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Novel Cross-Slip Mechanism of Pyramidal Screw Dislocations in Magnesium

机译:镁合金中锥体锥状错位的新型错位机制

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摘要

Compared to cubic metals, whose primary slip mode includes twelve equivalent systems, the lower crystalline symmetry of hexagonal close-packed metals results in a reduced number of equivalent primary slips and anisotropy in plasticity, leading to brittleness at the ambient temperature. At higher temperatures, the ductility of hexagonal close-packed metals improves owing to the activation of secondary < c + a > pyramidal slip systems. Thus, understanding the fundamental properties of corresponding dislocations is essential for the improvement of ductility at the ambient temperature. Here, we present the results of large-scale ab initio calculations for < c + a > pyramidal screw dislocations in magnesium and show that their slip behavior is a stark counterexample to the conventional wisdom that a slip plane is determined by the stacking fault plane of dislocations. A stacking fault between dissociated partial dislocations can assume a nonplanar shape with a negligible energy cost and can migrate normal to its plane by a local shuffling of atoms. Partial dislocations dissociated on a {2 (1) over bar(1) over bar2} plane "slither" in the {01 (1) over bar1} plane, dragging the stacking fault with them in response to an applied shear stress. This finding resolves the apparent discrepancy that both {2 (1) over bar(1) over bar2} and {01 (1) over bar1} slip traces are observed in experiments while ab initio calculations indicate that dislocations preferably dissociate in the {2 (1) over bar(1) over bar2} planes.
机译:相较于立方晶金属,其主要滑模包含十二个等效体系,六方密堆积金属的较低晶体对称性导致等效滑模数量减少和塑性各向异性,导致环境温度下的脆性。在较高的温度下,六角形密堆积金属的延展性由于次级锥体滑移系统的激活而提高。因此,了解相应位错的基本性质对于改善环境温度下的延展性至关重要。在这里,我们介绍了镁中锥形螺旋位错的大规模从头算计算结果,并表明它们的滑移行为与常规观点完全相反,该传统观点认为,滑移平面由硅的堆积断层确定脱臼。离解的部分位错之间的堆垛层错可以假定为非平面形状,能量成本可以忽略不计,并且可以通过原子的局部改组垂直于其平面迁移。在bar1}平面上的{01(1)上,bar2}平面上的“ barter”上的bar(1)上的{2(1)上的部分位错被解离,响应于所施加的剪切应力,与它们一起拖移堆垛层错。这一发现解决了明显的差异,即在实验中观察到{2(1)在bar(1)在bar2}和{01(1)在bar1}的滑动轨迹上,而从头算计算表明位错最好在{2( 1)在bar(1)在bar2}平面上。

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  • 来源
    《Physical review letters》 |2016年第22期|225501.1-225501.5|共5页
  • 作者单位

    Japan Atom Energy Agcy, Ctr Computat Sci & E Syst, 178-4-4 Wakashiba, Kashiwa, Chiba 2770871, Japan;

    Japan Atom Energy Agcy, Ctr Computat Sci & E Syst, 2-4 Shirakata Shirane, Tokai, Ibaraki 3191195, Japan;

    Japan Atom Energy Agcy, Ctr Computat Sci & E Syst, 2-4 Shirakata Shirane, Tokai, Ibaraki 3191195, Japan;

    Japan Atom Energy Agcy, Nucl Sci & Engn Ctr, 2-4 Shirakata Shirane, Tokai, Ibaraki 3191195, Japan;

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