初始张力作用下非对称层状压电板大挠度非线性几何响应

Chun‐Fu Chen, I-Wei Li
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引用次数: 0

摘要

研究了非对称压电层状板在初始张力作用下的大挠度非线性几何响应。利用冯·卡门板大挠度理论,并将其推广到含压电层的非对称层状板。首先,导出了非线性控制方程的无量纲形式,即侧向坡度和径向合力。利用问题的端固边界条件和迭代过程,以相应的侧向斜率线性解析解作为初始猜想,用数值有限差分法求解了这些方程。对于一个早期的单片板,在一个非常低的施加电压下,结果与文献中由于均匀横向载荷的单层情况的可用解决方案很好地一致,因此本方法是有效的。对于典型硅基材料制成的双层非对称板,结果表明,只有在中等初始张力和中等侧压力下,压电效应才会明显。在这种情况下,施加电压越高,中心偏转越大;因此,该板可以在相对低的预张力条件下过渡到膜上。然而,对于较高的预紧力或较大的侧向载荷,压电效应变得微不足道。此外,无论施加电压的大小如何,初始张力和横向载荷的影响可能合并成为主导,产生几乎相同的响应。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Nonlinear geometrical responses in large deflection of un-symmetrically layered piezo-electric plate under initial tension
The nonlinear geometrical responses in large deflection of an un-symmetrically piezo-electric layered plate under initial tension are studied. von Karman plate theory for large deflection is utilized and extended to an un-symmetrically layered plate including a piezoelectric layer. The nonlinear governing equations are derived, first, in a non-dimensional form in terms of lateral slope and radial force resultant. These equations are solved u sin g a numerical finite difference method with the aid of the clamped-ended boundary conditions of the problem and an iteration procedure, by taking the associated linear analytical solution of lateral slope as the initial guess. For an early monolithic plate under a very low applied voltage, the results agree well with available solutions for a single-layered case due to uniform lateral load in literature and thus the present approach is validated. For a two-layered un-symmetric plate made of typical silicon-based materials, the results show that piezoelectric effect seems to be apparent only up to a moderate initial tension and a moderate lateral pressure. Under this circumstance, the higher the applied voltage, the greater the central deflection; and hence the plate may transit to a membrane in a relatively low pretension condition. For a relatively high pretension or a severe lateral load, however, the piezoelectric effect becomes insignificant. Moreover, the effects of initial tension and lateral load may merge to become dominant, yielding nearly the same responses, regardless of the magnitude of the applied voltage.
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