<b>Effect of Pr<sub>6</sub>O<sub>11</sub> doping in electrical and microstructural properties of SnO<sub>2</sub>-based varistors<b>

The influence of the dopant Pr6O11 was investigated with regard to the electrical and microstructural properties of the system (98.95-x)%SnO2.1.0%CoO.0.05%Ta2O5.x%Pr6O11, where x = 0.05%, 0.10%, 0.30% and 0.50% in mol. Pr6O11 doping modifies the electrical behavior of the ceramics. The electrical pa...

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Main Authors: Hervê Stangler Irion, Eder Carlos Ferreira de Souza, André Vitor Chaves de Andrade, Sandra Regina Masetto Antunes, Augusto Celso Antunes
Format: Article
Language:English
Published: Universidade Estadual de Maringá 2014-04-01
Series:Acta Scientiarum: Technology
Subjects:
Online Access:http://186.233.154.254/ojs/index.php/ActaSciTechnol/article/view/17995
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spelling doaj-9ee67e47592c4682919077d065b69c942020-11-25T01:51:59ZengUniversidade Estadual de MaringáActa Scientiarum: Technology1806-25631807-86642014-04-0136223724410.4025/actascitechnol.v36i2.1799510610<b>Effect of Pr<sub>6</sub>O<sub>11</sub> doping in electrical and microstructural properties of SnO<sub>2</sub>-based varistors<b>Hervê Stangler Irion0Eder Carlos Ferreira de Souza1André Vitor Chaves de Andrade2Sandra Regina Masetto Antunes3Augusto Celso Antunes4Universidade Estadual de Ponta GrossaUniversidade Estadual de Ponta GrossaUniversidade Estadual de Ponta GrossaUniversidade Estadual de Ponta GrossaUniversidade Estadual de Ponta GrossaThe influence of the dopant Pr6O11 was investigated with regard to the electrical and microstructural properties of the system (98.95-x)%SnO2.1.0%CoO.0.05%Ta2O5.x%Pr6O11, where x = 0.05%, 0.10%, 0.30% and 0.50% in mol. Pr6O11 doping modifies the electrical behavior of the ceramics. The electrical parameters were: α = 8.0, EB = 319 V cm-1 and Vb = 0.66 V barrier-1 for the system without Pr6O11 and α = 17.0, EB = 853 V cm-1 and Vb = 1.15 V barrier-1 with the addition of 0.10% in mol Pr6O11. The system with 0.05% in mol Pr6O11 had the same non-linearity coefficient α as the system with 0.10% in mol. However, breakdown electrical field and voltage per barrier rates were lower (EB = 708 V cm-1 and Vb = 0.98 V barrier-1). The low rates in the breakdown electrical field enabled the varistor systems under study to be used in protection systems for low-voltage energy grids. In the case of Pr6O11 concentrations above 0.10% in mol, the presence of the dopant became deleterious to the varistor’s electrical characteristics. This effect was due to an increase in praseodymium stannate (Pr2Sn2O7) secondary phase. The crystalline phase coupled to the cassiterite (SnO2) phase was found with XRD and SEM/EDS and quantified by Rietveld’s refining method.http://186.233.154.254/ojs/index.php/ActaSciTechnol/article/view/17995characterizationtin dioxidepraseodymium oxidetantalum oxide
collection DOAJ
language English
format Article
sources DOAJ
author Hervê Stangler Irion
Eder Carlos Ferreira de Souza
André Vitor Chaves de Andrade
Sandra Regina Masetto Antunes
Augusto Celso Antunes
spellingShingle Hervê Stangler Irion
Eder Carlos Ferreira de Souza
André Vitor Chaves de Andrade
Sandra Regina Masetto Antunes
Augusto Celso Antunes
<b>Effect of Pr<sub>6</sub>O<sub>11</sub> doping in electrical and microstructural properties of SnO<sub>2</sub>-based varistors<b>
Acta Scientiarum: Technology
characterization
tin dioxide
praseodymium oxide
tantalum oxide
author_facet Hervê Stangler Irion
Eder Carlos Ferreira de Souza
André Vitor Chaves de Andrade
Sandra Regina Masetto Antunes
Augusto Celso Antunes
author_sort Hervê Stangler Irion
title <b>Effect of Pr<sub>6</sub>O<sub>11</sub> doping in electrical and microstructural properties of SnO<sub>2</sub>-based varistors<b>
title_short <b>Effect of Pr<sub>6</sub>O<sub>11</sub> doping in electrical and microstructural properties of SnO<sub>2</sub>-based varistors<b>
title_full <b>Effect of Pr<sub>6</sub>O<sub>11</sub> doping in electrical and microstructural properties of SnO<sub>2</sub>-based varistors<b>
title_fullStr <b>Effect of Pr<sub>6</sub>O<sub>11</sub> doping in electrical and microstructural properties of SnO<sub>2</sub>-based varistors<b>
title_full_unstemmed <b>Effect of Pr<sub>6</sub>O<sub>11</sub> doping in electrical and microstructural properties of SnO<sub>2</sub>-based varistors<b>
title_sort <b>effect of pr<sub>6</sub>o<sub>11</sub> doping in electrical and microstructural properties of sno<sub>2</sub>-based varistors<b>
publisher Universidade Estadual de Maringá
series Acta Scientiarum: Technology
issn 1806-2563
1807-8664
publishDate 2014-04-01
description The influence of the dopant Pr6O11 was investigated with regard to the electrical and microstructural properties of the system (98.95-x)%SnO2.1.0%CoO.0.05%Ta2O5.x%Pr6O11, where x = 0.05%, 0.10%, 0.30% and 0.50% in mol. Pr6O11 doping modifies the electrical behavior of the ceramics. The electrical parameters were: α = 8.0, EB = 319 V cm-1 and Vb = 0.66 V barrier-1 for the system without Pr6O11 and α = 17.0, EB = 853 V cm-1 and Vb = 1.15 V barrier-1 with the addition of 0.10% in mol Pr6O11. The system with 0.05% in mol Pr6O11 had the same non-linearity coefficient α as the system with 0.10% in mol. However, breakdown electrical field and voltage per barrier rates were lower (EB = 708 V cm-1 and Vb = 0.98 V barrier-1). The low rates in the breakdown electrical field enabled the varistor systems under study to be used in protection systems for low-voltage energy grids. In the case of Pr6O11 concentrations above 0.10% in mol, the presence of the dopant became deleterious to the varistor’s electrical characteristics. This effect was due to an increase in praseodymium stannate (Pr2Sn2O7) secondary phase. The crystalline phase coupled to the cassiterite (SnO2) phase was found with XRD and SEM/EDS and quantified by Rietveld’s refining method.
topic characterization
tin dioxide
praseodymium oxide
tantalum oxide
url http://186.233.154.254/ojs/index.php/ActaSciTechnol/article/view/17995
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