Re: [gmx-users] mdp-settings for charmm36 and lipid apl values

2013-05-10 Thread Patrick Fuchs
 they are)

For POPC, I get 59,7 A^2, and for POPE, I get 63,1 A^2.

The value for POPE would have been fine I suppose if it hadn't been for the
fact that the APL for POPC is smaller. Should it not be larger than POPE?

I notice in the Piggott-paper that they in the supplement for some
simulations of POPC also get APL's of around 59-60 (without POPE of
course), and that the results depend to some extent also on the usage of
TIP3P vs TIP3SP water models. I have been using normal TIP3P here.

Could anyone comment on (a) my mdp-file settings, and (b) the resulting
APL, and tell me if I should be worried about anything?

THANKS



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Re: [gmx-users] What is the autocorrelation time

2012-05-21 Thread Patrick Fuchs

Hi Erik,
your examples on H-bond acfs are interesting. I'm wondering about the 
distinct features which are non-exponential in your examples. What do 
you mean exactly? Could these features be due to rare (H-bonding) 
events, or in other words to poor sampling?
Intuitively, I'd say that the interpretation of the acf (at least for 
the decay and the decorelation) is always valid unless maybe if you have 
very poor statistics.

Ciao,

Patrick

Le 20/05/2012 16:12, Erik Marklund a écrit :

Dear Chris,

As I see it there one can interpret the acf and correlatation time
further for certain types of data. I'll use the h-bond autocorrelation
function as an example. Here the data is time series of logical true and
false, represented as ones and zeros. This type of acf can be direcly
interpreted as a probablity, and some quantities derived from the acf
can bear further meaning because of this.

I also thought that the nature of the data may be such there is a
non-exponential part, which makes the autocorreltaion time less valid,
or less connected to other intuitive concepts. Again, the h-bond acf has
distinct features which are non-exponential and the autocorreltaion time
derived from such acfs may in fact be misleading when the h-bond
kinetics is to be determined.

Hope that makes sense. I's be happy to hear from you if you disagree.

Best,

Erik

19 maj 2012 kl. 04.01 skrev Christopher Neale:


Dear Erik:

I thought about your comment for a while and I have come to understand
that you are correct. The exponential (or integral) autocorrelation
time is a mathematical construct and is defined as such. What I was
looking for was an interpretation of the autocorrelation time in terms
of the time required to decorrelate the sampling.

As to whether or not this will depend on the nature of the data, I
don't really understand your conjecture. If the interpretation of the
autocorrelation time depends on the nature of the data, then that
implies to me that a single scalar value is useless in this case. I
don't understand how it could be useful to represent the
autocorrelation time by a single number if that number does not mean
anything on its own. If you have time, I would appreciate if you could
elaborate on this point.

Thank you,
Chris.

-- original message --

Aren't you looking for an interpretation rather than a definition? And
will this not depend on the nature of the data?

Best,

Erik

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Husargatan 3, Box 596, 75124 Uppsala, Sweden
phone: +46 18 471 6688 fax: +46 18 511 755
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Re: [gmx-users] What is the autocorrelation time

2012-05-18 Thread Patrick Fuchs

Hi Chris,
I understand your question, this autocorrelation time puzzled me for a 
long time as well. Not far from the interpretation you give, Scott 
Feller defines it (http://dx.doi.org/10.1007/978-1-59745-519-0_7) as the 
time a given observable takes to lose the memory of its previous state, 
or in other words the time it takes to relax (that's why it's sometimes 
called relaxation time). He also discusses it as a tool to choose the 
block size for calculating an error estimate of an observable (one 
single simulation can be used as independant samples if each block size 
is  autocorrelation time).
We also had a nice discussion some years ago on the mailing list on free 
energy calculation and error estimate: 
http://lists.gromacs.org/pipermail/gmx-users/2007-May/027281.html. John 
Chodera pointed me to a useful article from Wolfhard Janke (the link in 
the discussion is broken, here's the new one: 
http://www2.fz-juelich.de/nic-series/volume10/janke2.pdf). There you'll 
find a rigorous mathematical definition of autocorrelation time. Quoting 
this paper This shows more clearly that only every 2 tau_int 
iterations the measurements are approximately uncorrelated and gives a 
better idea of the relevant effective size of the statistical sample 
(tau_int is the integrated autocorrelation time; as you said the 
autocorrelation function is usually a single exponential, but sometimes 
it's more complex and one needs to evaluate it by integration of the 
autocorrelation function).
After all these considerations, the autocorrelation time can be seen as 
a tool to assess the time that is needed to have a good estimate of an 
observable: the simulation must be many many times longer than the 
autocorrelation time. And sometimes it's directly related to 
experimental observables (i.e. NMR relaxation experiments).

Hope it's useful,

Patrick

Le 16/05/2012 23:39, Christopher Neale a écrit :

Thank you Stephane.

Unfortunately, neither of those links contains the information that I am
seeking. Those links contain some example plots of autocorrelation
functions including a discussion of time-spans over which the example
time-series is autocorrelated and when it is not, but neither link
defines the (exponential or integral) autocorrelation time except to
show a plot and indicate when it is non-zero and when it fluctuates
about zero.

For example, I already know that the autocorrelation time describes the
exponential decay of the correlation and that two values drawn from the
same simulation are statistically independent if they are separated by a
sufficient number of (accurate) autocorrelation times, but this
information is not exactly a definition of the autocorrelation time.

I am hoping to find a definition of the autocorrelation time in terms of
the probability of drawing uncorrelated samples, although any complete
definition will do.

If anybody else has the time, I would appreciate it.

Thank you,
Chris.

-- original message --

Probably these links give you simple and clear response for your
question
http://idlastro.gsfc.nasa.gov/idl_html_help/Time-Series_Analysis.html
and http://www.statsoft.com/textbook/time-series-analysis/ HTH Stephane




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Re: [gmx-users] a question about ensemble

2012-05-05 Thread Patrick Fuchs

Interesting discussion indeed. I'm just thinking that there might be
no fundamental difference to other thermostats. There's nothing in the
way that causes the friction, but then again, there's no physical
particle that causes the stochastic term in v-rescale, and the
Nosé-Hover particle is not physically touching the atoms either.  In
all cases the surroundings couples to the atoms in a way that can't be
seen in e.g. a test tube.


Erik



Hi Erik,

yes, that is a good point, which I haven't really thought about.
Indeed, in a macroscopic system heat will have to diffuse from the edges 
of the container to the inside of the system. In the simulations, the 
rescaling of velocities is done on all the atoms at the same time, 
either on a local or global basis. For the use of SD in explicit 
systems, the friction and stochastic terms (with the carefully chosen 
friction coeffictient) can be seen as applying one thermostat per degree 
of freedom. So Florian, I think you should change your view about the 
random kicks and friction as a way to modify velocities for 
thermostating, which is different from mimicking solvant effects in 
implicit simulations (even if it uses also the friction and random 
forces). What we want is that the thermostat samples the proper 
canonical ensemble. Then if it does, what also matters is to be aware 
whether it affects other properties, notably dynamics (because rescaling 
velocities will in general pertubs dynamics). There has been a nice 
discussion some years ago in the GROMACS mailing list about that: 
http://lists.gromacs.org/pipermail/gmx-users/2008-July/035302.html. Also 
Bussi and Parrinello discuss this aspect in that paper: 
http://dx.doi.org/10.1016/j.cpc.2008.01.006.

Ciao,

Patrick

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Re: [gmx-users] a question about ensemble

2012-05-03 Thread Patrick Fuchs

Hi Florian,


I remark that Langevin method is used also for explicit water system!


But there a big question arises to me. The thermostatting by Langevin is
achieved due to random kicks. If I simulate all atoms explicitly, there
is only vacuum between the atoms. Where do the random kicks come from
and how do I set gamma, which is actually related to the viscosity of
the medium I am simulating in? If my medium is vacuum, then gamma should
be zero, shouldn't it, and gamma=0 means no coupling, and hence,
Newton's equation of motion are recovered.

I am not an expert with the Langevin thermostat, so this are serious
questions that arise to me now. Furthermore I also thought, that
Langevin dynamics were exactly established for a description of a system
within a medium.
The use of Langevin dynamics (SD) to mimic solvant implicitely or as a 
thermostat in explicit systems depends on the friction coefficient you 
choose. It has to be chosen with care, see for example 
http://dx.doi.org/10.1007/b99427 or the GROMACS manual. In explicit 
simulations, SD with the appropriate choice of friction coefficient can 
be seen as a local thermostat. The advantage is that it samples the 
canonical ensemble (in the old versions of GROMACS it was the only way 
to get the canonical ensemble before the implementation of Nose-Hoover 
or velocity rescaling).

Ciao,

Patrick
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Re: [gmx-users] REST simulation

2011-12-13 Thread Patrick Fuchs

Hi Otto,
you have to equilibrate at each lambda value! The unscaled Hamiltionian 
is your lowest temperature, say 300K, which corresponds to lambda=0. 
You generate the highest temperature by appropriately scaling the 
Hamiltonian, say 600K, which corresponds to lambda=1. Then you create n 
directories, one for each replica. In each directory, you set a 
different lambda value from 0 to 1 in the mdp file and you equilibrate 
each replica. At the end, you obtain n gro files that can serve as input 
to generate n tpr files for the REMD run.
I think this is the standard flow for REMD as explained in: 
http://www.gromacs.org/Documentation/How-tos/REMD. The only difference 
is that you use a different lambda value, so a different Hamiltonian, 
instead of a different temperature for each replica.

Ciao,

Patrick

Le 13/12/2011 11:46, Otto Master a écrit :

Hi Patrick,
thanks for your help. What I still do not understand is, how I can
set-up the replica simulation starting from the two equilibrated
systems. What do I have to put into the .mdp file and in the grompp
command to consider the two equilibrated configurations and further
obtain the tpr files for the different replica for different lambda
values to interpolate between the two configuration. I would be very
glad if you could help me on that.

All the best
Otto

On Mon, Dec 12, 2011 at 1:50 PM, Patrick Fuchs
patrick.fu...@univ-paris-diderot.fr
mailto:patrick.fu...@univ-paris-diderot.fr wrote:

Hi Otto,
yes I copied those two files you mentionned (also .rtp for charges)
in some specific directory to apply the appropriate scaling. But
according to the authors this REST implementation, you just need
that for the highest temperature (for the lowest, the Hamiltonian
is unchanged) and then intermediate temperatures are interpolated
using the lambda factor. So for equilibrating each replica, you just
need to set the appropriate lambda value.
Now I'd consider Mark's advice to use the -pp flag of grompp which
might be convenient for scripting the scaling of the potential.
Ciao,

Patrick

Le 12/12/2011 12:56, Otto Master a écrit :

Hi Patrick,
Thanks a lot for your reply. Just to be sure, you create for
every replicate a copy of the original force field, and after
you manipulate the parameter in ffnonbonded.itp and
ffbonded.itp. Then you go for each replicate through the usual
simulation preparation steps (minimisation, nvt, equilibration
...). The result of this you use for the replicate exchange
simulation.

Thanks a lot
Otto

On 12 Dec 2011, at 10:42, Patrick
Fuchspatrick.fuchs@univ-__paris-diderot.fr
mailto:patrick.fu...@univ-paris-diderot.fr  wrote:

Hi Otto,
in my lab we tried to implement this REST variant in GROMACS
as proposed by those authors. We figured out that it was
easier to manipulate directly the parameters files in the
top directory. There you know exactly what you are doing;
recall that some interactions (i.e. solvent/solvent) mustn't
be scaled whereas some others have to be scaled
(solute/solute and solute/solvent).
It's probably possible to do it in the tpr file, but it
looked less trivial to me: i) you have to know how atoms are
coded in the file (e.g. in the functype[???]=LJ_SR[...]
matrix, you have to understand how atom numbers are coded
there), ii) you have to regenerate a tpr from plain text
file; it's probably doable, but I don't know how. Actually,
maybe some developers can tell if it's possible.
Good luck,

Patrick

Le 08/12/2011 19:01, Otto Master a écrit :

Dear gromacs users,

Recently I stumbled over following paper:
T. Terakawa, T. Kameda, and S. Takada, On Easy
Implementation of a
Variant of the Replica Exchange with Solute Tempering in
GROMACS.
Journal of Computational Chemistry 32 (2011) 1228-1234.

The authors suggested an easy way to run this kind of
simulation with
Gromacs, without even changing the code. The only thing
that is need, is
the the rescaling of the parameters in the parameter
file. Since the
reduction of the replica number is quite appealing to me
I wonder which
file I have to change? Actually, I thought of
manipulating the .tpr file
or to rescale and creating the force fields for every
replicate. Is this
feasible, or is there a better way?

Manipulating the .tpr file could be easier, since

Re: [gmx-users] REST simulation

2011-12-13 Thread Patrick Fuchs

Hi Otto,
do you know how to use the free energy code in GROMACS for running 
alchemical transformations (such as thermodynamic integration)? I 
strongly suggest first to be confortable with that code before trying to 
implement REST. In such alchemical calculations, you have to specify two 
topologies, one for state A and one for state B. Then simulations at 
each lambda value is a linear interpolation between state A and state B, 
such as H = (1-lambda)*H[A] + lambda*H[B]. In the case of REST, one 
simulation at an intermediate lambda value is also a linear 
interpolation between topology A (ref T, unscaled Hamiltonian) and 
topology B (highest T, scaled Hamiltonian). You thus have to build a 
topology for both A *and* B (how to do that is well described in the 
manual). Once you have this dual topology, you just have to set lambda 
for each replica.

Ciao,

Patrick

Le 13/12/2011 14:05, Otto Master a écrit :

Hi Patrick,
again thanks a lot for your valuable help. But I do not get my head
around how to tell grompp that for lambda=0 I would like to use the the
unscaled Hamiltonian and for lambda=1 the highest temperature. In the
tutorial the change in temperature is a number which is passed to the
pre-processor, but for REST a number (lambda=0 and lambda=1) corresponds
to different topology, which are written in a file. I do not know how to
specify that. What is the identifier or should I pass something
additionally to grompp, referring to the two topology files?

Ciao,
Otto

On Tue, Dec 13, 2011 at 1:23 PM, Patrick Fuchs
patrick.fu...@univ-paris-diderot.fr
mailto:patrick.fu...@univ-paris-diderot.fr wrote:

Hi Otto,
you have to equilibrate at each lambda value! The unscaled
Hamiltionian is your lowest temperature, say 300K, which
corresponds to lambda=0. You generate the highest temperature by
appropriately scaling the Hamiltonian, say 600K, which corresponds
to lambda=1. Then you create n directories, one for each replica. In
each directory, you set a different lambda value from 0 to 1 in the
mdp file and you equilibrate each replica. At the end, you obtain n
gro files that can serve as input to generate n tpr files for the
REMD run.
I think this is the standard flow for REMD as explained in:
http://www.gromacs.org/__Documentation/How-tos/REMD
http://www.gromacs.org/Documentation/How-tos/REMD. The only
difference is that you use a different lambda value, so a different
Hamiltonian, instead of a different temperature for each replica.
Ciao,

Patrick

Le 13/12/2011 11:46, Otto Master a écrit :

Hi Patrick,

thanks for your help. What I still do not understand is, how I can
set-up the replica simulation starting from the two equilibrated
systems. What do I have to put into the .mdp file and in the grompp
command to consider the two equilibrated configurations and further
obtain the tpr files for the different replica for different lambda
values to interpolate between the two configuration. I would be very
glad if you could help me on that.

All the best
Otto

On Mon, Dec 12, 2011 at 1:50 PM, Patrick Fuchs
patrick.fuchs@univ-paris-__diderot.fr
mailto:patrick.fu...@univ-paris-diderot.fr
mailto:patrick.fuchs@univ-__paris-diderot.fr
mailto:patrick.fu...@univ-paris-diderot.fr wrote:

Hi Otto,
yes I copied those two files you mentionned (also .rtp for
charges)
in some specific directory to apply the appropriate scaling. But
according to the authors this REST implementation, you just need
that for the highest temperature (for the lowest, the
Hamiltonian
is unchanged) and then intermediate temperatures are
interpolated
using the lambda factor. So for equilibrating each replica,
you just
need to set the appropriate lambda value.
Now I'd consider Mark's advice to use the -pp flag of grompp
which
might be convenient for scripting the scaling of the potential.
Ciao,

Patrick

Le 12/12/2011 12:56, Otto Master a écrit :

Hi Patrick,
Thanks a lot for your reply. Just to be sure, you create for
every replicate a copy of the original force field, and
after
you manipulate the parameter in ffnonbonded.itp and
ffbonded.itp. Then you go for each replicate through the
usual
simulation preparation steps (minimisation, nvt,
equilibration
...). The result of this you use for the replicate exchange
simulation.

Thanks a lot
Otto

On 12 Dec 2011, at 10:42, Patrick
Fuchspatrick.fuchs@univ-paris-diderot.fr
mailto:patrick.fuchs

Re: [gmx-users] Gromos parameters for atom type OA

2011-12-12 Thread Patrick Fuchs

Hi,
slightly off-thread, I'd like to add that the oxygen parameters of 53a6 
have been recently refined in a new set called 53a6OXY 
(http://pubs.acs.org/doi/abs/10.1021/ct1006407). So this ends up in new 
values for LJ and charges for the OA atom (as well as for other oxygen 
atoms).

Cheers,

Patrick

Le 09/12/2011 20:03, Javier Cerezo a écrit :

GROMOS force field builds the LJ parameters by multiplication of the
square-rooted parameters per atom type (hence the SQRT(C6) and SQRT(C12)
labels). In the case of the repulsion term (C12), up to three of such
parameters are possible: SQRT(C12(1)) SQRT(C12(2)) SQRT(C12(3)), when
combined with other atoms, depending on the desired repulsion strength
(e.g. the enhanced C12(3) repulsion is used to keep charged groups
separated). Which of the three is used depends on the combination of
atoms, and is specified in an (asymmetric) matrix (see pages 14 and 15
in the pdf pages of 45a3 and 54a6 force fields from the GROMOS site, or
in the ifp file the last lines for each atom type containing 1, 2
and 3). For the case of OA, this matrix specifies that the second C12
term is to be used when OA encountes another OA. So, according, to the
ifp line you showed:

C12(OA-OA) = SQRT(C12(2))_OA * SQRT(C12(2))_OA = 1.227E-3 * 1.227E-3 =
1.50553E-6

Which is the same for 45a3 and 54a6 force fields.

Differences in the parameters will show up only in the cases where the
SQRT(C12(1)) term for OA is to be used (e.g C12(OA-CH2))

Javier

El 09/12/11 16:12, Samuli Ollila escribió:

Dear all,

I was comparing Gromos 45a3 and 53a6 force fields and I found
something which I cannot understand. The atom type OA is described in
ffG45a3nb.itp as:
;name at.num mass charge ptype c6 c12
OA 8 0.000 0.000 A 0.0022619536 1.505529e-06
and in ffG53a6nb.itp:
OA 8 0.000 0.000 A 0.0022619536 1.505529e-06
which are same parameters.

However, according to Gromos developers the atom type OA has been
changed between Gromos 45a3 and 53a6. The parameters given by Gromos
developers for 45a3 are
# IAC TYPE SQRT(C6) SQRT(C12(1)) SQRT(C12(2)) SQRT(C12(3))
3 OA 0.04756 1.1250E-3 1.227E-3 0.0
and for 53a6
3 OA 0.04756 1.100E-3 1.227E-3 0.0

The actual numbers are different for parameters used in Gromacs since
the way to write parameters is different.

My problem is that there is difference in OA type between 45a3 and
53a6 in parameters given by Gromos developers but not in the files
distributed in Gromacs package. Can someone explain this?

BR,
Samuli Ollila




--
Javier CEREZO BASTIDA
Ph.D. Student
Physical Chemistry
Universidad de Murcia
30100, Murcia (SPAIN)
T: (0034)868887434





--
___
Patrick FUCHS
Dynamique des Structures et Interactions des Macromolécules Biologiques
INTS, INSERM UMR-S665, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-43-06-50-19
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Re: [gmx-users] REST simulation

2011-12-12 Thread Patrick Fuchs

Hi Otto,
in my lab we tried to implement this REST variant in GROMACS as proposed 
by those authors. We figured out that it was easier to manipulate 
directly the parameters files in the top directory. There you know 
exactly what you are doing; recall that some interactions (i.e. 
solvent/solvent) mustn't be scaled whereas some others have to be scaled 
(solute/solute and solute/solvent).
It's probably possible to do it in the tpr file, but it looked less 
trivial to me: i) you have to know how atoms are coded in the file (e.g. 
in the functype[???]=LJ_SR[...] matrix, you have to understand how atom 
numbers are coded there), ii) you have to regenerate a tpr from plain 
text file; it's probably doable, but I don't know how. Actually, maybe 
some developers can tell if it's possible.

Good luck,

Patrick

Le 08/12/2011 19:01, Otto Master a écrit :

Dear gromacs users,

Recently I stumbled over following paper:
T. Terakawa, T. Kameda, and S. Takada, On Easy Implementation of a
Variant of the Replica Exchange with Solute Tempering in GROMACS.
Journal of Computational Chemistry 32 (2011) 1228-1234.

The authors suggested an easy way to run this kind of simulation with
Gromacs, without even changing the code. The only thing that is need, is
the the rescaling of the parameters in the parameter file. Since the
reduction of the replica number is quite appealing to me I wonder which
file I have to change? Actually, I thought of manipulating the .tpr file
or to rescale and creating the force fields for every replicate. Is this
feasible, or is there a better way?

Manipulating the .tpr file could be easier, since it unifies (right?)
the parameters from the different force fields, before sending it to the
mdrun application. But for this I would like to understand the tpr file
first.There are quite a lot of entries and first I try to understand LJ
interactions and how they are defined in this file. I found two entries

LJ14
  functype[154]=LJ14, c6A= 0.e+00, c12A= 0.e+00,
c6B= 0.e+00, c12B= 0.e+00
  functype[155]=LJ14, c6A= 4.46680887e-03, c12A= 4.74702711e-06,
c6B= 4.46680887e-03, c12B= 4.74702711e-06

which corresponds to following interactions

   LJ-14:
  nr: 876
  iatoms:
 0 type=154 (LJ14) 0 4
 1 type=155 (LJ14) 0 5

When I tried to calculate the parameters from the combination rules (in
this case Gromos 53A6 force field), I found (the highlighted columns
contain the original parameters for the specific atom groups from the
Gromos  documentation and the calculated value for combining the two
parameters:




sqrt(C6i) (from ff) sqrt(C6j) (from ff) sqrt(C6i)*sqrt(C6j) 
value
from tpr file
functype[154]=LJ14, c6A=CH3 H   0.09805 0   0   
0.00E+00
functype[155]=LJ14, c6A=CH3 CH1 0.09805 0.0779  
0.007638095 4.47E-03
functype[156]=LJ14, c6A=C   CH2 0.04838 0.08642 
0.0041813.33E-03
functype[157]=LJ14, c6A=C   C   0.04838 0.04838 
0.002340624 2.34E-03


The values for N, C, O, H seems to be OK, but I have problems to get the
same value, when CH1, CH2, CH3 are involved. Since I do not have too
much experience, I would like to know how the value from the .tpr file
can be derived.

The other entry for LJ potential is the short range term LJ_SR (.tpr file

ffparams:
   atnr=11
   ntypes=170
  functype[0]=LJ_SR, c6= 9.61380266e-03, c12= 2.66462448e-05
  functype[1]=LJ_SR, c6= 4.74365894e-03, c12= 1.14699596e-05
  functype[2]=LJ_SR, c6= 4.66325786e-03, c12= 5.1618e-06

Unfortunately, I do not find the section where the function is assigned
to a specific pair of interaction. Where are these functions assigned to
a specific interaction? Furthermore, is it possible to distinguish
between intra-nonbonded (solute-solute) and inter-bonded (water-solute)
interaction?

For you this might be an easy question to answer, and you immediately
realize there is a beginner at work, but nevertheless I would appreciate
any help.

All the best
Otto




--
___
Patrick FUCHS
Dynamique des Structures et Interactions des Macromolécules Biologiques
INTS, INSERM UMR-S665, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-43-06-50-19
E-mail address: patrick.fu...@univ-paris-diderot.fr
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Re: [gmx-users] REST simulation

2011-12-12 Thread Patrick Fuchs
 intra-nonbonded (solute-solute) and inter-bonded (water-solute)
interaction?

For you this might be an easy question to answer, and you immediately
realize there is a beginner at work, but nevertheless I would appreciate
any help.

All the best
Otto




--
___
Patrick FUCHS
Dynamique des Structures et Interactions des Macromolécules Biologiques
INTS, INSERM UMR-S665, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-43-06-50-19
E-mail address: patrick.fu...@univ-paris-diderot.fr
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___
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Dynamique des Structures et Interactions des Macromolécules Biologiques
INTS, INSERM UMR-S665, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-43-06-50-19
E-mail address: patrick.fu...@univ-paris-diderot.fr
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Re: [gmx-users] REST simulation

2011-12-12 Thread Patrick Fuchs

Hi Mark,
good to know, this -pp option of grompp is very useful. Thanks!
Ciao,

Patrick

Le 12/12/2011 12:55, Mark Abraham a écrit :

On 12/12/2011 8:42 PM, Patrick Fuchs wrote:

Hi Otto,
in my lab we tried to implement this REST variant in GROMACS as
proposed by those authors. We figured out that it was easier to
manipulate directly the parameters files in the top directory. There
you know exactly what you are doing; recall that some interactions
(i.e. solvent/solvent) mustn't be scaled whereas some others have to
be scaled (solute/solute and solute/solvent).
It's probably possible to do it in the tpr file, but it looked less
trivial to me: i) you have to know how atoms are coded in the file
(e.g. in the functype[???]=LJ_SR[...] matrix, you have to understand
how atom numbers are coded there), ii) you have to regenerate a tpr
from plain text file; it's probably doable, but I don't know how.
Actually, maybe some developers can tell if it's possible.


It's possible, but far from desirable to attempt to manipulate the
contents of the .tpr directly.

Instead, use grompp -pp to write a complete stand-alone topology, which
you can then use as input to a script to do the appropriate solute
parameter scaling for each replica. Then use grompp normally on the new
set of .top files to generate a set of .tpr files that differ not only
in lambda but in their solute parameters.

Mark


Good luck,

Patrick

Le 08/12/2011 19:01, Otto Master a écrit :

Dear gromacs users,

Recently I stumbled over following paper:
T. Terakawa, T. Kameda, and S. Takada, On Easy Implementation of a
Variant of the Replica Exchange with Solute Tempering in GROMACS.
Journal of Computational Chemistry 32 (2011) 1228-1234.

The authors suggested an easy way to run this kind of simulation with
Gromacs, without even changing the code. The only thing that is need, is
the the rescaling of the parameters in the parameter file. Since the
reduction of the replica number is quite appealing to me I wonder which
file I have to change? Actually, I thought of manipulating the .tpr file
or to rescale and creating the force fields for every replicate. Is this
feasible, or is there a better way?

Manipulating the .tpr file could be easier, since it unifies (right?)
the parameters from the different force fields, before sending it to the
mdrun application. But for this I would like to understand the tpr file
first.There are quite a lot of entries and first I try to understand LJ
interactions and how they are defined in this file. I found two entries

LJ14
functype[154]=LJ14, c6A= 0.e+00, c12A= 0.e+00,
c6B= 0.e+00, c12B= 0.e+00
functype[155]=LJ14, c6A= 4.46680887e-03, c12A= 4.74702711e-06,
c6B= 4.46680887e-03, c12B= 4.74702711e-06

which corresponds to following interactions

LJ-14:
nr: 876
iatoms:
0 type=154 (LJ14) 0 4
1 type=155 (LJ14) 0 5

When I tried to calculate the parameters from the combination rules (in
this case Gromos 53A6 force field), I found (the highlighted columns
contain the original parameters for the specific atom groups from the
Gromos documentation and the calculated value for combining the two
parameters:




sqrt(C6i) (from ff) sqrt(C6j) (from ff) sqrt(C6i)*sqrt(C6j) value
from tpr file
functype[154]=LJ14, c6A= CH3 H 0.09805 0 0 0.00E+00
functype[155]=LJ14, c6A= CH3 CH1 0.09805 0.0779 0.007638095 4.47E-03
functype[156]=LJ14, c6A= C CH2 0.04838 0.08642 0.004181 3.33E-03
functype[157]=LJ14, c6A= C C 0.04838 0.04838 0.002340624 2.34E-03


The values for N, C, O, H seems to be OK, but I have problems to get the
same value, when CH1, CH2, CH3 are involved. Since I do not have too
much experience, I would like to know how the value from the .tpr file
can be derived.

The other entry for LJ potential is the short range term LJ_SR (.tpr
file

ffparams:
atnr=11
ntypes=170
functype[0]=LJ_SR, c6= 9.61380266e-03, c12= 2.66462448e-05
functype[1]=LJ_SR, c6= 4.74365894e-03, c12= 1.14699596e-05
functype[2]=LJ_SR, c6= 4.66325786e-03, c12= 5.1618e-06

Unfortunately, I do not find the section where the function is assigned
to a specific pair of interaction. Where are these functions assigned to
a specific interaction? Furthermore, is it possible to distinguish
between intra-nonbonded (solute-solute) and inter-bonded (water-solute)
interaction?

For you this might be an easy question to answer, and you immediately
realize there is a beginner at work, but nevertheless I would appreciate
any help.

All the best
Otto








--
___
Patrick FUCHS
Dynamique des Structures et Interactions des Macromolécules Biologiques
INTS, INSERM UMR-S665, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-43-06-50-19
E-mail address: patrick.fu...@univ-paris-diderot.fr
Web Site: http://www.dsimb.inserm.fr/~fuchs
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Re: [gmx-users] compressing a box of water droplets into a homogeneous solution of liquid water

2011-03-24 Thread Patrick Fuchs

Hi Chris,
I fully agree with your analysis about the effect of non-bonded 
interactions that accelerate the collapse when the layer of vacuum 
around the system is thin. I also observed that it is way faster to 
reach equilibrium density in this case.

Ciao,

Patrick

Le 23/03/2011 21:06, chris.ne...@utoronto.ca a écrit :

Thanks Patrick and Andre!

We repeated this with a few box sizes just to get a quick handle on it.
The equilibrium volume is about 64 nm^3. If we start with a volume of
1000 nm^3 then the overall box does not collapse at all within 200 ps of
NPT Langevin dynamics at 1 atm.If we start with a volume of 200 nm^3,
then it does collapse to approximately 64 nm^3 within 200 ps of such
simulation.

My best guess is that the rapid collapse is driven by nonbonded
interactions and thus the rapid collapse does not occur when the system
is so large with such low density that water forms isolated vapour
droplets that do not interact with each other by LJ interactions. Sure,
it is expected to collapse eventually from the 1 atm pressure coupling,
and we have also observed that high pressure works, but at 1 atm it
might take a very long time to reach equilibrium.

I agree with Andre that none of this matters to regular simulations as
there is no good reason to go through this type of state when one wants
to simulate dense liquids. I just found it curious that Berendsen
pressure coupling at 1 atm was not sufficient to quickly equilibrate the
volume in a system where the vacuum regions are large in comparison to
the LJ cutoffs.

Chris.

-- original message --

Hi Chris,
I experienced the same kind of thing. In the process of building a box
of liquid (organic solvent), at some point I wanted to get rid of a
layer of vacuum around my system. So for shrinking the box I used
similar settings as you and found also that the collapse was going
slower than I'd have expected.
One solution to accelerate this (if your goal is to shrink the box) is
to increase the pressure (to say 100 atm). But it's important to stop
the simulation in time (i.e. once the layer of vacuum has disapeared)
otherwise the system shrinks too much and density is off.
So to come back to your system which has a very big layer of vacuum
around, and according to my experience, the volume is probably
decreasing but too slowly to see anything signigicant (compared to the
initial value) in 200 ps .
Ciao,

Patrick

Le 21/03/2011 16:53, chris.ne...@utoronto.ca a écrit :

[Hide Quoted Text]
Dear users:

I recently came across a system that was composed of tip4p water vapor
droplets separated by vacuum. This system is what you might get if you
did a NVT simulation of water with a box that was 10 times too large for
the number of water molecules.

I was surprised to see that this system did not collapse to any
significant extent during 200 ps of NPT equilibration at 1 atm using the
Berendsen thermostat with tau_p=1.0 and the sd integrator and a colombic
cut-off. (We also tried a number of other integrator/pressure coupling
combinations with the same results).

I had assumed that such collapse would occur quite rapidly. This does
not seem to be the case (no noticeable contraction within 200 ps).

Has anybody else done anything like this? Can anybody comment on their
expectations/experience of collapse from the gas state to the liquid
state under standard NPT conditions?

Thank you,
Chris.



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 new E-mail address: patrick.fu...@univ-paris-diderot.fr 
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Dynamique des Structures et Interactions des Macromolécules Biologiques
INTS, INSERM UMR-S665, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-47-34-74-31
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Re: [gmx-users] compressing a box of water droplets into a homogeneous solution of liquid water

2011-03-23 Thread Patrick Fuchs

Hi Chris,
I experienced the same kind of thing. In the process of building a box 
of liquid (organic solvent), at some point I wanted to get rid of a 
layer of vacuum around my system. So for shrinking the box I used 
similar settings as you and found also that the collapse was going 
slower than I'd have expected.
One solution to accelerate this (if your goal is to shrink the box) is 
to increase the pressure (to say 100 atm). But it's important to stop 
the simulation in time (i.e. once the layer of vacuum has disapeared) 
otherwise the system shrinks too much and density is off.
So to come back to your system which has a very big layer of vacuum 
around, and according to my experience, the volume is probably 
decreasing but too slowly to see anything signigicant (compared to the 
initial value) in 200 ps .

Ciao,

Patrick

Le 21/03/2011 16:53, chris.ne...@utoronto.ca a écrit :

Dear users:

I recently came across a system that was composed of tip4p water vapor
droplets separated by vacuum. This system is what you might get if you
did a NVT simulation of water with a box that was 10 times too large for
the number of water molecules.

I was surprised to see that this system did not collapse to any
significant extent during 200 ps of NPT equilibration at 1 atm using the
Berendsen thermostat with tau_p=1.0 and the sd integrator and a colombic
cut-off. (We also tried a number of other integrator/pressure coupling
combinations with the same results).

I had assumed that such collapse would occur quite rapidly. This does
not seem to be the case (no noticeable contraction within 200 ps).

Has anybody else done anything like this? Can anybody comment on their
expectations/experience of collapse from the gas state to the liquid
state under standard NPT conditions?

Thank you,
Chris.



--
___
 new E-mail address: patrick.fu...@univ-paris-diderot.fr 
Patrick FUCHS
Dynamique des Structures et Interactions des Macromolécules Biologiques
INTS, INSERM UMR-S665, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-47-34-74-31
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Re: [gmx-users] Can g_wham support using different temperature for different windows?

2011-02-23 Thread Patrick Fuchs
 along the reaction coordinates, which
is the z-distance
   between peptide and membrane. This figure
(http://www.flickr.com/photos/lijg/5467080971/) shows some of the
configurations at certain reaction coordinates.
  
 
  Are you not sampling configurations outside of the membrane (i.e. in
water)? I would think that would solve your problem. You don't show any
configurations in which the peptide is completely dissociated from the
membrane. I don't know your objectives, but I would think that if you
could completely extract the peptide from the membrane after passing
through it, this would solve your problem.
 
   (2) In each window, I used the corresponding configuration that
generated by the pulling simulation as initial input and run umbrella
sampling. The size of each window is 0.15 nm, but close to the bilayer
cneter (e.g., -0.6d0.6), I have
   increased number of windows so that the width of the window is to
be 0.05 or 0.1 nm, I also tried to use different force constant in these
windows.
  
   From the figure (http://www.flickr.com/photos/lijg/5467080971/) ,
we can classify the peptide conformation to be either extended
(interacting with two bilayers) or compact (interacting with only one
bilayer). Ideally, the peptide conformation should be similar for d=x
and d=-x. The problem is that the configuration of peptide is not
symmetric with respect to the bilayer center. For example, the peptide
configuration is compact at d=0.6 and d=0.9, but the peptide is extended
at d=-0.6 and d=-0.9. This leads Hysteresis. If I use g_wham to generate
PMF, then the PMF is not symmetric with respect to the bilayer center.
Using more number of windows and different force constant did not remove
the problem.
  
   In my opinion, at least in some windows, the peptide should sample
both compact and extended structure. But what I found is that the windowed
 
  Don't pre-judge the model :) Also, as I said before, there is no
reason to suspect that MARTINI will produce any meaningful secondary
structure changes. It was not parameterized to do so.
 
   umbrella simulation depends on the initial peptide conformation. If
the initial peptide conformation is compact, then after 100 ns, it is
still compact; if the initial peptide in that window is extended, the
final configuration is also extended. I also tried to run longer
equilibrium time (e.g., 200 ns), but the problem still exists.
  
 
  Sounds like a limitation of the force field model.
 
   My question is how to increase sampling of the peptide
conformation? I just think of two choices:
   (1) use high temperature (e.g., 500K) at those bad windows. As I
mentioned, I am wondering if g_wham can unbias the effect of using
different temperatures in different windows.
   (2) use REMD in those bad windows. These need a lot of
computational resources.
  
 
  Neither of these will be useful in generating a sensible PMF curve.
WHAM needs a single temperature for proper weighting. If you start
including different temperatures in different regions of phase space, I
would imagine the weighting would be completely incorrect.
 
  Note that SMD is not the only option for generating starting
configurations. If you think that certain orientations or configurations
are correct, you can build them yourself, but keep in mind that you'll
have to justify this procedure to a skeptical audience.
 
  -Justin
 
   Is there any other method to deal with the insufficient sampling?
   Any suggestions are welcome, thanks for your time reading this email!
  
   Cheers,
   Jianguo
  
  
  

   *From:* Justin A. Lemkul jalem...@vt.edu mailto:jalem...@vt.edu
mailto:jalem...@vt.edu mailto:jalem...@vt.edu
   *To:* Gromacs Users' List gmx-users@gromacs.org
mailto:gmx-users@gromacs.org mailto:gmx-users@gromacs.org
mailto:gmx-users@gromacs.org
   *Sent:* Tuesday, 22 February 2011 11:13:05
   *Subject:* Re: [gmx-users] Can g_wham support using different
temperature for different windows?
 



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Dynamique des Structures et Interactions des Macromolécules Biologiques
INTS, INSERM UMR-S665, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-47-34-74-31
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Re: [gmx-users] InflateGRO and trimer simulation

2010-01-10 Thread patrick fuchs

Hi,
the new inflategro with the 'doughnut mode'
(http://www.csb.bit.uni-bonn.de/inflategro.html) might do what you want.
Ciao,

Patrick

Justin A. Lemkul a écrit :



On 1/10/10 5:17 AM, KM wrote:

Hello Gromacs Users,

I would like to run a simulation of a trimer in a DPPC membrane. I
really like the elegant solution that inflategro script offers,
however I'm afraid I won't be able to use it, because I need to have
lipids in a small space between the monomers right in the center of
the box and these will certainly get deleted during the whole
procedure. I also need to keep the waters that come with the structure
of the protein.
Do you have any idea how I can elegantly embed my trimer in a
membrane, possibly using somehow modified inflategro?

Christopher


I've built multimeric systems with InflateGRO, but with a lot less 
constraints than you have :)  You can, for instance, run an inflation 
step with a very minimal scaling factor (like 1.01 or 1.05) and a very 
small cutoff (7 or so, but you'd have to play around with this) so you 
essentially delete lipids in place without moving them too much.  I 
don't know if the necessary lipids between the monomers will be affected.


As for preserving water molecules, you could probably just extract their 
coordinates from a suitably-oriented starting structure and paste them 
into the InflateGRO output.


None of this requires modifying InflateGRO, but will likely require a 
lot of trial and error, if it even works, given the very specific nature 
of what you need.


-Justin



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Dynamique des Structures et Interactions des Macromolécules Biologiques
INTS, INSERM UMR-S665, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-47-34-74-31
Web Site: http://www.dsimb.inserm.fr/~fuchs
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Re: [gmx-users] P-N vector orientation

2009-02-13 Thread patrick fuchs

Hi,
as Nicolas suggested you can use my program g_tilt to do such an 
analysis. Instead of giving the whole backbone as a selection, simply 
give the 2 atoms (P  N). Initially g_tilt uses the first eigen vector 
of the inertia matrix of the atom selection, so you might want to 
simplify the code to calculate the PN vector (using [xN-xP,yN-yP,zN-zP]).

Ciao,

Patrick

Nicolas a écrit :

Hello,

I just remember that you might be interested by g_tilt developed by 
Patrick Fuchs.:


   http://www.dsimb.inserm.fr/~fuchs/download/
   http://www.dsimb.inserm.fr/%7Efuchs/download/

Its purpose is to calculate the orientation of an helix in a bilayer, 
however it might tweaked to calculate the NP dipole orientation. I've 
done that one time, but it was only for a particular lipid in a 
membrane, not for the whole bilayer. IIRW, the result was the same than 
the one of my scripts and the calculation was much faster.


Nicolas

ANINDITA GAYEN a écrit :

Dear Xavier Periole
 I am a GROMACS user, presently working with DMPC  
bilayer.. I want to calculate the orientation of the head groups P-N 
vector. From gmx-users,  I have came to know that you have a program 
that can determine the angle of the PN vector (or what ever pair of 
atoms) relative to the z axis.
If possible, can you please provide me that program or tell me how can 
i calculate that?


Thanks in advance.

Ms. Anindita Gayen
C/O Dr. Chaitali Mukhopadhyay
Senior Research Fellow
Department of Chemistry
University of Calcutta
92, A. P. C. Road
Kolkata-700 009
India



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Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?

2009-01-14 Thread patrick fuchs
 in lam_ssi_rpi_usysv_proc_read_env ()
Missing separate debuginfos, use: debuginfo-install
e2fsprogs-libs-1.41.3-2.fc10.x86_64 glibc-2.9-3.x86_64
libICE-1.0.4-4.fc10.x86_64 libSM-1.1.0-2.fc10.x86_64
libX11-1.1.4-6.fc10.x86_64 libXau-1.0.4-1.fc10.x86_64
libXdmcp-1.0.2-6.fc10.x86_64 libxcb-1.1.91-5.fc10.x86_64
(gdb) where
#0 0x00770c70 in lam_ssi_rpi_usysv_proc_read_env ()
#1 0x00784a39 in lam_ssi_rpi_usysv_advance_common ()
#2 0x0074a1e0 in _mpi_req_advance ()
#3 0x0073ea90 in MPI_Wait ()
#4 0x0074d800 in MPI_Sendrecv ()
#5 0x004aebfd in gmx_sum_qgrid_dd ()
#6 0x004b40bb in gmx_pme_do ()
#7 0x00479a58 in do_force_lowlevel ()
#8 0x004d1d32 in do_force ()
#9 0x004214d2 in do_md ()
#10 0x0041bea0 in mdrunner ()
#11 0x00422b94 in main ()
(gdb)
===
   
   
Cheers,
   
Patrick
   
  
  
   


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Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?

2009-01-13 Thread patrick fuchs
...?
Cheers,
   
Patrick
   
Berk Hess a écrit :
 Hi,

 If your simulations no longer produce output, but still run
 and there is no error or warning message,
 my guess would be that they are waiting for MPI communication.
 But the developers any many users are using 4.0 and I have
 not heard from problems like this, so I wonder if the problem
 could be somewhere else.

 Could you (or have your tried to) continue your simulation
 from the last checkpoint (mdrun option -cpi) before the hang,
 to see if it crashes quickly then?

 Berk

  Date: Fri, 12 Dec 2008 13:42:43 +0100
  From: bernhard.kn...@meduniwien.ac.at
  To: gmx-users@gromacs.org
  Subject: Subject: Re: Re: [gmx-users] Gromacs 4 bug?
 
  Mark wrote:
 
   What's happening in the log files? What's the latest
   information in
 the
   checkpoint files? Could there be some issue with file system
 availability?
 
  Hi Mark
 
  Unfortunaltey I already deleted the simulation files which 
got stuck
  after 847ps. But here is the output of another simulation 
done on the
  same system but with an other pdb file. This one gets stuck 
after

   179ps
  with the following output:
 
  The latest thing the checkpoint file says is:
 
  imb F 3% step 89700, will finish Wed Jul 1 09:11:00 2009
  imb F 3% step 89800, will finish Wed Jul 1 09:02:51 2009
 
  The predcition for 1st of July is not surprising since I am 
always
  parameterizing the simulation with 200ns to avoid to restart 
it if

  something interesting happens in the last frames.
 
  for the .log file it is:
 
  Writing checkpoint, step 88000 at Thu Dec 11 16:34:31 2008
 
  Energies (kJ/mol)
  G96Angle Proper Dih. Improper Dih. LJ-14 Coulomb-14
  7.83753e+03 3.64068e+03 2.45951e+03 1.29167e+03 5.13688e+04
  LJ (SR) Coulomb (SR) Coul. recip. Potential Kinetic En.
  3.82346e+05 -2.48883e+06 -3.51313e+05 -2.39119e+06 4.57648e+05
  Total Energy Temperature Pressure (bar) Cons. rmsd ()
  -1.93355e+06 3.10014e+02 1.09267e-01 2.14030e-05
 
  DD step 88999 load imb.: force 3.1%
 
  Step Time Lambda
  89000 178.2 0.0
 
  Energies (kJ/mol)
  G96Angle Proper Dih. Improper Dih. LJ-14 Coulomb-14
  8.03089e+03 3.59681e+03 2.42628e+03 1.20942e+03 5.12341e+04
  LJ (SR) Coulomb (SR) Coul. recip. Potential Kinetic En.
  3.81539e+05 -2.48602e+06 -3.51307e+05 -2.38929e+06 4.56901e+05
  Total Energy Temperature Pressure (bar) Cons. rmsd ()
  -1.93239e+06 3.09508e+02 1.64627e+01 2.08518e-05
 
 
  the disk is also free df -h says 2.3G out of 666G used.
 
  The only difference between the system with gromacs 3.3 and
   gromacs 4 is
  that gromacs 4 is running under suse 11 while gromacs 3.3 is
   running on
  a node with suse 10. But I dont think this can be the problem?
 
  cheers
  Bernhard
 
 
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Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?

2009-01-13 Thread patrick fuchs
 
 new postal address !!!
Patrick FUCHS
Equipe de Bioinformatique Genomique et Moleculaire
INTS, INSERM UMR-S726, Université Paris Diderot,
6 rue Alexandre Cabanel, 75015 Paris
Tel : +33 (0)1-44-49-30-57 - Fax : +33 (0)1-47-34-74-31
Web Site: http://www.dsimb.inserm.fr/~fuchs
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Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?

2009-01-08 Thread patrick fuchs

Hi Berk,
I tried this fix, but mdrun_mpi is still hanging. I'll try to use the 
debugger by the end of the week and let you know.

Cheers,

Patrick

Berk Hess a écrit :

Hi,

My guess is that this is not the problem.
But it is very easy to try, so please do.
The diff for src/gmxlib/pbc.c is:
392c392,393
 try[d] == 0;
---
  try[d] = 0;
  pos[d] = 0;

Berk

  Date: Tue, 6 Jan 2009 18:37:20 +0100
  From: patrick.fu...@univ-paris-diderot.fr
  To: gmx-users@gromacs.org
  Subject: Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?
 
  Hi,
 
   I also fixed a problem with unitialized variables for pbc calculations
   in trilinic boxes.
   But up till now I have not observed any effect of this bug.
   Is your box triclinic?
  Yes it is. So shall I test your corrected version ?
 
  Patrick
 



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Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?

2009-01-06 Thread patrick fuchs
 it is:
   
Writing checkpoint, step 88000 at Thu Dec 11 16:34:31 2008
   
Energies (kJ/mol)
G96Angle Proper Dih. Improper Dih. LJ-14 Coulomb-14
7.83753e+03 3.64068e+03 2.45951e+03 1.29167e+03 5.13688e+04
LJ (SR) Coulomb (SR) Coul. recip. Potential Kinetic En.
3.82346e+05 -2.48883e+06 -3.51313e+05 -2.39119e+06 
4.57648e+05

Total Energy Temperature Pressure (bar) Cons. rmsd ()
-1.93355e+06 3.10014e+02 1.09267e-01 2.14030e-05
   
DD step 88999 load imb.: force 3.1%
   
Step Time Lambda
89000 178.2 0.0
   
Energies (kJ/mol)
G96Angle Proper Dih. Improper Dih. LJ-14 Coulomb-14
8.03089e+03 3.59681e+03 2.42628e+03 1.20942e+03 5.12341e+04
LJ (SR) Coulomb (SR) Coul. recip. Potential Kinetic En.
3.81539e+05 -2.48602e+06 -3.51307e+05 -2.38929e+06 
4.56901e+05

Total Energy Temperature Pressure (bar) Cons. rmsd ()
-1.93239e+06 3.09508e+02 1.64627e+01 2.08518e-05
   
   
the disk is also free df -h says 2.3G out of 666G used.
   
The only difference between the system with gromacs 3.3 and
 gromacs 4 is
that gromacs 4 is running under suse 11 while gromacs 3.3 is
 running on
a node with suse 10. But I dont think this can be the 
problem?

   
cheers
Bernhard
   
   
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6 rue Alexandre Cabanel, 75015 Paris
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Please

Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?

2009-01-06 Thread patrick fuchs
 I already deleted the simulation files 
which

 got stuck
  after 847ps. But here is the output of another simulation
 done on the
  same system but with an other pdb file. This one gets 
stuck

 after
   179ps
  with the following output:
 
  The latest thing the checkpoint file says is:
 
  imb F 3% step 89700, will finish Wed Jul 1 09:11:00 2009
  imb F 3% step 89800, will finish Wed Jul 1 09:02:51 2009
 
  The predcition for 1st of July is not surprising 
since I am

 always
  parameterizing the simulation with 200ns to avoid to 
restart

 it if
  something interesting happens in the last frames.
 
  for the .log file it is:
 
  Writing checkpoint, step 88000 at Thu Dec 11 
16:34:31 2008

 
  Energies (kJ/mol)
  G96Angle Proper Dih. Improper Dih. LJ-14 Coulomb-14
  7.83753e+03 3.64068e+03 2.45951e+03 1.29167e+03 
5.13688e+04

  LJ (SR) Coulomb (SR) Coul. recip. Potential Kinetic En.
  3.82346e+05 -2.48883e+06 -3.51313e+05 -2.39119e+06
   4.57648e+05
  Total Energy Temperature Pressure (bar) Cons. rmsd ()
  -1.93355e+06 3.10014e+02 1.09267e-01 2.14030e-05
 
  DD step 88999 load imb.: force 3.1%
 
  Step Time Lambda
  89000 178.2 0.0
 
  Energies (kJ/mol)
  G96Angle Proper Dih. Improper Dih. LJ-14 Coulomb-14
  8.03089e+03 3.59681e+03 2.42628e+03 1.20942e+03 
5.12341e+04

  LJ (SR) Coulomb (SR) Coul. recip. Potential Kinetic En.
  3.81539e+05 -2.48602e+06 -3.51307e+05 -2.38929e+06
   4.56901e+05
  Total Energy Temperature Pressure (bar) Cons. rmsd ()
  -1.93239e+06 3.09508e+02 1.64627e+01 2.08518e-05
 
 
  the disk is also free df -h says 2.3G out of 666G used.
 
  The only difference between the system with gromacs 
3.3 and

   gromacs 4 is
  that gromacs 4 is running under suse 11 while gromacs 
3.3 is

   running on
  a node with suse 10. But I dont think this can be the
   problem?
 
  cheers
  Bernhard
 
 
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Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?

2008-12-17 Thread patrick fuchs
 2.42628e+03 1.20942e+03 5.12341e+04
  LJ (SR) Coulomb (SR) Coul. recip. Potential Kinetic En.
  3.81539e+05 -2.48602e+06 -3.51307e+05 -2.38929e+06 4.56901e+05
  Total Energy Temperature Pressure (bar) Cons. rmsd ()
  -1.93239e+06 3.09508e+02 1.64627e+01 2.08518e-05
 
 
  the disk is also free df -h says 2.3G out of 666G used.
 
  The only difference between the system with gromacs 3.3 and
   gromacs 4 is
  that gromacs 4 is running under suse 11 while gromacs 3.3 is
   running on
  a node with suse 10. But I dont think this can be the problem?
 
  cheers
  Bernhard
 
 
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Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?

2008-12-15 Thread patrick fuchs

Hi,
I have exactly the same problem under Fedora 9 on a dual-quadricore 
(Intel Xeon E5430, 2.66 GHz) computer. Gromacs-4.0.2 is hanging (same 
for gromacs-4.0.0) after a couple of minutes of simulation. Sometimes, 
it even hangs very quickly before the simulation reaches the writing of 
the first checkpoint file (in fact the time length before the hang 
occurs is chaotic, sometimes a couple of minutes, or a few seconds). The 
CPUs are still loaded but nothing goes to the output (on any file log, 
xtc, trr, edr...). All gromacs binaries were standardly compiled with 
--enable-mpi and the latest lam-7.1.4. As Bernhard and Antoine I don't 
see anything strange in the log file.
I have another computer single quadricore (Intel Xeon E5430, 2.66 GHz) 
under Fedora 8 and the same system (same mdp, topology etc...) is 
running fine with gromacs-4.0.2 (compiled with lam-7.1.4 as well). So 
would it be possible that there's something wrong going on with FC9 and 
lam-7.1.4...?

Cheers,

Patrick

Berk Hess a écrit :

Hi,

If your simulations no longer produce output, but still run
and there is no error or warning message,
my guess would be that they are waiting for MPI communication.
But the developers any many users are using 4.0 and I have
not heard from problems like this, so I wonder if the problem
could be somewhere else.

Could you (or have your tried to) continue your simulation
from the last checkpoint (mdrun option -cpi) before the hang,
to see if it crashes quickly then?

Berk

  Date: Fri, 12 Dec 2008 13:42:43 +0100
  From: bernhard.kn...@meduniwien.ac.at
  To: gmx-users@gromacs.org
  Subject: Subject: Re: Re: [gmx-users] Gromacs 4 bug?
 
  Mark wrote:
 
   What's happening in the log files? What's the latest information in 
the
   checkpoint files? Could there be some issue with file system 
availability?

 
  Hi Mark
 
  Unfortunaltey I already deleted the simulation files which got stuck
  after 847ps. But here is the output of another simulation done on the
  same system but with an other pdb file. This one gets stuck after 179ps
  with the following output:
 
  The latest thing the checkpoint file says is:
 
  imb F 3% step 89700, will finish Wed Jul 1 09:11:00 2009
  imb F 3% step 89800, will finish Wed Jul 1 09:02:51 2009
 
  The predcition for 1st of July is not surprising since I am always
  parameterizing the simulation with 200ns to avoid to restart it if
  something interesting happens in the last frames.
 
  for the .log file it is:
 
  Writing checkpoint, step 88000 at Thu Dec 11 16:34:31 2008
 
  Energies (kJ/mol)
  G96Angle Proper Dih. Improper Dih. LJ-14 Coulomb-14
  7.83753e+03 3.64068e+03 2.45951e+03 1.29167e+03 5.13688e+04
  LJ (SR) Coulomb (SR) Coul. recip. Potential Kinetic En.
  3.82346e+05 -2.48883e+06 -3.51313e+05 -2.39119e+06 4.57648e+05
  Total Energy Temperature Pressure (bar) Cons. rmsd ()
  -1.93355e+06 3.10014e+02 1.09267e-01 2.14030e-05
 
  DD step 88999 load imb.: force 3.1%
 
  Step Time Lambda
  89000 178.2 0.0
 
  Energies (kJ/mol)
  G96Angle Proper Dih. Improper Dih. LJ-14 Coulomb-14
  8.03089e+03 3.59681e+03 2.42628e+03 1.20942e+03 5.12341e+04
  LJ (SR) Coulomb (SR) Coul. recip. Potential Kinetic En.
  3.81539e+05 -2.48602e+06 -3.51307e+05 -2.38929e+06 4.56901e+05
  Total Energy Temperature Pressure (bar) Cons. rmsd ()
  -1.93239e+06 3.09508e+02 1.64627e+01 2.08518e-05
 
 
  the disk is also free df -h says 2.3G out of 666G used.
 
  The only difference between the system with gromacs 3.3 and gromacs 4 is
  that gromacs 4 is running under suse 11 while gromacs 3.3 is running on
  a node with suse 10. But I dont think this can be the problem?
 
  cheers
  Bernhard
 
 
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Re: Subject: Re: Re: [gmx-users] Gromacs 4 bug?

2008-12-15 Thread patrick fuchs
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Re: [gmx-users] flexible organic solvents

2008-08-20 Thread patrick fuchs

Hi,
additionally to the remaks of Andreas there are some parameters in the 
GROMOS force field G53a5/6 for the solvents you want to simulate (see 
the original paper). A good read of chapter five of the manual and to 
all the files in the $GMX/share/top directory should let you build those 
models. Note there's also a decane.itp there, which uses the 
Ryckaert-Bellemans potential (as in Berger lipids).
One comment on the chair to boat (or more exactly twist-boat) 
transition, the enthalpy barrier has been estimated to ~ 10 kcal/mol by 
ab initio and MM2 calculations. It is thus unlikely to observe any 
transition within a few nanoseconds if you start from a chair 
conformation at room temperature.

Ciao,

Patrick

Kukol, Andreas a écrit :

Yes that should be possible without big problems. The Gromacs manual and Wiki 
pages about how to build a topology is a good starting point.

Then you could try the gromacs program x2top to generate a topology, or the 
Prodrg2 server.

Andreas


-Original Message-
From: [EMAIL PROTECTED] [mailto:[EMAIL PROTECTED]
On Behalf Of Sascha Rehm
Sent: 14 August 2008 12:03
To: gmx-users@gromacs.org
Subject: [gmx-users] flexible organic solvents

Dear Gromacs users,

I simulate proteins with different organic solvents like toluene,
cyclohexane or isopentane. Right now, I used rigid body models for these
solvents, made and simulated with Amber. For my future work, I unse
Gromacs and need to rebuild these solvents.

Can I build a cyclohexane model, which is more flexible and can change
from chair conformation to boat conformation and vice versa? And how do
I build a non-rigid Isopentane with internal degrees of freedom?

Hope, this is not a stupid questions, but I searched quite a while the
mailing list and also google, but did nearly find nothing about other
common (flexible) solvents.
Can someone give me a hint, which keywords I should use to search or
where I can find some informations/tutorials/explanations?

Thanks a lot,

Sascha
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Re: [gmx-users] Problem with lipid simulations

2008-04-01 Thread patrick fuchs

Hi Chandu,
this looks like you have two statements #include lipid.itp, so check 
all your *.top and *.itp files.

Ciao,

Patrick

[EMAIL PROTECTED] a écrit :

Dear All,
I have been trying to simulate a small peptide in a DMPC lipid bylayer.
Same setup is working fine in one computer (cluster) but I am getting the
following error message in another cluster.
grompp_mpi -f test.mdp -c lipid_protein.gro -p topology.top -o test.tpr


checking input for internal consistency...
calling /lib/cpp...
processing topology...
WARNING 1 [file lipid.itp, line 14]:
  Overriding atomtype LO
WARNING 2 [file lipid.itp, line 15]:
  Overriding atomtype LOM
WARNING 3 [file lipid.itp, line 16]:
  Overriding atomtype LNL
WARNING 4 [file lipid.itp, line 17]:
  Overriding atomtype LC
WARNING 5 [file lipid.itp, line 18]:
  Overriding atomtype LH1
WARNING 6 [file lipid.itp, line 19]:
  Overriding atomtype LH2
WARNING 7 [file lipid.itp, line 20]:
  Overriding atomtype LP
WARNING 8 [file lipid.itp, line 21]:
  Overriding atomtype LOS
WARNING 9 [file lipid.itp, line 22]:
  Overriding atomtype LP2
WARNING 10 [file lipid.itp, line 23]:
  Overriding atomtype LP3
Cleaning up temporary file grompp16bicP
---
Program grompp_mpi, VERSION 3.3.1
Source code file: fatal.c, line: 416

Fatal error:
Too many warnings, grompp_mpi terminated
---

Please let me know how to get rid of this problem.

Thanks in advance

Regards
Chandu



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Re: [gmx-users] Gromacs force field discussion

2008-03-03 Thread patrick fuchs

Hi David,
since updated GROMOS force fields are now available within GROMACS, I
agree one does not need to use ffgmx, at least for standard simulations.
The only problem is for lipid/protein simulations. The only publicly
available I know that runs under GROMACS is the combination of Berger
lipids with ffgmx (on the website of Peter Tieleman). For someone
starting a project of lipid/protein simulations, there is a priori no
other public alternative (using GROMACS), although I know some new
parameters are about to be published.
Cheers,

Patrick

David van der Spoel a écrit :

Reay, Andrew wrote:

Hi,
I am trying to find out why the Gromacs force field is no longer 
recommended for use.  I've searched the mailing list archives for 
quite awhile to find the discussion but have been unsuccessful.  Can 
anybody tell me where to find that discussion?  Thanks very much.


The never has bee a GROMACS force field, although we named it such to 
avoid confusion with official GROMOS force fields. What used to be 
called the GROMACS force field was basically GROMOS87 + changes due to 
Van Buuren  Berendsen (J.Phys.Chem. 97 [1993] 9206) plus changes on 
aromatic groups from an unpublished paper from the Van Gusteren group 
(these parameters are given in my paper in J.Biomol. NMR  8 (1996) 
p.229). This is described in the manual. In other words there is no good 
description of ths force field in a single paper. For good reasons the 
Van Gunsteren group have updated their GROMOS force field on a number of 
occasions, and these force field are now supported in GROMACS, along 
with a few others. Although it is still possible to use the old 
parameter set, please do not call it The GROMACS force field, but use 
the description above. Most referees fro scientific papers will (should) 
raise their eyebrows when reading that this parameter set was used, so 
this is another reason to shy away from it.




Andy
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Re: [gmx-users] g_dist producing inconsistent values

2008-02-08 Thread Patrick Fuchs

Hi,
another quick and dirty tip (but at least it works !) is to generate a 
new trajectory using trjconv with a huge layer of vacuum on the Z 
direction (assuming your membrane normal is oriented along Z): you can 
do that with the -box option with a large value for Z. If you just put 
only the phosphorous atoms in there this won't generate a large file.

Cheers,

Patrick

Alan Dodd a écrit :

- Original Message 
From: David van der Spoel [EMAIL PROTECTED]
To: Discussion list for GROMACS users gmx-users@gromacs.org
Sent: Thursday, February 7, 2008 6:35:55 PM
Subject: Re: [gmx-users] g_dist producing inconsistent values

[EMAIL PROTECTED] wrote:
I've since found the source of my problem - the program was measuring 
the (marginally shorter) distance across the PBC boundary, rather than 
the distance
within the box.  Unfortunately there doesn't seem to be a way to turn 
PBC images off (correct me if I'm wrong?), so I guess I'm going to do 
some jiggerypokery with the data and some math.
Distance larger than half a box size are ill-defined anyway in a PBC 
simulation. 


-What do you mean?  I'd assumed that simply having enough water separating a 
bilayer from its periodic image that no water 'saw' both bilayers would be 
sufficient; is this not the case?



In some special cases you can do this, for instance within a 
protein it would work. I've implemented -nopbc options in some programs 
but not in g_dist yet. Please put it on the developer wishlist. on the wiki.


-Done.  Until then, I'm using g_traj -ox -com and doing the math with my own 
script.  Many thanks for the various alternative techniques suggested.


  

Never miss a thing.  Make Yahoo your home page. 
http://www.yahoo.com/r/hs

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Re: [gmx-users] About g_msd

2008-01-16 Thread Patrick Fuchs
/users.php







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


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Re: [gmx-users] About g_msd (and noise)

2008-01-16 Thread Patrick Fuchs
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Re: [gmx-users] Re: Where is the GROMOS87 force field when using pdb2gmx

2007-11-08 Thread Patrick Fuchs

Hi Erik,
but I did read many works in the literature that used G43a*, even yours 
in BJ (2006). I basically agree that the 'philosophy' of the Berger 
lipids is derived from OPLS, thus using this latter force field is 
probably best suited for peptide/lipid simulation in conjunction with 
Berger lipids (like in Tieleman et al 2006 J. Phys.: Condens. Matter 18 
S1221-S1234, or your last paper in press in Proteins). But apart from 
self-consistency, is it so a problem to mix Berger lipids with a GROMOS 
derived force field ? I ask you that because *many* previous works used 
Berger lipids with ffgmx (and this latter is probably still in use even 
if deprecated). So what is right ?
It would probably be worth doing a systematic comparison of the use of 
different protein force fields with Berger lipids. The above ref of P. 
Tieleman goes in this direction.

Cheers,

Patrick

Erik Lindahl a écrit :

Hi,

On Nov 7, 2007, at 5:40 PM, maria goranovic wrote:


Thanks for the help, David. Actually, I just realized I was trying to
decide based on mailing list archives which, in some cases, are 5
years old. My mistake. I will use the 43a2 field for my protein.

Is there any standard procedure to combine 43a2 with the berger force
field (ffgmx) for lipids ?


Don't do it. The berger force field is mostly derived from OPLS, so 
you will (again) find it much easier to defend your choices if you mix 
it with OPLS-AA/L instead.


Cheers,

Erik

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Re: [gmx-users] what is the force function for proper dihedrals

2007-08-31 Thread Patrick Fuchs

Hi Chris,
I've been searching for this as well. You might get some clues in the 
following article, but I didn't have time to read it:
T. Schlick, A Recipe for Evaluating and Differentiating Cos phi 
Expressions,   J. Comp. Chem.,  10:951-956, May (1989)

I'm interested if you find any pointer to a book or paper on this issue.
Cheers,

Patrick

Chris Neale a écrit :

Hello,

The manual does a good job at explaining the potential energy function 
for all types of interactions. For bonded interactions the manual also 
describes the force function for every type except dihedrals. The 
Allan and Tildesley bool also lacks this information. It's one thing 
to know that the force is the negative gradient of the potential 
energy, but for proper dihedrals it is not trivial to determine this.


If anybody knows the force function for proper dihedrals then I would 
greatly appreciate a reply.


Thanks,
Chris.
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Re: [gmx-users] g_bundle!

2007-06-20 Thread Patrick Fuchs

Hi,
I wrote a program to calculate the tilt angle between a helix axis and 
the bilayer normal called g_tilt. It's available here 
http://condor.ebgm.jussieu.fr/~fuchs/download/. There you'll find also a 
program to calculate the azimuthal rotation (g_rotation).
I plan to upload these contributions on the GROMACS website when I have 
time :-)

Ciao,

Patrick

priyanka srivastava a écrit :

Dear All,

I want to calculate tilt angle of a peptide inserted
inside the lipid bilayer (i.e. angle between the
helical axis and bilayer normal). From previous posts
I got an idea that g_bundle wud solve my problem.

I am issuing the following on the command line:

g_bundle -f test.xtc -s test.tpr -na 2 -z -tu ps

This asks me to Select a group of top and a group of
bottom atoms

Group 0 (  System) has 12877 elements
Group 1 ( Protein) has   102 elements
Group 2 (   Protein-H) has79 elements
Group 3 ( C-alpha) has10 elements
Group 4 (Backbone) has31 elements
Group 5 (   MainChain) has41 elements
Group 6 (MainChain+Cb) has49 elements
Group 7 ( MainChain+H) has54 elements
Group 8 (   SideChain) has48 elements
Group 9 ( SideChain-H) has38 elements
Group10 ( Prot-Masses) has   102 elements

when I chose 1 and 1 it gives all angles as 90,
which is wrong and bun_tiltr is reported as nan. The
manual says that the program reads two index groups
and divides both of them in -na parts.
I am a lil confused! what should be my choice here?

regards,
Pri...




   

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Re: [gmx-users] Polarizability

2007-05-21 Thread Patrick Fuchs

Hi,
there's a very recent paper of the GROMOS team, where they evaluate the 
free energy of polarization (with the 'Charge-on-Spring' model):

http://pubs.acs.org/cgi-bin/abstract.cgi/jpcbfk/asap/abs/jp0706477.html
Their code is already working, but under the GROMOS software...
Ciao,

Patrick

Jones de Andrade a écrit :

Hi David

They have published a few paper on water and alcohols. The charm crew
have done a few more. Amber is actually split into two IIRC, with point
dipoles as well as shell models (that means either or).


I've found two papers for charmm polariability. But I'll only be able to 
try to find it in the library or to ask for the authors tomorrow at 
least. But thanks for the information!  ;)


On the other hand, I could not yet find any published material from 
amber using shell models. Is this only an inside group discussion?


I think there is not a lot of difference, but shell models are easier to
implement.


I think too. In reality, there is no visible rational reason for this 
fear of me, is more like a feeling, so I'll try to find something more 
on it.


But I do agree that it's much likely that the shell model is much easier 
to implement, if not faster to execute also. :)


I am working on shell models a bit (not enough...)


Me too. Specially cause this is long terms plans (2+ years from now).

But thanks a lot for all information, David. Helped a lot.

Sincerally yours,

Jones




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Re: [gmx-users] Polarizability

2007-05-21 Thread Patrick Fuchs

Hi Jones,
Charge-on-spring model is another name for shell model.
Here's what's written in the introduction of the paper:
[...]in the charge-on-spring (or Drude-oscillator or shell) model, an
additional point charge is attached to a polarizable center that
can adapt its position to the electric field to induce a net
dipole.[...]
Ciao,

Patrick

Jones de Andrade a écrit :

Hi Patrick.

Just got this paper here, thanks for the indication.

This may sound like a dumb question, but: am I wrong, or the shell 
model and the charge on a spring model differ only by the fact that 
the VdW interation is also floating aroung in the shell model but 
not in the charge on a spring one?


Thanks a lot,

Jones

On 5/21/07, *Patrick Fuchs* [EMAIL PROTECTED] 
mailto:[EMAIL PROTECTED] wrote:


Hi,
there's a very recent paper of the GROMOS team, where they evaluate the
free energy of polarization (with the 'Charge-on-Spring' model):
http://pubs.acs.org/cgi-bin/abstract.cgi/jpcbfk/asap/abs/jp0706477.html
http://pubs.acs.org/cgi-bin/abstract.cgi/jpcbfk/asap/abs/jp0706477.html
Their code is already working, but under the GROMOS software...
Ciao,

Patrick

Jones de Andrade a écrit :
  Hi David
 
  They have published a few paper on water and alcohols. The
charm crew
  have done a few more. Amber is actually split into two IIRC,
with point
  dipoles as well as shell models (that means either or).
 
 
  I've found two papers for charmm polariability. But I'll only be
able to
  try to find it in the library or to ask for the authors tomorrow at
  least. But thanks for the information!  ;)
 
  On the other hand, I could not yet find any published material from
  amber using shell models. Is this only an inside group discussion?
 
  I think there is not a lot of difference, but shell models
are easier to
  implement.
 
 
  I think too. In reality, there is no visible rational reason
for this
  fear of me, is more like a feeling, so I'll try to find
something more
  on it.
 
  But I do agree that it's much likely that the shell model is much
easier
  to implement, if not faster to execute also. :)
 
  I am working on shell models a bit (not enough...)
 
 
  Me too. Specially cause this is long terms plans (2+ years from now).
 
  But thanks a lot for all information, David. Helped a lot.
 
  Sincerally yours,
 
  Jones
 
 
 

 
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Re: [gmx-users] Very large fluctuations in dg/dl

2007-05-08 Thread Patrick Fuchs

Hi John,
thanks a lot for your reply.
Indeed, the standard deviation I presented in my previous post is the one 
of dg/dl samples. I was just surprised by the fact the std. dev. is always 
larger than the value itself (since I'm starting with FE calculation I had 
no expectation of what the behavior would be and needed a confirmation).
I was also suprised about the convergence of the mean. I put a plot 
for each lambda value at the URL:

http://condor.ebgm.jussieu.fr/~fuchs/download/convergence.png
(at each time step, I recalculate the mean from the beginning). My first 
observation was that 1 ns seemed to be a minimum for certain lambda values
(e.g. lambda=0.70). I sometimes read in literature that some authors 
used a few hundreds of ps, which seemed (to me) not sufficient for 
proper convergence.
Now, if we come back to the error estimate of the mean, I found (for 
lambda=0.00) 0.2 kJ/mol using block averaging (using the -ee option of 
g_analyze), which is reasonable I imagine (even if higher precisions 
have been described in literature). I'm not sure whether this is the same

way of calculating the uncertainty compared to what you proposed.
Can you confirm?
I will have a look to the book you mentioned, thanks for the pointer.
Cheers,

Patrick

On Mon, 7 May 2007, John D. Chodera wrote:


Hi Patrick,


I find a reasonable DeltaGsol value of 8.6 kJ/mol for methane (compared
to 8.7 in Geerke  van Gunsteren, ChemPhysChem 2006, 7, 671 ? 678) but
I get really huge fluctuations in the values of dg/dl:
lambda=0.00: 5.0 +/- 10.8 (mean +/- standard deviation)
lambda=0.05: 4.3 +/- 11.2


Is the standard deviation you quote here the standard deviation of the dg/dl 
samples, or the standard deviation of the mean?


If the former, then this behavior is totally expected: While the standard 
deviation of a random variable (your dg/dl samples) may be large, with enough 
sampling, we can get a very precise estimate of the mean.  More sampling will 
not change the standard deviation of the dg/dl samples, but it will reduce 
the standard error in the mean, which is what we need for precise estimates 
of free energy differences.


The uncertainty in the estimate of dg/dl is given simply by

ddg/dl = sigma / sqrt(N / g)

where here, sigma is the standard deviation of your dg/dl samples, N is the 
number of data points you have collected, and g is something called the 
statistical inefficiency, which can be estimated from the correlation time 
of your dg/dl samples.  More information on this sort of analysis can be 
found in reference [1] below.


Once you have the uncertainty in each estimate of dg/dl, you still have to 
combine these to get the uncertainty estimate for the integrated free energy 
difference using standard propagation of error.  This depends on your choice 
of quadrature for TI.  David Mobley has done a lot of this, and I'm sure 
would be willing to help if you had trouble figuring it out.


Good luck!

- John

[1] W. Janke. Statistical analysis of simulations: Data correlations and 
error estimation. In J. Grotendorst, D. Marx, and A. Murmatsu, editors, 
Quantum Simulations of Complex Many-Body Systems: From Theory to Algorithms, 
volume 10, pages 423?445. John von Neumann Institute for Computing, 2002.


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Postdoctoral researcher, Pande lab| Lab phone : 650.723.1097
Department of Chemistry, Stanford University  | Lab fax   : 650.724.4021
http://www.dillgroup.ucsf.edu/~jchodera
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Date: Mon, 07 May 2007 16:41:26 +0200
From: Patrick Fuchs [EMAIL PROTECTED]
Subject: [gmx-users] Very large fluctuations in dg/dl
To: gmx-users@gromacs.org
Message-ID: [EMAIL PROTECTED]
Content-Type: text/plain; charset=windows-1252; format=flowed

Hi Gromacs users,
I have a few questions related to solvation free energy calculation via
thermodynamic integration.
I'm trying to reproduce some literature data (on e.g. methane,
methanol...) using the GROMOS G53a6 force field. I followed the tutorial
of David Mobley (thanks to him BTW), but I used the standard non bonded
options of the G53a6 force field (instead of OPLS). For each lambda
value I do a minimization, a 10 ps NVT followed by a 20 ps NPT
equilibration, and a 1 ns NVT production using the sd integrator. I used
21 lambda values (0.00, 0.05...1.00).
Here's my topology file:
begining of methane.top
; topology for a methane molecule

; include GROMOS53a6 force field
#include ffG53a6.itp

;;; begin methane definition ;;;
[ moleculetype ]
; Name   nrexcl
METH 3

[ atoms ]
;nr type resnr residue atom cgnr charge masstypeB chargeB massB
1  CH4  1 METHC1   00. 16.0430 DUM   0.  16.04300
;; end methane definition 

; include water topology
#ifdef FLEX_SPC
#include flexspc.itp
#else
#include spc.itp
#endif

[ system ]
; name
1 methane molecule in water

[ molecules ]
; name  number
METH1
SOL

Re: [gmx-users] Very large fluctuations in dg/dl

2007-05-08 Thread Patrick Fuchs

Hi Berk and Tsjerk,
sounds reassuring since the last version of the GROMOS force field (G53a5 
and a6) has been parametrized to reproduce DGsol using reaction field.
But, you agree Berk that when you want to calculate the solvation free 
energy in the GROMOS philosophy (e.g. for reproducing or computing new 
parameters), you have to use RF even if energy conservation might not

be as good as with PME?
Thanks for your answers and your interest in the thread.
Cheers,

Patrick

On Tue, 8 May 2007, Berk Hess wrote:






From: Tsjerk Wassenaar [EMAIL PROTECTED]
Reply-To: Discussion list for GROMACS users gmx-users@gromacs.org
To: Discussion list for GROMACS users gmx-users@gromacs.org
Subject: Re: [gmx-users] Very large fluctuations in dg/dl
Date: Tue, 8 May 2007 06:39:50 +0200

Hi Berk,

Just a question relating to your reply (should be a new thread
maybe...). The Gromos force fields were parameterized (for use) with
cutoff/RF. PME is of course better for energy conservation, but the
inclusion of the interactions beyond the cut-off may give rise to
deviant behaviour from the force field. Could you enlighten me on this
issue?

Thanks,

Tsjerk


Luckily it does not.
And PME is not only better for energy conservation, but also captures
long-range interaction, which for instance leads to more stable proteins.
I have compared solvation free energies for G53A6 with reaction-field
and PME and found no differences:

B. Hess and N. van der Vegt
Hydration Thermodynamic Properties of Amino Acid Analogues: A Systematic 
Comparison of Biomolecular Force Fields and Water Models

J. Phys. Chem. B 110, 17616 (2006)
http://dx.doi.org/10.1021/jp0641029

Berk.



On 5/7/07, Berk Hess [EMAIL PROTECTED] wrote:




From: Patrick Fuchs [EMAIL PROTECTED]
Reply-To: Discussion list for GROMACS users gmx-users@gromacs.org
To: gmx-users@gromacs.org
Subject: [gmx-users] Very large fluctuations in dg/dl
Date: Mon, 07 May 2007 16:41:26 +0200

Hi Gromacs users,
I have a few questions related to solvation free energy calculation via
thermodynamic integration.
I'm trying to reproduce some literature data (on e.g. methane,
methanol...) using the GROMOS G53a6 force field. I followed the tutorial
of David Mobley (thanks to him BTW), but I used the standard non bonded
options of the G53a6 force field (instead of OPLS). For each lambda
value I do a minimization, a 10 ps NVT followed by a 20 ps NPT
equilibration, and a 1 ns NVT production using the sd integrator. I used
21 lambda values (0.00, 0.05...1.00).
Here's my topology file:
begining of methane.top
; topology for a methane molecule

; include GROMOS53a6 force field
#include ffG53a6.itp

;;; begin methane definition ;;;
[ moleculetype ]
; Name   nrexcl
METH 3

[ atoms ]
;nr type resnr residue atom cgnr charge masstypeB chargeB massB
  1  CH4  1 METHC1   00. 16.0430 DUM   0.  16.04300
;; end methane definition 

; include water topology
#ifdef FLEX_SPC
#include flexspc.itp
#else
#include spc.itp
#endif

[ system ]
; name
1 methane molecule in water

[ molecules ]
; name  number
METH1
SOL 893
-end of methane.top

And here is my mdp file for lambda=0:
---begining of prod.mdp-
title   = production NVT methane/water
cpp = /lib/cpp
; OPTIONS FOR BOND CONSTRAINTS
constraints = all-bonds
; RUN CONTROL PARAMETERS
integrator  = sd
tinit   = 0
dt  = 0.002
nsteps  = 50 ; 1000 ps
; NUMBER OF STEPS FOR CENTER OF MASS MOTION REMOVAL
nstcomm = 100
; OUTPUT CONTROL OPTIONS
nstxout  = 500
nstvout  = 500
nstfout  = 0
nstlog   = 500
nstenergy= 100
nstxtcout= 5000
xtc-precision= 1000
; NON BONDED STUFF
ns_type =  grid
nstlist= 5
rlist  = 0.8
coulombtype= generalized-reaction-field
rcoulomb   = 1.4
rvdw   = 1.4
epsilon_rf = 54.0
;OPTIONS FOR TEMPERATURE COUPLING
tc_grps  = system
tau_t= 0.1 ; inverse langevin friction cst
ref_t= 300
;OPTIONS FOR PRESSURE COUPLING
Pcoupl   = no
tau_p= 0.5
compressibility  = 4.5e-5
ref_p= 1.0
; FREE ENERGY CONTROL STUFF
free_energy  = yes
init_lambda  = 0.00
delta_lambda = 0
sc_alpha = 0.5
sc-power = 1.0
sc-sigma = 0.3
; VELOCITY GENERATION
gen_vel  = yes
gen_temp = 300
gen_seed = -1
-end of prod.mdp
I find a reasonable DeltaGsol value of 8.6 kJ/mol for methane (compared
to 8.7 in Geerke  van Gunsteren, ChemPhysChem

Re: [gmx-users] Very large fluctuations in dg/dl

2007-05-08 Thread Patrick Fuchs

Hi Berk,
I just wanted a confirmation because it's a critical aspect. Beyond the 
debate between PME and RF, I always read it was important to be consistent

with the (early) force field parameterization when deriving new parameters.
Even if it does not make any difference for solvation free energy, I 
imagine this can give some differences on other properties (e.g. heat of 
vaporization...), or if you want your new parameters to be consistent with

the remaining of the force field.
Ciao,

Patrick

On Tue, 8 May 2007, Berk Hess wrote:


Hi,

I don't understand why you ask this.
Or didn't you read or understand my previous answer?

Reaction-field and PME give exactly the same solvation free-energies,
so you can just as well derive parameters for the GROMOS force-field
using PME.

Berk.



From: Patrick Fuchs [EMAIL PROTECTED]
Reply-To: Discussion list for GROMACS users gmx-users@gromacs.org
To: Discussion list for GROMACS users gmx-users@gromacs.org
Subject: Re: [gmx-users] Very large fluctuations in dg/dl
Date: Tue, 8 May 2007 12:45:32 +0200 (CEST)

Hi Berk and Tsjerk,
sounds reassuring since the last version of the GROMOS force field (G53a5 
and a6) has been parametrized to reproduce DGsol using reaction field.
But, you agree Berk that when you want to calculate the solvation free 
energy in the GROMOS philosophy (e.g. for reproducing or computing new 
parameters), you have to use RF even if energy conservation might not

be as good as with PME?
Thanks for your answers and your interest in the thread.
Cheers,

Patrick

On Tue, 8 May 2007, Berk Hess wrote:






From: Tsjerk Wassenaar [EMAIL PROTECTED]
Reply-To: Discussion list for GROMACS users gmx-users@gromacs.org
To: Discussion list for GROMACS users gmx-users@gromacs.org
Subject: Re: [gmx-users] Very large fluctuations in dg/dl
Date: Tue, 8 May 2007 06:39:50 +0200

Hi Berk,

Just a question relating to your reply (should be a new thread
maybe...). The Gromos force fields were parameterized (for use) with
cutoff/RF. PME is of course better for energy conservation, but the
inclusion of the interactions beyond the cut-off may give rise to
deviant behaviour from the force field. Could you enlighten me on this
issue?

Thanks,

Tsjerk


Luckily it does not.
And PME is not only better for energy conservation, but also captures
long-range interaction, which for instance leads to more stable proteins.
I have compared solvation free energies for G53A6 with reaction-field
and PME and found no differences:

B. Hess and N. van der Vegt
Hydration Thermodynamic Properties of Amino Acid Analogues: A Systematic 
Comparison of Biomolecular Force Fields and Water Models

J. Phys. Chem. B 110, 17616 (2006)
http://dx.doi.org/10.1021/jp0641029

Berk.


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[gmx-users] Very large fluctuations in dg/dl

2007-05-07 Thread Patrick Fuchs

Hi Gromacs users,
I have a few questions related to solvation free energy calculation via
thermodynamic integration.
I'm trying to reproduce some literature data (on e.g. methane,
methanol...) using the GROMOS G53a6 force field. I followed the tutorial
of David Mobley (thanks to him BTW), but I used the standard non bonded
options of the G53a6 force field (instead of OPLS). For each lambda
value I do a minimization, a 10 ps NVT followed by a 20 ps NPT
equilibration, and a 1 ns NVT production using the sd integrator. I used
21 lambda values (0.00, 0.05...1.00).
Here's my topology file:
begining of methane.top
; topology for a methane molecule

; include GROMOS53a6 force field
#include ffG53a6.itp

;;; begin methane definition ;;;
[ moleculetype ]
; Name   nrexcl
METH 3

[ atoms ]
;nr type resnr residue atom cgnr charge masstypeB chargeB massB
 1  CH4  1 METHC1   00. 16.0430 DUM   0.  16.04300
;; end methane definition 

; include water topology
#ifdef FLEX_SPC
#include flexspc.itp
#else
#include spc.itp
#endif

[ system ]
; name
1 methane molecule in water

[ molecules ]
; name  number
METH1
SOL 893
-end of methane.top

And here is my mdp file for lambda=0:
---begining of prod.mdp-
title   = production NVT methane/water
cpp = /lib/cpp
; OPTIONS FOR BOND CONSTRAINTS
constraints = all-bonds
; RUN CONTROL PARAMETERS
integrator  = sd
tinit   = 0
dt  = 0.002
nsteps  = 50 ; 1000 ps
; NUMBER OF STEPS FOR CENTER OF MASS MOTION REMOVAL
nstcomm = 100
; OUTPUT CONTROL OPTIONS
nstxout  = 500
nstvout  = 500
nstfout  = 0
nstlog   = 500
nstenergy= 100
nstxtcout= 5000
xtc-precision= 1000
; NON BONDED STUFF
ns_type =  grid
nstlist= 5
rlist  = 0.8
coulombtype= generalized-reaction-field
rcoulomb   = 1.4
rvdw   = 1.4
epsilon_rf = 54.0
;OPTIONS FOR TEMPERATURE COUPLING
tc_grps  = system
tau_t= 0.1 ; inverse langevin friction cst
ref_t= 300
;OPTIONS FOR PRESSURE COUPLING
Pcoupl   = no
tau_p= 0.5
compressibility  = 4.5e-5
ref_p= 1.0
; FREE ENERGY CONTROL STUFF
free_energy  = yes
init_lambda  = 0.00
delta_lambda = 0
sc_alpha = 0.5
sc-power = 1.0
sc-sigma = 0.3
; VELOCITY GENERATION
gen_vel  = yes
gen_temp = 300
gen_seed = -1
-end of prod.mdp
I find a reasonable DeltaGsol value of 8.6 kJ/mol for methane (compared
to 8.7 in Geerke  van Gunsteren, ChemPhysChem 2006, 7, 671 – 678) but
I get really huge fluctuations in the values of dg/dl:
lambda=0.00: 5.0 +/- 10.8 (mean +/- standard deviation)
lambda=0.05: 4.3 +/- 11.2
...
lambda=1.00: -0.3 +/- 4.0
Furthermore, each of these mean value is very slow at converging (1 ns
seems a minimum for certain lambda values...).
I can't get reasonable fluctuations even if I sample more. In addition, 
there are very frequent warnings in the log file such as:


Large VCM(group rest):  0.01363,  0.00818,  0.01147, 
ekin-cm:  3.09490e+00


Here are my questions:
1) Has someone an idea of what could be the cause of these [very] large
fluctuations? Does it come from my setup, or is this a normal behavior?
2) Are these 'Large VCM(group rest)' warnings related to the use of sd 
integrator (when I switch to md integrator, I no longer get these 
warnings) ?

Thanks for your answer,

Patrick
--
___
Patrick FUCHS
Equipe de Bioinformatique Genomique et Moleculaire
INSERM U726, Universite Paris 7
Case Courrier 7113
2, place Jussieu, 75251 Paris Cedex 05, FRANCE
Tel : +33 (0)1-44-27-77-16 - Fax : +33 (0)1-43-26-38-30
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Re: [gmx-users] Creation of an index file with seperate lipid leaflets

2006-11-09 Thread Patrick Fuchs

Hi,
I've written a python script that does what you want.
I cleaned the script (make_2leaflets_index) and put it on my web page at 
the following URL:

http://condor.ebgm.jussieu.fr/~fuchs/download/index.html
Hope it helps.
Ciao,

Patrick

Jay Mashl a écrit :

Wasted work would be bad ;)

Rather than headgroup orientation, maybe try looking at atom distributions 
along the bilayer normal direction.  Neutron scattering experiments show that 
for atom groups far from the bilayer midplane, the corresponding z-coordinates 
form two distinct distributions.  So one way could be the following. Pick a 
headgroup atom and obtain its z-coordinate. Have make_ndx accept this value as 
input. Search the system by looping over lipids and ask whether that atom type 
has a z-coordinate within some amount around the input value. From this you 
know the membership of the leaflets.  A more automatic way would be to have the 
program first discern the distribution and then reread the system to decide the 
leaflet membership.


Jay


On Wed, 8 Nov 2006, Alan Dodd wrote:

Wouldn't shuffle/sort undo all the good work?  I did
wonder if I should have labelled the lipids in
different leaflets as different molecule types, or
different chains, but it's a bit late now...

--- Jay Mashl [EMAIL PROTECTED] wrote:


On Wed, 8 Nov 2006, Alan Dodd wrote:

Has anyone already created a way to generate an

index

file with the atoms from the two leaflets of a

bilayer

listed seperately?  I can't believe it hasn't

already

been done, but can't find a direct description of

a

solution.  I'm attempting a modification to

make_ndx,

(or perhaps something considerably less ambitious,
judging by the way it's going so far) to permit

lipid

selection based on headgroup orientation, though

I'd

quite like to save myself the effort.
Incidentally, splitres and splitat seem to be the
wrong way around, unless I'm misunderstanding them

-

they do the opposite of what they say.  From the
gromacs 3.3.1 source download I did on April of

this

year.

Reordering the lipids into leaflets in your starting
coordinate 
file might be a good idea. If you anticipate lipid
exchange between leaflets, 
then a more general tool like what you suggest would

be helpful.

Jay

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INSERM U726, Universite Paris 7
Case Courrier 7113
2, place Jussieu, 75251 Paris Cedex 05, FRANCE
Tel : +33 (0)1-44-27-77-16 - Fax : +33 (0)1-43-26-38-30
E-mail : [EMAIL PROTECTED]
Web Site: http://www.ebgm.jussieu.fr/~fuchs
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Re: [gmx-users] can we calculate chemical shifts

2006-05-16 Thread Patrick Fuchs

You may also try SHIFTCALC : http://www.shef.ac.uk/NMR/mainframepage.html

Patrick

David van der Spoel a écrit :


Richa taimni wrote:


Dear all,
my question is that is it possible to calculate
chemical shift with the help of gromacs software.

You want to get the latest software from the David Case group at 
Scripps for that.



Regards,
Richa

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Case Courrier 7113
2, place Jussieu, 75251 Paris Cedex 05, FRANCE
Tel : +33 (0)1-44-27-77-16 - Fax : +33 (0)1-43-26-38-30
E-mail : [EMAIL PROTECTED]
Web Site: http://www.ebgm.jussieu.fr/~fuchs

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Re: [gmx-users] Please Help: Still facing problems with installing Gromacs 3.3.1 on SGI Irix

2006-04-20 Thread Patrick Fuchs

Hi,
I met the same kind of problem with gromacs 3.2.1, and could quickly fix 
it, by replacing e.g.
{ evStepOptions[evLINFIX], FALSE, etSTR, {evParams[evLINFIX]}, == { 
-linfix, FALSE, etSTR, {evSelections[evLINFIX]}, etc...

See  http://www.gromacs.org/pipermail/gmx-users/2004-May/010404.html

Patrick

Akshay Patny a écrit :


SUBJECT: Still facing problems with installing Gromacs 3.3.1 on SGI Irix

 


Hi

 

As suggested by Dr. Spoel, I removed one of the semicolons before the 
double semicolon in one of the lines in the file gmx_chi.c


 

I re-installed again and this time it gave me the following error. Can 
you suggest what is going wrong and how can I fix it now?




cc-1028 cc: ERROR File = make_edi.c, Line = 579

  The expression used must have a constant value.

 


  { evStepOptions[evLINFIX], FALSE, etSTR, {evParams[evLINFIX]},

^

 


cc-1028 cc: ERROR File = make_edi.c, Line = 581

  The expression used must have a constant value.

 


  { evStepOptions[evLINACC], FALSE, etSTR, {evParams[evLINACC]},

^

 


cc-1028 cc: ERROR File = make_edi.c, Line = 583

  The expression used must have a constant value.

 


  { evStepOptions[evRADFIX], FALSE, etREAL, {radfix},

^

 


cc-1552 cc: WARNING File = make_edi.c, Line = 622

  The variable bTop is set but never used.

 


  bool bTop, bM, bFit1;

   ^

 


3 errors detected in the compilation of make_edi.c.

*** Error code 2 (bu21)

*** Error code 1 (bu21)

*** Error code 1 (bu21)



 


I really appreciate your help.

 


Kind Regards

Akshay

 


Akshay Patny

 

 


**Akshay Patny***

*

**Graduate Research Assistant**
Faser Hall 417, Department of Medicinal Chemistry

Research Institute of Pharmaceutical Sciences
University of Mississippi
University, MS 38677
E-mail: [EMAIL PROTECTED] mailto:[EMAIL PROTECTED]
Tel: 662-915-1286 (office); Web: www.olemiss.edu http://www.olemiss.edu

 




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Tel : +33 (0)1-44-27-77-16 - Fax : +33 (0)1-43-26-38-30
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Re: [gmx-users] Compilation problem on SGI ORIGIN 3800

2006-03-02 Thread Patrick Fuchs

David van der Spoel a écrit :


Patrick Fuchs wrote:


Hi gmx users,
I'm trying to compile gromacs in // on an SGI ORIGIN 3800. For the 
monoCPU version it went well (thanks to very good advices on previous 
E-mails of the gmx list), but for the parallel version, I encountered 
a problem. Here are the steps I followed :

setenv CPPFLAGS -I/opt/mpt/1.4.0.3/usr/include -I/usr/local/include
setenv LDFLAGS -L/opt/mpt/1.4.0.3/usr/lib 
-L/usr/local/lib/fftw2.1.5/lib32

setenv LIBS -lmpi
./configure --enable-mpi --prefix=/home/fuchs/software/gromacs 
--program-suffix=_mpi --disable-float --disable-fortran --disable-nice

- This step went OK

make mdrun
- at the beginning it went OK
...
(cd ./src/kernel  make mdrun ; exit 0)
   /bin/sh ../../libtool --mode=link mpicc  -O3 
-OPT:IEEE_arithmetic=3 -OPT:rsqrt=ON -SWP:loop_overhead -INLINE:=ON 
-LNO:opt=1 -LNO:ou_further=3 -OPT:Olimit=0:roundoff=3:alias=typed 
-woff 1174 -D__INLINE_INTRINSICS -I/usr/freeware/include/libxml2   
-L/opt/mpt/1.4.0.3/usr/lib -L/usr/local/lib/fftw2.1.5/lib32  -woff 84 
-o mdrun  glaasje.o gctio.o init_sh.o  ionize.o do_gct.o relax_sh.o  
xutils.o md.o mdrun.o genalg.o ../mdlib/libmd_mpi_d.la 
../gmxlib/libgmx_mpi_d.la  -lnsl -lrfftw_mpi -lfftw_mpi -lrfftw 
-lfftw -lm -lmpi -lXm -lXt  -lSM -lICE -lXext -lX11  
-L/usr/freeware/lib32 -lxml2 -lz -lm
libtool: link: warning: library 
`/usr/local/lib/fftw2.1.5/lib32/librfftw_mpi.la' was moved.


This might be a problem.

libtool: link: warning: library 
`/usr/local/lib/fftw2.1.5/lib32/libfftw_mpi.la' was moved.
libtool: link: warning: library 
`/usr/local/lib/fftw2.1.5/lib32/librfftw.la' was moved.libtool: link: 
warning: library `/usr/local/lib/fftw2.1.5/lib32/libfftw.la' was moved.
libtool: link: warning: library 
`/usr/local/lib/fftw2.1.5/lib32/librfftw_mpi.la' was moved.
libtool: link: warning: library 
`/usr/local/lib/fftw2.1.5/lib32/libfftw_mpi.la' was moved.
libtool: link: warning: library 
`/usr/local/lib/fftw2.1.5/lib32/librfftw.la' was moved.libtool: link: 
warning: library `/usr/local/lib/fftw2.1.5/lib32/libfftw.la' was moved.
mpicc -O3 -OPT:IEEE_arithmetic=3 -OPT:rsqrt=ON -SWP:loop_overhead 
-INLINE:=ON -LNO:opt=1 -LNO:ou_further=3 
-OPT:Olimit=0:roundoff=3:alias=typed -woff 1174 -D__INLINE_INTRINSICS 
-I/usr/freeware/include/libxml2 -woff 84 -o mdrun glaasje.o gctio.o 
init_sh.o ionize.o do_gct.o relax_sh.o xutils.o md.o mdrun.o 
genalg.o  -L/opt/mpt/1.4.0.3/usr/lib -L/usr/local/lib/fftw2.1.5/lib32 
../mdlib/.libs/libmd_mpi_d.a -L/usr/freeware/lib32 
../gmxlib/.libs/libgmx_mpi_d.a -lnsl 
/usr/local/lib/fftw2.1.5/lib32/librfftw_mpi.a 
/usr/local/lib/fftw2.1.5/lib32/libfftw_mpi.a 
/usr/local/lib/fftw2.1.5/lib32/librfftw.a 
/usr/local/lib/fftw2.1.5/lib32/libfftw.a -lmpi -lXm -lXt -lSM -lICE 
-lXext -lX11 -lxml2 -lz -lm

cc: Warning: -OPT options are ignored
cc: Warning: -OPT options are ignored
cc: Warning: -SWP options are ignored
cc: Warning: -OPT options are ignored
uld:
Object file format error in: glaasje.o: bad symbolic header (magic 
number)


Something wrong with this file, delete it.


*** Error code 1 (bu21)
*** Error code 1 (bu21)

I didn't find any similar case in the mailing list, and I'm wondering 
where could it come from.

Does someone have an idea on how to fix that ?
Thanks !

Patrick

Could it be that you have restarted the compilation with differen 
flags? In that case you will have to do

make distclean

On SGI machines it has always been a problem to install the compilers, 
this problem is however hard to distinguish from others.

You might want to start from scratch if make distclean doesn't do it.


Thank you David,
I made a distclean and then used the following :
setenv CPPFLAGS -I/opt/mpt/1.4.0.3/usr/include -I/usr/local/include
setenv LDFLAGS -L/opt/mpt/1.4.0.3/usr/lib -L/usr/local/lib/fftw2.1.5/lib32
setenv LIBS -lmpi
setenv MPICC cc
./configure --enable-mpi --prefix=/home/fuchs/software/gromacs 
--program-suffix=_mpi --disable-float --disable-nice

make mdrun
And it worked ! The thing missing was the line 'setenv MPICC cc', and 
that makes all the difference. The option --disable-fortran has no 
effect wether it's used or not, as long as 'setenv MPICC cc' has been set.

Ciao,

Patrick

--
___
Patrick FUCHS
Equipe de Bioinformatique Genomique et Moleculaire
INSERM U726, Universite Paris 7
Case Courrier 7113
2, place Jussieu, 75251 Paris Cedex 05, FRANCE
Tel : +33 (0)1-44-27-77-16 - Fax : +33 (0)1-43-26-38-30
E-mail : [EMAIL PROTECTED]
Web Site: http://www.ebgm.jussieu.fr/~fuchs

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