Statistical mechanics of surface tension. It is shown that we can derive the expression of surface tension in terms of disrtribution functions from purely statistical considerations regarding surface tension as the increase in free energy for an increase of unit area of the interface between the liquid and vapor phases.
The expression obtained is
γ=1/2∫∫…∫dφ12/dR12x212-Z212/R12ρS(2)(Z, R12)dZ1dv12,
where γ is the surface tension, φ12 is the intermolecular potential and ρS(2) (Z, R12) is the excess pair density reckoned relative to an arbitrary Gibbs dividing surface. The above expression can be transformed into
γ=∫(pN-pT)dZ1
where
pN(Z)=kTρ(1)(Z1)-1/2∫∫…∫dv12∫Z1Z1-Z12dφ12/dR12Z12/R12ρ(2)(ζ, R12)dζ,
pT(Z1)=kTρ(1)(Z1)-1/2∫∫…∫dv12dφ12/dR12x122/R12ρ(2)(Z1, R12).
The results coincide with those of kirkwood and Buff which were derived by calculating stresses directly.