[gmx-users] Question about the Marrink's CG model

2009-09-09 Thread Li Yang
Dear GMXers:

I'm sorry to disturb you.

I have a question about the Marrink's coarse-grained model, Marrink, et al. 
Coarse Grained Model for Semiquantitative Lipid Simulations. J. Phys. Chem. B 
2004, 108, 750-760.

In the Marrink's CG model, the electrostatic Coulombic potential is computed 
via cutoff scheme. In the original paper, the cutoff method is employed with 
relative dielectric constant \epsilon=20 for explicit screening. Does it mean 
the parameter of force field is only customized for the cutoff method? As known 
that the Ewald method is better than the cutoff scheme for the long-range 
electrostatic interaction. I want to know whether the Ewald method is also OK 
for this model? How can I test it? I have simulated a similar system via two 
method respectively, which includes a big charged nano-scale particle (~6nm). 
But I find that the results of cutoff scheme are quite different from the PME's 
results. I don't know which one is right.


Another question is how to get the relative dielectric constant for a CG model. 
I'm not familiar with this topic, but I think it is the key of the above 
question perhaps. Yet, there are not some details in the original paper. In 
some other paper about different CG models, I don't find some information about 
this topic. Could someone please give me some refs about the computational 
details?


Thank you very much.

Li Yang


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[gmx-users] how to compute bending modulus of the membrane with NPs

2009-02-24 Thread Li Yang
Dear all

I'm trying to measure the bending modulus (Kc) of lipid bilayer. I've
found some papers, showing that spectral intensity needs to be
calculated using the wave vector q. This method has been applied
directly for pure membrane, or for bilayers with cholesterol.

In my simulations, there is a colloid particle immerses into the inner
or adsorbs on the surface of the lipid bilayer. I want to compute how
the interaction of particles to affect the bending modulus of the
membrane. But I'm not sure whether this method can be applied directly
in above cases? If not, how can I get it? What about the spontaneous
curvature?

Thank you very much. Any suggestion or reference will be appreciated!

Li Yang



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RE: RE: [gmx-users] how to set pull code in gmx 4

2008-10-20 Thread Li Yang


Hi Berk

Thanks for your reply


If you use pull_geometry=distance you need to set the reference distance,
which would be (assuming you want 1 nm):
pull_init1 = 1
  

Sorry for my poor expression.

Take a example, In gmx 3.3, the pull dimension and position can be 
writen as:

pull_type = umbrella ; umbrella sampling
pull_dim = N N Y ; pulling performed in Z dimension
pos1 = 0 0 1 ; the reference distance in Z dimension is 1nm

In gmx 4, for pull_init1 = 1, which dimension of the reference 
distance does it mean ?
Or say, there is still a single pulling performed in one dimension, like 
gmx 3.3, and when setting pull_dim = N N Y, the pull init1=1 means 
the reference distance in Z dimension is 1nm; while pull_dim=Y N N 
means the reference distance in X dimension is 1nm?


Maybe my thinking sounds stupid, I don't know.
Waiting for your reply.

Li Yang


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[gmx-users] how to set pull code in gmx 4

2008-10-18 Thread Li Yang
Dear all

I cannot understand the explanations about settings of pull code in the
gmx 4.

Take a example, there are two particles in the system, and I want to
reproduce the LJ potential using umbrella sampling.
The settings in gmx 3.3.3 is following:
=
..
runtype = umbrella
ngroups = 1
group_1 = Arg2
reference_group = Arg1
..
pulldim = N N Y
K1 = 700
POS1 = 0 0 1
==

But I don't know how to set it in gmx 4
Following is the settings in gmx 4:
==
; COM PULLING
; Pull type: no, umbrella, constraint or constant_force
pull = umbrella ; --- runtype in gmx 3.3.3
; Pull geometry: distance, direction, cylinder or position
pull_geometry = distance
; Select components for the pull vector. default: Y Y Y
pull_dim = N N Y ; --- pulldim in gmx 3.3.3
; Cylinder radius for dynamic reaction force groups (nm)
pull_r1 = 1
; Switch from r1 to r0 in case of dynamic reaction force
pull_r0 = 1.5
pull_constr_tol = 1e-06
pull_start = no
pull_nstxout = 10
pull_nstfout = 1
; Number of pull groups
pull_ngroups = 1 ; --- ngroups in gmx 3.3.3
; Group name, weight (default all 1), vector, init, rate (nm/ps),
kJ/(mol*nm^2)
pull_group0 = Arg2 ; --- reference_group in gmx 3.3.3
pull_weights0 =
pull_pbcatom0 = 0
pull_group1 = Arg1 ; --- group1 in gmx 3.3.3
pull_weights1 =
pull_pbcatom1 = 0
pull_vec1 = 0.0 0.0 0.0
pull_init1 = 0.0
pull_rate1 = 0
pull_k1 = 700 ; --- k1 in gmx 3.3.3
pull_kB1 = 0
==
if right, which parameter corresponds with pos1 in gmx3.3.3?

I must apologize in advance if I miss some details in the manual.

Thank you very much

Li Yang

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[gmx-users] Re: gmx-users Digest, Vol 53, Issue 90

2008-09-21 Thread Li Yang
Hi Ran

Thank you for your reply. I'm sorry that I miss the message.

(1) 6 eigenvalues represent rotation and translation. For (very) small
molecules, these can be quite substantial, see Carlsson and Aqvist, /J.
Phys. Chem. B,/ *109* (13), 6448 -6456, 2005. By fitting you remove the
rotation and translation. You can search the literature for papers that
discuss the QH approximation as well. The motions are not really
harmonic - this is why it's an approximation.

I've received very similar results to Carlsson and Aqvist for benzene
and palmatic acid with GMX.

(2) The values you get depend on the sampling and the conversion of the
simulations. To improve sampling, you have to store the coordinates
frequently enough (so you get more samples). In addition, the simulation
should be long enough to give you meaningful results - and both depend
on the system which you study. Checking for convergence can be done by
repeating the calculations on different time windows, as you suggested.
Sorry, I don't quite catch your mind. How to get the convergence variation of 
the entropy? Whether or not the time split method is right? eg, time points: 
0, 1, 2, 3, 4, 5.  and time stage:0-1, 0-2, 0-3, 0-4, 0-5, right?  why not 0-1, 
1-2, 2-3, 3-4, 4-5. In the maillist of gmx, the latter is not wrong because of 
undersampling, I don't know this meaning. Could you please offer me some 
suggestions or refs?

The method of covariance matrix  QH can estimate the up-limit of entropy, how 
to know the error band ?

Thank you very much.

 (3) In entropy calculations, a system need to run a long time for entropy 
 convergence, the time seems to be longer than the one which needed for 
 energy convergence. While, for equilibrium thermodynamics simulations, how 
 to justify whether or not the system has achieving a equilibrium stage, 
 based on energy convergence or entropy confvergence?

 (4) For the example mentioned in the paper Ioan 
 Andricioaei_JChemPhys2001_115_6289. I use your perl script for entropy 
 calculation. But I don't reproduce the result. The needed time of entropy 
 convergence is longer than the time mentioned in the paper, and so larger of 
 my entropy. 
 I don't know why, perphas the simulation conditions is not right. My 
 simulation files are included in the attachment. Could you give some 
 suggestions? 
 BTW, in line 77 of your script: $w=$ev*$u*10**(-18), Does 10^-18 mean 
 nm^-2?
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[gmx-users] how to measure the surface tension of membrane by inclusion

2008-07-17 Thread Li Yang
Hi

I have some questions about the surface tension calculations:

1. For the formula, \gamma_m=(P_N - P_L) * L_z / 2, is it only 
available for a flat surface, like a lipid bilayer in water ?  For example, the 
surface fluctuation of lipid bilayer often occur in the simulation, sometimes, 
the surface is not flat but bending, in such a case, is the formula still 
available? What about the vesicle?

2. In my system, there are a bilayer patch and a NP of ~10nm, they are 
all in water. At the beginning (state 1), NP and the bilayer don't contact each 
other. After some nanoseconds runtime, NP adsorbs on the surface of the bilayer 
(state 2). Finally(state 3), the NP embeds into the inner of the lipid bilayer. 

In this case, how can I measure the changing surface tension during the 
simulation?  Is the formula above available for my system?
In state 1, is that meaning there are four interface in the system? What about 
the case (state 2,3) that the NP contacting the bilayer ?

I hope I've describe my questions clearly. Any suggestion or recommended 
reference will be appreciated.

Thank you very much.

Sincerely


Li Yang
[EMAIL PROTECTED]
  2008-07-17
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