Abstract

The phase transformation behavior between massive γ (γm) phase and γ lamellae was studied through interrupted quenching from single α-phase region and α+γ two-phase region in a Ti–48Al–3Nb-0.5Ta alloy. Massive α→γm phase transformation temperature T0 is confirmed to be 1400 °C (in α+γ two-phase region). Combining with the thermodynamic analysis, it indicates that the formation of γm phase is gradually inhibited with the decrease of quenching temperature, instead fine γ lamellae are preferred. In this case EBSD (Electron back scattered diffraction) and HRTEM (high resolution transmission electron microscope) have shown that besides nucleating on α grain boundary, γm phase can nucleate on defects in the interior of an α grain with Blackburn orientation relationship or nucleate on fine γ lamellae along close-packed {111}γ with orientation relationship of [121‾] γlamellae//[1‾11]γm1// [101‾1‾]α2 at their interface. Furthermore, the ledge growth mechanism of γm phase is identified.

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