Re: [gmx-users] pbc and tpr file

2007-12-12 Thread Tsjerk Wassenaar
Hi Tang,

It doesn't hurt to check (i.e. you should check ;)) whether the .tpr file
contains the protein in one piece, if you want to use it as a reference
structure for rmsd calculations. You can extract the coordinates from the
.tpr file using editconf and then have a look. Actually, you should've done
this prior to removing jumps from the trajectory, since you must be sure to
remove the jumps in the right way (check the archives for more discussion on
these issues).

Cheers,

Tsjerk

On Dec 12, 2007 1:42 AM, Mark Abraham [EMAIL PROTECTED] wrote:

 tangxuan wrote:
  hi all,
   I want to calculate the rmsd of my protein. If I remove the jump in the
  xtc file or trr file, what should I do with tpr file?

 Nothing. Depending on your inputs to g_rms, it might provide your
 reference structure.

 Mark
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Junior UD (post-doc)
Biomolecular NMR, Bijvoet Center
Utrecht University
Padualaan 8
3584 CH Utrecht
The Netherlands
P: +31-30-2539931
F: +31-30-2537623
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Re: [gmx-users] Gel Phase in DMPC using Berger force field ??

2007-12-12 Thread Jochen Hub

Hi Eric,

thanks a lot for clarifying this. I suspect that getting a resonable 
transition temperature between liquid and gel phase might be rather 
challenging...but yes, as you said, would be interesting...


Cheers,
Jochen


Eric Jakobsson wrote:

Several points:

What is called the Berger force field was actually developed by 
See-Wing Chiu in our lab and presented in a 1995 paper.  The Berger et 
al paper tested this force field against another candidate and found 
that it was better, and that is the paper that has been cited ever since.


See-Wing did tests of the necessary VDW cut-off for accuracy against 
what seemed like the most sensitive test, the value of the dipole 
potential at the water-lipid interface, and concluded that one should 
use a cut-off of at least 18 angstroms.


The van der Waals parameters for the hydrocarbon tails were 
reparameterized in a paper we published a few years ago, and in that 
paper we verified that the 18 angstrom cutoff was required for an 
accurate liquid hydrocarbon simulation also.


Recently See-Wing has reparameterized the van der Waals parameters in 
the lipid head groups, using specific volumes of liquids comprised of 
small molecules that are part of the head group.  The resulting force 
fields, which retain the partial charges of the Berger-Chiu field, 
work very well in replicating x-ray structure factors of lipids with 
various chain compositions, but he has not yet tried to do gel 
phase--that would be interesting.  The journal ms. is still sitting on 
my desk, I am afraid, but there is a pretty good description of the 
parameterization in a chapter in a book that Scott Feller is editing, 
which we can send on request, as well as the lipid complete force 
field in itself.  We believe it is state of the art at this time.


Best,
Eric
At 10:22 AM 12/11/2007, you wrote:

Hi Steffen,

thanks a lot for your reply.
-what are your VdW cutoffs? Berger lipids absolutely need the 
0.8/1.4 nm

twin range cutoff for working properly. Are you using PME for
electrostatics?

I used a LJ-cutoff at 1.0nm. That's what was used for the original 
Berger-Paper (*O Berger, O Edholm and F Jähnig, */Biophysical 
Journal/ 72: 2002-2013 (1997). Shouldn't this be all right?


And I used PME (which was indeed not used in the original work.


-how did you set up the pressure coupling?


I used weak coupling (tau=1.0ps)


-900 waters are not really much, the head groups will probably interact
with their mirror images due to pbc. Try a lot more (thought about
1?) for having a real bilayer in a solution.


I also tried with more water, the gel phase did not appear either.


From my experience, the Berger lipids are well defined for a specific
temperature, but if you go up/down the temperature scale, they are not
really following the experimental values/phase behaviour. By the way:
experimental data on lipid order parameters varies considerably
throughout the complete literature, so don't rely onto that too much as
well.
Sorry for giving more questions than answers, but that's the shitty 
part

with lipid bilayers in MD...
Steffen


Thanks again,
Jochen



--

Jochen Hub
Max Planck Institute for Biophysical Chemistry
Computational biomolecular dynamics group
Am Fassberg 11
D-37077 Goettingen, Germany
Email: jhub[at]gwdg.de

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-
Eric Jakobsson, Ph.D.
Professor, Department of Molecular and Integrative Physiology, and of 
Biochemistry, and of the Center for Biophysics and Computational Biology
Senior Research Scientist, National Center for Supercomputing 
Applications

Professor, Beckman Institute for Advanced Science and Technology
3261 Beckman Institute, mc251
University of Illinois, Urbana, IL 61801
ph. 217-244-2896  Fax 217 244 9757




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--

Jochen Hub
Max Planck Institute for Biophysical Chemistry
Computational biomolecular dynamics group
Am Fassberg 11
D-37077 Goettingen, Germany
Email: jhub[at]gwdg.de
 


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Re: [gmx-users] rvdw vs cut-off / different types of non bonded interactions

2007-12-12 Thread David van der Spoel



On Wed, 12 Dec 2007, Claus Valka wrote:


Dear Sir,

I would try to be more precise.

example1 mdp file:
rlist = (greater or equal to rvdw)
vdw-type = Switch
rvdw-switch=5.56
rvdw=8.9


are you aware that gromacs usues nm for distance?

you can find the functional form of the shift/switch function in the 
manual.



Between the value 5.56 and 8.9 gromacs uses cubic
spline?

example2 mdp file:

rlist=5.56
vdw-type = Cut-off
rvdw-switch=0 (this value here should be irrelevant)
rvdw=8.9

Gromacs uses cubic spline after the value 8.9 till LJ
to go to zero?

And which is the difference of rlist if someone uses
vdw-type = Cut-off instead of vdw-type = Switch? It
would have been nice to have images of these options
so as to be better understood.
Because it is stated in the manual:
rlist: (1) [nm]
cut-off distance for the short-range neighbor list
and also:
Switch
...The neighbor search cut-off rlist should be 0.1 to
0.3 nm LARGER than rvdw...
Isn't this a little bit contradictive?

As far as twin cutoffs are concerned if we want to
find out the total energy of the non bonded
interactions we have to add LJ-14 + LJ(SR) + LJ(LR)?

With tabulated potentials can I use different cutoffs
for different types of atoms? Judging from your answer
about system wide cutoffs I understand that even
though I might use tabulated potentials, I won't be
able to use different cutoffs for the different types
of atoms I have. Am I correct?

Yours Sincerely,
Nikos


--- Mark Abraham [EMAIL PROTECTED] schrieb:


Claus Valka wrote:

Hello,




3rd question: Which is the difference between the
S(hort)R(ange) LJ and LJ 1-4? For me the short

range

interactions are the 1-4LJ, yet it seems that this

is

not the case.


GROMACS uses twin-range cutoffs (see manual), so
LJ-SR is inside the
shorter cutoff, and LJ-LR is outside.


4th question: I want after 1,45*#963; till
2,33*#963; to use the cubic spline in such a way

that

the LJ potential will go smoothly to zero at
2,33#963;. If I use the biggest #963; I have,

then

in the mdp file rvdw-switch=5.56 and rvdw=8.9.

Between

these two values does the cubic spline work as a
switch function using vdw-type = Switch ?


Please find a way to describe your problem with
plain ASCII text.


5th question: Given the above if I use vdw-type
=Cut-off and rvdw=8.9 then gromacs will use cubic
spline till the LJ will reach zero for a value

greater

than 8.9, yet to me uknown? If this is not the

case

how LJ goes to zero with this option?


I don't understand what you're asking.


6th question: If I want to use a quintic spline
between 1,45*#963; till 2,33*#963;(cut-off

value)

for the different combination of atoms(they have
different #949; and #963;), then should I use a
tabulated potential? And if I do that which will

be

the meaning of cutoffs in the mdp file as I would

like

them to be different for each of the different

types

of atoms I have? Can I use different cut-offs for

the

different types of atoms I have?


The cut-offs are a system-wide property.

Mark
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[gmx-users] asking for recommendations

2007-12-12 Thread michelle yap

Hi!

I am a student currently using GROMACS (which I am new at)  for a study on 
iota-carrageenan. The starting structures used are already in a double helix 
configuration. One file contains two ten-monomer iota-carrageenan chains coiled 
into a double helix; the other two files (differing only in the arrangement of 
the helices) consist of three double helices, each helix consists of two 
six-monomer chains. These were simulated at two conditions - high temp and room 
temp - for 20 ns each. The double helix should theoretically uncoil. However, 
no such uncoiling was observed. I was tasked to perform analysis tools to 
possibly provide other reasons for the observed results apart from modeling 
limitations (i.e. relatively short length and simulation time). As of the 
moment, I am doing g_hbond for h-bond analysis. Could you please recommend 
other analysis tools that are likely to be useful in my research?

Thank you!
_
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Re: [gmx-users] Gel Phase in DMPC using Berger force field ??

2007-12-12 Thread Eric Jakobsson
Yes, this should be attempted.  Perhaps the 
ultimate test of a force field is to nail a phase change.


At 03:34 AM 12/12/2007, you wrote:

Hi Eric,

thanks a lot for clarifying this. I suspect that 
getting a resonable transition temperature 
between liquid and gel phase might be rather 
challenging...but yes, as you said, would be interesting...


Cheers,
Jochen


Eric Jakobsson wrote:

Several points:

What is called the Berger force field was 
actually developed by See-Wing Chiu in our lab 
and presented in a 1995 paper.  The Berger et 
al paper tested this force field against 
another candidate and found that it was better, 
and that is the paper that has been cited ever since.


See-Wing did tests of the necessary VDW cut-off 
for accuracy against what seemed like the most 
sensitive test, the value of the dipole 
potential at the water-lipid interface, and 
concluded that one should use a cut-off of at least 18 angstroms.


The van der Waals parameters for the 
hydrocarbon tails were reparameterized in a 
paper we published a few years ago, and in that 
paper we verified that the 18 angstrom cutoff 
was required for an accurate liquid hydrocarbon simulation also.


Recently See-Wing has reparameterized the van 
der Waals parameters in the lipid head groups, 
using specific volumes of liquids comprised of 
small molecules that are part of the head 
group.  The resulting force fields, which 
retain the partial charges of the Berger-Chiu 
field, work very well in replicating x-ray 
structure factors of lipids with various chain 
compositions, but he has not yet tried to do 
gel phase--that would be interesting.  The 
journal ms. is still sitting on my desk, I am 
afraid, but there is a pretty good description 
of the parameterization in a chapter in a book 
that Scott Feller is editing, which we can send 
on request, as well as the lipid complete force 
field in itself.  We believe it is state of the art at this time.


Best,
Eric
At 10:22 AM 12/11/2007, you wrote:

Hi Steffen,

thanks a lot for your reply.

-what are your VdW cutoffs? Berger lipids absolutely need the 0.8/1.4 nm
twin range cutoff for working properly. Are you using PME for
electrostatics?
I used a LJ-cutoff at 1.0nm. That's what was 
used for the original Berger-Paper (*O Berger, 
O Edholm and F Jähnig, */Biophysical Journal/ 
72: 2002-2013 (1997). Shouldn't this be all right?


And I used PME (which was indeed not used in the original work.


-how did you set up the pressure coupling?

I used weak coupling (tau=1.0ps)


-900 waters are not really much, the head groups will probably interact
with their mirror images due to pbc. Try a lot more (thought about
1?) for having a real bilayer in a solution.

I also tried with more water, the gel phase did not appear either.


From my experience, the Berger lipids are well defined for a specific
temperature, but if you go up/down the temperature scale, they are not
really following the experimental values/phase behaviour. By the way:
experimental data on lipid order parameters varies considerably
throughout the complete literature, so don't rely onto that too much as
well.
Sorry for giving more questions than answers, but that's the shitty part
with lipid bilayers in MD...
Steffen

Thanks again,
Jochen



--

Jochen Hub
Max Planck Institute for Biophysical Chemistry
Computational biomolecular dynamics group
Am Fassberg 11
D-37077 Goettingen, Germany
Email: jhub[at]gwdg.de

___
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-
Eric Jakobsson, Ph.D.
Professor, Department of Molecular and 
Integrative Physiology, and of Biochemistry, 
and of the Center for Biophysics and Computational Biology

Senior Research Scientist, National Center for Supercomputing Applications
Professor, Beckman Institute for Advanced Science and Technology
3261 Beckman Institute, mc251
University of Illinois, Urbana, IL 61801
ph. 217-244-2896  Fax 217 244 9757




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--

Jochen Hub
Max Planck Institute for Biophysical Chemistry
Computational biomolecular dynamics group
Am Fassberg 11
D-37077 Goettingen, Germany

Re: [gmx-users] asking for recommendations

2007-12-12 Thread Tsjerk Wassenaar
Hi Michelle,

What reasons do you have suggesting factors other than modelling
limitations? Is there experimental data regarding the time scale of
uncoiling? I would guess it would take longer than 20 ns. Also, you should
consider that you're looking at a single molecule. The observation of
uncoiling in vitro or in silico involves many molecules, of which one may
stay coiled for a long time (maybe the one you're looking at in your
simulation).

You might try to express the properties of your helix in terms of number of
hydrogen bonds, helix length, helix radius and helix bending, in which you
could observe trends towards more loose states, suggesting the onset of
uncoiling. But it would also be better to try and extend the simulations.

Cheers,

Tsjerk

On Dec 12, 2007 9:57 AM, michelle yap [EMAIL PROTECTED] wrote:


 Hi!

 I am a student currently using GROMACS (which I am new at)  for a study on
 iota-carrageenan. The starting structures used are already in a double helix
 configuration. One file contains two ten-monomer iota-carrageenan chains
 coiled into a double helix; the other two files (differing only in the
 arrangement of the helices) consist of three double helices, each helix
 consists of two six-monomer chains. These were simulated at two conditions -
 high temp and room temp - for 20 ns each. The double helix should
 theoretically uncoil. However, no such uncoiling was observed. I was tasked
 to perform analysis tools to possibly provide other reasons for the
 observed results apart from modeling limitations (i.e. relatively short
 length and simulation time). As of the moment, I am doing g_hbond for h-bond
 analysis. Could you please recommend other analysis tools that are likely to
 be useful in my research?

 Thank you!
 _
 Get your free suite of Windows Live services today!

 http://www.get.live.com/wl/all___
 gmx-users mailing listgmx-users@gromacs.org
 http://www.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at http://www.gromacs.org/search before posting!
 Please don't post (un)subscribe requests to the list. Use the
 www interface or send it to [EMAIL PROTECTED]
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-- 
Tsjerk A. Wassenaar, Ph.D.
Junior UD (post-doc)
Biomolecular NMR, Bijvoet Center
Utrecht University
Padualaan 8
3584 CH Utrecht
The Netherlands
P: +31-30-2539931
F: +31-30-2537623
___
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Re: [gmx-users] rvdw vs cut-off / different types of non bonded interactions

2007-12-12 Thread Claus Valka
Dear Sir,

I'm absolutely aware that gromacs uses nm for
distance. The values should be 0.556 and 0.89. I used
them only for reference purposes and I hope that this
didn't cause any misanderstanding so as to point me to
the manual. If this is the case of not understanding
my questions, I deeply appologize.

Yours Sincerely,
Nikos
--- David van der Spoel [EMAIL PROTECTED]
schrieb:

 
 
 On Wed, 12 Dec 2007, Claus Valka wrote:
 
  Dear Sir,
 
  I would try to be more precise.
 
  example1 mdp file:
  rlist = (greater or equal to rvdw)
  vdw-type = Switch
  rvdw-switch=5.56
  rvdw=8.9
 
 are you aware that gromacs usues nm for distance?
 
 you can find the functional form of the shift/switch
 function in the 
 manual.
 
  Between the value 5.56 and 8.9 gromacs uses cubic
  spline?
 
  example2 mdp file:
 
  rlist=5.56
  vdw-type = Cut-off
  rvdw-switch=0 (this value here should be
 irrelevant)
  rvdw=8.9
 
  Gromacs uses cubic spline after the value 8.9 till
 LJ
  to go to zero?
 
  And which is the difference of rlist if someone
 uses
  vdw-type = Cut-off instead of vdw-type = Switch?
 It
  would have been nice to have images of these
 options
  so as to be better understood.
  Because it is stated in the manual:
  rlist: (1) [nm]
  cut-off distance for the short-range neighbor list
  and also:
  Switch
  ...The neighbor search cut-off rlist should be 0.1
 to
  0.3 nm LARGER than rvdw...
  Isn't this a little bit contradictive?
 
  As far as twin cutoffs are concerned if we want to
  find out the total energy of the non bonded
  interactions we have to add LJ-14 + LJ(SR) +
 LJ(LR)?
 
  With tabulated potentials can I use different
 cutoffs
  for different types of atoms? Judging from your
 answer
  about system wide cutoffs I understand that even
  though I might use tabulated potentials, I won't
 be
  able to use different cutoffs for the different
 types
  of atoms I have. Am I correct?
 
  Yours Sincerely,
  Nikos
 
 
  --- Mark Abraham [EMAIL PROTECTED]
 schrieb:
 
  Claus Valka wrote:
  Hello,
 
 
  3rd question: Which is the difference between
 the
  S(hort)R(ange) LJ and LJ 1-4? For me the short
  range
  interactions are the 1-4LJ, yet it seems that
 this
  is
  not the case.
 
  GROMACS uses twin-range cutoffs (see manual), so
  LJ-SR is inside the
  shorter cutoff, and LJ-LR is outside.
 
  4th question: I want after 1,45*#963; till
  2,33*#963; to use the cubic spline in such a
 way
  that
  the LJ potential will go smoothly to zero at
  2,33#963;. If I use the biggest #963; I have,
  then
  in the mdp file rvdw-switch=5.56 and rvdw=8.9.
  Between
  these two values does the cubic spline work as a
  switch function using vdw-type = Switch ?
 
  Please find a way to describe your problem with
  plain ASCII text.
 
  5th question: Given the above if I use vdw-type
  =Cut-off and rvdw=8.9 then gromacs will use
 cubic
  spline till the LJ will reach zero for a value
  greater
  than 8.9, yet to me uknown? If this is not the
  case
  how LJ goes to zero with this option?
 
  I don't understand what you're asking.
 
  6th question: If I want to use a quintic spline
  between 1,45*#963; till 2,33*#963;(cut-off
  value)
  for the different combination of atoms(they have
  different #949; and #963;), then should I use
 a
  tabulated potential? And if I do that which will
  be
  the meaning of cutoffs in the mdp file as I
 would
  like
  them to be different for each of the different
  types
  of atoms I have? Can I use different cut-offs
 for
  the
  different types of atoms I have?
 
  The cut-offs are a system-wide property.
 
  Mark
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  http://www.gromacs.org/search before posting!
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  http://www.gromacs.org/mailing_lists/users.php
 
 
 
 
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 überfliegen. Dies und viel mehr bietet das neue
 Yahoo! Mail - www.yahoo.de/mail
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 http://www.gromacs.org/search before posting!
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Re: [gmx-users] Gel Phase in DMPC using Berger force field ??

2007-12-12 Thread Zoltan Varga
Dear all,

For the gel-to-liquid crystalline phase transition in DPPC and DPPE there is a 
paper:
Leekumjorn and Sum, BBA, 1768 (2007) 354-365
I've found it several month ago and I haven't red through it completely, but 
they used the Berger force field.

Best,
Zoltan

Eric Jakobsson [EMAIL PROTECTED] wrote: Yes, this should be attempted.  
Perhaps the 
ultimate test of a force field is to nail a phase change.

At 03:34 AM 12/12/2007, you wrote:
Hi Eric,

thanks a lot for clarifying this. I suspect that 
getting a resonable transition temperature 
between liquid and gel phase might be rather 
challenging...but yes, as you said, would be interesting...

Cheers,
Jochen


Eric Jakobsson wrote:
Several points:

What is called the Berger force field was 
actually developed by See-Wing Chiu in our lab 
and presented in a 1995 paper.  The Berger et 
al paper tested this force field against 
another candidate and found that it was better, 
and that is the paper that has been cited ever since.

See-Wing did tests of the necessary VDW cut-off 
for accuracy against what seemed like the most 
sensitive test, the value of the dipole 
potential at the water-lipid interface, and 
concluded that one should use a cut-off of at least 18 angstroms.

The van der Waals parameters for the 
hydrocarbon tails were reparameterized in a 
paper we published a few years ago, and in that 
paper we verified that the 18 angstrom cutoff 
was required for an accurate liquid hydrocarbon simulation also.

Recently See-Wing has reparameterized the van 
der Waals parameters in the lipid head groups, 
using specific volumes of liquids comprised of 
small molecules that are part of the head 
group.  The resulting force fields, which 
retain the partial charges of the Berger-Chiu 
field, work very well in replicating x-ray 
structure factors of lipids with various chain 
compositions, but he has not yet tried to do 
gel phase--that would be interesting.  The 
journal ms. is still sitting on my desk, I am 
afraid, but there is a pretty good description 
of the parameterization in a chapter in a book 
that Scott Feller is editing, which we can send 
on request, as well as the lipid complete force 
field in itself.  We believe it is state of the art at this time.

Best,
Eric
At 10:22 AM 12/11/2007, you wrote:
Hi Steffen,

thanks a lot for your reply.
-what are your VdW cutoffs? Berger lipids absolutely need the 0.8/1.4 nm
twin range cutoff for working properly. Are you using PME for
electrostatics?
I used a LJ-cutoff at 1.0nm. That's what was 
used for the original Berger-Paper (*O Berger, 
O Edholm and F Jähnig, */Biophysical Journal/ 
72: 2002-2013 (1997). Shouldn't this be all right?

And I used PME (which was indeed not used in the original work.

-how did you set up the pressure coupling?
I used weak coupling (tau=1.0ps)

-900 waters are not really much, the head groups will probably interact
with their mirror images due to pbc. Try a lot more (thought about
1?) for having a real bilayer in a solution.
I also tried with more water, the gel phase did not appear either.

 From my experience, the Berger lipids are well defined for a specific
temperature, but if you go up/down the temperature scale, they are not
really following the experimental values/phase behaviour. By the way:
experimental data on lipid order parameters varies considerably
throughout the complete literature, so don't rely onto that too much as
well.
Sorry for giving more questions than answers, but that's the shitty part
with lipid bilayers in MD...
Steffen
Thanks again,
Jochen



--

Jochen Hub
Max Planck Institute for Biophysical Chemistry
Computational biomolecular dynamics group
Am Fassberg 11
D-37077 Goettingen, Germany
Email: jhub[at]gwdg.de

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Integrative Physiology, and of Biochemistry, 
and of the Center for Biophysics and Computational Biology
Senior Research Scientist, National Center for Supercomputing Applications
Professor, Beckman Institute for Advanced Science and Technology
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[gmx-users] problem using makehole program

2007-12-12 Thread nur avneet
Dear All
i started makehole program...but am facing problems setting
the  mdp parameters.

when i gave mdrun command i get an error..that i cant make out:
the command i gave is:- 
/usr/local/gromacs/i686-pc-linux-gnu/bin/mdrun -v -hole -holep hpgr.mdp -s 
dmpc_water_1ns.tpr -o cecmel311334_dmpc_hole_1ns.trr -c 
cecmel311334_dmpc_hole_1ns.gro -e cecmel311334_dmpc_hole_1ns.edr -g 
cecmel311334_dmpc_hole_1ns.log

 WARNING 1 [file , line 1]:
   Unknown left-hand molsurf_log in parameter file
 
 Reading ASCII grasp surface
 atomic surface: allocating list of nn vertex of each
 of 16853 atoms 
 atomic surface: reading surface data from file
 grasp_sur_ascii
 atomic surface: reading 6712 vertices and normals
 and
 13420 triangles...done
 
 Back Off! I just backed up gsurf.log to
 ./#gsurf.log.1#
 starting mdrun 'dmpc $ 3655 water in constant
area
 0.596'
 50 steps,   1000.0 ps.
 
 
 Back Off! I just backed up
 cecmel311334_dmpc_hole_1ns.trr to
 ./#cecmel311334_dmpc_hole_1ns.trr.2#
 
 Back Off! I just backed up insidesurf.pdb to
 ./#insidesurf.pdb.2#
 Fatal error: Don't worry, this is in fact a normal
 stop in debugsurf mode: 
 now check insidegr.pdb and molsurfpdb.pdb
 
And when i try to open molsurfpdb.pdb...vmd shows
error, that no of bonds is too much. so the file
doesnt open. and 'insidegr.pdb' named file is not formed in my directory.

please guide me through

I am attaching the *.mdp file with this mail. 

regards
nur

   
-
 Save all your chat conversations. Find them online.

hpgr.mdp
Description: 3875843079-hpgr.mdp
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Re: [gmx-users] Methanol SOL :Number of solventmolecules = 0

2007-12-12 Thread sharada










Dear Dr. Xavier Periole,
Thank you for guiding me through. I could solve the problem of setting up the 
system for minimization. However  When  started minimization run for 2000 steps 
with steepest descent , I encountered yet another problem. which is as follows 
..
Methanol optimization:
Started Steepest Descents on node 0 Tue Dec 11 17:48:57 2007
Removing pbc first time
Done rmpbc
Steepest Descents:
   Tolerance (Fmax)   =  1.0e+01
   Number of steps= 2000
Grid: 4 x 5 x 4 cells
calc_bor: cg0=0, cg1=553, ncg=553
CG0[0]=0, CG1[0]=553
CG0[1]=0, CG1[1]=0
calc_bor: cg0=0, cg1=553, ncg=553
CG0[0]=0, CG1[0]=553
CG0[1]=0, CG1[1]=0
Configuring nonbonded kernels...
Testing AMD 3DNow support... not present.
Testing ia32 SSE support... present.
Step   Time Lambda
  00.00.0
calc_bor: cg0=0, cg1=553, ncg=553
CG0[0]=0, CG1[0]=553
CG0[1]=0, CG1[1]=0
Program mdrun, VERSION 3.3
Source code file: nsgrid.c, line: 226
Range checking error:
Explanation: During neighborsearching, we assign each particle to a grid
based on its coordinates. If your system contains collisions or parameter
errors that give particles very high velocities you might end up with some
coordinates being +-Infinity or NaN (not-a-number). Obviously, we cannot
put these on a grid, so this is usually where we detect those errors.
Make sure your system is properly energy-minimized and that the potential
energy seems reasonable before trying again.
Variable ci has value -2147483648. It should have been within [ 0 .. 80 ]
Please report this to the mailing list (gmx-users@gromacs.org)

Now where do I go from here? Its asking me to energy minimize the system which 
is what I am trying to do ! What is this ci value and why is it so high? Kindly 
help me I am once again stuck.  Furthermore, when I minimized  the same peptide 
in SPC216 water box of 1108 water molecules for 2000 steps this error did not 
appear. When I compared the md.log files in both the cases I found that in case 
of water optimization of SPC water was enabled where as this line for methanol 
was missing which  should mean that the energies are shooting off  scale is 
that right ? Should I optimize my system in vacuo before simmulating in 
methanol? 
Water optimization:
{Generated table with 500 data points for 1-4 LJ12.
Tabscale = 500 points/nm
Enabling SPC water optimization for 1108 molecules.
Initiating Steepest Descents
Center of mass motion removal mode is Linear
We have the following groups for center of mass motion removal:
  0:  rest, initial mass: 3396
Started Steepest Descents on node 0 Wed Dec 12 15:52:11 2007
Removing pbc first time
Done rmpbc
Steepest Descents:
   Tolerance (Fmax)   =  1.0e+01
   Number of steps= 2000
Going to use C-settle (1108 waters)
wo = 0.33, wh =0.33, wohh = 3, rc = 0.08165, ra = 0.0384897
rb = 0.0192449, rc2 = 0.1633, rone = 1, dHH = 0.1633, dOH = 0.1
Grid: 4 x 5 x 4 cells}
regards
sharada
 
-- Original Message --
From: Xavier Periole [EMAIL PROTECTED]
To: Discussion list for GROMACS users gmx-users@gromacs.org
Date: Tue, 11 Dec 2007 12:07:27 +0100
Subject: Re: Fw:  Re: [gmx-users] Methanol SOL :Number of solvent molecules 
= 0
in your agg2t.top you should replace the last line :
SOLXXX
by:
Methanol XXX
which is the name of the molecule.
You should also remove the angle definition in methanol.itp. Placing
a ; at the beginning of the line is enough.
XAvier
On Tue, 11 Dec 2007 15:40:04 +0530 (IST)
  sharada  [EMAIL PROTECTED] wrote:
 Dear Mark Abraham,
 I have changed MeoH to SOL in .gro and .itp files and also changed the 
#include line  to methanol.itp
 It now seemed to have written the solvent molecules in the top file with SOL 
as the name with atom types of methanol. 
 When I ran grompp program as following I get the error as shown below: I am 
also attaching the .gro,.itp,.top files. for information.  Did I miss out 
anything ? 
 grompp -f em.mdp -c agg2_b4em.gro -p agg2.top -o agg2_em.tpr
 [EMAIL PROTECTED] Aggregates]$ grompp -f em.mdp -c agg2_b4em.gro -p agg2.top 
 -o 
agg2_em.tpr
  
 Option   Type  Value  Description
 --
   -[no]h   bool no  Print help info and quit
   -[no]X   bool no  Use dialog box GUI to edit command line options
-niceint  0  Set the nicelevel
   -[no]v   boolyes  Be loud and noisy
-time   real -1  Take frame at or first after this time.
  -npint  1  Generate statusfile for # nodes
 -[no]shuffle   bool no  Shuffle molecules over nodes
-[no]sort   bool no  Sort molecules according to X coordinate
 creating statusfile 

Re: [gmx-users] pbc and tpr file

2007-12-12 Thread tangxuan
Hi, 
Thanks for your reply. The protein I simulated has 16 subunits. I
checked the protein struture (no jump) in the tpr file and there are no
contacts between each subunits. The protein structure in the fist frame
of simulation seems ok, but has jumps. Two strucutres are very different
and I do not why? Therefore,  something strange (rotation) will happen
to the system after I remove jumps in the trajectory.  Do you think it
is right to produce a new reference structure from the first frame by
tpbconv?


Thanks

Tang
On Wed, 2007-12-12 at 09:03 +0100, Tsjerk Wassenaar wrote:
 Hi Tang,
 
 It doesn't hurt to check (i.e. you should check ;)) whether the .tpr
 file contains the protein in one piece, if you want to use it as a
 reference structure for rmsd calculations. You can extract the
 coordinates from the .tpr file using editconf and then have a look.
 Actually, you should've done this prior to removing jumps from the
 trajectory, since you must be sure to remove the jumps in the right
 way (check the archives for more discussion on these issues). 
 
 Cheers,
 
 Tsjerk
 
 On Dec 12, 2007 1:42 AM, Mark Abraham [EMAIL PROTECTED] wrote:
 tangxuan wrote:
  hi all,
   I want to calculate the rmsd of my protein. If I remove the
 jump in the
  xtc file or trr file, what should I do with tpr file?
 
 
 Nothing. Depending on your inputs to g_rms, it might provide
 your 
 reference structure.
 
 Mark
 
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 -- 
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 Junior UD (post-doc)
 Biomolecular NMR, Bijvoet Center
 Utrecht University
 Padualaan 8 
 3584 CH Utrecht
 The Netherlands
 P: +31-30-2539931
 F: +31-30-2537623 
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Re: [gmx-users] literature on GROMOS96 43b1 force field and vacuum simulations

2007-12-12 Thread Xavier Periole

On Wed, 12 Dec 2007 11:24:01 +0100
 Carsten Baldauf [EMAIL PROTECTED] wrote:

dear all//
i am looking for literature describing the gromos 96 force fields, 
especially the vacuum force field 43b1. unfortunately i don't find much 
besides the gromos manual ...


look for gromos force field you should find it easily. You can also
go to the web page of van Gunsteren's group at the ETH.


do you have any suggestions/hints?
thank you very much//
carsten

p.s.: just in case you would want to perform a md simulation of a 
peptide/protein in vacuum, which force field would you choose and why?


Depends what you want to do with the simulation. However in a general
manner there are no force field that is known to describe a protein/peptide
in vacuum with any relative realism.



--
dr carsten baldauf
biotechnologisches zentrum der tu dresden
http://www.biotec.tu-dresden.de/pisabarro
http://www.biotec.tu-dresden.de/~carstenb

Molecular Docking, Complexity, and Optimization
See http://pacosy.informatik.uni-leipzig.de/MDCO-2007/

Please avoid sending me Word or PowerPoint attachments.
See http://www.gnu.org/philosophy/no-word-attachments.html

No Software Patents!
See http://www.ffii.org/index.en.html

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-
XAvier Periole - PhD

NMR  Molecular Dynamics Group
University of Groningen
The Netherlands
http://md.chem.rug.nl/~periole
-
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[gmx-users] Is there any way to do r^3 distance dependence?

2007-12-12 Thread Arthur Roberts

Hi, all,

I know that Gromacs has the capability of restraining a molecule with  
r^6 distance dependence.   Is there any way to do r^3 distance  
dependence?


Best wishes,
Art Roberts
University of Washington
Department of Medicinal Chemistry
Seattle, WA 98195
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[gmx-users] Re: Diagnosing an explosion

2007-12-12 Thread Steven Kirk
Apologies for replying to myself - maybe I can sharpen up some of my 
original questions below:



Reply below

 
 I am having a problem with my BD simulation either crashing with a Range 
 error or locking up the mdrun process completely.
 
 I am running Gromacs 3.3.1 (must use this version ATM because HPC 
 provider has not upgraded yet) on a quad core Intel machine, w/ Fedora 
 Core 7.
 
 I have 1000 'particles' in a cubic box (configuration here:
 
 http://datavet.hv.se/personal/SK/publicfiles/colloid.pdb
 
 where the particles are placed randomly with no two particle centres 
 closer than 4 nm.
 
 The particles are defined in the topology here:
 
 ; Complete topology file

 ;
 ; particles.itp
 
 [ defaults ]

 1  1  no  1.0  1.0
 
 [ atomtypes ]

 AR   28699.81134   0.00   A   1.0   1.0
 
 Looks like you are using dimensionless eps and sigma while using 
 otherwise MD units (e.g. T). Check chapter 2 of the manual. You want to 
 multiply your T by boltz (0.008314 or something like that) probably.


Aha! Thank you David.

My goal was to use MD units in everything, since my tabulated data file 
was extracted from another GROMACS simulation and is hence already in MD 
units (kJ/mol vs. nm), and I would prefer to specify temperatures in K.


My reason for specifying 1.0 for the last two parameters was that I 
thought this would allow me to use, unscaled, the tabulated potential 
(which is already in MD units).


If I want to do this, what alternative values should I use for the last 
two parameters on the [ atomtypes ] line above (given that I am really 
only using the g(r) and g''(r) columns to hold my potential data: the 
h(r) and h''(r), which I don't care about, are all zeroes) ?


If I change the combination type to 2 or 3 in the  [ defaults ] line, 
will this remove the unit scaling problem ?


I have checked Chapter 2 in the manual and I am still unsure how to 
handle this.


I took your advice (which matches with manual Section 2.4 on *reduced* 
units) and scaled my temperature to 2.494353 =  300K * 0.008314. This 
did not give a crash, but increasing the timestep and decreasing bd_fric 
made the problem return.


Scaling the temperature value in this way did not fix the 'equilibration 
around 2x requested temperature' problem mentioned below - g_energy 
still shows the temperature settling at a numerical value around 4.988.


Can anyone suggest a reason for this strange thermostat behaviour ?

Many thanks,
Steve Kirk

--
Dr. Steven R. Kirk   [EMAIL PROTECTED], [EMAIL PROTECTED]
Dept. of Technology, Mathematics  Computer Science  (P)+46 520 223215
University West  (F)+46 520 223299
P.O. Box 957 Trollhattan 461 29 SWEDEN   http://taconet.webhop.org
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[gmx-users] Gel Phase in DMPC using Berger force field ?? -- Focus: naming convention

2007-12-12 Thread chris . neale

Several points:

What is called the Berger force field was
actually developed by See-Wing Chiu in our lab
and presented in a 1995 paper.  The Berger et al
paper tested this force field against another
candidate and found that it was better, and that
is the paper that has been cited ever since.


I agree that it is incorrect to refer to this as the Berger  
forcefield, although I have myself referred to it in this way for  
informal discussions. If one were to discuss the important  
contributions I would refer to the following papers  
(Jorgensen_1988/Egberts_1994/Chiu_1995/Chiu_1996/Berger_1997), and of  
course the Ryckaert-Bellemans contribution is also important.

Perhaps I have missed some, but in that case it is not intentional.

I would be interested to participate in a discussion about the naming  
convention for these parameters. For example, it is unclear to me why  
one would refer to them as the 'Chiu parameters' as opposed to the  
'Egbert parameters', or even the 'Ryckaert-Bellemans lipid  
parameters'. I would also accept an acronym from the first authors  
such as RBJECB. For detailed methods sections I am in the habit of  
referring to it by a chronological sentence as opposed to by a short  
name, but for informal discussion a short name is certainly convenient.


To be clear, I am not arguing against calling then the 'Chiu  
parameters' but would be in favour of more discussions on the topic.


Chris.



See-Wing did tests of the necessary VDW cut-off
for accuracy against what seemed like the most
sensitive test, the value of the dipole potential
at the water-lipid interface, and concluded that
one should use a cut-off of at least 18 angstroms.

The van der Waals parameters for the hydrocarbon
tails were reparameterized in a paper we
published a few years ago, and in that paper we
verified that the 18 angstrom cutoff was required
for an accurate liquid hydrocarbon simulation also.

Recently See-Wing has reparameterized the van der
Waals parameters in the lipid head groups, using
specific volumes of liquids comprised of small
molecules that are part of the head group.  The
resulting force fields, which retain the partial
charges of the Berger-Chiu field, work very well
in replicating x-ray structure factors of lipids
with various chain compositions, but he has not
yet tried to do gel phase--that would be
interesting.  The journal ms. is still sitting on
my desk, I am afraid, but there is a pretty good
description of the parameterization in a chapter
in a book that Scott Feller is editing, which we
can send on request, as well as the lipid
complete force field in itself.  We believe it is
state of the art at this time.

Best,
Eric





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[gmx-users] is there performance data for GROMACS on Blue Gene/L?

2007-12-12 Thread Mark Abraham
Does anybody have access to any performance data for GROMACS on a Blue 
Gene/L system? I'm putting together a proposal for some time on such a 
machine, and some moderately accurate costings would be nice.


Mark
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[gmx-users] Density Deferences between spc216 and tip4p water models

2007-12-12 Thread csreddy
Dear All,
I was trying  create a  box (cubic 10 10 10) of water. I am a bit
surprised by looking at the density deferences between spc216 and tip4p
water models. I am giving the brief output below.

genbox -cs tip4p.gro -box 10 10 10

Output configuration contains 131540 atoms in 32885 residues
Volume :1000 (nm^3)
Density: 1639.65 (g/l)
Number of SOL molecules:  32885


genbox -cs spc2i6.gro -box 10 10 10

Output configuration contains 99678 atoms in 33226 residues
Volume :1000 (nm^3)
Density: 993.966 (g/l)
Number of SOL molecules:  33226

What would be the reason for this drastic differences in density? How can
I make it into 1000 (g/l) by using above command.

Thanks in advance.
Regards
Chandu


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