Molecular orbital calculations have been carried out of the basicities of substituted pyridines in the gas phase at the HF/6-31G*, MP2/6-31G*, and B3LYP/6-31G* levels and in solution based on the isodensity surface-polarized continuum model (IPCM). The correlated gas-phase MO basicities, especially at the MP2 level, agree well with the experimental gas-phase results. The IPCM model with MP2/6-31G* and B3LYP/6-31G* geometries also reproduces well the solvation free energy difference, Δ G ° s, between the pyridinium ion and neutral pyridine in water, although it leads to a somewhat greater negative slope for the p K a (aq) vs σ plot (ρ aq = −8.6 and −9.0 at the MP2/6-31G* and B3LYP/6-31G* levels, respectively, in contrast to the experimental slope of ρ aq = −5.8). The model predicts a linear correlation between the theoretical (IPCM) ρ values in solution and the Onsager dielectric function (ε − 1)/(2ε + 1). The estimate of ion solvation free energy for H + in acetonitrile ( G ° s = −250.4 kcal mol -1 ) indicates that there is a constant p K a difference of Δ pK a (=p K a (AN) − p K a (W)) = 7.7. This is due solely to the H + ion solvation free energy difference of 10.5 kcal mol -1 between acetonitrile and water with near unity (1.02) slope for the δp K a (AN) vs δp K a (W) plot. The π donor effect of strong para π acceptors ( p -CN, p -NO 2, etc.) on the p K a values of pyridinium ions was found in the gas phase as well as in solution.
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Lee et al. (1999) studied this question.
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