The intermolecular forces that cause surface tension in multiphase sys
tems at equilibrium give rise to pressure gradients in nonequilibrium
systems. The present paper treats such systems within a framework of t
hermodynamics and continuum mechanics and uses a generalization of the
conceptual experiment of Rowlinson and Widom which applies to systems
with curved interfaces and to nonequilibrium situations where the pha
se interfaces are not fully developed. The pressure tensor has a compo
nent p(n) acting in the direction normal to the concentration gradient
and a component p(t) acting in the plane tangent to the surface of co
nstant concentration where p(n) - p(t) = kappa(delc)2 The concentratio
n gradient causes an additional volumetric force not present in homoge
neous fluids: dF/dV = - kappa(delc)2 (1/R1 + 1/R2) n + del(s)kappa(del
c)2 Here, kappa is the gradient energy parameter appearing in the Land
au-Ginzburg functional, c is the concentration of the key component, R
1 and R2 are the principal radii of curvature for the surface of const
ant constration, n is a unit vector normal to that surface, and del(s)
is the gradient along the surface. The volumetric force generates pre
ssure gradients in systems with curved interfaces at equilibrium or ca
n drive flow in nonequilibrium situations.