Excess Gibbs energy models which are widely used in modelling thermody
namic properties of multicomponent liquid phases are based on the assu
mption that long-range density or concentration fluctuations can be ne
glected. This assumption is no longer valid near a system's critical p
oint, where large density or concentration fluctuations effectively ma
sk the identity of the system and produce universal phenomena which ha
ve been well studied in simple liquid-vapor and liquid-liquid systems.
Based on the Landau-Ginzburg-Wilson theory of fluctuations, a crossov
er procedure has been developed to incorporate the effects of critical
fluctuations into a classical excess Gibbs energy model. As an exampl
e, we have applied our crossover procedure to the Non-Random Two-Liqui
d (NRTL) excess Gibbs energy model. This crossover procedure involves
the use of transformed variables for temperature and concentration and
the addition of a fluctuation term to the classical excess Gibbs ener
gy. The resulting transformed Gibbs energy has the universal scaling b
ehavior near the consolute critical point and has a smooth crossover t
o classical behavior far away from the consolute critical point. (C) 1
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