[gmx-users] OPLS parametrizaton
Justin A. Lemkul
jalemkul at vt.edu
Tue Apr 5 21:18:51 CEST 2011
Marcelo Silva wrote:
> Em 02-04-2011 0:33, Justin A. Lemkul escreveu:
>>
>>
>> Marcelo Silva wrote:
>>> Hi,
>>>
>>> I am trying to simulate mixtures of ethanol and trifluoroethanol and
>>> I would like to use the same parameters used on OPLS parametrization.
>>>
>>> On the OPLS1996 paper the authors starts by stating that they've used
>>> 267 molecules and "The box size varied from approximately 26 26 26
>>> Å for methanol to 37 37 37 Å for cyclohexane". In my simulations
>>> I am considering using 500 molecules (each box vector would be around
>>> 37 Å).
>>>
>>> "In most cases, the intermolecular nonbonded interactions were
>>> truncated at 11Å based on roughly the center-of-mass separations with
>>> quadratic smoothing of the interaction energy to zero over the last
>>> 0.5 Å (...) A standard correction was made for the Lennard-Jones
>>> interactions neglected beyond the cutoff."
>>>
>>> Trying to interpret what is written I think the correct way to treat
>>> cut-offs and energy corrections would be like this:
>>>
>>> ---------------------------------------
>>> Cut-offs
>>>
>>> rlist = 1.4
>>> coulombtype = Reaction-field-zero
>>> rcoulomb = 1.1
>>> rcuolomb_shift = 0.6
>>> vdwtype = shift
>>> rvdw = 1.1
>>> rvdw_switch = 0.6
>>>
>>> Dispersion Correction
>>>
>>> DispCorr = EnerPress
>>>
>>> ---------------------------------------
>>>
>>> However I have some doubts because I'm using a box with a different
>>> number of molecules/ different size (should I change the cutoffs to
>>> 15Å like it was for cyclohexane?) and I'm not sure about using
>>> Reaction-field-zero instead of the shift function for coulombic
>>> interactions.
>>>
>>> Could you please help me confirm this parameters so I can run a
>>> simulation in the same conditions as OPLS was parameterized (although
>>> using MC and not MD).
>>>
>>
>> I don't think there is a perfectly clear answer to this. OPLS was
>> initially designed for MC with some special functional forms and is
>> now applied to MD using all manner of settings. Commonly, one sees
>> rcoulomb=rvdw=rlist=1.0 or 1.4 in conjunction with PME. There have
>> been a variety of systematic force field comparisons in recent years.
>> You should consult those to see what their specific recommendations
>> are with respect to proper settings, although many of them focus on
>> proteins.
>>
>> -Justin
>>
>>> Best regards,
>>>
>>> Marcelo
>>
>
> Just to test it, I used this options (nstlist = 5 with timestep 1fs):
>
> ; Cut-offs
>
> rlist = 1.4
> coulombtype = Switch
> rcoulomb = 1.1
> rcuolomb_shift = 1.05
> vdwtype = Switch
> rvdw = 1.1
> rvdw_switch = 1.05
>
> ; Dispersion Correction
>
> DispCorr = EnerPres
>
> and compared to vdw plain cutoff at 1.1 and PME with cutoff 1.1 nm
> (rlist = 1.1 nm also). The big difference in the output seems to be with
> the Coulomb (SR) term:
>
> -1.25490e+05 kj/mol with Switch
> -5.38895e+03 kj/mol with PME
>
> With switch I get a low density for ethanol (about 0.3 g/ml). What could
> be the problem with the simulation using switch? By the way does gromacs
> use a different switch function depending on the forcefield?
>
The manual warns of artifacts that arise from switching functions. So there is
not a "problem" with switch, per se, rather an intrinsic limitation in accuracy.
I would imagine the low density arises from completely neglecting (via
truncation) any long-range electrostatics terms that PME (and to some extent,
other long-range methods) otherwise includes.
The switch function is not force field-dependent.
-Justin
> Best regards,
>
> Marcelo
>
--
========================================
Justin A. Lemkul
Ph.D. Candidate
ICTAS Doctoral Scholar
MILES-IGERT Trainee
Department of Biochemistry
Virginia Tech
Blacksburg, VA
jalemkul[at]vt.edu | (540) 231-9080
http://www.bevanlab.biochem.vt.edu/Pages/Personal/justin
========================================
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