| 研究生: |
李瑋志 Lee, Wei-Chei |
|---|---|
| 論文名稱: |
(BiFeO3-BaTiO3)系統之合成、特性、及介電性質 Synthesis, Characteristic, and Dielectric Properties of (BiFeO3-BaTiO3) System |
| 指導教授: |
黃啟原
Huang, Chi-Yuen |
| 學位類別: |
碩士 Master |
| 系所名稱: |
工學院 - 資源工程學系 Department of Resources Engineering |
| 論文出版年: | 2004 |
| 畢業學年度: | 92 |
| 語文別: | 中文 |
| 論文頁數: | 95 |
| 中文關鍵詞: | 無鉛壓電 |
| 外文關鍵詞: | lead free piezoelectric ceramics |
| 相關次數: | 點閱:42 下載:6 |
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近來由於環保意識高漲,使得含有對人體之健康有疑慮元素的材料將會被逐步禁用。於電子陶瓷中影響最大的將會是壓電陶瓷,由於現今壓電陶瓷所使用的材料最大宗為PZT,而這類含鉛之材料雖然早在數年前就被明令將被禁用,但由於其替代品開發之困難,故至今其限期不斷在延後,但尋找可替代之材料仍為現今刻不容緩之議題。
而(BiFeO3-BaTiO3) 系統,則因BaTiO3 具有鐵電及壓電性質,而BiFeO3也具有鐵電性質,因而其固溶系統被認為有機會具有良好之壓電行為。故本研究將針對本固溶系統做詳盡的晶體結構以及基本介電性質分析,並藉由實驗結果繼續探討其作為壓電材料之可能性。經實驗結果可確定下面幾點。第一,提出xBiFeO3-(1-x)BaTiO3) 之製程,並且可將燒結體密度達到94%以上。第二,詳盡說明本固溶系統晶體變化之過程,於x = 0.07 及0.68 分別將由etragonal 轉變為Cubic 再變為Hexagonal,且經由計算得到其晶格常數、晶格體積及理論密度值。第三,得到一系列成分於不同頻率下之介電常數,也同時由性質及結構說明了MPB之存在,並提出影響本系統電性質表現的主要因素為MPB及Fe3+之價數不穩定。第四,確定了此固溶系統具有壓電特性,且優於純BaTiO3。
Recently, because the raise of environmental sense making some materials containing with harmful health elements will be inhibited. The biggest influence of electric ceramics will be piezoelectric ceramics. Because the most important material of piezoelectric ceramics is PZT, and this containing Pb material have been inhibited
at few years before, but owning to the difficulty of finding the substitution make the time- limited is always be extended. In (BiFeO3-BaTiO3) system, because of BaTiO3 have piezoelectric and ferroelectric property, BiFeO3 have ferroelectric property, so we predict this solid solution system will have good performance in piezoelectric
property. In this research will detailed study in crystal structure and basic dielectric
property of this solid solution system. Depending on results, we will continue to study
the possibility of it applied in piezoelectric material. According to the results, we can
make sure the following points. First of all, providing a processing of (BiFeO3-BaTiO3) and it can make the relative density of sintering bulk up to 94%; Second, detailed show the transformation of this solid solution system, at x = 0.07 and
0.68 separately, it will from tetragonal transform to cubic and hexagonal. By calculating, we can get lattice parameters, lattice volume, and theoretical density; Third, getting dielectric constant at different frequency of each component, and from
property and structure are showing the existence of MPB. Bringing up the main factors affect electric property is MPB and the unstable valence of Fe3+. Fourth, confirming this solid solution system is piezoelectric and better than pure BaTiO3.
1. O. Muller and R. Roy, The Major Ternary Structural Families, Springer,
2. B. D. Cullity, Elements of X-Ray Diffraction, 2nd Ed.,Wiley, New
3. I. Sosnowska, P. Przenioslo, P. Fischer, and V. A. Murashov, “Neutron
Diffraction Studies of The Crystal and Magnetic Structures of BiFeO3
and Bi0.93La0.07FeO3,” J. Magn. & Magn. Mater., 160, 384-385, 1996.
4. A. S. Bhalla, R. Guo, and R. Roy, “The perovskite structure – a review
of its role in ceramic science and technology,” Mat. Res. Innovat., 4,
5. W. D. Kingery, H. K. Bowen, and D. R. Uhlmann, Introduction to
ceramics, 2nd Ed.,John Wiley and Sons, New York, 1976.
6. G. D. Achenbach, W. J. James, and R. Gerson, “Preparation of
Single-Phase Polycrystalline BiFeO3,” J. Am. Ceram. Soc., 50, 437,
7. Yu. E. Roginskaya, Yu. Ya. Tomashpol’skii, Yu. N. Venevtsev, V. M.
Petrov, and G. S. Zhdanov, “The Nature of the Dielectric and Magnetic
Properties of BiFeO3,” Soviet Phys. JETP., 44, 1418, 1966.
8. R. T. Smith, G. D. Achenbach, R. Gerson, and W. J. James, “Dielectric
Properties of Solid Solution of BiFeO3 with Pb(Ti, Zr)O3 at High
Temperature and High Frequency,” J. Appl. Phys., 39, 70, 1968.
9. M. M. Kumar, A. Srinivas, and S. V. Suryanarayana, “Structure
Property Relations in BiFeO3/BaTiO3 Solid Solution,” J. Appl. Phys.,
10. M. M. Kumar, and V. R. Palkar, “Ferroelectricity in a Pure BiFeO3
Ceramic,” Appl. Phys. Lett., 76, 2764-2766, 2000.
11. J. R. Teague, R. Gerson, and W. J. James, “Dielectric Hysteresis in
Single Crystal,” Solid State Comm., 8, 1073, 1970.
12. B. Jaffe, W. R. Cook, and H. Jaffe, Piezoelectric ceramics, William R.
Cook, Jr. and Hans Jaffe Gould Inc., Cleveland, 1971.
13. G. Arlt, D. Hennings, and G. With, “Dielectric Properties of
Fine-Grained Barium Titanate Ceramics,” J. Appl. Phys., 58,
1625, 1985.
14. C. G. Bergeron and S. H. Risbud, Introduction to Phase Equilibria in
Ceramics, The American Ceramic Society Inc., Columbus, 1984.
15. I. H. Ismailzade, R. M. Ismailov, A. I. Alekberov, and F. M. Salaev,
“Investigation of the Magnetoelectric Effect in Solid Solution of the
System BiFeO3-BaTiO3 and BiFeO3-PbTiO3,” Phys. Stat. Sol. (a), 68,
K81, 1981.
16. M. M. Kumar, S. Srinath, G. S. Kumar, and S. V. Suryanarayana,
“Spontaneous Magnetic Moment in BiFeO3-BaTiO3 Solid Solutions at
Low Temperature,” J. Magn. Magn. Mater., 188, 203, 1998.
17. M. M. Kumar, and S. V. Suryanarayana, “Relaxor Behavior in
BaTiO3,” J. Appl. Phys., 76, 1330-1333, 2000.
18. M. M. Kumar, M. B. Suresh, and S. V. Suryanarayana, “Dielectric
Relaxation in Ba0.96Bi0.04Ti0.96Fe0.04O3,” J. Appl. Phys., 84, 6811-6185,
1998.
19. K. Ueda, H. Tabata, and T. Kawai, “Coexistence of Ferroelectricity
and Ferromagnetism in BiFeO3-BaTiO3 Thin Films at Room
Temperature,” J. Appl. Phys., 75, 555-557, 1999.
20. 吳朗,電子陶瓷(壓電),全欣科技圖書,31-32,1994。
21. C. Y. Huang, Thermal expansion behavior of sodium zirconium
phosphate structure type materials, Ph. D. thesis, The Pennsylvania
State University, U. S. A.,1990.
22.向性一,鈦酸鋇粉末鐵電區與介電性質之研究。國立成功大學礦
冶及材料科學研究所博士論文,1995。