Lee-Ping Wang wrote:
Hi everyone,
I've been trying to get a microcanonical (energy conserving, NVE) MD run
with periodic boundary conditions. I'm using the provided box of 216
water molecules and the SPC force field (flexible). When I turn PBC
off, the energy RMSD is <0.01kJ/mol with a 0.1fs t
Hi everyone,
I've been trying to get a microcanonical (energy conserving, NVE) MD run
with periodic boundary conditions. I'm using the provided box of 216
water molecules and the SPC force field (flexible). When I turn PBC
off, the energy RMSD is <0.01kJ/mol with a 0.1fs time step (energy is
con
You should use neither, at least not for Coulomb. Only PME can be used for
systems containing charges. For system containing exclusively neutral
molecules, you can use a shift function, if the cut-off is longer than the
range of the interaction. For water that would be roughly 1.2 nm.
Be that
A B wrote:
Please refer to my recent paper, J. Chem. Theor. Comp. 2 (2006) 1-11.
Yes, this is exactly what I mean - an appropriate smoothing function
("shift") works fine, but simple group-based truncation does not; that
this does not work has indeed been known since long before GROMACS was
Please refer to my recent paper, J. Chem. Theor. Comp. 2 (2006) 1-11.
Yes, this is exactly what I mean - an appropriate smoothing function
("shift") works fine, but simple group-based truncation does not; that this
does not work has indeed been known since long before GROMACS was born.
Mayb
can you please send this paper to me? email address : [EMAIL PROTECTED]
regards,
karamyog.On 5/22/06, David van der Spoel <[EMAIL PROTECTED]> wrote:
A B wrote:> I am curious about the reason for the heating that allegedly occurs with> cutoffs in NVE simulations ("The use of (electrostatic) cutoff
A B wrote:
I am curious about the reason for the heating that allegedly occurs with
cutoffs in NVE simulations ("The use of (electrostatic) cutoffs is well
known to cause heating in NVE simulations."). This should not, and does
not, happen if an appropriate smoothing function is applied. Does t
I am curious about the reason for the heating that allegedly occurs with
cutoffs in NVE simulations ("The use of (electrostatic) cutoffs is well
known to cause heating in NVE simulations."). This should not, and does not,
happen if an appropriate smoothing function is applied. Does this heating
karamyog singh wrote:
I guess since after the first run, the forces between atoms is not
zero(only negligible), when i do the 2nd run, the atoms start moving
under the action of these forces and since there is no temperature
scaling or pressure scaling, we can or might see an increase in KE as
I want a constant energy simulation at 0.01 K . Is it possible. I
cannot keep increasing my cut off because for that i have to increase
my box size.
I have tried so many times but the temperature increases and neither is the energy constant. :(
-
karamyog. :(On 5/19/06, karamyog singh <[EMAIL PROT
I guess since after the first run, the forces between atoms is not
zero(only negligible), when i do the 2nd run, the atoms start moving
under the action of these forces and since there is no temperature
scaling or pressure scaling, we can or might see an increase in KE as
in my case. So an increase
karamyog singh wrote:
Well, I am back. Remember my first and second mdruns. In my second,
after stablizing my initial configuration in the 1st md run, I used cut
off upto 6.3 whereas the potential minima is at 0.309. 6.3 is quite
large a distance compared to 0.309. In the second run, the kinet
Well, I am back. Remember my first and second mdruns. In my second,
after stablizing my initial configuration in the 1st md run, I used cut
off upto 6.3 whereas the potential minima is at 0.309. 6.3 is quite
large a distance compared to 0.309. In the second run, the
kinetic energy increases which
karamyog singh wrote:
I know where the minimum is and I said exactly what you did. However I
interpreted the potential becoming 0 as the point before r-min. The
potential once becomes 0 before minimum potential value. I thought you
were referring to that point and that is why i got confused and
I know where the minimum is and I said exactly what you did. However I
interpreted the potential becoming 0 as the point before r-min. The
potential once becomes 0 before minimum potential value. I thought you
were referring to that point and that is why i got confused and asked
you further questio
karamyog singh wrote:
I placed the atoms randomly means i used random atomic positions, not
velocities. The velocities were 0 initially and then I generated
velocities at 0.01 K.(1st MD run to get a stable configuration) After
that I subjected this structure that I got to NVE.(2nd MD run) Now o
I placed the atoms randomly means i used random atomic positions, not
velocities. The velocities were 0 initially and then I generated
velocities at 0.01 K.(1st MD run to get a stable configuration) After
that I subjected this structure that I got to NVE.(2nd MD run) Now over
here I will try with n
karamyog singh wrote:
I exactly did that. I initially thought that since I have placed the
atoms randomly so it is probable that atoms experience large forces and
since I am not allowing any temperature scaling etc. , I am getting
large KE. Therefore I first minimized my configuration. I got a
I exactly did that. I initially thought that since I have placed the
atoms randomly so it is probable that atoms experience large forces and
since I am not allowing any temperature scaling etc. , I am getting
large KE. Therefore I first minimized my configuration. I got a frozen
structure by doing
karamyog singh wrote:
I almost removed everything. I am generating initial velocity at 0.01 K
so the system should freeze. Its a dilute gas. But somehow I am getting
very large velocites i.e. very large KE of the whole system.
That .mdp looks fine for NVE. Use g_energy -w to see the evolution
I almost removed everything. I am generating initial velocity at 0.01 K
so the system should freeze. Its a dilute gas. But somehow I am getting
very large velocites i.e. very large KE of the whole system.
here is my .mdp file.
---
integrator = md
t
karamyog singh wrote:
my system is simple gas and is interacting under simple LJ potential.
isn't there a simpler way to do a simulation for a constant energy mode?
It doesn't get any more simple than "don't do anything"! In gromacs,
something approximating NVE is the result of doing nothing.
my system is simple gas and is interacting under simple LJ potential.
isn't there a simpler way to do a simulation for a constant energy mode?
i can remove pressure couling and temp. coupling. what kind of rigorous
bond constraint algos do you mean? can you throw some more light on
this topic?
th
karamyog singh wrote:
dear gromaxers.. how do i simulate a system under constant energy mode.
Don't perturb the energy that is, don't use temperature or pressure
regulation and use rigorous bond constraint algorithms. Be aware that
use of cut-offs is inherently non-conservative of energy.
dear gromaxers.. how do i simulate a system under constant energy mode.
thanking you guys in advance.
-
karamyog.
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