Radial distribution function: Difference between revisions
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==Density Expansion of the radial distribution function== | ==Density Expansion of the radial distribution function== | ||
The radial distribution function of a compressed gas may be expanded in powers of the density (Ref. 2) | The '''radial distribution function''' of a compressed gas may be expanded in powers of the density (Ref. 2) | ||
:<math>\left. {\rm g}(r) \right. = e^{-\beta \Phi(r)} (1 + \rho {\rm g}_1 (r) + \rho^2 {\rm g}_2 (r) + ...)</math> | :<math>\left. {\rm g}(r) \right. = e^{-\beta \Phi(r)} (1 + \rho {\rm g}_1 (r) + \rho^2 {\rm g}_2 (r) + ...)</math> | ||
where <math>\rho</math> is the number of molecules per unit volume. The | where <math>\rho</math> is the number of molecules per unit volume and <math>\Phi(r)</math> | ||
is the [[intermolecular pair potential]]. The | |||
function <math>{\rm g}(r)</math> is normalized to the value 1 for large distances. | function <math>{\rm g}(r)</math> is normalized to the value 1 for large distances. | ||
As is known, <math>{\rm g}_1 (r)</math>, <math>{\rm g}_2 (r)</math>, ... can be expressed by | As is known, <math>{\rm g}_1 (r)</math>, <math>{\rm g}_2 (r)</math>, ... can be expressed by | ||
[[cluster integrals]] in which the position of of two particles is kept fixed. | [[Cluster diagrams | cluster integrals]] in which the position of of two particles is kept fixed. | ||
In classical mechanics, and on the assumption of additivity of intermolecular forces, one has | In classical mechanics, and on the assumption of additivity of intermolecular forces, one has | ||
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is the [[Mayer f-function]] | is the [[Mayer f-function]] | ||
:<math>\left. f(r) \right. = e^{-\beta | :<math>\left. f(r) \right. = e^{-\beta \Phi(r)} -1</math> | ||
and | and | ||
Revision as of 14:44, 25 June 2007
Density Expansion of the radial distribution function
The radial distribution function of a compressed gas may be expanded in powers of the density (Ref. 2)
where is the number of molecules per unit volume and is the intermolecular pair potential. The function is normalized to the value 1 for large distances. As is known, , 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 {\rm g}_2 (r)} , ... can be expressed by cluster integrals in which the position of of two particles is kept fixed. In classical mechanics, and on the assumption of additivity of intermolecular forces, one has
- 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 {\rm g}_1 (r_{12})= \int f (r_{13}) f(r_{23}) ~{\rm d}r_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 {\rm g}_2 (r_{12})= \frac{1}{2}({\rm g}_1 (r_{12}))^2 + \varphi (r_{12}) + 2\psi (r_{12}) + \frac{1}{2} \chi (r_{12})}
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 r_{ik}} is the distance 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 |r_i -r_k|} , 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 f(r)} is the Mayer f-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. f(r) \right. = e^{-\beta \Phi(r)} -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 \varphi (r_{12}) = \int f (r_{13}) f (r_{24}) f (r_{34}) ~ {\rm d}r_3 {\rm d}r_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 \psi (r_{12}) = \int f (r_{13}) f (r_{23}) f (r_{24}) f (r_{34}) ~ {\rm d}r_3 {\rm d}r_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 \chi (r_{12}) = \int f (r_{13}) f (r_{23}) f (r_{14}) f (r_{24}) f (r_{34}) ~ {\rm d}r_3 {\rm d}r_4}
References
- John G. Kirkwood and Elizabeth Monroe Boggs "The Radial Distribution Function in Liquids", Journal of Chemical Physics 10 pp. 394-402 (1942)
- B. R. A. Nijboer and L. Van Hove "Radial Distribution Function of a Gas of Hard Spheres and the Superposition Approximation", Physical Review 85 pp. 777 - 783 (1952)