The Characteristic of <inline-formula><math display="inline"><semantics><mrow><mrow><mo mathvariant="bold">{</mo><mn mathvariant="bold">10</mn></mrow><mover accent="true"><mrow><mn mathvariant="bold">1</mn></mrow><mo stretchy="false" mathvariant="bold">¯</mo></mover><mrow><mn mathvariant="bold">2</mn><mo mathvariant="bold">}</mo><mo mathvariant="bold"><</mo><mn mathvariant="bold">10</mn></mrow><mover accent="true"><mrow><mn mathvariant="bold">1</mn></mrow><mo stretchy="false" mathvariant="bold">¯</mo></mover><mover accent="true"><mrow><mn mathvariant="bold">1</mn></mrow><mo stretchy="false" mathvariant="bold">¯</mo></mover><mo>></mo></mrow></semantics></math></inline-formula> Twin of Ti-10V-2Fe-3Al under Planar Wave Detonation

oleh: Tong Wang, Ping Yang, Jin Zhang, Xin-Fu Gu

Format: Article
Diterbitkan: MDPI AG 2023-10-01

Deskripsi

The microstructure evolution of the twin of TB6 (Ti-10V-2Fe-3Al) under planar wave detonation was studied. The initial microstructure of the alloy consists of an α and β phase. It is found that twin deformation is operated in only the α phase due to the limited slip system in this phase. α grains are mainly rotated from <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>{</mo><mn>10</mn></mrow><mover accent="true"><mrow><mn>1</mn></mrow><mo stretchy="false">¯</mo></mover><mrow><mn>0</mn><mo>}</mo></mrow></mrow></semantics></math></inline-formula> to <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>{</mo><mn>0002</mn><mo>}</mo></mrow></mrow></semantics></math></inline-formula> during the deformation due to the <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>{</mo><mn>10</mn></mrow><mover accent="true"><mrow><mn>1</mn></mrow><mo stretchy="false">¯</mo></mover><mrow><mn>2</mn><mo>}</mo><mo><</mo><mn>10</mn></mrow><mover accent="true"><mrow><mn>1</mn></mrow><mo stretchy="false">¯</mo></mover><mover accent="true"><mrow><mn>1</mn></mrow><mo stretchy="false">¯</mo></mover><mo>></mo></mrow></semantics></math></inline-formula> twin. Twin variant selection is found in this study, and the orientation of all <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>{</mo><mn>10</mn></mrow><mover accent="true"><mrow><mn>1</mn></mrow><mo stretchy="false">¯</mo></mover><mrow><mn>2</mn><mo>}</mo></mrow></mrow></semantics></math></inline-formula> twins is oriented at <inline-formula><math xmlns="http://www.w3.org/1998/Math/MathML" display="inline"><semantics><mrow><mrow><mo>{</mo><mn>0002</mn><mo>}</mo></mrow></mrow></semantics></math></inline-formula> in different α grains with different deformation degrees. The twin variant selection is well explained based on the strain relaxation along the loading axis and the Schmid factor for twinning shear.