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Dynamic strain aging during the plastic flow of metals

机译:金属塑性流动过程中的动态应变时效

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In the present paper, in order to better understand the third type "dynamic strain aging" occurring during the plastic flow of metals, the uniaxial compressive experimental data ever obtained in University of California, San Diego using an Instron servo-hydraulic testing machine and the Hopkinson technique are systematically analysed. These experimental data cover the plastic flow stress of several fcc, hcp, bcc polycrystalline materials and several alloys at a broad range of temperatures (77K - 1,100K) and strain rates (0.001/s - 10,000/s). In analysis, the appearing region of the "dynamic strain aging " under different temperatures and strain rates are respectively plotted by the curves of stress vs temperature, and stress vs strain for fcc, hcp and bcc metals. The results show that: (1) this third type "dynamic strain aging " occurs in all hcp, bcc and fcc polycrystalline or alloy materials, and there are different profiles of stress-strain curve; (2) the "dynamic strain aging "occurs in a matching coincidence of the temperature and strain rate, its temperature region will shift to higher region with increasing strain rates; (3) bcc materials do not have an initial pre-straining strain as the onset of work-hardness rate change for the "'dynamic strain aging "; and (4) based on the explanations of dynamic strain aging with serration curves (Portevin-Lechatelier effect) and other explaining mechanisms of references, The mechanism of third DSA is thought as the rapid/continuous formation of the solute atmospheres at the mobile dislocation core by the pipe diffusion along vast collective forest dislocations to result in a continuous rise curve of flow stress. Finally, several conclusions are also presented.
机译:在本文中,为了更好地理解在金属塑性流动过程中发生的第三种“动态应变时效”,曾在加利福尼亚大学圣地亚哥分校使用Instron伺服液压测试机获得了单轴压缩实验数据。对霍普金森技术进行了系统分析。这些实验数据涵盖了多种fcc,hcp,bcc多晶材料和几种合金在很宽的温度范围(77K-1,100K)和应变速率(0.001 / s-10,000 / s)下的塑性流动应力。在分析中,分别通过应力与温度以及fcc,hcp和bcc金属的应力与应变曲线绘制了在不同温度和应变速率下“动态应变时效”的出现区域。结果表明:(1)在所有hcp,bcc和fcc多晶或合金材料中均发生这种第三种“动态应变时效”,并且应力-应变曲线具有不同的轮廓; (2)“动态应变时效”发生在温度和应变率的同时,其温度区域随着应变率的增加而向较高的区域移动。 (3)密件抄送材料没有初始的预应变,因为“动态应变时效”使工作硬度发生变化。 (4)基于带有锯齿曲线的动态应变时效的解释(Portevin-Lechatelier效应)和其他参考机理的解释,第三次DSA的机理被认为是在移动位错中心快速/连续形成溶质气氛。沿集体森林错位的管道扩散导致流动应力的连续上升曲线。最后,还提出了一些结论。

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