IEEE Trans Ultrason Ferroelectr Freq Control. 2017 Dec;64(12):1849-1856. doi: 10.1109/TUFFC.2017.2748901. Epub 2017 Sep 4.
The quality factor (Q) spectrum of a piezoceramic resonator, as a Q-factor frequency dependence for the specific resonator and its vibrational modes, was determined under baseline low-excitation level with a new approach proposed. The theoretical prediction was experimentally confirmed that the resonator Q-factor increases with frequency nearly linearly from the resonance reaching its maximum near the antiresonance. For the industrial PZT-5A piezoceramic the antiresonance-to-resonance quality factor ratio is 1.8 to 2.4 as much, depending on the type of vibration. As the theory states, this effect is directly related to the piezoelectric "losses" in piezoceramics, usually represented by the imaginary part of complex piezocoefficients, which have a unique property of lowering the total cumulative energy dissipation in a resonator in certain frequency intervals. Based on the electromechanical Q-factor (EMQ) concept, a new relatively simple method was proposed for the piezoelectric loss factor determination at just a single resonance frequency-it requires measurements of the resonance Q-factor and its frequency derivative at the resonance, or the first and second frequency derivatives of the immittance phase at the resonance. Experimentally determined is close to near 0.8 of its upper (positive) phenomenological limit in the conventional PZT-5A piezoceramic at the basic vibrational modes. The piezoelectric loss factor, theoretically reaching the upper limit, can provide extremely high value of the Q-factor (near the fundamental antiresonance) with possible an order of magnitude EMQ increase. That paradoxical fact for the piezoelectric "losses" is a novel possible way of improving the piezoceramic performance and operation.
压电陶瓷谐振器的品质因数 (Q) 谱,作为特定谐振器及其振动模式的 Q 因子频率依赖性,是在新提出的低激励水平基准下确定的。理论预测得到了实验证实,即谐振器的 Q 因子随频率几乎呈线性增加,从谐振达到反谐振附近的最大值。对于工业 PZT-5A 压电陶瓷,反谐振到谐振的品质因数比为 1.8 到 2.4,具体取决于振动类型。正如理论所述,这种效应与压电陶瓷中的“损耗”直接相关,通常由复压电系数的虚部表示,它具有在特定频率间隔内降低谐振器中总累积能量耗散的独特特性。基于机电 Q 因子 (EMQ) 概念,提出了一种新的相对简单的方法,用于在单个谐振频率下确定压电损耗因子——它需要测量谐振 Q 因子及其在谐振时的频率导数,或导纳相位在谐振时的第一和第二频率导数。在基本振动模式下,实验确定的常规 PZT-5A 压电陶瓷的近 0.8 接近其上限(正)唯象极限。理论上达到上限的压电损耗因子可以提供极高的 Q 因子值(接近基本反谐振),可能会使 EMQ 增加一个数量级。对于压电“损耗”来说,这一矛盾的事实是改善压电陶瓷性能和运行的一种新的可能途径。