Mean spherical approximation: Difference between revisions
Carl McBride (talk | contribs) mNo edit summary |
Carl McBride (talk | contribs) mNo edit summary |
||
| Line 12: | Line 12: | ||
where <math>h_{ij}(r)</math> and <math>c_{ij}(r)</math> are the total and the direct correlation functions for two spherical | where <math>h_{ij}(r)</math> and <math>c_{ij}(r)</math> are the total and the direct correlation functions for two spherical | ||
molecules of ''i'' and ''j'' species, <math>\sigma_i</math> is the diameter of '''i'' species of molecule. | molecules of ''i'' and ''j'' species, <math>\sigma_i</math> is the diameter of '''i'' species of molecule. | ||
Duh and Haymet (Eq. 9 | Duh and Haymet (Eq. 9 Ref. 4) write the MSA approximation as | ||
:<math>g(r) = \frac{c(r) + \beta \Phi_2(r)}{1-e^{\beta \Phi_1(r)}}</math> | :<math>g(r) = \frac{c(r) + \beta \Phi_2(r)}{1-e^{\beta \Phi_1(r)}}</math> | ||
where | where <math>\Phi_1</math> and <math>\Phi_2</math> comes from the [[WCA division]] of the [[Lennard-Jones]] potential. | ||
By introducing the definition (Eq. 10 \cite{JCP_1995_103_02625}) | By introducing the definition (Eq. 10 \cite{JCP_1995_103_02625}) | ||
| Line 32: | Line 32: | ||
#[JSP_1978_19_0317_nolotengoSpringer] | #[JSP_1978_19_0317_nolotengoSpringer] | ||
#[JSP_1980_22_0661_nolotengoSpringer] | #[JSP_1980_22_0661_nolotengoSpringer] | ||
#[JCP_1995_103_02625] | |||
Revision as of 13:12, 23 February 2007
The Lebowitz and Percus mean spherical approximation (MSA) (1966) (Ref. 1) closure is given by
The Blum and Hoye mean spherical approximation (MSA) (1978-1980) (Refs 2 and 3) closure is given by
and
where and are the total and the direct correlation functions for two spherical molecules of i and j species, is the diameter of 'i species of molecule. Duh and Haymet (Eq. 9 Ref. 4) write the MSA approximation as
where 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 \Phi_1} and 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 \Phi_2} comes from the WCA division of the Lennard-Jones potential. By introducing the definition (Eq. 10 \cite{JCP_1995_103_02625})
- 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 s(r) = h(r) -c(r) -\beta \Phi_2 (r)}
one can arrive at (Eq. 11 \cite{JCP_1995_103_02625})
- 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 B(r) \approx B^{\rm MSA}(s) = \ln (1+s)-s}
The Percus Yevick approximation may be recovered from the above equation by setting 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 \Phi_2=0} .
References
- [PR_1966_144_000251]
- [JSP_1978_19_0317_nolotengoSpringer]
- [JSP_1980_22_0661_nolotengoSpringer]
- [JCP_1995_103_02625]