A continuum model for ion evaporation from a drop: effect of curvature andcharge on ion solvation energy

A drop of liquid is treated as a continuum medium with surface tension gamm a and dielectric constant epsilon. The energy Delta (surface + electrostati c) required to extract a solvated ion from the drop can then be determined as part of a well posed problem as a function of the initial number z + 1 o f elementary charges in the drop and its initial radius R'. Instead of a di rect numerical attack on the full model, a geometrically simpler situation is analyzed, in which the drop and the solvated ion are taken to be either spheres or spherical caps after or prior to detachment, respectively. This simplified model is closely related to the full continuous problem when the radius R-i of the solvated ion is small (R-i/R' << 1), and the main drop i s not near the Rayleigh limit. This model problem is solved analytically in the limit epsilon << 1. When z = 0 and 1/R' = 0 one recovers Born's result , where Delta = 2.7 eV for monovalent ions in water, which exceeds by some 0.3 eV the experimental value for the alkali ions. In the limit of small io ns one recovers the results of Gamero et al. [5], Delta = Delta G(Born) - e (2)[F(z)+alpha]/(4 pi epsilon(0)R'), though surface tension effects shift t he constant cr from 4/5 to 2/3, The effect of finite ion diameter is determ ined numerically for the two-spheres model. When the solvation energy at ze ro curvature and charge is Delta G(born), small ions do not evaporate from water drops. When this value is reduced to fit available experimental data, a narrow ion evaporation window appears for drops charged near the Rayleig h limit with z similar to 12 or less. The domain in (z, R') space leading t o ion evaporation is broader for the case of formamide. The micro-hydrodyna mic process of escape of a singly charged nanodrop from a larger drop requi res a large activation energy. It is hence indistinguishable from Iribarne- Thomson ion evaporation, and radically different from a Coulomb explosion. (C)2000 Elsevier Science B.V. All rights reserved.