Weeks, The roughening transition, in Ordering in Strongly Fluctuating Condensed Matter Sys-tems, Edited by T. Croxton, John Wiley & Sons, New York, 1986, Chapter 5. Poniewierski, in Fluid Interfacial Phenomena, Edited by C.A. Widom, Molecular Theory of Capillarity, Oxford University Press, New York and London, 1982. Godrèche, Cambridge University Press, Cambridge, 1992. Nozières, Shape and growth of crystals, in: Solids Far From Equilibrium, Edited by C. Lifshitz, Statistical Physics, 3rd edition, Pergamon Press, Oxford, 1978. ![]() Isenberg, The Science of Soap Films and Soap Bubbles, Dover, 1992.ī. Everett, Basic Principles of Colloid Science, Royal Society of Chemistry, London, 1988, 244 pp. the question of a satisfactory definition of the term 'surface' or 'interface' (which may be a better word than 'sur-face' because-unless the solid is sus-pended in a vacuum-it is in contact with a gas, a liquid, or. Ong, World Scientific, Singapore, 1995, 430 pp.ĭ.H. Surface Phenomena Characteristics of solid surfaces and general problems related to surface phenomena were the subjects of the. Drzaic, Liquid Crystal Dispersions, Series on Liquid Crystals, vol. Sonin, Surface Physics of Thermotropic Liquid Crystals, Usp. Gast, Physical Chemistry of Surfaces, John Wiley & Sons, Inc., New York, 1997, 784 pp. This process is experimental and the keywords may be updated as the learning algorithm improves.Ī.W. These keywords were added by machine and not by the authors. Monolayers and bilayers of surfactants are reviewed in Chapter 14. In this chapter, we consider surface effects both for isotropic and for anisotropic media. For example, bounded volumes of liquid crystals in equilibrium contain topologically stable defects that are stable exclusively because of the surface conditions, as in Fig. However, there can also be global consequences of surface interactions. Because the volume-to-surface ratio grows with the system size, the local surface effects are often neglected when a large system is considered. These differences lead to local changes that normally occur over length scales of a few atomic radii. ![]() The most obvious effect of the confinement is local: Molecular interactions in the bulk and at the boundaries are different. Real samples of condensed matter phases are necessarily bounded.
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