Measurement of thermal depolarization effects in piezoelectric coefficients of soft PZT ceramics via the frequency and direct methods

dc.contributor.authorFialka, Jiřícs
dc.contributor.authorBeneš, Petrcs
dc.contributor.authorMichlovská, Lenkacs
dc.contributor.authorKlusáček, Stanislavcs
dc.contributor.authorPikula, Stanislavcs
dc.contributor.authorDohnal, Přemyslcs
dc.contributor.authorHavránek, Zdeněkcs
dc.coverage.issue11cs
dc.coverage.volume36cs
dc.date.issued2016-09-01cs
dc.description.abstractDepolarization at high temperatures around the Curie point constitutes an important yet difficultly measurable material property of piezoelectric (PZT) ceramics. The common vibrometric technique (d33 meters) is not suitable for the measurement of temperature dependences, and therefore we used the frequency method to perform the desired procedures. The indicator selected to show the depolarization state in the piezoelectric ceramics consisted in the piezoelectric charge coefficient, whose value can be effectively measured via the above-mentioned frequency technique. The accuracy of the method was verified via comparing a d33 meter constructed by the authors (as described in this paper) and also by means of differently sized cylinders of ceramics NCE51, which are designed for longitudinal length modes. Based on the obtained results, we established a measurement methodology to exactly determine the value of the Curie point that corresponded to the phase transition to a cubic crystallographic structure. The experiment also confirmed the applicability of progressively controlled depolarization of PZT ceramics by high temperature in the range of between 350 and 370 °C, and it defined the temperature limits at which there occur irreversible changes of the piezoelectric properties of PZT ceramics. In the measured NCE51 material, the limit for irreversible changes was equal to 95% of the Curie temperature (368 °C).en
dc.description.abstractDepolarization at high temperatures around the Curie point constitutes an important yet difficultly measurable material property of piezoelectric (PZT) ceramics. The common vibrometric technique (d33 meters) is not suitable for the measurement of temperature dependences, and therefore we used the frequency method to perform the desired procedures. The indicator selected to show the depolarization state in the piezoelectric ceramics consisted in the piezoelectric charge coefficient, whose value can be effectively measured via the above-mentioned frequency technique. The accuracy of the method was verified via comparing a d33 meter constructed by the authors (as described in this paper) and also by means of differently sized cylinders of ceramics NCE51, which are designed for longitudinal length modes. Based on the obtained results, we established a measurement methodology to exactly determine the value of the Curie point that corresponded to the phase transition to a cubic crystallographic structure. The experiment also confirmed the applicability of progressively controlled depolarization of PZT ceramics by high temperature in the range of between 350 and 370 °C, and it defined the temperature limits at which there occur irreversible changes of the piezoelectric properties of PZT ceramics. In the measured NCE51 material, the limit for irreversible changes was equal to 95% of the Curie temperature (368 °C).en
dc.formattextcs
dc.format.extent2727-2738cs
dc.format.mimetypeapplication/pdfcs
dc.identifier.citationJournal of the European Ceramic Society. 2016, vol. 36, issue 11, p. 2727-2738.en
dc.identifier.doi10.1016/j.jeurceramsoc.2016.03.036cs
dc.identifier.issn0955-2219cs
dc.identifier.orcid0000-0001-8541-8155cs
dc.identifier.orcid0000-0002-3712-7107cs
dc.identifier.orcid0000-0002-7963-1715cs
dc.identifier.orcid0000-0002-9849-1105cs
dc.identifier.orcid0000-0002-4437-0412cs
dc.identifier.orcid0000-0003-1163-4458cs
dc.identifier.orcid0000-0002-8761-6590cs
dc.identifier.other124661cs
dc.identifier.researcheridG-8696-2014cs
dc.identifier.researcheridB-1805-2008cs
dc.identifier.researcheridB-1133-2014cs
dc.identifier.researcheridH-2234-2016cs
dc.identifier.researcheridA-6017-2016cs
dc.identifier.researcheridAAE-2611-2021cs
dc.identifier.researcheridD-7933-2012cs
dc.identifier.scopus56087172100cs
dc.identifier.scopus7006828688cs
dc.identifier.scopus25621760100cs
dc.identifier.scopus9336430800cs
dc.identifier.scopus37062829400cs
dc.identifier.scopus54981039700cs
dc.identifier.urihttp://hdl.handle.net/11012/209273
dc.language.isoencs
dc.publisherElsevier Ltd.cs
dc.relation.ispartofJournal of the European Ceramic Societycs
dc.relation.urihttp://www.sciencedirect.com/science/article/pii/S0955221916301625cs
dc.rightsCreative Commons Attribution-NonCommercial-NoDerivatives 4.0 Internationalcs
dc.rights.accessopenAccesscs
dc.rights.sherpahttp://www.sherpa.ac.uk/romeo/issn/0955-2219/cs
dc.rights.urihttp://creativecommons.org/licenses/by-nc-nd/4.0/cs
dc.subjectPZT ceramicsen
dc.subjectPiezoelectric charge coefficienten
dc.subjectCurie temperatureen
dc.subjectFrequency methoden
dc.subjectVibrometric methoden
dc.subjectPZT ceramics
dc.subjectPiezoelectric charge coefficient
dc.subjectCurie temperature
dc.subjectFrequency method
dc.subjectVibrometric method
dc.titleMeasurement of thermal depolarization effects in piezoelectric coefficients of soft PZT ceramics via the frequency and direct methodsen
dc.title.alternativeMeasurement of thermal depolarization effects in piezoelectric coefficients of soft PZT ceramics via the frequency and direct methodsen
dc.type.driverarticleen
dc.type.statusPeer-revieweden
dc.type.versionacceptedVersionen
sync.item.dbidVAV-124661en
sync.item.dbtypeVAVen
sync.item.insts2025.10.14 15:17:55en
sync.item.modts2025.10.14 09:52:29en
thesis.grantorVysoké učení technické v Brně. Fakulta elektrotechniky a komunikačních technologií. Ústav automatizace a měřicí technikycs
thesis.grantorVysoké učení technické v Brně. Středoevropský technologický institut VUT. Kybernetika pro materiálové vědycs
thesis.grantorVysoké učení technické v Brně. Středoevropský technologický institut VUT. Pokročilé polymerní materiály a kompozitcs

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