Re: [gmx-users] RE: heat capacity etc. (Thomas Koller)

2011-03-12 Thread David van der Spoel

On 2011-03-12 07.52, Thomas Koller wrote:

Thanks,

the equation for the heat capacity is:

c(P) = delta(H(average))/delta(T(average))

So do it have to take the fluctuations (which are listed with g_energy) of 
U(tot) and pV as well as of T to calculate c(P)? The problem is the delta.

The same is with the thermal compressibility:

a(P) = 1/V(average) * delta(V(average))/delta(T(average))

Another question: Why should I take U(tot) and not only the potential for c(P)? 
The same is for the heat of vaporization, here also with U(tot)?

Regards,
Thomas

You need to compute the enthalpy = Etot + pV. The fluctuations in Etot 
and pV are correlated and compensate each other to some extent, and 
hence you need to sum the two first and compute the fluctuations afterward.


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Re: [gmx-users] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread David van der Spoel

On 2011-03-12 06.09, Denny Frost wrote:

I am running MD simulations on Liquid/Liquid interfaces and measuring
the interfacial tension between them.  I have found that the readings in
NVT simulations are close to experimental values, but have a lot of
variation.  I run NPT simulations on the exact same system and find the
results show very little variation, but the values are far from
experimental results.  Does anyone know why this happens?

Please be more specific. How do you do NPT simulations? This may 
influence the result. To get good result I would suggest to do pressure 
coupling only in the normal direction and to turn off dispersion 
corrections to the pressure.


--
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Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
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Re: [gmx-users] versions

2011-03-12 Thread David van der Spoel

On 2011-03-12 08.54, mohsen ramezanpour wrote:

Dear All

How can I read and work on outputs of one  version of Gromacs with tools
of other version?
Because I have run my program on cluster(version 4.5.3) ,but I need to
work with them in v.4.0.7

Suppose I have to work with this version and there is not any way to
change versions neighter on cluster no on my laptop
Please let me know if there is any solution
thanks in advance for your guidances
Mohsen

you can read xtc and edr from newer version in most of the cases but not 
tpr. You have to make old tprs. If it is *your* laptop you can upgrade 
gromacs of course.


--
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Dept. of Cell  Molec. Biol., Uppsala University.
Box 596, 75124 Uppsala, Sweden. Phone:  +46184714205.
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Re: [gmx-users] versions

2011-03-12 Thread Francesco Oteri

Hi mohsen,
I think that I need to work with them in v.4.0.7  means that you need 
to ANALYZE your trajectory with gmx4.0.7. Is it correct?

If this is the case, problem should not arise with trajectory files.

You should have problems only with topology that is not back-compatible.
However, for the majority of gmx programs, a pdb file that represents 
your system is sufficient.


If you strictly need a .tpr file, I suggest you to create a new topology 
with the 4.0.7 version.



Il 12/03/2011 08:54, mohsen ramezanpour ha scritto:

Dear All

How can I read and work on outputs of one  version of Gromacs with 
tools of other version?
Because I have run my program on cluster(version 4.5.3) ,but I need to 
work with them in v.4.0.7


Suppose I have to work with this version and there is not any way to 
change versions neighter on cluster no on my laptop

Please let me know if there is any solution
thanks in advance for your guidances
Mohsen


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Re: [gmx-users] versions

2011-03-12 Thread mohsen ramezanpour
thanks for your replies.

Yes,you are correct.
Actually I need to analyze my trajectories and energy files .
I tried but I couldn't use from my energy.edr file in old version(4.0.7),it
say:
it seems you want to read edr file from version 4.1 or latter with old
version 
Please let me know how can I solve this problem
Thanks in advance

On Sat, Mar 12, 2011 at 1:38 PM, Francesco Oteri
francesco.ot...@gmail.comwrote:

 Hi mohsen,
 I think that I need to work with them in v.4.0.7  means that you need to
 ANALYZE your trajectory with gmx4.0.7. Is it correct?
 If this is the case, problem should not arise with trajectory files.

 You should have problems only with topology that is not back-compatible.
 However, for the majority of gmx programs, a pdb file that represents your
 system is sufficient.

 If you strictly need a .tpr file, I suggest you to create a new topology
 with the 4.0.7 version.


 Il 12/03/2011 08:54, mohsen ramezanpour ha scritto:

  Dear All

 How can I read and work on outputs of one  version of Gromacs with tools
 of other version?
 Because I have run my program on cluster(version 4.5.3) ,but I need to
 work with them in v.4.0.7

 Suppose I have to work with this version and there is not any way to
 change versions neighter on cluster no on my laptop
 Please let me know if there is any solution
 thanks in advance for your guidances
 Mohsen


 --
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 http://lists.gromacs.org/mailman/listinfo/gmx-users
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Re: [gmx-users] versions

2011-03-12 Thread mohsen ramezanpour
The exact Error is this:

Program g_energy, VERSION 4.0.7
Source code file: ../../../../src/gmxlib/enxio.c, line: 118

Fatal error:
You are trying to read an edr file of GROMACS version 4.1 or later with
GROMACS version 4.0





On Sat, Mar 12, 2011 at 2:46 PM, mohsen ramezanpour 
ramezanpour.moh...@gmail.com wrote:

 thanks for your replies.

 Yes,you are correct.
 Actually I need to analyze my trajectories and energy files .
 I tried but I couldn't use from my energy.edr file in old version(4.0.7),it
 say:
 it seems you want to read edr file from version 4.1 or latter with old
 version 
 Please let me know how can I solve this problem
 Thanks in advance

 On Sat, Mar 12, 2011 at 1:38 PM, Francesco Oteri 
 francesco.ot...@gmail.com wrote:

 Hi mohsen,
 I think that I need to work with them in v.4.0.7  means that you need to
 ANALYZE your trajectory with gmx4.0.7. Is it correct?
 If this is the case, problem should not arise with trajectory files.

 You should have problems only with topology that is not back-compatible.
 However, for the majority of gmx programs, a pdb file that represents your
 system is sufficient.

 If you strictly need a .tpr file, I suggest you to create a new topology
 with the 4.0.7 version.


 Il 12/03/2011 08:54, mohsen ramezanpour ha scritto:

  Dear All

 How can I read and work on outputs of one  version of Gromacs with tools
 of other version?
 Because I have run my program on cluster(version 4.5.3) ,but I need to
 work with them in v.4.0.7

 Suppose I have to work with this version and there is not any way to
 change versions neighter on cluster no on my laptop
 Please let me know if there is any solution
 thanks in advance for your guidances
 Mohsen


 --
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 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at
 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
 Please don't post (un)subscribe requests to the list. Use the www
 interface or send it to gmx-users-requ...@gromacs.org.
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[gmx-users] Regarding DCCM analysis with g_covar available in user contributed section

2011-03-12 Thread bipin singh
Hello,
I am using g_covar vailable in user contributed section (by Ran Friedman)
the description available for the package is as follows:

This package contains a modified version of g_covar, which can print a
matrix
of atomic correlation coefficients (with -xpmc) and write all pairs with a
correlation  0.5 to a log file (with -clog). Otherwise it is the same as
the
original program.
The xpm correlation matrix shows only cross-correlations larger than 0.5
(absolute values) on the upper triangle and all values on the lower
triangle. Thus, the upper triangle displays only the most correlated
motions.

As stated that the upper triangle only shows the cross-correlation greater
than
0.5, but I am also getting some negative correlation values(blue regions) in
above triangle.
I don't know what is the region behind this.
Plz help me to understand this behaviour.
I have attached my xpm matrix file generated using g_covar.
-- 
*
-
Thanks and regards
Bipin Singh
*
*
*
attachment: coor.xpm-- 
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Re: [gmx-users] versions

2011-03-12 Thread David van der Spoel

On 2011-03-12 12.23, mohsen ramezanpour wrote:

The exact Error is this:

Program g_energy, VERSION 4.0.7
Source code file: ../../../../src/gmxlib/enxio.c, line: 118

Fatal error:
You are trying to read an edr file of GROMACS version 4.1 or later with
GROMACS version 4.0


Upgrade gromacs.





On Sat, Mar 12, 2011 at 2:46 PM, mohsen ramezanpour
ramezanpour.moh...@gmail.com mailto:ramezanpour.moh...@gmail.com wrote:

thanks for your replies.

Yes,you are correct.
Actually I need to analyze my trajectories and energy files .
I tried but I couldn't use from my energy.edr file in old
version(4.0.7),it say:
it seems you want to read edr file from version 4.1 or latter with
old version 
Please let me know how can I solve this problem
Thanks in advance

On Sat, Mar 12, 2011 at 1:38 PM, Francesco Oteri
francesco.ot...@gmail.com mailto:francesco.ot...@gmail.com wrote:

Hi mohsen,
I think that I need to work with them in v.4.0.7  means that
you need to ANALYZE your trajectory with gmx4.0.7. Is it correct?
If this is the case, problem should not arise with trajectory files.

You should have problems only with topology that is not
back-compatible.
However, for the majority of gmx programs, a pdb file that
represents your system is sufficient.

If you strictly need a .tpr file, I suggest you to create a new
topology with the 4.0.7 version.


Il 12/03/2011 08:54, mohsen ramezanpour ha scritto:

Dear All

How can I read and work on outputs of one  version of
Gromacs with tools of other version?
Because I have run my program on cluster(version 4.5.3) ,but
I need to work with them in v.4.0.7

Suppose I have to work with this version and there is not
any way to change versions neighter on cluster no on my laptop
Please let me know if there is any solution
thanks in advance for your guidances
Mohsen


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--
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] Questions about implementing G56A_CARB parameters

2011-03-12 Thread Jon Kapla

Hi,

I'm about to simulate a disaccaride in water.
Reading through the paper from Hansen and Hünenberger:

A reoptimized GROMOS force field for hexopyranose-based carbohydrates 
accounting for the relative free energies of ring conformers, anomers, 
epimers, hydroxymethyl rotamers, and glycosidic linkage conformers.
?Hansen, H. S.; Hünenberger, P. H. /Journal of computational chemistry/. 
2010.

doi: 10.1002/jcc.21675

it seems like a very rigid work and a good force field to use, since it 
is directly based on the G53a6 ff already included in gromacs.


In the above paper they state that they introduce some things not 
implemented according to the buildup rules and functionals of the 
gromos96 program (but part of the upcoming version as of November 2010 
though). These  things are mainly the ability to use other torsional 
phase shifts than 0 and 180 degrees and the addition of some 1-3 
Lennard-Jones interactions for improved six ring stability.


The torsion angle function given in the gromacs manual is exactly the 
same as they give in the paper above.


 Thus, my first question is if gromacs have any restrictions on the 
phase shifts, or if I directly can use the additional shifts of -60 and 
60 degrees from 56A_CARB.


The second question is about the 1-3 interactions. What's the best way 
of implementing this? Can I use an nrexcl of 2 and then add the wanted 
interactions to the pair list and all other to the excluded 
interactions? Do you have any other suggestions?


Best regards
Jon Kapla




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Re: [gmx-users] Can gmx change a, b of 3D pbc box but remain c in constant-NPT MD?

2011-03-12 Thread Justin A. Lemkul



英雄不再寂寞 wrote:

Dear gmxers,
   I want to perform a constant-NPT MD simulation using gmx. By default, 
a,b,c of 3D pbc box can change to compatile with the density. Whether 
can gmx change a,b of 3D pbc box but unchange c? Please give me some 
hints. Thanks a lot.
 


Set the compressibility of whichever direction you need to be constant to zero. 
 This would require anisotropic or semi-isotropic coupling to allow other 
dimensions to scale.


-Justin


Yours sincerely,
Chaofu Wu, Dr.



--


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] Possible free energy bug?

2011-03-12 Thread Justin A. Lemkul


Hi All,

I believe I have a resolution to all of this.  It comes down to compilers and 
FFTW.  I had always used the same compilers to build all my Gromacs versions 
(gcc-4.2.2 on Linux, gcc-3.3 on OSX) with the same version of FFTW (3.0.1), 
primarily for reasons of continuity.  Bug 715 that I posted before was due to a 
problem with FFTW, not Gromacs; upgrading to 3.2.2 solves the issue.  As well, 
the combination of gcc-4.4.5 + FFTW 3.2.2 allows for successful free energy runs 
in my tests thus far on Linux.  Dependency issues on the OS X partition prevent 
me from doing any upgrades, so we're out of luck there, unfortunately.  I will 
report back if any other weird behavior results, but I believe the problem is 
solved.


I am no compiler/library guru, but it would seem to me that we've reached a 
point where certain minimum versions must be required for certain prerequisites. 
 I would suggest that prior to the next release, we come up with a list of what 
should be considered stable minimum requirements (compiler versions, FFTW, 
anything else) to post on the website and perhaps the manual.  As it stands now, 
the prerequisites for installation would seem to be satisfied by any C compiler 
and any version of FFTW.  Gromacs happily compiles under most conditions, but 
shows some weird behavior if one is not using optimal dependencies.


Thanks to all for their input!

-Justin

Justin A. Lemkul wrote:



Michael Shirts wrote:

Hi, all-

Have you tried running

constraints = hbonds?

That might eliminate some of the constraint issues.  Much less likely
for LINCS to break or have DD issues if only the hbonds are
constrained.  2 fs is not that big a deal for the heteroatom bonds.



I haven't yet, but I'll add it to my to-do list.  I was trying to keep 
as many things consistent between my 3.3.3 and 4.5.3 input files as 
possible, so I could diagnose any issues, but at this point, anything is 
worth a shot.


Thanks!

-Justin


Best,
Michael

On Thu, Mar 10, 2011 at 8:04 PM, Justin A. Lemkul jalem...@vt.edu 
wrote:

Hi Matt,

Thanks for the extensive explanation and tips.  I'll work through 
things and
report back.  It will take a while to get things going through 
(unless one
of the early solutions works!) since I have no admin access to 
install new
compilers, libraries, etc. and for some reason the only thing I can 
ever get

to work in my home directory is Gromacs itself.  The joys of an aging
cluster.

We recently got access to gcc-4.4.5 on Linux, but we're stuck with 
3.3 on OS

X, so there's at least a bit of hope for one partition.

Thanks again.

-Justin

Matthew Zwier wrote:

Hi Justin,

I should have specified that the segfault happened for us after we got
similar warnings and errors (DD and/or LINCS), so the segfault may
have been tangential.  Given that everything about your system worked
before GROMACS 4.5, it's possible that your older compilers are
generating code that's incompatible with the GROMACS assembly loops
(which you are likely running with, as they are the default option on
most mainstream processors).  The bug you mentioned in your original
post also has my antennae twitching about bad machine code.

If that's indeed happening, it's almost certainly some bizarre
alignment issue, something like half of a float is getting overwritten
on the way into or out of the assembly code, which corruption would
trigger the results you describe.  It's also distantly possible that
GROMACS is working fine, but your copy of FFTW or BLAS/LAPACK (more
likely the latter) has alignment problems.  One final possibility
(which would explain the failure on YellowDog but unfortunately not
the failure on OS X) is that GCC is generating badly-aligned code for
auto-vectorized Altivec loops, which is still a problem for Intel's
SIMD instructions on 32-bit x86 architectures even with GCC 4.4.  I've
also observed MPI gather/reduce operations to foul up alignment (or
rigidly enforce it where badly compiled code is relying on broken
alignment) under exceedingly rare circumstances, usually involving
different libraries compiled with different compilers (which is
generally a bad idea for scientific code anyway).

Okay...so all of that said, there are a few things to try:

1) Recompile GROMACS using -O2 instead of -O3; that'll turn off the
automatic vectorizer (on Yellow Dog) and various other relatively
risky optimizations (on both platforms).  CFLAGS=-O2 -march=powerpc
in the environment AND on the configure command line would do that.
Check your build logs to make sure it took, though, because if you
don't do it exactly right, configure will ignore your directives and
merrily set up GROMACS to compile with -O3, which is the most likely
culprit for badly-aligned code.

2) Recompile GROMACS specifying a forced alignment flag.  I have no
experience with PowerPC, but -malign-natural and -malign-power look
like good initial guesses.  That's probably going to cause more
problems than it solves, but if you have a 

[gmx-users] RE: Regarding DCCM analysis with g_covar available in user contributed section

2011-03-12 Thread Ran Friedman
Hi,
As stated below the upper half of the triangle shows correlations having r0.5 
or r-0.5, that is |r|0.5
Ran


From: bipin singh [bipinel...@gmail.com]
Sent: 12 March 2011 12:27
To: Discussion list for GROMACS users
Cc: r.fried...@bioc.uzh.ch
Subject: Regarding DCCM analysis with g_covar available in user contributed 
section

Hello,
I am using g_covar vailable in user contributed section (by Ran Friedman) the 
description available for the package is as follows:

This package contains a modified version of g_covar, which can print a matrix
of atomic correlation coefficients (with -xpmc) and write all pairs with a
correlation  0.5 to a log file (with -clog). Otherwise it is the same as the
original program.
The xpm correlation matrix shows only cross-correlations larger than 0.5
(absolute values) on the upper triangle and all values on the lower
triangle. Thus, the upper triangle displays only the most correlated motions.

As stated that the upper triangle only shows the cross-correlation greater than
0.5, but I am also getting some negative correlation values(blue regions) in 
above triangle.
I don't know what is the region behind this.
Plz help me to understand this behaviour.
I have attached my xpm matrix file generated using g_covar.
--
-
Thanks and regards
Bipin Singh


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[gmx-users] RE: heat capacity etc. (Thomas Koller)

2011-03-12 Thread Thomas Koller
I dont know exactly what you mean. Here you can see my output data:


Energy  AverageRMSDFluct.  Drift  Tot-Drift
---
Potential -48.8499  1.82144  1.81841 -0.00781553  -0.3638
Kinetic En.50.7548  1.42996  1.42991 -0.000872827 -0.0406286
Total Energy   1.90489  2.32653  2.3236  -0.00868836  -0.404429
Temperature298.15   8.40003  8.39975 -8.84014e-05 -0.238666
Pressure (bar) 1.66395  713.24   713.236  0.00302056   8.15491
Volume 21.0391  0.179301 0.178412-2.2873e-05 -0.0617527
pV-0.45227  903.541  903.536  0.00377916   10.203
Heat Capacity Cv:  13.3969 J/mol K (factor = 0.0460384)
Isothermal Compressibility: 3.71208e-05 /bar
Adiabatic bulk modulus:26939.1  bar

i) How should I calculate the isobaric heat capacity with this values, bu udage 
of the Fluct. in the 3rd column?

ii) How is the isothermal compressibility here calculated?

Regards,
Thomas
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Re: [gmx-users] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread aldi asmadi
David,

I have a question that is still related to your reply.  If the bulk
liquid NPT and the interfacial liquid-vapor NVT simulations are
performed using dispersion corrections to the pressure and energy,
while the intefacial liquid-liquid NPAT simulation don't use any
correction, can we say that all results are valid since we don't give
the same treatment for all systems?

In the NPT and NVT calculations, we apply corrections in order to
reduce the discrepancy between the calculated and experimental
properties (say density and surface tension) as small as possible.
Here we have more confidence that our molecules in systems behave
accordingly judging from the macroscopic values we obtain.  Meanwhile,
in the NPAT calculation, we don't use such correction meaning that the
property (say interfacial tension) is expected to deviate more from
the experimental value? This indicates that the system behaves
differently in comparison to the same simulation conducted with
correction?

Many thanks,
Aldi


On Sat, Mar 12, 2011 at 11:44 AM, David van der Spoel
sp...@xray.bmc.uu.se wrote:
 On 2011-03-12 06.09, Denny Frost wrote:

 I am running MD simulations on Liquid/Liquid interfaces and measuring
 the interfacial tension between them.  I have found that the readings in
 NVT simulations are close to experimental values, but have a lot of
 variation.  I run NPT simulations on the exact same system and find the
 results show very little variation, but the values are far from
 experimental results.  Does anyone know why this happens?

 Please be more specific. How do you do NPT simulations? This may influence
 the result. To get good result I would suggest to do pressure coupling only
 in the normal direction and to turn off dispersion corrections to the
 pressure.

 --
 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.se    http://folding.bmc.uu.se
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Re: [gmx-users] versions

2011-03-12 Thread Francesco Oteri

That are different way:
1. Performing analysis directly on the cluster where 4.5.3 is installed
2. Installing gmx 4.5.3 on you laptop.
3. Writing a program that converts from 4.5.3 to 4.0.7



Il 12/03/2011 12:16, mohsen ramezanpour ha scritto:

thanks for your replies.

Yes,you are correct.
Actually I need to analyze my trajectories and energy files .
I tried but I couldn't use from my energy.edr file in old 
version(4.0.7),it say:
it seems you want to read edr file from version 4.1 or latter with 
old version 

Please let me know how can I solve this problem
Thanks in advance

On Sat, Mar 12, 2011 at 1:38 PM, Francesco Oteri 
francesco.ot...@gmail.com mailto:francesco.ot...@gmail.com wrote:


Hi mohsen,
I think that I need to work with them in v.4.0.7  means that you
need to ANALYZE your trajectory with gmx4.0.7. Is it correct?
If this is the case, problem should not arise with trajectory files.

You should have problems only with topology that is not
back-compatible.
However, for the majority of gmx programs, a pdb file that
represents your system is sufficient.

If you strictly need a .tpr file, I suggest you to create a new
topology with the 4.0.7 version.


Il 12/03/2011 08:54, mohsen ramezanpour ha scritto:

Dear All

How can I read and work on outputs of one  version of Gromacs
with tools of other version?
Because I have run my program on cluster(version 4.5.3) ,but I
need to work with them in v.4.0.7

Suppose I have to work with this version and there is not any
way to change versions neighter on cluster no on my laptop
Please let me know if there is any solution
thanks in advance for your guidances
Mohsen


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Re: [gmx-users] RE: heat capacity etc. (Thomas Koller)

2011-03-12 Thread David van der Spoel

On 2011-03-12 14.00, Thomas Koller wrote:

I dont know exactly what you mean. Here you can see my output data:


Energy  AverageRMSDFluct.  Drift  Tot-Drift
---
Potential -48.8499  1.82144  1.81841 -0.00781553  -0.3638
Kinetic En.50.7548  1.42996  1.42991 -0.000872827 -0.0406286
Total Energy   1.90489  2.32653  2.3236  -0.00868836  -0.404429
Temperature298.15   8.40003  8.39975 -8.84014e-05 -0.238666
Pressure (bar) 1.66395  713.24   713.236  0.00302056   8.15491
Volume 21.0391  0.179301 0.178412-2.2873e-05 -0.0617527
pV-0.45227  903.541  903.536  0.00377916   10.203
Heat Capacity Cv:  13.3969 J/mol K (factor = 0.0460384)
Isothermal Compressibility: 3.71208e-05 /bar
Adiabatic bulk modulus:26939.1  bar

i) How should I calculate the isobaric heat capacity with this values, bu udage 
of the Fluct. in the 3rd column?

ii) How is the isothermal compressibility here calculated?

Regards,
Thomas

You have to read up, check Allen  Tildesly or something like that.

To get the enthalpy you have to extract the total energy graph and and 
the volume graph and sum Etot + p time Volume (in xmgrace or excel, 
whatever). Then compute the fluctuations from that. You have to do it 
all manually.


The heat capacity above is meaningless, this is why we have improved 
that in newer gmx version. Note that if you have used Berendsen T and/or 
P coupling you can not compute any fluctuation properties from your 
simulations.


--
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] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread Denny Frost
I have run NPT simulations using isotropic and semiisotropic coupling with
the same results.  I have never done coupling in just one direction though,
how do you do this?.  I have never used Dispersion corrections.  It seems to
me that this would help, rather than hurt though since, as Aldi said, it
will make the system closer to experimental values.  I will give this a try
and see what happens.  My question still remains - why do NPT and NVT
simulations give such different values for surface tension?
Denny Frost

On Sat, Mar 12, 2011 at 6:40 AM, aldi asmadi aldi.asm...@gmail.com wrote:

 David,

 I have a question that is still related to your reply.  If the bulk
 liquid NPT and the interfacial liquid-vapor NVT simulations are
 performed using dispersion corrections to the pressure and energy,
 while the intefacial liquid-liquid NPAT simulation don't use any
 correction, can we say that all results are valid since we don't give
 the same treatment for all systems?

 In the NPT and NVT calculations, we apply corrections in order to
 reduce the discrepancy between the calculated and experimental
 properties (say density and surface tension) as small as possible.
 Here we have more confidence that our molecules in systems behave
 accordingly judging from the macroscopic values we obtain.  Meanwhile,
 in the NPAT calculation, we don't use such correction meaning that the
 property (say interfacial tension) is expected to deviate more from
 the experimental value? This indicates that the system behaves
 differently in comparison to the same simulation conducted with
 correction?

 Many thanks,
 Aldi


 On Sat, Mar 12, 2011 at 11:44 AM, David van der Spoel
 sp...@xray.bmc.uu.se wrote:
  On 2011-03-12 06.09, Denny Frost wrote:
 
  I am running MD simulations on Liquid/Liquid interfaces and measuring
  the interfacial tension between them.  I have found that the readings in
  NVT simulations are close to experimental values, but have a lot of
  variation.  I run NPT simulations on the exact same system and find the
  results show very little variation, but the values are far from
  experimental results.  Does anyone know why this happens?
 
  Please be more specific. How do you do NPT simulations? This may
 influence
  the result. To get good result I would suggest to do pressure coupling
 only
  in the normal direction and to turn off dispersion corrections to the
  pressure.
 
  --
  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
  --
  gmx-users mailing listgmx-users@gromacs.org
  http://lists.gromacs.org/mailman/listinfo/gmx-users
  Please search the archive at
  http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
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 interface
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[gmx-users] trjorder, what and how does es count (amount solvent atoms or molecules)?

2011-03-12 Thread Henri Mone
Dear Gromacs Users,

I'm using trjorder with the following options:

$ trjorder -f systemWithSolv.xtc -n system.atom.ndx -s system.pdb -r
0.35  -nshell system0.35.nshell.xvg

As the first group I select all the atoms of a single TYR residue,
which is part of a larger protein. As the second group I select all
the solvent atoms (TIP3P). For a radius of 3.5 A I observe in most
frames the number 8, the observations range from 0 to even 20. What
does this number mean exactly?
For TIP3P the OH2-H1 and OH2-H2 distance is approx. 1A and the H1 and
H2 distance is approx. 1.6A.  This gives a volume of 4.2A^3 for
TIP3P. A sphere of 3.5A would have a volume of 14.6A^3. As a first
order approximation this would suggest for non buried TYR residue
about 3 to 4 TIP3P molecules which could fit in this sphere. This
differs from the number 8 which trjorder measures.

My questions are:
1. What does trajorder count? Does it count the number of solvent
atoms or of solvent molecules?
2. How does trajorder count? If trajorder counts the amount of
molecules. Is it sufficient that a single atom of the molecules is in
the sphere to be included in the counting or must all atoms of the
molecule be in the sphere to be included in the counting?

Thanks,
Henri
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Re: [gmx-users] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread David van der Spoel

On 2011-03-12 16.45, Denny Frost wrote:

I have run NPT simulations using isotropic and semiisotropic coupling
with the same results.  I have never done coupling in just one direction
though, how do you do this?.  I have never used Dispersion corrections.
It seems to me that this would help, rather than hurt though since, as
Aldi said, it will make the system closer to experimental values.  I
will give this a try and see what happens.  My question still remains -
why do NPT and NVT simulations give such different values for surface
tension?
Denny Frost


You don't give any values so it is hard to judge.
- NVT may have completely wrong pressure
- Dispersion correction assumes a homogeneous system as regards the 
average disperson constant per volume, which you probably do not have. 
E.g. in an ice/water surface dispersion correction may induce melting.


The dispersion correction is *not* to bring your system closer to 
experiment but rather to correct for the use of a cut-off.


- Coupling in one direction: specify e.g.
ref-p = 0 0 1
compressibility = 0 0 4e-5
tau_p = 0 0 5


On Sat, Mar 12, 2011 at 6:40 AM, aldi asmadi aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com wrote:

David,

I have a question that is still related to your reply.  If the bulk
liquid NPT and the interfacial liquid-vapor NVT simulations are
performed using dispersion corrections to the pressure and energy,
while the intefacial liquid-liquid NPAT simulation don't use any
correction, can we say that all results are valid since we don't give
the same treatment for all systems?

In the NPT and NVT calculations, we apply corrections in order to
reduce the discrepancy between the calculated and experimental
properties (say density and surface tension) as small as possible.
Here we have more confidence that our molecules in systems behave
accordingly judging from the macroscopic values we obtain.  Meanwhile,
in the NPAT calculation, we don't use such correction meaning that the
property (say interfacial tension) is expected to deviate more from
the experimental value? This indicates that the system behaves
differently in comparison to the same simulation conducted with
correction?

Many thanks,
Aldi


On Sat, Mar 12, 2011 at 11:44 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:
  On 2011-03-12 06.09, Denny Frost wrote:
 
  I am running MD simulations on Liquid/Liquid interfaces and
measuring
  the interfacial tension between them.  I have found that the
readings in
  NVT simulations are close to experimental values, but have a lot of
  variation.  I run NPT simulations on the exact same system and
find the
  results show very little variation, but the values are far from
  experimental results.  Does anyone know why this happens?
 
  Please be more specific. How do you do NPT simulations? This may
influence
  the result. To get good result I would suggest to do pressure
coupling only
  in the normal direction and to turn off dispersion corrections to the
  pressure.
 
  --
  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.se mailto:sp...@xray.bmc.uu.se
http://folding.bmc.uu.se
  --
  gmx-users mailing list gmx-users@gromacs.org
mailto:gmx-users@gromacs.org
  http://lists.gromacs.org/mailman/listinfo/gmx-users
  Please search the archive at
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--
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] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread Denny Frost
Is that using anisotropic pressure coupling?

On Sat, Mar 12, 2011 at 8:55 AM, David van der Spoel
sp...@xray.bmc.uu.sewrote:

 On 2011-03-12 16.45, Denny Frost wrote:

 I have run NPT simulations using isotropic and semiisotropic coupling
 with the same results.  I have never done coupling in just one direction
 though, how do you do this?.  I have never used Dispersion corrections.
 It seems to me that this would help, rather than hurt though since, as
 Aldi said, it will make the system closer to experimental values.  I
 will give this a try and see what happens.  My question still remains -
 why do NPT and NVT simulations give such different values for surface
 tension?
 Denny Frost


 You don't give any values so it is hard to judge.
 - NVT may have completely wrong pressure
 - Dispersion correction assumes a homogeneous system as regards the average
 disperson constant per volume, which you probably do not have. E.g. in an
 ice/water surface dispersion correction may induce melting.

 The dispersion correction is *not* to bring your system closer to
 experiment but rather to correct for the use of a cut-off.

 - Coupling in one direction: specify e.g.
 ref-p = 0 0 1
 compressibility = 0 0 4e-5
 tau_p = 0 0 5


 On Sat, Mar 12, 2011 at 6:40 AM, aldi asmadi aldi.asm...@gmail.com
 mailto:aldi.asm...@gmail.com wrote:

David,

I have a question that is still related to your reply.  If the bulk
liquid NPT and the interfacial liquid-vapor NVT simulations are
performed using dispersion corrections to the pressure and energy,
while the intefacial liquid-liquid NPAT simulation don't use any
correction, can we say that all results are valid since we don't give
the same treatment for all systems?

In the NPT and NVT calculations, we apply corrections in order to
reduce the discrepancy between the calculated and experimental
properties (say density and surface tension) as small as possible.
Here we have more confidence that our molecules in systems behave
accordingly judging from the macroscopic values we obtain.  Meanwhile,
in the NPAT calculation, we don't use such correction meaning that the
property (say interfacial tension) is expected to deviate more from
the experimental value? This indicates that the system behaves
differently in comparison to the same simulation conducted with
correction?

Many thanks,
Aldi


On Sat, Mar 12, 2011 at 11:44 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:
  On 2011-03-12 06.09, Denny Frost wrote:
 
  I am running MD simulations on Liquid/Liquid interfaces and
measuring
  the interfacial tension between them.  I have found that the
readings in
  NVT simulations are close to experimental values, but have a lot of
  variation.  I run NPT simulations on the exact same system and
find the
  results show very little variation, but the values are far from
  experimental results.  Does anyone know why this happens?
 
  Please be more specific. How do you do NPT simulations? This may
influence
  the result. To get good result I would suggest to do pressure
coupling only
  in the normal direction and to turn off dispersion corrections to
 the
  pressure.
 
  --
  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.se mailto:sp...@xray.bmc.uu.se

http://folding.bmc.uu.se
  --
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mailto:gmx-users@gromacs.org

  http://lists.gromacs.org/mailman/listinfo/gmx-users
  Please search the archive at
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 --
 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
 --
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at
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Re: [gmx-users] trjorder, what and how does es count (amount solvent atoms or molecules)?

2011-03-12 Thread Justin A. Lemkul



Henri Mone wrote:

Dear Gromacs Users,

I'm using trjorder with the following options:

$ trjorder -f systemWithSolv.xtc -n system.atom.ndx -s system.pdb -r
0.35  -nshell system0.35.nshell.xvg

As the first group I select all the atoms of a single TYR residue,
which is part of a larger protein. As the second group I select all
the solvent atoms (TIP3P). For a radius of 3.5 A I observe in most
frames the number 8, the observations range from 0 to even 20. What
does this number mean exactly?
For TIP3P the OH2-H1 and OH2-H2 distance is approx. 1A and the H1 and
H2 distance is approx. 1.6A.  This gives a volume of 4.2A^3 for
TIP3P. A sphere of 3.5A would have a volume of 14.6A^3. As a first
order approximation this would suggest for non buried TYR residue
about 3 to 4 TIP3P molecules which could fit in this sphere. This
differs from the number 8 which trjorder measures.

My questions are:
1. What does trajorder count? Does it count the number of solvent
atoms or of solvent molecules?


trjorder -h:

With option -nshell the number of molecules within a shell of radius -r
around the reference group are printed.


2. How does trajorder count? If trajorder counts the amount of
molecules. Is it sufficient that a single atom of the molecules is in
the sphere to be included in the counting or must all atoms of the
molecule be in the sphere to be included in the counting?



Check the code.  If nothing else, your approximation is off.  Would a sphere of 
0.35 nm completely encompass your whole Tyr residue?  The distance are 
presumably based on a radius of 0.35 nm of each of the constituent atoms, making 
for a somewhat larger effective volume.


-Justin


Thanks,
Henri


--


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] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread David van der Spoel

On 2011-03-12 16.59, Denny Frost wrote:

Is that using anisotropic pressure coupling?


yes.
just try it


On Sat, Mar 12, 2011 at 8:55 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:

On 2011-03-12 16.45, Denny Frost wrote:

I have run NPT simulations using isotropic and semiisotropic
coupling
with the same results.  I have never done coupling in just one
direction
though, how do you do this?.  I have never used Dispersion
corrections.
It seems to me that this would help, rather than hurt though
since, as
Aldi said, it will make the system closer to experimental values.  I
will give this a try and see what happens.  My question still
remains -
why do NPT and NVT simulations give such different values for
surface
tension?
Denny Frost


You don't give any values so it is hard to judge.
- NVT may have completely wrong pressure
- Dispersion correction assumes a homogeneous system as regards the
average disperson constant per volume, which you probably do not
have. E.g. in an ice/water surface dispersion correction may induce
melting.

The dispersion correction is *not* to bring your system closer to
experiment but rather to correct for the use of a cut-off.

- Coupling in one direction: specify e.g.
ref-p = 0 0 1
compressibility = 0 0 4e-5
tau_p = 0 0 5


On Sat, Mar 12, 2011 at 6:40 AM, aldi asmadi
aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
wrote:

David,

I have a question that is still related to your reply.  If
the bulk
liquid NPT and the interfacial liquid-vapor NVT simulations are
performed using dispersion corrections to the pressure and
energy,
while the intefacial liquid-liquid NPAT simulation don't use any
correction, can we say that all results are valid since we
don't give
the same treatment for all systems?

In the NPT and NVT calculations, we apply corrections in
order to
reduce the discrepancy between the calculated and experimental
properties (say density and surface tension) as small as
possible.
Here we have more confidence that our molecules in systems
behave
accordingly judging from the macroscopic values we obtain.
  Meanwhile,
in the NPAT calculation, we don't use such correction
meaning that the
property (say interfacial tension) is expected to deviate
more from
the experimental value? This indicates that the system behaves
differently in comparison to the same simulation conducted with
correction?

Many thanks,
Aldi


On Sat, Mar 12, 2011 at 11:44 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se
mailto:sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:
  On 2011-03-12 06.09, Denny Frost wrote:
 
  I am running MD simulations on Liquid/Liquid interfaces and
measuring
  the interfacial tension between them.  I have found that the
readings in
  NVT simulations are close to experimental values, but have a
lot of
  variation.  I run NPT simulations on the exact same system and
find the
  results show very little variation, but the values are far from
  experimental results.  Does anyone know why this happens?
 
  Please be more specific. How do you do NPT simulations? This may
influence
  the result. To get good result I would suggest to do pressure
coupling only
  in the normal direction and to turn off dispersion
corrections to the
  pressure.
 
  --
  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.se mailto:sp...@xray.bmc.uu.se
mailto:sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se

http://folding.bmc.uu.se
  --
  gmx-users mailing list gmx-users@gromacs.org
mailto:gmx-users@gromacs.org
mailto:gmx-users@gromacs.org mailto:gmx-users@gromacs.org

  http://lists.gromacs.org/mailman/listinfo/gmx-users
  Please search the archive at
  http://www.gromacs.org/Support/Mailing_Lists/Search before
posting!
  Please don't post (un)subscribe requests to the list. Use the www
interface
  or send it to gmx-users-requ...@gromacs.org
mailto:gmx-users-requ...@gromacs.org

Re: [gmx-users] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread Denny Frost
Thanks for answering that question about dispersion, that makes sense.
Also, The values I currently get with NPT are around 58 mN/m, while the
average values I get for NVT are around 16 mN/m, but with a variance of
nearly 100% of that value.  I'm beginning to see why you only do pressure
coupling in the z direction, but gromacs 4.5.3 won't let you specify tau_p =
0.  Any other way to do pressure coupling in just the z direction?
Denny

On Sat, Mar 12, 2011 at 8:59 AM, Denny Frost dsfr...@cableone.net wrote:

 Is that using anisotropic pressure coupling?


 On Sat, Mar 12, 2011 at 8:55 AM, David van der Spoel sp...@xray.bmc.uu.se
  wrote:

 On 2011-03-12 16.45, Denny Frost wrote:

 I have run NPT simulations using isotropic and semiisotropic coupling
 with the same results.  I have never done coupling in just one direction
 though, how do you do this?.  I have never used Dispersion corrections.
 It seems to me that this would help, rather than hurt though since, as
 Aldi said, it will make the system closer to experimental values.  I
 will give this a try and see what happens.  My question still remains -
 why do NPT and NVT simulations give such different values for surface
 tension?
 Denny Frost


 You don't give any values so it is hard to judge.
 - NVT may have completely wrong pressure
 - Dispersion correction assumes a homogeneous system as regards the
 average disperson constant per volume, which you probably do not have. E.g.
 in an ice/water surface dispersion correction may induce melting.

 The dispersion correction is *not* to bring your system closer to
 experiment but rather to correct for the use of a cut-off.

 - Coupling in one direction: specify e.g.
 ref-p = 0 0 1
 compressibility = 0 0 4e-5
 tau_p = 0 0 5


 On Sat, Mar 12, 2011 at 6:40 AM, aldi asmadi aldi.asm...@gmail.com
 mailto:aldi.asm...@gmail.com wrote:

David,

I have a question that is still related to your reply.  If the bulk
liquid NPT and the interfacial liquid-vapor NVT simulations are
performed using dispersion corrections to the pressure and energy,
while the intefacial liquid-liquid NPAT simulation don't use any
correction, can we say that all results are valid since we don't give
the same treatment for all systems?

In the NPT and NVT calculations, we apply corrections in order to
reduce the discrepancy between the calculated and experimental
properties (say density and surface tension) as small as possible.
Here we have more confidence that our molecules in systems behave
accordingly judging from the macroscopic values we obtain.  Meanwhile,
in the NPAT calculation, we don't use such correction meaning that the
property (say interfacial tension) is expected to deviate more from
the experimental value? This indicates that the system behaves
differently in comparison to the same simulation conducted with
correction?

Many thanks,
Aldi


On Sat, Mar 12, 2011 at 11:44 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:
  On 2011-03-12 06.09, Denny Frost wrote:
 
  I am running MD simulations on Liquid/Liquid interfaces and
measuring
  the interfacial tension between them.  I have found that the
readings in
  NVT simulations are close to experimental values, but have a lot
 of
  variation.  I run NPT simulations on the exact same system and
find the
  results show very little variation, but the values are far from
  experimental results.  Does anyone know why this happens?
 
  Please be more specific. How do you do NPT simulations? This may
influence
  the result. To get good result I would suggest to do pressure
coupling only
  in the normal direction and to turn off dispersion corrections to
 the
  pressure.
 
  --
  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.se mailto:sp...@xray.bmc.uu.se

http://folding.bmc.uu.se
  --
  gmx-users mailing list gmx-users@gromacs.org
mailto:gmx-users@gromacs.org

  http://lists.gromacs.org/mailman/listinfo/gmx-users
  Please search the archive at
  http://www.gromacs.org/Support/Mailing_Lists/Search before
 posting!
  Please don't post (un)subscribe requests to the list. Use the www
interface
  or send it to gmx-users-requ...@gromacs.org
mailto:gmx-users-requ...@gromacs.org.

  Can't post? Read http://www.gromacs.org/Support/Mailing_Lists
 
--
gmx-users mailing list gmx-users@gromacs.org
mailto:gmx-users@gromacs.org

http://lists.gromacs.org/mailman/listinfo/gmx-users
Please search the archive at
http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
Please don't post (un)subscribe requests to the list. Use the
www interface or send it to 

Re: [gmx-users] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread David van der Spoel

On 2011-03-12 17.17, Denny Frost wrote:

Thanks for answering that question about dispersion, that makes sense.
Also, The values I currently get with NPT are around 58 mN/m, while the
average values I get for NVT are around 16 mN/m, but with a variance of
nearly 100% of that value.  I'm beginning to see why you only do
pressure coupling in the z direction, but gromacs 4.5.3 won't let you
specify tau_p = 0.  Any other way to do pressure coupling in just the z
direction?

check manual.
maybe there is only one tau_p value.

Denny

On Sat, Mar 12, 2011 at 8:59 AM, Denny Frost dsfr...@cableone.net
mailto:dsfr...@cableone.net wrote:

Is that using anisotropic pressure coupling?


On Sat, Mar 12, 2011 at 8:55 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:

On 2011-03-12 16.45, Denny Frost wrote:

I have run NPT simulations using isotropic and semiisotropic
coupling
with the same results.  I have never done coupling in just
one direction
though, how do you do this?.  I have never used Dispersion
corrections.
It seems to me that this would help, rather than hurt though
since, as
Aldi said, it will make the system closer to experimental
values.  I
will give this a try and see what happens.  My question
still remains -
why do NPT and NVT simulations give such different values
for surface
tension?
Denny Frost


You don't give any values so it is hard to judge.
- NVT may have completely wrong pressure
- Dispersion correction assumes a homogeneous system as regards
the average disperson constant per volume, which you probably do
not have. E.g. in an ice/water surface dispersion correction may
induce melting.

The dispersion correction is *not* to bring your system closer
to experiment but rather to correct for the use of a cut-off.

- Coupling in one direction: specify e.g.
ref-p = 0 0 1
compressibility = 0 0 4e-5
tau_p = 0 0 5


On Sat, Mar 12, 2011 at 6:40 AM, aldi asmadi
aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com wrote:

David,

I have a question that is still related to your reply.
  If the bulk
liquid NPT and the interfacial liquid-vapor NVT
simulations are
performed using dispersion corrections to the pressure
and energy,
while the intefacial liquid-liquid NPAT simulation don't
use any
correction, can we say that all results are valid since
we don't give
the same treatment for all systems?

In the NPT and NVT calculations, we apply corrections in
order to
reduce the discrepancy between the calculated and
experimental
properties (say density and surface tension) as small as
possible.
Here we have more confidence that our molecules in
systems behave
accordingly judging from the macroscopic values we
obtain.  Meanwhile,
in the NPAT calculation, we don't use such correction
meaning that the
property (say interfacial tension) is expected to
deviate more from
the experimental value? This indicates that the system
behaves
differently in comparison to the same simulation
conducted with
correction?

Many thanks,
Aldi


On Sat, Mar 12, 2011 at 11:44 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se
mailto:sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se
wrote:
  On 2011-03-12 06.09, Denny Frost wrote:
 
  I am running MD simulations on Liquid/Liquid interfaces and
measuring
  the interfacial tension between them.  I have found that the
readings in
  NVT simulations are close to experimental values, but
have a lot of
  variation.  I run NPT simulations on the exact same
system and
find the
  results show very little variation, but the values are
far from
  experimental results.  Does anyone know why this happens?
 
  Please be more specific. How do you do NPT simulations?
This may
influence
  the result. To get good result I would suggest to do pressure
coupling only
  in 

Re: [gmx-users] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread Denny Frost
No, it requires six, acutally, for aniisotropic coupling.  I decided to use
semi-isotropic coupling with the xy compressibilities set to 4.5e-15 (it
won't accept 0).  This should keep the walls parallel to the z axis from
moving and accomplish the same thing.  Does this sound right?

On Sat, Mar 12, 2011 at 9:24 AM, David van der Spoel
sp...@xray.bmc.uu.sewrote:

 On 2011-03-12 17.17, Denny Frost wrote:

 Thanks for answering that question about dispersion, that makes sense.
 Also, The values I currently get with NPT are around 58 mN/m, while the
 average values I get for NVT are around 16 mN/m, but with a variance of
 nearly 100% of that value.  I'm beginning to see why you only do
 pressure coupling in the z direction, but gromacs 4.5.3 won't let you
 specify tau_p = 0.  Any other way to do pressure coupling in just the z
 direction?

 check manual.
 maybe there is only one tau_p value.

 Denny

 On Sat, Mar 12, 2011 at 8:59 AM, Denny Frost dsfr...@cableone.net
 mailto:dsfr...@cableone.net wrote:

Is that using anisotropic pressure coupling?


On Sat, Mar 12, 2011 at 8:55 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:

On 2011-03-12 16.45, Denny Frost wrote:

I have run NPT simulations using isotropic and semiisotropic
coupling
with the same results.  I have never done coupling in just
one direction
though, how do you do this?.  I have never used Dispersion
corrections.
It seems to me that this would help, rather than hurt though
since, as
Aldi said, it will make the system closer to experimental
values.  I
will give this a try and see what happens.  My question
still remains -
why do NPT and NVT simulations give such different values
for surface
tension?
Denny Frost


You don't give any values so it is hard to judge.
- NVT may have completely wrong pressure
- Dispersion correction assumes a homogeneous system as regards
the average disperson constant per volume, which you probably do
not have. E.g. in an ice/water surface dispersion correction may
induce melting.

The dispersion correction is *not* to bring your system closer
to experiment but rather to correct for the use of a cut-off.

- Coupling in one direction: specify e.g.
ref-p = 0 0 1
compressibility = 0 0 4e-5
tau_p = 0 0 5


On Sat, Mar 12, 2011 at 6:40 AM, aldi asmadi
aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com wrote:

David,

I have a question that is still related to your reply.
  If the bulk
liquid NPT and the interfacial liquid-vapor NVT
simulations are
performed using dispersion corrections to the pressure
and energy,
while the intefacial liquid-liquid NPAT simulation don't
use any
correction, can we say that all results are valid since
we don't give
the same treatment for all systems?

In the NPT and NVT calculations, we apply corrections in
order to
reduce the discrepancy between the calculated and
experimental
properties (say density and surface tension) as small as
possible.
Here we have more confidence that our molecules in
systems behave
accordingly judging from the macroscopic values we
obtain.  Meanwhile,
in the NPAT calculation, we don't use such correction
meaning that the
property (say interfacial tension) is expected to
deviate more from
the experimental value? This indicates that the system
behaves
differently in comparison to the same simulation
conducted with
correction?

Many thanks,
Aldi


On Sat, Mar 12, 2011 at 11:44 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se
mailto:sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se

wrote:
  On 2011-03-12 06.09, Denny Frost wrote:
 
  I am running MD simulations on Liquid/Liquid interfaces and
measuring
  the interfacial tension between them.  I have found that
 the
readings in
  NVT simulations are close to experimental values, but
have a lot of
  variation.  I run NPT simulations on the exact same
system and
find the
  results show very 

Re: [gmx-users] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread David van der Spoel

On 2011-03-12 17.28, Denny Frost wrote:

No, it requires six, acutally, for aniisotropic coupling.  I decided to
use semi-isotropic coupling with the xy compressibilities set to 4.5e-15
(it won't accept 0).  This should keep the walls parallel to the z axis
from moving and accomplish the same thing.  Does this sound right?

with semiisotropic you need only two values, with anisotropic either 3 
or 6 values. Zero compressibility should work.

On Sat, Mar 12, 2011 at 9:24 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:

On 2011-03-12 17.17, Denny Frost wrote:

Thanks for answering that question about dispersion, that makes
sense.
Also, The values I currently get with NPT are around 58 mN/m,
while the
average values I get for NVT are around 16 mN/m, but with a
variance of
nearly 100% of that value.  I'm beginning to see why you only do
pressure coupling in the z direction, but gromacs 4.5.3 won't
let you
specify tau_p = 0.  Any other way to do pressure coupling in
just the z
direction?

check manual.
maybe there is only one tau_p value.

Denny

On Sat, Mar 12, 2011 at 8:59 AM, Denny Frost
dsfr...@cableone.net mailto:dsfr...@cableone.net
mailto:dsfr...@cableone.net mailto:dsfr...@cableone.net wrote:

Is that using anisotropic pressure coupling?


On Sat, Mar 12, 2011 at 8:55 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se
mailto:sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:

On 2011-03-12 16.45, Denny Frost wrote:

I have run NPT simulations using isotropic and
semiisotropic
coupling
with the same results.  I have never done coupling
in just
one direction
though, how do you do this?.  I have never used
Dispersion
corrections.
It seems to me that this would help, rather than
hurt though
since, as
Aldi said, it will make the system closer to
experimental
values.  I
will give this a try and see what happens.  My question
still remains -
why do NPT and NVT simulations give such different
values
for surface
tension?
Denny Frost


You don't give any values so it is hard to judge.
- NVT may have completely wrong pressure
- Dispersion correction assumes a homogeneous system as
regards
the average disperson constant per volume, which you
probably do
not have. E.g. in an ice/water surface dispersion
correction may
induce melting.

The dispersion correction is *not* to bring your system
closer
to experiment but rather to correct for the use of a
cut-off.

- Coupling in one direction: specify e.g.
ref-p = 0 0 1
compressibility = 0 0 4e-5
tau_p = 0 0 5


On Sat, Mar 12, 2011 at 6:40 AM, aldi asmadi
aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
wrote:

David,

I have a question that is still related to your
reply.
  If the bulk
liquid NPT and the interfacial liquid-vapor NVT
simulations are
performed using dispersion corrections to the
pressure
and energy,
while the intefacial liquid-liquid NPAT
simulation don't
use any
correction, can we say that all results are
valid since
we don't give
the same treatment for all systems?

In the NPT and NVT calculations, we apply
corrections in
order to
reduce the discrepancy between the calculated and
experimental
properties (say density and surface tension) as
small as
possible.
Here we have more confidence that our molecules in
systems behave
accordingly judging from the macroscopic values we
obtain.  Meanwhile,
in the NPAT calculation, we don't use 

Re: [gmx-users] Surface tension readings in NVT vs NPT simulations

2011-03-12 Thread Denny Frost
It won't take zero with the berendsen thermostat, but I only wish to do weak
coupling for now.  Yes, I only specified the two values for semiisotropic.
What I'm asking is will this setup only do z-pressure coupling?

On Sat, Mar 12, 2011 at 9:32 AM, David van der Spoel
sp...@xray.bmc.uu.sewrote:

 On 2011-03-12 17.28, Denny Frost wrote:

 No, it requires six, acutally, for aniisotropic coupling.  I decided to
 use semi-isotropic coupling with the xy compressibilities set to 4.5e-15
 (it won't accept 0).  This should keep the walls parallel to the z axis
 from moving and accomplish the same thing.  Does this sound right?

  with semiisotropic you need only two values, with anisotropic either 3 or
 6 values. Zero compressibility should work.

 On Sat, Mar 12, 2011 at 9:24 AM, David van der Spoel
 sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se wrote:

On 2011-03-12 17.17, Denny Frost wrote:

Thanks for answering that question about dispersion, that makes
sense.
Also, The values I currently get with NPT are around 58 mN/m,
while the
average values I get for NVT are around 16 mN/m, but with a
variance of
nearly 100% of that value.  I'm beginning to see why you only do
pressure coupling in the z direction, but gromacs 4.5.3 won't
let you
specify tau_p = 0.  Any other way to do pressure coupling in
just the z
direction?

check manual.
maybe there is only one tau_p value.

Denny

On Sat, Mar 12, 2011 at 8:59 AM, Denny Frost
dsfr...@cableone.net mailto:dsfr...@cableone.net
mailto:dsfr...@cableone.net mailto:dsfr...@cableone.net
 wrote:

Is that using anisotropic pressure coupling?


On Sat, Mar 12, 2011 at 8:55 AM, David van der Spoel
sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se
mailto:sp...@xray.bmc.uu.se mailto:sp...@xray.bmc.uu.se
 wrote:

On 2011-03-12 16.45, Denny Frost wrote:

I have run NPT simulations using isotropic and
semiisotropic
coupling
with the same results.  I have never done coupling
in just
one direction
though, how do you do this?.  I have never used
Dispersion
corrections.
It seems to me that this would help, rather than
hurt though
since, as
Aldi said, it will make the system closer to
experimental
values.  I
will give this a try and see what happens.  My question
still remains -
why do NPT and NVT simulations give such different
values
for surface
tension?
Denny Frost


You don't give any values so it is hard to judge.
- NVT may have completely wrong pressure
- Dispersion correction assumes a homogeneous system as
regards
the average disperson constant per volume, which you
probably do
not have. E.g. in an ice/water surface dispersion
correction may
induce melting.

The dispersion correction is *not* to bring your system
closer
to experiment but rather to correct for the use of a
cut-off.

- Coupling in one direction: specify e.g.
ref-p = 0 0 1
compressibility = 0 0 4e-5
tau_p = 0 0 5


On Sat, Mar 12, 2011 at 6:40 AM, aldi asmadi
aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com
mailto:aldi.asm...@gmail.com mailto:aldi.asm...@gmail.com

wrote:

David,

I have a question that is still related to your
reply.
  If the bulk
liquid NPT and the interfacial liquid-vapor NVT
simulations are
performed using dispersion corrections to the
pressure
and energy,
while the intefacial liquid-liquid NPAT
simulation don't
use any
correction, can we say that all results are
valid since
we don't give
the same treatment for all systems?

In the NPT and NVT calculations, we apply
corrections in
order to
reduce the discrepancy between the calculated and
experimental
properties (say density and surface tension) as
small as

RE: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation Fault

2011-03-12 Thread Steve Vivian
Based on a preliminary test using multiple threads, the issue is not
resolved.
This leads me to believe that my Unit Cell is not built properly.

Below is the procedure used to build the unit cell.  I have reviewed it many
times, but I would appreciate any input regarding potential improvements,
specifically on the line using trjconv in the EM/Shrink loop.

Safe up to here, (I hope)...

cat KALP_newbox.gro dppc128_whole.gro  system.gro

update minim.mdp
; Strong position restraints for InflateGRO
#ifdef STRONG_POSRES
#include strong_posre.itp
#endif

Create Strong Position Restraint for protein
genrestr -f KALP_newbox.gro -o strong_posre.itp -fc 10 10 10

Scale Lipid positions by a factor of 4
perl inflategro.pl system.gro 4 DPPC 14 system_inflated.gro 5 area.dat

Begin loop of repeated Energy Minimizations and Shrinking 
(repeat loop approximately 25 times until area is approx 71 Ang sq)
Begin LOOP (from n=1 to n = 26)
grompp -f minim.mdp -c systm_inf_n.gro -p topol.top -o em_n.tpr
mdrun -v -deffnm em_n
trjconv -s em_n.tpr -f em_n.gro -o em_n_out.gro -pbc mol -ur compact
perl inflategro.pl em_n_out.gro 0.95 DPPC 0 sys_shr_1.gro 5
ar_shr1.dat
End LOOP

Add water 
Add ions
Re-run EM
Equilibrate (and watch it all explode)





-Original Message-
From: gmx-users-boun...@gromacs.org [mailto:gmx-users-boun...@gromacs.org]
On Behalf Of Justin A. Lemkul
Sent: Thursday, March 10, 2011 12:56 PM
To: Discussion list for GROMACS users
Subject: Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation
Fault



Steve Vivian wrote:
 On 03/08/2011 10:23 PM, Justin A. Lemkul wrote:


 Steve Vivian wrote:

 New to Gromacs.

 Worked my way through the tutorial with relatively few issues until 
 the Equilibration stage.  My system blows up!!

 Returned to the Topology stage and rebuilt my system ensuring that I 
 followed the procedure correctly for the InflateGro process.  It 
 appears to be correct, reasonable lipid area, no water inside my 
 bilayer, vmd shows a structure which appears normal (although I am 
 new to this).  There are voids between bilayer and water molecules, 
 but this is to be expected, correct?

 Energy Minimization repeatedly produces results within the expected 
 range.

 Again system blows up at equilibration, step 0 segmentation fault.  
 Regardless of whether I attempt the NVT or Anneal_Npt process (using 
 the provided mdp files, including the updates for restraints on the 
 protein and the lipid molecules).

 I have attempted many variations of the nvt.mdp and anneal_npt.mdp 
 files hoping to resolve my issue, but with no success.  I will post 
 the log information from the nvt.mdp file included in the tutorial.

 Started mdrun on node 0 Tue Mar  8 15:42:35 2011

Step   Time Lambda
   00.00.0

 Grid: 9 x 9 x 9 cells
Energies (kJ/mol)
G96AngleProper Dih.  Improper Dih.  
 LJ-14 Coulomb-14
 8.52380e+016.88116e+012.23939e+01   
 -3.03546e+012.71260e+03
 LJ (SR)  Disper. corr.   Coulomb (SR)   
 Coul. recip. Position Rest.
 1.49883e+04   -1.42684e+03   -2.78329e+05   
 -1.58540e+052.57100e+00
   PotentialKinetic En.   Total 
 Energy  Conserved En.   Temperature
-4.20446e+05*1.41436e+141.41436e+14
 1.41436e+141.23343e+12*
  Pres. DC (bar) Pressure (bar)   Constr. rmsd
-1.56331e+025.05645e+121.18070e+01


 As you can see the Potential Energy is reasonable, but the Kinetic 
 Energy and Temperature seem unrealistic.

 I am hoping that this is enough information for a more experienced 
 Gromacs user to provide guidance. Note:  that I have tried all of the 
 suggestions that I read on the mailing list and in the blowing up 
 section of the manual, specifically:
 -reduced time steps in Equilibration Stages
 -reduced Fmax during EM stage (down as low as 100kJ which did not help)
 -modified neighbours list parameters

 Any help is appreciated. I can attach and forward any further 
 information as required, please let me know.


 Which Gromacs version are you using?  It looks like you're running in 
 serial, is that correct?  Otherwise, please provide your mdrun command 
 line.  If you're using version 4.5.3 in serial, I have identified a 
 very problematic bug that seems to affect a wide variety of systems 
 that could be related:

 Yes I am currently using Gromacs 4.5.3 in serial.
 
 http://redmine.gromacs.org/issues/715

 I have seen even the most robust tutorial systems fail as well, as 
 some new lab members experienced the same problem.  The workaround is 
 to run in parallel.

 If I understand you correctly, the recommended workaround is to 
 re-configure gromacs 4.5.3 with mpi enabled and complete the 
 Equilibration and 

Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation Fault

2011-03-12 Thread Justin A. Lemkul



Steve Vivian wrote:

Based on a preliminary test using multiple threads, the issue is not
resolved.
This leads me to believe that my Unit Cell is not built properly.

Below is the procedure used to build the unit cell.  I have reviewed it many
times, but I would appreciate any input regarding potential improvements,
specifically on the line using trjconv in the EM/Shrink loop.

Safe up to here, (I hope)...

cat KALP_newbox.gro dppc128_whole.gro  system.gro

update minim.mdp
; Strong position restraints for InflateGRO
#ifdef STRONG_POSRES
#include strong_posre.itp
#endif

Create Strong Position Restraint for protein
genrestr -f KALP_newbox.gro -o strong_posre.itp -fc 10 10 10

Scale Lipid positions by a factor of 4
perl inflategro.pl system.gro 4 DPPC 14 system_inflated.gro 5 area.dat

Begin loop of repeated Energy Minimizations and Shrinking 
(repeat loop approximately 25 times until area is approx 71 Ang sq)

Begin LOOP (from n=1 to n = 26)
grompp -f minim.mdp -c systm_inf_n.gro -p topol.top -o em_n.tpr
mdrun -v -deffnm em_n
trjconv -s em_n.tpr -f em_n.gro -o em_n_out.gro -pbc mol -ur compact
perl inflategro.pl em_n_out.gro 0.95 DPPC 0 sys_shr_1.gro 5
ar_shr1.dat
End LOOP

Add water 
Add ions

Re-run EM


What is the outcome of EM?

-Justin


Equilibrate (and watch it all explode)





-Original Message-
From: gmx-users-boun...@gromacs.org [mailto:gmx-users-boun...@gromacs.org]
On Behalf Of Justin A. Lemkul
Sent: Thursday, March 10, 2011 12:56 PM
To: Discussion list for GROMACS users
Subject: Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation
Fault



Steve Vivian wrote:

On 03/08/2011 10:23 PM, Justin A. Lemkul wrote:


Steve Vivian wrote:

New to Gromacs.

Worked my way through the tutorial with relatively few issues until 
the Equilibration stage.  My system blows up!!


Returned to the Topology stage and rebuilt my system ensuring that I 
followed the procedure correctly for the InflateGro process.  It 
appears to be correct, reasonable lipid area, no water inside my 
bilayer, vmd shows a structure which appears normal (although I am 
new to this).  There are voids between bilayer and water molecules, 
but this is to be expected, correct?


Energy Minimization repeatedly produces results within the expected 
range.


Again system blows up at equilibration, step 0 segmentation fault.  
Regardless of whether I attempt the NVT or Anneal_Npt process (using 
the provided mdp files, including the updates for restraints on the 
protein and the lipid molecules).


I have attempted many variations of the nvt.mdp and anneal_npt.mdp 
files hoping to resolve my issue, but with no success.  I will post 
the log information from the nvt.mdp file included in the tutorial.


Started mdrun on node 0 Tue Mar  8 15:42:35 2011

   Step   Time Lambda
  00.00.0

Grid: 9 x 9 x 9 cells
   Energies (kJ/mol)
   G96AngleProper Dih.  Improper Dih.  
LJ-14 Coulomb-14
8.52380e+016.88116e+012.23939e+01   
-3.03546e+012.71260e+03
LJ (SR)  Disper. corr.   Coulomb (SR)   
Coul. recip. Position Rest.
1.49883e+04   -1.42684e+03   -2.78329e+05   
-1.58540e+052.57100e+00
  PotentialKinetic En.   Total 
Energy  Conserved En.   Temperature
   -4.20446e+05*1.41436e+141.41436e+14
1.41436e+141.23343e+12*

 Pres. DC (bar) Pressure (bar)   Constr. rmsd
   -1.56331e+025.05645e+121.18070e+01


As you can see the Potential Energy is reasonable, but the Kinetic 
Energy and Temperature seem unrealistic.


I am hoping that this is enough information for a more experienced 
Gromacs user to provide guidance. Note:  that I have tried all of the 
suggestions that I read on the mailing list and in the blowing up 
section of the manual, specifically:

-reduced time steps in Equilibration Stages
-reduced Fmax during EM stage (down as low as 100kJ which did not help)
-modified neighbours list parameters

Any help is appreciated. I can attach and forward any further 
information as required, please let me know.


Which Gromacs version are you using?  It looks like you're running in 
serial, is that correct?  Otherwise, please provide your mdrun command 
line.  If you're using version 4.5.3 in serial, I have identified a 
very problematic bug that seems to affect a wide variety of systems 
that could be related:



Yes I am currently using Gromacs 4.5.3 in serial.


http://redmine.gromacs.org/issues/715

I have seen even the most robust tutorial systems fail as well, as 
some new lab members experienced the same problem.  The workaround is 
to run in parallel.


If I understand you correctly, the recommended workaround is to 
re-configure gromacs 4.5.3 with mpi enabled and complete the 

Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation Fault

2011-03-12 Thread Justin A. Lemkul



Steve Vivian wrote:

Based on a preliminary test using multiple threads, the issue is not
resolved.
This leads me to believe that my Unit Cell is not built properly.

Below is the procedure used to build the unit cell.  I have reviewed it many
times, but I would appreciate any input regarding potential improvements,
specifically on the line using trjconv in the EM/Shrink loop.

Safe up to here, (I hope)...

cat KALP_newbox.gro dppc128_whole.gro  system.gro

update minim.mdp
; Strong position restraints for InflateGRO
#ifdef STRONG_POSRES
#include strong_posre.itp
#endif

Create Strong Position Restraint for protein
genrestr -f KALP_newbox.gro -o strong_posre.itp -fc 10 10 10

Scale Lipid positions by a factor of 4
perl inflategro.pl system.gro 4 DPPC 14 system_inflated.gro 5 area.dat

Begin loop of repeated Energy Minimizations and Shrinking 
(repeat loop approximately 25 times until area is approx 71 Ang sq)

Begin LOOP (from n=1 to n = 26)
grompp -f minim.mdp -c systm_inf_n.gro -p topol.top -o em_n.tpr
mdrun -v -deffnm em_n
trjconv -s em_n.tpr -f em_n.gro -o em_n_out.gro -pbc mol -ur compact
perl inflategro.pl em_n_out.gro 0.95 DPPC 0 sys_shr_1.gro 5


One problem here: you start the loop every time with system_inf_n?  What is 
system_inf_n?  It seems that you should start one (non-loop) shrink and then 
process the subsequent shrinking steps from there.  At the end of the loop, you 
write to sys_shr_1.gro, which then never gets used again.


-Justin


ar_shr1.dat
End LOOP

Add water 
Add ions

Re-run EM
Equilibrate (and watch it all explode)





-Original Message-
From: gmx-users-boun...@gromacs.org [mailto:gmx-users-boun...@gromacs.org]
On Behalf Of Justin A. Lemkul
Sent: Thursday, March 10, 2011 12:56 PM
To: Discussion list for GROMACS users
Subject: Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation
Fault



Steve Vivian wrote:

On 03/08/2011 10:23 PM, Justin A. Lemkul wrote:


Steve Vivian wrote:

New to Gromacs.

Worked my way through the tutorial with relatively few issues until 
the Equilibration stage.  My system blows up!!


Returned to the Topology stage and rebuilt my system ensuring that I 
followed the procedure correctly for the InflateGro process.  It 
appears to be correct, reasonable lipid area, no water inside my 
bilayer, vmd shows a structure which appears normal (although I am 
new to this).  There are voids between bilayer and water molecules, 
but this is to be expected, correct?


Energy Minimization repeatedly produces results within the expected 
range.


Again system blows up at equilibration, step 0 segmentation fault.  
Regardless of whether I attempt the NVT or Anneal_Npt process (using 
the provided mdp files, including the updates for restraints on the 
protein and the lipid molecules).


I have attempted many variations of the nvt.mdp and anneal_npt.mdp 
files hoping to resolve my issue, but with no success.  I will post 
the log information from the nvt.mdp file included in the tutorial.


Started mdrun on node 0 Tue Mar  8 15:42:35 2011

   Step   Time Lambda
  00.00.0

Grid: 9 x 9 x 9 cells
   Energies (kJ/mol)
   G96AngleProper Dih.  Improper Dih.  
LJ-14 Coulomb-14
8.52380e+016.88116e+012.23939e+01   
-3.03546e+012.71260e+03
LJ (SR)  Disper. corr.   Coulomb (SR)   
Coul. recip. Position Rest.
1.49883e+04   -1.42684e+03   -2.78329e+05   
-1.58540e+052.57100e+00
  PotentialKinetic En.   Total 
Energy  Conserved En.   Temperature
   -4.20446e+05*1.41436e+141.41436e+14
1.41436e+141.23343e+12*

 Pres. DC (bar) Pressure (bar)   Constr. rmsd
   -1.56331e+025.05645e+121.18070e+01


As you can see the Potential Energy is reasonable, but the Kinetic 
Energy and Temperature seem unrealistic.


I am hoping that this is enough information for a more experienced 
Gromacs user to provide guidance. Note:  that I have tried all of the 
suggestions that I read on the mailing list and in the blowing up 
section of the manual, specifically:

-reduced time steps in Equilibration Stages
-reduced Fmax during EM stage (down as low as 100kJ which did not help)
-modified neighbours list parameters

Any help is appreciated. I can attach and forward any further 
information as required, please let me know.


Which Gromacs version are you using?  It looks like you're running in 
serial, is that correct?  Otherwise, please provide your mdrun command 
line.  If you're using version 4.5.3 in serial, I have identified a 
very problematic bug that seems to affect a wide variety of systems 
that could be related:



Yes I am currently using Gromacs 4.5.3 in serial.


http://redmine.gromacs.org/issues/715

I have seen even the most 

Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation Fault

2011-03-12 Thread Steve Vivian

On 03/12/2011 12:51 PM, Justin A. Lemkul wrote:
Getting hard to follow, so I put my new comments in blue.
Output from Energy Minimization

Steepest Descents converged to Fmax  1000 in 1814 steps
Potential Energy  = -3.81270276926664e+05
Maximum force =  9.38712770623942e+02 on atom 2292
Norm of force =  2.88274347161761e+01





Steve Vivian wrote:

Based on a preliminary test using multiple threads, the issue is not
resolved.
This leads me to believe that my Unit Cell is not built properly.

Below is the procedure used to build the unit cell.  I have reviewed 
it many
times, but I would appreciate any input regarding potential 
improvements,

specifically on the line using trjconv in the EM/Shrink loop.

Safe up to here, (I hope)...

cat KALP_newbox.gro dppc128_whole.gro  system.gro

update minim.mdp
; Strong position restraints for InflateGRO
#ifdef STRONG_POSRES
#include strong_posre.itp
#endif

Create Strong Position Restraint for protein
genrestr -f KALP_newbox.gro -o strong_posre.itp -fc 10 10 10

Scale Lipid positions by a factor of 4
perl inflategro.pl system.gro 4 DPPC 14 system_inflated.gro 5 area.dat

Begin loop of repeated Energy Minimizations and Shrinking (repeat 
loop approximately 25 times until area is approx 71 Ang sq)

Begin LOOP (from n=1 to n = 26)
grompp -f minim.mdp -c systm_inf_n.gro -p topol.top -o em_n.tpr
mdrun -v -deffnm em_n
trjconv -s em_n.tpr -f em_n.gro -o em_n_out.gro -pbc mol -ur compact
perl inflategro.pl em_n_out.gro 0.95 DPPC 0 sys_shr_1.gro 5


One problem here: you start the loop every time with system_inf_n?  
What is system_inf_n?  It seems that you should start one (non-loop) 
shrink and then process the subsequent shrinking steps from there.  At 
the end of the loop, you write to sys_shr_1.gro, which then never gets 
used again.


-Justin

Put my comments in blue to make it easier to read.

I apologize for the poor description here.
The first loop begins with the System_inflate.gro file created in the 
earlier process.  The rest of the first loop is shown.


At the beginning of the second loop, the input file is 
system_shrink_1.gro, which was the output file at the end of loop 1.  
Proceed through the loop, updating the n from 1 to 2 in each step.  
Output file is system_shrink_2.gro.


Input file for loop 3 is system_shrink_3.gro, 

Output from loop 26 is system_shrink_26.gro and output on screen 
provides information on updated Lipid area which has achieved target value.


Then proceed to add water (after changing vdw radius of C atoms)
Add ions
EM again
Then Equilibrate.


Output from Energy Minimization (after addition of water and ions)

Steepest Descents converged to Fmax  1000 in 1814 steps
Potential Energy  = -3.81270276926664e+05
Maximum force =  9.38712770623942e+02 on atom 2292
Norm of force =  2.88274347161761e+01






ar_shr1.dat
End LOOP

Add water Add ions
Re-run EM
Equilibrate (and watch it all explode)





-Original Message-
From: gmx-users-boun...@gromacs.org 
[mailto:gmx-users-boun...@gromacs.org]

On Behalf Of Justin A. Lemkul
Sent: Thursday, March 10, 2011 12:56 PM
To: Discussion list for GROMACS users
Subject: Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 
Segmentation

Fault



Steve Vivian wrote:

On 03/08/2011 10:23 PM, Justin A. Lemkul wrote:


Steve Vivian wrote:

New to Gromacs.

Worked my way through the tutorial with relatively few issues 
until the Equilibration stage.  My system blows up!!


Returned to the Topology stage and rebuilt my system ensuring that 
I followed the procedure correctly for the InflateGro process.  It 
appears to be correct, reasonable lipid area, no water inside my 
bilayer, vmd shows a structure which appears normal (although I am 
new to this).  There are voids between bilayer and water 
molecules, but this is to be expected, correct?


Energy Minimization repeatedly produces results within the 
expected range.


Again system blows up at equilibration, step 0 segmentation 
fault.  Regardless of whether I attempt the NVT or Anneal_Npt 
process (using the provided mdp files, including the updates for 
restraints on the protein and the lipid molecules).


I have attempted many variations of the nvt.mdp and anneal_npt.mdp 
files hoping to resolve my issue, but with no success.  I will 
post the log information from the nvt.mdp file included in the 
tutorial.


Started mdrun on node 0 Tue Mar  8 15:42:35 2011

   Step   Time Lambda
  00.00.0

Grid: 9 x 9 x 9 cells
   Energies (kJ/mol)
   G96AngleProper Dih.  Improper Dih.  
LJ-14 Coulomb-14
8.52380e+016.88116e+012.23939e+01   
-3.03546e+012.71260e+03
LJ (SR)  Disper. corr.   Coulomb 
(SR)   Coul. recip. Position Rest.
1.49883e+04   -1.42684e+03   -2.78329e+05   
-1.58540e+052.57100e+00
  Potential   

Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation Fault

2011-03-12 Thread Justin A. Lemkul



Steve Vivian wrote:

  On 03/12/2011 12:51 PM, Justin A. Lemkul wrote:
Getting hard to follow, so I put my new comments in blue.
Output from Energy Minimization

Steepest Descents converged to Fmax  1000 in 1814 steps
Potential Energy  = -3.81270276926664e+05
Maximum force =  9.38712770623942e+02 on atom 2292
Norm of force =  2.88274347161761e+01





Steve Vivian wrote:

Based on a preliminary test using multiple threads, the issue is not
resolved.
This leads me to believe that my Unit Cell is not built properly.

Below is the procedure used to build the unit cell.  I have reviewed 
it many
times, but I would appreciate any input regarding potential 
improvements,

specifically on the line using trjconv in the EM/Shrink loop.

Safe up to here, (I hope)...

cat KALP_newbox.gro dppc128_whole.gro  system.gro

update minim.mdp
; Strong position restraints for InflateGRO
#ifdef STRONG_POSRES
#include strong_posre.itp
#endif

Create Strong Position Restraint for protein
genrestr -f KALP_newbox.gro -o strong_posre.itp -fc 10 10 10

Scale Lipid positions by a factor of 4
perl inflategro.pl system.gro 4 DPPC 14 system_inflated.gro 5 area.dat

Begin loop of repeated Energy Minimizations and Shrinking (repeat 
loop approximately 25 times until area is approx 71 Ang sq)

Begin LOOP (from n=1 to n = 26)
grompp -f minim.mdp -c systm_inf_n.gro -p topol.top -o em_n.tpr
mdrun -v -deffnm em_n
trjconv -s em_n.tpr -f em_n.gro -o em_n_out.gro -pbc mol -ur compact
perl inflategro.pl em_n_out.gro 0.95 DPPC 0 sys_shr_1.gro 5


One problem here: you start the loop every time with system_inf_n?  
What is system_inf_n?  It seems that you should start one (non-loop) 
shrink and then process the subsequent shrinking steps from there.  At 
the end of the loop, you write to sys_shr_1.gro, which then never gets 
used again.


-Justin

Put my comments in blue to make it easier to read.

I apologize for the poor description here. 
The first loop begins with the System_inflate.gro file created in the 
earlier process.  The rest of the first loop is shown.


At the beginning of the second loop, the input file is 
system_shrink_1.gro, which was the output file at the end of loop 1.  
Proceed through the loop, updating the n from 1 to 2 in each step.  
Output file is system_shrink_2.gro.


Input file for loop 3 is system_shrink_3.gro, 

Output from loop 26 is system_shrink_26.gro and output on screen 
provides information on updated Lipid area which has achieved target value.


Then proceed to add water (after changing vdw radius of C atoms)
Add ions
EM again
Then Equilibrate.
 


Output from Energy Minimization (after addition of water and ions)

Steepest Descents converged to Fmax  1000 in 1814 steps
Potential Energy  = -3.81270276926664e+05
Maximum force =  9.38712770623942e+02 on atom 2292
Norm of force =  2.88274347161761e+01




This output indicates to me that the system is completely reasonable.  If you 
send me your .gro and .top (off-list), I will try to debug and report back if I 
can find anything.


To confirm, you are using Gromacs 4.5.3?  What version of FFTW?  What hardware? 
 What compilers were used for the installation?


-Justin






ar_shr1.dat
End LOOP

Add water Add ions
Re-run EM
Equilibrate (and watch it all explode)





-Original Message-
From: gmx-users-boun...@gromacs.org 
[mailto:gmx-users-boun...@gromacs.org]

On Behalf Of Justin A. Lemkul
Sent: Thursday, March 10, 2011 12:56 PM
To: Discussion list for GROMACS users
Subject: Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 
Segmentation

Fault



Steve Vivian wrote:

On 03/08/2011 10:23 PM, Justin A. Lemkul wrote:


Steve Vivian wrote:

New to Gromacs.

Worked my way through the tutorial with relatively few issues 
until the Equilibration stage.  My system blows up!!


Returned to the Topology stage and rebuilt my system ensuring that 
I followed the procedure correctly for the InflateGro process.  It 
appears to be correct, reasonable lipid area, no water inside my 
bilayer, vmd shows a structure which appears normal (although I am 
new to this).  There are voids between bilayer and water 
molecules, but this is to be expected, correct?


Energy Minimization repeatedly produces results within the 
expected range.


Again system blows up at equilibration, step 0 segmentation 
fault.  Regardless of whether I attempt the NVT or Anneal_Npt 
process (using the provided mdp files, including the updates for 
restraints on the protein and the lipid molecules).


I have attempted many variations of the nvt.mdp and anneal_npt.mdp 
files hoping to resolve my issue, but with no success.  I will 
post the log information from the nvt.mdp file included in the 
tutorial.


Started mdrun on node 0 Tue Mar  8 15:42:35 2011

   Step   Time Lambda
  00.00.0

Grid: 9 x 9 x 9 cells
   Energies (kJ/mol)
   G96AngleProper Dih.  Improper 

Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation Fault

2011-03-12 Thread Justin A. Lemkul



Steve Vivian wrote:

On 03/12/2011 01:36 PM, Justin A. Lemkul wrote:



Steve Vivian wrote:

  On 03/12/2011 12:51 PM, Justin A. Lemkul wrote:
Getting hard to follow, so I put my new comments in blue.
Output from Energy Minimization

Steepest Descents converged to Fmax  1000 in 1814 steps
Potential Energy  = -3.81270276926664e+05
Maximum force =  9.38712770623942e+02 on atom 2292
Norm of force =  2.88274347161761e+01





Steve Vivian wrote:

Based on a preliminary test using multiple threads, the issue is not
resolved.
This leads me to believe that my Unit Cell is not built properly.

Below is the procedure used to build the unit cell.  I have 
reviewed it many
times, but I would appreciate any input regarding potential 
improvements,

specifically on the line using trjconv in the EM/Shrink loop.

Safe up to here, (I hope)...

cat KALP_newbox.gro dppc128_whole.gro  system.gro

update minim.mdp
; Strong position restraints for InflateGRO
#ifdef STRONG_POSRES
#include strong_posre.itp
#endif

Create Strong Position Restraint for protein
genrestr -f KALP_newbox.gro -o strong_posre.itp -fc 10 10 
10


Scale Lipid positions by a factor of 4
perl inflategro.pl system.gro 4 DPPC 14 system_inflated.gro 5 area.dat

Begin loop of repeated Energy Minimizations and Shrinking (repeat 
loop approximately 25 times until area is approx 71 Ang sq)

Begin LOOP (from n=1 to n = 26)
grompp -f minim.mdp -c systm_inf_n.gro -p topol.top -o em_n.tpr
mdrun -v -deffnm em_n
trjconv -s em_n.tpr -f em_n.gro -o em_n_out.gro -pbc mol -ur 
compact

perl inflategro.pl em_n_out.gro 0.95 DPPC 0 sys_shr_1.gro 5


One problem here: you start the loop every time with system_inf_n?  
What is system_inf_n?  It seems that you should start one (non-loop) 
shrink and then process the subsequent shrinking steps from there.  
At the end of the loop, you write to sys_shr_1.gro, which then never 
gets used again.


-Justin

Put my comments in blue to make it easier to read.

I apologize for the poor description here. The first loop begins with 
the System_inflate.gro file created in the earlier process.  The rest 
of the first loop is shown.


At the beginning of the second loop, the input file is 
system_shrink_1.gro, which was the output file at the end of loop 1.  
Proceed through the loop, updating the n from 1 to 2 in each step.  
Output file is system_shrink_2.gro.


Input file for loop 3 is system_shrink_3.gro, 

Output from loop 26 is system_shrink_26.gro and output on screen 
provides information on updated Lipid area which has achieved target 
value.


Then proceed to add water (after changing vdw radius of C atoms)
Add ions
EM again
Then Equilibrate.


Output from Energy Minimization (after addition of water and ions)

Steepest Descents converged to Fmax  1000 in 1814 steps
Potential Energy  = -3.81270276926664e+05
Maximum force =  9.38712770623942e+02 on atom 2292
Norm of force =  2.88274347161761e+01




This output indicates to me that the system is completely reasonable.  
If you send me your .gro and .top (off-list), I will try to debug and 
report back if I can find anything.


To confirm, you are using Gromacs 4.5.3?  What version of FFTW?  What 
hardware?  What compilers were used for the installation?


-Justin



Using Gromacs 4.5.3 and FFTW 3.2.2 both compiled for double precision.
It has been a while since I compiled so I'm not exactly sure, but I 
recall updating gcc and gfortran during the process.
Hardware, what type of specifics are you looking for?  # of processors 
and speed?

Attached are current Energy Minimized file and topology file.



Hardware and compiler specs are unnecessary.  The problem is the coordinate file 
itself.  Look at it in your favorite visualization program and you will see that 
the lipid headgroups are completely collapsed in on one another.  I don't know 
how or why this happened.  If you're using the DPPC topology from Tieleman and 
the .mdp files given in the tutorial, I see no reason for this totally unstable 
configuration.  I have never used double precision (and it is not necessary for 
standard MD, and only serves to slow your runs down), so it would be interesting 
to see if the problem is a result of double vs. single precision.  I can 
successfully re-minimize the coordinate file you sent me using single precision:


Steepest Descents converged to Fmax  1000 in 335 steps
Potential Energy  = -6.3605750e+04
Maximum force =  7.1865680e+02 on atom 115
Norm of force =  3.9649860e+01

For now, I would suggest you test the precision issue.  Install Gromacs again 
(making note of your compiler versions, because this is important to know!) in 
single precision and try to re-minimize the system and proceed.  No need to 
completely re-build it, as you should be able to just run a new EM on your 
existing system like I did.


-Justin


Steve.









ar_shr1.dat
End LOOP

Add water Add ions
Re-run EM
Equilibrate (and watch it all 

[gmx-users] terminated but not completely

2011-03-12 Thread mohsen ramezanpour
Dear All

I run a simulation for  4 days.
Unfortunately it terminated,but not completely,1 steps from 2 has
done.
Is there any way to run the continue of my files?
Thanks in advance for your guidances
Best Regards
-- 
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Re: [gmx-users] Fwd: KALP-15 in DPPC Tutorial Step 0 Segmentation Fault

2011-03-12 Thread Steve Vivian

On 03/12/2011 02:10 PM, Justin A. Lemkul wrote:



Steve Vivian wrote:

On 03/12/2011 01:36 PM, Justin A. Lemkul wrote:



Steve Vivian wrote:

  On 03/12/2011 12:51 PM, Justin A. Lemkul wrote:
Getting hard to follow, so I put my new comments in blue.
Output from Energy Minimization

Steepest Descents converged to Fmax  1000 in 1814 steps
Potential Energy  = -3.81270276926664e+05
Maximum force =  9.38712770623942e+02 on atom 2292
Norm of force =  2.88274347161761e+01





Steve Vivian wrote:

Based on a preliminary test using multiple threads, the issue is not
resolved.
This leads me to believe that my Unit Cell is not built properly.

Below is the procedure used to build the unit cell.  I have 
reviewed it many
times, but I would appreciate any input regarding potential 
improvements,

specifically on the line using trjconv in the EM/Shrink loop.

Safe up to here, (I hope)...

cat KALP_newbox.gro dppc128_whole.gro  system.gro

update minim.mdp
; Strong position restraints for InflateGRO
#ifdef STRONG_POSRES
#include strong_posre.itp
#endif

Create Strong Position Restraint for protein
genrestr -f KALP_newbox.gro -o strong_posre.itp -fc 10 10 
10


Scale Lipid positions by a factor of 4
perl inflategro.pl system.gro 4 DPPC 14 system_inflated.gro 5 
area.dat


Begin loop of repeated Energy Minimizations and Shrinking (repeat 
loop approximately 25 times until area is approx 71 Ang sq)

Begin LOOP (from n=1 to n = 26)
grompp -f minim.mdp -c systm_inf_n.gro -p topol.top -o em_n.tpr
mdrun -v -deffnm em_n
trjconv -s em_n.tpr -f em_n.gro -o em_n_out.gro -pbc mol -ur 
compact

perl inflategro.pl em_n_out.gro 0.95 DPPC 0 sys_shr_1.gro 5


One problem here: you start the loop every time with 
system_inf_n?  What is system_inf_n?  It seems that you should 
start one (non-loop) shrink and then process the subsequent 
shrinking steps from there.  At the end of the loop, you write to 
sys_shr_1.gro, which then never gets used again.


-Justin

Put my comments in blue to make it easier to read.

I apologize for the poor description here. The first loop begins 
with the System_inflate.gro file created in the earlier process.  
The rest of the first loop is shown.


At the beginning of the second loop, the input file is 
system_shrink_1.gro, which was the output file at the end of loop 
1.  Proceed through the loop, updating the n from 1 to 2 in each 
step.  Output file is system_shrink_2.gro.


Input file for loop 3 is system_shrink_3.gro, 

Output from loop 26 is system_shrink_26.gro and output on 
screen provides information on updated Lipid area which has 
achieved target value.


Then proceed to add water (after changing vdw radius of C atoms)
Add ions
EM again
Then Equilibrate.


Output from Energy Minimization (after addition of water and ions)

Steepest Descents converged to Fmax  1000 in 1814 steps
Potential Energy  = -3.81270276926664e+05
Maximum force =  9.38712770623942e+02 on atom 2292
Norm of force =  2.88274347161761e+01




This output indicates to me that the system is completely 
reasonable.  If you send me your .gro and .top (off-list), I will 
try to debug and report back if I can find anything.


To confirm, you are using Gromacs 4.5.3?  What version of FFTW?  
What hardware?  What compilers were used for the installation?


-Justin



Using Gromacs 4.5.3 and FFTW 3.2.2 both compiled for double precision.
It has been a while since I compiled so I'm not exactly sure, but I 
recall updating gcc and gfortran during the process.
Hardware, what type of specifics are you looking for?  # of 
processors and speed?

Attached are current Energy Minimized file and topology file.



Hardware and compiler specs are unnecessary.  The problem is the 
coordinate file itself.  Look at it in your favorite visualization 
program and you will see that the lipid headgroups are completely 
collapsed in on one another.  I don't know how or why this happened.  
If you're using the DPPC topology from Tieleman and the .mdp files 
given in the tutorial, I see no reason for this totally unstable 
configuration.  I have never used double precision (and it is not 
necessary for standard MD, and only serves to slow your runs down), so 
it would be interesting to see if the problem is a result of double 
vs. single precision.  I can successfully re-minimize the coordinate 
file you sent me using single precision:


Steepest Descents converged to Fmax  1000 in 335 steps
Potential Energy  = -6.3605750e+04
Maximum force =  7.1865680e+02 on atom 115
Norm of force =  3.9649860e+01

For now, I would suggest you test the precision issue.  Install 
Gromacs again (making note of your compiler versions, because this is 
important to know!) in single precision and try to re-minimize the 
system and proceed.  No need to completely re-build it, as you should 
be able to just run a new EM on your existing system like I did.


-Justin

Questions regarding re-compiling FFTW and Gromacs

Re: [gmx-users] Possible free energy bug? (NOT SOLVED)

2011-03-12 Thread Justin A. Lemkul


Hi All,

Unfortunately, my positive news was a false alarm.  Intermediate values of 
lambda are sporadically failing at different times.  Some jobs exit at time 
zero, others last somewhat longer (several hundred ps) before failing.  I'm 
going to keep working on the suggestions I got before about compilation options 
and such, but for now I will post the error output to see if it provides any 
clues about what's wrong:


Warning: Only triclinic boxes with the first vector parallel to the x-axis and 
the second vector in the xy-plane are supported.
Warning: Only triclinic boxes with the first vector parallel to the x-axis and 
the second vector in the xy-plane are supported.

 Box (3x3):
Box[0]={ nan,  0.0e+00,  0.0e+00}
Box[1]={ nan,  nan,  nan}
Box[2]={ nan,  nan,  nan}
 Can not fix pbc.
Warning: Only triclinic boxes with the first vector parallel to the x-axis and 
the second vector in the xy-plane are supported.

 Box (3x3):
Box[0]={ nan,  0.0e+00,  0.0e+00}
Box[1]={ nan,  nan,  nan}
Box[2]={ nan,  nan,  nan}
 Can not fix pbc.
 Box (3x3):
Box[0]={ nan,  0.0e+00,  0.0e+00}
Box[1]={ nan,  nan,  nan}
Box[2]={ nan,  nan,  nan}
 Can not fix pbc.
Warning: Only triclinic boxes with the first vector parallel to the x-axis and 
the second vector in the xy-plane are supported.

 Box (3x3):
Box[0]={ nan,  0.0e+00,  0.0e+00}
Box[1]={ nan,  nan,  nan}
Box[2]={ nan,  nan,  nan}
 Can not fix pbc.
[n921:01432] *** Process received signal ***
[n921:01432] Signal: Segmentation fault (11)
[n921:01432] Signal code: Address not mapped (1)
[n921:01432] Failing at address: 0xfffe10af11c0
[n921:01432] [ 0] [0x100428]
[n921:01432] [ 1] [0xfcc01f4]
[n921:01432] [ 2] 
/home/rdiv1001/gromacs-4.5.3-linux_gcc445_fftw322/bin/mdrun_4.5.3_gcc_mpi(gmx_pme_do-0x51df30) 
[0x1010c0e8]
[n921:01432] [ 3] 
/home/rdiv1001/gromacs-4.5.3-linux_gcc445_fftw322/bin/mdrun_4.5.3_gcc_mpi(do_force_lowlevel-0x560cd0) 
[0x100c88c8]
[n921:01432] [ 4] 
/home/rdiv1001/gromacs-4.5.3-linux_gcc445_fftw322/bin/mdrun_4.5.3_gcc_mpi(do_force-0x50b084) 
[0x1011f594]
[n921:01432] [ 5] 
/home/rdiv1001/gromacs-4.5.3-linux_gcc445_fftw322/bin/mdrun_4.5.3_gcc_mpi(do_md-0x5bbb78) 
[0x1006cac0]
[n921:01432] [ 6] 
/home/rdiv1001/gromacs-4.5.3-linux_gcc445_fftw322/bin/mdrun_4.5.3_gcc_mpi(mdrunner-0x5c26f8) 
[0x10065e98]
[n921:01432] [ 7] 
/home/rdiv1001/gromacs-4.5.3-linux_gcc445_fftw322/bin/mdrun_4.5.3_gcc_mpi(main-0x5b7964) 
[0x10070cec]

[n921:01432] [ 8] /lib64/libc.so.6 [0x80aaed8858]
[n921:01432] [ 9] /lib64/libc.so.6(__libc_start_main-0x1471f8) [0x80aaed8ad0]
[n921:01432] *** End of error message ***

I have not yet compiled with debugging enabled, but I can if that will be 
useful.

-Justin

Justin A. Lemkul wrote:


Hi All,

I believe I have a resolution to all of this.  It comes down to 
compilers and FFTW.  I had always used the same compilers to build all 
my Gromacs versions (gcc-4.2.2 on Linux, gcc-3.3 on OSX) with the same 
version of FFTW (3.0.1), primarily for reasons of continuity.  Bug 715 
that I posted before was due to a problem with FFTW, not Gromacs; 
upgrading to 3.2.2 solves the issue.  As well, the combination of 
gcc-4.4.5 + FFTW 3.2.2 allows for successful free energy runs in my 
tests thus far on Linux.  Dependency issues on the OS X partition 
prevent me from doing any upgrades, so we're out of luck there, 
unfortunately.  I will report back if any other weird behavior results, 
but I believe the problem is solved.


I am no compiler/library guru, but it would seem to me that we've 
reached a point where certain minimum versions must be required for 
certain prerequisites.  I would suggest that prior to the next release, 
we come up with a list of what should be considered stable minimum 
requirements (compiler versions, FFTW, anything else) to post on the 
website and perhaps the manual.  As it stands now, the prerequisites for 
installation would seem to be satisfied by any C compiler and any 
version of FFTW.  Gromacs happily compiles under most conditions, but 
shows some weird behavior if one is not using optimal dependencies.


Thanks to all for their input!

-Justin

Justin A. Lemkul wrote:



Michael Shirts wrote:

Hi, all-

Have you tried running

constraints = hbonds?

That might eliminate some of the constraint issues.  Much less likely
for LINCS to break or have DD issues if only the hbonds are
constrained.  2 fs is not that big a deal for the heteroatom bonds.



I haven't yet, but I'll add it to my to-do list.  I was 

Re: [gmx-users] terminated but not completely

2011-03-12 Thread ZHAO Lina
-cpi  state.cpt -append

try to add those two options at the end of your mdrun

lina


On Sun, Mar 13, 2011 at 5:53 AM, mohsen ramezanpour 
ramezanpour.moh...@gmail.com wrote:

 Dear All

 I run a simulation for  4 days.
 Unfortunately it terminated,but not completely,1 steps from 2 has
 done.
 Is there any way to run the continue of my files?
 Thanks in advance for your guidances
 Best Regards


 --
 gmx-users mailing listgmx-users@gromacs.org
 http://lists.gromacs.org/mailman/listinfo/gmx-users
 Please search the archive at
 http://www.gromacs.org/Support/Mailing_Lists/Search before posting!
 Please don't post (un)subscribe requests to the list. Use the
 www interface or send it to gmx-users-requ...@gromacs.org.
 Can't post? Read http://www.gromacs.org/Support/Mailing_Lists

-- 
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