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Measuring Electrical Properties of Thin Film Fuel Cell Electrodes by In Situ Infrared Spectroscopy

机译:用原位红外光谱法测量薄膜燃料电池电极的电性能

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摘要

The mixed conducting perovskites (ABO_3) containing rare and alkaline earth metals on the A-site and a transition metal on the B-site are commonly used as cathodes for solid oxide fuel cells (SOFC).[1-4] To measure their electrical conductivity is very important to understand their electrochemical properties. Although the bulk electrical conductivity (specific conductance) of perovskite oxides has been intensively studied as a function of temperature or oxygen partial pressure (P_(02)),[5-8] in situ measurements of the conductivity of these materials in contact with the electrolyte as in a SOFC configuration have hardly been reported. To measure the in-plane conductivity of an electrode film on the electrolyte, a substrate with high resistance would be required for diminishing the leakage current through the substrate. Therefore, it is particularly difficult to measure the conductivity of electrodes on the electrolyte in a wide range of temperature since the electrolyte becomes highly conductive at high temperature. In addition, it is also hardly possible to reliably measure the (local) conductivity of films with insulating inhomogeneities such as pores or cracks by electrical methods. In this study, we report the electrical conductivity of perovskite La_0.6Sr_0. 4CoO_(3_δ) (LSC) thin films on yttria-stabilized zirconia (YSZ) electrolyte quantitatively obtained by in situ infrared (IR) spectroscopy. This method enables a reliable measurement of the electronic conductivity of the electrodes as part of the SOFC configuration regardless of leakage current through the substrate and cracks in the film, and avoids the necessity of preparing ohmic contacts to the film. We also show that IR spectra with applied external bias on the LSC film enable to determine the electrical conductivity of the film in the wide range of effective oxygen partial pressures.
机译:通常在固体氧化物燃料电池(SOFC)的阴极上使用混合导电钙钛矿(ABO_3),该混合钙钛矿在A位上包含稀土和碱土金属,在B位上包含过渡金属。[1-4]测量其电学电导率对于了解其电化学性质非常重要。尽管已经深入研究了钙钛矿氧化物的整体电导率(比电导)与温度或氧分压(P_(02))的关系,[5​​-8]这些材料与钙钛矿接触时的电导率的原位测量。几乎没有关于SOFC构造的电解质的报道。为了测量电解质上的电极膜的面内电导率,将需要具有高电阻的基板以减小通过基板的泄漏电流。因此,由于电解质在高温下变得高度导电,因此特别难以在宽温度范围内测量电极在电解质上的电导率。另外,也几乎不可能通过电学方法可靠地测量具有绝缘不均匀性例如孔或裂缝的膜的(局部)电导率。在这项研究中,我们报告了钙钛矿La_0.6Sr_0的电导率。通过原位红外(IR)光谱定量获得的氧化钇稳定氧化锆(YSZ)电解质上的4CoO_(3_δ)(LSC)薄膜。该方法使得能够可靠地测量作为SOFC配置一部分的电极的电子电导率,而不管通过基板的泄漏电流和薄膜中的裂缝如何,并且避免了与薄膜形成欧姆接触的必要。我们还表明,在LSC薄膜上施加外部偏压的红外光谱能够确定在宽范围的有效氧分压下薄膜的电导率。

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  • 来源
    《Advanced Materials》 |2012年第48期|6507-6512|共6页
  • 作者单位

    Max-Planck-Institute for Solid State Research Heisenbergstr. 1, D-70569 Stuttgart, Germany,Energy Materials and Convergence Research Department Korea Institute of Energy Research 102 Cajeongro, Yuseonggu;

    Max-Planck-Institute for Solid State Research Heisenbergstr. 1, D-70569 Stuttgart, Germany;

    Max-Planck-Institute for Solid State Research Heisenbergstr. 1, D-70569 Stuttgart, Germany;

    Max-Planck-Institute for Solid State Research Heisenbergstr. 1, D-70569 Stuttgart, Germany;

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