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0.7BiFeO3-0.3BaTiO3+1mol% MnO2(0.7BFO-0.3BTO) ceramics were synthesized by conventional solid-state powder method under different calcination temperatures (Tcal) between 770 and 830 °C. The phase structure, microstructure, and ferroelectric and piezoelectric properties changed greatly depending on the applied Tcal. Benefitting from the formation of low defect levels and large grain size and an appropriate morphotropic phase boundary (MPB) with the rhombohedral-to-pseudocubic phase ratio = 49.1 : 50.9, BFO-BTO ceramics calcined at 785 °C showed the best ferroelectric, piezoelectric, and insulating properties (Pr = 23.1 μC/cm2, EC = 25.8 kV/cm, d33 = 167.8 pC/N, kp = 0.342%). Above Tcal = 800 °C, however, the ferroelectric and piezoelectric properties deteriorated because volatilization of Bi and reduction of Fe caused a poor insulating property and high degree of chemical inhomogeneity. Moreover, the ceramics calcined at 785 °C showed a high Curie temperature (TC) of 509.2 °C and excellent thermal aging resistance of d33 up to 450 °C, demonstrating great potential for use in high-temperature applications. 相似文献
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Takaaki Tsurumi Shuichi Ozawa Satoshi Wada 《Journal of Sol-Gel Science and Technology》2003,26(1-3):1037-1040
Pb(Zr0.53Ti0.47)O3 (PZT) films of 10 to 50 m in thickness were prepared by a new sol-gel process using an interfacial polymerization technique. The interfacial polymerization process is that an alkoxide precursor solution is poured on the surface of water in a container to form a gel film at the interface between the two immiscible liquids. The precursor solution was prepared by adding PZT alkoxide solution, PZT powders coated with Pb5Ge3O11 (PG), and a surfactant into hexane solvent. After the polymerization at the interface, the gel films were gently placed on a silicon substrate by draining the water in the container. The gel films containing PZT powders were sintered at 950°C for 10 min to obtain crystallized PZT films. The remanent polarization of a PZT thick film was 33.1 C/cm2. The piezoelectric d
33 constant measured with a Mach-Zehnder interferometer was 225 pm/V and was independent of frequency from 0.2 to 3 kHz. 相似文献
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The microdamage of porous transversely isotropic piezoelectric materials under complex macrostress is studied. The microdamages are modeled by pores. The damage of a microvolume is defined by the generalized Huber-Mises failure criterion for a transversely isotropic medium. The ultimate strength is a random function of coordinates with exponential or Weibull distribution. The stress-strain state and effective properties of the material are determined from the stochastic equations of electroelasticity. The deformation and microdamage equations are closed by the porosity balance equations. Deformation curves are plotted for two values of macrostrain or macrostress and different values of electric intensity. The influence of electric intensity on the microdamage of piezoelectric materials is studied__________Translated from Prikladnaya Mekhanika, Vol. 41, No. 3, pp. 79–92, March 2005. 相似文献
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K.S. Challagulla 《哲学杂志》2013,93(14):1197-1222
A micromechanical model based on the asymptotic homogenization technique has been developed to predict the complete elastic, dielectric and piezoelectric properties of a general 2-2 layered piezoelectric composite where the constituent phases are elastically anisotropic and piezoelectrically active. Two classes of layered piezoelectric composites (i.e. longitudinally and transversely layered) are considered in two widely different ceramic- and polymer-based systems and their effective properties are obtained in the limits of both large-volume (i.e. bulk) and small-volume (i.e. thin-film) systems. It is demonstrated that: (i) in the bulk, ceramic–ceramic layered composite system, the elastic, piezoelectric, and dielectric properties of the composites vary linearly with volume fraction of the second phase, while in the bulk ceramic–polymer layered composite system, the corresponding properties vary non-linearly with volume fraction of the second phase; (ii) in the prismatic (thin-film) layered piezoelectric composite system, the non-vanishing, effective elastic, piezoelectric and dielectric properties vary linearly with the volume fraction of the second phase for both the longitudinally and transversely layered composite structures in the ceramic–ceramic and the ceramic–polymer composite systems; (iii) the ceramic–polymer piezoelectric layered composites that incorporate a low density polymeric phase with lower acoustic impedance generally exhibit enhanced piezoelectric coupling constants and lowered acoustic impedance; (iv) the longitudinally layered composites exhibit higher piezoelectric coupling constants and lower acoustic impedance compared to that of the transversely layered composites; and (v) the best combination of properties for applications such as hydrophones (i.e. the highest piezoelectric coupling constants and the lowest acoustic impedance) is obtained in the ceramic–polymer, longitudinally layered, thin-film, piezoelectric composites. 相似文献
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智能结构有限元动力模型的建立及主动振动控制和抑制 总被引:4,自引:1,他引:4
采用一种新的压电板单元,建立了含有分布压电传感元件和执行元件结构(智能结构)的有限元动力模型。利用两种反馈控制律,研究了智能结构振动控制与抑制的问题,并提出了智能结构主动振动控制和抑制的一种方法。最后,提供了数值示例,说明本文提出方法的应用。 相似文献
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H. Sahota 《Continuum Mechanics and Thermodynamics》2004,16(1-2):163-175
Ferroelectric materials exhibit complex behaviour upon electric and mechanical loading. Their change of polarization and length is accompanied by hysteresis. The so-called butterfly loop characterizing the strain due to an applied electric field is striking. As these materials are used in technical applications as sensors, actuators, and non-volatile memory units, the ability to simulate these hysteretic phenomena is important. Here, a one-dimensional model is proposed that is capable of describing the qualitative behaviour of widely used perovskite-type ferroelectric materials.Received: 3 July 2003, Accepted: 10 July 2003 相似文献
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V. M. Shul'ga 《International Applied Mechanics》2005,41(7):766-769
An approach is proposed to calculate the natural frequencies and modes of vibrations of cylindrically anisotropic piezoelectric
cylinders. The frequency equation is derived, and the frequency spectrum is analyzed
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Translated from Prikladnaya Mekhanika, Vol. 41, No. 7, pp. 68–72, July 2005. 相似文献