Second virial coefficient: Difference between revisions
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==Hard spheres== | ==Hard spheres== | ||
For hard | For the [[hard sphere model]] one has (McQuarrie, 1976, eq. 12-40) | ||
:<math>B_{2}(T)= - \frac{1}{2} \int_0^\sigma \left(\langle 0\rangle -1 \right) 4 \pi r^2 dr | :<math>B_{2}(T)= - \frac{1}{2} \int_0^\sigma \left(\langle 0\rangle -1 \right) 4 \pi r^2 dr | ||
</math> | </math> | ||
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:<math>B_{2}= \frac{2\pi\sigma^3}{3}</math> | :<math>B_{2}= \frac{2\pi\sigma^3}{3}</math> | ||
Note that <math>B_{2}</math> for the | Note that <math>B_{2}</math> for the hard sphere is independent of [[temperature]]. | ||
==See also== | ==See also== | ||
*[[Virial equation of state]] | *[[Virial equation of state]] |
Revision as of 12:43, 22 January 2008
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.
Isihara-Hadwiger formula
The Isihara-Hadwiger formula was discovered simultaneously and independently by Isihara and the Swiss mathematician Hadwiger in 1950. The second virial coefficient for any hard convex body is given by the exact relation
or
where
where is the volume, , the surface area, and the mean radius of curvature.
References
- A. Isihara "Determination of Molecular Shape by Osmotic Measurement", Journal of Chemical Physics 18 pp. 1446-1449 (1950)
- Akira Isihara and Tsuyoshi Hayashida "Theory of High Polymer Solutions. I. Second Virial Coefficient for Rigid Ovaloids Model", Journal of the Physical Society of Japan 6 pp. 40-45 (1951)
- Akira Isihara and Tsuyoshi Hayashida "Theory of High Polymer Solutions. II. Special Forms of Second Osmotic Coefficient", Journal of the Physical Society of Japan 6 pp. 46-50 (1951)
- H. Hadwiger "" Mh. Math. 54 pp. 345- (1950)
- H. Hadwiger "" Experimentia 7 pp. 395- (1951)
- H. Hadwiger "Altes und Neues über Konvexe Körper" Birkäuser Verlag (1955)
Hard spheres
For the hard sphere model one has (McQuarrie, 1976, eq. 12-40)
leading to
Note that for the hard sphere is independent of temperature.