Martynov Sarkisov Vompe: Difference between revisions
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:<math>\left.\phi\right. = \rho \epsilon \beta</math> | :<math>\left.\phi\right. = \rho \epsilon \beta</math> | ||
where <math>\phi</math> is short-ranged. The [[WCA division]] of the [[Lennard-Jones]] potential was used. | where <math>\phi</math> is short-ranged. The [[WCA division]] of the [[Lennard-Jones model |Lennard-Jones]] potential was used. | ||
(Notice that the Martynov-Sarkisov-Vompe closure, for a hard sphere fluid, becomes the [[Martynov Sarkisov]] closure). | (Notice that the Martynov-Sarkisov-Vompe closure, for a hard sphere fluid, becomes the [[Martynov Sarkisov]] closure). | ||
Revision as of 18:27, 20 March 2007
The Martynov-Sarkisov-Vompe (MSV) (1999) (Eq. 33 Ref. 1) closure is given in terms of the bridge function
- 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 B^{(2)}(r) = - \frac{1}{2} (\omega - \phi)^2}
where
- 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 \left.\phi\right. = \rho \epsilon \beta}
where 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} is short-ranged. The WCA division of the Lennard-Jones potential was used. (Notice that the Martynov-Sarkisov-Vompe closure, for a hard sphere fluid, becomes the Martynov Sarkisov closure).