Second virial coefficient: Difference between revisions
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==See also== | ==See also== | ||
*[[Virial equation of state]] | *[[Virial equation of state]] | ||
*[[Osmotic virial coefficients]] | |||
*[[Boyle temperature]] | *[[Boyle temperature]] | ||
*[[Joule-Thomson effect#Joule-Thomson coefficient | Joule-Thomson coefficient]] | *[[Joule-Thomson effect#Joule-Thomson coefficient | Joule-Thomson coefficient]] | ||
==References== | ==References== | ||
[[Category: Virial coefficients]] | [[Category: Virial coefficients]] | ||
Revision as of 13:57, 13 August 2007
The second virial coefficient is usually written as B or as . The second virial coefficient represents the initial departure from ideal-gas behavior. The second virial coefficient, in three dimensions, is given by
where is the intermolecular pair potential, T is the temperature and is the Boltzmann constant. Notice that the expression within the parenthesis of the integral is the Mayer f-function.
For any hard convex body
The second virial coefficient for any hard convex body is given by the exact relation
where
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 V} is the volume, 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} , the surface area, 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 R} the mean radius of curvature.
Hard spheres
For hard spheres one has (McQuarrie, 1976, eq. 12-40)
- 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_{2}(T)= - \frac{1}{2} \int_0^\sigma \left(\langle 0\rangle -1 \right) 4 \pi r^2 dr }
leading to
- 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_{2}= \frac{2\pi\sigma^3}{3}}
Note that 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_{2}} for the hard sphere is independent of temperature.