Dear all,
I am using GROMACS-4.6.5 for studying gas hydrates and related
systems.
A useful order parameter which indicates water to hydrate transition is the
F4 order parameter where F4 is related to the H--O--O--H dihedral angle for
a pair of water molecules.
It is found that F4
Dear all,
I am using GROMACS-4.6.5 for studying gas hydrates and related
systems.
A useful order parameter which indicates water to hydrate transition is the
F4 order parameter where F4 is related to the H--O--O--H dihedral angle for
a pair of water molecules
Exact expression for F4 can be
Hello,
I guess it is not unusual for gaseous systems to have positive energy. I
hope that the Fmax criteria is satisfied.
Sujith.
On Wed, Aug 12, 2015 at 10:30 AM, Sunil Ghimire ghimiresuni...@gmail.com
wrote:
I mean potential energy of system (1600 argon atoms) is positive after
energy
Dear all,
I am studying the CH4-CO2-H2O mixture at low T(270K) and high P (20 bar).
Forcefields used: CH4 : Single point LJ site; CO2 : EPM2 (Rigid with two
virtual sites); H2O: TIP4P.
I computed the free energy of solvation for a CH4 molecule in H2O in the
presence of CO2 at different
Hello Justin,
Thanks for the mail.
I am interested in knowing whether the particle type assigned has any role
in the way it is treated by the program. For both virtual sites and the
regular atoms, interaction parameters and mass are assigned. So in Gromacs,
does the particle type (A or V) has
Dear Justin,
I am following your tutorial about CO2 topology using virtual sites.
I find that in the topology provided, you have not reassigned the particle
type as virtual (V) for the C and O atoms (which are treated as the virtual
sites in the model). Instead, they are directly selected from
Dear Justin,
I am following your tutorial about CO2 topology using virtual sites.
I find that in the topology provided, you have not reassigned the particle
type as virtual (V) for the C and O atoms (which are treated as the virtual
sites in the model). Instead, they are directly selected from
Hello,
I am observing nucleation and growth of bubbles in a solution of methane
in water with methane present at various levels of supersaturation.
The system consists of a total 0f 2000 molecules in a cubic box with the
number of CH4 varying from 80 to 200. I am using a single point Lennard
/6qnoy5o4/strange-behavior-of-water-droplet-on-a-solid-surface-with-verlet-cutoff-scheme-in-gmx-5-0-4
).
Regards,
Jan
2015-07-18 8:53 GMT+02:00 sujithkakkat . sujithk...@gmail.com:
Hello,
I am observing nucleation and growth of bubbles in a solution of
methane
in water
Dear all,
I am simulating a system of small hydrophobic solutes ( CH4) dissolved
in water. Simulations are performed in the NPT simulation, and I would like
to determine the diffusion coefficients from MSD plots. I have two related
questions;
(1) Is the thermostat going to seriously affect
Dear all,
Is it possible that a model for a simple molecule (say CO2) which can
accurately predict macroscopic properties (like density), but still can
have error in the microscopic behavior, like diffusivity or the pair
interaction functions ? Please share your thoughts.
Regards,
Sujith.
are you able to reproduce the original
parametrization results?
Mark
On Tue, Feb 3, 2015 at 8:04 AM, sujithkakkat . sujithk...@gmail.com
wrote:
Dear all,
I tried simulating the CO2-water mixture with CO2 at a low
concentration (0.003 mole fraction) at various temperatures at 1 atmos
Dear all,
I went through the mails about the use of virtual sites for
representing linear molecules like CO2. I also read that GROMACS cannot
handle angle bending potentials at 180 degrees in an appropriate manner.
My system consists of EPM2-CO2 dissollved in TIP4- H2O.
I
for some
distances however.
Erik
Kind regards,
Erik
On 9 Dec 2014, at 06:39, sujithkakkat . sujithk...@gmail.com wrote:
Dear all,
I read in *Phys. Chem. Chem. Phys., 2009, 11, 10427-10437*, that the
radial distribution function is directly related to Potential of mean
Dear all,
I read in *Phys. Chem. Chem. Phys., 2009, 11, 10427-10437*, that the
radial distribution function is directly related to Potential of mean force
through RDF=exp(-PMF/kT).
My question is why would someone worry about computing PMF in a simple
case like interaction between two
Dear all,
I am trying to simulate a water-carbondioxide system at 250K and
30bar. The system consists of 85 CO2 and 1204 water molecules in a 3x3x4 nm
box.
I used EPM2 and TIP4P potentials for CO2 and water following *Energy
Environ. Sci., 2012, 5, 7033-7041* where the authors
, if it could, it would drive the system to HCO3-/H3O+, which is an
energetically more favorable way to store CO2 in water.
Cheers,
Tsjerk
On Dec 8, 2014 6:50 AM, sujithkakkat . sujithk...@gmail.com wrote:
Dear all,
I am trying to simulate a water-carbondioxide system at 250K
Dear all,
I am studying a water-methane system with tip4p-Ice for water and
oplsaa for methane.
What I want to try is modify the intermolecular non-bonded interaction
between methane and water. I just want to multiply the combination rule
(geometric mean) used to obtain the mean well depth
Hello,
I would like to know if it is possible to plot the RDF of water
molecules belonging to the solvation shell of a solute. I mean, I want to
know the effect of the solute on the water arrangement in the solvation
shell. Is there a way to do this?
Regards,
Sujith.
--
Gromacs Users
On Thu, May 22, 2014 at 8:18 PM, sujithkakkat . sujithk...@gmail.com
wrote:
Hello,
I would like to know if it is possible to plot the RDF of water
molecules belonging to the solvation shell of a solute. I mean, I want to
know the effect of the solute on the water arrangement
On Tue, May 20, 2014 at 12:50 PM, sujithkakkat . sujithk...@gmail.com
wrote:
Hello,
I am working on a water-methane system with OPLSAA for methane and
TIP4P/Ice for water.
What I find strange is that after solvating the methane molecule with
water
(tip4p/ice) using the genbox
Hello,
I am working on a water-methane system with OPLSAA for methane and
TIP4P/Ice for water.
What I find strange is that after solvating the methane molecule with water
(tip4p/ice) using the genbox routine, the density appears to be very high
at 1661.04 (g/l) . The number of water molecules
at 8:58 PM, Justin Lemkul jalem...@vt.edu wrote:
On 5/14/14, 12:39 AM, sujithkakkat . wrote:
Hello Justin and others,
Thank you for the response . Here are mode details of the system; ( in
the order ; MDP settings, itp and top files) . The system consists of 460
water molecules and 1
Dear all,
I am running simulations for a water-CO2 system using the OPLSAA
forcefield, where I use TIP4P/Ice water model and the EPM2 model for CO2.
After energy minimization I found the value of potential energy to be
positive, and also the maximum force value was high (I requested Fmax 10
Hello Justin and others,
Thank you for the response . Here are mode details of the system; ( in
the order ; MDP settings, itp and top files) . The system consists of 460
water molecules and 1 CO2 molecule . I am trying to find the free energy
of solvation for CO2 in water at various
Dear all,
I want to study a system consisting of water, methane and CO2. I will
use TIP4P/Ice , OPLSAA and EPM2 models respectively for the components .
My problem is, how do I make a choice of the cutoff lengths, for a
system which uses different molecular models which were
Hello Justin,
I found that in the virtual sites section of your tutorial, the energy
values of the system large positive . You had warned in the topology file
that the choice of the partial charges used are not guaranteed to work
always with OPLSAA . However, the momentum of inertial values
Hello Justin,
I tried the free energy calculations in your tutorial at different sets
of conditions. Also I repeated a simulation at the same conditions with
same parameters, thrice on the same computer on same number of processors.
The results in the three cases where different (4.16 +/- 0.19
constraint_algorithm= LINCS
continuation= no
lincs_order = 4
lincs_iter = 1
lincs_warnangle = 30
Regards,
Sujith.
On Wed, Mar 12, 2014 at 5:28 PM, Justin Lemkul jalem...@vt.edu wrote:
On 3/12/14, 7:51 AM, sujithkakkat . wrote
be that you've appended to a previous 5ns
trajectory, not run a new trajectory. Check the .log file and the length of
time you expected this job to run (wall and simulation).
Mark
On Fri, Mar 14, 2014 at 9:02 AM, sujithkakkat . sujithk...@gmail.com
wrote:
Hello,
This time I tried
Hello,
After a while I got back to the problem posted here. This issue was the
large value for average pressure(~25 bar against the reference pressure of
1 bar) in NPT simulations with parrinello rahman barostat. The system
studied is cyclohexane-water system with an interface.
The forcefield
Hello,
I am following justin lemkul's tutorials for the cyclohexane-water
biphasic system using Gromos96 forcefield.
Things went well till NVT equilibration where I had this Blowing up issue.
Shortening the time step alone did not help, and it was difficult for me
to figure out what was
Dear GROMACS users,
I am new to GROMACS, and recently started using the version 4.6.5.
I have seen a lot of NPT related issues raised earlier in this forum, but
in my case the error looks much more severe.
I am following Justin Lemkul's tutorial (
Hello,
Thank you both for the comments. I am using gromos96 forcefield . I read
a little bit and as you said the nonbonded cutoff has to be higher.
The tau_p=5ps was chosen , since the manual mentions that the value has to
be raised by 4-5 times on going from berendsen to parrinello-rahman
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