储能科学与技术 ›› 2020, Vol. 9 ›› Issue (2): 415-424.doi: 10.19799/j.cnki.2095-4239.2020.0011

• 庆祝陈立泉院士八十寿辰专刊 • 上一篇    下一篇

固体氧化物燃料电池高催化活性阴极材料SrFeF x O3- x - δ

董旭1, 杜志鸿1,2, 张旸1, 李科云1, 赵海雷1,2()   

  1. 1. 北京科技大学材料科学与工程学院,北京 100083
    2. 新能源材料与技术北京市重点实验室,北京 100083
  • 收稿日期:2020-01-05 修回日期:2020-01-12 出版日期:2020-03-05 发布日期:2020-03-15
  • 通讯作者: 赵海雷 E-mail:hlzhao@ustb.edu.cn
  • 作者简介:董旭(1995—),女,硕士研究生,研究方向为固体氧化物燃料电池阴极材料,E-mail:kindadongxu@163.com
  • 基金资助:
    国家重点研发计划重点专项(2018YFB1502202);国家自然科学基金(21805006);中国博士后科学基金资助项目(2016M600041┫。)

SrFeF x O3- x - δ cathode with high catalytic activity for solid oxide fuel cells

DONG Xu1, DU Zhihong1,2, ZHANG Yang1, LI Keyun1, ZHAO Hailei1,2()   

  1. 1. School of Materials Science and Engineering, University of Science and Technology Beijing, Beijing 100083, China
    2. Beijing Municipal Key Laboratory of New Energy Materials and Technologies, Beijing 100083, China
  • Received:2020-01-05 Revised:2020-01-12 Online:2020-03-05 Published:2020-03-15
  • Contact: Hailei ZHAO E-mail:hlzhao@ustb.edu.cn

摘要:

该工作制备了F离子掺杂的SrFeF x O3- x - δ (SFF x x=0、0.125、0.25)阴极材料,研究了F离子掺杂对材料结构及电化学性能的影响。结果表明,F离子的引入可使材料在室温下保持立方结构,F离子掺杂显著提高SFF x 的电子电导率、降低材料的热膨胀系数、提高材料的氧表面交换系数和体扩散系数,降低电极反应的极化电阻,改善材料的电化学催化特性。电极反应动力学过程研究表明,F掺杂可显著促进氧分子的解离过程,以SFF x 与Sm0.2Ce0.8O2- δ (物质的量比1:1)的混合材料为复合阴极,以La0.9Sr0.1Ga0.8Mg0.2O3- δ (300 μm)为电解质并作为支撑体,NiO-Gd0.1Ce0.9O2- δ 为阳极组装单电池。研究发现,F掺杂提高了电池的功率密度,当x=0.25时,700 oC和 850 oC时最大功率密度分别可达446和962 mW·cm-2

关键词: 固体氧化物燃料电池, 阴极, 钙钛矿, 氟离子掺杂, 电极反应动力学过程

Abstract:

SrFeO3- δ is a widely studied cathode material for solid oxide fuel cells owing to its good mixed electronic and oxygen ionic conductivity and considerable catalytic activity. However, SrFeO3- δ usually has a tetragonal structure at room temperature, and the tetragonal-to-cubic phase transition at high temperatures produces volume change, which poses the risk of structural deterioration. In addition, its catalytic activity toward oxygen reduction needs to be improved further. In this study, fluorine substitution of oxygen was employed to modulate the lattice structure of SrFeO3- δ as a cathode material and improve its various properties. F-ion-doped SrFeF x O3- x - δ (SFF x , x = 0, 0.125, and 0.25) materials were synthesized via the sol-gel process. The effects of F ion doping on the lattice structure, thermal expansion coefficient, electrical conductivity, oxygen surface exchange coefficient, oxygen bulk diffusion coefficient, polarization resistance, electrode reaction kinetics, and cell performance were investigated through X-ray diffraction (XRD), scanning electron microscopy (SEM) and electrochemical characterization techniques. The results show that the partial substitution of O ions by F ions (x = 0.25) can stabilize the cubic structure of SrFeF x O3- x - δ at room temperature owing to a decreased tolerance factor, decreased iron valence, and increased Fe ion size. Both cell parameters and cell volume increase with F ion doping content. The F ion doping decreases the thermal expansion coefficient but increases the electrical conductivity of SFFx. With F ion doping, the oxygen surface exchange coefficient (K ex) and bulk diffusion coefficient (D chem) of the material improve, which is correlated with the effective reduction of the polarization resistance (R p) of the materials by F substitution. By monitoring the impedance change of each component process with a change in oxygen partial pressure, the electrode reaction kinetics study reveals that F ion doping considerably enhances the dissociation process of oxygen molecules on the surface of SFF x . For materials with an F-doping amount of x = 0.25, the R p value is 0.508, 0.173, 0.077, 0.039, and 0.023 Ω·cm2 at 650, 700, 750, 800, and 850 °C, respectively. Single cells were constructed using SFF x and Sm0.2Ce0.8O2- δ (1∶1) as the cathode, La0.9Sr0.1Ga0.8Mg0.2O3- δ (300 μm) as the electrolyte, La0.4Ce0.6O2- δ as the buffer layer, and NiO-Gd0.1Ce0.9O2- δ as the anode. Humidified H2 and air were fed as the fuel and oxidant, respectively. The cell tests show that the F ion doping significantly increases the peak power density of the cells. For materials with x = 0.25, the maximum power density can reach 446 and 962 mW·cm-2 at 700 °C and 850 °C, respectively.

Key words: solid oxide fuel cells, cathode, perovskite, fluorine doping, electrode reaction kinetics

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