to run
the version 3.3.1 .tpr file through the version 3.2 tpbconv program to
get a new .tpr file, or would it yield the same error?
Thanks for any suggestions
--Michael Skaug
University of California Davis
___
gmx-users mailing listgmx-users
One other thing I would point out is that the solvation free energy is
dependent on concentration. you will get a different result with 4
polymer chains vs 3 vs 3, etc. Make sure you understand the
dependence. Also, the free energy will depend on the polymer chain
length.
Polymer and finite con
no additional constraints but with
"comm_mode = Angular" i get results somewhere inbetween the two cases
above.
my specs:
Gromacs version: 4.5.3
Linux 2.6.35-23-generic Ubuntu x86_64
gcc version 4.4.5
I am not sure whether i overlooked something in my input,
or whether there's
, as in: "removing" something thats
negative)
is that correct? ... and if so, why does it, seemingly, not apply in the above
Gedankenexperiment?
Yours truly (and maybe some other people) would really appreciate if somebody
in
the know
would clarify that!
thanks in advance!
Michael
> Michael: your mdp options indicated using US and my stance is that, > using
>US, you are incorrect to say that "And you will get the SAME > result if you
>do this calculation in one or in three dimensions > (pulldim NNY or pulldim
>YYY)".
this has nothin
mircial at sjtu.edu.cn mircial at sjtu.edu.cn wrote
> I am using GROMACS package to do molecular dynamics
> simulations under OPLS_AA force field. I encounter
> some problems when preparing the topology files
> of small molecules (ligands).My questions are as follows:
> 1, how to chose the atom
Hi, all-
Have you tried running
constraints = hbonds?
That might eliminate some of the constraint issues. Much less likely
for LINCS to break or have DD issues if only the hbonds are
constrained. 2 fs is not that big a deal for the heteroatom bonds.
Best,
Michael
On Thu, Mar 10, 2011 at 8
> I am doing free energy calculation in Gromacs and want to get an error
> estimate of my results. Is it possible to compute the autocorrelation time
> of dVpot/dlambda in Gromacs using a certain length of trajectory such as 10
> ns? Thanks a lot
The amount of simulation time required to compute t
er:
i) is there any limit to the size of tau_t I am supposed to use? or
ii) is there any other way to accelerate convergence?
FTR: I also tried using two tc_grps (one for each particle)
but, at least qualitatively, i see the same results.
thanks in advance for any help!
regards,
Michael
===
I recently came across a paper (J. Phys. Chem. B 2005, 109,
10441-10448) in which the authors found that using implicit
solvent with explicit ions you easily end up with all the
ions cuddling up in clusters ... which is obviously an artefact.
That is, if you do use this combination you certainl
are oscillating as expected, but the forces on the
reference group are close to, but not exactly(!) zero.
i am not sure how to interpret this ...
cheers
Michael
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Please search the archive
e searched the net for this error and didn't find any answer. Did anybody
see this error? and what should i do with it..
Thanks,
Michael
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Ignacio,
I would be very interested in a rigid body capability.
On 3/28/2011 5:45 AM, gmx-users-requ...@gromacs.org wrote:
Is there still interest in rigid-body simulation?
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x27;d appreciate any suggestions!
(below is my mdp file.)
cheers,
Michael
mdp file:
integrator = md
;
dt = 0.001
tinit= 0
nsteps = 10
nstxtcout= 0
nstxout = 1000
nstvout = 0
nstfout
Elisabeth,
You CAN, in fact calculate the contribution of the reciprocal part
of the PME energy to the binding energy between two components in
a heterogeneous system, its just quite tedious...
say, your system is molecules A and B for which you want to know
the interaction energy, and the rest
Elisabeth wrote:
> The point is in my case there is no option other than ignoring LR since LR
> is not covered by shift or switch functions but at least what PME reports
> for SR is more accurate.
not really ... PME electrostatic energy is a sum of two contributions
LR and SR ... and only the SU
which making sugar topologies is as straight forward as making
topologies for amino acids, or if there is no such thing for which FF is
making a sugar topology the least tedious?
BTW: I want to model simple sugar molecules, monomers,
dimers (no polymers)
thanks!
Michael
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seen something similar ?
i'd appreciate any suggestions!
thanks
Michael
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Please don&
ling= no
constraints = hbonds
constraint_algorithm = lincs
morse= no
---
On 5/30/11 8:45 PM, Michael D. Daily wrote:
Thanks for the recommendations everyone. I tried all of the mdp
changes recommended by Justin (increase rlist, rvdw, etc to 2.0;
change T-coup
https://sites.google.com/site/thomasevangelidishomepage/
--
Michael D. Daily, Ph.D.
Postdoctoral Fellow
Qiang Cui group
Department of Chemistry
University of Wisconsin-Madison
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Hi everyone. I'm doing a simulation of a system where a peptide is linked to a
surface and an AFM tip is brought in contact to do force measurements.
The AFM tip moves very slowly (1nm/ms), so I'm simulating stationary tips at
various distances. Does anyone know the most direct measurement f
>
>
I've also seen people use PyMOL's builder to do this. Either way, you'll
need to take (a lot of) extra care to minimize your linker and make sure
that it looks reasonable.
-Michael
> Nevertheless, I'd suggest simply omitting that part of the protein and
> capp
> It also depends whether or not you use constant pressure, in which case it
> makes sense to increase the time to long enough to let the volume relax.
> I still do not understand why people do NVT REMD, because it makes all but
> one replica have a pressure that is not the ambient pressure.
If al
system
so problems are documented. I'm also working on the updates to free
energy code in 4.6, so I want to make sure this will be solved there
as well.
Best,
Michael
On Fri, Mar 23, 2012 at 7:16 AM, Sabine Reisser wrote:
> Hi Mark,
>
> with FE, without PR : same error
> without FE
Sabine, thanks for filing it in redmine! Having a record helps a lot.
Can you also attach all your input files to the redmine filing? It
can only really be debugged if the input files you used are included.
Best,
Michael
On Fri, Mar 23, 2012 at 9:11 AM, Justin A. Lemkul wrote:
>
>
&g
unless I can reproduce the error you are describing out of the box,
its unlikely I will be able to find it.
Additionally, it would be easiest if the files were deposited as a
redmine bug report, so that the information is centrally located.
Best,
Michael
On Thu, May 10, 2012 at 12:23 PM, francesco
Gromacs already supports replica exchange -- what particularly are you
implementing?
Equilibration of pressure is always a good idea -- even if you are
running NVT simulations, you want to get them to be at the equilibrium
volume for your system and temperature choice, which will require
equilibra
There's a fair amount of interest for more general support for Monte
Carlo methods in GROMACS 5.0. However, there is no any current
support for configuration bias Monte Carlo (or any other kind of MC)
currently in the code.
On Fri, Jun 1, 2012 at 12:10 PM, Benjamin Haley wrote:
> Hello,
>
> I
> Could you tell me is there any difference of different Tau_t ussage (
> inverse friction in case of Stochastic dynamics) for simulation of
> water-soluble as well as membrane-proteins ? In the first case I'm
> using tau_t 2ps that is lower than internal water friction. In the
> second case one pa
I assume PLUMED will be implemented for Gromacs 4.6, as many PLUMED
developers use Gromacs. Perhaps any PLUMED lurkers on the list can
speak up. . . .
On Wed, Jan 16, 2013 at 9:20 AM, Mark Abraham wrote:
> The GROMACS team has no plans for that. The usual problem here is that
> everybody would l
Hi, Joakim-
Expanded ensemble is still a bit experimental. I don't immediately
see any problem that jump right out, but if you go to
http://redmine.gromacs.org/ and file a bug report, including giving
example files that cause the problem, I can take a look at it.
On Tue, Feb 5, 2013 at 6:00 AM,
The coordinates and velocities that are printed (and that are used to
calculate the properties like energy, virial, etc) are always
consistent with the constraints. The exact order of how things are
done often depends on the integrator. For example, velocity scaling
can be done before or after co
Ah, now perhaps I see that I misread the question - it could have been
phrased more clearly. If Erik understood it correctly, then the
answer to the question is: It depends on the integrator. The
simulation is not constrained to a particular temperature or pressure
- rather, the dynamics are modi
My personal opinion is that for large protein-protein calculations,
the free energy should be computed through potential of mean force
calculations, NOT alchemical methods, using the endpoints (properly
corrected) to determine the free energy of association.
There are a number of tutorials and exa
There is no theoretical reason to exclude it. The CMAP code is routed
differently in the logic, and was put in at the same time the free
energy code was, so it's just software engineering issues.
This is a good candidate for inclusion in 5.0 if enough people request.
On Wed, Feb 27, 2013 at 1:04
Hi, Joakim-
Hamiltonian exchange only should work if there is a lambda coupling
parameter that defines the potential at each state. You need to
define your pulling potential so that the coupling-lambda parameter
can be used to define the different pulling location centers along
your trajectory.
Great -- if it doesn't seem to be working the way it should after some
playing around, then submit it as a redmine issue, and I'll take a
look.
On Fri, Mar 8, 2013 at 2:51 AM, Joakim Jämbeck wrote:
> Dear Michael,
>
> Thank you for your reply.
>
> Yes, it is relative
more general multistate lambda vector formalism for 5.0.
If you have suggestions, let me know.
I'd be happy to look over input files or give additional advice on a
specific setup.
On Tue, Apr 2, 2013 at 12:52 PM, Dejun Lin wrote:
> Hi Michael,
>
> Do the codes now support walk
You have to change atom types. For example:
[ atomtypes ]
;name bond_typemasscharge ptype sigma epsilon
h1h1 0. 0. A 2.47135e-01 6.56888e-02
h1_pert h1 0. 0. A 2.47135e-01 3.56888e-02
; perturbed
The
Quick check here -- is 4.6 behaving correctly? I actually spent some
time working on REMD in 4.6, and it seems to be behaving correctly in
my hands with temperature and pressure control.
Thanks for any additional info on this!
On Thu, May 2, 2013 at 8:18 AM, Mark Abraham wrote:
> On Thu, May 2
l try gmx-4.6.1
>
> On May 2, 2013, at 2:26 PM, Michael Shirts wrote:
>
>> Quick check here -- is 4.6 behaving correctly? I actually spent some
>> time working on REMD in 4.6, and it seems to be behaving correctly in
>> my hands with temperature and pressure cont
I
> turned it off during compilation …
>
> You could try to run on particle decomposition to see if you get a problem …
> it should one quite quick.
>
> On May 2, 2013, at 2:36 PM, Michael Shirts wrote:
>
>> Both. So if 4.6.1 doesn't work, I want to know so we
Summarizing!
On Fri, May 3, 2013 at 12:31 AM, XAvier Periole wrote:
>
> Are confirming that you reproduce the problem with gmx-4.6.1 or simply
> summarizing in case we lose track :))
>
> On May 2, 2013, at 23:31, Michael Shirts wrote:
>
>> So to summarize -- the pr
I can't think of any instance where nose-hoover chains provides an
advantage over nose-hoover in a large system -- all the demonstrations
of superiority are in model systems that are not particularly chaotic.
As the system gets more chaotic, it matters less.
I would go with md, nose-hoover (w/o c
that are solved by NH chains are for small toy
systems.
On Sun, Jun 2, 2013 at 2:17 AM, James Starlight wrote:
> Michael,
>
>
> thanks for suggestions.
>
> the main reason of ussage N-H with chains is the assumption that simple N-H
> does not provide ergodicity of the system
It only matters for running on Folding@Home. For other users of
gromacs, it doesn't do anything.
On Tue, Jun 26, 2012 at 3:50 PM, Bao Kai wrote:
> Hi, all,
>
> I am wondering what the --enable-fahcore option of configure means. I
> got the explanation from configure --help of "create a library
s for any advice!
michael
mdp:
integrator = sd
nsteps = 10
dt = 0.002
;
pbc = xyz
nstcomm = 100
comm_grps = System
;
nstxtcout =
0
nstenergy = 100
ns
Hi,
i just performed a free energy TI calculation, to get the
free energy of solvation of water in water (the chemical potential of water)
i stuck closely to the templates given in the tutoral by justin lemkul.
The final result i get with g_bar looks good, and the number is within the
error-bars
hi
as suggested in: http://www.gromacs.org/Developer_Zone/Roadmap/GROMACS_4.6
i do:
prompt> git clone git://git.gromacs.org/gromacs.git
Cloning into 'gromacs'...
remote: Counting objects: 119131, done.
remote: Compressing objects: 100% (21428/21428), done.
remote: Total 119131 (delta 100642), re
id
here ? if this is so
it might be a good idea making g_bar read tpr files to give a warning in such a
case ...
i guess for now i'll wait for a stable 4.6 - any ideas when this will be there?
thanks!
michael
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eparate calculations (mutation in vacuum and mutation in
solvent)
compare?
cheers
michael
===
Why be happy when you could be normal?
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t now constraints are not applied to waters at all (O and
H look as if they move independently)
it also didn't help renaming the water molecule, residue and atom names ...
any suggestions on how i can apply atom-based cut-off with lincs or shake to
water?
thanks
her in terms of methods nor
references)
I don't know what P. H. Hünenberger said in his talk, but i am mostly concerned
about correction terms discussed here: J. Phys. Chem. 1996, 100, 1206-1215
thanks,
michael
===
Why be happy when you could be normal?
--
g
The implementation of BAR in gromacs is pretty hard for me to follow
because of how everything is stored noncompactly in the histogram. In
4.6, both can be computed from the same dhdl.xvg file, so it might be
easier to track down possible bugs.
On Fri, Jun 29, 2012 at 2:24 PM, David van der Spoel
ncy than the nonbondeds, which will be another useful way to get
longer times steps. We also have planned to implement a Monte Carlo
barostat, which will give exactly the correct NPT distribution for any
integrator.
Best,
Michael
On Fri, Jul 27, 2012 at 2:01 PM, Katie Maerzke wrote:
> Hi all -
&
Hello All -- I'm trying to do a normal modes analysis of a fairly
large crystal system (~20,000 atoms) in double-precision GROMACS. The
system is xy periodic with 2 9-3 walls, and has periodic molecules. I
first minimized the structure with L-BFGS to 1e-5 tolerance with
switched vdW interactions an
n, it will be possible
to parameterize lipids that behave correctly.
Best,
Michael
On Sun, Aug 19, 2012 at 3:16 PM, David Ackerman wrote:
> Hello,
>
> I was wondering when it is appropriate to use Dispersion Correction
> for lipid bilayers, or which setting (no, EnerPres, or Ener) is
(?), but we can plan now. Note that withe errors this
big, 100-200 ps should be enough to see what's going on, so it can be
done rapidly. Drop me a line off the list to figure out details?
Best,
Michael
On Fri, Aug 24, 2012 at 9:22 AM, David van der Spoel
wrote:
> Hi,
>
> we have terrib
I've done some extensive testing (paper on testing method in the
works) and vrescale gives a very accurate ensemble very well for NVT.
Parrinello-Rahman and MTTK are the only algorithms that are correct
for NPT. Berendsen barostat is not. Note that there is a bug with
vrescale + md-vv + that is f
up tweaks, but let's start with 4.5 scaling info!
Best,
Michael Shirts
Assistant Professor
Department of Chemical Engineering
University of Virginia
michael.shi...@virginia.edu
(434)-243-1821
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> However, the time value (4 in this example) is limited to 6 digits.
Sounds like this should be increased? There's a pending change to
replica exchange, so this could be added to 4.6 without disrupting the
release timing.
On Wed, Sep 26, 2012 at 11:22 AM, Andreas Zink wrote:
> Dear all,
>
> I
Hi, all-
There are some issues with MTTK + constraints that are being worked
out for 4.6. The good thing is, I have developed some sensitive tests
of the correct volume distribution (see
http://arxiv.org/abs/1208.0910) and the errors in PR are very, very
small. I would recommend using md + PR for
It's in review with JCTC right now.
On Thu, Nov 22, 2012 at 2:19 PM, ABEL Stephane 175950
wrote:
> Hello,
>
> This is a very nice and interesting work, Michael. Thank you for the efforts
> you made in writing this paper. I hope you will publish it.
>
Hi, all-
I would recommend using Parrinellio-Rahman + Nose-Hoover md + at least
until 4.6.
A random-walk drift in the conserved energy is actually what MTTK
gives -- it's not as conserved as, say, energy conservation, it just
has an expectation value of zero drift over time, which means that the
> In the absence of PBC, you simply have an infinite system. In a loose
> sense, that may be NVT, but V is infinite, so whether or not you can
> consider that to be constant or not is theoretical math above what I know :)
A real molecule in vacuum is usually NVE -- it is not coupled to the
enviro
Hi, I'm making a lipid topology for DPPG in the charmm forcefield in gromacs
4.5. I'm putting it together from pieces of what already exists as suggested
in the charmm files. I noticed that there are charge groups in the original
charmm files, and these were reflected in the gromacs topology i
that should help in
making a CHARMM27 DPPG rtp entry (if you wish to use the CHARMM27
lipids rather than the CHARMM36 ones).
Cheers
Tom
On 06/08/11 00:22, Michael McGovern wrote:
Hi, I'm making a lipid topology for DPPG in the charmm forcefield in gromacs
4.5. I'm putting i
= 1.1
This should work quite well -- you might get some drift after 1-2 ns,
but not much. I'm working on developing suggested PME parameters
right now for highly quantitative work, but it's not quite ready yet.
Michael Shirts
Assistant Professor
De
Hamiltonian replica exchange is planned for 4.6, and is being beta
tested by some users.
On Tue, Aug 16, 2011 at 2:39 PM, Sanku M wrote:
> Hi,
> I was wondering whether hamiltonian replica exchange simulation has been
> implemented in latest version of gromacs . Or, is there any other way of
veloping suggested PME parameters
> right now for highly quantitative work, but it's not quite ready yet.
>
>
>
> Michael Shirts
> Assistant Professor
> Department of Chemical Engineering
> University of Virginia
> michael.shi...@virginia.edu
> (
Hi all,
I am looking for a relatively easy way to make minor modifications to a
solvated system in gromacs without having to replace the whole solvent
layer. Specifically, I'm swapping out some molecules (technically, just
swapping residue and atom names) in a MARTINI model and I think this cause
rrible starting structure - fortunately the system can be
regenerated from scratch with a new lipid config overnight.
On Wed, Aug 17, 2011 at 11:54 PM, Mark Abraham wrote:
> On 18/08/2011 4:32 PM, Michael Daily wrote:
>
>> Hi all,
>>
>> I am looking for a relatively easy way to ma
And I am happy to report that this method produces a viable starting
structure :)
On Thu, Aug 18, 2011 at 7:02 PM, Michael Daily wrote:
> I tried an experiment similar to yours - after converting the POPE's to
> POPC's when I remove all waters that are near the (lipid-emulsified
ws 2.35 A as the vdw radius
for all lipid groups, which I fear will cause inaccurate calculations in
APBS. Has anyone had this problem before?
Mike
--
====
Michael D. Daily
Postdoctoral research associate
Pacific Northwest National Lab (PNNL)
509-375-4581
(form
;, 'O11','C12'],
'GL1' : ['C13', 'O14', 'C15', 'O16'],
'GL2' : ['C32', 'O33', 'C34', 'O35'],
etc.
For some atoms it's obvious which MARTINI groups they belong in, but o
ted.
Mike
On Tue, Aug 30, 2011 at 3:06 AM, XAvier Periole wrote:
>
> it must be some example of mapping lipids on the website: cgmartini.nl
>
> On Aug 30, 2011, at 3:55 AM, Michael Daily wrote:
>
> Hi all,
>
> I am trying to reverse-map some martini lipids to united a
such as the demux.pl script?)
Thanks,
Michael
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>
--
Michael D. Daily
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Pacific Northwest National Lab (PNNL)
509-375-4581
(formerly Qiang Cui group, University of Wisconsin-Madison)
--
gmx-u
hanks,
--
Michael D. Daily
Postdoctoral research associate
Pacific Northwest National Lab (PNNL)
509-375-4581
(formerly Qiang Cui group, University of Wisconsin-Madison)
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P
of worms)
thanks in advance for any help!
cheers
Michael
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Best,
Michael
On Thu, Oct 6, 2011 at 2:42 PM, Justin A. Lemkul wrote:
>
>
> Fabian Casteblanco wrote:
>>
>> Hello Justin,
>>
>> I have a question about your tutorial. If I want to mutate one small
>> group of a molecule, I would
FEP is a poorly defined term. It can either mean 1) making small
changes 'alchemical' changes in the molecules and computing the free
energies by any method (BAR, TI, etc), or 2) it can mean specifically
computing the free energies by exponentially averaging the potential
energy differences. Basi
> So BAR is only
> referring to the mathematical code used to calculate the overall free
> energy for the FEP, correct?
Yes. The information required is the same, with the exception that
exponential averaging requires energy differences from only one state,
whereas BAR requires energy differences
e:
http://pubs.acs.org/doi/abs/10.1021/jp0735987
for some additional information.
Members of the Gromacs team are working behind the scenes for various
possible solutions to the problem for nonisotropic systems. Don't
expect anything until 5.0, though.
Best,
Michael
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> Is anyone aware of any benchmark analysis about the implementation of the
> amber99sb force field (or any of its variants: 99sb-ildn, 99sb-nmr) in
> GROMACS and AMBER. I am interested to know in what extend the energies
> correlate and if the results agree with experimental data.
Whether the res
Hi everyone. I'm doing a simulation in gromacs using the charmm36 parameters
from the gromacs website. The parameters don't seem to have carbohydrates,
which are part of the charmm36 force field. In particular, I need parameters
for trehalose. Is there anywhere I can find these parameters in a
ACS manual, online tutorials etc.
Can anybody help me with this problem or guide me to appropriate tutorial.
Thanks in advance.
Michael
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> It should also be noted (and obvious now that I actually look into it) that
> using dispersion correction results in both the latent heat of vapourisation
> and density of the alkanes being over estimated (for both Cut-off and
> Reaction Field, and by the same amount).
That may not be quite t
An important final point is that you can always see EXACTLY what
grompp is putting into the B state by running gmxdump on the resulting
tpr. It's a LOT of information, but all in text all the interactions
are listed explicitly there.
On Mon, Jun 10, 2013 at 6:20 PM, Justin Lemkul wrote:
>
>
> On
If you are computing enthaply in the NPT ensemble, P is constant, and
is the applied pressure.
The "pressure" quantity calculated from the KE and the virial is not
the pressure. It is a quantity that when averaged over time is equal
the pressure. Only the average is meaningful macroscopically.
and Conference Steering Committee
Michael Shirts (chair)
Angel Garcia
Berk Hess
Yu-Shan Lin
Erik Lindahl
Peter Kasson
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> or should i be doing < U+*ref_p > = ?
More specifically, + *ref_p = H
isn't really meaningful thing. I mean, you can define something
such that = H, but that's not really thermodynamics.
> example system gives = -1168 kJ/mol and i find = -725 kJ/mol either
Interesting. What material at
Hi, Sonia-
Gromacs 4.6.2 (some bug fixes vs 4.6.1) with the example files you
point out from Alchemistry.org should work well for expanded ensemble.
David Mobley and I have been validating expanded ensemble and replica
exchange, and the files posted there now are stable for all sizes of
systems,
No.
This is a statistical mechanical issue, not a GROMACS issue. For
interacting systems, entropy is a quantity describing the system as a
whole, and cannot be defined for different parts of the system, at
least not in any way such that the individual components can be added
together.
I'm also n
Have you checked out the -ndec option for trjconv? If you have a high
precision format (.trr, or .xtc if they are stored with sufficient
precision) you can print out a .gro file (that gromacs can read) with
higher precision.
Gromacs can read .gro files with increased precisions in the
coordinates
Hi, all-
This not a problem with W-L, but is instead something that is wrong
with a particular combination of mdp options that are not working for
expanded ensemble simulations. W-L can equilibrate to incorrect
distributions because it decreases the weights too fast (more on that
later), but that
You need to have different pull parameters at the end states. Right
now, pull-kB1 is not defined in your code, so there is nothing to
interpolate to: it assume pull-kB1 = pull-k1.
Longer scale -- one would want to define reference distances that
change with lambda within the same simulation, but l
- I'd have
to dig a bit to get you good results on that . . .
On Tue, Jul 16, 2013 at 3:19 PM, Dejun Lin wrote:
> Hi Michael,
>
> Thanks for the reply. Just a quick follow-up. Do you think the overlap of
> energy histogram between different lambdas matter for lambda-dynamics in
&g
Ah, this is a force field issue -- urey-bradley terms are not
supported free energy calculations. However, since only restraints are
changing, this warning doesn't really need to be there.
It would be relatively simple to put in a check to allow this to work,
but it might take a week or two to get
4.5.7 does not support Hamiltonian exchange. It says all properties
are the same, because all the temperatures and pressures are the same
-- it won't switch the umbrellas.
On Wed, Jul 17, 2013 at 3:30 PM, Parisa wrote:
> Hi Michael,
>
> I think that this is an issue with the gro
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