Journal of the Metal Finishing Society of Japan
Online ISSN : 1884-3395
Print ISSN : 0026-0614
ISSN-L : 0026-0614
Reaction of Porous Anodic Oxide Films on Aluminum with Hot Water
IV Analysis of the Film Structure by Gravimetry and Porefilling Method
Mitsuru KODAHideaki TAKAHASHIMasaichi NAGAYAMA
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1983 Volume 34 Issue 9 Pages 460-466

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Abstract

Porous anodic oxide films formed on Al in an oxalic acid solution were hydrated for various periods by reaction with hot water. As reported earlier, the hydrous oxide is formed on the entire surface of the pore-walls to fill up the pores in about 10min, and then the hydration slowly continues from the outer surface so that the outermost part of the film becomes completely hydrated. Using gravimetric data and assuming the composition and density of the hydrous oxide to be Al2O3⋅2H2O and 2.6, the thickness of the fully hydrated portion of the film, Hhy, the thickness of the film portion containing the unhydrated pore-wall, Hox, and the thickness of the unhydrated pore-wall, δ, were calculated. In another series of experiments, the hydrated films were re-anodized with constant currents, ir, of 0.01 and 0.5mA/cm2 in a neutral borate solution to examine potential-time characteristics. For the smaller anodizing current, the steady potentials are related to the thicknesses of the barrier layers remaining unhydrated; they agree well with those estimated from capacitance measurements. Re-anodizing with the larger current causes dehydration of the hydrous oxide in the pores at the barrier layer/hydrous oxide layer interface, and voids produced by the dehydration are filled up with new oxide formed by the transport of Al3+ ion through the barrier layer. The growth of the barrier layer is reflected in the voltage-time characteristics. The transport number of Al3+ ion, TAl3+, was found to be 0.24. Using this value, Hog was estimated from the voltage-time curve. The values of Hox obtained as a function of the hydration time, th, were in good agreement with those estimated by gravimetry.

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