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  4. Crossover from capillary wave to van der Waals regime for fluid interfaces in two dimensions very close to the critical point
 
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Crossover from capillary wave to van der Waals regime for fluid interfaces in two dimensions very close to the critical point

Journal
The Journal of Chemical Physics
Journal Volume
93
Journal Issue
9
Pages
6800-6803
Date Issued
1990
Author(s)
Chen, L.-J.
Knackstedt, M.
Robert, M.
LI-JEN CHEN  
DOI
10.1063/1.458949
URI
http://www.scopus.com/inward/record.url?eid=2-s2.0-0040192228&partnerID=MN8TOARS
http://scholars.lib.ntu.edu.tw/handle/123456789/289022
Abstract
An analytic expression is derived for the interfacial profile of a liquid-vapor or a liquid-liquid phase equilibrium by assuming, in accord with current ideas, that the equilibrium interface consists of an intrinsic interface of the nonclassical van der Waals type broadened by capillary wave fluctuations. It is shown that in two dimensions of space, the interfacial thickness exhibits a crossover with change of critical exponent from capillary wave behavior at low and near-critical temperatures, to van der Waals behavior at temperatures very close to the critical temperature. The location of the crossover temperature is determined by the ratio of the critical amplitudes of the root-mean squared interfacial thickness and the bulk correlation length. From available experimental data and theory, an estimate of the order of magnitude of the critical amplitude ratio is made, from which the crossover is found to occur in the temperature range 3×10-4 K < (T c - T) < 0.3 K. In the currently accessible temperature range, the capillary wave prediction prevails, in contrast to the case of three-dimensional systems. © 1990 American Institute of Physics.
Type
journal article

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