The mechanism of hydrophobic solvation depends on solute radius

We model the aqueous solvation of a nonpolar solute as a function of its radius. We use a simplified statistical mechanical model of water, the Mercedes Bent (MB) model, in NPT Monte Carlo simulations, This model has previously been shown to predict qualitatively the volume anomalies of pure water and the free energy, enthalpy, entropy, heat capacity, and volume change for inserting a nonpolar solute into water, We find a very different mechanism far the aqueous solvation of large nonpolar solutes (much larger than a water) than for smaller solutes. Small solute transfer involves a large hydrophobic heat capacity; its disaffinity for cold water (room temperature or below) is due to the ordering of the neighboring waters (entropic), while its disaffinity for hot wafer is due to the breaking of hydrogen bonds among the neighboring waters (enthalpic). In contrast, transferring large nonpolar solutes into water involves no Such large changes in heat capacity or entropy. In this regard, large nonpolar solutes are not "hydrophobic"; their solvation follows classical regular solution theory. Putting a large nonpolar surface into water breaks hydrogen bonds at all temperatures Therefore, the traditional "iceberg" model that first-shell water structure melts out with temperature should not apply to large solutes. These results also explain why the free energy of creating an oil/water interface (75 cal Angstrom (-2) mol(-1)) is greater than threefold for small molecule transfers (25 cal Angstrom (-2) mol(-1)). A key conclusion is that hydrophobicity depends not only on the surface area of a solute but also on its shape and curvature.