Abstract
A fluid confined between two parallel walls that exert different (competitive) surface fields may exhibit phase equilibria strikingly different from those found for equal fields. Macroscopic arguments and an explicit mean-field analysis predict that if the fields are such that the fluid wets one wall and dries the other (above a certain critical wetting transition temperature Tw) coexistence of two phases can only occur, for finite wall separation L, when T<Tc,L, where the critical temperature Tc,L lies below Tw. A scaling Ansatz suggests & where βs is the exponent that describes the growth of the wetting layer.