Cargando…

Gd(3+) and Bi(3+) co-substituted cubic zirconia; (Zr(1−x−y)Gd(x)Bi(y)O(2−δ)): a novel high κ relaxor dielectric and superior oxide-ion conductor

Solid oxide fuel cells (SOFCs) offer several advantages over lower temperature polymeric membrane fuels cells (PMFCs) due to their multiple fuel flexibility and requirement of low purity hydrogen. In order to decrease the operating temperature of SOFCs and to overcome the high operating cost and mat...

Descripción completa

Detalles Bibliográficos
Autores principales: Yadav, Akanksha, Prakash, Rajiv, Singh, Preetam
Formato: Online Artículo Texto
Lenguaje:English
Publicado: The Royal Society of Chemistry 2022
Materias:
Acceso en línea:https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9105713/
https://www.ncbi.nlm.nih.gov/pubmed/35702234
http://dx.doi.org/10.1039/d2ra01867e
_version_ 1784708108205948928
author Yadav, Akanksha
Prakash, Rajiv
Singh, Preetam
author_facet Yadav, Akanksha
Prakash, Rajiv
Singh, Preetam
author_sort Yadav, Akanksha
collection PubMed
description Solid oxide fuel cells (SOFCs) offer several advantages over lower temperature polymeric membrane fuels cells (PMFCs) due to their multiple fuel flexibility and requirement of low purity hydrogen. In order to decrease the operating temperature of SOFCs and to overcome the high operating cost and materials degradation challenges, the Cubic phase of ZrO(2) was stabilized with simultaneous substitution of Bi and Gd and the effect of co-doping on the oxide-ion conductivity of Zr(1−x−y)Bi(x)Gd(y)O(2−δ) was studied to develop a superior electrolyte separator for SOFCs. Up to 30% Gd and 20% Bi were simultaneously substituted in the cubic ZrO(2) lattice (Zr(1−x−y)Gd(x)Bi(y)O(2−δ), x + y ≤ 0.4, x ≤ 0.3 and y ≤ 0.2) by employing a solution combustion method followed by multiple calcinations at 900 °C. Phase purity and composition of the material is confirmed by powder XRD and EDX measurements. The formation of an oxygen vacant Gd/Bi co-doped cubic zirconia lattice was also confirmed by Raman spectroscopy study. With the incorporation of Bi(3+) and Gd(3+) ions, the cubic Zr(1−x−y)Bi(x)Gd(y)O(2−δ) phase showed relaxor type high κ dielectric behaviour (ε′ = 9725 at 600 °C at applied frequency 20 kHz for Zr(0.6)Bi(0.2)Gd(0.2)O(1.8)) with T(m) approaching 600 °C. The high polarizability of the Bi(3+) ion coupled with synergistic interaction of Bi and Gd in the host ZrO(2) lattice seems to create the more labile oxide ion vacancies that enable superior oxide-ion transport resulting in high oxide ion conductivity (σ(o) > 10(−2) S cm(−1), T > 500 °C for Zr(0.6)Bi(0.2)Gd(0.2)O(1.8)) at relatively lower temperatures.
format Online
Article
Text
id pubmed-9105713
institution National Center for Biotechnology Information
language English
publishDate 2022
publisher The Royal Society of Chemistry
record_format MEDLINE/PubMed
spelling pubmed-91057132022-06-13 Gd(3+) and Bi(3+) co-substituted cubic zirconia; (Zr(1−x−y)Gd(x)Bi(y)O(2−δ)): a novel high κ relaxor dielectric and superior oxide-ion conductor Yadav, Akanksha Prakash, Rajiv Singh, Preetam RSC Adv Chemistry Solid oxide fuel cells (SOFCs) offer several advantages over lower temperature polymeric membrane fuels cells (PMFCs) due to their multiple fuel flexibility and requirement of low purity hydrogen. In order to decrease the operating temperature of SOFCs and to overcome the high operating cost and materials degradation challenges, the Cubic phase of ZrO(2) was stabilized with simultaneous substitution of Bi and Gd and the effect of co-doping on the oxide-ion conductivity of Zr(1−x−y)Bi(x)Gd(y)O(2−δ) was studied to develop a superior electrolyte separator for SOFCs. Up to 30% Gd and 20% Bi were simultaneously substituted in the cubic ZrO(2) lattice (Zr(1−x−y)Gd(x)Bi(y)O(2−δ), x + y ≤ 0.4, x ≤ 0.3 and y ≤ 0.2) by employing a solution combustion method followed by multiple calcinations at 900 °C. Phase purity and composition of the material is confirmed by powder XRD and EDX measurements. The formation of an oxygen vacant Gd/Bi co-doped cubic zirconia lattice was also confirmed by Raman spectroscopy study. With the incorporation of Bi(3+) and Gd(3+) ions, the cubic Zr(1−x−y)Bi(x)Gd(y)O(2−δ) phase showed relaxor type high κ dielectric behaviour (ε′ = 9725 at 600 °C at applied frequency 20 kHz for Zr(0.6)Bi(0.2)Gd(0.2)O(1.8)) with T(m) approaching 600 °C. The high polarizability of the Bi(3+) ion coupled with synergistic interaction of Bi and Gd in the host ZrO(2) lattice seems to create the more labile oxide ion vacancies that enable superior oxide-ion transport resulting in high oxide ion conductivity (σ(o) > 10(−2) S cm(−1), T > 500 °C for Zr(0.6)Bi(0.2)Gd(0.2)O(1.8)) at relatively lower temperatures. The Royal Society of Chemistry 2022-05-13 /pmc/articles/PMC9105713/ /pubmed/35702234 http://dx.doi.org/10.1039/d2ra01867e Text en This journal is © The Royal Society of Chemistry https://creativecommons.org/licenses/by/3.0/
spellingShingle Chemistry
Yadav, Akanksha
Prakash, Rajiv
Singh, Preetam
Gd(3+) and Bi(3+) co-substituted cubic zirconia; (Zr(1−x−y)Gd(x)Bi(y)O(2−δ)): a novel high κ relaxor dielectric and superior oxide-ion conductor
title Gd(3+) and Bi(3+) co-substituted cubic zirconia; (Zr(1−x−y)Gd(x)Bi(y)O(2−δ)): a novel high κ relaxor dielectric and superior oxide-ion conductor
title_full Gd(3+) and Bi(3+) co-substituted cubic zirconia; (Zr(1−x−y)Gd(x)Bi(y)O(2−δ)): a novel high κ relaxor dielectric and superior oxide-ion conductor
title_fullStr Gd(3+) and Bi(3+) co-substituted cubic zirconia; (Zr(1−x−y)Gd(x)Bi(y)O(2−δ)): a novel high κ relaxor dielectric and superior oxide-ion conductor
title_full_unstemmed Gd(3+) and Bi(3+) co-substituted cubic zirconia; (Zr(1−x−y)Gd(x)Bi(y)O(2−δ)): a novel high κ relaxor dielectric and superior oxide-ion conductor
title_short Gd(3+) and Bi(3+) co-substituted cubic zirconia; (Zr(1−x−y)Gd(x)Bi(y)O(2−δ)): a novel high κ relaxor dielectric and superior oxide-ion conductor
title_sort gd(3+) and bi(3+) co-substituted cubic zirconia; (zr(1−x−y)gd(x)bi(y)o(2−δ)): a novel high κ relaxor dielectric and superior oxide-ion conductor
topic Chemistry
url https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9105713/
https://www.ncbi.nlm.nih.gov/pubmed/35702234
http://dx.doi.org/10.1039/d2ra01867e
work_keys_str_mv AT yadavakanksha gd3andbi3cosubstitutedcubiczirconiazr1xygdxbiyo2danovelhighkrelaxordielectricandsuperioroxideionconductor
AT prakashrajiv gd3andbi3cosubstitutedcubiczirconiazr1xygdxbiyo2danovelhighkrelaxordielectricandsuperioroxideionconductor
AT singhpreetam gd3andbi3cosubstitutedcubiczirconiazr1xygdxbiyo2danovelhighkrelaxordielectricandsuperioroxideionconductor