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Numerical implementation of a 3D continuum theory of dislocation dynamics and application to micro-bending

机译:位错动力学的3D连续体理论的数值实现及其在微弯中的应用

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Crystal plasticity is governed by the motion of lattice dislocations. Although continuum theories of static dislocation assemblies date back to the 1950s, the line-like character of these defects posed serious problems for the development of a continuum theory of plasticity which is based on the averaged dynamics of dislocation systems. Only recently the geometrical problem of performing meaningful averages over systems of moving, oriented lines has been solved. Such averaging leads to the definition of a dislocation density tensor of second order along with its evolution equation. This tensor can be envisaged as the analogue of the classical dislocation density tensor in an extended space which includes the line orientation as an independent variable. In the current work, we discuss the numerical implementation of a continuum theory of dislocation evolution that is based on this dislocation density measure and apply this to some simple benchmark problems as well as to plane-strain micro-bending.
机译:晶体可塑性受晶格位错运动的支配。尽管静态位错组件的连续理论可以追溯到1950年代,但这些缺陷的线状特征为基于连续位错系统平均动力学的可塑性连续性理论的发展提出了严重的问题。直到最近,才解决了在移动的,定向的线的系统上执行有意义的平均的几何问题。这种平均导致对第二级位错密度张量及其演化方程的定义。该张量可被设想为扩展空间中经典位错密度张量的类似物,该扩展空间包括线方向作为自变量。在当前的工作中,我们讨论了基于位错密度测度的位错演化连续理论的数值实现,并将其应用于一些简单的基准问题以及平面应变的微弯曲。

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