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Strain rate sensitivity and strain hardening exponent during the isothermal compression of Ti60 alloy

机译:Ti60合金等温压缩过程中的应变率敏感性和应变硬化指数

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In this paper, the flow stress was investigated in detail during the isothermal compression of Ti60 alloy. The strain rate sensitivity and the strain hardening exponent of Ti60 alloy were calculated based on the flow stress-strain curves. The results showed that the softening effect in the α + β two-phase region was more significant than that in the β single-phase region due to the change in the deformation heat of the alloy. An initial yield drop was observed at or above 1273 K and in the strain rate range of 0.1-10.0 s~(-1). The β phase became the continuous phase above 1273 K, which led to little temperature dependence of flow stress. The maximum m value of 0.34 occurred at 1253 K and a strain rate of 0.001 s~(-1) during the isothermal compression of Ti60 alloy. The strain rate sensitivity at a strain of 0.7 and a strain rate of 10.0 s~(-1)decreased with increasing deformation temperature after a peak value. And the m values decreased with increasing strain rate. This phenomenon could be reasonably explained based on the microstructure evolution during the isothermal compression of Ti60 alloy. The strain hardening exponent increased with increasing deformation temperature at the strain rates of 0.001 s~(-1),1.0 s~(-1) and 10.0s~(-1). The variation of strain hardening exponent with strain was observed to be dependent on the strain rate and the deformation temperature.
机译:本文详细研究了Ti60合金等温压缩过程中的流变应力。基于流变应力-应变曲线,计算了Ti60合金的应变速率敏感性和应变硬化指数。结果表明,由于合金变形热的变化,α+β两相区的软化效果比β单相区的软化效果更显着。在等于或高于1273 K且应变速率范围为0.1-10.0 s〜(-1)时,观察到了初始屈服下降。 β相成为高于1273 K的连续相,导致流动应力对温度的依赖性很小。 Ti60合金等温压缩过程中,最大m值为0.34,出现在1253 K,应变速率为0.001 s〜(-1)。峰值后,随着变形温度的升高,应变为0.7,应变率为10.0 s〜(-1)时的应变率敏感性降低。随着应变率的增加,m值减小。可以根据Ti60合金等温压缩过程中的微观组织演变合理地解释这种现象。应变硬化指数随变形温度的升高而增加,应变速率分别为0.001 s〜(-1),1.0 s〜(-1)和10.0s〜(-1)。观察到应变硬化指数随应变的变化取决于应变速率和变形温度。

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