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铁电单晶Pb(Mg_(1/3)Nb_(2/3))O_3-0.32PbTiO_3的实验及本构模型研究 被引量:2

EXPERIMENTAL AND CONSTITUTIVE MODEL STUDY OF Pb(Mg_(1/3)Nb_(2/3))O_3-0.32PbTiO_3 RELAXOR FERROELECTRIC SINGLE CRYSTAL POLED ALONG〈001〉CRYSTALLOGRAPHIC DIRECTION
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摘要 对压力作用下沿[001]晶向极化的Pb(Mg_(1/3)Nb_(2/3))O_3-0.32PbTiO_3(PMN-0.32PT)弛豫型铁电单晶的应力应变行为进行了实验研究,实验结果表明铁电单晶〈001〉晶向的应力应变行为和铁电多晶有本质的不同,是传统的电畴翻转机理所难以解释的,所提出的极化旋转(相变)模型合理地解释了实验中观察到的现象;基于提出的极化旋转(相变)模型,采用细观力学方法建立了铁电单晶的细观本构模型.在模型中采用黏塑性公式描述铁电单晶可能的8个相变系统的相变行为.为了验证模型的可靠性,用该模型模拟了铁电单晶〈001〉晶向的应力应变实验曲线.计算表明,该模型能较好地模拟铁电单晶〈001〉晶向的相变行为. The stress and strain properties of 〈001〉 oriented PMN-0.32PT relaxor ferroelectric single crystals are investigated in this paper. Obtained results show that the stress and strain behavior along 〈001〉 crystallographic direction is different from that of the ferroelectric polycrystal. Polarization rotation models are developed to explain the observed behaviors of PMN-0.32PT. Based on the experimental phase transformation mechanism of ferroelectric single crystal, a constitutive model of ferroelectric single crystal is proposed using micromechanical method. In the model, the phase transformation systems on 8 possible sliding planes are characterized by a viscoplastic law. The behavior of ferroelectric single crystal is then derived from phenomenal crystallographic theory through the transformation strain on sliding planes. The developed model is applied to simulate the experimental stress-strain curve of 〈001〉 oriented PMN-0.32PT. It is shown that the model can faithfully capture the key characteristics of the observed constitutive behavior of 〈001〉 oriented PMN-0.32PT.
出处 《力学学报》 EI CSCD 北大核心 2007年第6期767-773,共7页 Chinese Journal of Theoretical and Applied Mechanics
基金 国家自然科学基金(90205030 10472088 10425210) 全国优秀博士论文基金(200129)资助项目.~~
关键词 弛豫型铁电单晶 极化旋转(相变) 黏塑性模型 本构 细观力学 relaxor ferroelectric single crystal, polarization rotation (phase transformation), viscoplastic model constitutive micro-mechanics
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参考文献19

  • 1Park SE, Shrout TR. Ultrahigh strain and piezoelectric behavior in relaxor ferroelectric based single crystal. J Appl Phys, 1997, 82(4): 1804-1811.
  • 2Uesu Y, Matsuda M, Yamada Y, et al. Symmetry of high piezoelectric Pb-based complex perovskites at the morphotropic phase boundary: Ⅰ. Neutron diffraction study on Pb(Zn1/3Nb2/3)O-3-9%PbTiO3. d Phys Soc Jpn, 2002, 71:960-965.
  • 3Priya S, Ryu J, Cross LE, et al. Investigation of the ferroelectric orthorhombic phase in the Pb(Zn1/3N2/3)O3- PbTiO3 system. Ferroelectrics, 2002, 274:121-126.
  • 4Singh AK, Pandey D. Evidence for MB and Mc phases in the morphotropic phase boundary region of (1- x)[Pb(Mg1/3 Nb2/3)Oa]-xPbTiO3: a rietveld study. Phys Rev B, 2003, 67:064102-064115.
  • 5Kiat JM, Uesu Y, Dkhil B, et al. Monoclinic structure of unpoled morphotropic high piezoelectric PMNPT and PZN-PT compounds. Phys Rev B, 2002, 65: 064106-064110.
  • 6Ye ZG. Crystal chemistry and domain structure of relaxor piezocrystals, curr opin solid state mater. Sci, 2002, 6: 35-44.
  • 7Noheda B, Cox DE, Shirane G, et al. Phase diagram of theferroelectric relaxor (1-x)Pb(Mg1/3 Nb2/3)O3-xPbTiO3 crystals. Phys Rev B, 2002, 66:054104.
  • 8Fu H, Cohen RE, Polarization rotation mechanism for ultrahigh electromechanical response in single-crystal piezoelectrics. Nature, 2000, 403:281-283.
  • 9Liu SF, Park SE, Shrout TR, et al. Electric field dependence of piezoelectric properties for rhombohedral 0.955Pb(Zn1/3 Nb2/3)O3-0.045PbTiO3 single crystals. J Appl Phys, 1999, 85:2810.
  • 10Bell AJ. Phenomenologically derived electric fieldtemperature phase diagrams and piezoelectric coefficients for single crystal barium titanate under fields along different axes. J Appl Phys, 2001, 89:3907-3914.

二级参考文献18

  • 1Fan D, Li CQ. Nonlinear electric-mechanical behavior of a soft PZT-51 ferroelectric ceramic. Journal of Materials Science, 1999, 34:4001~4010.
  • 2Zhou DY, Kamlah M, Munz D. Uniaxial compressive stress dependence of the high-field dielectric and piezoelectric performance of soft PZT piezocermics. J Mater Res, 2004,19(3): 834~841.
  • 3Chaplya PM, Carman GP. Dielectric and piezoelectric response of lead zirconate-lead titanate at high electric and mechanical loads in terms of non- 180° domain wall motion.J Appl Phys, 2001, 90:5278~5286.
  • 4Cao H, Evans A. Nonlinear deformation of ferroelectric ceramics. J Am Ceram Soc, 1993, 76(4): 890~895.
  • 5Schaufele AB, Hardtl KH. Ferroelectric properties of lead zirconate titanate ceramics. J Am Ceram Soc, 1996,79(10): 2637~2640.
  • 6Fett T, Munz D, Thun G. Stress-strain behaviour of a soft PZT ceramic under tensile and compression loading and a transverse electric field. Ferroelectric, 2003, 297:83~90.
  • 7Fett T, Munz D, Thun G. Nonsymmetry in the deformation behaviour of PZT. Journal of Materials Science Letters,1998, 17:261~265.
  • 8Fett T, Munz D, Thun G. Nonsymmetric deformation behaviour of lead zirconate titanate determined in bening tests. J Am Cerm Soc, 1998, 81(1): 269~272.
  • 9Fett T, Munz D. Measurement of Young's moduli for lead zirconate titanate(PZT) ceramics. Journal of Testing and Evaluation, 2000, 28(1): 27~35.
  • 10Burcsu E, Ravichandran G, Bhattacharya K. Large electrostrictive actuation of barium tianate single crystals.Journal of the Mechanics and Physics of Solids, 2004, 52:823~846.

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