首页> 外文期刊>IEEE Transactions on Ultrasonics, Ferroelectrics, and Frequency Control >Flexural Vibrations and Resonance of Piezoelectric Cantilevers with a Nonpiezoelectric Extension
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Flexural Vibrations and Resonance of Piezoelectric Cantilevers with a Nonpiezoelectric Extension

机译:具有非压电扩展的压电悬臂的弯曲振动和共振

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摘要

A piezoelectric cantilever (PEC) is a flexural transducer consisting of a piezoelectric layer [e.g., lead zirconate titanate (PZT)] bonded to a nonpiezoelectric layer (e.g., stainless steel). A PEC with a thin nonpiezoelectric extension has two distinctive sections, each with a different thickness, different axial density, and elastic-modulus profiles and has been increasingly used as an in-situ biosensor. It has the advantages of dipping only the nonpiezoelectric extension part in an aqueous solution without electrically insulating the piezoelectric section as well as serving as the bonding pad for receptor immobilization. In this study, we examined the effect of the thin nonpiezoelectric extension on the flexural resonance spectrum and resonance vibration waveforms of PEC; in particular, how the length ratio between the piezoelectric section and the nonpiezoelectric extension section affects the resonance frequencies and resonance peak intensities of PEC. Theoretical resonance frequencies and resonance vibration waveforms were obtained using an analytical transcendental equation we derived by solving the flexural wave equation. Both experimental and theoretical results showed that the two-section structure distorted the flexural vibration waveforms from those of PEC without an extension. As a result, the higher-mode resonance peaks of PEC with a nonpiezoelectric extension could be higher than the first resonance peak due to the two-section structure. With PEC that has a piezoelectric section of 0.25-mm thick PZT bonded to 0.07 mm thick stainless steel of various length l1 and a 0.07-mm thick nonpiezoelectric extension of length I2, we showed that the first-mode-to-second-mode resonance peak intensity ratio had a maximum of 5.6 at I1/I2 = 0.75 and the first-mode- to-second-mode resonance frequency ratio a minimum of 2.2 at I1/I2 = 1.8. These findings will undoubtedly help optimize the design and perf-normance of PEC.
机译:压电悬臂(PEC)是一种挠曲换能器,由结合到非压电层(例如不锈钢)的压电层[例如锆钛酸铅(PZT)]组成。具有薄的非压电延伸的PEC具有两个不同的部分,每个部分具有不同的厚度,不同的轴向密度和弹性模量轮廓,并且已越来越多地用作原位生物传感器。其优点是仅将非压电延伸部分浸入水溶液中而不使压电部分电绝缘,并且具有用作受体固定的结合垫的优点。在这项研究中,我们研究了薄的非压电延伸对PEC的弯曲共振谱和共振振动波形的影响。特别地,压电部分和非压电延伸部分之间的长度比如何影响PEC的共振频率和共振峰强度。理论上的共振频率和共振振动波形是使用我们通过求解弯曲波方程得出的解析先验方程获得的。实验和理论结果均表明,该两段式结构使弯曲振动波形与PEC的弯曲振动波形不发生扩展。结果,由于具有两部分结构,具有非压电扩展的PEC的较高模式共振峰可能高于第一共振峰。对于具有0.25 mm厚的PZT压电部分的PEC,该压电部分结合到各种长度l1的0.07 mm厚的不锈钢上,以及长度为I2的0.07 mm厚的非压电延伸部分,我们证明了第一模式到第二模式共振在I1 / I2 = 0.75时,峰值强度比最大为5.6,在I1 / I2 = 1.8时,第一模式到第二模式共振频率比为最小2.2。这些发现无疑将有助于优化PEC的设计和性能。

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