首页> 美国卫生研究院文献>Sensors (Basel Switzerland) >Equivalent Circuit Model of Low-Frequency Magnetoelectric Effect in Disk-Type Terfenol-D/PZT Laminate Composites Considering a New Interface Coupling Factor
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Equivalent Circuit Model of Low-Frequency Magnetoelectric Effect in Disk-Type Terfenol-D/PZT Laminate Composites Considering a New Interface Coupling Factor

机译:考虑新的界面耦合因子的盘形Terfenol-D / PZT层状复合材料的低频磁电效应等效电路模型

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摘要

This paper describes the modeling of magnetoelectric (ME) effects for disk-type Terfenol-D (Tb0.3Dy0.7Fe1.92)/PZT (Pb(Zr,Ti)O3) laminate composite at low frequency by combining the advantages of the static elastic model and the equivalent circuit model, aiming at providing a guidance for the design and fabrication of the sensors based on magnetoelectric laminate composite. Considering that the strains of the magnetostrictive and piezoelectric layers are not equal in actual operating due to the epoxy resin adhesive bonding condition, the magnetostrictive and piezoelectric layers were first modeled through the equation of motion separately, and then coupled together with a new interface coupling factor kc, which physically reflects the strain transfer between the phases. Furthermore, a theoretical expression containing kc for the transverse ME voltage coefficient αv and the optimum thickness ratio noptim to which the maximum ME voltage coefficient corresponds were derived from the modified equivalent circuit of ME laminate, where the interface coupling factor acted as an ideal transformer. To explore the influence of mechanical load on the interface coupling factor kc, two sets of weights, i.e., 100 g and 500 g, were placed on the top of the ME laminates with the same thickness ratio n in the sample fabrication. A total of 22 T-T mode disk-type ME laminate samples with different configurations were fabricated. The interface coupling factors determined from the measured αv and the DC bias magnetic field Hbias were 0.11 for 500 g pre-mechanical load and 0.08 for 100 g pre-mechanical load. Furthermore, the measured optimum thickness ratios were 0.61 for kc = 0.11 and 0.56 for kc = 0.08. Both the theoretical ME voltage coefficient αv and optimum thickness ratio noptim containing kc agreed well with the measured data, verifying the reasonability and correctness for the introduction of kc in the modified equivalent circuit model.
机译:本文结合静电的优点,对低频下的碟形Terfenol-D(Tb0.3Dy0.7Fe1.92)/ PZT(Pb(Zr,Ti)O3)层压复合材料的磁电(ME)效应进行建模。弹性模型和等效电路模型,旨在为基于磁电层压复合材料的传感器的设计和制造提供指导。考虑到由于环氧树脂胶粘条件,磁致伸缩层和压电层的应变在实际操作中不相等,因此首先通过运动方程分别对磁致伸缩层和压电层建模,然后使用新的界面耦合因子耦合在一起kc,物理上反映了相之间的应变传递。此外,从ME叠层的改进等效电路推导了包含横向ME电压系数αv的kc和最大ME电压系数所对应的最佳厚度比noptim的理论表达式,其中界面耦合系数充当理想变压器。为了探究机械载荷对界面耦合系数kc的影响,在样品制造过程中,以相同的厚度比n将两组砝码(即100 g和500 g)放置在ME层压板的顶部。总共制造了22个具有不同配置的T-T模式盘式ME层压板样品。由测得的αv和直流偏置磁场Hbias确定的界面耦合系数对于500 g机械前负荷为0.11,对于100 g机械前负荷为0.08。此外,测得的最佳厚度比对于kc = 0.11为0.61,对于kc = 0.08为0.56。包含kc的理论ME电压系数αv和最佳厚度比noptim与实测数据吻合良好,验证了在改进的等效电路模型中引入k c 的合理性和正确性。

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