Weeks-Chandler-Andersen perturbation theory: Difference between revisions
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The '''Weeks-Chandler- | The '''Weeks-Chandler-Andersen perturbation theory''' <ref>[http://dx.doi.org/10.1063/1.1674820 John D. Weeks, David Chandler and Hans C. Andersen "Role of Repulsive Forces in Determining the Equilibrium Structure of Simple Liquids", Journal of Chemical Physics '''54''' pp. 5237-5247 (1971)]</ref> is based on the following | ||
decomposition of the [[intermolecular pair potential]] (in particular, the [[Lennard-Jones model | Lennard-Jones potential]] ): | decomposition of the [[intermolecular pair potential]] (in particular, the [[Lennard-Jones model | Lennard-Jones potential]]): | ||
The reference system pair potential is given by (Eq, 4 | The reference system pair potential is given by (Eq, 4): | ||
:<math> | :<math> | ||
| Line 22: | Line 22: | ||
</math> | </math> | ||
==Ben-Amotz-Stell reformulation== | ==Ben-Amotz-Stell reformulation== | ||
<ref>[http://dx.doi.org/10.1021/jp037810s Dor Ben-Amotz and George Stell "Reformulation of Weeks-Chandler-Andersen Perturbation Theory Directly in Terms of a Hard-Sphere Reference System", Journal of Physical Chemistry B '''108''' pp. 6877-6882 (2004)]</ref> | |||
==See also== | |||
*[[Weeks-Chandler-Andersen reference system model]] | |||
==References== | ==References== | ||
<references/> | |||
[[category: perturbation theory]] | [[category: perturbation theory]] | ||
Latest revision as of 17:10, 13 December 2017
The Weeks-Chandler-Andersen perturbation theory [1] is based on the following decomposition of the intermolecular pair potential (in particular, the Lennard-Jones potential):
The reference system pair potential is given by (Eq, 4):
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \Phi_{\rm repulsive} (r) = \left\{ \begin{array}{ll} \Phi_{\rm LJ}(r) + \epsilon & {\rm if} \; r < 2^{1/6}\sigma \\ 0 & {\rm if} \; r \ge 2^{1/6}\sigma \end{array} \right. }
and the perturbation potential is given by (Eq, 5 Ref. 1):
- Failed to parse (SVG (MathML can be enabled via browser plugin): Invalid response ("Math extension cannot connect to Restbase.") from server "https://wikimedia.org/api/rest_v1/":): {\displaystyle \Phi_{\rm attractive} (r) = \left\{ \begin{array}{ll} -\epsilon & {\rm if} \; r < 2^{1/6}\sigma \\ \Phi_{\rm LJ}(r) & {\rm if} \; r \ge 2^{1/6}\sigma \end{array} \right. }
Ben-Amotz-Stell reformulation[edit]
See also[edit]
References[edit]
- ↑ John D. Weeks, David Chandler and Hans C. Andersen "Role of Repulsive Forces in Determining the Equilibrium Structure of Simple Liquids", Journal of Chemical Physics 54 pp. 5237-5247 (1971)
- ↑ Dor Ben-Amotz and George Stell "Reformulation of Weeks-Chandler-Andersen Perturbation Theory Directly in Terms of a Hard-Sphere Reference System", Journal of Physical Chemistry B 108 pp. 6877-6882 (2004)