard to figure out the POPG CG  
topology.
That is certainly not that easy. A lot of parameterizations efforts  
have to be

involved.

No, thats easy because you are working with a coarse grained model.  
There are are only few types of particles possible. The only tricky  
ones are the head groups which the paper does mention.

If the bead type is given in the paper then the work is easier.
My point is that assimilate CG with simple is a big mistake!




BTW, the paper does give a short description about the topology of  
POPG
The best is probably to ask the authors of that paper to share their  
topology,

which they should.



I also tried in the martini web page, but I just found the  
martini_v2.0_lipids.itp file.


Could anyone help me to find such topology?

Thanks a lot for your time,

Salvador

Windows Live: Make it easier for your friends to see what you’re up  
to on Facebook.


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[gmx-users] Re: Chloroform (CHCl3) solvent box for G53a5 force field

2009-10-23 Thread Pablo Englebienne
Following up on the previous message, I noticed that the topology I 
previously sent (including 10 bonds) works for a minimization, but not 
for an MD simulation. grompp issues the following warning:


WARNING 1 [file topol.top, line 29]:
 Molecule type 'CHCL3' has 10 constraints.
 For stability and efficiency there should not be more constraints than
 internal number of degrees of freedom: 9.

I therefore used the following .itp file, with only the C-H and C-Cl bonds:

--[chcl3.itp]--
[ moleculetype ]
; Namenrexcl
CHCL3 1

[ atoms ]
;   nr   type  resnr residue  atom   cgnr charge   mass  
typeBchargeB  massB

1   HCHL  1  CHCL3   HChL  1  0.082  1.008
2   CCHL  1  CHCL3   CChL  1  0.179 12.011
3  CLCHL  1  CHCL3  CLCh1  1 -0.087 35.453
4  CLCHL  1  CHCL3  CLCh2  1 -0.087 35.453
5  CLCHL  1  CHCL3  CLCh3  1 -0.087 35.453

[ bonds ]
;  aiaj functc0c1c2c3
   1 2 2gb_39
   2 3 2gb_40
   2 4 2gb_40
   2 5 2gb_40

[ angles ]
;  aiajak functc0c1
c2c3

   1 2 3 2  ga_43
   1 2 4 2  ga_43
   1 2 5 2  ga_43
   3 2 4 2  ga_44
   3 2 5 2  ga_44
   4 2 5 2  ga_44

[ exclusions ]
1 2 3 4 5
2 1 3 4 5
3 1 2 4 5
4 1 2 3 5
5 1 2 3 4
--[chcl3.itp]--

These are the steps I took:
- build a box with 216 CHCL3 molecules with genbox
- adjusted the density to 1479 with editconf
- minimized the box to F100 (steep, 5 steps)
- equilibrated NVT (position restrained C), 100ps, 300K, tau_t 0.1
- equilibrated NPT (position restrained C), 100ps, 300K, 1bar, tau_t 
0.1, tau_p 2.0, compressibility 1e-4 (from CRC handbook)


Until here, everything looks decent, except for relatively large 
fluctuations in T (RMSD ~9K) and density (RMSD ~10kg m-3).


I then performed an unconstrained MD, 1ns, otherwise identical 
parameters to NPT equilibration. Temp (300K) and density (1450 kg m-3) 
stable, but fluctuating (RMSD 8 and 20 respectively).


In order to compare the results with Tironi and van Gunsteren, Molecular 
Physics 1994, 83, 381, who used the same GROMOS parameters: Epot = -28.6 
+/- 0.3 kJ/mol, density 1520 +/- 12 kg m-3.


This is the output I get from g_energy:

Energy  Average   RMSD Fluct.  Drift  
Tot-Drift

---
Potential  -4720.16119.141118.978 -0.0215895   
-21.5896


Therefore molar Epot = -(-4720)/216 = 21.9 kJ/mol. What factors could be 
accountable for the decrease wrt the reported value of 28.4? 
Experimental deltaHv is 31.4 kJ/mol (same reference).


Would there be any other parameters I should check before using this 
solvent box in production runs?


Regards,
Pablo

--
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Institute of Complex Molecular Systems (ICMS)
Eindhoven University of Technology, TU/e
PO Box 513, HG -1.26
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Tel +31 40 247 5349

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[gmx-users] how to stop duplicate atoms from being deleted

2009-10-23 Thread Jennifer Williams


Hello

I am studying a mesoporous silica for which there is no topology in  
gromacs-to try to automate the process of generating a topology file  
(x2top doesn?t work), I am using pdb2gmx (or rather trying to).


I have parameters for my silica structure and have added a new section  
for my molecule to the .rtp file, .atp file, atommass.dat,  
atom_nom.dbl, nb.itp and bon.itp files.


The problem is that when I use my .pdb file to generate a topology,  
pdb2gmx checks for duplicates and removes almost all of my atoms. It  
leaves only one of each type. I should have a few hundred of each atom  
type?here is the output from pdb2gmx?


Analyzing pdb file
There are 1 chains and 0 blocks of water and 1 residues with 4284 atoms
  chain  #res #atoms
  1 ' ' 1   4284
All occupancies are one

All ok up to here?and then?.

Processing chain 1 (4284 atoms, 1 residues)
There are 552 donors and 2580 acceptors
There are 1603 hydrogen bonds
Checking for duplicate atoms
Now there are 4 atoms. Deleted 4280 duplicates.

Can anyone explain why this is happening? ?none of my atoms have the  
same coordinates. Is there a file that I have forgotten to alter?  Is  
there is fix to turn off the checking of duplicate atoms? I don?t want  
any of my atoms to be deleted!


Below I paste an extract of my pdb file?

CRYST1   46.421   43.630   75.838  90.00  90.00 120.00 P 1   1
ATOM  1  SI   MCM   1 -21.090  -1.951 -29.596  1.00  0.00  SI
ATOM  2  SI   MCM   1 -21.090  -1.951 -10.636  1.00  0.00  SI
??..
ATOM   1153  OMCM   1  20.602 -18.404 -20.904  1.00  0.00   O
ATOM   1154  OMCM   1  20.602 -18.404  -1.945  1.00  0.00   O
?
ATOM   3181  OH   MCM   1  -6.620 -18.769 -32.169  1.00  0.00
ATOM   3182  OH   MCM   1  -6.620 -18.769 -13.210  1.00  0.00
.
ATOM   3733  HMCM   1  -6.674 -18.381 -33.035  1.00  0.00   H
ATOM   3734  HMCM   1  -6.616 -18.600 -14.144  1.00  0.00   H

Any advice appreciated,

Thanks in advance



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Scotland, with registration number SC005336.


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Re: [gmx-users] how to stop duplicate atoms from being deleted

2009-10-23 Thread Justin A. Lemkul
Quoting Jennifer Williams jennifer.willi...@ed.ac.uk:


 Hello

 I am studying a mesoporous silica for which there is no topology in
 gromacs-to try to automate the process of generating a topology file
 (x2top doesn?t work), I am using pdb2gmx (or rather trying to).

 I have parameters for my silica structure and have added a new section
 for my molecule to the .rtp file, .atp file, atommass.dat,
 atom_nom.dbl, nb.itp and bon.itp files.

 The problem is that when I use my .pdb file to generate a topology,
 pdb2gmx checks for duplicates and removes almost all of my atoms. It
 leaves only one of each type. I should have a few hundred of each atom
 type?here is the output from pdb2gmx?

 Analyzing pdb file
 There are 1 chains and 0 blocks of water and 1 residues with 4284 atoms
chain  #res #atoms
1 ' ' 1   4284
 All occupancies are one

 All ok up to here?and then?.

 Processing chain 1 (4284 atoms, 1 residues)
 There are 552 donors and 2580 acceptors
 There are 1603 hydrogen bonds
 Checking for duplicate atoms
 Now there are 4 atoms. Deleted 4280 duplicates.

 Can anyone explain why this is happening? ?none of my atoms have the
 same coordinates. Is there a file that I have forgotten to alter?  Is
 there is fix to turn off the checking of duplicate atoms? I don?t want
 any of my atoms to be deleted!

You have all of your atoms defined within one residue.  I'm assuming your .rtp
entry contains the definition of a single repeat unit, so each monomer should
be a separate residue.  The coordinates don't matter, it's because within each
residue, you have the same atom names, so pdb2gmx removes them when it finds
them.


 Below I paste an extract of my pdb file?


I'm assuming you'll have to probably reconstruct this file to re-organize the
atoms to define continuous residues.  It appears they are grouped by atom name,
which is probably not what you want.

-Justin

 CRYST1   46.421   43.630   75.838  90.00  90.00 120.00 P 1   1
 ATOM  1  SI   MCM   1 -21.090  -1.951 -29.596  1.00  0.00  SI
 ATOM  2  SI   MCM   1 -21.090  -1.951 -10.636  1.00  0.00  SI
 ??..
 ATOM   1153  OMCM   1  20.602 -18.404 -20.904  1.00  0.00   O
 ATOM   1154  OMCM   1  20.602 -18.404  -1.945  1.00  0.00   O
 ?
 ATOM   3181  OH   MCM   1  -6.620 -18.769 -32.169  1.00  0.00
 ATOM   3182  OH   MCM   1  -6.620 -18.769 -13.210  1.00  0.00
 .
 ATOM   3733  HMCM   1  -6.674 -18.381 -33.035  1.00  0.00   H
 ATOM   3734  HMCM   1  -6.616 -18.600 -14.144  1.00  0.00   H

 Any advice appreciated,

 Thanks in advance



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


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Graduate Research Assistant
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalem...@vt.edu | (540) 231-9080
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin/


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Re: [gmx-users] Re: Chloroform (CHCl3) solvent box for G53a5 force field

2009-10-23 Thread Justin A. Lemkul



Pablo Englebienne wrote:
Following up on the previous message, I noticed that the topology I 
previously sent (including 10 bonds) works for a minimization, but not 
for an MD simulation. grompp issues the following warning:


WARNING 1 [file topol.top, line 29]:
 Molecule type 'CHCL3' has 10 constraints.
 For stability and efficiency there should not be more constraints than
 internal number of degrees of freedom: 9.

I therefore used the following .itp file, with only the C-H and C-Cl bonds:



If bonds are supposed to be defined between, i.e. H-Cl and Cl-Cl, then this may 
not be appropriate.  Instead, you could perhaps set the covalent bonds as 
[constraints] in the topology, leaving the other nonbonded bonds as [bonds] 
(and then use constraints = none in the .mdp file, so only the [constraints] 
are used).



--[chcl3.itp]--
[ moleculetype ]
; Namenrexcl
CHCL3 1

[ atoms ]
;   nr   type  resnr residue  atom   cgnr charge   mass  
typeBchargeB  massB

1   HCHL  1  CHCL3   HChL  1  0.082  1.008
2   CCHL  1  CHCL3   CChL  1  0.179 12.011
3  CLCHL  1  CHCL3  CLCh1  1 -0.087 35.453
4  CLCHL  1  CHCL3  CLCh2  1 -0.087 35.453
5  CLCHL  1  CHCL3  CLCh3  1 -0.087 35.453

[ bonds ]
;  aiaj functc0c1c2c3
   1 2 2gb_39
   2 3 2gb_40
   2 4 2gb_40
   2 5 2gb_40

[ angles ]
;  aiajak functc0c1
c2c3

   1 2 3 2  ga_43
   1 2 4 2  ga_43
   1 2 5 2  ga_43
   3 2 4 2  ga_44
   3 2 5 2  ga_44
   4 2 5 2  ga_44

[ exclusions ]
1 2 3 4 5
2 1 3 4 5
3 1 2 4 5
4 1 2 3 5
5 1 2 3 4
--[chcl3.itp]--

These are the steps I took:
- build a box with 216 CHCL3 molecules with genbox
- adjusted the density to 1479 with editconf
- minimized the box to F100 (steep, 5 steps)
- equilibrated NVT (position restrained C), 100ps, 300K, tau_t 0.1
- equilibrated NPT (position restrained C), 100ps, 300K, 1bar, tau_t 
0.1, tau_p 2.0, compressibility 1e-4 (from CRC handbook)




What is the purpose of position restraints here?

Until here, everything looks decent, except for relatively large 
fluctuations in T (RMSD ~9K) and density (RMSD ~10kg m-3).




Probably a consequence of restraining the starting structure.  I'd say you're 
not equilibrating appropriately with position restraints imposed.


I then performed an unconstrained MD, 1ns, otherwise identical 
parameters to NPT equilibration. Temp (300K) and density (1450 kg m-3) 
stable, but fluctuating (RMSD 8 and 20 respectively).


In order to compare the results with Tironi and van Gunsteren, Molecular 
Physics 1994, 83, 381, who used the same GROMOS parameters: Epot = -28.6 
+/- 0.3 kJ/mol, density 1520 +/- 12 kg m-3.


This is the output I get from g_energy:

Energy  Average   RMSD Fluct.  Drift  
Tot-Drift
--- 

Potential  -4720.16119.141118.978 -0.0215895   
-21.5896


Therefore molar Epot = -(-4720)/216 = 21.9 kJ/mol. What factors could be 
accountable for the decrease wrt the reported value of 28.4? 
Experimental deltaHv is 31.4 kJ/mol (same reference).




Insufficient equilibration, and a variety of factors within the .mdp file.  If 
you want feedback on run parameters, you'll have to post the .mdp.


-Justin

Would there be any other parameters I should check before using this 
solvent box in production runs?


Regards,
Pablo



--


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


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Re: [gmx-users] how to stop duplicate atoms from being deleted

2009-10-23 Thread Jennifer Williams


Hi Justin,

Thanks for the reply. I am in fact studying one huge molecule. All of  
my atoms are bonded together in one large structure (kind of like a  
zeolite) so I have necessarily defined them as a single residue.


There is no way I can split this molecule into smaller subunits and  
thus define a number of residues-it wouldn't make sense to do so.


Yes in my .rtp file I have only defined each atom type once. To define  
each and every atom in my one residue would mean defining 4284 atoms!


I am having real trouble in creating topology files for my structure.  
At the moment, the only way I can do this is by using a tool in  
DL_POLY to create a field file and then manually change it to a .top  
file. This is really fiddely and I have a number of similar structures  
to do this for. I was hoping that I could do a similar step in Gromacs  
and get a .top file straight away-even if it means a bit more work  
setting it up.


Is there any hope or is pdb2gmx simply not designed to work for this  
sort of system?


Thanks

Jenny


Quoting Justin A. Lemkul jalem...@vt.edu:


Quoting Jennifer Williams jennifer.willi...@ed.ac.uk:



Hello

I am studying a mesoporous silica for which there is no topology in
gromacs-to try to automate the process of generating a topology file
(x2top doesn?t work), I am using pdb2gmx (or rather trying to).

I have parameters for my silica structure and have added a new section
for my molecule to the .rtp file, .atp file, atommass.dat,
atom_nom.dbl, nb.itp and bon.itp files.

The problem is that when I use my .pdb file to generate a topology,
pdb2gmx checks for duplicates and removes almost all of my atoms. It
leaves only one of each type. I should have a few hundred of each atom
type?here is the output from pdb2gmx?

Analyzing pdb file
There are 1 chains and 0 blocks of water and 1 residues with 4284 atoms
   chain  #res #atoms
   1 ' ' 1   4284
All occupancies are one

All ok up to here?and then?.

Processing chain 1 (4284 atoms, 1 residues)
There are 552 donors and 2580 acceptors
There are 1603 hydrogen bonds
Checking for duplicate atoms
Now there are 4 atoms. Deleted 4280 duplicates.

Can anyone explain why this is happening? ?none of my atoms have the
same coordinates. Is there a file that I have forgotten to alter?  Is
there is fix to turn off the checking of duplicate atoms? I don?t want
any of my atoms to be deleted!


You have all of your atoms defined within one residue.  I'm assuming  
 your .rtp

entry contains the definition of a single repeat unit, so each monomer should
be a separate residue.  The coordinates don't matter, it's because   
within each

residue, you have the same atom names, so pdb2gmx removes them when it finds
them.



Below I paste an extract of my pdb file?



I'm assuming you'll have to probably reconstruct this file to re-organize the
atoms to define continuous residues.  It appears they are grouped by  
 atom name,

which is probably not what you want.

-Justin


CRYST1   46.421   43.630   75.838  90.00  90.00 120.00 P 1   1
ATOM  1  SI   MCM   1 -21.090  -1.951 -29.596  1.00  0.00
SI
ATOM  2  SI   MCM   1 -21.090  -1.951 -10.636  1.00  0.00
SI

??..
ATOM   1153  OMCM   1  20.602 -18.404 -20.904  1.00  0.00
 O
ATOM   1154  OMCM   1  20.602 -18.404  -1.945  1.00  0.00
 O

?
ATOM   3181  OH   MCM   1  -6.620 -18.769 -32.169  1.00  0.00
ATOM   3182  OH   MCM   1  -6.620 -18.769 -13.210  1.00  0.00
.
ATOM   3733  HMCM   1  -6.674 -18.381 -33.035  1.00  0.00
 H
ATOM   3734  HMCM   1  -6.616 -18.600 -14.144  1.00  0.00
 H


Any advice appreciated,

Thanks in advance



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


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


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Dr. Jennifer Williams
Institute for 

Re: [gmx-users] how to stop duplicate atoms from being deleted

2009-10-23 Thread Justin A. Lemkul



Jennifer Williams wrote:


Hi Justin,

Thanks for the reply. I am in fact studying one huge molecule. All of my 
atoms are bonded together in one large structure (kind of like a 
zeolite) so I have necessarily defined them as a single residue.




I would argue that you have a polymer, which can certainly be handled by 
pdb2gmx.  See below.


There is no way I can split this molecule into smaller subunits and thus 
define a number of residues-it wouldn't make sense to do so.




If you have a lot of repetition, I would think it would be quite easy to split 
it apart.


Yes in my .rtp file I have only defined each atom type once. To define 
each and every atom in my one residue would mean defining 4284 atoms!




If you have a repeating structure, you have a polymer, so you can just decompose 
a repeat unit into a single .rtp entry.  That's the entire purpose of pdb2gmx, 
we certainly wouldn't want to create an .rtp entry for every single possible 
protein either!


For more information, see here:

http://www.gromacs.org/Documentation/How-tos/Polymers

I am having real trouble in creating topology files for my structure. At 
the moment, the only way I can do this is by using a tool in DL_POLY to 
create a field file and then manually change it to a .top file. This is 
really fiddely and I have a number of similar structures to do this for. 
I was hoping that I could do a similar step in Gromacs and get a .top 
file straight away-even if it means a bit more work setting it up.


Is there any hope or is pdb2gmx simply not designed to work for this 
sort of system?




You can certainly use pdb2gmx, it is intended to be versatile so it can be used 
with any repeating structure of monomers, homogenous (like a repeating polymer) 
or heterogenous (like a protein).  See the link above.


-Justin


Thanks

Jenny


Quoting Justin A. Lemkul jalem...@vt.edu:


Quoting Jennifer Williams jennifer.willi...@ed.ac.uk:



Hello

I am studying a mesoporous silica for which there is no topology in
gromacs-to try to automate the process of generating a topology file
(x2top doesn?t work), I am using pdb2gmx (or rather trying to).

I have parameters for my silica structure and have added a new section
for my molecule to the .rtp file, .atp file, atommass.dat,
atom_nom.dbl, nb.itp and bon.itp files.

The problem is that when I use my .pdb file to generate a topology,
pdb2gmx checks for duplicates and removes almost all of my atoms. It
leaves only one of each type. I should have a few hundred of each atom
type?here is the output from pdb2gmx?

Analyzing pdb file
There are 1 chains and 0 blocks of water and 1 residues with 4284 atoms
   chain  #res #atoms
   1 ' ' 1   4284
All occupancies are one

All ok up to here?and then?.

Processing chain 1 (4284 atoms, 1 residues)
There are 552 donors and 2580 acceptors
There are 1603 hydrogen bonds
Checking for duplicate atoms
Now there are 4 atoms. Deleted 4280 duplicates.

Can anyone explain why this is happening? ?none of my atoms have the
same coordinates. Is there a file that I have forgotten to alter?  Is
there is fix to turn off the checking of duplicate atoms? I don?t want
any of my atoms to be deleted!


You have all of your atoms defined within one residue.  I'm assuming 
 your .rtp
entry contains the definition of a single repeat unit, so each monomer 
should
be a separate residue.  The coordinates don't matter, it's because  
within each
residue, you have the same atom names, so pdb2gmx removes them when it 
finds

them.



Below I paste an extract of my pdb file?



I'm assuming you'll have to probably reconstruct this file to 
re-organize the
atoms to define continuous residues.  It appears they are grouped by 
 atom name,

which is probably not what you want.

-Justin


CRYST1   46.421   43.630   75.838  90.00  90.00 120.00 P 1   1
ATOM  1  SI   MCM   1 -21.090  -1.951 -29.596  1.00  0.00   
SI
ATOM  2  SI   MCM   1 -21.090  -1.951 -10.636  1.00  0.00   
SI

??..
ATOM   1153  OMCM   1  20.602 -18.404 -20.904  1.00  0.00   
 O
ATOM   1154  OMCM   1  20.602 -18.404  -1.945  1.00  0.00   
 O

?
ATOM   3181  OH   MCM   1  -6.620 -18.769 -32.169  1.00  0.00
ATOM   3182  OH   MCM   1  -6.620 -18.769 -13.210  1.00  0.00
.
ATOM   3733  HMCM   1  -6.674 -18.381 -33.035  1.00  0.00   
 H
ATOM   3734  HMCM   1  -6.616 -18.600 -14.144  1.00  0.00   
 H


Any advice appreciated,

Thanks in advance



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


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Re: [gmx-users] scripts to generate topology CG

2009-10-23 Thread Francesco Pietra
Hello Sunny:
I had already generated a valid .itp file for my protein using
seq2itp. That .itp works for both the protein itself and the protein
graphically inserted into a bilayer. When I add graphically further
water it does not work any more. I thought there is something else
that manages water without putting it everywhere. That script does not
help.

thanks
francesco

On Wed, Oct 21, 2009 at 3:46 PM, sunny mishra mishra.su...@gmail.com wrote:
 There is a seq2itp.pl script provided by martini folks in their
 website. You can get it from there.

 Sunny

 On Wed, Oct 21, 2009 at 9:42 AM, Francesco Pietra
 francesco.pie...@accademialucchese.it wrote:
 Hi:
 I am looking for scripts that generate topology in coarse grained.
 Thanks for indications.

 francesco pietra
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Re: [gmx-users] scripts to generate topology CG

2009-10-23 Thread Justin A. Lemkul



Francesco Pietra wrote:

Hello Sunny:
I had already generated a valid .itp file for my protein using
seq2itp. That .itp works for both the protein itself and the protein
graphically inserted into a bilayer. When I add graphically further
water it does not work any more. I thought there is something else
that manages water without putting it everywhere. That script does not
help.



In order to get a solution to your problem, I think you're going to have to 
explain your methodology more clearly, including command lines and actual error 
messages.  How are you adding water graphically?  Is genbox not working?  Can 
you not simply grep for the number of water molecules, i.e.:


grep W solvated.gro | wc -l

and use that number in the topology?

-Justin


thanks
francesco

On Wed, Oct 21, 2009 at 3:46 PM, sunny mishra mishra.su...@gmail.com wrote:

There is a seq2itp.pl script provided by martini folks in their
website. You can get it from there.

Sunny

On Wed, Oct 21, 2009 at 9:42 AM, Francesco Pietra
francesco.pie...@accademialucchese.it wrote:

Hi:
I am looking for scripts that generate topology in coarse grained.
Thanks for indications.

francesco pietra
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--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
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] how to calculate the vaporation enthalpy of pure small organic compound

2009-10-23 Thread Jinyao Wang
 Hi gmx-users,
I want to  calcualted the the vaporation enthalpy of benzaldehyde 
 I think that the the vaporation enthalpy is the sum of non-bond interacion 
among the benzaldehyde molecule.
So I made a NPT system simulation including 512 benzaldehyde molecule.  
The following is the intermolecule nonbond interaction using the g_energy.  

 LJ-(SR)= -21128.7 Kj/mol
 LJ-(LR)= -889.855 Kj/mol
 Coulomb-(SR)= -3884.6 Kj/mol
 Coul.-recip = -2261.51 Kj/mol
  the sum of non-bond interaction = LJ-(SR) + LJ-(LR) + Coulomb-(SR) + 
Coul.-recip = 28164.665 Kj/mol
   But the experimental value of he vaporation enthalpy = 50.3 Kj/mol
I have no ideal that why they have so much different. Now I don't know how to 
solve it.
Any suggestion will be appreciated.
 
 This following is my md.mdp file.

title   =  fws 
cpp =  /usr/bin/cpp 
constraints =   all-bonds
integrator  =  md
dt  =  0.002; ps !
nsteps  =  50   ; total 1ns
nstcomm =  1
nstxout =  500
nstvout =  0
nstfout =  0
nstlist =  10 
ns_type =  grid
rlist   =  1.0
coulombtype =  PME
rcoulomb=  1.0
vdwtype =  cut-off
rvdw=  1.4
fourierspacing  =  0.12
fourier_nx  =  0
fourier_ny  =  0
fourier_nz  =  0
pme_order   =  6
ewald_rtol  =  1e-5
optimize_fft=  yes
; Berendsen temperature coupling is on in three groups
Tcoupl  =  berendsen
tau_t   =  0.1
tc_grps =  system
ref_t   =  298.15
; Pressure coupling is on
Pcoupl  =  berendsen
tau_p   =  2.0
compressibility =  4.6e-5
ref_p   =  1.0
; Generate velocites is on at 323.15 K.
gen_vel =  yes
gen_temp=  298.15
gen_seed   =  173529

   
    Jinyao Wang
wan...@ciac.jl.cn
  2009-10-23
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Re: [gmx-users] how to calculate the vaporation enthalpy of pure small organic compound

2009-10-23 Thread Justin A. Lemkul



Jinyao Wang wrote:

 Hi gmx-users,
I want to  calcualted the the vaporation enthalpy of benzaldehyde 
 I think that the the vaporation enthalpy is the sum of non-bond interacion among the benzaldehyde molecule.
So I made a NPT system simulation including 512 benzaldehyde molecule.  
The following is the intermolecule nonbond interaction using the g_energy.	


 LJ-(SR)= -21128.7 Kj/mol
 LJ-(LR)= -889.855 Kj/mol
 Coulomb-(SR)= -3884.6 Kj/mol
 Coul.-recip = -2261.51 Kj/mol
  the sum of non-bond interaction = LJ-(SR) + LJ-(LR) + Coulomb-(SR) + 
Coul.-recip = 28164.665 Kj/mol
   But the experimental value of he vaporation enthalpy = 50.3 Kj/mol
I have no ideal that why they have so much different. Now I don't know how to 
solve it.
Any suggestion will be appreciated.
 


These are totals for the intermolecular energy of the system.  I'm guessing you 
didn't use -nmol 512 to calculate these results?


-Justin


 This following is my md.mdp file.

title   =  fws 
cpp =  /usr/bin/cpp 
constraints =   all-bonds

integrator  =  md
dt  =  0.002; ps !
nsteps  =  50   ; total 1ns
nstcomm =  1
nstxout =  500
nstvout =  0
nstfout =  0
nstlist =  10 
ns_type =  grid

rlist   =  1.0
coulombtype =  PME
rcoulomb=  1.0
vdwtype =  cut-off
rvdw=  1.4
fourierspacing  =  0.12
fourier_nx  =  0
fourier_ny  =  0
fourier_nz  =  0
pme_order   =  6
ewald_rtol  =  1e-5
optimize_fft=  yes
; Berendsen temperature coupling is on in three groups
Tcoupl  =  berendsen
tau_t   =  0.1
tc_grps =  system
ref_t   =  298.15
; Pressure coupling is on
Pcoupl  =  berendsen
tau_p   =  2.0
compressibility =  4.6e-5
ref_p   =  1.0
; Generate velocites is on at 323.15 K.
gen_vel =  yes
gen_temp=  298.15
gen_seed   =  173529

   
    Jinyao Wang
wan...@ciac.jl.cn
  2009-10-23




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--


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


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Re: [gmx-users] how to calculate the vaporation enthalpy of pure small organic compound

2009-10-23 Thread David van der Spoel

Justin A. Lemkul wrote:



Jinyao Wang wrote:

 Hi gmx-users,
I want to  calcualted the the vaporation enthalpy of benzaldehyde  I 
think that the the vaporation enthalpy is the sum of non-bond 
interacion among the benzaldehyde molecule.So I made a NPT system 
simulation including 512 benzaldehyde molecule.  The following is the 
intermolecule nonbond interaction using the g_energy.   


 LJ-(SR)= -21128.7 Kj/mol
 LJ-(LR)= -889.855 Kj/mol
 Coulomb-(SR)= -3884.6 Kj/mol
 Coul.-recip = -2261.51 Kj/mol
  the sum of non-bond interaction = LJ-(SR) + LJ-(LR) + Coulomb-(SR) + 
Coul.-recip = 28164.665 Kj/mol

   But the experimental value of he vaporation enthalpy = 50.3 Kj/mol
I have no ideal that why they have so much different. Now I don't know 
how to solve it.

Any suggestion will be appreciated.
 


These are totals for the intermolecular energy of the system.  I'm 
guessing you didn't use -nmol 512 to calculate these results?


And then subtract the gas-phase energy (with com removed) and add kT.


-Justin


 This following is my md.mdp file.

title   =  fws cpp =  /usr/bin/cpp 
constraints =   all-bonds

integrator  =  md
dt  =  0.002; ps !
nsteps  =  50   ; total 1ns
nstcomm =  1
nstxout =  500
nstvout =  0
nstfout =  0
nstlist =  10 ns_type =  grid
rlist   =  1.0
coulombtype =  PME
rcoulomb=  1.0
vdwtype =  cut-off
rvdw=  1.4
fourierspacing  =  0.12
fourier_nx  =  0
fourier_ny  =  0
fourier_nz  =  0
pme_order   =  6
ewald_rtol  =  1e-5
optimize_fft=  yes
; Berendsen temperature coupling is on in three groups
Tcoupl  =  berendsen
tau_t   =  0.1
tc_grps =  system
ref_t   =  298.15
; Pressure coupling is on
Pcoupl  =  berendsen
tau_p   =  2.0
compressibility =  4.6e-5
ref_p   =  1.0
; Generate velocites is on at 323.15 K.
gen_vel =  yes
gen_temp=  298.15
gen_seed   =  173529


   
    Jinyao Wang
wan...@ciac.jl.cn
  2009-10-23




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

2009-10-23 Thread Francesco Pietra
On Fri, Oct 23, 2009 at 4:14 PM, Justin A. Lemkul jalem...@vt.edu wrote:


 Francesco Pietra wrote:

 Hello Sunny:
 I had already generated a valid .itp file for my protein using
 seq2itp. That .itp works for both the protein itself and the protein
 graphically inserted into a bilayer. When I add graphically further
 water it does not work any more. I thought there is something else
 that manages water without putting it everywhere. That script does not
 help.


 In order to get a solution to your problem, I think you're going to have to
 explain your methodology more clearly, including command lines and actual
 error messages.  How are you adding water graphically?  Is genbox not
 working?  Can you not simply grep for the number of water molecules, i.e.:

 grep W solvated.gro | wc -l

 and use that number in the topology?

 -Justin

I'll organize to explain in more details. The methodology (all-atoms)
is explained in a few papers of mine and supplementary material, for
example: F. Pietra “ Docking and MD simulations of the interaction of
the tarantula peptide psalmotoxin‑1 with ASIC1a channels using  a
homology model” J. Chem. Inf. Model. 2009, 49, 972-977.

thanks
francesco




 thanks
 francesco

 On Wed, Oct 21, 2009 at 3:46 PM, sunny mishra mishra.su...@gmail.com
 wrote:

 There is a seq2itp.pl script provided by martini folks in their
 website. You can get it from there.

 Sunny

 On Wed, Oct 21, 2009 at 9:42 AM, Francesco Pietra
 francesco.pie...@accademialucchese.it wrote:

 Hi:
 I am looking for scripts that generate topology in coarse grained.
 Thanks for indications.

 francesco pietra
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 --
 

 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 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: Re: how to calculate the vaporation enthalpy of pure small organic compound (Justin A. Lemkul)

2009-10-23 Thread Jinyao Wang
Dear Justin,
  Thank you for your help. I indeed didn't use the option -nmol 512. 



Jinyao Wang wrote:
  Hi gmx-users,
 I want to  calcualted the the vaporation enthalpy of benzaldehyde 
  I think that the the vaporation enthalpy is the sum of non-bond interacion 
 among the benzaldehyde molecule.
 So I made a NPT system simulation including 512 benzaldehyde molecule.  
 The following is the intermolecule nonbond interaction using the g_energy.   
 
  LJ-(SR)= -21128.7 Kj/mol
  LJ-(LR)= -889.855 Kj/mol
  Coulomb-(SR)= -3884.6 Kj/mol
  Coul.-recip = -2261.51 Kj/mol
   the sum of non-bond interaction = LJ-(SR) + LJ-(LR) + Coulomb-(SR) + 
 Coul.-recip = 28164.665 Kj/mol
But the experimental value of he vaporation enthalpy = 50.3 Kj/mol
 I have no ideal that why they have so much different. Now I don't know how 
 to solve it.
 Any suggestion will be appreciated.
  

These are totals for the intermolecular energy of the system.  I'm guessing 
you 
didn't use -nmol 512 to calculate these results?

-Justin

  This following is my md.mdp file.
 
 title   =  fws 
 cpp =  /usr/bin/cpp 
 constraints =   all-bonds
 integrator  =  md
 dt  =  0.002; ps !
 nsteps  =  50   ; total 1ns
 nstcomm =  1
 nstxout =  500
 nstvout =  0
 nstfout =  0
 nstlist =  10 
 ns_type =  grid
 rlist   =  1.0
 coulombtype =  PME
 rcoulomb=  1.0
 vdwtype =  cut-off
 rvdw=  1.4
 fourierspacing  =  0.12
 fourier_nx  =  0
 fourier_ny  =  0
 fourier_nz  =  0
 pme_order   =  6
 ewald_rtol  =  1e-5
 optimize_fft=  yes
 ; Berendsen temperature coupling is on in three groups
 Tcoupl  =  berendsen
 tau_t   =  0.1
 tc_grps =  system
 ref_t   =  298.15
 ; Pressure coupling is on
 Pcoupl  =  berendsen
 tau_p   =  2.0
 compressibility =  4.6e-5
 ref_p   =  1.0
 ; Generate velocites is on at 323.15 K.
 gen_vel =  yes
 gen_temp=  298.15
 gen_seed   =  173529 
 
 �
���Jinyao Wang
 wan...@ciac.jl.cn
 ��2009-10-23
 
 
 
 
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-- 


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
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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End of gmx-users Digest, Vol 66, Issue 157
**

= = = = = = = = = = = = = = = = = = = =


致
礼!
 
 
Jinyao Wang
wan...@ciac.jl.cn
  2009-10-23

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Fwd: [gmx-users] scripts to generate topology CG

2009-10-23 Thread Francesco Pietra
-- Forwarded message --
From: Francesco Pietra francesco.pie...@accademialucchese.it
Date: Fri, Oct 23, 2009 at 5:01 PM
Subject: Re: [gmx-users] scripts to generate topology CG
To: jalem...@vt.edu, Discussion list for GROMACS users gmx-users@gromacs.org


On Fri, Oct 23, 2009 at 4:14 PM, Justin A. Lemkul jalem...@vt.edu wrote:


 Francesco Pietra wrote:

 Hello Sunny:
 I had already generated a valid .itp file for my protein using
 seq2itp. That .itp works for both the protein itself and the protein
 graphically inserted into a bilayer. When I add graphically further
 water it does not work any more. I thought there is something else
 that manages water without putting it everywhere. That script does not
 help.


 In order to get a solution to your problem, I think you're going to have to
 explain your methodology more clearly, including command lines and actual
 error messages.  How are you adding water graphically?  Is genbox not
 working?  Can you not simply grep for the number of water molecules, i.e.:

 grep W solvated.gro | wc -l

 and use that number in the topology?

I forgot to add that the graphic program uses the above grep command,
giving the same number of W as the line command. The number of DCCP is
diminished by those deleted in inserting the protein, but the grompp
command complains that .gro does not matches .top. If no further water
is added graphically, everything works.


 -Justin

I'll organize to explain in more details. The methodology (all-atoms)
is explained in a few papers of mine and supplementary material, for
example: F. Pietra “ Docking and MD simulations of the interaction of
the tarantula peptide psalmotoxin‑1 with ASIC1a channels using  a
homology model” J. Chem. Inf. Model. 2009, 49, 972-977.

thanks
francesco




 thanks
 francesco

 On Wed, Oct 21, 2009 at 3:46 PM, sunny mishra mishra.su...@gmail.com
 wrote:

 There is a seq2itp.pl script provided by martini folks in their
 website. You can get it from there.

 Sunny

 On Wed, Oct 21, 2009 at 9:42 AM, Francesco Pietra
 francesco.pie...@accademialucchese.it wrote:

 Hi:
 I am looking for scripts that generate topology in coarse grained.
 Thanks for indications.

 francesco pietra
 ___
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 http://lists.gromacs.org/mailman/listinfo/gmx-users
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 Can't post? Read http://www.gromacs.org/mailing_lists/users.php

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 --
 

 Justin A. Lemkul
 Ph.D. Candidate
 ICTAS Doctoral Scholar
 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] scripts to generate topology CG

2009-10-23 Thread Justin A. Lemkul



Francesco Pietra wrote:

On Fri, Oct 23, 2009 at 4:14 PM, Justin A. Lemkul jalem...@vt.edu wrote:


Francesco Pietra wrote:

Hello Sunny:
I had already generated a valid .itp file for my protein using
seq2itp. That .itp works for both the protein itself and the protein
graphically inserted into a bilayer. When I add graphically further
water it does not work any more. I thought there is something else
that manages water without putting it everywhere. That script does not
help.


In order to get a solution to your problem, I think you're going to have to
explain your methodology more clearly, including command lines and actual
error messages.  How are you adding water graphically?  Is genbox not
working?  Can you not simply grep for the number of water molecules, i.e.:

grep W solvated.gro | wc -l

and use that number in the topology?

-Justin


I'll organize to explain in more details. The methodology (all-atoms)
is explained in a few papers of mine and supplementary material, for
example: F. Pietra “ Docking and MD simulations of the interaction of
the tarantula peptide psalmotoxin‑1 with ASIC1a channels using  a
homology model” J. Chem. Inf. Model. 2009, 49, 972-977.



I read the methods there, and one of your own references therein, but it doesn't 
really help that much.  I understand what you're aiming for, but atomistic 
system preparation in AMBER and coarse-grain system preparation in GROMACS is 
like comparing apples and oranges.  Seeing details of successful methodology 
doesn't illuminate the problems you're currently having.  I still don't know 
what you're trying to do in GROMACS that's causing a problem.


Again, it would be helpful to see the commands you're issuing, and any other 
pertinent information (especially error messages, topology snippets, etc) to 
better diagnose your problem.  If solvation is the issue, I maintain that genbox 
can do the job much like Leap does in AMBER.  You may have to take a few tips 
from this page about adding water:


http://www.gromacs.org/Documentation/How-tos/Membrane_Simulations

-Justin


thanks
francesco




thanks
francesco

On Wed, Oct 21, 2009 at 3:46 PM, sunny mishra mishra.su...@gmail.com
wrote:

There is a seq2itp.pl script provided by martini folks in their
website. You can get it from there.

Sunny

On Wed, Oct 21, 2009 at 9:42 AM, Francesco Pietra
francesco.pie...@accademialucchese.it wrote:

Hi:
I am looking for scripts that generate topology in coarse grained.
Thanks for indications.

francesco pietra
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--


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


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--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
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: Fwd: [gmx-users] scripts to generate topology CG

2009-10-23 Thread Justin A. Lemkul



Francesco Pietra wrote:


grep W solvated.gro | wc -l

and use that number in the topology?


I forgot to add that the graphic program uses the above grep command,


I don't understand this statement.


giving the same number of W as the line command. The number of DCCP is
diminished by those deleted in inserting the protein, but the grompp
command complains that .gro does not matches .top. If no further water
is added graphically, everything works.


This is where exact commands (in sequence) really help, or at least a stepwise 
procedure.  Are you adding a protein into a box that contains DCCP+water, or are 
you inserting the protein into DCCP, then adding water?


What is the exact error that grompp is giving you?  That the number of 
coordinates don't match? atom names don't match?


-Justin

--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
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] How can measure the end-yo end distance of a peptide from the .xtc file

2009-10-23 Thread haifeng YUAN

Dear all,
I would like to get the distance information of the small 
peptide chain from the .xtc file, but the g_mindist seems can only get 
the distance information from one group to another. How I can get the 
end to end distance? I mean  the distance between an end atom  of the 
short chain to the other end atom?

Thanks in advance.

Cheers,
Haifeng YUAN

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Re: [gmx-users] How can measure the end-yo end distance of a peptide from the .xtc file

2009-10-23 Thread Justin A. Lemkul



haifeng YUAN wrote:

Dear all,
I would like to get the distance information of the small 
peptide chain from the .xtc file, but the g_mindist seems can only get 
the distance information from one group to another. How I can get the 
end to end distance? I mean  the distance between an end atom  of the 
short chain to the other end atom?


g_dist with appropriate index groups.

-Justin


Thanks in advance.

Cheers,
Haifeng YUAN

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--


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


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Re: [gmx-users] how to stop duplicate atoms from being deleted

2009-10-23 Thread Jennifer Williams


Thanks again for the help. I?ve given it a go but am not overly  
confident or exactly sure how I would translate this method to my  
system.


This is because rather than having a chain with a well defined start  
and finish I have a giant covalent structure (like a web) where each  
silicon is tetrahedrally bound to oxygen (as in quartz).


 O?
 |
  ?O-Si-O ?
 |
 O?

Here I describe my efforts so far.

I have defined a monomer (my internal unit) as an SiO4 tetrahedra.
Therefore each monomer would have to form 4 bonds with other monomers.  
I have defined my internal residue like this:


; Internal residue
[ MCM_I ]
 [ atoms ]
   SISI1.280 1
   O1O1   -0.640 1
   O2O2   -0.640 1
   O3O3   -0.640 1
   O4O4   -0.640 1

  [ bonds ]
SIO1
SIO2
SIO3
SIO4
O1   -SI
O2   -SI
O3   +SI
O4   +SI

As an aside-This means that each residue is not neutral as the charges  
cancel out over the entire molecule and not over a single residue-I am  
not sure of the implications of this.


To complicate matters, in my structure not all of the oxygens are  
bonded oxygens (i.e where each O is bonded to 2 silicons, some of the  
oxygens terminate in hydroxyl groups). This means that I have will  
have 3 types of terminal/starting chain


1. Si, O, O, OH
2. SI, O, OH, OH
3. SI, OH, OH, OH (the group which really does terminate)

Here are my terminal and starting residues:


; terminal residue 1 (3OH groups)
[ MCM_T1 ]
 [ atoms ]
   SISI 1.280 1
  OH1OH1   -0.502 1
   H1H1 0.206 1
  OH2OH2   -0.502 1
   H2H2 0.206 1
  OH3OH3   -0.502 1
   H3H3 0.206 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SI   OH2
SI   OH3
SIO4
OH1   H1
OH2   H2
OH3   H3
 O4  -SI

; terminal residue 2 (2 OH groups)
[ MCM_T2 ]
 [ atoms ]
  SISI 1.280 1
  OH1   OH1-0.502 1
   H1H1 0.206 1
  OH2   OH2-0.502 1
   H2H2 0.206 1
   O3O3-0.640 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SI   OH2
SIO3
SIO4
OH1   H1
OH2   H2
 O3  -SI
 O4  -SI


; terminal residue 3 (1 OH group)
[ MCM_T3 ]
 [ atoms ]
  SI   SI 1.280 1
  OH1   OH1-0.502 1
   H1H1 0.206 1
   O2O2-0.640 1
   O3O3-0.640 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SIO2
SIO3
SIO4
OH1H1
 O2  -SI
 O3  -SI
 O4  -SI

As each of these groups could equally be starting groups-I have  
defined them as such by changing the minus sign to a plus


; starting residue 1
[ MCM_S1 ]
 [ atoms ]
  SISI1.280 1
  OH1OH1   -0.502 1
   H1H1 0.206 1
  OH2OH2   -0.502 1
   H2H2 0.206 1
  OH3OH3   -0.502 1
   H3H3 0.206 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SI   OH2
SI   OH3
SIO4
 O4  +SI

; starting residue 2
[ MCM_T2 ]
 [ atoms ]
  SISI 1.280 1
  OH1   OH1-0.502 1
   H1H1 0.206 1
  OH2   OH2-0.502 1
   H2H2 0.206 1
   O3O3-0.640 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SI   OH2
SIO3
SIO4
 O3  +SI
 O4  +SI


; starting residue 3
[ MCM_T3 ]
 [ atoms ]
  SI   SI 1.280 1
  OH1   OH1-0.502 1
   H1H1 0.206 1
   O2O2-0.640 1
   O3O3-0.640 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SIO2
SIO3
SIO4
 O2  +SI
 O3  +SI
 O4  +SI


There are a few problems with this:

1.	I don?t know how to go about splitting my large .pdb file into  
monomers. At the moment it is ordered by atomtype VMD doesn?t  
recognise my self- defined SiO2 tetrahedra as monomers so I can?t sort  
using that. There is no way I can do this manually by looking at the  
coordinates.


2.	Looking at the terminal residue 1 for example, I have defined the  
only non-bonded oxygen as O4-however it could equally be O1, O2 or  
O3-this leads to a number of possible combinations of my terminal and  
internal residues.


3.	There is in fact no such thing as a terminal residue (except in the  
case of Terminal residue 1 which is rare). It is more common to have a  
2 OH groups on a silicon meaning the other oxygens bond to further  
residues.


I can see how this method works nicely for a chain but having a four  
coordinate system really complicates things! I have run a very simple  
pdb file using pdb2gmx, the new .rtp file above and a handwritten .pdb  
file with 2 monomers.
The result is that pdb2gmx  is creating extra bonds between the  
Silicon of one monomer and the oxygen of the next meaning I am getting  
a 5-coordinate Silicon.


Pdb2gmx doesn?t seem to be able to distinguish based on bond distances  

Re: [gmx-users] how to stop duplicate atoms from being deleted

2009-10-23 Thread Justin A. Lemkul



Jennifer Williams wrote:


Thanks again for the help. I?ve given it a go but am not overly 
confident or exactly sure how I would translate this method to my system.


This is because rather than having a chain with a well defined start and 
finish I have a giant covalent structure (like a web) where each silicon 
is tetrahedrally bound to oxygen (as in quartz).


 O?
 |
  ?O-Si-O ?
 |
 O?

Here I describe my efforts so far.

I have defined a monomer (my internal unit) as an SiO4 tetrahedra.   
Therefore each monomer would have to form 4 bonds with other monomers. I 
have defined my internal residue like this:


; Internal residue
[ MCM_I ]
 [ atoms ]
   SISI1.280 1
   O1O1   -0.640 1
   O2O2   -0.640 1
   O3O3   -0.640 1
   O4O4   -0.640 1

  [ bonds ]
SIO1
SIO2
SIO3
SIO4
O1   -SI
O2   -SI
O3   +SI
O4   +SI

As an aside-This means that each residue is not neutral as the charges 
cancel out over the entire molecule and not over a single residue-I am 
not sure of the implications of this.


To complicate matters, in my structure not all of the oxygens are bonded 
oxygens (i.e where each O is bonded to 2 silicons, some of the oxygens 
terminate in hydroxyl groups). This means that I have will have 3 types 
of terminal/starting chain


1. Si, O, O, OH
2. SI, O, OH, OH
3. SI, OH, OH, OH (the group which really does terminate)

Here are my terminal and starting residues:


; terminal residue 1 (3OH groups)
[ MCM_T1 ]
 [ atoms ]
   SISI 1.280 1
  OH1OH1   -0.502 1
   H1H1 0.206 1
  OH2OH2   -0.502 1
   H2H2 0.206 1
  OH3OH3   -0.502 1
   H3H3 0.206 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SI   OH2
SI   OH3
SIO4
OH1   H1
OH2   H2
OH3   H3
 O4  -SI

; terminal residue 2 (2 OH groups)
[ MCM_T2 ]
 [ atoms ]
  SISI 1.280 1
  OH1   OH1-0.502 1
   H1H1 0.206 1
  OH2   OH2-0.502 1
   H2H2 0.206 1
   O3O3-0.640 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SI   OH2
SIO3
SIO4
OH1   H1
OH2   H2
 O3  -SI
 O4  -SI


; terminal residue 3 (1 OH group)
[ MCM_T3 ]
 [ atoms ]
  SI   SI 1.280 1
  OH1   OH1-0.502 1
   H1H1 0.206 1
   O2O2-0.640 1
   O3O3-0.640 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SIO2
SIO3
SIO4
OH1H1
 O2  -SI
 O3  -SI
 O4  -SI

As each of these groups could equally be starting groups-I have defined 
them as such by changing the minus sign to a plus


; starting residue 1
[ MCM_S1 ]
 [ atoms ]
  SISI1.280 1
  OH1OH1   -0.502 1
   H1H1 0.206 1
  OH2OH2   -0.502 1
   H2H2 0.206 1
  OH3OH3   -0.502 1
   H3H3 0.206 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SI   OH2
SI   OH3
SIO4
 O4  +SI

; starting residue 2
[ MCM_T2 ]
 [ atoms ]
  SISI 1.280 1
  OH1   OH1-0.502 1
   H1H1 0.206 1
  OH2   OH2-0.502 1
   H2H2 0.206 1
   O3O3-0.640 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SI   OH2
SIO3
SIO4
 O3  +SI
 O4  +SI


; starting residue 3
[ MCM_T3 ]
 [ atoms ]
  SI   SI 1.280 1
  OH1   OH1-0.502 1
   H1H1 0.206 1
   O2O2-0.640 1
   O3O3-0.640 1
   O4O4-0.640 1

  [ bonds ]
SI   OH1
SIO2
SIO3
SIO4
 O2  +SI
 O3  +SI
 O4  +SI


There are a few problems with this:

1.I don?t know how to go about splitting my large .pdb file into 
monomers. At the moment it is ordered by atomtype VMD doesn?t recognise 
my self- defined SiO2 tetrahedra as monomers so I can?t sort using that. 
There is no way I can do this manually by looking at the coordinates.


2.Looking at the terminal residue 1 for example, I have defined the 
only non-bonded oxygen as O4-however it could equally be O1, O2 or 
O3-this leads to a number of possible combinations of my terminal and 
internal residues.


3.There is in fact no such thing as a terminal residue (except in 
the case of Terminal residue 1 which is rare). It is more common to have 
a 2 OH groups on a silicon meaning the other oxygens bond to further 
residues.


I can see how this method works nicely for a chain but having a four 
coordinate system really complicates things! I have run a very simple 
pdb file using pdb2gmx, the new .rtp file above and a handwritten .pdb 
file with 2 monomers.
The result is that pdb2gmx  is creating extra bonds between the Silicon 
of one monomer and the oxygen of the next meaning I am getting a 
5-coordinate Silicon.


Pdb2gmx doesn?t seem to be able to distinguish based on bond 

Re: [gmx-users] how to stop duplicate atoms from being deleted

2009-10-23 Thread Justin A. Lemkul



Justin A. Lemkul wrote:

I can see how this rapidly becomes difficult :)  I don't believe that 
pdb2gmx can handle such multi-directional bonding, since the residues 
that are connected are not necessarily numerically sequential.


I should amend this statement (typing quicker than the brain can keep up!) - It 
is not that pdb2gmx cannot handle multi-directional bonding, it is moreso that I 
don't think it cannot be done using the +/- convention of the .rtp files.


Using specbond.dat, as I suggested before, should be a viable alternative.

-Justin

--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
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] positional restraint

2009-10-23 Thread krishnakumar
Hi,

I was wondering if it would be possible to apply positional restraint to an
atom w.r.t an arbitrary coordinate.

Say for eg. I want to constrain the distance between an atom and the
origin(0,0,0) during MD.
Is it possible to  do that in GROMACS.

Thanks
Krishna
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[gmx-users] Which membrane result is more reliable?

2009-10-23 Thread Kirill Bessonov
Hello Justin,

You helped me before, and I am grateful for that. So basically my summer
research had ended up with the following results:

I have included my *.ipt files this message is long.

*My question: 1)why once simulation is giving  me stable aplha-helix and
other is not if membranes are similar and conditions kept constant.

* 2) Which result to use, most probale. Does lipid
density might of affected the stability?



-200ns  Simulation of the same peptide in the DMPC only box and in
DMPC/DMPE box [1:1 ratio] but results are different and I want to ask why as
this data will go as part of the paper.

*System:* peptide that is placed on TOP of the membrane, interacting with
lipids (no inserted into the membrane, but floating on top) and above there
are water molecules
*
DMPC membrane simulation - STABLE Peptide Helix, no uncoiling:*

- 248 DMPC molecules
-Box 9.03 x 9.03 x 10.15 as found at the bottom of gro file (I think this
dimensions are nm units?)
- Threfore I calculated that Area per Lipid is only: 2facesx90.3^2
A^2/248DMPC = 65.75 A^2/lipid which is low

- When I was using InflatGro(which I modified to be much more friendly and
accepts 2 lipids) to check the lipid density the values were:
___

Input *.gro file to shrink or expand:dmpc.gro
Enter  membrane re-scaling factor (default=0.95):*1*
Enter Lipid#1 name (e.g. DMPC):DMPC
Enter Lipid#2 name (e.g. DMPE) otherwise ENTER:
For spacial overlap estimation between lipids...
Please enter distance cutoff value between lipids in A(default = 14):14
Output file name(e.g.'inflated.gro'):rm.gro
Gridsize for area per lipid calculations in A(default = 5):5

TOTAL Area per protein: 1.5 nm^2 or 150.00 A^2
*TOTAL Area per lipid:   0.67  nm^2   or  67.26  A^2*  -- why different
from prev. calculation, slightly smaller?

Area per protein, upper half:  0.000 nm^2or  0.000 A^2
Area per lipid, upper leaflet :  0.632  nm^2 or 63.210 A^2

Area per protein, lower half:   1.50 nm^2or 150.00  A^2
Area per lipid, lower leaflet :   0.73  nm^2 or  73.43 A^2
___

Total Energy:

Statistics over 82987501 steps [ 109970.0078 thru 275945. ps ], 1 data
sets
All averages are exact over 82987501 steps

Energy  Average   RMSD Fluct.  Drift
Tot-Drift
---
*Total Energy-891474 *kJ/mol   1132.811131.48
-0.00114556   -190.135

T-Protein   309.844  25.330725.3304
-2.37026e-06  -0.393404



*DMPE/DMPC membrane simulation - Becomes UNSTABLE after 100ns simulation
time *

- 93 DMPC and 93 DMPE molecules
-Density: 2faces*68.2*68.2 / 186 lipids = 50 A^2/lipid

- InflateGro results:
_
TOTAL Area per protein: 0 nm^2   or   0.00 A^2
*TOTAL Area per lipid:   0.49  nm^2   or  48.52  A^2* again smaller?

Area per protein, upper half:  0.000 nm^2or  0.000 A^2
Area per lipid, upper leaflet :  0.485  nm^2 or 48.517 A^2

Area per protein, lower half:   0.00 nm^2or   0.00  A^2
Area per lipid, lower leaflet :   0.49  nm^2 or  48.52 A^2

Writing Area per lipid...
Done!
___

DMPC: has 46 atoms and DMPE: has 46 atoms

Total Energy:
Statistics over 10001 steps [ 0. thru 20.0156 ps ], 1 data sets
All averages are exact over 10001 steps

Energy  Average   RMSD
Fluct. Drift  Tot-Drift
---
*Total Energy-477439 kJ/mol *   839.231790.016
-0.0049046-980.92
T-Protein_DMPC_DMPE 309.657 3.27193.27189 -9.55346e-08
-0.0191069




I used the same *.mdp file
*I used following dmpe.ipt  and dmpc files * attached that to my 1st
impression are identical
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Re: [gmx-users] Which membrane result is more reliable?

2009-10-23 Thread Justin A. Lemkul



Kirill Bessonov wrote:

Hello Justin,

You helped me before, and I am grateful for that. So basically my summer 
research had ended up with the following results:


I have included my *.ipt files this message is long.

*My question: 1)why once simulation is giving  me stable aplha-helix and 
other is not if membranes are similar and conditions kept constant.


* 2) Which result to use, most probale. Does lipid 
density might of affected the stability?




-200ns  Simulation of the same peptide in the DMPC only box and in 
DMPC/DMPE box [1:1 ratio] but results are different and I want to ask 
why as this data will go as part of the paper.


There is nothing that suggests to me you should expect similar results under 
these different conditions.  Many proteins will behave wildly differently in the 
presence of different headgroup charges and chemical functional groups.


As for DMPC, the quaternary amine group is capable of electrostatic 
interactions, while DMPE can participate in hydrogen bonding as well as 
electrostatic interactions, within the lipids and also with the protein.  I can 
think of one example immediately where PE and PC headgroups induce structural 
changes in proteins, I'm sure there are more.




*System:* peptide that is placed on TOP of the membrane, interacting 
with lipids (no inserted into the membrane, but floating on top) and 
above there are water molecules

_*
DMPC membrane simulation - STABLE Peptide Helix, no uncoiling:*_

- 248 DMPC molecules
-Box 9.03 x 9.03 x 10.15 as found at the bottom of gro file (I think 
this dimensions are nm units?)


Yes, per Chapter 2 in the GROMACS manual, the standard unit of length is nm.

- Threfore I calculated that Area per Lipid is only: 2facesx90.3^2 
A^2/248DMPC = 65.75 A^2/lipid which is low




Can you guarantee that no part of your protein occupies this lateral space?  If 
the protein is interacting with the lipids, I would think that this calculation 
is inappropriate.


- When I was using InflatGro(which I modified to be much more friendly 
and accepts 2 lipids) to check the lipid density the values were:


The InflateGRO code (by its own admission) also overestimates area per lipid.  I 
would not use these data at face value.  Might I put in a plug for a program 
developed in our own lab, designed for these exact situations:


http://www.bevanlab.biochem.vt.edu/GridMAT-MD/

snip


I used the same *.mdp file
*I used following dmpe.ipt  and dmpc files * attached that to my 1st 
impression are identical




There are no attachments.  I don't know what you mean by claiming they are 
identical.  PE and PC lipids behave differently.


-Justin








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--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
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] positional restraint

2009-10-23 Thread Justin A. Lemkul



krishnakumar wrote:

Hi,

I was wondering if it would be possible to apply positional restraint to 
an atom w.r.t an arbitrary coordinate.


Say for eg. I want to constrain the distance between an atom and the 
origin(0,0,0) during MD.

Is it possible to  do that in GROMACS.



I don't believe there is a way to implement an absolute restraint, nor do I 
immediately see why it would be meaningful.  You could, however, build your 
system so the atom of interest is placed appropriately and simply use position 
restraints on it.


-Justin


Thanks
Krishna




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--


Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
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: Re: how to calculate the vaporation enthalpy of pure small organic compound (David van der Spoel)

2009-10-23 Thread Jinyao Wang
Hi David,
Thank you for your help. I am very sorry to trouble you.
I have know your means that the gas-phase energy should be considered.
But I am confused that you said the gas-phase energy (with com removed) and 
add kT.
What is the gas-phase energy (with com removed)  and Could you talk about the 
details?

 
 Jinyao Wang wrote:
  Hi gmx-users,
 I want to  calcualted the the vaporation enthalpy of benzaldehyde  I 
 think that the the vaporation enthalpy is the sum of non-bond 
 interacion among the benzaldehyde molecule.So I made a NPT system 
 simulation including 512 benzaldehyde molecule.  The following is the 
 intermolecule nonbond interaction using the g_energy.   

  LJ-(SR)= -21128.7 Kj/mol
  LJ-(LR)= -889.855 Kj/mol
  Coulomb-(SR)= -3884.6 Kj/mol
  Coul.-recip = -2261.51 Kj/mol
   the sum of non-bond interaction = LJ-(SR) + LJ-(LR) + Coulomb-(SR) + 
 Coul.-recip = 28164.665 Kj/mol
But the experimental value of he vaporation enthalpy = 50.3 Kj/mol
 I have no ideal that why they have so much different. Now I don't know 
 how to solve it.
 Any suggestion will be appreciated.
  
 
 These are totals for the intermolecular energy of the system.  I'm 
 guessing you didn't use -nmol 512 to calculate these results?

And then subtract the gas-phase energy (with com removed) and add kT.


Jinyao Wang
wan...@ciac.jl.cn
  2009-10-24
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[gmx-users] Does GMX compute coulomb interaction between oxygen and hydrogen in SPC water model?

2009-10-23 Thread xuji
Hi all gromcas users:

In SPC water model, it only has oxygen-oxygen VDW interactons. 
So is it the same with coulomb interatctions?

Thanks for any advice in advance!

2009-10-24 



Ji Xu
The State Key Laboratory of Multiphase Complex System
Institute of Process Engineering
Chinese Academy of Sciences
Beijing 100190, China
Tel.: +86 10 8262 3713-804 
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Re: [gmx-users] Does GMX compute coulomb interaction between oxygen and hydrogen in SPC water model?

2009-10-23 Thread Mark Abraham
xuji wrote:
 Hi all gromcas users:
  
 In SPC water model, it only has oxygen-oxygen VDW interactons.
 So is it the same with coulomb interatctions?

No, otherwise it would be a one-point water model. All SPC water atoms
have partial charges - see spc.itp.

Mark
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