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Thermoelastic Damping in Partially Covered Bilayer Microbeam Resonators with Two-Dimensional Heat Conduction

机译:具有二维热传导的部分覆盖双层微观谐振器的热弹性阻尼

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Thermoelastic damping (TED) has been proved as an intrinsic mechanism of energy dissipation in the microelectromechanical systems (MEMS) resonators. However, the previous TED models developed for the fully covered bilayer beam resonators cannot be used for the partially covered cases. This paper firstly derives an analytical TED model for partially covered bilayer microbeams. The bilayer beam performs small-amplitude vibration in pure bending mode, and the mode shape is achieved from the dynamic of Euler-Bernoulli beam. To obtain the coupled temperature field, Green's functions are utilized to solve the heat conduction along thickness and length directions within the framework of Fourier's law. The expression for TED is derived in the form of an infinite series. The present TED model can reduce to that of a fully covered bilayer beam, and matches well with the finite element method (FEM). The behaviors of TED spectrum are investigated comprehensively. Two comparable Debye peaks are noticed at approximately two corresponding critical frequencies. The partial coating greatly reduces the peak values at high critical frequency, but causes an additional TED peak at low critical frequency. The TED peaks of the coating slightly increase as the length increases. The effects of the length and position of the metal coating on the TED at the fundamental frequency are significant. To reduce TED, the metal coating should be located away from the substrate clamped end. This paper provides a developing methodology for controlling TED. (C) 2020 Elsevier Ltd. All rights reserved.
机译:热弹性阻尼(TED)已被证明是微机电系统(MEMS)谐振器中能量耗散的一种内在机制。然而,以前为完全覆盖的双层梁谐振器开发的TED模型不能用于部分覆盖的情况。本文首先推导了部分覆盖双层微束的TED解析模型。双层梁在纯弯曲模式下进行小振幅振动,振型由Euler-Bernoulli梁的动力学实现。为了获得耦合温度场,在傅里叶定律的框架内,利用格林函数求解沿厚度和长度方向的热传导。TED的表达式是以无穷级数的形式导出的。目前的TED模型可以简化为完全覆盖双层梁的模型,并且与有限元法(FEM)匹配良好。对TED光谱的行为进行了全面的研究。在大约两个相应的临界频率处发现了两个可比较的德拜峰。局部涂层大大降低了高临界频率下的峰值,但在低临界频率下会产生额外的TED峰值。涂层的TED峰随长度的增加略有增加。金属涂层的长度和位置对TED基频的影响是显著的。为了减少TED,金属涂层应远离基材夹紧端。本文提供了一种控制TED的开发方法。(C) 2020爱思唯尔有限公司版权所有。

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