Microstructure Evolution during High-Temperature Deformation of Ti-5Al-5V-2Mo-1Cr-1Fe Alloy under Compression
Autor: | Aditya Sarkar, S.V.S.N. Murty, V. Anil Kumar, M.J.N.V. Prasad, R. K. Gupta |
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Rok vydání: | 2021 |
Předmět: |
010302 applied physics
Materials science Mechanical Engineering Alloy 02 engineering and technology Deformation (meteorology) engineering.material 021001 nanoscience & nanotechnology Microstructure 01 natural sciences Isothermal process Hot working Mechanics of Materials Phase (matter) 0103 physical sciences engineering Dynamic recrystallization General Materials Science Lamellar structure Composite material 0210 nano-technology |
Zdroj: | Journal of Materials Engineering and Performance. 30:3258-3272 |
ISSN: | 1544-1024 1059-9495 |
DOI: | 10.1007/s11665-021-05660-0 |
Popis: | Hot isothermal compression testing of Ti-5Al-5V-2Mo-1Cr-1Fe alloy exhibiting lamellar (α/β) microstructure was performed using a deformation simulator. The flow curves of the alloy were obtained as a function of temperature around its beta transus (‘Tβ’, the allotropic transformation temperature from HCP to BCC phase) at different strain rates in the range of 10−2-10 s−1. The apparent activation energy ‘Q’ for the alloy under these hot working conditions was found to be ~ 644 and ~ 317 kJ mol−1 in two-phase (α + β) and single-phase β regimes, respectively. Distinct constitutive relationships for the alloy have been established at various temperature regimes. Dynamic material model was employed to generate the processing maps and thereby evaluate the stable domains for hot working of this alloy. Deformation below the ‘Tβ’ led to α lamellae kinking followed by fragmentation and dynamic recrystallization of α phase. While deformation above ‘Tβ’ resulted in serrated β boundary, an indicative of dynamic recovery (DRV) of β phase. The processing maps along with the detailed post-deformed microstructural examination showed that the optimum/safe working domains for processing of the alloy are ‘T’ = 1123-1163 K and ‘ $$\dot{\varepsilon }$$ ’ = 10−2-10 s−1. |
Databáze: | OpenAIRE |
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