| 研究生: |
胡佩麗 Hu, Pei-Lee |
|---|---|
| 論文名稱: |
鋇鈷及鋇鉍氧化物合成與熱電性質之研究 Synthesis & Thermoelectric properties of Barium Cobaltates & Barium Bismuthates |
| 指導教授: |
齊孝定
Qi, Xiao-Ding |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 材料科學及工程學系 Department of Materials Science and Engineering |
| 論文出版年: | 2015 |
| 畢業學年度: | 103 |
| 語文別: | 中文 |
| 論文頁數: | 71 |
| 中文關鍵詞: | BaCoO3 、BaBiO3 、熱電材料 、熱電係數 |
| 外文關鍵詞: | BaCoO3, BaBiO3, thermoelectric, Seebeck coefficient |
| 相關次數: | 點閱:87 下載:5 |
| 分享至: |
| 查詢本校圖書館目錄 查詢臺灣博碩士論文知識加值系統 勘誤回報 |
相對傳統的合金熱電材料而言,氧化物熱電材料在空氣環境中具有更好的化學穩定性,因而更適合於中高溫區的應用。本實驗以固態反應法合成兩種複合氧化物材料,即 BaCoO3 和 BaBiO3,探討其熱電性質,以及改變氧計量比或摻雜其他元素對熱電性質的影響。X-射綫繞射證實在 800℃ 於空氣中結燒 24 小時可得單一相之 BaCoO3。若將燒結溫度升至 900℃ 以上,樣品會形成一種缺氧的新相 BaCoO2.6,密度亦隨之減少。若再將樣品於 800℃ 退火,缺氧相會變囘 BaCoO3,證明為可逆相變。熱電測量顯示,若樣品燒結溫度為 800℃,在 BaCoO3 中摻雜鎳與鋅不僅會使電阻率降低,也會提高熱電係數。若燒結溫度為 950℃ 隨後在 800℃ 退火,雖然 X-射綫繞射顯示樣品仍為 BaCoO3 相,但摻雜鎳與鋅會使電阻率上升,熱電係數下降。前者的熱電係數在 300700K 為正值,而後者的熱電係數在 300500K 為負值,500K 以上轉變為正值,顯示有兩種類型載子共存的現象。BaCoO3 系列樣品所測得的熱電功率因數皆很低,最佳值在 973K 時僅為 23 μWm-1k-2。BaBiO3 的合成條件為 800℃ 在空氣中燒結 12 小時,隨後在 600℃ 於氧氣中退火 24 小時以降低電阻率,其數值在室溫時約為 104 cm,在 973K 降為 5.95 cm,但仍然太大而不適合於熱電應用。
Compared to the traditional thermoelectric alloys, oxide thermoelectrics have a better chemical stability in air and therefore are better suited for the applications in the mid to high temperature regions. In this thesis, two complex oxides, i.e. BaCoO3 and BaBiO3, were synthesized by the solid state reaction method and their potentials as the thermoelectric material were investigated. The influence of the oxygen stoichiometry and doping of other elements were also studied. X-ray diffraction (XRD) indicated that the BaCoO3 samples sintered at 800 C in air for 24 hrs had a pure phase. If the sintering temperature was raised to 900 C, an oxygen deficient phase, i.e. BaCoO2.6, was formed with a reduced density. The BaCoO3 phase could be recovered after the oxygen deficient phase was annealed at 800 C, indicating that the phase transition was reversible. Thermoelectric measurements showed that if the samples were prepared at 800 C, Ni or Zn doping would result in a decrease in electrical resistivity but an increase in Seebeck coefficient, however, if the samples were sintered at 900 C followed by annealing at 800 C, the Ni or Zn doping would result in opposite results although XRD indicated that both samples had the same BaCoO3 phase. The 800 C sintered samples had positive Seebeck coefficients at 300700 K, while the Seebeck coefficients of the 800 C annealed samples showed negative values at 300500 K and then turned into positive values over 500 K, indicating the coexistence of both types of charge carriers. All the BaCoO3 samples showed small power factors with the highest value of 23 Wm-1K-2. The BaBiO3 samples of a pure phase were sintered in air at 800 C for 12 hrs, followed by annealing at 600 C in oxygen for 24 hrs to decrease the electrical resistivity, which had the values of 104 cm at room temperature and 5.95 cm at 973 K that were far too large for the thermoelectric application.
[1] 黃振東、徐振庭, "熱電材料," 科學發展, 2013 年.
[2] M. G. K. K. R. Poeppelmeier, Prog .Solid state chem, vol. 36, p. 40.
[3] M. Shimada, Y. Takeda, H. Taguchi, F. Kanamaru, and M. Koizumi, "Growth of single crystals of BaFe4+O3(12L), BaNi4+O3(2L) and BaCo4+O3(2L) under high oxygen pressure," Journal of Crystal Growth, vol. 29, pp. 75-76, May 1975.
[4] N. Raghu, V. Ravi, and T. R. N. Kutty, "ZnO varistors with BaCoO3−x (0.12>x>0) as the only formulating phase," Materials Research Bulletin, vol. 26, pp. 261-268, April 1991.
[5] X. Li, Y. Luo, and X. Liu, "Preparation and electrical properties of perovskite ceramics in the system BaBi1−xSbxO3 (0≤x≤0.5)," Journal of Alloys and Compounds, vol. 509, pp. 5373-5375, 28 April 2011.
[6] D. D. Pollock, "Thermoelectricity: Theory, Thermometry, Tool,," American Society for Testing and Materials, Philadelphia, PA, vol. ASTM Special Technical Publication 852, 1985.
[7] T.J.Seebeck, "Magnetic polarization of metals and minerals," p. 265, 1823.
[8] D.M.Rowe, "CRC Handbook of Thermoelectrics," 1994.
[9] H. E. Duckworth, "Electricity and Magnetism," New York: Holt, Rinehart and Winston, pp. 180-181, 1960.
[10] M. Ohtaki, "Oxide Thermoelectric Materials for Heat-to-Electricity Direct Energy Conversion," Novel Carbon Resour. Sci. Newsl, 2010.
[11] Y. Yang, F. Y. Ma, C. H. Lei, Y. Y. Liu, and J. Y. Li, "Nonlinear asymptotic homogenization and the effective behavior of layered thermoelectric composites," Journal of the Mechanics and Physics of Solids, vol. 61, pp. 1768-1783, August 2013.
[12] H. A. F. Charles P. Poole, Richard J. Creswick, "Superconductivity," pp. 475-476, 2013.
[13] 葉建弦, "固態熱電材料在廢熱回收領域之應用," ITRI 工業技術研究院, 2014.
[14] C. Felser, K. Yamaura, and R. J. Cava, "The Electronic Structure of Hexagonal BaCoO3," Journal of Solid State Chemistry, vol. 146, pp. 411-417, September 1999.
[15] K. Yamaura, H. W. Zandbergen, K. Abe, and R. J. Cava, "Synthesis and Properties of the Structurally One-Dimensional Cobalt Oxide Ba1−xSrxCoO3 (0≤x≤0.5)," Journal of Solid State Chemistry, vol. 146, pp. 96-102, August 1999.
[16] V. Pardo, P. Blaha, M. Iglesias, K. Schwarz, D. Baldomir, and J. E. Arias, "Magnetic structure and orbital ordering in BaCoO3 from first-principles calculations," Physical Review B, vol. 70, p. 144422, 29 October 2004.
[17] B. Yan, M. Jansen, and C. Felser, "A large-energy-gap oxide topological insulator based on the superconductor BaBiO3," Nat Phys, vol. 9, pp. 709-711, November 2013.
[18] D. Marx, P. Radaelli, J. Jorgensen, R. Hitterman, D. Hinks, S. Pei, et al., "Metastable behavior of the superconducting phase in the BaBi1-xPbxO3 system," Physical Review B, vol. 46, pp. 1144-1156, 1992.
[19] Y. Horie, T. Fukami, and S. Mase, "First order structural phase transition in BaPb1−xBixO3 and the scaling law," Solid State Communications, vol. 62, pp. 471-474, May 1987.
[20] "Synthesis, structure and superconductivity in theBa1−-xKxBiO3-y system,"
Nature 333, pp. 836 - 838, 30 June 1988.
[21] "Synthesis of Ba1-xKxBiO3 ceramic specimens:Electron paramagnetic resonance and microwave absorption," Phys. Rev. B vol. 53, 27 September 1995.
[22] Y. Luo and X. Liu, "High temperature NTC BaTiO3-based ceramic resistors," Materials Letters, vol. 59, pp. 3881-3884, December 2005.
[23] J. Ryu, K.-Y. Kim, J.-J. Choi, B.-D. Hahn, W.-H. Yoon, B.-K. Lee, et al., "Highly Dense and Nanograined NiMn2O4Negative Temperature coefficient Thermistor Thick Films Fabricated by Aerosol-Deposition," Journal of the American Ceramic Society, vol. 92, pp. 3084-3087, 2009.