2014-01-28 Jakub Krajniak <[email protected]>:
> On Monday, 27 January 2014 04:47:22 UTC+1, Christoph Junghans wrote:
>>
>> (...)
>>
>> >> The theory behind Boltzmann inversion assumes a Boltzmann distribution
>> >> (NVT).
>> >> Which thermostat are you using? For Espresso++ Langevin thermostat
>> >> should to the same as stochastic dynamics.
>> >
>> >
>> > Actually I have moved to Gromacs to not complicate too much. When I look
>> > on
>> > the
>> > temperature, it is kept correctly during the simulation (with sd
>> > integrator).
>> >
>> > The strange thing is with rdfs. In the attachment there is a tgt and
>> > .new
>> > A-A.dist
>> > from step_001. The shapes seem similar but the y-values are different.
>> > In
>> > the next
>> > steps the rdfs look totally different (and the .conv value rise
>> > enormous).
>> 1.) Your target distribution is really noisy, which will lead to a
>> very noisy initial potential, maybe a bigger spacing would help.
>> 2.) It seems the first update makes the A-A potential too attractive,
>> hence you get the really high peak at x=0.42, maybe you will need to
>> scale the update with a factor like 0.1 (postupd scale).
>
>
> I am very appreciate for your help. The scale factor helped to remove this
> huge difference.  I am wondering why I encountered that. Is it possible that
> it is because of bond interaction? I have defined the exclusion list for
> .top so
> this should be handled and the behavior does not changed.
This is very system-dependent, in most cases this means your initial
potential isn't good enough.

>
> Best regards,
> Jakub Krajniak
>
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-- 
Christoph Junghans
Web: http://www.compphys.de

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