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PZT95/5铁电陶瓷晶粒度对冲击波作用下击穿电压的影响 被引量:4

Influence of Grain Size on Breakdown Voltage of PZT95/5 Ferroelectric Ceramics under Shock Compression
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摘要 在气炮加载条件下,分别测试了两种晶粒度的PZT95/5铁电陶瓷样品在冲击波作用下的击穿电压,并采用Weibull分布分析了所获得数据.结果表明,PZT95/5铁电陶瓷在冲击波作用下的击穿电压分布可以用二参数Weibull分布模型描述,从击穿电压密度分布函数和失效率函数来看,晶粒度为2.5μm的PZT95/5样品的击穿电压分布优于晶粒度为7μm的PZT95/5样品击穿电压分布. Breakdown voltages of two kinds of PZT95/5 ferroelectric ceramics with different grain sizes were investigated under shock compression. Weibull distribution model was used to analyze the experimental data. The results show that the breakdown voltage of PZT95/5 samples can be described by two parameter Weibull distribution. According to the density function and failure probability function of the Weibull distribution, PZT95/5 ceramics with fine grains possess more optimum breakdown voltage distribution than PZT95/5 ceramics with coarse grains.
出处 《无机材料学报》 SCIE EI CAS CSCD 北大核心 2005年第4期1019-1024,共6页 Journal of Inorganic Materials
关键词 PZT95/5铁电陶瓷 击穿电压 冲击波 晶粒度 PZT95/5 ferroelectric ceramics shock compression breakdown voltage grain size
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  • 1Voigt J A, Sipola D L, et al. SAND98-2750, Sandia National Laboratories, Albuquerque, NM, 1998.7-8.
  • 2Storz L J, Dungan R H. SAND85-1612, Sandia National Laboratories, Albuquerque, NM, 1985.3-4.
  • 3Lysne P C. J. Appl. Phys., 1977, 48(1): 4565.
  • 4温殿英,林其文.冲击波压缩PZT-95/5铁电陶瓷的电介质击穿[J].高压物理学报,1998,12(3):199-206. 被引量:10
  • 5贺红亮.中国工程物理研究院流体物理研究所内部资料[Z].,2003..
  • 6Setchell R E, Montgomery S T, Chhabildas L C, et al. in Shock Compression of Condensed Matter-1999, In:Funish M D, et al. ed. AIP Conference Proceedings 429, 2000. 979-982.

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同被引文献43

  • 1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,2000,22(z1):43-48. 被引量:3
  • 2贺元吉,张亚洲,李传胪.冲击应力加载下PZT95/5电响应的试验研究[J].功能材料与器件学报,2004,10(2):245-250. 被引量:1
  • 3曾涛,董显林,毛朝梁,梁瑞虹,杨洪.孔隙率及晶粒尺寸对多孔PZT陶瓷介电和压电性能的影响及机理研究[J].物理学报,2006,55(6):3073-3079. 被引量:14
  • 4王永令 袁万宗 等.铁电体爆-电换能的实验研究[J].物理学报,1983,32(6):780-780.
  • 5Setchell R E. The Effect of Shock Stress and Field Strength on the Shock-Induced Depoled of Normally Poled PZT95/5 [A]. //Furnish M D. Shock Compression of Condensed Matter-1999 [C], NewYork: Elsevier Science Publishers B V,2000:979-982.
  • 6Viogt J A,Sipola D L. Solution Synthesis and Processing of PZT Materials for Neutron Generate Applications [R].SAND98-2750,1998.
  • 7Setchell R E. Effect of Initial Porosity on the Shock Response of Normally Poled PZT95/5 [A].//Furnish M D,Thadhani N N, Horie Y. Shock Compression of Condensed Matter-2001 [C]. NewYork: Elsevier Science Publishers B V, 2002 : 209-212.
  • 8Fleddermamm Charles B,Nation J A.Ferroelectric sources and their application to pulsed power:A Review.IEEE Trans on Plasma Science,1997,25(2):212
  • 9Прищеnенко АБ,Третьяков ДВ.Функционирование генератора частоты с рабочим теломиз ферромагнетика и сегнетоэлектрика.ЭЛЕКТРИЧЕСТВО,2000,4:61
  • 10Neilson F W.Effects of strong shocks in ferroelectric materials.Bull Am Phys Soc,1957,2:302

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