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Heterointerface Effect in Accelerating the Cathodic Oxygen Reduction for Intermediate-Temperature Solid Oxide Fuel Cells
A solid-state mixing method was adopted to prepare a new Pr(0.8)Sr(0.2)Fe(0.7)Ni(0.3)O(3−δ)-Pr(1.2)Sr(0.8)Fe(0.4)Ni(0.6)O(4+δ) (PSFN(113-214)) composite cathode oxide for the solid oxide fuel cells (SOFCs). Herein, heterointerface engineering was investigated for the performance enhancement. It was...
Autores principales: | , , , , , , , |
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Formato: | Online Artículo Texto |
Lenguaje: | English |
Publicado: |
Frontiers Media S.A.
2022
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Materias: | |
Acceso en línea: | https://www.ncbi.nlm.nih.gov/pmc/articles/PMC9425036/ https://www.ncbi.nlm.nih.gov/pubmed/36051624 http://dx.doi.org/10.3389/fchem.2022.959863 |
Sumario: | A solid-state mixing method was adopted to prepare a new Pr(0.8)Sr(0.2)Fe(0.7)Ni(0.3)O(3−δ)-Pr(1.2)Sr(0.8)Fe(0.4)Ni(0.6)O(4+δ) (PSFN(113-214)) composite cathode oxide for the solid oxide fuel cells (SOFCs). Herein, heterointerface engineering was investigated for the performance enhancement. It was found that the oxygen vacancy content could be increased by mixing the PSFN(214) with PSFN(113), which gave rise to the formation of a heterostructure, and resulted in the promotion of oxygen ion transport as well as the specific surface area. The optimum mixing ratio 5:5 resulted in the highest oxygen vacancy content and the largest specific surface area, indicating the strongest interface effect. Polarization resistance of PSFN(113-214) (5:5) was 0.029 Ω cm(2) at 800°C, which was merely 24% of PSFN(113) and 39% of PSFN(214). The corresponding maximum power density was 0.699 W cm(−2), which was nearly 1.44 times of PSFN(113) and 1.24 times of PSFN(214). Furthermore, the voltage attenuation rate after 100 h was merely 0.0352% h(−1). Therefore, the new PSFN(113-214) composite could be a prospective cathode oxide for SOFCs. |
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