paper

Colligative properties of solutions: II. Vanishing concentrations

arXiv:math-ph/0407035 · doi:10.1007/s10955-005-3017-1

Abstract

We continue our study of colligative properties of solutions initiated in math-ph/0407034. We focus on the situations where, in a system of linear size , the concentration and the chemical potential scale like and , respectively. We find that there exists a critical value $\xit$ such that no phase separation occurs for $ξ\le\xit$ while, for $ξ>\xit$, the two phases of the solvent coexist for an interval of values of . Moreover, phase separation begins abruptly in the sense that a macroscopic fraction of the system suddenly freezes (or melts) forming a crystal (or droplet) of the complementary phase when reaches a critical value. For certain values of system parameters, under ``frozen'' boundary conditions, phase separation also ends abruptly in the sense that the equilibrium droplet grows continuously with increasing and then suddenly jumps in size to subsume the entire system. Our findings indicate that the onset of freezing-point depression is in fact a surface phenomenon.

27 pages, 1 fig; see also math-ph/0407034 (both to appear in JSP)

Colligative properties of solutions: II. Vanishing concentrations · wovepaper