6533b7dbfe1ef96bd1271642

RESEARCH PRODUCT

Phase separation versus wetting: A mean field theory for symmetrical polymer mixtures confined between selectively attractive walls

Kurt BinderBurkhard DünwegThomas Flebbe

subject

BinodalPhysics and Astronomy (miscellaneous)Mean field theoryCondensed matter physicsAntisymmetric relationChemistryPhase (matter)Volume fractionGeneral EngineeringInverseBoundary value problemWettingAtomic and Molecular Physics and Optics

description

Partially compatible symmetrical (N A # N B = N) binary mixtures of linear flexible polymers (A, B) are considered in the presence of two equivalent walls a distance D apart, assuming that both walls preferentially adsorb the same component. Using a Flory-Huggins type mean field approach analogous to previous work studying wetting phenomena in the semi-infinite version of this model, where D → ∞, it is shown that a single phase transition occurs in this thin film geometry, namely a phase separation between an A-rich and a B-rich phase (both phases include the bulk of the film). The coexistence curve is shifted to smaller values of the inverse Flory-Huggins parameter x -1 with decreasing D, indicating enhanced compatibility the thinner the film. In addition, due to the surface enrichment of the preferred species (B), the critical volume fraction of A monomers is shifted away from Φ crit = 0.5 (where it occurs for D → ∞ due to the symmetry of the model) to the B-rich side. This behavior is fully analogous to the results established previously for the Ginzburg-Landau model of small molecule mixtures and to Monte Carlo simulations of corresponding lattice gas models. We argue that for symmetric walls the stable solutions always are described by volume fraction profiles Φ(z) that are symmetric as function of the distance z across the film around its center, but sometimes the system is inhomogeneous in the lateral direction parallel to the film, due to phase coexistence between A-rich and B-rich phases. Antisymmetric profiles obtained by other authors for symmetric boundary conditions are only metastable solutions of the mean field equations. The surface excess of B, whose logarithmic divergence as In |Φ - Φ coex | signals complete wetting for D → ∞, stays finite (and, in fact, rather small) for finite D: hence studies of wetting phenomena in thin film geometry need to be analyzed with great care.

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