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Title: Liquid-drop formalism and free-energy surfaces in binary homogeneous nucleation theory

Journal Article · · Journal of Chemical Physics
DOI:https://doi.org/10.1063/1.479470· OSTI ID:355432
 [1];  [2];  [3]
  1. Department of Applied Physics, University of Kuopio, P.O. Box 1627, 70211 Kuopio (Finland)
  2. Department of Applied Science, Brookhaven National Laboratory, Upton, New York 11973 (United States)
  3. Department of Physics, P.O. Box 9, 00014 University of Helsinki, Helsinki (Finland)

Three different derivations of the classical binary nucleation theory are considered in detail. It is shown that the derivation originally presented by Wilemski [J. Chem. Phys. {bold 80}, 1370 (1984)] is consistent with more extensive derivations [Oxtoby and Kashchiev, J. Chem. Phys. {bold 100}, 7665 (1994)]; Debenedetti, {ital Metastable Liquids: Concepts and Principles} (Princeton University Press, Princeton, 1996) if and only if the assumption is made that the surface of tension of the binary nucleus coincides with the dividing surface specified by the surface condition {summation}n{sub si}v{sub li}=0, where the n{sub si} denote surface excess numbers of molecules of species {ital i}, and the v{close_quote}s are partial molecular volumes. From this condition, it follows that (1) the surface tension is curvature independent and (2) that the nucleus volume is V={summation}n{sub li}v{sub li}={summation}g{sub i}v{sub li}, where the n{sub li} are the numbers of molecules in the uniform liquid phase of the droplet model encompassed by the surface of tension, and the g{sub i} are the total molecular occupation numbers contained by the nucleus. We show, furthermore, that the above surface condition leads to explicit formulas for the surface excess numbers n{sub si} in the nucleus. Computations for the ethanol{endash}water system show that the surface number for water molecules (n{sub s,H{sub 2}O}) causes the negative occupation numbers (g{sub H{sub 2}O}) obtained earlier using the classical nucleation theory. The unphysical behavior produced by the classical theory for surface active systems is thus a direct consequence of the assumption of curvature independence of surface tension. Based on the explicit formulas for n{sub si}, we calculate the full free-energy surfaces for binary nucleation in the revised classical theory and compare these with the free-energy surfaces in the Doyle (unrevised classical) theory. Significant differences in nucleus size and composition are found between these models and they are related to surface excess density. It is shown that only for the revised classical theory is the nucleus composition consistent with the Gibbs dividing surface model. {copyright} {ital 1999 American Institute of Physics.}

OSTI ID:
355432
Journal Information:
Journal of Chemical Physics, Vol. 111, Issue 5; Other Information: PBD: Aug 1999
Country of Publication:
United States
Language:
English

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