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Bounds and self-consistent estimates for elastic constants of random polycrystals with hexagonal, trigonal, and tetragonal symmetries

机译:具有六边形,三角和四边形对称性的随机多晶的弹性常数的界和自洽估计

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摘要

Peselnick, Meister, and Watt have developed rigorous methods for bounding elastic constants of random polycrystals based on the Hashin-Shtrikman variational principles. In particular, a fairly complex set of equations that amounts to an algorithm has been presented previously for rinding the bounds on effective elastic moduli for polycrystals having hexagonal, trigonal, and tetragonal symmetries. A more analytical approach developed here, although based on the same ideas, results in a new set of compact formulas for all the cases considered. Once these formulas have been established, it is then straightforward to perform what could be considered an analytic continuation of the formulas (into the region of parameter space between the bounds) that can subsequently be used to provide self-consistent estimates for the elastic constants in all cases. This approach is very similar in spirit but differs in its details from earlier work of Willis, showing how Hashin-Shtrikman bounds and certain classes of self-consistent estimates may be related. These self-consistent estimates always lie within the bounds for physical choices of the crystal elastic constants and for all the choices of crystal symmetry considered. For cubic symmetry, the present method reproduces the self-consistent estimates obtained earlier by various authors, but the formulas for both bounds and estimates are generated in a more symmetric form. Numerical values of the estimates obtained this way are also very comparable to those found by the Gubernatis and Krumhansl coherent potential approximation (or CPA), but do not require computations of scattering coefficients.
机译:Peselnick,Meister和Watt根据Hashin-Shtrikman变分原理开发了严格的方法来约束随机多晶的弹性常数。特别地,先前已经提出了相当复杂的方程组,其相当于一种算法,用于对具有六边形,三角和四边形对称性的多晶进行有效弹性模量的边界冲洗。尽管基于相同的思想,但此处开发出了一种更具分析性的方法,可针对所有考虑的情况得出一套新的紧凑公式。一旦建立了这些公式,就可以直接执行公式的解析连续化(进入边界之间的参数空间区域),随后可以用来为公式中的弹性常数提供自洽估计。所有情况。这种方法在精神上非常相似,但是其细节与Willis的早期工作有所不同,这说明了Hashin-Shtrikman边界与某些类别的自洽估计之间的关系。对于晶体弹性常数的物理选择和所考虑的所有晶体对称性选择,这些自洽的估计值始终在范围之内。对于三次对称,本方法再现了早些时候由不同作者获得的自洽估计,但是边界和估计的公式均以更对称的形式生成。用这种方法获得的估计值也与古贝纳提斯和克鲁姆汉斯相干势近似(或CPA)发现的值非常可比,但是不需要计算散射系数。

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