Ni3(Si,Ti)单晶的塑性流动

T. Takasugi, S. Watanabe, O. Izumi, N.K. Fat-Halla
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引用次数: 37

摘要

通过压缩试验测量了l12型Ni3(Si, Ti)的流变应力随温度、应变速率、取向和合金成分的变化规律。随着温度的升高,临界分解剪应力(CRSS)从77 K开始逐渐升高,达到峰值后迅速下降。取向接近[011]和[1̄11]的单晶在峰值温度以下表现出八面体滑移(111)[1̄01],在峰值温度以上表现出立方滑移(001)[1̄10],而取向接近[001]的单晶在整个温度范围内表现出八面体滑移{111}。CRSS在峰值温度以下取决于取向和合金成分,而在峰值温度以上取决于取向和应变速率。峰值温度与取向有关,但与应变速率和合金成分无关。结果表明,Ni3(Si, Ti)单晶的变形机制与Ni3Al、Ni3Ga和Ni3Ge等其他ni基L12单晶的变形机制非常相似;在低温下,与APB在(111)平面上解离的超偏位运动通过向(001)平面的微交叉滑移而变得坚固。在高温下,根据取向的不同,有两种变形模式。取向远离[001]的单晶的变形是由于(001)[1̄10]滑移的Peierls-Nabarro机制造成的,而取向接近[001]的单晶的变形是由于(111)[1̄01]滑移的“扩散”过程的侵入造成的。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Plastic flow of Ni3(Si,Ti) Single crystals

The flow stress of L12-type Ni3(Si, Ti) by the compression test was measured as a function of temperature, strain rate, orientation and alloy composition. The critical resolved shear stress (CRSS) increased from 77 K, reached a peak, and then decreased rapidly with increasing temperature. The single crystals with orientations close to [011] and [1&#x0304;11] showed the operations of octahedral slips (111) [1&#x0304;01] below the peak temperature and of cube slips (001) [1&#x0304;10] above the peak temperature, whereas those with orientation close to [001] showed the operations of octahedral slips {111} over the entire temperatures. The CRSS depended on the orientation and alloy composition below the peak temperature but on the orientation and the strain rate above the peak temperature. The peak temperature was dependent on the orientation but almost independent of the strain rate and alloy composition. It is suggested that the deformation mechanisms for Ni3(Si, Ti) single crystals are quite similar to those for other Ni-based L12 single crystals such as Ni3Al, Ni3Ga and Ni3Ge; at low temperatures the dislocation movement of the superpartials dissociated on (111) plane with APB became sessile by micro cross slip to (001) plane. At high temperatures, two deformation modes were operative, depending on the orientation. The deformation of the single crystals with orientations far from [001] is due to the Peierls-Nabarro mechanism of (001) [1&#x0304;10] slip, whereas the deformation of the single crystals with orientations close to [001] is due to the intrusion of the “diffusive” process of (111) [1&#x0304;01] slip.

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