Widom test-particle method: Difference between revisions

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The excess [[chemical potential]] is given by
[[Benjamin Widom]] proposed an elegant, general method to obtain
the excess [[chemical potential]] of a system that is being
simulated. A ''test particle'' is introduced in a random
location, and <math>\Delta\Phi</math>, the difference
in [[internal energy]] before and after the insertion,
is computed. (For pairwise interactions, this would
just be the interaction potential energy between the randomly
placed test particle and the ''N'' particles that the system is comprised of.)
The particle is not actually inserted (at variance with [[Monte Carlo in the grand-canonical ensemble|grand canonical MC ]]).


:<math>\mu^{ex} = -k_BT \ln \langle e^{-\Phi/k_bT}\rangle_N</math>
The excess chemical potential is given by


where <math>k_B</math> is the [[Boltzmann constant]], ''T'' is the [[temperature]], ''N'' is the number of particles within the system and <math>\Phi</math> is the interaction potential energy between the randomly placed test particle and the ''N'' particles that the system is comprised of.
:<math>\mu^{ex} = -k_BT \log \langle e^{-\Delta\Phi/k_bT}\rangle_N ,</math>
 
where <math>k_B</math> is the [[Boltzmann constant]] and ''T'' is the [[temperature]].
==References==
==References==
#[http://dx.doi.org/10.1063/1.1734110 B. Widom "Some Topics in the Theory of Fluids", Journal of Chemical Physics '''39''' pp. 2808-2812 (1963)]
#[http://dx.doi.org/10.1063/1.1734110 B. Widom "Some Topics in the Theory of Fluids", Journal of Chemical Physics '''39''' pp. 2808-2812 (1963)]

Revision as of 23:04, 29 January 2008

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Benjamin Widom proposed an elegant, general method to obtain the excess chemical potential of a system that is being simulated. A test particle is introduced in a random location, and , the difference in internal energy before and after the insertion, is computed. (For pairwise interactions, this would just be the interaction potential energy between the randomly placed test particle and the N particles that the system is comprised of.) The particle is not actually inserted (at variance with grand canonical MC ).

The excess chemical potential is given by

where is the Boltzmann constant and T is the temperature.

References

  1. B. Widom "Some Topics in the Theory of Fluids", Journal of Chemical Physics 39 pp. 2808-2812 (1963)
  2. B. Widom "Potential-distribution theory and the statistical mechanics of fluids", Journal of Physical Chemistry 86 pp. 869 - 872 (1982)
  3. David S. Corti "Alternative derivation of Widom's test particle insertion method using the small system grand canonical ensemble", Molecular Physics 93 pp. 417-420 (1998)