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1.
杨娜娜  陈轩  汪尧进 《物理学报》2018,67(15):157508-157508
磁电异质结是由铁磁和铁电材料通过连接层耦合而成,其磁电效应来源于铁电相的压电效应和铁磁相的磁致伸缩效应.相对于颗粒混相磁电复合材料,层状磁电异质结材料具有更高的磁电耦合系数和更低的介电损耗,使得其在磁场传感器、能量收集器、天线以及存储器等领域都有着巨大的应用前景.本综述重点总结了磁电异质结材料的发展历程以及相关应用领域的最新进展,最后评述了磁电异质结材料发展的挑战和前景展望.  相似文献   

2.
施展  南策文 《物理学报》2004,53(8):2766-2770
采用格林函数方法给出了三相复合材料的磁电系数的解析式,对稀土-铁合金/压电陶瓷/高分子(Terfenol-D/PZT/PVDF)三相颗粒复合材料的磁电系数进行了计算.计算结果给出了复合材料的磁电性能与材料显微结构的关系,包括三相颗粒复合材料的磁电性能随组分、颗粒的长径比、PZT颗粒的电极化方向以及外磁场的变化趋势,可为实验设计提供参考和指导.通过合理设计,三相磁电复合材料的性能可以达到数百mV/A.作为一种新的磁电复合材料,三相颗粒复合材料有望成为一种新型高性能易制备的磁电材料. 关键词: 磁电效应 复合材料 格林函数  相似文献   

3.
周剑平  施展  刘刚  何泓材  南策文 《物理学报》2006,55(7):3766-3771
磁致伸缩和压电复合材料通过机械力作用可获得较大的磁电效应,由Terfenol-D粉末与树脂黏接剂构成压磁相,和压电陶瓷PZT黏结在一起,形成1-3型柱状阵列结构,可获得很大的磁电转换系数.采用有限元方法,对此结构的复合材料进行静态分析.复合材料的介电常数和磁电系数的计算结果和实验数值一致,得到样品中应力、应变和电极化分布情况及其关系,并给出进一步提高磁电转换系数的途径,该种复合方式有望成为一种新型高性能的磁电结构. 关键词: 复合材料 磁电效应 有限元  相似文献   

4.
鲍丙豪  骆英 《物理学报》2011,60(6):67504-067504
基于纵向极化压电材料及纵向磁化磁致伸缩材料的压电和压磁方程与磁电元件运动方程,给出磁电元件开路电压表达式;鉴于压电材料高输出阻抗的特点,考虑测试仪器的有限输入阻抗和传输信号引线电缆电容,通过建立等效电路模型推出了非开路情况下磁电电压计算式,取不同材料参数对磁电电压进行了数值计算.研究表明,材料参数、电路参数对输出电压均产生影响.对磁伸材料两端面受非均匀偏置磁场产生外力的非自由边界磁电效应进行研究发现,恒外力作用使压电元件产生不可检测的稳恒电压. 关键词: 纵向极化 磁电效应 磁电元件 层叠材料  相似文献   

5.
于歆杰  吴天逸  李臻 《物理学报》2013,62(5):58503-058503
本文完整推导了无直流偏磁条件下, 磁致伸缩材料和压电材料黏接而得的磁电层状复合材料输出电压、电流、磁电系数表达式, 制备了多个样品并实现了电能无线传输系统. 对样品的测试结果验证了理论分析的正确性. 进一步试验结果表明: 磁电层状复合材料的输出具有倍频特性, 材料长度与谐振频率成反比, 谐振状态下样品可在20 Oe的磁场中输出接近100 V (有效值)开路电压, 样品最大传输功率为520 mW (此为该传输方式下公开报道的最大功率), 功率密度为1.21 W/cm3, 样品最大传输效率达35%, 30°以内的偏转角度对材料的输出无显著影响. 试验结果表明, 基于Metglas/PFC磁电层状复合材料是小体积、 小功率、 对传输效率不甚敏感的电能无线传输应用的一种非常有前景的实现方式. 关键词: 磁电复合材料 无线能量传输  相似文献   

6.
利用弹性力学模型,基于铁电相与铁磁相的本构方程,建立磁电复合材料的本构方程,推导2-2型非理想耦合的磁电双层、三层复合薄膜的纵向、横向磁电(ME)电压系数.研究铁磁相材料铁酸镍(NFO)和铁电相材料铌镁酸铅-钛酸铅(PMNT)复合的磁电效应,分析复合材料的磁电电压系数与PMNT体积分数、界面耦合参数、两相体积比及复合总层数的关系.结果表明两相材料的性能、体积分数以及耦合系数、复合层数都影响磁电电压系数.  相似文献   

7.
辛成舟  马健男  马静  南策文 《物理学报》2018,67(15):157502-157502
选用多种切型铌酸锂(LiNbO_3)单晶,研究了铁基非晶合金(Metglas)/LiNbO_3叠层复合材料基于伸缩-剪切模式的磁电耦合性能,揭示了铌酸锂单晶压电系数与复合材料剪切磁电耦合系数的对应关系,在使用铌酸锂xzt/30~?切型时得到了最优化剪切磁电系数.通过SrFe12O19薄磁带提供偏置磁场,Metglas/LiNbO_3磁电复合材料可在没有外加直流磁场时实现剪切磁电响应,并在0.991 MHz和3.51 MHz频率时分别测出了谐振磁电系数,有望将铌酸锂基剪切磁电复合材料用于高频磁场探测.  相似文献   

8.
楼国锋  于歆杰  卢诗华 《物理学报》2018,67(2):27501-027501
针对长片型磁电层状复合材料,提出了一种适用于准静态和动态磁场激励的引入界面耦合系数的等效电路模型,旨在为基于长片型磁电层状复合材料的传感器、换能器等器件的设计、制作和应用提供理论指导.考虑到磁电层状复合材料实际工作过程中磁致伸缩层和压电层的应变并不相同,首先利用运动方程分别对磁致伸缩层和压电层进行建模,提出了一个从物理上反映相间应变传递的界面耦合系数表达式,然后利用一个变比恰为界面耦合系数的理想变压器将两层材料的等效电路耦合,构成改进的磁电层状复合材料的等效电路模型,得到包含界面耦合系数的磁电电压系数和最佳层合比的表达式.对12个具有不同尺寸和负载条件的样品进行实验,制作过程中承受500g砝码负载的样品的界面耦合系数为0.15,最佳层合比为0.57;承受100g砝码负载的样品的界面耦合系数为0.10,最佳层合比为0.50.磁电电压系数和最佳层合比的实验值与各自包含界面耦合系数的理论值基本符合,证明了改进的等效电路模型的合理性和正确性.  相似文献   

9.
TbDyFe/PZT层状复合材料的磁电效应研究   总被引:7,自引:0,他引:7       下载免费PDF全文
万红  谢立强  吴学忠  刘希从 《物理学报》2005,54(8):3872-3877
磁致伸缩/压电复合材料通过磁致伸缩和压电效应的乘积而可以获得大的磁电效应.用磁控溅射方法制备了TbDyFe/PZT层状复合材料,实验测试了TbDyFe/PZT两层及TbDyFe/PZT/TbDyFe三层复合材料的磁电电压系数随周期磁场频率的变化关系,并采用有限元数值计算方法对两种材料的磁电电压系数进行了计算.研究结果表明,实验测试曲线与数值计算结果符合很好,所制备的层状复合材料在共振频率处存在最大的磁电电压系数值,由于两层板与三层板的振动模式不同,三层复合板的共振频率远高于两层复合板的共振频率.在非共振频率下,三层复合板的磁电转换效应高于两层复合板.有限元计算结果还显示,磁电层状复合材料的磁电电压系数随磁致伸缩层厚度的增加而增大. 关键词: 磁电效应 层合板 TbDyFe 有限元分析  相似文献   

10.
多铁性磁电器件研究进展   总被引:1,自引:0,他引:1       下载免费PDF全文
俞斌  胡忠强  程宇心  彭斌  周子尧  刘明 《物理学报》2018,67(15):157507-157507
多铁性材料可以实现力、电、磁等多物理场之间的相互耦合,在小尺寸、快速响应和低功耗的磁电器件领域具有重要的应用前景.在应用需求的推动下,以具有磁电耦合效应的多铁性材料为基础的磁电器件在设计、微纳加工和性能优化等方面的研究取得了持续的进展.本文简要介绍了基于磁电耦合效应的几种原型器件的最新进展,包括可调谐电感、滤波器、磁电存储器、能量回收器、磁电传感器和磁电天线等,分析总结了各种磁电器件的工作原理及其性能表现,讨论了当前多铁性磁电器件研究所面临的问题和挑战,并提出了改进磁电器件性能的研究方向.  相似文献   

11.
Considering the significant nonlinear magnetoelectric (ME) characteristics in laminated ME composites, we build a numerical model of magnetic-mechanical-electric coupling effect based on the nonlinear magnetostrictive constitutive relation. The change of the ME field coefficients with bias magnetic field predicted by this model shows good agreement with the experimental result, both qualitatively and quantitatively. Furthermore, this paper considers and predicts the magnetoelectric conversion charateristics of laminated ME composites, calculates and analyzes the influence of the thickness ratio of magnetostrictive layer, the geometrical size of laminated composites, the saturation magnetization, and the types of piezoelectric materials on the ME conversion coefficient of ME laminated composites. We believe that this research provides a theoretical basis for the production of magnetoelectric devices with good magnetoelectric conversion characteristics.  相似文献   

12.
A theoretical model is presented for frequency dependence of magnetoelectric (ME) effect in piezoelectric-magnetostrictive disk-ring composite structures. Expressions for ME voltage coefficients in piezoelectric-magnetostrictive (PE-MS) disk-ring and MS-PE disk-ring are obtained by solving elastodynamic equations. The calculated resonance frequency and frequency dependence of ME voltage coefficients are in good agreement with the experimental results. This model indicates better mechanical coupling in disk-ring structure than that in traditional layered structure, and this may be responsible for the enhancing ME effect. The analysis suggests the disk-ring composites structures are promising for magnetoelectric applications.  相似文献   

13.
This paper gives an overview about the basic ideas of magnetoelectric materials. Up to now single-phase materials show the magnetoelectric effect only below room temperature. Mixing a magnetostrictive with a piezoelectric component is a way to overcome this limitation. This delivers a composite which can exhibit a magnetoelectric effect even at room temperature and higher. Possible candidates for these composites (piezoelectric as well as magnetostrictive) are shown, examples from literature and own results are given. The most important coupling mechanism (magnetization, magnetostriction, local stress, charge) between the magnetostrictive and the piezoelectric phase are discussed. Hints for a direct coupling between the electric polarization and the magnetization are also presented. Different measurement methods for determining the magnetoelectric coefficient are discussed. Representative results as obtained on a technical useful composite between 50% Co-Ferrite+50% BaTiO3 are given. The behavior of a simple “mixed” structure with that of a “core-shell” structure is compared. The later gives a 20-times larger magnetoelectric coefficient.  相似文献   

14.
Magnetic, magnetoelectric and dielectric properties of multiferroic CoFe2O4–Pb(Fe1/2Nb1/2)O3 composites prepared as bulk ceramics were compared with those of tape cast and cofired laminates consisting of alternate ferrite and relaxor layers. X-ray diffraction analysis and Scanning Electron Microscope observations of ceramic samples revealed two-phase composition and fine grained microstructure with uniformly distributed ferrite and relaxor phases. High and broad maxima of dielectric permittivity attributed to dielectric relaxation were found for ceramic samples measured in a temperature range from −55 to 500 °C at frequencies 10 Hz–2 MHz. Magnetic hysteresis, zero-field cooled (ZFC) and field cooled (FC) curves, and dependencies of magnetization on temperature for both magnetoelectric composites were measured with a vibrating sample magnetometer in an applied magnetic field up to 80 kOe at 4–400 K. The hysteresis loops obtained for composites are typical of a mixture of the hard magnetic material with a significant amount of the paramagnet. The bifurcation of ZFC–FC magnetizations observed for both composites implies spin-glass behavior. Magnetoelectric properties at room temperature were investigated as a function of dc magnetic field (0.3–7.2 kOe) and frequency (10 Hz–10 kHz) of ac magnetic field. Both types of composites exhibit a distinct magnetoelectric effect. Maximum values of magnetoelectric coefficient attained for the layered composites exceed 200 mV/(cm Oe) and are almost three times higher than those for particulate composites.  相似文献   

15.
Lead-free multiferroic magnetoelectric composites consisting of ferrimagnetic Ni0.93Co0.02Mn0.05Fe1.95O4 (NMF) and ferroelectric Na0.5Bi0.5TiO3 (NBT) phases were synthesized by the solid-state sintering method. The presence of constituent phases in composites was confirmed by X-ray diffraction (XRD) and scanning electron microscopy (SEM). A systematic study of dc conductivity as a function of temperature (RT −450 °C) revealed that the conduction is due to small polarons. The effect of constituent phase variation on the dielectric constant and piezoelectric strength (d33) was examined. The composites exhibited typical magnetic hysteresis (MH) loops at room temperature. Furthermore, magnetoelectric (ME) output was evaluated as a function of applied magnetic field, which is a product property of the constituent phases. The compound 50% NMF–50%NBT is a new lead-free magnetoelectric composite with 155 μV/cm ME output, which may have potential applications.  相似文献   

16.
Our studies comprise electrical dielectric and magnetoelectric properties of CoFe2O4 (CFO) and Pb(Mg1/3Nb2/3)0.67Ti0.33O3 [PMN-PT] magnetoelectric composites. The individual phases were prepared by conventional ceramic method. The particulate composites of ferrite and ferroelectric phases were prepared in ferroelectric rich region. Presence of both the phases in the composites was confirmed using X-ray diffraction techniques. The scanning electron microscopic images recorded in backscattered mode were used to study the microstructure of composites. Lattice constant, dielectric constant, electrical resistivity, ferroelectric, and magnetic properties of individual as well as particulate composites were studied. Further the bi-layer composites were made using the discs obtained from the powders of individual phases where hot press technique was employed to obtain disc of individual phases. CFO phase used in bi-layer composites was obtained using chemical co-precipitation technique. Magnetoelectric (ME) measurements were carried out on both, particulate and layered magnetoelectric composites. Comparison of ME signal obtained from particulate and layered composites revealed that the layered composites gives superior magnetoelectric signal. ME data obtained for layered composites show good agreement with the theoretical model.  相似文献   

17.
Laminated magnetoelectric (ME) composites with various thickness ratios were optimized, fabricated and experimentally investigated in this work. The Terfenal-D/PZT specimens with optimal thickness ratio between the magnetostrictive phase and piezoelectric phase, and two other values were tested for their ME coupling performance. The coupling voltage output increases linearly with the increase of DC bias magnetic field. The ME voltage coefficient increases more than 100 times in the resonance state for the optimal laminate. The DC bias magnetic field affects the ME voltage coefficient significantly, and also has little effect on the resonant frequency. The strength of AC magnetic field also slightly affects the ME voltage coefficient in resonance state, but does not affect the resonant state under which the same DC magnetic field is required. The experimental results can help understand the coupling performance of ME composite under bias magnetic field and prompt the application of ME devices.  相似文献   

18.
We present systematic studies that comprise phase connectivity and dielectric, multiferroic (MF) and magnetoelectric (ME) properties of (x) Ni0.8Co0.2Fe2O4+(1−x) Pb(Mg1/3Nb2/3)0.67Ti0.33O3 [where x=0.15, 0.30 and 0.45] ME composites prepared by conventional solid-state reaction method. Scanning electron microscopic images of the composites predict different types of connectivity schemes viz 3-0, 3-1 and 3-3. The phase transition temperature of PMN-PT is independent of Ni0.8Co0.2Fe2O4 content. Room temperature P-E and M-H loops indicate the simultaneous existence of ferroelectric/magnetic ordering. In order to study the possibility of monitoring electrical ordering by means of a magnetic field, ME measurements were carried out. The composition-dependent phase connectivity was well co-related to formation of percolation path and inturn magnetoelectric output.  相似文献   

19.
Using the idea of “stress-field-controlled graded ferroelectrics”, a ring-shaped composite system of Pb(Zr,Ti)O3/Terfenol-D was fabricated. The magnetoelectric coupling of the composite was investigated. A resonant peak was observed at frequency of 69.6 kHz. The magnetoelectric frequency spectrum was found to relate to the polarity of the applied magnetic field, resulting in positive and negative magnetoelectric effects around the resonant point. Analysis shows that elastic resonance of the composite decides the resonant frequency and the magnetostrictive state of the Terfenol-D was responsible for the magnetoelectric coupling at different frequencies.  相似文献   

20.
Results of detailed structural, dielectric, magnetic and magnetoelectric studies of (x)PbZr0.52Ti0.48O3-(1−x)Mn0.3Co0.6Zn0.4Fe1.7O4 composites where x=65, 70, 75 and 80 are shown in this work. Manganese substituted cobalt ferrites are known to exhibit large strain derivative (dx/dH) and on the other hand substitution of Zn in pure cobalt ferrite is known to enhance its permeability μ and permittivity ε. The choice of ferrite as Mn, Zn simultaneously substituted cobalt ferrite (MCZFO) is made keeping in view that for good magnetoelectric (ME) voltage coefficient the magnetostrictive constituent phase of the composite should have large strain derivative (dx/dH) along with large permittivity and permeability. It is shown here that although the dielectric transition temperature changes significantly with change in the mole ratio of the two component phases, magnetic transition temperature (much less compared to the bulk cobalt ferrite) is relatively non-responsive to the changing molar ratio of the two component phases. In the vicinity of the magnetic transition temperature we observed an anomaly in tan δ vs. T plots, which indicates a possible magnetoelectric coupling in the samples. Magnetoelectric voltage coefficient (αE) has been measured using static magnetoelectric method. Highest magnetoelectric voltage coefficient (αE=0.312 mV/cmOe) is obtained for sample 80:20 at HDC=1000 Oe.  相似文献   

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