As polar surfaces in solvent are brought together, they experience a large repulsive interaction, termed the solvation pressure. The solvation pressure between rough surfaces, such as lipid bilayers, has been shown previously to decay exponentially with distance between surfaces. In this paper, we compare measured values of the salvation pressure between bilayers and the dipole potential for monolayers in equilibrium with bilayers. For a variety of polar solvents and lipid phases, we rind a correlation between the measured solvation pressures and dipole potentials. Analysis of the data indicates that the magnitude of the salvation pressure is proportional to the square of the dipole potential. Our experiments also show that the oriented dipoles in the lipid headgroup region, including those of both the lipid and solvent molecules, contribute to the dipole potential. We argue that (i) the field produced by these interfacial dipoles polarizes the interbilayer solvent molecules giving rise to the solvation pressure and (ii) both the solvation pressure and the dipole potential decay exponentially with distance from the bilayer surface, with a decay constant that depends on the packing density of the interbilayer solvent molecules (1-2 i in water).These results may have importance in cell adhesion, adsorption of proteins to membranes, characteristics of channel permeability, and the interpretation of electrokinetic experiments.The close approach of adjacent biological or lipid bilayer membranes is resisted by several repulsive pressures, one being the solvation or hydration pressure (if the solvent is water). The solvation pressure is thought to be the dominant interbilayer repulsive pressure for bilayer separations of about 5-20 A (1-6). For rough surfaces, such as lipid bilayers, it has been found that the solvation pressure, Ph, decays exponentially with increasing separations, such that Ph = Poexp(-df/A), where df is the distance between adjacent bilayers (1, 2, 4-6) and A is the decay length. A goal of both experimentalists and theoreticians is to determine characteristics of the surface and solvents that give rise to specific values of P0 and A.Numerous theoretical treatments (7-19) have been proposed to explain the range and magnitude of the solvation pressure. Most theories are general in that they do not consider the molecular structure of the solvated surface or the specific interactions of the surface with the solvent. However, it is generally agreed that solvation repulsion arises from the polarization and reorganization of solvent molecules near the membrane surface.In their pioneering studies to explain the magnitude of the hydration pressure between specific lipid bilayers, Cevc and Marsh (13,20) proposed that the electric field that polarizes solvent molecules arises from fixed charges and perpendicular components of the "multipole surface charge densities" in the polar headgroup of lipids. Using a theory based on polarization of water molecules by the lipid headgroups, they concluded that P=...