Free Energy of a Nonuniform System. I. Interfacial Free Energy

Свободная энергия неоднородной системы. I. Интерфейсная свободная энергия
John W. Cahn, J. E. Hilliard
1958-02-01

composition gradient terminterface thickness Critical scalinginterfacial free energynonuniform system free energy
It is shown that the free energy of a volume V of an isotropic system of nonuniform composition or density is given by : NV∫V [f0(c)+κ(▿c)2]dV, where NV is the number of molecules per unit volume, ▿c the composition or density gradient, f0 the free energy per molecule of a homogeneous system, and κ a parameter which, in general, may be dependent on c and temperature, but for a regular solution is a constant which can be evaluated. This expression is used to determine the properties of a flat interface between two coexisting phases. In particular, we find that the thickness of the interface increases with increasing temperature and becomes infinite at the critical temperature Tc, and that at a temperature T just below Tc the interfacial free energy σ is proportional to (Tc−T)32. The predicted interfacial free energy and its temperature dependence are found to be in agreement with existing experimental data. The possibility of using optical measurements of the interface thickness to provide an additional check of our treatment is briefly discussed.
1
For a regular solution κ is a constant that can be evaluated.
2
Just below Tc the interfacial free energy σ scales as (Tc − T)^{3/2}.
3
Optical measurements of interface thickness could provide an experimental check of the theoretical treatment.
4
The free energy density of a nonuniform isotropic system is NV[f0(c) + κ(∇c)^2], where NV is molecules per unit volume, f0 is homogeneous free energy per molecule, ∇c the composition/density gradient, and κ a (generally composition- and temperature-dependent) parameter.
5
The predicted magnitude and temperature dependence of σ agree with existing experimental data.
6
Using this free energy form, the thickness of a flat interface between coexisting phases increases with temperature and diverges (becomes infinite) at the critical temperature Tc.

Flat interface between two coexisting phases in an isotropic nonuniform system

Interfacial free energy and related properties (interface thickness, temperature dependence, especially σ ∝ (Tc−T)^{3/2} near criticality) derived from a gradient-expansion free-energy functional

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1958-02-01
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John W. Cahn
J. E. Hilliard
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