Second virial coefficient

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The second virial coefficient is usually written as B or as B2. The second virial coefficient represents the initial departure from ideal-gas behavior. The second virial coefficient, in three dimensions, is given by

B2(T)=−12∫(⟨exp(−Φ12(r)kBT)⟩−1)4πr2dr

where Φ12(r) is the intermolecular pair potential, T is the temperature and kB 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

B2=RS+V

or

B2V=1+3α

where

α=RS3V

where V is the volume, S, the surface area, and R the mean radius of curvature.

References

  1. A. Isihara "Determination of Molecular Shape by Osmotic Measurement", Journal of Chemical Physics 18 pp. 1446-1449 (1950)
  2. 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)
  3. 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)
  4. H. Hadwiger "" Mh. Math. 54 pp. 345- (1950)
  5. H. Hadwiger "" Experimentia 7 pp. 395- (1951)
  6. 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)

B2(T)=−12∫0σ(⟨0⟩−1)4πr2dr

leading to

B2=2πσ33

Note that B2 for the hard sphere is independent of temperature.

See also

References