Quasi-static model of microelectromechanical cantilever

A. Lai, A.A. Rahman, W. Wong
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Abstract

The modeling of the microelectromechanical cantilever is governed by the Navierpsilas equation for elasticity and the Maxwellpsilas equation for electrostatic. The computational analysis comprised of the electrostatic analysis and the mechanical analysis [1]. The electric field is derived from the potential difference between the cantilever and the ground (reference plate). The surface force due to the potential difference is then fed to the mechanical analysis module to compute the deformation of the micromechanical structure. The analysis is done iteratively until an equilibrium state is reached. The deformation of the micromechanical structure as gives rise to the redistribution of the electric charges on the surface of the structure, hence a change in the electric field. Deformation of the microelectromechanical structure as well as the redistribution of the electric charges requires a re-meshing of the domains after each iterative step. The proposed model adopts an uncoupled quasi-static approach together with a dasiamoving meshpsila algorithm. The model is used to simulate the reaction of the cantilever due to the change in the electric field.
微机电悬臂梁的准静态模型
采用Navierpsilas弹性方程和Maxwellpsilas静电方程对微机电悬臂梁进行建模。计算分析包括静电分析和力学分析两部分。电场是由悬臂梁和地面(基准板)之间的电位差导出的。然后将由电位差产生的表面力输入到力学分析模块,以计算微机械结构的变形。分析迭代进行,直到达到平衡状态。微观机械结构的变形引起结构表面电荷的重新分布,从而引起电场的变化。微机电结构的变形以及电荷的重新分布需要在每个迭代步骤后重新划分域。该模型采用一种非耦合的准静态方法和一种移动网格算法。该模型用于模拟悬臂梁在电场变化下的反作用力。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
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