“…In the case of a plane interface, the excess, surface part of the functional of grand thermodynamic potential Ω s has the form [2,6,8] , (1) , (2) where A is the area of the interface, p is the pressure, µ is the chemical potential, ρ is the number density, and T is the temperature; the subscript s indicates the quantities relating to the equilibrium coexistence of phases. The function ψ takes into account the effect of nonuniform distribution of particles in the system and, in the general case, depends on various derivatives of one-particle density ρ(z) (square of gradient , Laplacian ∆ρ, and so on).…”