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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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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