Pillai Minu A, Ebenezer D D, Deenadayalan Ezhilarasi
Department of Instrumentation and Control Engineering, National Institute of Technology, Tiruchirappalli 620015, Tamil Nadu, India.
Naval Physical and Oceanographic Laboratory, Kochi 682021, Kerala, India.
J Acoust Soc Am. 2017 Aug;142(2):718. doi: 10.1121/1.4996852.
A model is presented of a composite beam with one elastic and one piezoelectric layer. A reduced set of piezoelectric equations of state that has only the longitudinal components of stress and strain and the transverse components of electric field and charge density is consistently used to include the effect of piezoelectric coupling in all the equations. The equi-potential boundary conditions on the electrodes, the open-circuit condition, and the Gauss condition are satisfied. The position of the neutral axis and the dynamic equilibrium equation are derived after including the effect of piezoelectric coupling. All equations are combined to derive an equation of motion that contains only the displacement and the mechanical excitation. The solution to the equation is expressed in terms of a complete set of functions and an auxiliary function that contains the electric potential. The latter is needed to satisfy piezoelectric boundary conditions at the ends of the beam. The electric potential varies along the length of the beam and has a quadratic variation between the electrodes. Analytical expressions for displacement and potential, and numerical results at low frequencies and in the neighborhood of resonance, are presented for certain sets of boundary conditions.
本文提出了一种由一个弹性层和一个压电层组成的复合梁模型。始终使用一组简化的压电状态方程,该方程仅包含应力和应变的纵向分量以及电场和电荷密度的横向分量,以便在所有方程中纳入压电耦合效应。满足电极上的等电位边界条件、开路条件和高斯条件。在考虑压电耦合效应后,推导出中性轴的位置和动态平衡方程。将所有方程组合起来,得到一个仅包含位移和机械激励的运动方程。该方程的解用一组完备函数和一个包含电势的辅助函数表示。后者是满足梁端部压电边界条件所必需的。电势沿梁的长度变化,在电极之间呈二次变化。针对某些边界条件集,给出了位移和电势的解析表达式以及低频和共振附近的数值结果。