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首页> 外文期刊>Proceedings of the Royal Society. Mathematical, physical and engineering sciences >A 'non-local' variational approach to the elastic energy minimization of martensitic polycrystals
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A 'non-local' variational approach to the elastic energy minimization of martensitic polycrystals

机译:马氏体多晶弹性能最小化的“非局部”变分方法

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摘要

Solid-solid phase transformations in polycrystals are considered in the context of energy minimization. The energy of a single crystal is specified by a non-convex multi-well energy function, in the approximation of infinitesimal deformations. The number of wells corresponds to the number of distinct phases and each is assumed to have the same isotropic elastic modulus. The polycrystal's energy is defined a priori via minimization of the energy functional with proper account of the orientation distribution, with respect to all 'kinematically admissible' displacement fields. A variational principle of Hashin-Shtrikman type is derived for the polycrystal's energy by developing and generalizing the approach of Bruno and co-workers. The variational principle involves a non-local functional with a Green's function-related kernel operating on trial 'transformation fields' which are appropriately constrained to accommodate both the single crystal's constitutive law and the polycrystal's texture. For a statistically uniform polycrystal, the variational principle is reformulated to require minimization with respect to all possible two-point correlation functions of 'submicrostructure', compatible with the texture. This variational principle is applied to derive upper bounds for a statistically uniform polycrystal by employing a 'separation of scales', i.e. by constraining the set of trial fields to those with the property that the scale of the trial submicrostructure is much finer than the scale of the polycrystal's texture. Subsequent optimization with respect to this submicrostructure for each particular orientation reveals a connection with relaxation of a single crystal 'with fixed volume fractions' and associated H-measures as discussed by Kohn. The resulting upper bound is developed and compared with a bound derived by Bruno et al. For some examples the new bound is demonstrated to be sharper than the latter, as a result of an improved optimization procedure. The present approach also extends that of Bruno et al. to more general orientation distribution statistics and clarifies the effect of incompatibility of transformation strains in the single crystals for the overall performance of polycrystals. [References: 34]
机译:在能量最小化的背景下考虑了多晶中的固-固相变。在无穷小变形的近似值中,单晶体的能量由非凸多阱能量函数指定。孔的数量对应于不同相的数量,并且假定每个相具有相同的各向同性弹性模量。相对于所有“运动学上允许的”位移场,通过适当考虑取向分布,通过使能量功能最小化来预先定义多晶的能量。通过发展和推广Bruno及其同事的方法,得出了多晶能量的Hashin-Shtrikman型变分原理。变分原理涉及非本地函数,其中格林函数相关的核在试验的“变换场”上运行,这些“变换场”受到适当约束,以适应单晶的本构律和多晶的织构。对于统计上均一的多晶,重新定义了变分原理,要求对与纹理兼容的“亚微结构”的所有可能的两点相关函数进行最小化。通过采用“比例尺分离”,即通过将一组试验场约束为具有试验亚显微结构的尺寸比其尺寸小得多的特性,可以应用这种变分原理来得出统计上均匀的多晶的上限。多晶的纹理。对于每个特定方向,针对该亚显微结构的后续优化揭示了与单晶“具有固定体积分数”的弛豫和相关的H度量相关的联系,正如Kohn所讨论的。产生的上限被开发并与Bruno等人得出的上限进行比较。对于某些示例,由于改进的优化程序,新边界被证明比后者更清晰。本方法还扩展了Bruno等人的方法。可以得到更一般的取向分布统计数据,并阐明了单晶中相变应变的不相容性对多晶整体性能的影响。 [参考:34]

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