金属和合金中理论应变引起的弹性异常

J. Marschall, F. Milstein
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引用次数: 4

摘要

晶体的理论大应变弹性响应一直是人们感兴趣的课题。尽管在各种理论计算中使用了各种原子模型,但在很大程度上被忽略的考虑因素是当布里渊区边界由于变形而与费米表面接触时发生的异常应力和弹性模量变化。目前的工作合理化了BCC和FCC晶体轴向载荷的这些现象。针对(100)单轴加载的具体情况,进行了各种伪势模型的计算。其中q为倒易晶格向量,kf为费米波数,lambda 1为(100)载荷中的轴向拉伸,z为价态,结果总结为lambda 1(即λ 1在q=2kf处)对z的“临界值”图。还给出了Al在q至2kf时弹性模量Cij的伪势模型计算示例。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Theoretical strain-induced elastic anomalies in metals and alloys
The theoretical large-strain elastic response of crystals has long been a subject of interest. Although various atomic models have been used in a variety of theoretical computations, considerations that have largely been neglected are the anomalous stress and elastic moduli variations that occur when a Brillouin zone boundary is brought into contact with the Fermi surface as a result of deformation. The present work rationalises these occurrences for axial loadings of BCC and FCC crystals. Various pseudopotential model computations are carried out for the specific case of (100) uniaxial loading. With q a reciprocal lattice vector, kf the Fermi wavenumber, lambda 1 the axial stretch in (100) loading and z the valence, the results are summarised as plots of the 'critical value' of lambda 1 (i.e. lambda 1 at q=2kf) against z. Examples of pseudopotential model computations of the elastic moduli Cij of Al as q to 2kf are also presented.
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