2006
DOI: 10.1016/j.ces.2006.05.013
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Phase equilibrium of a liquid droplet formed on a solid particle

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Cited by 9 publications
(3 citation statements)
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“…The wetting degree m equals the cosine of the contact angle θ, i.e., m¼ cos θ. We neglect the effect of the disjoining pressure (Kuni, Shchekin, Rusanov, & Widom, 1996;Mitrovic, 2006) which is defined as the difference between the pressure of the film and the pressure in the bulk phase, because the surface of solid particle is only partial…”
Section: The Derivation Of the Modified Expressionmentioning
confidence: 99%
“…The wetting degree m equals the cosine of the contact angle θ, i.e., m¼ cos θ. We neglect the effect of the disjoining pressure (Kuni, Shchekin, Rusanov, & Widom, 1996;Mitrovic, 2006) which is defined as the difference between the pressure of the film and the pressure in the bulk phase, because the surface of solid particle is only partial…”
Section: The Derivation Of the Modified Expressionmentioning
confidence: 99%
“…p δ denotes the disjoining pressure, 27,28 which is defined as the difference between the pressure of the film and the pressure in the bulk phase, A 0 is the Hamaker constant, 28 and δ is the film thickness. The surface of solid particle is only partial wetting in our context, and therefore, the liquid phase forms as some separate spherical cap shaped droplets with a finite contact angle on the surface.…”
Section: Kinetic Modelmentioning
confidence: 99%
“…They have been comprehensively studied in the past, and the reader is referred to the treatises of Derjaguin et al [2] and Israelachvili [3] as well as references therein. When the liquid film completely covers the wall surface at a thickness larger than the range of molecular interaction, equilibrium state establishes among the phases, e.g., [4].…”
Section: Introductionmentioning
confidence: 99%