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Dynamic Electromechanical Coupling of Piezoelectric Bending Actuators

机译:压电弯曲执行器的动态机电耦合

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摘要

Electromechanical coupling defines the ratio of electrical and mechanical energy exchanged during a flexure cycle of a piezoelectric actuator. This paper presents an analysis of the dynamic electromechanical coupling factor (dynamic EMCF) for cantilever based piezoelectric actuators and provides for the first time explicit expressions for calculation of dynamic EMCF based on arrangement of passive and active layers, layer geometry, and active and passive materials selection. Three main cantilever layer configurations are considered: unimorph, dual layer bimorph and triple layer bimorph. The actuator is modeled using standard constitutive dynamic equations that relate deflection and charge to force and voltage. A mode shape formulation is used for the cantilever dynamics that allows the generalized mass to be the actual mass at the first resonant frequency, removing the need for numerical integration in the design process. Results are presented in the form of physical insight from the model structure and also numerical evaluations of the model to provide trends in dynamic EMCF with actuator design parameters. For given material properties of the active and passive layers and given system overall damping ratio, the triple layer bimorph topology is the best in terms of theoretically achievable dynamic EMCF, followed by the dual layer bimorph. For a damping ratio of 0.035, the dynamic EMCF for an example dual layer bimorph configuration is 9% better than for a unimorph configuration. For configurations with a passive layer, the ratio of thicknesses for the passive and active layers is the primary geometric design variable. Choice of passive layer stiffness (Young’s modulus) relative to the stiffness of the material in the active layer is an important materials related design choice. For unimorph configurations, it is beneficial to use the highest stiffness possible passive material, whereas for triple layer bimorph configurations, the passive material should have a low stiffness. In all cases, increasing the transverse electromechanical coupling coefficient of the active material improves the dynamic EMCF.
机译:机电耦合限定了在压电致动器的挠曲循环期间交换的电能和机械能的比率。本文对悬臂压电致动器的动态机电耦合系数(dynamic EMCF)进行了分析,并首次提供了基于无源和有源层的排列,层的几何形状以及有源和无源材料的动态EMCF的显式表达式。选择。考虑了三种主要的悬臂层配置:单晶,双层双晶和三层双晶。使用标准的本构动力学方程对执行器进行建模,该方程将偏转和电荷与力和电压相关联。模态公式用于悬臂动力学,使广义质量成为第一共振频率下的实际质量,从而消除了设计过程中数值积分的需要。结果以物理洞察力的形式从模型结构中呈现出来,并以模型的数值评估形式呈现,以提供带有执行器设计参数的动态EMCF趋势。对于给定的有源和无源层材料属性以及给定的系统整体阻尼比,就理论上可实现的动态EMCF而言,三层双压电晶片拓扑是最佳的,其次是双层双压电晶片。对于0.035的阻尼比,示例双层双压电晶片配置的动态EMCF比单压电晶片配置好9%。对于具有无源层的配置,无源层和有源层的厚度比是主要的几何设计变量。相对于有源层中材料刚度的被动层刚度(杨氏模量)的选择是与材料相关的重要设计选择。对于单压电晶片配置,最好使用尽可能高的刚度被动材料,而对于三层双压电晶片配置,被动材料应具有较低的刚度。在所有情况下,增加活性材料的横向机电耦合系数都会改善动态EMCF。

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