to look at the table of existing parameters). I've been looking
through the top directory and can't find them anywhere. Can anyone give
me a pointer to where they are? Or are they hardwired into the code
somewhere?
Thanks so much,
David
--
David Mobley
dmob...@gmail.com
504-383-3662
--
gmx-users
and Hunenberger papers from J. Chem. Phys (2006 or 2007) and references
therein. The good news is that for simple spherical ions KH have worked
out the relevant corrections. The bad news is that if you move away from
simple spherical ions you've got problems.
David Mobley
On Fri, Dec 16, 2011 at 6:41 AM
be documented in the manual since (with this behavior)
knowing what value of dihre-fc one is using is critical to knowing what
dihedral restraint strength one is using.
Thanks.
--
David Mobley
dmob...@gmail.com
504-383-3662
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Please
can do some benchmarking myself
as well but I thought I'd check in with the list first.
Thanks so much,
David
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SUNITA GUPTA
David Mobley
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...@gromacs.org on behalf of David Mobley
Sent: Thu 8/6/2009 2:38 PM
To: Mauricio Carrillo Tripp
Cc: Discussion list for GROMACS users
Subject: [gmx-users] Re: Free Energy Calculation
Hi,
Sorry for the delay answering. These questions are better put on the
GROMACS users list.
1) Yes
?
Peter Nagy
The University of Toledo
-Original Message-
From: gmx-users-boun...@gromacs.org on behalf of David Mobley
Sent: Thu 8/6/2009 2:38 PM
To: Mauricio Carrillo Tripp
Cc: Discussion list for GROMACS users
Subject: [gmx-users] Re: Free Energy Calculation
Hi,
Sorry
I agree with Carsten. See perhaps the discussion at www.alchemistry.org as
well.
On Fri, Aug 7, 2009 at 2:35 AM, Carsten Kutzner ckut...@gwdg.de wrote:
On Aug 6, 2009, at 10:57 PM, Ragnarok sdf wrote:
I am performing FEP do obtain the dimerization of a protein in
membrane. The lambda
Hi,
Sorry for the delay answering. These questions are better put on the
GROMACS users list.
1) Yes -- the Berendsen barostat does not sample the correct
distribution of pressures.
2) Regenerating velocities is fine for a couple of reasons: (a) we are
after thermodynamics, not dynamics,
a patched 3.3.x to
compare to), given the number of times we were burned by free energy
bugs in 3.3.x.
Thanks for your help.
David Mobley, Ph.D.
Assistant Professor of Chemistry
University of New Orleans
New Orleans, LA 70148
dlmob...@uno.edu
Office 504-280-6445
Fax 504-280-6860
You may also want to look at www.alchemistry.org, as it has some
general information about how these should be set up.
On Wed, Mar 18, 2009 at 8:02 PM, Justin A. Lemkul jalem...@vt.edu wrote:
Again, *please keep all Gromacs-related correspondence on the mailing list*
The type of information
David,
Both your gro files are wrong, the definition of gro files has never
changed. Do you mean to say this has ever worked?
Yes, it worked fine in 3.3.x. I would point out that trjconv has an
-ndec option which, if used to output a gro file, will generate
high-precision gro files as output.
Berk,
I checked the gro manual page:
http://www.gromacs.org/documentation/reference_4.0/online/gro.html
and found out that it is actually pretty clear.
Note that it is fixed format, but with flexible precision which is derived
from the space between the decimal points.
Thanks. I was looking
-users@gromacs.org
Subject: Re: [gmx-users] shake for water
David Mobley wrote:
All,
A quick question on constraints... I'm using TIP4P-Ew in gromacs
3.3.2
and am concerned with reproducing energies from another code very
precisely for several specific
All,
I'm trying to run a zero-step mdrun in 4.0.3 (basically just to
evaluate the energy of a specific configuration). I've done this test
in 3.3.x and am trying to check if 4.0.3 gives the same energies. I'm
also comparing against another simulation package. To this end, I have
my starting
Berk,
Another question, just to be sure.
Have you actually checked that the other code really gets the distances
right up to 1e-12?
Yes.
Berk
Date: Thu, 5 Feb 2009 12:03:21 -0600
From: dmob...@gmail.com
To: gmx-users@gromacs.org
Subject: [gmx-users] shake for water
All,
A quick
No, it is not the square.
The code does a small 'a' approximation: (1+a)^2=1+2a+a^2 is approx 1+2a.
I have also tested/benchmark shake in gromacs for my first lincs paper
and the plincs paper and it always behaved the way I thought it would.
The problem is not that you need more iterations
-users] shake for water
Berk Hess wrote:
Date: Thu, 5 Feb 2009 19:35:09 +0100
From: sp...@xray.bmc.uu.se
To: gmx-users@gromacs.org
Subject: Re: [gmx-users] shake for water
David Mobley wrote:
All,
A quick question on constraints... I'm using TIP4P-Ew in gromacs
to establish some level of consequence that
the preferred state for the protein in the absence of the copper isn't
the unfolded state (I'm not talking experimentally, here -- I'm
talking about with your particular parameters).
David Mobley, Ph.D.
Assistant Professor of Chemistry
University of New
All,
A quick question on constraints... I'm using TIP4P-Ew in gromacs 3.3.2
and am concerned with reproducing energies from another code very
precisely for several specific snapshots. I am doing a zero-step mdrun
of a setup with one small molecule and two tip4p-ew water molecules.
Anyway, I have
Perhaps this is obvious, but typically you only want to do free energy
perturbation if you are interested in computing a free energy
difference. If you are merely interested in structural properties of a
different system (in this case, the protein without the copper there)
you can simply make the
loops,
for sure it was in 3.3.
I have fixed this for the upcoming Gromacs 4.0.4 release.
I assume this bug also caused the cut-off dependence that David
Mobley observed.
I have done a lot of free energy calculation with tip4p and never
noticed
any problems. This was because I always had
to submit errata for two different papers I've published in which
I used the TIP4P-Ew water model in combination with GROMACS. I urge
you to check your own studies that have used TIP4P/TIP4P-Ew and see if
they are affected.
David Mobley
Assistant Professor
Department of Chemistry
University of New
you to check your own studies that have used TIP4P/TIP4P-Ew and see if
they are affected.
David Mobley
Assistant Professor
Department of Chemistry
University of New Orleans
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Bob,
I'm computing the relative binding free energies of DNA bases on a
nanotube using the protocol listed here:
http://www.dillgroup.ucsf.edu/group/wiki/index.php/Free_Energy:_Tutorial
I'm using the following steps:
1. Turn off all charges on base
2. Transform LJ parameters
3. Turn on all
me that
this would probably be the case but I haven't ever seen a publication
on this.
David
David Mobley, Ph.D.
Assistant Professor of Chemistry
University of New Orleans
New Orleans, LA 70148
dlmob...@uno.edu
Office 504-280-6445
Fax 504-280-6860
Thanks,
Chris.
-- original message --
Eudes
From: David Mobley dmob...@gmail.com
Subject: Re: [gmx-users] Free energy of transfer with accuracy
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID:
bc2c99750812110524r1aee080av4ac07eed79b4b...@mail.gmail.com
Content-Type: text/plain; charset=ISO-8859-1
Hi
?) way to do this would be to transfer the solute to vacuum from
each solvent and then take the difference in the vacuum transfer free
energies. Please clarify which you're doing so we can help better.
David Mobley, Ph.D.
Assistant Professor of Chemistry
University of New Orleans
New Orleans, LA
Bob,
When performing a relative binding free energy calculation, I
understand that it is a good practice to separate the transformation
of charges of the ligand and the transformation of vdW parameters into
two calculations. However, is it advisable to completely discharge the
ligand before
, 11 Dec 2008 07:24:26 -0600
From: David Mobley [EMAIL PROTECTED]
Subject: Re: [gmx-users] Free energy of transfer with accuracy
To: Discussion list for GROMACS users gmx-users@gromacs.org
Message-ID:
[EMAIL PROTECTED]
Content-Type: text/plain; charset=ISO-8859-1
Hi,
Hi gmx-users
do not currently have RA support for
students, I anticipate having some in the near future, and in the
meantime anyone joining my group would be supported by a TA position.
Thanks for your time.
David Mobley, Ph.D.
Assistant Professor of Chemistry
University of New Orleans
New Orleans, LA 70148
Hi,
As long as you end up with the same charge in the initial and final
states, you should be OK. It's only if your total transformation
involves a change of net charge that you need to worry. So you should
be fine if you turn off the charges on D, change the LJ interactions,
and turn back on
the forwards and backwards mutation free energy are
more consistant if I do not change the mass. Accidentally?
LQ
On Thu, Jun 19, 2008 at 4:26 AM, David Mobley [EMAIL PROTECTED] wrote:
You can change the mass if you like. Basically, the net free energy
change associated with changing the mass
Sorry to be slow to chime in here, but there are several reasons one
might run into hysteresis, even when not using slow growth:
1) The aforementioned bug
2) Topology errors
3) Convergence problems.
Of 3), there could be many different types. A recurring source of
these problems is when people
You can change the mass if you like. Basically, the net free energy
change associated with changing the mass should end up being zero so
it will be irrelevant. The mass of course affects the dynamics and
things like the velocities, but based on equipartition you can
convince yourself that the free
Bob,
Berk is right. Essentially, it would be easy if we could accurately
compute, say, the total enthalpy of our two systems and simply
subtract. Unfortunately it's very hard to converge this quantity
(basically, subtracting two very large numbers where the error bars
are bigger than the
Justin and Michael,
Just to clarify here, I don't think you want the long cutoff in
vacuum scheme to give you the same results as the PME in vacuum
scheme. That is, if you use PME in vacuum with a periodic box, you
will be including copies of the long-range unscreened electrostatic
interactions
Yes, what he said.
On Mon, May 19, 2008 at 3:00 PM, van Bemmelen
[EMAIL PROTECTED] wrote:
Hi Justin,
You shouldn't use PME in vacuo. Just use pbc=no and infinite (i.o.w.: no)
cutoffs.
I'm not entirely sure why PME takes such a long time, but I can give a very
wild guess. It may have
at 4:12 PM, David Mobley [EMAIL PROTECTED] wrote:
Bob,
Hello everyone,
I'm trying to calculate the free energy of binding of DNA bases on a
carbon nanotube. I'm running some tests to make sure that I'm doing
everything correctly. One thing I tried was turning off all the atom
Bob,
Hello everyone,
I'm trying to calculate the free energy of binding of DNA bases on a
carbon nanotube. I'm running some tests to make sure that I'm doing
everything correctly. One thing I tried was turning off all the atom
charges of the DNA base and then turning them back on again.
Chris,
I think you are correct here. For binding calculations there is
probably a further trick relating to how to define an unbound state
that has a well-defined concentration. This I think depends on how one
is pulling -- i.e. doing simple radial PMFs is probably a bad idea,
because to even
Dear Eudes,
I don't have time to provide personalized help with this at present.
You'll be better off writing the gromacs forum. You may also want to
refer to the general information on performing free energy
calculations at http://www.alchemistry.org and previous posts on the
gromacs users list.
Berk,
The problem could be in the constraints.
Gromacs 3 constrains the forces during EM by adding c*f to the coordinates,
constraining those and then dividing the constraint displacement by c.
This limits the accuracy.
In Gromacs 4 I have implemented force constraining for LINCS and
Berk,
I assume you are using a rigid water model, and thus constraints via SETTLE.
Yes, OK.
Constraining is required to measure the size of the force (for convergence
and
step size adjustment) and to make correct steps without enormous extra
displacements in the direction of the force
Berk,
Hmm. Is this different from how other packages handle this issue? I
have never had the recurring problems with minimization in GROMACS
that I have in other packages. Even though, strangely enough, water is
a common feature in most of the simulations I run.
That was backwards. I
All,
I often have problems with minimization in gromacs, but now I think I
have something a little more systematic to say.
First, my system: I am simulating a short peptide in a mix of two
co-solvents. I use a program called packmol which can start pack
specified number of molecules into a box
Xavier,
I was surprised by the value you use for emstep=1.0e-8. This is the
maximum step size and is in nm! I think that's where your problem is.
I added this recently in testing because I thought perhaps the problem
could be due to using too large of steps. It does not help. So
everything I
Mark,
However should you find yourself on a very flat area of the PES, then
the smaller the step size, the closer it will look to flat, and thus to
have converged to a stationary point. Flat is of course relative to
the step size
Right. But of course the problem here has is that the
Dear Christian,
mmh, just my 0.02€: I guess in a very rough energy landscape (as in
solvated peptides or proteins) this is not generally true, because
with small steps the system might get stuck in the next tiny local
minimum, while with a larger step size it may jump across it.
And I
Bob,
I don't believe that it is implemented. Developers: It probably should
be, since the other restraints can be perturbed.
In the interim, it's pretty straightforward to compute the dV/dlambda
for restraining from the restraint energy if you know the value of the
dihedral angle (which you can
Regarding amb2gmx.pl, it should work for converting whole systems from
Amber, but this may depend on the box geometry you are using. In
particular I think it is OK with cubic boxes but not some of the more
fancy geometries. The other option is just to convert your
protein+ligand and solvate using
Bob,
Unfortunately, I'm having problems including the correct restraints in
my topology file. First off, the form of the angle restraint in
Gromacs involves 4 (2 pairs) atoms. The restraint in the Boresch paper
assumes that the angle is between 3 atoms. Is there anyway to apply
the
just not
seeing something correctly?
Bob
On Mon, Feb 25, 2008 at 2:47 PM, David Mobley [EMAIL PROTECTED] wrote:
Robert,
I am not sure which manual you are looking at, but in the GROMACS 3.3
manual, equation 4.70 gives the dihedral restraint as harmonic.
David
Robert,
I am not sure which manual you are looking at, but in the GROMACS 3.3
manual, equation 4.70 gives the dihedral restraint as harmonic.
David
On Mon, Feb 25, 2008 at 10:10 AM, Robert Johnson
[EMAIL PROTECTED] wrote:
Hello everyone,
I am trying to calculate the absolute free energy of
Maik,
Assume, you take the interconversion of ethane to methanol in solvent in
one step.
You sample hardcore at 11 evenly spaced lambda values for, lets say, 2
ns each.
You get the dG/dl mean from every run and integrate via simpson to get a
total DG.
Hold on, if you are doing this
I think I can probably shed a little bit of light here, although Mark
is getting close in the last chapter of his e-mail.
Basically, pdb2gmx works well for parameterizing proteins, which the
chromophore in question isn't, I'm sure. Since we do lots of
protein-ligand simulations, where the ligand
to determine my DeltaG values. Bonded parameters
remain untouched. I follow closely the procedure posted by David Mobley at
the
DillGroup Wiki site, changing only a few parameters for my simulation, as I am
using Gromos96, not OPLS-AA.
Thanks. This is a good intro -- helps to know what level of help
like he
would have needed to (a) read the entire history of the mailing list,
and (b) wade through all of the old bugzillas.
Thanks,
David
On Feb 16, 2008 3:19 PM, David Mobley [EMAIL PROTECTED] wrote:
Dear Justin,
I'll preface this message by saying that this is my first foray into free
on this) and get help from someone else on there, or i will be
able to attend to it (in that forum) in a few days.
Thanks,
David Mobley
On Feb 11, 2008 5:14 AM, [EMAIL PROTECTED] wrote:
Dear david,
i 'm a beginner in molecular dynamics. I was doing the tutorial of md
group, hydration free energy
: mgoette[at]mpi-bpc.mpg.de
mgoette2[at]gwdg.de
WWW : http://www.mpibpc.gwdg.de/groups/grubmueller/
David Mobley wrote:
Maik,
I simulated a switching process (slow growth TI) over 10ns of ethane to
methanol with hardcore slow-growth in water (365 TIP4P waters,PME) and
in vacuum
All,
I'm using do_dssp to do some secondary structure analysis. I have a
peptide with two nonstandard residues, one at the N-terminus and one
at the C-terminus, and a total of N residues. The output of do_dssp
only contains information on N-2 residues (numbered 1 through N-2)
while my trajectory
Chris,
At one point the forces were incorrrect in the dihedral restraints. I
*think* this was in 3.3 but one of the developers will probably know.
I have a note to this effect in one of my publications too but I
haven't the time to find it right now.
David
On Jan 26, 2008 10:43 PM, [EMAIL
potentials when turning
off the charges right? Thus, sc_alpha should be set to zero when
turning off charges?
Thanks,
Bob
On Jan 25, 2008 5:38 PM, David Mobley [EMAIL PROTECTED] wrote:
It will only be smooth if you don't use soft core (i.e. sc-alpha =0 ).
Best,
David Mobley
http
For what it's worth, I seem to recall that the ProDrg server itself
warns rather strongly about the charges being unreliable, and I
definitely agree with Berk here.
My favorite approach for modeling small molecules is to use the AMBER
GAFF small molecule force field in combination with one of
-alpha = 0.7 can lead to a fairly steep
dV/dlambda and some large forces near lambda=1, which is why I
recommend sc-alpha = 0.5. This parameter is actually fairly sensitive.
This *could* lead to crashes, but I don't know about
freezing/vibrating.
Let me know if this helps.
Best wishes,
David Mobley
.55 .20 .27
.13 .21
I can't find where it's explained what this information means. For
example, why are there x's between some numbers and not others?
Thanks!
David Mobley
UCSF
http://www.dillgroup.ucsf.edu/~dmobley
___
gmx-users
David,
The order is that from low temperature to high temperature (as you could
check from the edr files) and when swaps happen the coordinates and
boxes are exchanged between CPUs.
OK. In other words the replicas are always ordered by temperature.
As a follow-up question, is there an
I have further replica exchange questions...
The order is that from low temperature to high temperature (as you could
check from the edr files) and when swaps happen the coordinates and
boxes are exchanged between CPUs.
OK. In other words the replicas are always ordered by temperature.
Maik,
It just came to my mind, that the behaviour, I described in the first
mail will be quite dangerous, whenever #define statements are in the
topology, cause this would lead to the insertion of the FF-values in the
topology, when preprocessing, and then be copied into the B-state
Maik
I just found a strange behaviour of GROMACS, when processing topologies
with B-values. Maybe I just think of it as unintuitive/bug, but here we go:
e.g. OPLS
Consider an angle given (all atoms have B-values, which angle-parameter
can be found by GROMACS in the bonded.itp for the A-
file, but this is not at all
transparent.
I'll poke around in the source and see if I can figure out what's
going on but I thought I might be able to expedite things by an e-mail
to the list.
Thanks,
David Mobley
http://www.dillgroup.ucsf.edu/~dmobley
a bugzilla with an example input file, I think.
It's possible the problem is on my end somewhere, but as far as I can
tell I'm not doing anything I'm not supposed to...
Thanks,
David
On Jan 3, 2008 2:33 PM, David Mobley [EMAIL PROTECTED] wrote:
All,
I'm trying to simulate a peptide/water/cosolvent
a viable option.
Thanks,
David Mobley
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Probably the easiest way for you to get an answer to this is to look
up the references which discuss the parameterization of the GROMOS
force field. Consistency is the name of the game. See here:
http://wiki.gromacs.org/index.php/Parameterization
David
On Nov 25, 2007 1:21 AM, Q733 [EMAIL
David,
As Mark answered there is no out of thebox polarizability. AFAIK there
is no complete force field like that in Amber either, only Tinker has one.
Just to clarify here, AMBER has an implementation of AMOEBA, Jay
Ponder's polarizable force field that is also implemented in Tinker.
So yes,
David,
Interesting, does that include all the multipoles and buffered 7-14
potentials etc?
Yes. My understanding is that the implementation is somehow separate
from the main AMBER implementation and actually requires a copy of
Tinker to set up the input files, but this may have changed (I
Hi,
servaas michielssens wrote:
I used amb2gmx.pl (from http://chemistry.csulb.edu/ffamber/) to convert
an amber topology and restart file to a gromacs topology and structure
file and tried to continue the simulation in gromacs. I got the
following error message:
Constraint error in
Chris,
I don't know the answer to the exact question that you have posed, but
I instead suggest that getting rid of that water molecule is not a
good idea. You should rather minimize your system. While minimizing,
be sure to include
define=-DFLEXIBLE
in your .mdp file
Just out of
Nov 2007, David Mobley wrote:
Dear Bharat,
OK, I went ahead and ran with your topologies using my own run
scripts. My runs haven't finished yet, but looking at just
dV/dlambda values from equilibration, I seem to be seeing roughly
the same trends you do. In particular:
(1
).
Bharat, be sure you submit a bugzilla and we'll see how things go from
there. I may at some point try setting up some of my own relative free
energy topologies and see if I see the same effects, but I'm not
likely to have time for that for a couple days.
Thanks,
David
On 11/12/07, David Mobley
versus discharging is that
charging is where the A state has zero charges and the B state has
normal charges, and discharging is the reverse. So charging is the
scenario you describe, and discharging is the reverse.
David
Berk.
From: David Mobley [EMAIL PROTECTED]
Reply-To: Discussion list
Bharat,
Your values for the first set of calculations (the forward case?)
below look really weird. I suspect you have something messed up in
those runs. Have you checked that your define statements worked
properly, and checked your run input files? In particular, your
dv/dlambda is staying almost
Dear Bharat,
OK, I went ahead and ran with your topologies using my own run
scripts. My runs haven't finished yet, but looking at just
dV/dlambda values from equilibration, I seem to be seeing roughly
the same trends you do. In particular:
(1) The forward simulation always gives dv/dlambda
Hi,
By reactivating the barostat as mentioned below, I managed to recover LJ
energies within 0.1% for my test system, which was a box of 1136 waters.
So I applied the same thing to my system of interest (a 605 residue
protein with around 25000 waters). The only difference is that the run
was
Hi,
Everything goes fine till this point. Now, i do reverse transformations to
check for hysteresis. For vdw transformations, i get almost perfect
overlap of dG/dlambda vs lambda for forward and reverse transformations,
but for coloumb transformations, if i don't use soft-core potentials, i
Hi,
it is fairly straight FORWARD.. forward is from state A to state B, and
reverse is from state B to state A. Say for example, forward
transformation is going from ethane to methane. in this step, i define
three of the terminal hydrogen on say C2, with zero charges and C2 with
charge of
Hi,
i am extremely sorry here.. i am plotting dg/dl vs lambda of reverse
transformation onto that of forward with both axes reversed. so i
should expect overlap. this is consistent with whatever you are saying. i
am sorry for negligence and confusion.
And taking the negative?
but when i
Dear Michel,
Are you sure you're using 3.3.1? I have not checked this specific
issue -- but I have checked that if I run hydration free energy
calculations in patched 3.3.0, and again in patched 3.3.1, and do my
usual free energy analysis using mdrun -rerun, I get the same values.
That either
Hi,
Depends on what you mean by the potential energy of only the
protein. The protein alone in what environment? (And what do you hope
this will tell you?)
One thing you can do -- assuming this is what you want to do -- is
strip out all of the waters and then use mdrun -rerun to evaluate the
Just my unasked-for two cents: Langevin dynamics in water is probably
a poor substitute for some representation of water. Langevin can
provide some of the friction/noise of water -- but electrostatics
interactions are very different in water than in vacuum. Langevin
dynamics is probably not a
Hi,
is it possible to do thermodynamic integration in Gromacs using non-linear
scaling of the lamda paramerter?
I'm not sure exactly what you mean, so first I'll answer what I think
you mean, and then tell you what I think you ought to be asking. :)
If you mean, Is it possible to perform a
Hi,
Many
articles didn't give out the validation procedure of their topologies in
detail, are there some classic articles explaining how the forcefield we
used today, such as OPLS, GROMOS, AMBER and CHARMM , developed? I want to
know how they were deduced from the very beginning.
There is
First, thanks very much for your instruction. If quantum chemical
calculation does not have any physical meaning, how should I decide the
partial charge for a molecule?
David is correct, he was referring to Mulliken charges.
Again, there is no *right* answer to this, the name of the game is
All,
I may be in a hole of my own digging, here, but I've been trying to
simulate a large set of small molecules in explicit solvent. I'm using
the Amber GAFF parameters, converted over to GROMACS using our
amb2gmx.pl script.
The problem I'm running into is that for anything with a triple bond
Alan Dodd's suggestion is nice, but there isn't always a lot of
experimental data available for a particular molecule we can compare
with -- or perhaps we want to begin with good parameters and then
see if our method can reproduce experiment. Anyway, for whatever
reason it isn't always possible to
David,
On 10/16/07, David van der Spoel [EMAIL PROTECTED] wrote:
David Mobley wrote:
All,
I may be in a hole of my own digging, here, but I've been trying to
simulate a large set of small molecules in explicit solvent. I'm using
the Amber GAFF parameters, converted over to GROMACS
,
David Mobley
UCSF
http://www.dillgroup.ucsf.edu/~dmobley
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Dear Qin,
I believe the GROMACS manual recommends doing constant volume
equilibration prior to doing constant pressure equilibration. This is
what I always do. My understanding is that the Berendsen barostat
tends to be rather picky and crash (as you're seeing) when the
system is changing
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