期刊文献+

Microstructure and Thermoelectric Properties of Bi- and Cu-Substituted Ca_3Co_4O_9 Oxides

Microstructure and Thermoelectric Properties of Bi- and Cu-Substituted Ca_3Co_4O_9 Oxides
下载PDF
导出
摘要 Bi- and Cu-substituted Ca3Co4O9 samples were prepared by conventional solid-state reaction method and the effect of element substitution on the microstructures and thermoelectric properties was investigated. Partial substitution of Cu for Co leads to an increase in electrical conductivity and a decrease in Seebeck coefficient due to the rise of hole concentration. The microstructure of Cu-substituted sample is almost unchanged compared with undoped Ca3Co4O9. On the other hand, partial substitution of Bi for Ca gives rise to a significant increase in the grain size, and c-axis-oriented structure can be formed in Ca2.7Bi0.3Co4O9, resulting in an obvious increase in electrical conductivity. Cu and Bi co-substitution further increases the grain growth and the electrical conductivity of Ca2.7Bi0.3Co3.7Cu0.3O9. Thus, Cu and Bi co-substitution samples possess the optimal thermoelectric performance at high temperature and the highest value of power factor can reach 3.1×10^-4 Wm^-1.K^-2 at 1000 K. Bi- and Cu-substituted Ca3Co4O9 samples were prepared by conventional solid-state reaction method and the effect of element substitution on the microstructures and thermoelectric properties was investigated. Partial substitution of Cu for Co leads to an increase in electrical conductivity and a decrease in Seebeck coefficient due to the rise of hole concentration. The microstructure of Cu-substituted sample is almost unchanged compared with undoped Ca3Co4O9. On the other hand, partial substitution of Bi for Ca gives rise to a significant increase in the grain size, and c-axis-oriented structure can be formed in Ca2.7Bi0.3Co4O9, resulting in an obvious increase in electrical conductivity. Cu and Bi co-substitution further increases the grain growth and the electrical conductivity of Ca2.7Bi0.3Co3.7Cu0.3O9. Thus, Cu and Bi co-substitution samples possess the optimal thermoelectric performance at high temperature and the highest value of power factor can reach 3.1×10^-4 Wm^-1.K^-2 at 1000 K.
出处 《Journal of Materials Science & Technology》 SCIE EI CAS CSCD 2009年第1期105-108,共4页 材料科学技术(英文版)
基金 supported by the Foundation for University Key Teacher of Henan Province, China (2008136) Doctoral Fund of Henan Institute of Engineering(D2007011), China
关键词 CA3CO4O9 Element substitution MICROSTRUCTURE Thermoelectric properties Ca3Co4O9 Element substitution Microstructure Thermoelectric properties
  • 相关文献

参考文献10

  • 1E. Guilmeau,,H. Itahara,,T. Tani,,D. Chateigner,D. Grebille. Journal of Applied Physics . 2005
  • 2M. Prevel,,S. Lemonnier,,Y. Klien,,S. Hebert,,D. Chateigner,,B. Ouladdiaf,J.G. Noudem. Journal of Applied Physics . 2005
  • 3Y. Zhou,,I. Matsubara,,S. Horii,,T. Takeuchi,,R. Funa-hashi,,M. Shikano,,J. Shimoyama,,K. Kishio,,W. Shin,,N. Izu,N. Murayama. Journal of Applied Physics . 2003
  • 4J. Cheng,,Y. Sui,,H. Fu,,Z. Lu,,B. Wei,,Z. Qian,,J. Miao,,Z. Liu,,X. Huang,,R. Zhu,,X. Wang,W. Su. J. Alloy. Compd . 2006
  • 5J. Cheng,,Y. Sui,,H. Fu,,Z. Qian,,Z. Liu,,J. Miao,W. Su. Journal of Inorganic Materials . 2006
  • 6E. Guilmeau,,M. Mikami,,R. Funahashi,D. Chateigner. Journal of Materials Research . 2005
  • 7K. Park,,K.Y. Ko,,J.G. Kim,W.S. Cho. Materials Science and Engineering . 2006
  • 8R. Funahashi,,I. Matsubara,M. Shikano. Chemistry of Materials . 2001
  • 9Y. Li,,G.Y. Xu,M.P. Jiang. J. Mater. Sci. Tech-nol . 2006
  • 10Y. Liu,,Y. Lin,,Z. Shi,,C. Nan,Z. Shen. Journal of the American Ceramic Society . 2005

相关作者

内容加载中请稍等...

相关机构

内容加载中请稍等...

相关主题

内容加载中请稍等...

浏览历史

内容加载中请稍等...
;
使用帮助 返回顶部