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 TTc,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.
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Parry et al. (1990) studied this question.
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