R. Evans et al., ASYMPTOTIC DECAY OF LIQUID STRUCTURE - OSCILLATORY LIQUID-VAPOR DENSITY PROFILES AND THE FISHER-WIDOM LINE, Molecular physics, 80(4), 1993, pp. 755-775
Recent work has highlighted the existence of a unified theory for the
asymptotic decay of the density profile rho(r) of an inhomogeneous flu
id and of the bulk radial distribution function g(r). For a given shor
t-ranged interatomic potential rho(r) decays into bulk in the same fas
hion as g(r), i.e. with the same exponential decay length (alpha0(-1))
and, for sufficiently high bulk density (rho(b)) and/or temperature (
T), oscillatory wavelength (2pi/alpha1). The quantities alpha0 and alp
ha1 are determined by a linear stability analysis of the bulk fluid; t
hey depend on only the bulk direct correlation function. In this paper
we reintroduce the concept of the Fisher-Widom (FW) line. This line w
as originally introduced, in say the (rho(b), T) plane, as that which
separates pure exponential from exponentially damped oscillatory decay
of g(r). We explore the relevance of the FW line for the form of the
density profile at a liquid-vapour interface. Using a weighted density
approximation (WDA) density functional theory we locate the FW line f
or the square-well model of an atomic fluid. We find that this line cr
osses the liquid branch of the liquid-vapour coexistence curve at T/T(
c); almost-equal-to 0.9, where T(c) is the critical temperature. Accor
dingly, for T less than or similar to 0.9 T(c), very general statistic
al mechanical theory predicts damped oscillatory decay of the liquid-v
apour density profile into the bulk liquid. Since the amplitude of the
oscillations is not determined by the linear analysis we have calcula
ted explicit nonlinear numerical solutions of our WDA theory, using a
high quality finite element method. Our results show that in a mean-fi
eld treatment the amplitude of the oscillatory profile in the saturate
d liquid tail is about 2% of rho(b) at temperatures approaching the tr
iple point and decreases rapidly as T increases towards the FW line. T
he predictions of the asymptotic profile decay theory are confirmed by
our explicit results and the unified nature of the phenomena is illus
trated by comparing results for the liquid-vapour profile with profile
s calculated for attractive wall-liquid interfaces at the same bulk li
quid state point. The effects of capillary-wave fluctuations on the os
cillatory nature of liquid-vapour profiles, above the FW line, are dis
cussed, and we argue that while incorporating such fluctuations should
lead to a significant reduction in the amplitude of oscillations, in
d = 3, at least, there should be no change to the period and decay len
gth for the profile in the liquid tail. The implications of our result
s for other interfacial properties, for computer simulations of the li
quid-vapour interface, for studies of wetting transitions and for the
nature of the solvation force that arises when a fluid is confined bet
ween two planar walls are considered.