A disclosure of the role of frequency on the plasma electrolytic oxidation of AZ31 magnesium alloy in aluminate-tungstate electrolyte

TL;DR

This study investigates how varying current frequency affects the microstructure, composition, and appearance of plasma electrolytic oxidation coatings on AZ31 magnesium alloy in aluminate-tungstate electrolyte, revealing that higher frequencies produce thicker, darker, and more porous coatings.

Contribution

It provides new insights into the influence of current frequency on PEO coating properties and elucidates the formation mechanisms at different frequencies.

Findings

Higher frequency increases coating thickness, roughness, and porosity.

Coatings at higher frequencies have higher W/Al atomic ratios.

Micro-discharges are stronger and more gas evolution occurs at higher frequencies.

Abstract

Plasma electrolytic oxidation (PEO) was carried out to form black ceramic coatings on AZ31 magnesium alloy in aluminate-tungstate electrolyte. Influences of current frequency (such as 100, 1000 and 2000 Hz) on properties of the PEO coatings have been explored. It was found that increment of frequency led to coatings with higher thickness, higher roughness and darker appearance. In order to explore the coating formation mechanism at different frequencies, the micro-discharges at different frequencies were investigated by real-time imaging method. Microstructure of coatings was characterized by scanning electron microscopy (SEM) assisted with energy dispersive X-ray spectroscopy (EDS). Coatings formed at 100 Hz show the most compact microstructure while porosity of the coatings, both in the pore number and pore size, is greatly increased at higher frequencies. The coatings formed at higher frequencies show an increased atomic ratio of W/Al. The cancel of the negative pulse from the pulsed waveform can also lead to a higher W/Al ratio, and hence a darker coating. The higher porosity of the coatings was attributed to the stronger plasma discharges and gas evolution at higher frequencies. The stronger plasma discharge is induced by the fact that there is not sufficient time for the cooling down of discharge channels at higher frequencies.