Microstructure, mechanical properties and corrosion resistance of low-cost Ti–Al–Cr–Fe alloys processed via powder metallurgy

A variety of economical Ti–3Al–6Cr-xFe (x = 0, 1, 2 wt%) alloys were prepared utilizing typical powder metallurgy (cold pressing and sintering) to explore the impact of Fe concentration on the densification behavior, phase evolution, microstructure, mechanical properties and corrosion resistance. Th...

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Bibliographic Details
Published inMaterials chemistry and physics Vol. 317; p. 129197
Main Authors Zhou, Xiangxing, Fang, Haoyu, Li, Ruidi, Yuan, Tiechui
Format Journal Article
LanguageEnglish
Published Elsevier B.V 15.04.2024
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Summary:A variety of economical Ti–3Al–6Cr-xFe (x = 0, 1, 2 wt%) alloys were prepared utilizing typical powder metallurgy (cold pressing and sintering) to explore the impact of Fe concentration on the densification behavior, phase evolution, microstructure, mechanical properties and corrosion resistance. The inclusion of Fe increases the compressibility. The high diffusivity of the Fe element contributes to the densification but excessive Fe inclusion causes Kirkendall pores to develop. Therefore, Ti–3Al–6Cr–1Fe has the highest density. Every alloy is made up of intermetallic (TiCr2), α, and β phases. The proportion of the β phase rose with the addition of Fe. The optimal combination of mechanical characteristics was obtained by Ti–3Al–6Cr–1Fe (ultimate tensile strength of 1093 MPa and ductility of 3.1%), which is explained by the interaction of higher density and solid solution strengthening effects. Ti–3Al–6Cr–2Fe has the greatest corrosion resistance due to the relatively high density and maximum β phase proportion. •Innovative, economical Ti–Al–Cr–Fe alloys were created using a traditional press and sinter process.•Fe inclusion decreases the α phase fraction and raises the β phase proportion.•The highest density (98.8%) and strength (1093 MP) were observed in Ti–3Al–6Cr–1Fe sample.•Ti–3Al–6Cr–2Fe alloy exhibited the best corrosion resistance among all samples.
ISSN:0254-0584
1879-3312
DOI:10.1016/j.matchemphys.2024.129197