单晶MnZn铁氧体球面压痕的交叉滑移模式

S.E. Kadijk, A.Broese Van Groenou
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引用次数: 14

摘要

将加载球压痕对MnZn铁氧体晶体变形的实验扩展到(111)面。如前所示,在(001)和(110)平面上,变形由耦合滑移线组成。在< 110 >的Burgers矢量上讨论滑移模式的可能滑移面。在{110}、{111}和{100}滑移系统之间存在交叉滑移的假设下,给出了完整的描述。根据球面加载半空间的弹性方程,计算了分解剪应力(RSS),为分析提供了依据。位错的来源位于RSS最大的地方。假设滑移的传播比成核更容易,考虑了几种耦合滑移(“铅笔滑动”)的情况。通过计算从起点到交叉点之间的表面滑移线的长度,对模型进行了校核。实验数据显示差异很大,但平均而言,它们与模型一致。当RSS足够时,{100}和{111}是主要滑移系统。{100}仅在交叉滑移中被激发,其RSS值与{100}和{111}大致相同。传播停止的RSS分布也很广,为0.6-1.8 GPa,但在{100}处发现最小值。
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Cross-slip patterns by sphere indentations on single crystal MnZn ferrite

The experiments on the deformation of crystals of MnZn ferrite by indentation with a loaded sphere are extended to (111) planes. As shown before on (001) and (110) planes the deformation consists of coupled slip lines. The slip patterns are discussed in terms of the possible slip planes for a Burgers vector along 〈110〉. A complete description is given on the assumption of cross slip between the slip systems, {110}, {111} and {100}. The analysis is supported by calculations of the resolved shear stress (RSS) on the basis of the elastic equations for a halfspace loaded by a sphere. The source of dislocations is located where the RSS is largest. On the assumption that propagation of slip is easier than nucleation, several cases of coupled slip (“pencil glide”) are considered. A check on the model is made by calculating the length of the slip lines on the surface between the start and the cross-over. The experimental data show a wide spread, but on the average they agree with the model. {100} and {111} appear as primary slip systems when the RSS is sufficient. {100} is excited only in cross-slip, at about the same RSS values as for {100} and {111}. The RSS where propagation stops, show a wide spread too, 0.6–1.8 GPa, but the lowest minimum is found for {100}.

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