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New two-layer Ruddlesden—Popper cathode materials for protonic ceramics fuel cells

New two-layer Ruddlesden—Popper (RP) oxide La 0.25 Sr 2.75 FeNiO 7− δ (LSFN) in the combination of Sr 3 Fe 2 O 7− δ and La 3 Ni 2 O 7 −δ was successfully synthesized and studied as the potential active single-phase and composite cathode for protonic ceramics fuel cells (PCFCs). LSFN with the tetrago...

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Published in:Journal of advanced ceramics 2021-10, Vol.10 (5), p.1052-1060
Main Authors: Ling, Yihan, Guo, Tianming, Guo, Yangyang, Yang, Yang, Tian, Yunfeng, Wang, Xinxin, Ou, Xuemei, Feng, Peizhong
Format: Article
Language:English
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Summary:New two-layer Ruddlesden—Popper (RP) oxide La 0.25 Sr 2.75 FeNiO 7− δ (LSFN) in the combination of Sr 3 Fe 2 O 7− δ and La 3 Ni 2 O 7 −δ was successfully synthesized and studied as the potential active single-phase and composite cathode for protonic ceramics fuel cells (PCFCs). LSFN with the tetragonal symmetrical structure ( I 4/ mmm ) is confirmed, and the co-existence of Fe 3+ /Fe 4+ and Ni 3+ /Ni 2+ couples is demonstrated by X-ray photoelectron spectrometer (XPS) analysis. The LSFN conductivity is apparently enhanced after Ni doping in Fe-site, and nearly three times those of Sr 3 Fe 2 O 7 −δ , which is directly related to the carrier concentration and conductor mechanism. Importantly, anode supported PCFCs using LSFN-BaZr 0.1 Ce 0.7 Y 0.2 O 3 −δ (LSFN-BZCY) composite cathode achieved high power density (426 mW·cm −2 at 650 °C) and low electrode interface polarization resistance (0.26 Ω·cm 2 ). Besides, distribution of relaxation time (DRT) function technology was further used to analyse the electrode polarization processes. The observed three peaks (P1, P2, and P3) separated by DRT shifted to the high frequency region with the decreasing temperature, suggesting that the charge transfer at the electrode-electrolyte interfaces becomes more difficult at reduced temperatures. Preliminary results demonstrate that new two-layer RP phase LSFN can be a promising cathode candidate for PCFCs.
ISSN:2226-4108
2227-8508
DOI:10.1007/s40145-021-0488-8