Phenomenological nucleation theories are considered from the viewpoint
of Gibbs' surface thermodynamics. We point out, in defining the criti
cal nucleus, that it is important to make a distinction between the nu
mber of molecules enclosed by the surface of tension and the excess nu
mber of molecules over the uniform vapor phase. We show that, the Kelv
in equation should be employed in determining the size of the critical
nucleus even if the nucleus free energy contains a size-dependent sur
face energy term. Furthermore, we make use of the fact that the classi
cal form of Kelvin equation (containing the surface tension of a flat
interface) predicts the equimolar radius of the critical nucleus well
down to nuclei of about 40 molecules, and derive a new equation for th
e size-dependent surface tension that differs from the Tolman relation
. Density functional calculations support the new formula.