Nonlinear direct and indirect third harmonic generation in piezoelectric resonators by the intermodulation method

Citation
A. Albareda et al., Nonlinear direct and indirect third harmonic generation in piezoelectric resonators by the intermodulation method, REV SCI INS, 72(6), 2001, pp. 2742-2749
Citations number
16
Categorie Soggetti
Spectroscopy /Instrumentation/Analytical Sciences","Instrumentation & Measurement
Journal title
REVIEW OF SCIENTIFIC INSTRUMENTS
ISSN journal
00346748 → ACNP
Volume
72
Issue
6
Year of publication
2001
Pages
2742 - 2749
Database
ISI
SICI code
0034-6748(200106)72:6<2742:NDAITH>2.0.ZU;2-E
Abstract
Nonlinear characterization in power piezoelectric devices requires a knowle dge of what mechanisms are involved in the nonlinearity. For resonant devic es, it is considered that the origin of these nonlinearities is mechanical, and their effects are: the increase of losses, the shift of the resonant f requency, and the frequency hysteresis. These effects, which can be underst ood by the analysis of the impedance increase near the resonance, can arise from third harmonic generation (second overtone) due to the nonlinearities . This third harmonic can be generated by the cubic terms of the nonlinear constitutive equations (direct contribution), or by the quadratic terms whe n they perform twice consecutively (indirect contribution). The present wor k presents a quantitative evaluation of these two effects, using an intermo dulation method that allows us to know every harmonic generated by the nonl inearity, whether quadratic or cubic. The conclusion of this work is that f or the studied piezoelectric ceramics, with low and high losses, the indire ct effect is negligible compared with the direct contribution, being about 1000 times lower. (C) 2001 American Institute of Physics.