4.6 Article

Sn-Dy-Cu Triply Doped BaZr0.1Ce0.7Y0.2O3-?: A Chemically Stable and Highly Proton-Conductive Electrolyte for Low-Temperature Solid Oxide Fuel Cells

Journal

ACS SUSTAINABLE CHEMISTRY & ENGINEERING
Volume 10, Issue 16, Pages 5352-5362

Publisher

AMER CHEMICAL SOC
DOI: 10.1021/acssuschemeng.2c00807

Keywords

Protonic ceramic fuel cell; Triple-doping strategy; Chemical stability; BaCeO3; Sintering; Electrical property

Funding

  1. National Natural Science Foundation of China [91745203]

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BaCeO3-based proton conductors have limitations in practical applications due to low chemical stability and high sintering temperature. In this study, a triple-doping strategy was used to improve the chemical stability and conductivity of BaZr0.1Ce0.7Y0.2O3-delta(BZCY) electrolyte. The triply doped BaCe0.7Sn0.1Dy0.15Cu0.05O3-delta(BCSDCu) exhibited better properties compared to pristine BZCY, including lower sintering temperature and higher proton conductivity. The BCSDCu electrolyte achieved a competitive proton conductivity of 13.6 mS cm-1at 600 degrees C and a high power density of 390 mW cm-2 in an anode-supported single cell.
BaCeO3-based proton conductors have comparatively high-proton conductivity, but the low chemical stability andhigh sintering temperature seriously hinder their practicalapplications in protonic ceramic fuel cells. Herein, we demonstratethat this limitation can be conciliated by using a triple-dopingstrategy in a BaZr0.1Ce0.7Y0.2O3-delta(BZCY) electrolyte, where thetriply doped BaCe0.7Sn0.1Dy0.15Cu0.05O3-delta(BCSDCu) exhibitsbetter chemical stability and conductivity and lower sinteringtemperature compared with the pristine BZCY. The phase-pureBCSDCu can be obtained at the sintering temperature of 1100 degrees Cprepared by solid-state reaction. The dense BCSDCu (>95%) isachieved at 1350 degrees C, which is significantly lower than the 1550 degrees Cof BZCY. The BCSDCu presents competitive proton conductivityof 13.6 mS cm-1under a moist H2atmosphere at 600 degrees C. The anode-supported single cell with the BCSDCu (approximate to 40 mu m) as theelectrolyte reaches the highest power density of 390 mW cm-2at 600 degrees C. On the basis of the distribution of relaxation time analysis,we not only distinguish the contribution of grain and grain-boundary conductivities but also identify the rate-determining step of thesingle-cell performance. The protonic conductivities, mechanical properties, and impurity clean parts induced by grain size effects arediscussed for the BCSDCu proton conductor

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