The relative strengths of the driving mechanisms of this process may be determined using a triangular Teas graph. A parameter characterizing this process may be calculated via the Wodak-Janin approximation or the Shrake-Rupley algorithm. Empirical models of this process include the Abraham and Eisenberg-McLachlan equations. The influence of this process on the kinetic isotope effect is quantified by the Kresge-Gross-Butler equation. EEF1 and COSMO are implicit models of this process, which occurs at a rate dependent on the (*) accessible surface area. This process' Gibbs free energy is proportional to "one over vacuum permittivity minus one over relative permittivity" in the generalized Born model, which does not take into account the effect of polar molecules forming this process' namesake "shells" around central ions. For 10 points, nam
The relative strengths of the driving mechanisms of this process may be determined using a triangular Teas graph. A parameter characterizing this process may be calculated via the Wodak-Janin approximation or the Shrake-Rupley algorithm. Empirical models of this process include the Abraham and Eisenberg-McLachlan equations. The influence of this process on the kinetic isotope effect is quantified by the Kresge-Gross-Butler equation. EEF1 and COSMO are implicit models of this process, which occurs at a rate dependent on the (*) accessible surface area. This process' Gibbs free energy is proportional to "one over vacuum permittivity minus one over relative permittivity" in the generalized Born model, which does not take into account the effect of polar molecules forming this process' namesake "shells" around central ions. For 10 points, name this process that occurs at a lower rate than precipitation above the saturation concentration of the solute.
The relative strengths of the driving mechanisms of this process may be determined using a triangular Teas graph.
solvation [or  dissolution]