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具损伤压电层合微梁的坍塌特性研究

发布时间: 2022-10-29 08:30:05 来源:网友投稿


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摘 要:以压电层合微梁为研究对象,基于连续介质力学理论和Euler-Bernoulli梁理论,在考虑其尺寸效应和损伤效应的情况下,推导了具损伤压电层合微梁的非线性动力控制方程.采用伽辽金法和龙格库塔法进行求解,分析了多种参数对微梁结构坍塌特性的影响.结果表明,考虑几何非线性项使得损伤微梁具有更高的坍塌阈值电压;控制电压、微梁长度等参数的变化均对损伤微梁的坍塌阈值电压造成影响.最后,采用有限元软件进行仿真模拟计算,验证了理论计算结果的合理性.本文所得结论对微机电系统压电层合微梁结构的设计具有理论指导意义.

关键词:压电效应;层合微梁;损伤效应;尺寸效应;坍塌

中图分类号:O345 文献标识码:A

Abstract:The nonlinear pull-in behavior of piezoelectric laminated micro-beam was studied with consideration of the size effect and damage effect. Based on the theories of continuum mechanics and Euler-Bernoulli beam hypothesis, the nonlinear governing equation of piezoelectric laminated micro-beam with damage was established and solved in Galerkin method and Runge-Kutta method. The influence of various parameters on the pull-in voltage of the micro-beam was discussed, and the results have shown that the geometry nonlinearity can improve the value of critical pull-in voltage of the micro-beam; the changes of governing voltage, micro-beam length and other parameters have influences on the critical pull-in voltage of the micro-beam. Besides,the FEM software was used to carry out the check-up calculations, and the results were compared with the theoretical results. The findings of this research can offer guidance to the design of micro-structures.

Key words: miezoelectric effect; laminated micro-beam; damage effect; size effect; pull-in

MEMS作为智能化和集成化的微型系统在物理、生物、机械等多个行业中广泛运用.MEMS具有多种结构形式,其中压电微结构由于压电特性在MEMS结构中具有重要地位.一种主要的压电梁式微结构形式就是将压电片通过粘结剂粘结在弹性基体而形成层合压电微梁.层合压电微梁可作为执行器和传感器两种功能结构[1],研究层合压电微梁在电场中的力学特性具有重要的意义.

近年来国内外已有许多学者对梁式微结构在电场中的静动力特性进行研究.Pamidighantam等[2]基于Euler-Bernoulli梁理论研究了两端固支和悬臂结构形式压电微梁的静、动力学特性,并得到了微梁结构的静力坍塌阈值电压.Younis和Nayfeh[3]研究了电场作用下梁式微结构谐振器的响应特性.Chaterjee和Pohit[4]分析了几何非线性对微梁结构临界坍塌电压的影响.徐琳[5]在忽略边缘效应影响的情况下分别研究了平行板式微梁结构的坍塌行为和扭转式微执行器的坍塌行为.对于压电式微梁的研究,Yin等[6]采用修正偶应力理论研究了尺度效应对压电微梁的临界坍塌电压的影响.Azizi等[7]研究了上下两侧附有压电层对微梁静动力稳定性的影响.Vahdat等[8]研究了热弹性阻尼对上下表面附有压电层微梁结构的动力学特性的影响.陈昌萍等[9]通过引入参数剥离数研究了压电粘弹性微梁的粘附特征.Xiao等[10]建立压电层合微梁的尺寸效应通用模型,并使用修正偶应力理论和汉密尔顿原理分析了层合压电微梁的坍塌现象.以上所述的研究中,研究对象大多选取理想的、无缺陷的微梁结构,而对以具损伤微梁结构为对象的研究成果很少见.本文在考虑尺寸效应的情况下,研究具损伤层合压电微梁在电场作用中的坍塌特性,并讨论几何参数、控制电压等对临界坍塌电压的影响.

1 基本方程

2 结果与讨论

在本文算例中,选取微梁长度L=100 μm,压电层厚度hp=0.5 μm,基体层厚度hb=3 μm,梁宽度b=15 μm,悬臂梁与固定电极初始间距d=1 μm.

使用龙格库塔法求解无量纲常微分动力控制方程(12),得到几何非线性对微梁挠度的影响如图2所示.从图2中可知,随着负载电压的增加,微梁挠度随之增大,并当电压值超过临界坍塌电压以后,微梁的挠度变化不再稳定,并发生坍塌;几何非线性对压电微梁挠度变化趋势没有显著影响,但是可以减缓微梁的挠度变化趋势,使微梁临界坍塌电压增大.

3 有限元仿真计算

为了与理论计算结果进行对比分析,本文采用有限元软件ANSYS对悬臂压电层合微梁在静电场中的坍塌行为进行计算.在有限元计算中采用与数值分析中一致的微梁参数,并采用方程(6)和(7)中的等效弹性模量来考虑微梁尺寸效应和损伤的影响.微梁的有限元模型如图6所示,在压电层与静电层的接触面添加界面,通过界面在不同的分析场中传递载荷.对悬臂梁固定端的节点进行完全约束,真空介质层约束下端z方向自由度.为了避免加载过程电压冲击对坍塌的影响,采用斜坡负载方式对微梁施加电压.在求解过程中开启网格变形控制,保证单元的变形与结构场的变形同步.图7显示了V=40 V时微梁的挠度云图.微梁的右侧挠度最大,与固定极板接触的空气间隙变形小,真空介电层下端挠度为零,与理论相符合.

在其他条件均不变的情况下,记录不同负载电压下微梁自由端的挠度值可得出层合压电微梁的挠度与电压关系的曲线如图8所示.由图8可知,随着负载电压的增大,微梁的挠度同样增大,当负载电压接近坍塌临界电压时,微梁挠度会迅速增加使微梁与电极贴合.仿真结果与数值计算结果一致.

微梁长度和损伤变量对微梁挠度和临界坍塌电压的影响分析结果分别如图9和图10所示.当长度增加时微梁挠度变大,临界坍塌电压变小,损伤变量增大时微梁挠度也变大.仿真结果和数值分析结果一致.

数值计算和有限元分析2种方法获得的临界坍塌电压结果如图11所示,并在表1中将具体数据进行比较.从图11和表1中可以看出,在相同电压条件下ANSYS进行有限元计算得出的临界坍塌电压较低,与使用荣格库塔法得出的临界坍塌电压相差7.8%,表明了计算结果的合理性.

4 结 论

本文通过数值计算和有限元仿真两种方法对具损伤的悬臂压电微梁在电场作用下非线性坍塌行为进行研究,讨论了几何非线性、控制电压等参数对微梁坍塌行为的影响.研究结果表明,考虑几何非线性使微梁具有更高的坍塌阈值电压;控制电压和微梁长度增大可导致微梁坍塌阈值电压明显降低.材料损伤变量在一定范围内增大会使微梁挠度和临界坍塌电压发生降低.因此,压电微梁结构在使用过程中产生轻微损伤,可以通过改变控制电压使其继续满足工作要求,从而延长压电微梁结构的使用寿命.

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