The formation of a crystalline passivation layer on anodically dissolving m
etal surfaces is shown to involve a heterogeneous two-dimensional nucleatio
n of passivation oxide. The nucleation rate I-n (phi(a), phi, phi(0)) is ex
pressed as a function of the anode potential phi(a), energy of intermolecul
ar interactions within the nucleus (phi), and energy of its bonding to the
metal support (phi(0)) This function is one of the basic physical character
istics of the passivation of metals. In particular, it is important for fur
ther development of the theory of activation-passivation transitions.