Ionic Conduction and Application of Ba1.03Ce0.8Tm0.2O3−α Ceramic |
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Authors: | Ligan Qiu Maoyuan Wang |
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Institution: | School of Chemistry and Chemical Engineering, Yancheng Teachers University, Yancheng, Jiangsu 224051, China |
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Abstract: | Ba1.03Ce0.8Tm0.2O3?α ceramic with orthorhombic perovskite structure was prepared by conventional solid‐state reaction. The conductivity and ionic transport number of Ba1.03Ce0.8Tm0.2O3?α were measured by ac impedance spectroscopy and gas concentration cell methods in the temperature range of 500–900°C in wet hydrogen and wet air. Using the ceramic as solid electrolyte and porous platinum as electrodes, the hydrogen‐air fuel cell was constructed, and the cell performance was examined at 500–900°C. The results indicate that the specimen is a pure ionic conductor with the ionic transport number of 1 at 500–900°C in wet hydrogen. In wet air, the specimen is a mixed conductor of proton, oxide ion and electron hole. The protonic transport numbers are 0.071–0.018, and the oxide ionic transport numbers are 0.273–0.365. The conductivities of Ba1.03Ce0.8Tm0.2O3?α under wet hydrogen, wet air or fuel cell atmosphere are higher than those of Ba1.03Ce0.8RE0.2O3?α (RE?Y, Eu, Ho) reported previously by us. The fuel cell can work stably. At 900°C, the maximum power output density is 122.7 mW·cm?2, which is higher than that of our previous cell using Ba1.03Ce0.8RE0.2O3?α (RE?Y, Eu, Ho) as electrolyte. |
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Keywords: | Ba1 03Ce0 8Tm0 2O3− α ionic conductor ac impedance gas concentration cell fuel cell |
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