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    仇立干, 王茂元. Ionic Conduction and Fuel Cell Performance of Ba0.98Ce0.8Tm0.2O3-α Ceramic[J]. Chinese Journal of Chemical Physics , 2010, 23(6): 707-712. DOI: 10.1088/1674-0068/23/06/707-712
    Citation: 仇立干, 王茂元. Ionic Conduction and Fuel Cell Performance of Ba0.98Ce0.8Tm0.2O3-α Ceramic[J]. Chinese Journal of Chemical Physics , 2010, 23(6): 707-712. DOI: 10.1088/1674-0068/23/06/707-712

    Ionic Conduction and Fuel Cell Performance of Ba0.98Ce0.8Tm0.2O3-α Ceramic

    • The perovskite-type oxide solid solution Ba0.98Ce0.8Tm0.2O3-α was prepared by high tem-perature solid-state reaction and its single phase character was confirmed by X-ray diffrac-tion. The conduction property of the sample was investigated by alternating current impedance spectroscopy and gas concentration cell methods under different gases atmo-spheres in the temperature range of 500-900 oC. The performance of the hydrogen-air fuel cell using the sample as solid electrolyte was measured. In wet hydrogen, the sample is a pure protonic conductor with the protonic transport number of 1 in the range of 500-600 oC, a mixed conductor of proton and electron with the protonic transport number of 0.945-0.933 above 600 oC. In wet air, the sample is a mixed conductor of proton, oxide ion, and elec-tronic hole. The protonic transport numbers are 0.010-0.021, and the oxide ionic transport numbers are 0.471-0.382. In hydrogen-air fuel cell, the sample is a mixed conductor of proton, oxide ion and electron, the ionic transport numbers are 0.942-0.885. The fuel cell using Ba0.98Ce0.8Tm0.2O3-α as solid electrolyte can work stably. At 900 oC, the maximum power output density is 110.2 mW/cm2, which is higher than that of our previous cell using Ba0.98Ce0.8Tm0.2O3-α (x≤1, RE=Y, Eu, Ho) as solid electrolyte.
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