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Low-Pb High-Piezoelectric Ceramic System (1−x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3)
Piezoelectric materials, especially Pb-based piezoelectric materials, are widely used in the key components of sensors, actuators, and transducers. Due to the rising concern of the toxicity of Pb, global legislation has been adopted to restrict the use of Pb. Given that the available Pb-free piezoel...
Autores principales: | , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
MDPI
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9322182/ https://www.ncbi.nlm.nih.gov/pubmed/35888228 http://dx.doi.org/10.3390/ma15144760 |
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author | Zhou, Chao Li, Jiajing Zhang, Xiaoxiao Yu, Tiantian Zhang, Yin Yang, Sen |
author_facet | Zhou, Chao Li, Jiajing Zhang, Xiaoxiao Yu, Tiantian Zhang, Yin Yang, Sen |
author_sort | Zhou, Chao |
collection | PubMed |
description | Piezoelectric materials, especially Pb-based piezoelectric materials, are widely used in the key components of sensors, actuators, and transducers. Due to the rising concern of the toxicity of Pb, global legislation has been adopted to restrict the use of Pb. Given that the available Pb-free piezoelectric materials cannot replace the Pb-based ones for various reasons, we designed and fabricated a low-Pb piezoelectric solid-solution ceramic system, (1–x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3) (denoted as BZ(0.18)T–xBP(0.22)T herein). The crystal structure, ferroelectric, dielectric, and piezoelectric properties of the BZ(0.18)T–xBP(0.22)T system were systematically studied. With the increase in BP(0.22)T content, the structure of the samples changed from a rhombohedral phase to a tetragonal phase; the intermediate composition x = 0.5 was located at the morphotropic phase boundary of the system and corresponded to the state with the coexistence of the rhombohedral and tetragonal phases. Moreover, x = 0.5 exhibited the optimum comprehensive properties among all the samples, with a piezoelectric coefficient d(33) of 240 pC/N, a maximum dielectric temperature Tm of 121.1°C, and a maximum polarization Pm of 15 μC/cm(2). Our work verifies the validity of the route to design low-Pb high-piezoelectric materials and may stimulate the interests for exploring new low-Pb high-performance ferroelectric and piezoelectric materials. |
format | Online Article Text |
id | pubmed-9322182 |
institution | National Center for Biotechnology Information |
language | English |
publishDate | 2022 |
publisher | MDPI |
record_format | MEDLINE/PubMed |
spelling | pubmed-93221822022-07-27 Low-Pb High-Piezoelectric Ceramic System (1−x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3) Zhou, Chao Li, Jiajing Zhang, Xiaoxiao Yu, Tiantian Zhang, Yin Yang, Sen Materials (Basel) Article Piezoelectric materials, especially Pb-based piezoelectric materials, are widely used in the key components of sensors, actuators, and transducers. Due to the rising concern of the toxicity of Pb, global legislation has been adopted to restrict the use of Pb. Given that the available Pb-free piezoelectric materials cannot replace the Pb-based ones for various reasons, we designed and fabricated a low-Pb piezoelectric solid-solution ceramic system, (1–x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3) (denoted as BZ(0.18)T–xBP(0.22)T herein). The crystal structure, ferroelectric, dielectric, and piezoelectric properties of the BZ(0.18)T–xBP(0.22)T system were systematically studied. With the increase in BP(0.22)T content, the structure of the samples changed from a rhombohedral phase to a tetragonal phase; the intermediate composition x = 0.5 was located at the morphotropic phase boundary of the system and corresponded to the state with the coexistence of the rhombohedral and tetragonal phases. Moreover, x = 0.5 exhibited the optimum comprehensive properties among all the samples, with a piezoelectric coefficient d(33) of 240 pC/N, a maximum dielectric temperature Tm of 121.1°C, and a maximum polarization Pm of 15 μC/cm(2). Our work verifies the validity of the route to design low-Pb high-piezoelectric materials and may stimulate the interests for exploring new low-Pb high-performance ferroelectric and piezoelectric materials. MDPI 2022-07-07 /pmc/articles/PMC9322182/ /pubmed/35888228 http://dx.doi.org/10.3390/ma15144760 Text en © 2022 by the authors. https://creativecommons.org/licenses/by/4.0/Licensee MDPI, Basel, Switzerland. This article is an open access article distributed under the terms and conditions of the Creative Commons Attribution (CC BY) license (https://creativecommons.org/licenses/by/4.0/). |
spellingShingle | Article Zhou, Chao Li, Jiajing Zhang, Xiaoxiao Yu, Tiantian Zhang, Yin Yang, Sen Low-Pb High-Piezoelectric Ceramic System (1−x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3) |
title | Low-Pb High-Piezoelectric Ceramic System (1−x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3) |
title_full | Low-Pb High-Piezoelectric Ceramic System (1−x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3) |
title_fullStr | Low-Pb High-Piezoelectric Ceramic System (1−x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3) |
title_full_unstemmed | Low-Pb High-Piezoelectric Ceramic System (1−x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3) |
title_short | Low-Pb High-Piezoelectric Ceramic System (1−x)Ba(Zr(0.18)Ti(0.82))O(3)–x(Ba(0.78)Pb(0.22))TiO(3) |
title_sort | low-pb high-piezoelectric ceramic system (1−x)ba(zr(0.18)ti(0.82))o(3)–x(ba(0.78)pb(0.22))tio(3) |
topic | Article |
url | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9322182/ https://www.ncbi.nlm.nih.gov/pubmed/35888228 http://dx.doi.org/10.3390/ma15144760 |
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