Intermolecular pair potential

From SklogWiki

Jump to: navigation, search

[edit] Axially symmetric molecules

In general, the intermolecular pair potential for axially symmetric molecules, Φ12, is a function of five coordinates:

\left. \Phi_{12} \right. = \Phi_{12}(r, \theta_1, \phi_1, \theta_2, \phi_2)

The angles θi and φi can be considered to be polar angles, with the intermolecular vector, r, as the common polar axis. Since the molecules are axially symmetric, the angles ψi do not influence the value of Φ12. A very powerful expansion of this pair potential is due to Pople (Ref. 1 Eq. 2.1):

\left. \Phi_{12} \right. = 4\pi \sum_{L_1 L_2 m} L_1 L_2 m (r) Y_{L_1}^m (\theta_1, \phi_1) Y_{L_2}^m * (\theta_2, \phi_2),

where Y_L^m(\theta, \phi) are the spherical harmonics.

[edit] See also

[edit] References

  1. J. A. Pople "The Statistical Mechanics of Assemblies of Axially Symmetric Molecules. I. General Theory", Proceedings of the Royal Society of London. Series A, Mathematical and Physical Sciences 221 pp. 498-507 (1954)
Personal tools