Volume 44 Issue 9
Sep.  2024
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CUI Shitang, ZHAO Hongyu, DONG Fangdong, ZHANG Yongliang. Effect of phase transformation on wave speeds in TiNi alloy thin-walled tube[J]. Explosion And Shock Waves, 2024, 44(9): 091425. doi: 10.11883/bzycj-2023-0368
Citation: CUI Shitang, ZHAO Hongyu, DONG Fangdong, ZHANG Yongliang. Effect of phase transformation on wave speeds in TiNi alloy thin-walled tube[J]. Explosion And Shock Waves, 2024, 44(9): 091425. doi: 10.11883/bzycj-2023-0368

Effect of phase transformation on wave speeds in TiNi alloy thin-walled tube

doi: 10.11883/bzycj-2023-0368
  • Received Date: 2023-08-30
  • Rev Recd Date: 2024-05-10
  • Available Online: 2024-05-14
  • Publish Date: 2024-09-20
  • Shape memory alloys undergo phase transformation under strong impact loads, and the phase transformation has a significant impact on the dynamic mechanical response of their structural components. Based on the phase transformation critical criterion considering both hydrostatic pressure and deviatoric stress effects, an incremental constitutive model of phase transformation is derived. The analytical expression of characteristic wave speed under complex stress state is obtained based on the generalized characteristic theory. The characteristic wave speed is not only related to the mechanical parameters of the material itself (such as the tension-compression asymmetry and the modulus of the mixed phase), but also related to the stress state of the material. For TiNi alloys with volume expansion due to phase transformation, the increase of tensile-compressive asymmetry coefficient will increase the wave speed of slow waves, while having almost no effect on fast waves. At the short axis of the phase transformation ellipse (α = 90°), the wave speed of slow waves is the lowest and decreases significantly with the increase of the dimensionless modulus of the mixed phase. When the dimensionless modulus of the mixed phase increases from 2 to 5, the wave speed decreases by 36.2%, while the wave speed of fast waves reaches the maximum value c0, which is independent of the modulus of the mixed phase; at the long axis of the phase transformation ellipse (α = 180°), the speed of slow waves reaches the maximum value, and the wave speed of fast waves reaches the minimum value c2.
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