Percus Yevick: Difference between revisions
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:<math>\left.c(r)\right.= \left( e^{-\beta \Phi } -1\right) e^{\omega}= g - \omega - (e^{\omega} -1 -\omega)</math> | :<math>\left.c(r)\right.= \left( e^{-\beta \Phi } -1\right) e^{\omega}= g - \omega - (e^{\omega} -1 -\omega)</math> | ||
or (Eq. 2 of | or (Eq. 2 of Ref. 5) | ||
:<math>\left.g(r)\right. = e^{-\beta \Phi} (1+ \gamma(r))</math> | :<math>\left.g(r)\right. = e^{-\beta \Phi} (1+ \gamma(r))</math> | ||
| Line 34: | Line 34: | ||
Note: the restriction | Note: the restriction <math>-1 < \gamma (r) \leq 1</math> arising from the logarithmic term Ref. 6. | ||
A critical look at the PY was undertaken by Zhou and Stell in Ref. 7. | |||
A critical look at the PY was undertaken by Zhou and Stell in | |||
==References== | ==References== | ||
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#[PR_1958_110_000001] | #[PR_1958_110_000001] | ||
#[MP_1983_49_1495] | #[MP_1983_49_1495] | ||
#[PRA_1984_30_000999] | |||
#[JCP_2002_116_08517] | |||
#[JSP_1988_52_1389_nolotengoSpringer] | |||
Revision as of 12:15, 23 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
- 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.h-c\right.=y-1}
The PY closure can be written as (Ref. 3 Eq. 61)
- 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.f [ \gamma (r) ]\right. = [e^{-\beta \Phi} -1][\gamma (r) +1]}
or
- 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.c(r)\right.= {\rm g}(r)(1-e^{\beta \Phi})}
or (Eq. 10 in Ref. 4)
- 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.c(r)\right.= \left( e^{-\beta \Phi } -1\right) e^{\omega}= g - \omega - (e^{\omega} -1 -\omega)}
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]