Forces holding the particles of a condensed phase together (cohesive forces) become anisotropic in the phase boundary region, and their normal component becomes smaller compared to the parallel component. To simplify the description and facilitate theoretical treatment, the properties of the boundary region of a condensed phase are projected onto a two-dimensional surface (Gibbs ''dividing surface''). The tensile stress resulting from the anisotropic forces in the boundary region is then termed the interfacial tension. This quantity corresponds to the reversible work required to bring particles from the volume phase to the interface during enlargement of the former, and thus corresponds to the increase in free enthalpy of the system per unit surface area: