Percus Yevick: Difference between revisions
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#[JCP_2002_116_08517] | #[JCP_2002_116_08517] | ||
#[JSP_1988_52_1389_nolotengoSpringer] | #[JSP_1988_52_1389_nolotengoSpringer] | ||
[[Category: Integral equations]] | |||
Revision as of 12:19, 27 February 2007
If one defines a class of diagrams by the linear combination (Eq. 5.18 Ref.1) (See G. Stell in Ref. 2)
one has the exact integral equation
The Percus-Yevick integral equation sets D(r)=0. Percus-Yevick (PY) proposed in 1958 Ref. 3
The PY closure can be written as (Ref. 3 Eq. 61)
or
or (Eq. 10 in Ref. 4)
or (Eq. 2 of Ref. 5)
- 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.g(r)\right. = e^{-\beta \Phi} (1+ \gamma(r))}
or 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 \left.B(r)\right.= \ln (1+\gamma(r) ) - \gamma(r)}
Note: the restriction 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 -1 < \gamma (r) \leq 1}
arising from the logarithmic term Ref. 6.
A critical look at the PY was undertaken by Zhou and Stell in Ref. 7.
References
- [RPP_1965_28_0169]
- [P_1963_29_0517_nolotengoElsevier]
- [PR_1958_110_000001]
- [MP_1983_49_1495]
- [PRA_1984_30_000999]
- [JCP_2002_116_08517]
- [JSP_1988_52_1389_nolotengoSpringer]