Martynov Sarkisov Vompe: Difference between revisions
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Carl McBride (talk | contribs) m (New page: The Martynov-Sarkisov-Vompe (MSV) (1999) (Eq. 33 Ref. 1) closure is given in terms of the bridge function :<math>B^{(2)}(r) = - \frac{1}{2} (\omega - \phi)^2</math> where :<math>\left....) |
Carl McBride (talk | contribs) mNo edit summary |
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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 | where <math>\phi</math> is short-ranged. The [[WCA division]] of the [[Lennard-Jones]] potential was used. | ||
(Notice that the | (Notice that the Martynov-Sarkisov-Vompe closure, for a hard sphere fluid, becomes the [[Martynov Sarkisov]] closure). | ||
==References== | ==References== | ||
#[JCP_1999_110_03961] | #[JCP_1999_110_03961] | ||
Revision as of 12:48, 23 February 2007
The Martynov-Sarkisov-Vompe (MSV) (1999) (Eq. 33 Ref. 1) closure is given in terms of the bridge function
where
where 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).
References
- [JCP_1999_110_03961]