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首页> 外文期刊>Journal of Alloys and Compounds: An Interdisciplinary Journal of Materials Science and Solid-state Chemistry and Physics >Hot deformation behavior and microstructural evolution of Ti-22Al-25Nb-1.0B alloy prepared by elemental powder metallurgy
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Hot deformation behavior and microstructural evolution of Ti-22Al-25Nb-1.0B alloy prepared by elemental powder metallurgy

机译:用元素粉末冶金制备的Ti-22Al-25nb-1.0b合金的热变形行为和微观结构演化

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摘要

The hot deformation behavior of Ti-22Al-25Nb-1.0B alloy has been investigated at the temperature range of 1000-1200 °C and strain rate range of 0.001-1.0s~(-1) by hot compression tests. The micro-structural evolution with different InZ parameters was also analyzed by optical microscopy (OM) and transmission electron microscopy (TEM). Results showed that the flow stresses and microstructure evolution were sensitive to deformation parameters. The peak stress level decreased with increasing deformation temperature and decreasing strain rate. The hot deformation activation energy was calculated to be 524.02 kj/mol in the α2+B2 phase region and 378.59 kj/mol in the B2 phase region, respectively. Under conditions of high InZ values at 49.51 -47.21 in the α2+B2 phase region, cracking and localized plastic flow occurred, which should be avoided in hot working process. According to the microstructure evolution in TEM, it was found that the main soften mechanism transformed from dynamic recovery to dynamic recrystallization at low /nZ values. At high /nZ values obtained in the B2 phase region, the dislocation pile-up and dynamic recovery (DRV) can be found in the high InZ values rather than cracking or localized plastic flow due to low activation energy. The full dynamic recrystallization (DRX) occurs in the InZ values at 29.7-25.09. With decreasing the value of InZ to 24, the size of recrystallization grain becomes larger. The optimum hot working conditions are obtained at /nZ values at 45.34-25.09.
机译:通过热压缩试验在1000-1200℃和0.001-1.0s〜(-1)的温度范围内研究了Ti-22al-25nb-1.0b合金的热变形行为。还通过光学显微镜(OM)和透射电子显微镜(TEM)分析了具有不同inz参数的微结构演变。结果表明,流量应力和微观结构演化对变形参数敏感。随着变形温度的增加和应变速率降低,峰值应力水平降低。将热变形活化能量计算为α2+ B2相区域的524.02kJ / mol,分别在B2相区域中的378.59kJ / mol。在α2+ B2相位区域的49.51 -47.21处的高inz值的条件下,发生裂缝和局部塑料流动,在热工作过程中应该避免。根据TEM的微观结构演化,发现从动态恢复转化为低/ nz值的动态恢复变换。在B2相位区域中获得的高/ NZ值,位于高inz值中的位错堆积和动态恢复(DRV),而不是由于低激活能量而不是裂缝或局部塑性流量。完全动态再结晶(DRX)在INZ值发生在29.7-25.09。随着INZ至24的值下降,重结晶晶粒的尺寸变大。最佳的热工作条件是在45.34-25.09处获得/ NZ值。

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