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Elastic limit at macroscopic deformation of icosahedral Al-Pd-Mn single quasicrystals

机译:二十面体Al-Pd-Mn单准晶体宏观变形的弹性极限

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Al_(70.5)Pd_(21)Mn_(8.5) single quasicrystals were plastically deformed between 482 and 821℃. The strain rate sensitivity of the flow stress was measured by stress relaxation tests. At several temperatures, the dislocation structures were imaged by diffraction contrast in a high-voltage electron microscope for determining the dislocation densities. At all temperatures, the plastic deformation starts with a range of very high work-hardening. The transition point between almost elastic and elastic-plastic deformation is called the elastic limit. At low temperatures, the deformation was stopped at about 1.5 GPa to prevent fracture. Above about 580℃, the stress-strain curves bend down and show a yield point effect followed by a range of almost steady state deformation. At low temperatures, the elastic limit is much lower than the steady state flow stress or the maximum stresses reached without fracture. The activation parameters are different for the elastic limit, the range of high work-hardening and steady state deformation. The flow stresses are interpreted by the stress necessary to move individual dislocations and the athermal component due to the elastic interaction between dislocations. At low temperatures, a further component is necessary to explain the very high flow stresses reached by work-hardening.
机译:Al_(70.5)Pd_(21)Mn_(8.5)单准晶体在482至821℃之间发生塑性变形。通过应力松弛测试来测量流动应力的应变率敏感性。在几个温度下,通过在高压电子显微镜中的衍射对比对位错结构成像,以确定位错密度。在所有温度下,塑性变形都始于一系列非常高的加工硬化。几乎弹性变形和弹塑性变形之间的过渡点称为弹性极限。在低温下,变形在约1.5 GPa处停止,以防止断裂。在约580℃以上,应力-应变曲线向下弯曲并显示出屈服点效应,随后出现一系列几乎为稳态的变形。在低温下,弹性极限远低于稳态流动应力或达到的最大应力而不会破裂。激活参数因弹性极限,高加工硬化范围和稳态变形而不同。流动应力由移动单个位错和由于位错之间的弹性相互作用而产生的无热成分所必需的应力解释。在低温下,必须使用其他组件来说明加工硬化所达到的很高的流动应力。

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