  We present an overview of the recent progress that has been made in
understanding the origin of hydrophobic interactions. We discuss the different
character of the solvation behavior of apolar solutes at small and large length
scales. We emphasize that the crossover in the solvation behavior arises from a
collective effect, which means that implicit solvent models should be used with
care. We then discuss a recently developed explicit solvent model, in which the
solvent is not described at the atomic level, but rather at the level of a
density field. The model is based upon a lattice-gas model, which describes
density fluctuations in the solvent at large length scales, and a Gaussian
model, which describes density fluctuations at smaller length scales. By
integrating out the small length scale field, a Hamiltonian is obtained, which
is a function of the binary, large-length scale field only. This makes it
possible to simulate much larger systems than hitherto possible as demonstrated
by the application of the model to the collapse of an ideal hydrophobic
polymer. The results show that the collapse is dominated by the dynamics of the
solvent, in particular the formation of a vapor bubble of critical size.
Implications of these findings to the understanding of pressure denaturation of
proteins are discussed.
