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非均匀材料细观结构的定向分布函数(Ⅰ)——定向分布函数和不可约张量

郑泉水 邹文楠

郑泉水, 邹文楠. 非均匀材料细观结构的定向分布函数(Ⅰ)——定向分布函数和不可约张量[J]. 应用数学和力学, 2001, 22(8): 773-789.
引用本文: 郑泉水, 邹文楠. 非均匀材料细观结构的定向分布函数(Ⅰ)——定向分布函数和不可约张量[J]. 应用数学和力学, 2001, 22(8): 773-789.
ZHENG Quan-shui, ZOU Wen-nan. Orientation Distribution Functions for Microstructures of Heterogeneous Materials(Ⅰ)-Directional Distribution Functions and Irreducible Tensors[J]. Applied Mathematics and Mechanics, 2001, 22(8): 773-789.
Citation: ZHENG Quan-shui, ZOU Wen-nan. Orientation Distribution Functions for Microstructures of Heterogeneous Materials(Ⅰ)-Directional Distribution Functions and Irreducible Tensors[J]. Applied Mathematics and Mechanics, 2001, 22(8): 773-789.

非均匀材料细观结构的定向分布函数(Ⅰ)——定向分布函数和不可约张量

基金项目: 国家自然科学基金资助项目(19525207;19891180);霍英东教育基金会资助项目
详细信息
    作者简介:

    郑泉水(1961- ),男,江西人,教授,博士,教育部长江特聘教授.

  • 中图分类号: O331

Orientation Distribution Functions for Microstructures of Heterogeneous Materials(Ⅰ)-Directional Distribution Functions and Irreducible Tensors

  • 摘要: 在最近研究非均匀材料的物理和力学性质的各种基于细观力学的方法中,定向分布函数(ODF)和晶体定向分布函数(CODF)的概念起着重要的作用,它们分别定义在单位球面和旋转群上.本文通过两部分的内容,用具有不可约张量系数的傅立叶展开对它们分别作了深入的研究.群表示理论指出平方可积的定向分布函数可以展开为球谐函数的绝对收敛的傅立叶级数,而其中的球谐函数又能进一步用不可约张量表示.这样一些不可约张量系数的基本重要性在于它们刻划了材料组元和缺陷的体积、形状、相、位置的宏观或全局影响.第(Ⅰ)部分对定义在N维单位球上的定向分布函数的不可约张量Fourier展开的一般性质进行了研究,其中重点是构造二维和三维不可约张量的简单表示,以便于得到它们在各种点群(完全正交群的子群)对称性的约束形式;第(Ⅱ)部分给出了晶体定向分布函数的不可约张量展开的显式表示,并且给出了不可约张量以及定向分布函数和晶体定向分布函数不可约张量展开在各种点群下的约束形式.
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出版历程
  • 收稿日期:  2000-10-09
  • 修回日期:  2001-03-20
  • 刊出日期:  2001-08-15

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