Editing Martynov Sarkisov Vompe
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The | The Martynov-Sarkisov-Vompe (MSV) (1999) (Eq. 33 Ref. 1) closure is | ||
given in terms of the | given in terms of the bridge function | ||
:<math>B^{(2)}(r) = - \frac{1}{2} (\omega - \phi)^2</math> | :<math>B^{(2)}(r) = - \frac{1}{2} (\omega - \phi)^2</math> | ||
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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 [[ | where <math>\phi</math> 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). | (Notice that the Martynov-Sarkisov-Vompe closure, for a hard sphere fluid, becomes the [[Martynov Sarkisov]] closure). | ||
==References== | ==References== | ||
#[JCP_1999_110_03961] | |||
[ |