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Acta mater. 48 (2000) 4709–4714 www.elsevier.com/locate/actamat

GADOLINIA-DOPED CERIA AND YTTRIA STABILIZED ZIRCONIA INTERFACES: REGARDING THEIR APPLICATION FOR SOFC TECHNOLOGY
A. TSOGA1*, A. GUPTA1, A. NAOUMIDIS1 and P. NIKOLOPOULOS2
Institut fur Werkstoffe und Verfahren der Energietechnik (IWV1), Forschungszentrum Julich, D-52425 ¨ ¨ Julich, Germany and 2Chemical Engineering Department, University of Patras, GR 265 00 Patras, Greece ¨
1

Abstract—For solid oxide fuel cells (SOFCs) operating at intermediate temperatures the adjacency of the state-of-the-art yttria-stabilized zirconia (YSZ) electrolyte with ceria-based materials to both anodic and cathodic sides is regarded as crucial for the effectiveness of the cell. Solid-state reaction, however, and interdiffusion phenomena between YSZ and ceria-based materials can cause degradation of the electrolyte. When a gadolinia-doped-ceria (GDC) layer is used to protect YSZ against interaction with Co-containing cathodes, an unfavorable solid state reaction at the YSZ–GDC interface can be efficiently suppressed when a thin ( 1 µm thick) interlayer with nominal composition of Ce0.43Zr0.43Gd0.10Y0.04O1.93 is incorporated at the interface. When ceria is to be employed at the electrolyte–anode interface to reduce polarization losses, use of a ceria–40% vol Ni cermet is recommended, since suppression of the reactivity between YSZ and ceria can also be achieved in the presence of Ni. © 2000 Acta Metallurgica Inc. Published by Elsevier Science Ltd. All rights reserved. Keywords: Solid oxide fuel cells; Interface; Diffusion; Microstructure

1. INTRODUCTION

Reduction of the operation temperature of solid oxide fuel cells (SOFCs) from 900–1000°C to 700–800°C is of great importance because it means both a prolonged stack lifetime and a cost reduction, since the use of low-cost metallic components as separator materials is then possible. However, for the operation of SOFCs at intermediate temperature to be technically



References: 1. Ohno, Y., Nagata, S. and Sato, H., Solid State Ionics, 1981, 3/4, 439. 2. Yamamoto, O., Takeda, Y., Kanno, R. and Noda, M., Solid State Ionics, 1987, 22, 241. 3. Kawada, T., Sakai, N., Yokokawa, H., Dokiya, M. and Ansai, I., Solid State Ionics, 1989, 50, 189. 4. Syskakis, E., Stochniol, G., Naoumidis, A., Nickel, H., in Proceedings of the 2nd International Conference on Ceramics in Energy Applications, The Institute of Energy, London, UK, 1996, p. 91. 5. Godickermeier, M. and Gauckler, L. J., J. Electrochem. Soc., 1998, 145, 414. 6. Uchida, H., Arisaka, S. and Watanabe, M., Electrochem. Solid-State Lett., 1999, 2, 428. 7. Marina, O. A., Primdahl, S., Bagger, C. and Mogensen, M., in Proceedings of the 5th International SOFC Symposium, Vol. 40, ed. U. Stimming. The Electrochemical Society, 1997, p. 540. 8. Tsoga, A., Gupta, A., Naoumidis, A., Skarmoutsos, D. and Nikolopoulos, P., Ionics, 1999, 4, 234. 9. Tsoga, A., Naoumidis, A., Gupta, A. and Stover, D., ¨ Materials Science Forum 1999, 308–311, 794. 10. Tsoga, A., Naoumidis, A., Jungen, W. and Stover, D., ¨ Journal of the European Ceramic Society, 1999, 19, 907. 11. Tsoga, A., Naoumidis, A., and Stover, D., Solid State Ion¨ ics, 1999, 5, 175. 12. Shannon, R. D., Acta Cryst., 1976, A32, 751. 13. Wagner, C., Z. Physik. Chem., 1933, B21, 25. 14. Choudhury, N. S. and Patterson, J. W., J. Electrochem. Soc., 1971, 118, 1398. sion Vt d ln P(O2) (A5) (rsel sion) P1(O2) When considering a multilayer composite electrolyte, the current density through the external circuit, IL, is equal to the current density of each of the layers, calculated for each one using Equation (A4): RT 4F IL Iext,i (A6) Considering equation (A6) for all the layers of the electrolyte the equation system we use is then solved for fixed values of IL on condition that oxygen partial pressure inside the electrolyte is continuously reduced from P1(O2) 0.21 atm on the oxidant side to the oxygen partial pressure on the fuel side, corresponding to that of an H2 gas with 3% H2O. The calculations were performed at 800°C. The oxygen partial pressures at the interface are then used to determine the terminal voltage VTOT of the cell given by the sum of the partial voltage at the ends of each layer: n VTOT 1 Vt,i (A7)

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