[gmx-users] Negative pressure

2011-06-07 Thread Francisco Garcia
Dear user,

What is the physical significance of negative average pressure in NVT
MD simulations?

Thank you.
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[gmx-users] Optimal number of time origins in the calculation of block-averaged time correlation functions

2010-08-29 Thread Francisco Garcia
Dear users,

I am comparing different schemes for computing the self-diffusion of a
system. One of the approches
I am considering is using block averages.

I have a 50 ns long trajectory and I want to compute the
block-averaged diffusion constant as follows:

(1) Divide the trajectory into blocks of 2 ns (25 blocks of equal length)
(2) For each block compute the rmsd over all particles and Nt time
origins (25 diffusion constants in all)
(3) Compute the average and standard deviation of the 25 diffusion constants

Point (2) above is where things get tricky. When you read previous
works, authors are usually
not specific about the exact values of the parameters they used.
Currently I choose the number of origins
(Nt) and the correlation time (Tc) arbitrarily. It is obvious that the
maximum value of Nt is BL/2,
where BL is the length of each block and the maximum value of Tc =
delta_t * BL/2. My question
is how to determine the optimal number of time origins Nt and Tc per
block. Suggestions from
experienced users or any reference to an article which discusses a
scheme for choosing the Nt
and Tc would be much appreciated. I am a novice so kindly be as
specific as possible in your response.

Thank you very much
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[gmx-users] Stabilizing a heavy metal ion in solution

2010-07-12 Thread Francisco Garcia
Dear users,

I would like to know if users can give me a couple of suggestions on
how to control large temperature swings of a heavy metal ion like
Uranium in solution. The temperature of the metal ion fluctuates
considerably and hardly stabilizes--even in the long time limit while
the solvent temperature stabilizes easily. The gromacs 'what not to
do" list strongly discourages against coupling  the ion and solvent to
separate thermostats. I would like to know if experienced users can
give tips on how to alleviate this problem.
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[gmx-users] SPC/E water RDF

2010-05-28 Thread Francisco Garcia
Dear users,

Since I'm new to MD, I coded SPC/E water in the NVT emsemble.

Basic ingredients:

(1) Number of water molecules N=216
(2)   Mass of O = 16
  Mass of H = 1
(3)   Box density (Periodic Boundary Condition) is exactly 1g/cc (L
=18.6205 Angstrom)
(4)   SPC/E LJ parameters from Berendsen's original 1987 paper
(5)   Coulomb interaction: Ewald sum
  Real space ewald: Minimum image convention
  Ewald convergence parameter for reciprocal sum = 5/L (L is the
box length in Ang)
  Fourier cut-off for ewald reciprocal sum |G| =2*pi*|n|/L, where |n| < 27
(6)   Nose-Hoover chain NVT (single chain, single thermostat per chain)
(7) Time step 1 fs, velocity verlet solver, RATTLE was used to
constrain bond lengths and angle, and correct velocities.
(8) 100 ps equlibration, 400 ps production (configuration was saved every 25 fs)


Everything is fine (energies are stable, etc.) except the second peak
in the O-O rdf.
The first peak is fine but my second peak seems flat. I find this
troubling since
all the rdfs I've seen in literature as well the experimental plot
have a well-defined
second peak. I must mention that in all the papers I've seen the
ensemble is NPT (I've not seen NVT yet). In any case, I was expecting my result
to match previously published results closely.

Can anyone point out what I am doing wrong?? Is NVT not a good ensemble
for water simulation?? I'll appreciate it if someone can refer me to a paper
that discusses this.
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[gmx-users] SPC/E water rdf

2010-05-28 Thread Francisco Garcia
Dear users,

Since I'm new to MD, I coded SPC/E water in the NVT emsemble.

Basic ingredients:

(1) Number of water molecules N=216
(2)   Mass of O = 16
   Mass of H = 1
(3)   Box density (Periodic Boundary Condition) is exactly 1g/cc (L =
(4)   SPC/E LJ parameters from Berendsen's original 1987 paper
(5)   Coulomb interaction: Ewald sum
   Real space ewald: Minimum image convention
   Ewald convergence parameter for reciprocal sum = 5/L (L is the
box length in Ang)
   Fourier cut-off for ewald reciprocal sum |G| =2*pi*|n|/L, where |n| < 27
(6)   Nose-Hoover chain NVT (single chain, single thermostat per chain)
(7) Time step 1 fs, velocity verlet solver, RATTLE was used to
constrain bond lengths and angle, and correct velocities.
(8) 100 ps equlibration, 400 ps production (configuration was saved every 25 fs)


Everything is fine (energies are stable, etc.) except the second peak
in the O-O rdf.
The first peak is fine but my second peak seems flat. I find this
troubling since
all the rdfs I've seen in literature as well the experimental plot
have a well-defined
second peak. I must mention that in all the papers I've seen the
ensemble is NPT (I've not seen NVT yet). In any case, I was expecting my result
to match previously published results closely.

Can anyone point out what I am doing wrong?? Is NVT not a good ensemble
for water simulation?? I'll appreciate it if someone can refer me to a paper
that discusses this.
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[gmx-users] maximum cut-off in Minimum image convention

2010-05-26 Thread Francisco Garcia
Dear users,

I wish to ask a question regarding the maximum cut-off in the minimum
image convention (MIC).

According to my understanding, MIC ensures that the separation
between two particles i and j along each coordinate axes, namely,
xi- xj, yi-yj, and zi-zj, is in the interval (-0.5L, 0.5L), where L is the box
length (assumed the box to be cubic). This implies that
distance rij can vary between 0 and 0.5L*sqrt(3).
In order words the maximum separation should be less than half the diagonal:
 for example if i is located at (0,0,0) and j is located at the corner
(0.49L, 0.49L, 0.49L).

However, I read a couple of text books and online notes that claim
that if r > 0.5L, then MIC is violated.
Specifically, this means that 0.5L < rij < 0.5L*sqrt(3)  violates MIC.
I find this confusing. I have been grinding hard to understand this
point but I just
cannot figure it out.

In short my claim is that in MIC, rij can be at most half the diagonal
length whereas
the textbook says that rij can be at most half the box length.

If I am wrong, can someone explain the flaw in my argument?

Thanks!
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