Condensed Matter Physics, 2018, vol. 21, No. 2, 23602
DOI:10.5488/CMP.21.23602           arXiv:1806.09941

Title: Non-additive symmetric mixtures at selective walls
Author(s):
  A. Patrykiejew (Department for the Modelling of Physico-Chemical Processes, Faculty of Chemistry, Maria Curie-Skłodowska University, 20031 Lublin, Poland)

The results of Monte Carlo simulation of adsorption and wetting behaviour of a highly non-additive symmetric mixture at selective walls is discussed. We have concentrated on the interplay between the surface induced demixing in the adsorbed films and the properties of the bulk mixture, which exhibits a closed immiscibility loop. It has been shown that the wetting behaviour depends on the absolute values of the parameters determining the strengths of interaction between the mixture components and the surface, as well as on their difference. In general, an increase of the difference between the adsorption energies of the components leads to a decrease of the wetting temperature. In the cases when the wetting of non-selective walls occurs at the temperatures above the onset of demixing transition in the bulk, an increasing wall selectivity leads to a gradual decrease of the wetting temperature towards the triple point, in which the vapour coexists with the mixed and demixed liquid phases. When the wetting temperature at the non-selective wall is located below the onset of the demixing transition in the bulk mixture, an increase of the adsorption energy of the selected component causes the developing adsorbed films to demix and to show the reentrant mixing upon approaching the bulk coexistence. At the temperatures above the onset of the demixing transition in the bulk, the adsorbed films remain demixed up to the bulk coexistence and undergo the first-order wetting transition. A rather unexpected finding has been the observation of a gradual increase of the wetting temperature at highly selective walls.

Key words: wetting, Monte Carlo methods, surface driven phase separation
PACS: 68.08.Bc, 68.35.Rh, 07.05.Tp


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