Limiting ionic conductance (Λ 0 ) of rigid symmetrical unipositive ions in aqueous solution shows a strong temperature dependence. For example, Λ 0 more than doubles when the temperature is increased from 283 to 318 K. A marked variation also occurs when the solvent is changed from ordinary water (H 2 O) to heavy water (D 2 O). In addition, Λ 0 shows a nonmonotonic size dependence with a skewed maximum near Cs + . Although these important results have been known for a long time, no satisfactory theoretical explanation exists for these results. In this article we present a simple molecular theory which provides a nearly quantitative explanation in terms of microscopic structure and dynamics of the solvent. A notable feature of this theory is that it does not invoke any nonquantifiable models involving solvent-berg or clatherates . We find the strong temperature dependence of Λ 0 to arise from a rather large number of microscopic factors, each providing a small but nontrivial contribution, but all acting surprisingly in the same direction. This work, we believe, provides, for the first time, a satisfactory explanation of both the anomalous size and temperature dependencies of Λ 0 of unipositive ions in molecular terms. The marked change in Λ 0 as the solvent is changed from H 2 O to D 2 O is found to arise partly from a change in the dielectric relaxation and partly from a change in the effective interaction of the ion with the solvent.
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Biswas et al. (1997) studied this question.
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