Electrical conduction properties of the BZT–BST ceramics

0.5Ba(Zr0.2Ti0.8)O3-0.5(Ba0.7Sr0.3)TiO3 (BZT–BST) has been explored in recent times for potential applications in energy harvesting, electrocaloric and energy storage. To this end, energy harvesting/conversion and storage applications require an understanding of the conduction and loss mechanisms. T...

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Main Authors: Satyanarayan Patel, Harekrishna Yadav
Format: Article
Language:English
Published: World Scientific Publishing 2020-12-01
Series:Journal of Advanced Dielectrics
Subjects:
Online Access:http://www.worldscientific.com/doi/epdf/10.1142/S2010135X20500265
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spelling doaj-c45741c79f574ccf8bedab34b2c5ede02020-12-29T05:50:22ZengWorld Scientific PublishingJournal of Advanced Dielectrics2010-135X2010-13682020-12-011062050026-12050026-1310.1142/S2010135X2050026510.1142/S2010135X20500265Electrical conduction properties of the BZT–BST ceramicsSatyanarayan Patel0Harekrishna Yadav1Discipline of Mechanical Engineering, Indian Institute of Technology Indore, Indore, Madhya Pradesh, 453552, IndiaDiscipline of Mechanical Engineering, Indian Institute of Technology Indore, Indore, Madhya Pradesh, 453552, India0.5Ba(Zr0.2Ti0.8)O3-0.5(Ba0.7Sr0.3)TiO3 (BZT–BST) has been explored in recent times for potential applications in energy harvesting, electrocaloric and energy storage. To this end, energy harvesting/conversion and storage applications require an understanding of the conduction and loss mechanisms. The conduction mechanism in BZT–BST ceramics is studied using impedance spectroscopy (IS) at 0.1 Hz−3 MHz and 100−600∘C. Impedance study reveals the presence of two types of relaxation processes due to grain and grain boundary contributions. The relaxation time and dc conductivity activation energies are obtained as 1.12/1.3 eV and 1.05/1.2eV for bulk/grain boundary, respectively, and found that oxygen vacancies dominated electrical behavior. The relaxation mechanism follows non-Debye-type behavior. The high resistance of the grain (bulk) in the ferroelectric region does not contribute to the high losses; the losses probably result from the phase transition. Also, BZT–BST ceramics exhibit a negative temperature coefficient of resistance (NTCR) behaviour. From a practical application point of view in the temperature regime of 25–65∘C, the loss’s contribution is low. The significant contributions of loss result from the response of phase-transition in this temperature range (25–65∘C).http://www.worldscientific.com/doi/epdf/10.1142/S2010135X20500265electrical conductivityimpedance spectroscopyelectric moduluslead-free
collection DOAJ
language English
format Article
sources DOAJ
author Satyanarayan Patel
Harekrishna Yadav
spellingShingle Satyanarayan Patel
Harekrishna Yadav
Electrical conduction properties of the BZT–BST ceramics
Journal of Advanced Dielectrics
electrical conductivity
impedance spectroscopy
electric modulus
lead-free
author_facet Satyanarayan Patel
Harekrishna Yadav
author_sort Satyanarayan Patel
title Electrical conduction properties of the BZT–BST ceramics
title_short Electrical conduction properties of the BZT–BST ceramics
title_full Electrical conduction properties of the BZT–BST ceramics
title_fullStr Electrical conduction properties of the BZT–BST ceramics
title_full_unstemmed Electrical conduction properties of the BZT–BST ceramics
title_sort electrical conduction properties of the bzt–bst ceramics
publisher World Scientific Publishing
series Journal of Advanced Dielectrics
issn 2010-135X
2010-1368
publishDate 2020-12-01
description 0.5Ba(Zr0.2Ti0.8)O3-0.5(Ba0.7Sr0.3)TiO3 (BZT–BST) has been explored in recent times for potential applications in energy harvesting, electrocaloric and energy storage. To this end, energy harvesting/conversion and storage applications require an understanding of the conduction and loss mechanisms. The conduction mechanism in BZT–BST ceramics is studied using impedance spectroscopy (IS) at 0.1 Hz−3 MHz and 100−600∘C. Impedance study reveals the presence of two types of relaxation processes due to grain and grain boundary contributions. The relaxation time and dc conductivity activation energies are obtained as 1.12/1.3 eV and 1.05/1.2eV for bulk/grain boundary, respectively, and found that oxygen vacancies dominated electrical behavior. The relaxation mechanism follows non-Debye-type behavior. The high resistance of the grain (bulk) in the ferroelectric region does not contribute to the high losses; the losses probably result from the phase transition. Also, BZT–BST ceramics exhibit a negative temperature coefficient of resistance (NTCR) behaviour. From a practical application point of view in the temperature regime of 25–65∘C, the loss’s contribution is low. The significant contributions of loss result from the response of phase-transition in this temperature range (25–65∘C).
topic electrical conductivity
impedance spectroscopy
electric modulus
lead-free
url http://www.worldscientific.com/doi/epdf/10.1142/S2010135X20500265
work_keys_str_mv AT satyanarayanpatel electricalconductionpropertiesofthebztbstceramics
AT harekrishnayadav electricalconductionpropertiesofthebztbstceramics
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