Re: [gmx-users] NVE of water

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

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

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


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

2010-03-01 Thread Berk Hess

Hi,

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

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

Berk

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

2010-03-01 Thread Andrea
Thank you for your hints. I'll give it a try right now.

Regards,
Andrea

2010/3/1 Berk Hess g...@hotmail.com

 Hi,

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

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

 Berk

  Date: Mon, 1 Mar 2010 09:16:36 +0100
  From: r.fried...@bioc.uzh.ch
  To: gmx-users@gromacs.org
  Subject: Re: [gmx-users] NVE of water

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

2010-03-01 Thread David Chalmers
David,

I get a different simulation result if I use isotropic or anisotropic cells.
I am not sure yet which is (more) correct, but I would like to be able to
run both types to see.  I understand that a constrained anisotropic cell is
not completely anisotropic, but a fully anistropic one clearly doesn't work.

David


 Dear All,
 
 We are running some simulations using an anisotropic periodic cell.  We are
 getting 'cell runaway' with the cell becoming very long and thin.  This
 appears to being driven by the electrostatics of the system.  The simulation
 then dies because the smallest cell dimension is less than 2*cutoff.
 
 Is there a way that we can apply some constraints to the periodic cell?
 Why not use isotropic pressure coupling?
 
 
 Regards
 
 David



David Chalmers  Lab: 9903 9110
Faculty of Pharmacy, Monash University
381 Royal Pde, Parkville, Vic 3053. Australia
david.chalm...@pharm.monash.edu.au



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Re: [gmx-users] Constraining periodic cell

2010-03-01 Thread David van der Spoel

On 2010-03-01 09.49, David Chalmers wrote:

David,

I get a different simulation result if I use isotropic or anisotropic cells.
I am not sure yet which is (more) correct, but I would like to be able to
run both types to see.  I understand that a constrained anisotropic cell is
not completely anisotropic, but a fully anistropic one clearly doesn't work.

David


You did not say which algorithm you use either, but making the time 
constant longer might help. However, depending on your system, you may 
need substantial surface tension to keep the system neutral if you do 
use anisotropic coupling. We do not completely understand these effects 
yet, see e.g http://bugzilla.gromacs.org/show_bug.cgi?id=165 for 
additional discussions.




Dear All,

We are running some simulations using an anisotropic periodic cell.  We are
getting 'cell runaway' with the cell becoming very long and thin.  This
appears to being driven by the electrostatics of the system.  The simulation
then dies because the smallest cell dimension is less than 2*cutoff.

Is there a way that we can apply some constraints to the periodic cell?

Why not use isotropic pressure coupling?



Regards

David




David Chalmers  Lab: 9903 9110
Faculty of Pharmacy, Monash University
381 Royal Pde, Parkville, Vic 3053. Australia
david.chalm...@pharm.monash.edu.au






--
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] Constraining periodic cell

2010-03-01 Thread Berk Hess

Hi,

I would expect nearly any cell to deform to a very elongated shape,
unless it contains a solid (crystal). In most cases an elongated
shape has the lowest (electrostatic) energy. Therefore anisotropic
coupling is only useful for crystal simulations.

Berk

 Date: Mon, 1 Mar 2010 10:09:08 +0100
 From: sp...@xray.bmc.uu.se
 To: gmx-users@gromacs.org
 Subject: Re: [gmx-users] Constraining periodic cell
 
 On 2010-03-01 09.49, David Chalmers wrote:
  David,
 
  I get a different simulation result if I use isotropic or anisotropic cells.
  I am not sure yet which is (more) correct, but I would like to be able to
  run both types to see.  I understand that a constrained anisotropic cell is
  not completely anisotropic, but a fully anistropic one clearly doesn't work.
 
  David
 
 You did not say which algorithm you use either, but making the time 
 constant longer might help. However, depending on your system, you may 
 need substantial surface tension to keep the system neutral if you do 
 use anisotropic coupling. We do not completely understand these effects 
 yet, see e.g http://bugzilla.gromacs.org/show_bug.cgi?id=165 for 
 additional discussions.
 
 
  Dear All,
 
  We are running some simulations using an anisotropic periodic cell.  We 
  are
  getting 'cell runaway' with the cell becoming very long and thin.  This
  appears to being driven by the electrostatics of the system.  The 
  simulation
  then dies because the smallest cell dimension is less than 2*cutoff.
 
  Is there a way that we can apply some constraints to the periodic cell?
  Why not use isotropic pressure coupling?
 
 
  Regards
 
  David
 
  
 
  David Chalmers  Lab: 9903 9110
  Faculty of Pharmacy, Monash University
  381 Royal Pde, Parkville, Vic 3053. Australia
  david.chalm...@pharm.monash.edu.au
  
 
 
 
 
 -- 
 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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[gmx-users] RE: Anisotropic pressure control

2010-03-01 Thread Matteus Lindgren
= 1.2

 

coulombtype  = PME

rcoulomb-switch  = 0

rcoulomb = 1.2

epsilon-r= 1

epsilon_rf   = 1

vdw-type = Cut-off

rvdw-switch  = 0

rvdw = 1.4

DispCorr = EnerPres

table-extension  = 1.5

energygrp_table  = 

fourierspacing   = 0.12

pme_order= 4

ewald_rtol   = 1e-05

ewald_geometry   = 3d

optimize_fft = yes

 

Tcoupl   = Nose-hoover

tc-grps  = protres RUT solcl

tau_t= 0.1 0.1 0.1 

ref_t= 310 310 310 

Pcoupl   = Parrinello-Rahman

Pcoupltype   = anisotropic

tau_p= 2.0 2.0 2.0 2.0 2.0 2.0

compressibility  = 0.0 0.0 5e-5 0.0 0.0 0.0

ref_p= 0 0 1.01325 0 0 0

 

gen_vel  = yes

gen_temp = 310

gen_seed = 1993

 

constraints  = hbonds

constraint-algorithm = lincs

continuation = yes

lincs-order  = 4

lincs-iter   = 4

 

freezegrps   = frozen

freezedim= Y Y Y



 

Thanks

Matteus

- 

Matteus Lindgren, graduate student
Department of Chemistry, Umee University 
SE-901 87 Umee, Sweden
Phone:  +46 (0)90-7865368  

 

 

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[gmx-users] Continuous trajectory from trjconv?

2010-03-01 Thread Pablo Englebienne
Hi, I made an NpT MD simulation of 10 copies of the same small molecule 
in CHCl3 (dodecahedron unit cell) for 20 ns. I want to visualize the 
evolution of the system and the distance between the molecules. I tried 
to visualize the system, but I can't get a continuous trajectory (i.e., 
without jumps) without the solutes diffusing out of the simulation box. 
The same thing happens for the inter-molecule distance, it oscillates 
wildly between a reasonable value (say, 0.5 nm) and 1/2 the size of the 
periodic cell.


When I use trjconv with the -pbc nojump -ur compact options, the 
molecules diffuse out of the box, in a continuous trajectory, until they 
are way further apart than the size of the cell. When visualizing it in 
VMD, however, it turns out that not all molecules are isolated, but 
instead some are interacting with the periodic image of another 
molecule. I used pbc wrap from the PBCTools module within VMD and that 
brings all the molecules into a single cell, but then the trajectory is 
not continuous, with compounds jumping around the edges of the unit 
cell. It is then not straightforward to see the interaction among 
different molecules, as in some cases they are in opposite edges of the 
cell.


If I use the -pbc mol -ur compact option, all molecules stay within a 
single unit cell, but there are jumps across the border of the unit cell 
as in the above case.


I tried also using the -center, -fit rot+trans and -fit 
progressive options (with groups containing either all molecules or a 
single residue) but this ultimately gave the same results.


Would there be something else I could try to visualize the simulation so 
that the central unit cell would contain all residues in a continuous way?


Thanks in advance for reading, and more for replying!

Take care,
Pablo

--
Pablo Englebienne, PhD
Institute of Complex Molecular Systems (ICMS)
Eindhoven University of Technology, TU/e
PO Box 513, HG -1.26
5600 MB Eindhoven, The Netherlands
Tel +31 40 247 5349

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Re: [gmx-users] Continuous trajectory from trjconv?

2010-03-01 Thread Tsjerk Wassenaar
Hi Pablo,

You want to mutually exclusive things. That is by definition impossible.

Sorry,

Tsjerk

On Mon, Mar 1, 2010 at 11:02 AM, Pablo Englebienne p.englebie...@tue.nl wrote:
 Hi, I made an NpT MD simulation of 10 copies of the same small molecule in
 CHCl3 (dodecahedron unit cell) for 20 ns. I want to visualize the evolution
 of the system and the distance between the molecules. I tried to visualize
 the system, but I can't get a continuous trajectory (i.e., without jumps)
 without the solutes diffusing out of the simulation box. The same thing
 happens for the inter-molecule distance, it oscillates wildly between a
 reasonable value (say, 0.5 nm) and 1/2 the size of the periodic cell.

 When I use trjconv with the -pbc nojump -ur compact options, the molecules
 diffuse out of the box, in a continuous trajectory, until they are way
 further apart than the size of the cell. When visualizing it in VMD,
 however, it turns out that not all molecules are isolated, but instead some
 are interacting with the periodic image of another molecule. I used pbc
 wrap from the PBCTools module within VMD and that brings all the molecules
 into a single cell, but then the trajectory is not continuous, with
 compounds jumping around the edges of the unit cell. It is then not
 straightforward to see the interaction among different molecules, as in some
 cases they are in opposite edges of the cell.

 If I use the -pbc mol -ur compact option, all molecules stay within a
 single unit cell, but there are jumps across the border of the unit cell as
 in the above case.

 I tried also using the -center, -fit rot+trans and -fit progressive
 options (with groups containing either all molecules or a single residue)
 but this ultimately gave the same results.

 Would there be something else I could try to visualize the simulation so
 that the central unit cell would contain all residues in a continuous way?

 Thanks in advance for reading, and more for replying!

 Take care,
 Pablo

 --
 Pablo Englebienne, PhD
 Institute of Complex Molecular Systems (ICMS)
 Eindhoven University of Technology, TU/e
 PO Box 513, HG -1.26
 5600 MB Eindhoven, The Netherlands
 Tel +31 40 247 5349

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-- 
Tsjerk A. Wassenaar, Ph.D.

Computational Chemist
Medicinal Chemist
Neuropharmacologist
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Re: [gmx-users] RE: Anisotropic pressure control

2010-03-01 Thread Justin A. Lemkul



Matteus Lindgren wrote:
Thank you for the comment. 
I understand your confusion. Yes, the volume of the box volume should

fluctuate with pressure control but not on the large scale that I get. The
box fluctuates and does not seem to settle on a certain volume. I have tried
with the Berendsen algorithm as well but that run crashed. When I remove the
frozen TiO2 surface the box volume does not at all fluctuate as much. It
therefore seems to be some problem with the frozen atoms and pressure
control. 


Any ideas about this?



Does the simulation still crash under NVT conditions?  I know there has been a 
long-standing incompatibility of pressure coupling with frozen groups, although 
I believe that is the purpose of the new .mdp option refcoord_scaling - how 
are you setting this option?


-Justin


Thanks
Matteus
  


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   2. Re: simulation settings (Mark Abraham)
   3. Question about distance restraints,   energy minimization and
  time averaging. (Arthur Roberts)
   4. Re: Question about distance restraints,   energy minimization
  and time averaging. (Erik Marklund)
   5. NVE of water (Andrea)
   6. RE: Anisotropic pressure control (Dallas B. Warren)


--

Message: 1
Date: Sun, 28 Feb 2010 15:00:11 +0200
From: pol...@fh.huji.ac.il
Subject: [gmx-users] simulation settings
To: gmx-users@gromacs.org
Message-ID: 20100228150011.61721j3pdrw2e...@webmail.huji.ac.il
Content-Type: text/plain;   charset=UTF-8;  DelSp=Yes;
format=flowed

Dear Gromacs users and developers,
I want to perform simulation of peptide dissolved in water using NPT.  
For constant temperature I use Berendsen temperature coupling. Do I  
have to define tc-grps for 2 groups (protein and solvent) or I may use  
tc-grps =System.

What is the difference? The person who introduced gromacs to me uses
tc-grps =  Protein  Sol_Ions
but he is not sure why it should be in this way if at all
Can you, please elucidate this issue to me.
Thank you a lot.
Regina


This message was sent using IMP, the Internet Messaging Program.



--

Message: 2
Date: Mon, 01 Mar 2010 00:50:42 +1100
From: Mark Abraham mark.abra...@anu.edu.au
Subject: Re: [gmx-users] simulation settings
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID: 4b8a74b2.3050...@anu.edu.au
Content-Type: text/plain; charset=UTF-8; format=flowed

On 1/03/2010 12:00 AM, pol...@fh.huji.ac.il wrote:

Dear Gromacs users and developers,
I want to perform simulation of peptide dissolved in water using NPT.
For constant temperature I use Berendsen temperature coupling. Do I have
to define tc-grps for 2 groups (protein and solvent) or I may use
tc-grps =System.
What is the difference? The person who introduced gromacs to me uses
tc-grps = Protein Sol_Ions
but he is not sure why it should be in this way if at all
Can you, please elucidate this issue to me.


There's some quick advice here 
http://www.gromacs.org/Documentation/Terminology/Thermostats, otherwise 
consult some textbook material.


Mark


--

Message: 3
Date: Sun, 28 Feb 2010 10:25:24 -0800
From: Arthur Roberts aroberts99...@yahoo.com
Subject: [gmx-users] Question about distance restraints,energy
minimization and time averaging.
To: gmx users gmx-users@gromacs.org
Message-ID: 9ed0aa2d-c946-40bc-b85b-844962c4d...@yahoo.com
Content-Type: text/plain; charset=US-ASCII; format=flowed

Hi, all,

This is probably a very simple question.  Does time averaging apply,
when distance restraints are used during energy minimization (steepest
descent or conjugate gradient)?  Your input would be greatly
appreciated.

Art Roberts

Dr. Arthur Roberts, Ph.D.
University of California, San Diego
Skaggs School of Pharmacy and Pharmaceutical Sciences
9500 Gilman Drive #0703
La Jolla, CA 92093-0703

email: aroberts99...@yahoo.com
cell: 206-850-7468
skype=aroberts92122





--

Message: 4
Date: Sun, 28 Feb 2010 20:53:38 +0100
From: Erik Marklund er...@xray.bmc.uu.se
Subject: Re: [gmx-users] Question about 

[gmx-users] Re: Continuous trajectory from trjconv?

2010-03-01 Thread Pablo Englebienne

Thanks Tsjerk, I figured as much, but wanted to make sure I wasn't overlooking 
something...

Take care,
Pablo



Hi Pablo,

You want to mutually exclusive things. That is by definition impossible.

Sorry,

Tsjerk

On Mon, Mar 1, 2010 at 11:02 AM, Pablo Englebienne p.englebie...@tue.nl wrote:


Hi, I made an NpT MD simulation of 10 copies of the same small molecule in
CHCl3 (dodecahedron unit cell) for 20 ns. I want to visualize the evolution
of the system and the distance between the molecules. I tried to visualize
the system, but I can't get a continuous trajectory (i.e., without jumps)
without the solutes diffusing out of the simulation box. The same thing
happens for the inter-molecule distance, it oscillates wildly between a
reasonable value (say, 0.5 nm) and 1/2 the size of the periodic cell.

When I use trjconv with the -pbc nojump -ur compact options, the molecules
diffuse out of the box, in a continuous trajectory, until they are way
further apart than the size of the cell. When visualizing it in VMD,
however, it turns out that not all molecules are isolated, but instead some
are interacting with the periodic image of another molecule. I used pbc
wrap from the PBCTools module within VMD and that brings all the molecules
into a single cell, but then the trajectory is not continuous, with
compounds jumping around the edges of the unit cell. It is then not
straightforward to see the interaction among different molecules, as in some
cases they are in opposite edges of the cell.

If I use the -pbc mol -ur compact option, all molecules stay within a
single unit cell, but there are jumps across the border of the unit cell as
in the above case.

I tried also using the -center, -fit rot+trans and -fit progressive
options (with groups containing either all molecules or a single residue)
but this ultimately gave the same results.

Would there be something else I could try to visualize the simulation so
that the central unit cell would contain all residues in a continuous way?
  

Pablo Englebienne, PhD
Institute of Complex Molecular Systems (ICMS)
Eindhoven University of Technology, TU/e
PO Box 513, HG -1.26
5600 MB Eindhoven, The Netherlands
Tel +31 40 247 5349

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Re: [gmx-users] NVE of water

2010-03-01 Thread Justin A. Lemkul



Berk Hess wrote:

Hi,

Shake is not relevant for water and also a time step of 2 fs should be fine.
The cut-off's are the problem. You have a buffer size of 0.1 nm,
which is already smaller than 2 times the distance from the center of 
geometry

of a water molecule to a hydrogen. You need some additional distance
for water diffusion. I would use a buffer of 0.25 to 0.3 nm.
You don't list you coulombtype setting. Use pme (or if you want perfect 
energy
conservation: pme-switch), you can also use reaction-field-zero if you 
really don't

want to use PME.
Then use nstlist=-1, run a short simulation and check in at the end of 
your log file

that the neighbor list lifetime is somewhere between 5 and 20 steps.

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

to check or make one.


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

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

-Justin



Berk

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

2010-03-01 Thread Ran Friedman
Hi,

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

Ran

Justin A. Lemkul wrote:


 Berk Hess wrote:
 Hi,

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

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

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

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

 -Justin


 Berk

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

2010-03-01 Thread Mark Abraham

On 2/03/2010 12:39 AM, Ran Friedman wrote:

Hi,

I would still argue that double precision is important.


Oh? The discussion of Table 4 of 
http://pubs.acs.org/doi/abs/10.1021/ct700301q (2008 GROMACS 4 JCTC 
paper) suggested to me that single-precision NVE could be done well in 
GROMACS. Am I missing something?


Mark


My comment on SHAKE was based on CHARMM - in Gromacs it indeed doesn't
matter for water.

Ran

Justin A. Lemkul wrote:



Berk Hess wrote:

Hi,

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

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


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

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

-Justin



Berk

Date: Mon, 1 Mar 2010 09:16:36 +0100
From: r.fried...@bioc.uzh.ch
To: gmx-users@gromacs.org
Subject: Re: [gmx-users] NVE of water
  
Hi Andrea,
Did you use double precision? Also, I'd try a lower dt (say 1fs) and
shake tolerance (maybe 1E-8).
Good luck,
Ran
  
Andrea wrote:
  Dear users,

  for test purposes in order to set up a bigger system, I try to
run NVE
  simulations of SPC water, but the energy increases very
rapidely. My
  guess is that the cutoffs I use are not good for water. I that the
  case ( I would be grateful for a good reference for suitable SPC
water
  parameters) or do I miss something else?
  My parameter file for the NVE is:

  title = NVE
  cpp = /lib/cpp
  integrator = md
  dt = 0.002 ; ps ! = 2 fs
  nsteps = 5 ; total 100 ps
  nstxout = 5000
  nstvout = 5000
  nstxtcout = 0
  nstlog = 5000
  nstenergy = 5000
  nstlist = 10
  ns_type = grid
  rlist = 1.1

  unconstrained-start = yes
  constraints = all-bonds
  constraint_algorithm = shake
  shake_tol = 0.0001
  ;VdW
  vdwtype = Switch
  rvdw = 1.0 ; rvdw+ (0.1:0.3)= rlist
  rvdw_switch = 0.9
  gen_vel = no ; yes
  gen_temp = 300
  gen_seed = -1
  ;Temperature coupling
  tc_grps = system
  tcoupl = no ;nose-hoover
  tau_t = 0.1
  ref_t = 300
  ;Pressure coupling
  pcoupl = no
  optimize_fft = yes

  Any suggesions are really welcome.

  Thank you.

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

2010-03-01 Thread Berk Hess



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

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

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

Berk

 
 Ran
 
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[gmx-users] Temperature Coupling and Coupling-Groups

2010-03-01 Thread shayamra

Greetings dear Gromacs users,

I would like to create a membrane-protein simulations (popc + protein,  
water, Na Cl ions, using Berendsen thermostat) and I am not sure which  
coupling-groups I should use.

For example, why not couple the whole system together?

I do realize that this is a large request on this type of mailing  
list. I will also be happy to receive references to relevant literature.


Thanks in advance,
-Shay

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Re: [gmx-users] Temperature Coupling and Coupling-Groups

2010-03-01 Thread Justin A. Lemkul



shaya...@post.tau.ac.il wrote:

Greetings dear Gromacs users,

I would like to create a membrane-protein simulations (popc + protein, 
water, Na Cl ions, using Berendsen thermostat) and I am not sure which 
coupling-groups I should use.

For example, why not couple the whole system together?

I do realize that this is a large request on this type of mailing list. 
I will also be happy to receive references to relevant literature.


Most reports in the literature describe protein, lipids, and solvent+ions in 
separate groups.  The reasons for not coupling the whole system together are 
well-documented, and as a matter of fact, I just updated the Gromacs wiki this 
weekend to point to several papers describing this phenomenon:


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

There are also numerous threads in the list archive on this topic, likely with 
other references that I did not link.


-Justin



Thanks in advance,
-Shay



--


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] NVE of water

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


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

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

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

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

Best,
Ran

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Re: [gmx-users] Temperature Coupling and Coupling-Groups

2010-03-01 Thread shayamra

Hi Justin,
Thank you very much for your prompt reply. I will make sure to review  
the aforementioned references.


Regards,
-Shay

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




shaya...@post.tau.ac.il wrote:

Greetings dear Gromacs users,

I would like to create a membrane-protein simulations (popc +  
protein, water, Na Cl ions, using Berendsen thermostat) and I am  
not sure which coupling-groups I should use.

For example, why not couple the whole system together?

I do realize that this is a large request on this type of mailing  
list. I will also be happy to receive references to relevant  
literature.


Most reports in the literature describe protein, lipids, and  
solvent+ions in separate groups.  The reasons for not coupling the  
whole system together are well-documented, and as a matter of fact,  
I just updated the Gromacs wiki this weekend to point to several  
papers describing this phenomenon:


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

There are also numerous threads in the list archive on this topic,  
likely with other references that I did not link.


-Justin



Thanks in advance,
-Shay



--


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] Temperature Coupling and Coupling-Groups

2010-03-01 Thread David van der Spoel

On 3/1/10 5:13 PM, Justin A. Lemkul wrote:



shaya...@post.tau.ac.il wrote:

Greetings dear Gromacs users,

I would like to create a membrane-protein simulations (popc + protein,
water, Na Cl ions, using Berendsen thermostat) and I am not sure which
coupling-groups I should use.
For example, why not couple the whole system together?

I do realize that this is a large request on this type of mailing
list. I will also be happy to receive references to relevant literature.


Most reports in the literature describe protein, lipids, and
solvent+ions in separate groups. The reasons for not coupling the whole
system together are well-documented, and as a matter of fact, I just
updated the Gromacs wiki this weekend to point to several papers
describing this phenomenon:

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


That's interesting, thanks for putting this together Justin.
I haven't read the paper from the Tavan group completely, but I don't 
think they truly solve the problem, do they? It reads more like some 
workaround.


The origin of the problem is the lack of coupling between the different 
degrees of freedom, and as such one would expect united atom force 
fields to show this effect to a larger degree than all-atom force 
fields. It could also be that the use of constraints makes that the 
effective number of degrees of freedom per atom is different for 
proteins and water. It seems that this still hasn't been investigated 
properly...




There are also numerous threads in the list archive on this topic,
likely with other references that I did not link.





-Justin



Thanks in advance,
-Shay






--
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Dept. of Cell and Molecular Biology, Uppsala University.
Husargatan 3, Box 596,  75124 Uppsala, Sweden
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Re: [gmx-users] Temperature Coupling and Coupling-Groups

2010-03-01 Thread Justin A. Lemkul



David van der Spoel wrote:

On 3/1/10 5:13 PM, Justin A. Lemkul wrote:



shaya...@post.tau.ac.il wrote:

Greetings dear Gromacs users,

I would like to create a membrane-protein simulations (popc + protein,
water, Na Cl ions, using Berendsen thermostat) and I am not sure which
coupling-groups I should use.
For example, why not couple the whole system together?

I do realize that this is a large request on this type of mailing
list. I will also be happy to receive references to relevant literature.


Most reports in the literature describe protein, lipids, and
solvent+ions in separate groups. The reasons for not coupling the whole
system together are well-documented, and as a matter of fact, I just
updated the Gromacs wiki this weekend to point to several papers
describing this phenomenon:

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


That's interesting, thanks for putting this together Justin.
I haven't read the paper from the Tavan group completely, but I don't 
think they truly solve the problem, do they? It reads more like some 
workaround.




Right, I just included that paper because I came across it when exploring these 
thermostat issues myself, and I think they have a really nice discussion of some 
of the problems one faces when using thermostats, in general.  The paper also 
points to a lot of other references that delve more deeply into the underlying 
issues.


Hopefully these sorts of links will be useful.

-Justin

The origin of the problem is the lack of coupling between the different 
degrees of freedom, and as such one would expect united atom force 
fields to show this effect to a larger degree than all-atom force 
fields. It could also be that the use of constraints makes that the 
effective number of degrees of freedom per atom is different for 
proteins and water. It seems that this still hasn't been investigated 
properly...




There are also numerous threads in the list archive on this topic,
likely with other references that I did not link.





-Justin



Thanks in advance,
-Shay








--


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] correlation function 'time value' ?

2010-03-01 Thread Ramachandran G
Dear Mark and David,
   Thanks you,  i will check the paper very carefully and try again.

regards,
Rama

On Sat, Feb 27, 2010 at 1:13 AM, Mark Abraham mark.abra...@anu.edu.auwrote:

 On 27/02/2010 7:31 PM, Ramachandran G wrote:

 Dear Dr. van der Spoel:

 Thanks for the clarification in your reply. One more thing I was just
 curious is that, for C(t) =  f(x).f(x+t) ,
 what is the default value for t, which is often called correlation
 time, in gromacs for correlation function calculation, especially in
 g_hbond,
 and/or is it possible to customize the t in gromacs?


 t is not the correlation time. t is an arbitrary amount of time, at which
 the magnitude of C(t) indicates the extent to which f is correlated with
 itself when a set of samples are examined at time interval t. The
 (integrated) correlation time is the integral of (normalized) C(t) over 0 
 t  infinity. See section 8.5 of the manual. I also found the explanations
 in

 Wolff, U. Comput. Phys. Commun. 2004, 156, 143-153.
 Madras, N.; Sokal, A. D. J. Stat. Phys. 1988, 50, 109-186.

 useful.

 Mark

  On Fri, Feb 26, 2010 at 10:03 PM, David van der Spoel
 sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:

On 2010-02-27 03.27, Ramachandran G wrote:

Hi gromacs users:
  As you know autocorrelation function  C(t)

  C(t) = f(0).f(t)

't' value can start from 0 but, i would like to know what value
 does
gromacs use, more specifically for g_hbond.
Can anyone help me? Thank  you.

Rama

The  tell you that all time origins x are used, so
C(t) =  f(x).f(x+t) _x


--
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Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se

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[gmx-users] Re: Choice of value of rlist, rvdw and rcoulomb

2010-03-01 Thread Lum Nforbi
Dear Mark and Amit,

I appreciate your replies. I have read this portion of the gromacs
manual which talks about cut-offs, but I don't clearly understand the
physical significance of the choice of values. I am using for my experiments
vdwtype = cutoff, which is twin-range cut-off  with rlist = neighbour list
cut off and rvdw = vdw cut-off where rvdw = rlist.
 I have run three different experiments (NPT simulation of 200 particles
of oxygen at 80K ie liquid oxygen) but with different rlist and rvdw values
to evaluate the influence of these values on my Lennard-Jones plots. The
literature Lennard-Jones parameters for oxygen which I have been using are
epsilon = 0.939482 KJ/mol and sigma = 0.3433 nm. The book Computer
Simulation of Liquids by Allen and Tildesley recommends the use of rvdw =
2.5xsigma. In my case, if I use this recommendation, my rvdw value would be
0.86.

The values I have used and the results are as follows:

RLIST = 0.3, RVDW = 0.7
RESULT: RDF Plot converges to 1 (WORKS).

RLIST = 0.3, RVDW = 1.0
RESULT: RDF Plot converges to 0 after third peak (DOES NOT WORK).

RLIST = 0.7, RVDW = 0.7
RESULT: RDF Plot converges to 0 after third peak (DOES NOT WORK).

I know that the problem is not about equilibration, because the first
experiment which worked did not even equilibrate fully but gave the right
plot.
My question is: what is the physical significance of choosing these
values? I know that rlist is used as cut-off for neighbour list generation
and to specify which atom pairs are interacting, so that these interactions
can be calculated at every step of the simulation. rvdw specifies the radius
of atoms which will interact in a vdw manner. Why would a rvdw = 0.7 work
and rvdw = 1.0 not work looking at a system in a physical sense? 0.7 and 1.0
are both close to the recommended 0.86 value for rvdw, so why does one work
and not other? What could be happening in the system? If I don't understand
physically what these values really mean, I may never fully grasp what is
going on in the system. Please help me out.

The .mdp file I have used below is the same in all three cases, the only
modifications being the rlist and rvdw values.

integrator   = md ; a leap-frog algorithm for
integrating Newton's equations of motion
dt   = 0.002  ; time-step in ps
nsteps   = 50 ; total number of steps; total time (1
ns)

nstcomm  = 1  ; frequency for com removal
nstxout  = 1000   ; freq. x_out
nstvout  = 1000   ; freq. v_out
nstfout  = 0  ; freq. f_out
nstlog   = 100 ; energies to log file
nstenergy= 100 ; energies to energy file

nstlist  = 10 ; frequency to update neighbour list
ns_type  = grid   ; neighbour searching type
rlist= 0.3; cut-off distance for the short range
neighbour list
pbc  = xyz; Periodic boundary conditions:xyz,
use periodic boundary conditions in all directions
periodic_molecules   = no ; molecules are finite, fast molecular
pbc can be used

vdw-type = Cut-off; van der Waals interactions
rvdw = 0.7; distance for the LJ or Buckingham
cut-off

fourierspacing   = 0.135   ; max. grid spacing for the FFT grid
for PME
fourier_nx   = 0  ; highest magnitude in reciprocal
space when using Ewald
fourier_ny   = 0  ; highest magnitude in reciprocal
space when using Ewald
fourier_nz   = 0  ; highest magnitude in reciprocal
space when using Ewald
pme_order= 4  ; cubic interpolation order for PME
ewald_rtol   = 1e-5   ; relative strength of the
Ewald-shifted direct potential
optimize_fft = yes; calculate optimal FFT plan for the
grid at start up.
DispCorr = no ;

Tcoupl   = v-rescale  ; temp. coupling with vel. rescaling
with a stochastic term.
tau_t= 0.1; time constant for coupling
tc-grps  = OXY; groups to couple separately to temp.
bath
ref_t= 80 ; ref. temp. for coupling

Pcoupl   = berendsen  ; exponential relaxation pressure
coupling (box is scaled every timestep)
Pcoupltype   = isotropic  ; box expands or contracts evenly in
all directions (xyz) to maintain proper pressure
tau_p= 0.5; time constant for coupling (ps)
compressibility  = 4.5e-5 ; compressibility of solvent used in
simulation
ref_p= 1.0; ref. pressure for coupling (bar)

gen_vel  = yes; generate velocities according to a
Maxwell distr. at gen_temp
gen_temp = 80 ; temperature for 

[gmx-users] How to add a new non-bonded interaction into Gromacs

2010-03-01 Thread Tandia, Adama
Dear ALL:

I would like to add a new 2-body non-bonded interaction into Gromacs.
Has anybody done this yet? 
Help is dearly appreciated.

Regards,
Adama

Adama Tandia, Corning INC, SP-TD-01-01 Corning NY 14831 USA, Tel: 607
248 1036 -GoogleVoice: 708 433 9430

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Re: [gmx-users] Re: Choice of value of rlist, rvdw and rcoulomb

2010-03-01 Thread Justin A. Lemkul



Lum Nforbi wrote:

Dear Mark and Amit,

I appreciate your replies. I have read this portion of the gromacs 
manual which talks about cut-offs, but I don't clearly understand the 
physical significance of the choice of values. I am using for my 
experiments vdwtype = cutoff, which is twin-range cut-off  with rlist = 
neighbour list cut off and rvdw = vdw cut-off where rvdw = rlist. 
 I have run three different experiments (NPT simulation of 200 
particles of oxygen at 80K ie liquid oxygen) but with different rlist 
and rvdw values to evaluate the influence of these values on my 
Lennard-Jones plots. The literature Lennard-Jones parameters for oxygen 
which I have been using are epsilon = 0.939482 KJ/mol and sigma = 0.3433 
nm. The book Computer Simulation of Liquids by Allen and Tildesley 
recommends the use of rvdw = 2.5xsigma. In my case, if I use this 
recommendation, my rvdw value would be 0.86.


The values I have used and the results are as follows:

RLIST = 0.3, RVDW = 0.7
RESULT: RDF Plot converges to 1 (WORKS).

RLIST = 0.3, RVDW = 1.0
RESULT: RDF Plot converges to 0 after third peak (DOES NOT WORK).

RLIST = 0.7, RVDW = 0.7
RESULT: RDF Plot converges to 0 after third peak (DOES NOT WORK).

I know that the problem is not about equilibration, because the first 
experiment which worked did not even equilibrate fully but gave the 
right plot.


Just because you got the desired result does not mean what you did was right. 
Haphazard combinations of parameters lead to unpredictable and unreliable 
results.  I think your rlist is absurdly short - what motivated this choice? 
Why have you yet to use the value calculated based on the Allen and Tildesley 
rule of thumb (0.9 nm)?


My question is: what is the physical significance of choosing these 
values? I know that rlist is used as cut-off for neighbour list 
generation and to specify which atom pairs are interacting, so that 
these interactions can be calculated at every step of the simulation. 
rvdw specifies the radius of atoms which will interact in a vdw manner. 


To quote from the manual (section 4.6.3): In the neighbor list all
interaction pairs that fall within rlist are stored. Furthermore, the 
interactions between pairs that do not fall within rlist but do fall within 
max(rcoulomb,rvdw) are computed during NS, and the forces and energy are stored 
separately, and added to short-range forces at every time step between 
successive NS.


The neighbor list is updated every step for particles within rlist.  The 
neighbor list between rlist and rvdw is updated every nstlist steps; between 
these neighbor-searching steps, the neighbor list is considered to be constant. 
 Beyond rvdw, the van der Waals interaction is assumed to be zero (hence cut 
off).  I see that you're setting DispCorr = no, so you may be getting cutoff 
artifacts.  All long-range interactions should be attractive, so the problem 
with plain cutoffs is system expansion which is not compensated for when 
dispersion correction is off.


Why would a rvdw = 0.7 work and rvdw = 1.0 not work looking at a system 
in a physical sense? 0.7 and 1.0 are both close to the recommended 0.86 


Close enough does not mean good enough.  For a system of only LJ particles, your 
choice of rvdw will likely have a huge impact on your results.  You may just be 
getting some random success based on some fortuitous combination.


value for rvdw, so why does one work and not other? What could be 
happening in the system? If I don't understand physically what these 
values really mean, I may never fully grasp what is going on in the 
system. Please help me out.


I would suggest to you that you read some basic literature on force field 
derivation.  While not necessarily directly related to what you're doing, you 
could benefit from understanding how reliable parameter sets are determined.  If 
you don't comprehend what you're doing yet, you shouldn't be diving in head first.


-Justin



The .mdp file I have used below is the same in all three cases, the only 
modifications being the rlist and rvdw values.



--


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] g_cluster

2010-03-01 Thread ROHIT MALSHE
Hi All, Greetings !I have a question about g_cluster. I have a configuration of 
Lennard Jones particles. For each particle I calculate an individual bond 
orientational order parameter Q4. Based on this order parameter I want to 
calculate the clusters in the system. Meaning - particles connected to each 
other sharing similar values of Q4. How would I have to go about this problem 
?Thanks in advane. - Rohit
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SV: [gmx-users] Order parameter for unsaturated lipid chain in UAmodel

2010-03-01 Thread Tim Sirk
Sarah,

I remember some changes to the double bond awhile back, perhaps you're
using those?

POPC (Berger/Tielman) is normally 'smoother' as Justin says. Maybe
someone has a reference for the updates.


Tim Sirk


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Re: [gmx-users] How to add a new non-bonded interaction into Gromacs

2010-03-01 Thread Mark Abraham

On 2/03/2010 4:22 AM, Tandia, Adama wrote:

Dear ALL:

I would like to add a new 2-body non-bonded interaction into Gromacs.
Has anybody done this yet?
Help is dearly appreciated.


This is what user-tables are for. Check out the manual for detailed 
information.


Mark
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Re: [gmx-users] g_cluster

2010-03-01 Thread David van der Spoel

On 2010-03-02 00.13, ROHIT MALSHE wrote:

Hi All,

Greetings !

I have a question about g_cluster.

I have a configuration of Lennard Jones particles. For each particle I
calculate an individual bond orientational order parameter Q4. Based on
this order parameter I want to calculate the clusters in the system.
Meaning - particles connected to each other sharing similar values of
Q4. How would I have to go about this problem ?

Thanks in advane.

- Rohit

You need to implement a criterion like this in the program, instead of 
the RMSD matrix.


--
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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