High Tc lead–free Ba (Zr0.52Ti0.48)O3 positive temperature coefficient of resistivity (PTCR) ceramic was produced by the standard solid state reaction technique. X–ray diffraction pattern confirms the formation of the tetragonal perovskite structure of the ferroelectric sample. The conduction and relaxation mechanisms of the piezoelectric ceramic have been studied on the basis of activation energy. The relaxation mechanism is investigated for this sample based on the peaks of the imaginary part of electrical impedance and modulus spectra. The Cole-Cole plots indicate that the grain effect is influenced by the increase of temperature up to 200 °C and disappeared beyond this temperature. The temperature versus electrical resistivity plots show that a phase transition occurs at the Curie temperature, Tc =150 °C. The ceramic exhibits a PTCR jump of almost two orders of magnitude starting at 150 °C and ending at 275 °C with a high temperature coefficient of resistivity of ~25 % per °C. The electrical resistivity measurements also reveal that the sample shows semiconducting behavior beyond 275 °C with the value of negative temperature coefficient of resistivity of ~ 0.6% per °C.
Published in | International Journal of Mechanical Engineering and Applications (Volume 2, Issue 1) |
DOI | 10.11648/j.ijmea.20140201.13 |
Page(s) | 11-17 |
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Copyright © The Author(s), 2014. Published by Science Publishing Group |
Relaxation Mechanism, Conduction Mechanism, Impedance Spectroscopy, Modulus Spectroscopy
[1] | T. Lin, C. Hu, I. Lin, Journal of the American Ceramic Society 73 (1990) 531–536. |
[2] | P. Xiang, H. Takeda, T. Shiosaki, Applied Physics Letters 91 (2007) 162904. |
[3] | S.E. Park and T.R. Shrout, Journal of Applied Physics 82(1997)1804–1811. |
[4] | H. Fu, R.E. Cohen, Nature (London) 403 (2000) 281–283. |
[5] | U. Weber, G. Greuel, U. Boettger, S. Weber, D. Hennings, R. Waser, Journal of the American Ceramic Society 84 (2001) 759–766. |
[6] | F. Moura, A.Z. Simoes, B.D. Stojanovic, M.A. Zaghetea, E. Longo, J.A. Varela, Journal of Alloys and Compounds 462 (2008) 129–134. |
[7] | R. Farhi, M. Marssi, A. Simon, J. Ravez, European Physics Journal B 9 (1999) 599–604. |
[8] | K. Aliouane, A.G. Laidoudi, A. Simon, J. Ravez, Solid State Ionics 7(2005) 1324–1332. |
[9] | J. Bera, S.K. Rout, Materials Letters 59 (2005) 135–138. |
[10] | P. W. Haayman, R.R. Dam, H. A. Klassen, Geramn Patent Number 929 350 (1955). |
[11] | W. Heywang, Solid-State Electronics 3 (1961) 51–58. |
[12] | G. H. Jonker, Solid State Electronics 7 (1964) 895–903. |
[13] | W. Heywang, Journal of Materials Science 6 (1971)1214–1224. |
[14] | J. Daniels, K.H. Hardtl, R. Wenicke, Philips Technical Review 38 (1978/79) 73–82. |
[15] | O. Saburi, Journal of the Physical Society Japan 14 (1959) 1159–1174. |
[16] | K. Werner, Physics Review 82 (1955) 549-550. |
[17] | F.D. Morrison, D.C. Sinclair, A.R. West, Journal of the American Ceramic Society 84 (2001) 531–538. |
[18] | H. Beltrán, E. Cordoncillo, P. Escribano, D.C. Sinclair, A.R. West, Journal of Applied Physics 98, (2005) 094102. |
[19] | D.C. Sinclair, A.R. West, Journal of Materials Science 29 (1994) 6061-6068. |
[20] | M. Kosec, V. Bobnar, M. Hrovat, J. Bernard, B. Malic, J. Holc, Journal of Materials Research 19 (2004) 1849–1854. |
[21] | J. R. Macdonald, Impedance Spectroscopy, Wiley, New York, 1987. |
[22] | T.A. Nealon, Ferroelectrics 76 (1987) 377–382. |
[23] | J. C. Maxwell, Electricity and Magnetism, Oxford University Press, London, 1973. |
[24] | C.G. Koops, Physical Review 83 (1951) 121–124. |
[25] | C.A. Guarany, L.H.Z. Pelaio, E.B. Araujo, K. Yukimitu, J.C.S. Moraes, J.A. Eiras, Journal of Physics : Condensed Matter 15 (2003) 4851–4858. |
[26] | H. S. Maiti, R. N. Basu, Materials Research Bulletin 21(1986)1107–1114. |
[27] | W. Heywang, Journal of the American Ceramic Society, 47 (1964) 484–490. |
APA Style
Md. Azizar Rahman, Abdul Quader, A. K. M. Akther Hossain. (2014). Relaxation and Conduction Mechanisms of High Tc Lead-Free Ba (Zr,Ti)O3 Positive Temperature Coefficient of Resistivity Ceramic Using Impedance Spectroscopy. International Journal of Mechanical Engineering and Applications, 2(1), 11-17. https://doi.org/10.11648/j.ijmea.20140201.13
ACS Style
Md. Azizar Rahman; Abdul Quader; A. K. M. Akther Hossain. Relaxation and Conduction Mechanisms of High Tc Lead-Free Ba (Zr,Ti)O3 Positive Temperature Coefficient of Resistivity Ceramic Using Impedance Spectroscopy. Int. J. Mech. Eng. Appl. 2014, 2(1), 11-17. doi: 10.11648/j.ijmea.20140201.13
AMA Style
Md. Azizar Rahman, Abdul Quader, A. K. M. Akther Hossain. Relaxation and Conduction Mechanisms of High Tc Lead-Free Ba (Zr,Ti)O3 Positive Temperature Coefficient of Resistivity Ceramic Using Impedance Spectroscopy. Int J Mech Eng Appl. 2014;2(1):11-17. doi: 10.11648/j.ijmea.20140201.13
@article{10.11648/j.ijmea.20140201.13, author = {Md. Azizar Rahman and Abdul Quader and A. K. M. Akther Hossain}, title = {Relaxation and Conduction Mechanisms of High Tc Lead-Free Ba (Zr,Ti)O3 Positive Temperature Coefficient of Resistivity Ceramic Using Impedance Spectroscopy}, journal = {International Journal of Mechanical Engineering and Applications}, volume = {2}, number = {1}, pages = {11-17}, doi = {10.11648/j.ijmea.20140201.13}, url = {https://doi.org/10.11648/j.ijmea.20140201.13}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ijmea.20140201.13}, abstract = {High Tc lead–free Ba (Zr0.52Ti0.48)O3 positive temperature coefficient of resistivity (PTCR) ceramic was produced by the standard solid state reaction technique. X–ray diffraction pattern confirms the formation of the tetragonal perovskite structure of the ferroelectric sample. The conduction and relaxation mechanisms of the piezoelectric ceramic have been studied on the basis of activation energy. The relaxation mechanism is investigated for this sample based on the peaks of the imaginary part of electrical impedance and modulus spectra. The Cole-Cole plots indicate that the grain effect is influenced by the increase of temperature up to 200 °C and disappeared beyond this temperature. The temperature versus electrical resistivity plots show that a phase transition occurs at the Curie temperature, Tc =150 °C. The ceramic exhibits a PTCR jump of almost two orders of magnitude starting at 150 °C and ending at 275 °C with a high temperature coefficient of resistivity of ~25 % per °C. The electrical resistivity measurements also reveal that the sample shows semiconducting behavior beyond 275 °C with the value of negative temperature coefficient of resistivity of ~ 0.6% per °C.}, year = {2014} }
TY - JOUR T1 - Relaxation and Conduction Mechanisms of High Tc Lead-Free Ba (Zr,Ti)O3 Positive Temperature Coefficient of Resistivity Ceramic Using Impedance Spectroscopy AU - Md. Azizar Rahman AU - Abdul Quader AU - A. K. M. Akther Hossain Y1 - 2014/01/30 PY - 2014 N1 - https://doi.org/10.11648/j.ijmea.20140201.13 DO - 10.11648/j.ijmea.20140201.13 T2 - International Journal of Mechanical Engineering and Applications JF - International Journal of Mechanical Engineering and Applications JO - International Journal of Mechanical Engineering and Applications SP - 11 EP - 17 PB - Science Publishing Group SN - 2330-0248 UR - https://doi.org/10.11648/j.ijmea.20140201.13 AB - High Tc lead–free Ba (Zr0.52Ti0.48)O3 positive temperature coefficient of resistivity (PTCR) ceramic was produced by the standard solid state reaction technique. X–ray diffraction pattern confirms the formation of the tetragonal perovskite structure of the ferroelectric sample. The conduction and relaxation mechanisms of the piezoelectric ceramic have been studied on the basis of activation energy. The relaxation mechanism is investigated for this sample based on the peaks of the imaginary part of electrical impedance and modulus spectra. The Cole-Cole plots indicate that the grain effect is influenced by the increase of temperature up to 200 °C and disappeared beyond this temperature. The temperature versus electrical resistivity plots show that a phase transition occurs at the Curie temperature, Tc =150 °C. The ceramic exhibits a PTCR jump of almost two orders of magnitude starting at 150 °C and ending at 275 °C with a high temperature coefficient of resistivity of ~25 % per °C. The electrical resistivity measurements also reveal that the sample shows semiconducting behavior beyond 275 °C with the value of negative temperature coefficient of resistivity of ~ 0.6% per °C. VL - 2 IS - 1 ER -