Widom test-particle method: Difference between revisions
		
		
		
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Carl McBride (talk | contribs)  (New page: The excess chemical potential is given by  :<math>\mu^{ex} = -k_BT \ln \langle e^{-\Phi/k_bT}\rangle_N</math>  where <math>k_B</math> is the Boltzmann constant, ''T'' is the [[temp...)  | 
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#[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)]  | ||
#[http://dx.doi.org/10.1021/j100395a005  B. Widom "Potential-distribution theory and the statistical mechanics of fluids", Journal of Physical Chemistry '''86''' pp.  869 - 872 (1982)]  | #[http://dx.doi.org/10.1021/j100395a005  B. Widom "Potential-distribution theory and the statistical mechanics of fluids", Journal of Physical Chemistry '''86''' pp.  869 - 872 (1982)]  | ||
#[http://dx.doi.org/10.1080/002689798169104 David S.   | #[http://dx.doi.org/10.1080/002689798169104 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)]  | ||
[[category: computer simulation techniques]]  | [[category: computer simulation techniques]]  | ||
Revision as of 18:01, 22 September 2007
The excess chemical potential is given by
where is the Boltzmann constant, T is the temperature, N is the number of particles within the system and is the intermolecular pair potential.
References
- B. Widom "Some Topics in the Theory of Fluids", Journal of Chemical Physics 39 pp. 2808-2812 (1963)
 - B. Widom "Potential-distribution theory and the statistical mechanics of fluids", Journal of Physical Chemistry 86 pp. 869 - 872 (1982)
 - 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)