Dynamic Softening Mechanisms and Microstructure Evolution of TB18 Titanium Alloy during Uniaxial Hot Deformation
In this study, isothermal compression tests of TB18 titanium alloy were conducted using a Gleeble 3800 thermomechanical simulator for temperatures ranging from 650 to 880 °C and strain rates ranging from 0.001 to 10 s<sup>−1</sup>, with a constant height reduction of 60%, to investigate...
| Published in: | Metals |
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| Format: | Article |
| Language: | English |
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MDPI AG
2021-05-01
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| Online Access: | https://www.mdpi.com/2075-4701/11/5/789 |
| _version_ | 1850089032016461824 |
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| author | Qiang Fu Wuhua Yuan Wei Xiang |
| author_facet | Qiang Fu Wuhua Yuan Wei Xiang |
| author_sort | Qiang Fu |
| collection | DOAJ |
| container_title | Metals |
| description | In this study, isothermal compression tests of TB18 titanium alloy were conducted using a Gleeble 3800 thermomechanical simulator for temperatures ranging from 650 to 880 °C and strain rates ranging from 0.001 to 10 s<sup>−1</sup>, with a constant height reduction of 60%, to investigate the dynamic softening mechanisms and hot workability of TB18 alloy. The results showed that the flow stress significantly decreased with an increasing deformation temperature and decreasing strain rate, which was affected by the competition between work hardening and dynamic softening. The hyperbolic sine Arrhenius-type constitutive equation was established, and the deformation activation energy was calculated to be 303.91 kJ·mol<sup>−1</sup> in the (α + β) phase zone and 212.813 kJ·mol<sup>−1</sup> in the β phase zone. The processing map constructed at a true strain of 0.9 exhibited stability and instability regions under the tested deformation conditions. The microstructure characteristics demonstrated that in the stability region, the dominant restoration and flow-softening mechanisms were the dynamic recovery of β phase and dynamic globularization of α grains below transus temperature, as well as the dynamic recovery and continuous dynamic recrystallization of β grains above transus temperature. In the instability region, the dynamic softening mechanism was flow localization in the form of a shear band and a deformation band caused by adiabatic heating. |
| format | Article |
| id | doaj-art-b6ad7c91ed564df0b0befb614d9e331d |
| institution | Directory of Open Access Journals |
| issn | 2075-4701 |
| language | English |
| publishDate | 2021-05-01 |
| publisher | MDPI AG |
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| spelling | doaj-art-b6ad7c91ed564df0b0befb614d9e331d2025-08-20T00:09:42ZengMDPI AGMetals2075-47012021-05-0111578910.3390/met11050789Dynamic Softening Mechanisms and Microstructure Evolution of TB18 Titanium Alloy during Uniaxial Hot DeformationQiang Fu0Wuhua Yuan1Wei Xiang2College of Materials Science and Engineering, Hunan University, Changsha 410082, ChinaCollege of Materials Science and Engineering, Hunan University, Changsha 410082, ChinaDeyang Wanhang Die Forging Co., Ltd., China National Erzhong Group Co., Deyang 618013, ChinaIn this study, isothermal compression tests of TB18 titanium alloy were conducted using a Gleeble 3800 thermomechanical simulator for temperatures ranging from 650 to 880 °C and strain rates ranging from 0.001 to 10 s<sup>−1</sup>, with a constant height reduction of 60%, to investigate the dynamic softening mechanisms and hot workability of TB18 alloy. The results showed that the flow stress significantly decreased with an increasing deformation temperature and decreasing strain rate, which was affected by the competition between work hardening and dynamic softening. The hyperbolic sine Arrhenius-type constitutive equation was established, and the deformation activation energy was calculated to be 303.91 kJ·mol<sup>−1</sup> in the (α + β) phase zone and 212.813 kJ·mol<sup>−1</sup> in the β phase zone. The processing map constructed at a true strain of 0.9 exhibited stability and instability regions under the tested deformation conditions. The microstructure characteristics demonstrated that in the stability region, the dominant restoration and flow-softening mechanisms were the dynamic recovery of β phase and dynamic globularization of α grains below transus temperature, as well as the dynamic recovery and continuous dynamic recrystallization of β grains above transus temperature. In the instability region, the dynamic softening mechanism was flow localization in the form of a shear band and a deformation band caused by adiabatic heating.https://www.mdpi.com/2075-4701/11/5/789TB18 titanium alloydynamic softening mechanismdynamic recoverydynamic recrystallizationdynamic globularization |
| spellingShingle | Qiang Fu Wuhua Yuan Wei Xiang Dynamic Softening Mechanisms and Microstructure Evolution of TB18 Titanium Alloy during Uniaxial Hot Deformation TB18 titanium alloy dynamic softening mechanism dynamic recovery dynamic recrystallization dynamic globularization |
| title | Dynamic Softening Mechanisms and Microstructure Evolution of TB18 Titanium Alloy during Uniaxial Hot Deformation |
| title_full | Dynamic Softening Mechanisms and Microstructure Evolution of TB18 Titanium Alloy during Uniaxial Hot Deformation |
| title_fullStr | Dynamic Softening Mechanisms and Microstructure Evolution of TB18 Titanium Alloy during Uniaxial Hot Deformation |
| title_full_unstemmed | Dynamic Softening Mechanisms and Microstructure Evolution of TB18 Titanium Alloy during Uniaxial Hot Deformation |
| title_short | Dynamic Softening Mechanisms and Microstructure Evolution of TB18 Titanium Alloy during Uniaxial Hot Deformation |
| title_sort | dynamic softening mechanisms and microstructure evolution of tb18 titanium alloy during uniaxial hot deformation |
| topic | TB18 titanium alloy dynamic softening mechanism dynamic recovery dynamic recrystallization dynamic globularization |
| url | https://www.mdpi.com/2075-4701/11/5/789 |
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