Duh Haymet: Difference between revisions
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Carl McBride (talk | contribs) m (New page: The '''Duh-Haymet''' (Ref. 1) (1995) Padé (3/2) approximation for the Bridge function for the Lennard Jones system is (Eq. 13) <math>B(\gamma^{*})= - \frac{1}{2} \gamma^{*2} \left...) |
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Revision as of 14:20, 23 February 2007
The Duh-Haymet (Ref. 1) (1995) Padé (3/2) approximation for the Bridge function for the Lennard Jones system is (Eq. 13)
where (Eq. 10) where is the perturbative part of the pair potential (Note: in the WCA separation for the Lennard Jones system, the `perturbative part' is the attractive part).
References
- [JCP_1995_103_02625]