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Improved bounds on the energy-minimizing strains in martensitic polycrystals

机译:马氏体多晶中能量最小应变的改进界

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This paper is concerned with the theoretical prediction of the energy-minimizing (or recoverable) strains in martensitic polycrystals, considering a nonlinear elasticity model of phase transformation at finite strains. The main results are some rigorous upper bounds on the set of energy-minimizing strains. Those bounds depend on the polycrystalline texture through the volume fractions of the different orientations. The simplest form of the bounds presented is obtained by combining recent results for single crystals with a homogenization approach proposed previously for martensitic polycrystals. However, the polycrystalline bound delivered by that procedure may fail to recover the monocrystalline bound in the homogeneous limit, as is demonstrated in this paper by considering an example related to tetragonal martensite. This motivates the development of a more detailed analysis, leading to improved polycrystalline bounds that are notably consistent with results for single crystals in the homogeneous limit. A two-orientation polycrystal of tetragonal martensite is studied as an illustration. In that case, analytical expressions of the upper bounds are derived and the results are compared with lower bounds obtained by considering laminate textures.
机译:本文考虑了马氏体多晶中能量最小(或可恢复)应变的理论预测,考虑了有限应变下相变的非线性弹性模型。主要结果是在最小化能量的应变集合上有一些严格的上限。这些界限取决于通过不同取向的体积分数的多晶织构。通过将单晶的最新结果与先前针对马氏体多晶提出的均化方法相结合,可获得最简单的边界形式。但是,通过该程序传递的多晶结合物可能无法恢复均质极限中的单晶结合物,如本文通过考虑与四方马氏体有关的示例所证明的那样。这促使人们进行更详细的分析,从而改善了多晶界,这与均质极限内的单晶结果显着一致。以四方马氏体的两向多晶为例进行了研究。在那种情况下,导出上限的解析表达式,并将结果与​​通过考虑层压板纹理获得的下限进行比较。

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