Recent contributions to the passivity of iron and iron-base alloys were reviewed, and the anodic current-potential and film thickness-potential curves of iron, nickel and cobalt were shown along with the discussions of ionic current in and dissolution current of the passive film. There is a barrier oxide layer on the surface of passivated metals. For iron it is an iron-deficient magnetite layer, for nickel a layer of NiO with excess oxygen, and for cobalt a bi-layer of CoO/Co
3O
4. The ionic current in the barrier oxide layer on iron and in the outer barrier Co
3O
4 layer on cobalt obeys a field-assisted ion migration mechanism. This mechanism, however, does not hold for the barrier NiO layer on nickel and the inner CoO layer on cobalt. The dissolution current of the passive film is controlled by the potential difference across the Helmholtz layer at the film/solution interface, and a Tafel relation is found to hold between the film dissolution current and the overpotential at the Helmholtz layer, leading to the mechanism for iron as Fe
3+ (oxide)→Fe
3+ (solution) and for cobalt as Co
2+ (oxide)→Co
2+ (solution). A generalized theory was presented in which the metal passivity was attributed to the involvement of a thin oxide film into the structure of electrified interface between the metal and the solution. The passive film formed on a metal changes the electrical double layer at the metal/solution interface into a bi-layer structure consisting of a thin oxide layer and the Helmholtz layer at the film/solution interface, and thus the effective overpotential for metal ion transfer across the Helmholtz layer is reduced resulting in a decrease of metal dissolution rate.
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