Difference between revisions of "Duh Haymet"

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The  '''Duh-Haymet'''  (Ref. 1) (1995) Padé (3/2) approximation for the Bridge function for the [[Lennard-Jones model |Lennard-Jones]] system is (Eq. 13)
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The  '''Duh-Haymet'''  (Ref. 1) (1995) Padé (3/2) approximation for the [[bridge function]] for the [[Lennard-Jones model |Lennard-Jones]] system is (Eq. 13)
  
  

Latest revision as of 18:00, 26 June 2007

The Duh-Haymet (Ref. 1) (1995) Padé (3/2) approximation for the bridge function for the Lennard-Jones system is (Eq. 13)


B(\gamma^{*})= - \frac{1}{2} \gamma^{*2} \left[ \frac{1}{ \left[ 1+ \left( \frac{5\gamma^{*} +11}{7\gamma^{*} +9} \right) \gamma^{*}  \right]} \right]

where (Eq. 10)

\left. \gamma^{*}(r) \right.= \gamma (r)  - \beta \Phi_p(r)

where \Phi_p (r) is the perturbative (attractive) part of the pair potential.


References[edit]

  1. Der-Ming Duh and A. D. J. Haymet "Integral equation theory for uncharged liquids: The Lennard-Jones fluid and the bridge function", Journal of Chemical Physics 103 pp. 2625-2633 (1995)