CONDENSED MATTER: ELECTRONIC STRUCTURE, ELECTRICAL, MAGNETIC, AND OPTICAL PROPERTIES |
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Depolarization and Electrical Response of Porous PZT 95/5 Ferroelectric Ceramics under Shock Wave Compression |
WANG Zhi-Zhu1, JIANG Yi-Xuan1, ZHANG Pan1, WANG Xing-Zhe1**, HE Hong-Liang2 |
1Key Laboratory of Mechanics on Disaster and Environment in Western China (Ministry of Education), College of Civil Engineering and Mechanics, Lanzhou University, Lanzhou 730000 2National Key Laboratory of Shock Wave and Detonation Physics, Institute of Fluid Physics, China Academy of Engineering Physics, Mianyang 621900
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Cite this article: |
WANG Zhi-Zhu, JIANG Yi-Xuan, ZHANG Pan et al 2014 Chin. Phys. Lett. 31 077703 |
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Abstract The release of bound charges by shock wave loading of poled lead zirconate titanate (PZT 95/5) ferroelectric ceramics can result in a high-power electrical energy output. In this study, a theoretical formulation describing the depolarization and electrical response of porous PZT 95/5 ceramics in the normal mode to shock wave compression loading perpendicular to the polarization direction is developed. The depoling process in porous poled PZT 95/5 ceramics is analyzed by using a parallel circuit consisting of a current source, capacitance, conductance and a circuit load. This modeling takes the effects of porosity on wave velocity and remanent polarization and dielectric constant into account, and the effects of variations in dielectric constant and conductivity in the shocked region are assessed. The output current characteristics of porous PZT 95/5 ceramics under short-circuit and resistive load conditions are analyzed and compared with the experiment, with the results showing that theoretical predictions taking into consideration the porosity of ferroelectric ceramics are in close agreement with the experimentally measured electrical response of porous PZT 95/5 under shock wave compression loading.
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Published: 30 June 2014
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[1] Tkach Y, Shkuratov S I, Talantsev E F, Dickens J C, Kristiansen M Altgilbers L L and Tracy P T 2002 IEEE Trans. Plasma Sci. 30 1665 [2] Lysne P C and Percival C M 1975 J. Appl. Phys. 46 1519 [3] Lysne P C 1977 J. Appl. Phys. 48 4565 [4] Mock W and Holt W H 1978 J. Appl. Phys. 49 5846 [5] Timmerhaus K D and Barber M S 1978 High Pressure Science and Technology (New York: Plenum Press) p 20 [6] Setchell R E 2002 Shock Compression of Condensed Matter-2001 (American Institute of Physics) p 19 [7] Du J M, Zhang Y, Zhang F P, He H L and Wang H Y 2006 Acta Phys. Sin. 55 2584 (in Chinese) [8] Jiang D D, Du J M, Gu Y and Feng Y J 2012 J. Appl. Phys. 111 104102 [9] Jiang D D, Du J M, Gu Y and Feng Y J 2012 J. Phys. D: Appl. Phys. 45 115401 [10] Lan C H, Peng Y F, Long J D, Wang Q and Wang W D 2011 Chin. Phys. Lett. 28 088301 [11] Dungan R H and Storz L J 1985 J. Am. Ceram. Soc. 68 530 [12] Tuttle B A, Yang P, Gieske J H, Voigt J A, Scofield T W, Zeuch D H and Olson W L 2004 J. Am. Ceram. Soc. 84 1260 [13] Setchell R E 2003 J. Appl. Phys. 94 573 [14] Setchell R E 2005 J. Appl. Phys. 97 013507 [15] Setchell R E 2007 J. Appl. Phys. 101 053525 [16] Zeng T, Dong X, Mao C, Zhou Z and Yang H 2007 J. Eur. Ceram. Soc. 27 2025 [17] Nie H C, Dong X, Feng N, Chen X, Wang G, Gu Y, He H and Liu Y 2010 Mater. Res. Bull. 45 564 [18] Reynolds C E and Seay G E 1962 J. Appl. Phys. 33 2234 [19] Ramakrishnan N and Arunachalam V S 1990 J. Mater. Sci. 25 3930 [20] Anderson O L 1979 J. Geophys. Res. 84 3537 [21] Mock W and Holt W H 1980 Ferroelectrics 23 39 [22] Banno H 1987 Am. Ceram. Soc. Bull. 66 1332 [23] Feng N, Nie H, Chen X, Wang G, Dong X and He H 2010 Curr. Appl. Phys. 10 1387 [24] Feng N, Gu Y, Liu Y, Nie H, Chen X, Wang G, He H and Dong X 2010 Acta Phys. Sin. 59 8897 |
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