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首页> 外文期刊>Materials Science and Engineering >Flow softening mechanism of Ti-5Al-2Sn-2Zr-4Mo-4Cr with different initial microstructures at elevated temperature deformation
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Flow softening mechanism of Ti-5Al-2Sn-2Zr-4Mo-4Cr with different initial microstructures at elevated temperature deformation

机译:不同初始微观结构的Ti-5Al-2Sn-2Zr-4Mo-4Cr高温变形流动软化机理

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摘要

The flow softening mechanism of Ti-5Al-2Sn-2Zr-4Mo-4Cr with different initial microstructures was investigated considering the plastic deformation heat effect and the microstructure evolution. Two initial microstructures were employed: one initial microstructure A (MA) with equiaxed and elongated primary α grains, and another initial microstructure B (MB) with Widmanstaetten α platelets. The adiabatic plastic deformation effect was estimated by calculating the temperature rise, and the microstructure evolution was observed by using OM, TEM and EBSD. The results revealed that the initial microstructure B presented a higher flow softening effect at a certain deformation temperature and strain rate than the initial microstructure A. For both the two initial microstructures, the plastic deformation heat effect was one of the main factors for flow softening at the strain rates above 0.01 s~(-1) and the dynamic recovery dominated the shape of strain-stress curves at a strain rate of 0.01 s~(-1). The flow localization for the initial microstructure B at a strain rate of 5.0 s~(-1) was more evident, which led to the larger flow softening effect Moreover, the dynamic recrystallization for the initial microstructure A at the strain rates above 0.01 s~(-1) was another main factor for flow softening, and the platelet kinking/ bending for the initial microstructure B at all the deformation conditions played an important role in the flow softening, which was also responsible for the larger flow softening effect comparing with the initial microstructure A.
机译:考虑塑性变形热效应和组织演变,研究了具有不同初始组织的Ti-5Al-2Sn-2Zr-4Mo-4Cr的流动软化机理。使用了两种初始微结构:一种具有等轴和细长的初生α晶粒的初始微结构A(MA),以及另一种具有Widmanstaettenα血小板的初始微结构B(MB)。通过计算温度升高来估算绝热塑性变形效应,并使用OM,TEM和EBSD观察其微观结构演变。结果表明,在一定的变形温度和应变速率下,初始微观结构B呈现出比初始微观结构A更高的流动软化效果。对于这两个初始微观结构,塑性变形热效应是在20℃时流动软化的主要因素之一。在0.01 s〜(-1)以上的应变速率下,应变速率大于0.01 s〜(-1),动态恢复控制应变-应力曲线的形状。初始微观结构B在5.0 s〜(-1)应变速率下的流动局部化更加明显,这导致更大的流动软化效果。此外,初始微观结构A在高于0.01 s〜应变速率下的动态再结晶。 (-1)是造成流动软化的另一个主要因素,并且在所有变形条件下初始微观结构B的血小板扭结/弯曲在流动软化中都起着重要作用,这也与流动软化相比具有更大的流动软化作用。初始微观结构

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