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Formulation and characterization of a continuous crystal lattice orientation finite element method (LOFEM) and its application to dislocation fields

机译:连续晶格取向有限元法(LOFEM)的制定,表征及其在位错场中的应用

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Since the 1950s, a large body of work has been published on connecting the curvature of a crystal lattice to geometrically necessary dislocations densities of a crystal lattice. Studying dislocation transmission through grains and across their boundaries requires the lattice curvature to be preserved. However, traditional crystal plasticity models and their numerical implementations do not formally preserve lattice curvature. In this paper, a continuous crystal lattice orientation finite element method (LOFEM) is proposed to rectify this impediment to the inclusion of dislocation-based constitutive models. The methodology is first presented, and then it is demonstrated for tension and compression deformations of a copper polycrystal. It is shown that under the same deformation histories, the lattice continuity constraint alters the evolving state in comparison to the traditional approach, including retarding the rate at which the crystallographic texture strengthens under monotonic deformation. Taking advantage of the finite element representation of the lattice orientation, the Nye tensor is computed on lattices misoriented by deformation and is subsequently used to compute evolving dislocation density distributions. (C) 2019 Elsevier Ltd. All rights reserved.
机译:自1950年代以来,关于将晶格的曲率与晶格的几何必要位错密度联系起来的大量工作已经出版。研究通过晶粒并跨越其边界的位错传输需要保留晶格曲率。但是,传统的晶体可塑性模型及其数值实现并未正式保留晶格曲率。本文提出了一种连续晶格取向有限元方法(LOFEM),以纠正这一障碍,包括基于位错的本构模型。首先介绍了该方法,然后论证了铜多晶体的拉伸和压缩变形。结果表明,在相同的变形历史下,与传统方法相比,晶格连续性约束会改变其演化状态,包括阻碍晶体结构在单调变形下的强化速率。利用晶格取向的有限元表示,在因变形而错位的晶格上计算Nye张量,然后将其用于计算演化的位错密度分布。 (C)2019 Elsevier Ltd.保留所有权利。

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