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Homogenization of microsystem interconnects based on micropolar theory and discontinuous kinematics

机译:基于微极理论和不连续运动学的微系统互连的均质化

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In the present paper, the homogenized mechanical response of an interface in a microsystem interconnection is established on the basis of micropolar theory. The interface is treated as a finite RVE (representative volume element), across which macroscopic discontinuities occur as expressed in terms of the regularized discontinuous displacement and rotation fields. For the microstructure within the interfacial RVE, the micro-macro kinematical coupling is introduced as a second-order Taylor series expansion, along with a fluctuation term representing the microscopic displacement variation. In the second-order term of the expansion a restriction for the curvature is made, which motivates the adopted micropolar kinematics. Explicit expressions for the homogenized traction vector and the couple stress traction, associated with displacement and rotational jumps across the interface surface, are derived. A planar elastic interface is subjected to three basic deformation modes, i.e. the standard modes Ⅰ, Ⅱ and a non-conventional rotation mode, which are considered in the numerical examples representing a typical interconnect. A comparison to the results from the Taylor assumption is made, which shows that the Taylor assumption method produces an overstiffening of the interface.
机译:在本文中,基于微极性理论建立了微系统互连中界面的均质机械响应。该界面被视为有限的RVE(代表性体积元素),在其上会出现宏观的不连续性,用正规化的不连续位移和旋转场表示。对于界面RVE内的微观结构,引入了微宏观运动学耦合作为二阶泰勒级数展开,以及表示微观位移变化的波动项。在扩展的二阶项中,对曲率进行了限制,这激发了所采用的微极运动学。推导了均质化牵引力矢量和耦合应力牵引力的显式表达式,这些表达式与跨界面表面的位移和旋转跳跃有关。平面弹性界面经受三种基本变形模式,即标准模式Ⅰ,Ⅱ和非常规旋转模式,在代表典型互连的数值示例中考虑了这种模式。与泰勒假设的结果进行了比较,这表明泰勒假设方法会产生界面的过硬。

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