We have calculated the free energy of solvation for hard sphere solutes, as
large as 20 A in diameter, in two simple-point-charge models of water. The
se results were obtained using umbrella sampling of ensembles with fixed, a
mbient temperature and pressure. For the same water models, we have also ca
lculated the surface tension of a liquid-vapor interface at room temperatur
e. Analogous calculations were carried out for three thermodynamic states o
f the Lennard-Jones (LJ) fluid near liquid-vapor coexistence. For both wate
r and the LJ fluid at the conditions we have simulated. extrapolation of ou
r results suggests that the planar interface between coexisting liquid and
vapor phases has the same surface tension as the planar limit of hard spher
e solvation. We expect this correspondence to be a general result for fluid
s at thermodynamic states close to phase coexistence, as measured by the di
fference in chemical potential between bulk liquid and vapor phases, and fa
r from the critical point. The solvation free energies we have computed for
water and the LJ fluid cross over at microscopic solute sizes from a depen
dence on solute volume to an approximate dependence on solute surface area,
as predicted by Lum et al.