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Phys. Rev. E 81, 041604 (2010) [12 pages]

Thermal fluctuation forces and wetting layers in colloid-polymer mixtures: Derivation of an interface potential

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J. O. Indekeu1, D. G. A. L. Aarts2, H. N. W. Lekkerkerker3, Y. Hennequin4, and D. Bonn4,5
1Instituut voor Theoretische Fysica, Katholieke Universiteit Leuven, Celestijnenlaan 200D, B-3001 Leuven, Belgium
2Department of Chemistry, Physical and Theoretical Chemistry Laboratory, University of Oxford, South Parks Road, Oxford OX1 3QZ, United Kingdom
3Van ’t Hoff Laboratory, Utrecht University, Padualaan 8, 3584CH Utrecht, The Netherlands
4Van der Waals–Zeeman Institute, University of Amsterdam, Valckenierstraat 65, 1018XE Amsterdam, The Netherlands
5Laboratoire de Physique Statistique, Ecole Normale Supérieure, 24 Rue Lhomond, 75231 Paris Cedex 05, France

Received 20 November 2009; revised 23 February 2010; published 28 April 2010

We discuss wetting layers in phase-separated colloid-polymer mixtures adsorbed at a vertical wall, observed in recent laser scanning confocal microscopy experiments. Matching of colloid and solvent dielectric properties renders van der Waals forces negligible and provides a system governed by short-range forces and thermal fluctuations on which the subtle predictions of renormalization group (RG) theory for wetting can be tested. The width w of the fluid-fluid (“liquid-gas”) interface bounding the wetting layer scales with the square root of the wetting layer thickness , in qualitative agreement with RG theory for short-range complete wetting in three dimensions. The measured wetting layer thickness as a function of the height h above the horizontal plane of bulk phase separation is compared with two distinct theoretical predictions. A simple heuristic interface potential V(), first proposed in a previous report, is now fully derived, and confronted here with the interface potential based on the linear RG theory. The heuristic approach does not capture fully the RG treatment. While fundamental differences exist between the two approaches, the resulting predictions for (h) are almost identical. However, the theory does not follow the precise shape of the experimental curve of (h).

© 2010 The American Physical Society

URL:
http://link.aps.org/doi/10.1103/PhysRevE.81.041604
DOI:
10.1103/PhysRevE.81.041604
PACS:
68.08.Bc, 82.70.Dd, 68.35.Ct, 68.37.-d