Study on frequency dependence of polarized piezoceramics constants in equivalent circuits at weak electric fields (part III)

Introduction. It is acknowledged that electroelastic modules do not depend on the amplitude and frequency of oscillations. This approach is reflected in the Russian and foreign standards for determining the complete set of electro-elastic piezoceramics modules. For example, to determine d31 piezomod...

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Main Authors: V. V. Madorsky, I. E. Rogov, A. К. Kruglov
Format: Article
Language:Russian
Published: Don State Technical University 2019-06-01
Series:Advanced Engineering Research
Subjects:
Online Access:https://www.vestnik-donstu.ru/jour/article/view/1513
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spelling doaj-5a2d6881a7d24cbfa7df04e3bbb510fe2021-10-02T18:41:34ZrusDon State Technical UniversityAdvanced Engineering Research2687-16532019-06-0119214315010.23947/1992-5980-2019-19-2-143-1501413Study on frequency dependence of polarized piezoceramics constants in equivalent circuits at weak electric fields (part III)V. V. Madorsky0I. E. Rogov1A. К. Kruglov2Don State Technical UniversityDon State Technical UniversitySouthern Federal UniversityIntroduction. It is acknowledged that electroelastic modules do not depend on the amplitude and frequency of oscillations. This approach is reflected in the Russian and foreign standards for determining the complete set of electro-elastic piezoceramics modules. For example, to determine d31 piezomodule of a disc-shaped sample, it is required to take measurements in three frequency domains: in the first and second resonances, in the antiresonance region, and at frequencies much below 1 kHz. Accordingly, it is assumed that when determining d31, the modules of the ceramic under study in the frequency range from 1 KHz to the second resonance are independent of frequency. The work objective is to study the frequency dependence of electro-elastic ceramic modules. In this case, a disc-shaped sample from LZT (lead zirconate titanate) is used.Materials and Methods. Techniques of setting and solving problems of the stationary electroelasticity and sections of the electrical engineering basics are applied. To implement the finite element method, the perturbation technique and the ANSYS application package are used. The experimental results are processed in the MATLAB environment.Research Results. For the LZT piezoelectric ceramics, the frequency dependences of various modules (piezoelectric d31, dielectric ε33???????? and elastic modules of compliance ????????11, ????????12, ????????13) were investigated. Radial oscillations of a discshaped sample with electrodes on the ends were considered. The sample thickness was 1 mm, the diameter was 40 mm, and the oscillation range was up to 700 KHz. First, the frequency dependence was studied for the elastic ceramic modules from the determination of ten resonance frequencies. Then, the frequency dependence of d31and ε33???????? modules was determined from the measured values of the sample conductivity. For this purpose, we used the expression for the electrical conductivity obtained from the solution of the radial oscillations of the disc considering its thickness.Discussion and Conclusions. A technique is developed for determining the frequency dependence of LZT piezoelectric ceramic modules. The disc-shaped sample was studied in 15650 KHz frequency range. It is shown that in the range up to 650 KHz, ????????11, ????????12, ????????13 elastic modules with E superscript (it is omitted) or measured at dc field are practically independent of frequency. In the specified range, ε33????????, d31, kp constants have an insignificant frequency dependence for the considered radial oscillations.https://www.vestnik-donstu.ru/jour/article/view/1513piezoelectric ceramicselectro elastic modulesequivalent circuitfrequency dependencediscfinite-element techniqueperturbation method
collection DOAJ
language Russian
format Article
sources DOAJ
author V. V. Madorsky
I. E. Rogov
A. К. Kruglov
spellingShingle V. V. Madorsky
I. E. Rogov
A. К. Kruglov
Study on frequency dependence of polarized piezoceramics constants in equivalent circuits at weak electric fields (part III)
Advanced Engineering Research
piezoelectric ceramics
electro elastic modules
equivalent circuit
frequency dependence
disc
finite-element technique
perturbation method
author_facet V. V. Madorsky
I. E. Rogov
A. К. Kruglov
author_sort V. V. Madorsky
title Study on frequency dependence of polarized piezoceramics constants in equivalent circuits at weak electric fields (part III)
title_short Study on frequency dependence of polarized piezoceramics constants in equivalent circuits at weak electric fields (part III)
title_full Study on frequency dependence of polarized piezoceramics constants in equivalent circuits at weak electric fields (part III)
title_fullStr Study on frequency dependence of polarized piezoceramics constants in equivalent circuits at weak electric fields (part III)
title_full_unstemmed Study on frequency dependence of polarized piezoceramics constants in equivalent circuits at weak electric fields (part III)
title_sort study on frequency dependence of polarized piezoceramics constants in equivalent circuits at weak electric fields (part iii)
publisher Don State Technical University
series Advanced Engineering Research
issn 2687-1653
publishDate 2019-06-01
description Introduction. It is acknowledged that electroelastic modules do not depend on the amplitude and frequency of oscillations. This approach is reflected in the Russian and foreign standards for determining the complete set of electro-elastic piezoceramics modules. For example, to determine d31 piezomodule of a disc-shaped sample, it is required to take measurements in three frequency domains: in the first and second resonances, in the antiresonance region, and at frequencies much below 1 kHz. Accordingly, it is assumed that when determining d31, the modules of the ceramic under study in the frequency range from 1 KHz to the second resonance are independent of frequency. The work objective is to study the frequency dependence of electro-elastic ceramic modules. In this case, a disc-shaped sample from LZT (lead zirconate titanate) is used.Materials and Methods. Techniques of setting and solving problems of the stationary electroelasticity and sections of the electrical engineering basics are applied. To implement the finite element method, the perturbation technique and the ANSYS application package are used. The experimental results are processed in the MATLAB environment.Research Results. For the LZT piezoelectric ceramics, the frequency dependences of various modules (piezoelectric d31, dielectric ε33???????? and elastic modules of compliance ????????11, ????????12, ????????13) were investigated. Radial oscillations of a discshaped sample with electrodes on the ends were considered. The sample thickness was 1 mm, the diameter was 40 mm, and the oscillation range was up to 700 KHz. First, the frequency dependence was studied for the elastic ceramic modules from the determination of ten resonance frequencies. Then, the frequency dependence of d31and ε33???????? modules was determined from the measured values of the sample conductivity. For this purpose, we used the expression for the electrical conductivity obtained from the solution of the radial oscillations of the disc considering its thickness.Discussion and Conclusions. A technique is developed for determining the frequency dependence of LZT piezoelectric ceramic modules. The disc-shaped sample was studied in 15650 KHz frequency range. It is shown that in the range up to 650 KHz, ????????11, ????????12, ????????13 elastic modules with E superscript (it is omitted) or measured at dc field are practically independent of frequency. In the specified range, ε33????????, d31, kp constants have an insignificant frequency dependence for the considered radial oscillations.
topic piezoelectric ceramics
electro elastic modules
equivalent circuit
frequency dependence
disc
finite-element technique
perturbation method
url https://www.vestnik-donstu.ru/jour/article/view/1513
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AT akkruglov studyonfrequencydependenceofpolarizedpiezoceramicsconstantsinequivalentcircuitsatweakelectricfieldspartiii
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