纳米复合材料弹性性能微力学估计的等效包合法

L. Dormieux, E. Lemarchand, S. Brisard
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引用次数: 2

摘要

摘要非均质介质的经典细观力学方法假定相之间有完美的结合,这意味着位移和应力矢量在相之间的界面上是连续的。当涉及纳米包裹体时,必须考虑局部平衡中的应力矢量不连续。在此框架下,本文导出了考虑这些表面应力的Lippmann-Schwinger (L-S)方程的近似解。这种方法建议引入等效粒子的概念,将粒子与周围的界面结合起来,这可以直接在任何标准的均质化过程中实现,例如Mori-Tanaka方案。推导了球形夹杂物等效粒子刚度张量的解析表达式,适用于各种形状和尺寸的纳米夹杂物。最后,基于能量的分析证明了在给定体积下,如何控制弹性性能的急剧增加。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Equivalent Inclusion Approach for Micromechanics Estimates of Nanocomposite Elastic Properties
AbstractClassical micromechanics approaches for heterogeneous media assume perfect bonding between phases, implying that both displacement and stress vectors are continuous across the interface between the phases. When nanoinclusions are involved, a stress vector discontinuity in the local equilibrium has to be accounted for. In this framework, this paper derives an approximate solution of the Lippmann-Schwinger (L-S) equation, which accounts for these surface stresses. This approach suggests introducing the concept of an equivalent particle that combines the particle with the surrounding interface, which can be directly implemented in any standard homogenization procedure, such as the Mori-Tanaka scheme. Analytical expressions for the stiffness tensor of the equivalent particle is derived for spheroidal inclusions, accounting for a wide range of nanoinclusion shapes and dimensions. Finally, an energy-based analysis proves how the dramatic increase of the elastic properties is controlled, for a given volu...
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