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以PZT 95/5陶瓷为例,概述了铁电陶瓷在脉冲能源上的应用及材料对能源性能的影响.主要包括陶瓷的制备及性能、陶瓷的冲击放电机理和陶瓷的冲击放电效应及影响因素.通过比较我们认为,陶瓷的研制,特别是密度的改变对陶瓷的力学及电学性能影响较大.陶瓷冲击加载下的新应用,将带动陶瓷各方面性能的深入研究.

参考文献

[1] Fleddermann C.B.;Nation J.A. .Ferroelectric sources and their application to pulsed power: a review[J].IEEE Transactions on Plasma Science,1997(2):212-220.
[2] ПрищеnенкоАБ;ТретьяковДВ .Функционированиегенераторачастотысрабочимтеломизферромагнетикаисегнетоэлектрика[J].ЭЛЕКТРИЧЕСТВО,2000,4:61.
[3] Neilson F W .Effects of strong shocks in ferroelectric materials[J].Bulletin of the American Physical Society,1957,2:302.
[4] Bauer F;Vollrath K;L Eyraud et al.Ferroelectric energy conversion with PZT ceramics under shock loading[J].Journal of the American Ceramic Society,1980,63:268.
[5] Voigt J A;Sipola D L;Ewsuk K G et al.Solution Synthesis and Processing of PZT materials for Neutron Generator applications[R].SAND Report 98-2750,Sandia National Laboratories,1998.
[6] Haun M J;Furman E;Jang S J et al.Thermodynamic theory of the lead zirconate-titanate solid solution system,part Ⅰ:phenomenology[J].Ferroelectrics,1989,99:13.
[7] Fritz I J;Keck J D .Pressure-temperature phase diagrams for several modified lead zirconate ceramics[J].Journal of Chem Solids,1978,39:1163.
[8] Bruce A. Tuttle;Pin Yang;John H. Gieske .Pressure-Induced Phase Transformation of Controlled-Porosity Pb(Zr_(0.95)Ti_(0.05))O_3 Ceramics[J].Journal of the American Ceramic Society,2001(6):1260-1264.
[9] Shock wave compression of the ferroelectric ceramic Pb_(0.99)(Zr_(0.95)Ti_(0.05))_(0.98)Nb_(0.02)O_(3): Hugoniot states and constitutive mechanical properties[J].Journal of Applied Physics,2003(1):573-588.
[10] Setchell R E;Tuttle B A;Voigt J A.Microstructural effects on the shock response of PZT95/5[A].,2004:180.
[11] Furnish M D;Robbins J;Trott W M.Multi-dimensional validation impact tests on PZT 95/5 and ALOX[A].,2002:205.
[12] Setchell RE .Shock wave compression of the ferroelectric ceramic Pb-0.99(Zr0.95Ti0.05)(0.98)Nb0.02O3: Depoling currents[J].Journal of Applied Physics,2005(1):3507-1-3507-16-0.
[13] Montgomery S T;Brannon R M;Robbins J.Simulation of the effects of shock stress and electrical field strength on shock-induced depoling of normally poled PZT 95/5[A].,2002:201.
[14] Brannon R M;Montgomery S T;Aidun J B.Macroand meso-scale modeling of PZT ferroelectric ceramics[A].,2002:197.
[15] Yang P;Moore R H;Lockwood SJ .Chem-Prep PZT 95/5 for Neutron Generator Applications:The Effect of Pore Former Type and Density on the Depoling Behavior of Chemically Prepared PZT 95/5 Ceramics[R].SAND Report 2003-3866,Sandia National Laboratories,2003.
[16] Yu-Jinchang .A TEM study of crystal and domain structures of Nb-doped 95/5 PZT ceramics[J].Journal of Applied Physiology,1982,29:237.
[17] 贺元吉,张亚洲,李传胪.爆电换能的理论分析[J].国防科技大学学报,2000(Z1):43.
[18] 张砚宇,杜金梅,袁万宗.低密度PZT-95/5陶瓷流体静压相变实验研究[J].高压物理学报,2002(04):291-296.
[19] Du J M;Yuan W Z;Dong Q D et al.Effects of lateral rarefaction wave on phase-Transition of PZT-95/5 ceramics under shock-wave[J].Ferroelectrics,2001,254(01):329.
[20] 刘高旻,谭华,袁万宗,王海晏,张毅.冲击加载下PZT-95/5陶瓷铁电-反铁电相变实验研究[J].高压物理学报,2002(03):231-236.
[21] 张福平,贺红亮,杜金梅,王海晏,刘高旻.PZT95/5铁电陶瓷晶粒度对冲击波作用下击穿电压的影响[J].无机材料学报,2005(04):1019-1024.
[22] Ken Frazier .Pathfinders':Neutron generators qualified,Sandia teams meet final deadline,celebrate[J].Sandia Lab News,2001,53(01):1.
[23] Voigt J A;GregoryG E K;Jill S et al.PZT 95/5 material development for neutron generator applications[R].SAND Report 2001-0030P,Sandia National Laboratories,2001.
[24] Samara G V;Hansen L V .The Properties and Physics of the Slim-Loop Ferroelectric (SFE) (Pb0.71 Ba0.29)0.99 (Zr0.707Ti0.293)0.98 Bi0.02O3[R].SAND Report 98-2275,Sandia National Laboratories,1998.
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