Abstract
In this paper we apply the theory of Steele to the problem of determining the pairwise interactions between oppositely charged nonspherical ions imbedded in a vacuum. The diatomic model of Sweet and Steele was extended by superimposing at either end of each linear, symmetric rod a Coulombic center characterized by a r−1 distance dependence. With respect to the consequent charge—charge interactions, a value of the Onsager coupling parameter was chosen which allowed a more detailed study of the relative importance of Lennard-Jones versus Coulombic forces; in effect, the ions were assumed to be only partially charged. Coefficients in the expansion of the potential energy function were calculated numerically, and changes in the profiles of the resulting curves [Ul,l′,m(r) as a function of interionic distance] were noted for different values of R/σ (where R is the length of the rod and σ is the usual Lennard-Jones range parameter). The trends observed were compared with those found by Sweet and Steele in their study of the diatomic model.
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