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ORIENTATION DISTRIBUTION FUNCTIONS FOR MICROSTRUCTURES OF HETEROGENEOUS MATERIALS (Ⅰ)-DIRECTIONAL DISTRIBUTION FUNCTIONS AND IRREDUCIBLE TENSORS

机译:异质材料微观结构的方向分布函数(Ⅰ)-方向分布函数和不可约张量

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In this two-part paper, a thorough investigation is made on Fourier expansions with irreducible tensorial coefficients for orientation distribution functions (ODFs) and crystal orientation distribution functions (CODFs), which are scalar functions defined on the unit sphere and the rotation group, respectively. Recently it has been becoming clearer and clearer that concepts of ODF and CODF play a dominant role in various micrornechanically-based approaches to mechanical and physical properties of heterogeneous materials. The theory of group representations shows that a square integrable ODF can be expanded as an absolutely convergent Fourier series of spherical harmonics and these spherical harmonics can further be expressed in terms of irreducible tensors. The fundamental importance of such irreducible tensorial coefficients is that they characterize the macroscopic or overall effect of the orientation distribution of the size, shape, phase, position of the material constitutions and defects. In Part (Ⅰ), the investigation about the irreducible tensorial Fourier expansions of ODFs defined on the N-dimensional (N-D) unit sphere is carried out. Attention is particularly paid to constructing simple expressions for 2- and 3-D irreducible tensors of any orders in accordance with the convenience of arriving at their restricted forms imposed by various point-group (the synonym of subgroup of the full orthogonal group) symmetries. In the continued work - Part (Ⅱ), the explicit expression for the irreducible tensorial expansions of CODFs is established.The restricted forms of irreducible tensors and irreducible tensorial Fourier expansions of ODFs and CODFs imposed by various point-group syrnmetries are derived.
机译:在这个由两部分组成的论文中,对具有不可约张量系数的定向分布函数(ODF)和晶体定向分布函数(CODF)的傅里叶展开进行了深入研究,它们分别是在单位球体和旋转组上定义的标量函数。 。最近,越来越清楚的是,ODF和CODF的概念在各种基于微机械的方法中对异质材料的机械和物理特性起着主导作用。群表示理论表明,平方可积ODF可以作为绝对收敛的球谐函数的傅里叶级数展开,并且这些球谐函数可以进一步用不可约张量表示。这种不可还原的张量系数的根本重要性在于,它们表征了材料成分和缺陷的尺寸,形状,相,位置的取向分布的宏观或整体影响。在第一部分中,对在N维(N-D)单位球面上定义的ODF的不可约张量傅里叶展开进行了研究。特别要注意的是,为了方便获得由各种点群(完全正交群的子群的同义词)所施加的限制形式的便利性,为任何阶数的2和3D不可约张量构造简单表达式。在续篇(二)中,建立了CODF不可约张量展开的明确表示,并推导了ODF和CODF的不可约张量和不可约张量傅里叶展开的受限形式。

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