• 제목/요약/키워드: Magnetoelectric voltage coefficient

검색결과 15건 처리시간 0.018초

$CoFe_2O_4-PZT$ 복합체의 Magnetoelectric 효과 (Magnetoelectric Effect in$CoFe_2O_4-PZT$Composites)

  • 최임구;권순주;박수현;정윤희
    • 한국자기학회지
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    • 제7권6호
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    • pp.285-292
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    • 1997
  • Cobalt ferrite와 Pb(Zr, Ti) $O_{3}$ 복합체를 고상 반응법으로 제조하여, magnetoelectric 효과를 조사하였다. 소결 시간과 cobalt ferrite의 부피비가 증가함에 따라 magnetoelectric 전압 계수의 최대값이 증가하였다. 한편, 이 최댜값을 나타내는 자기장은 소결 시간 증가에 따라 낮은 쪽으로, cobalt ferrite 부피 증가에 따라 높은 쪽으로 이동하였다. 이러한 현상들은 각 상의 입자 크기 변화와 이에 따른 응력 전달 변화, 자화 및 분극 용이도로 설명되었다. 비화학당량 조성인 $Co_{1.02}$F $e_{1.98}$ $O_{4}$를 사용하여, 이제까지 발표된 최대 효과보다 약 30% 높은 0.174 V/cm Oe 의 magnetoelectric 전압 계수 값을 얻었다.얻었다.

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High Magnetoelectric Properties in 0.68Pb(Mg1/3Nb2/3)O3-0.32PbTiO3 Single Crystal and Terfenol-D Laminate Composites

  • Ryu, Jung-Ho;Priya, Shashank;Uchino, Kenji;Kim, Hyoun-Ee;Viehland, Dwight
    • 한국세라믹학회지
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    • 제39권9호
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    • pp.813-817
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    • 2002
  • Magnetoelectric(ME) laminate composites of $Pb(Mg_{1/3}Nb_{2/3})O_3-PbTiO_3 (PMN-PT)$ and Terfenol-D were prepared by sandwiching single crystals of PMN-PT between Terfenol-D disks. The magnetoelectric voltage coefficient (dE/dH) of the composite was determined to be 10.30 V/cm${\cdot}$Oe, at 1 kHz and under a dc magnetic bias of 0.4 T. The value of dE/dH is ∼80 times higher than either that of naturally occurring magnetoelectrics or artificially-grown magnetoelectric composites. This superior magnetoelectric voltage coefficient is attributed to the high piezoelectric voltage constant as well as the high elastic compliance of PMN-PT single crystal and the large magnetostrictive response of Terfenol-D.

Load Resistance Influence of Magnetoelectric Characteristics on NiZnFe2O4+PZT Composites for Magnetoelectric Sensors

  • Ryu, Ji-Goo;Chung, Su-Tae
    • 센서학회지
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    • 제22권6호
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    • pp.379-386
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    • 2013
  • The influences of the load resistance $R_L$ on the magnetoelectric (ME) characteristics of $NiZnFe_2O_4+PZT$ composite were investigated in the non-resonance frequency range. The ME coefficient peak increases with increasing $R_L$, but the frequency indicating the ME coefficient peak decreases with increasing $R_L$. The maximum output power peak is approximately $9.3{\times}10^{-10}mW/Oe$ near $R_L=3.3M{\Omega}$ at f=280 Hz, and the ME coefficient seems to be saturated at $R_L>20M{\Omega}$. This frequency shift effect of $R_L$ shows that the frequency range for an ME sensor application can be modulated with the appropriate value of $R_L$. The ME output voltage has a good linear response to the ac field Hac and shows fair stability over a range of temperatures. The measured non-linearity of this sample is approximately 0.8%. This sample will allow for a low-strength magnetic ac-field sensor. The result from this sample will serve as basic data for a signal-processing circuit system.

Effect of Bias Magnetic Field on Magnetoelectric Characteristics in Magnetostrictive/Piezoelectric Laminate Composites

  • Chen, Lei;Luo, Yulin
    • Journal of Magnetics
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    • 제20권4호
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    • pp.347-352
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    • 2015
  • The magnetoelectric (ME) characteristics for Terfenol-D/PZT laminate composite dependence on bias magnetic field is investigated. At low frequency, ME response is determined by the piezomagnetic coefficient $d_{33,m}$ and the elastic compliance $s_{33}^H$ of magnetostrictive material, $d_{33,m}$ and $s_{33}^H$ for Terfenol-D are inherently nonlinear and dependent on $H_{dc}$, leading to the influence of $H_{dc}$ on low-frequency ME voltage coefficient. At resonance, the mechanical quality factor $Q_m$ dependences on $H_{dc}$ results in the differences between the low-frequency and resonant ME voltage coefficient with $H_{dc}$. In terms of ${\Delta}E$ effect, the resonant frequency shift is derived with respect to the bias magnetic field. Considering the nonlinear effect of magnetostrictive material and $Q_m$ dependence on $H_{dc}$c, it predicts the low-frequency and resonant ME voltage coefficients as a function of the dc bias magnetic field. A good agreement between the theoretical results and experimental data is obtained and it is found that ME characteristics dependence on $H_{dc}$ are mainly influenced by the nonlinear effect of magnetostrictive material.

A High-sensitivity Passive Magnetic Transducer Based on PZT Plates and a Fe-Ni Fork Substrate

  • Li, Ping;Wen, Yumei;Jia, Chaobo;Li, Xinshen
    • Journal of Magnetics
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    • 제16권3호
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    • pp.271-275
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    • 2011
  • This paper proposes a magnetoelectric (ME) composite transducer structure consisting of a magnetostrictive H-type Fe-Ni fork substrate and piezoelectric PZT plates. The fork composite structure has a higher ME voltage coefficient compared to other ME composite structures due to the higher quality (Q) factor. The ME sensitivity of the fork structure reaches 12 V/Oe (i.e., 150 V/cm Oe). The fork composite with two PZT plates electrically connected in series exhibits over 5 times higher ME voltage coefficient than the output of the rectangle structure in the same size. The experiment shows the composite of a Fe-Ni fork substrate and PZT plates has a significantly enhanced ME voltage coefficient and a higher ME sensitivity relative to the prior sandwiched composite laminates. By the use of a lock-in amplifier with 10 nV resolution, this transducer can detect a weak magnetic field of less than $10^{-12}$ T. This transducer can also be designed for a magnetoelectric energy harvester due to its passive high-efficiency ME energy conversion.

The Dumb-bell Shaped Magnetostrictive/Piezoelectric Transducer

  • Li, Jianzhong;Wen, Yumei;Li, Ping
    • Journal of Magnetics
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    • 제16권4호
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    • pp.461-465
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    • 2011
  • Traditional magnetostrictive/piezoelectric laminate composites are generally in the regular geometries such as rectangles or disks. To explore properties of the irregular geometry magnetostrictive/piezoelectric transducer in the fundamental resonant frequency, a step dumb-bell shaped Magnetoelectric (ME) transducer is presented in this study. Both analytical and experimental investigations are carried out for the dumb-bell shaped transducer in the fundamental frequency. Comparing with the traditional rectangular transducer, the theory shows the resonant frequency of dumb-bell shaped transducer is reduced 31%, and the experiment gives the result of that is 37% which is independent of dc magnetic fields. The ratio of magnetoelectric voltage coefficient (MEVC) between the dumb-bell shaped and rectangular shaped transducers in theory is 66% comparing with that of in experiment is varying from 140% to 33% when the dc field is increased from 0 Oe to 118 Oe.

(1-x) [0.5PZT-0.25PNN-0.25PZN]- x [Ni0.9Zn0.1Fe2O4] 세라믹스의 압전/자성 성질 및 자기전기적 효과 (Piezoelectric/magnetic Properties and Magnetoelectric Effects in (1-x) [0.5PZT-0.25PNN-0.25PZN] - x [Ni0.9Zn0.1Fe2O4] Particulate Ceramic Composites)

  • 박영권;손세모;류지구;정수태
    • 한국전기전자재료학회논문지
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    • 제23권11호
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    • pp.869-874
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    • 2010
  • Magnetoelectric composites with compositions (1-x)[0.5PZT-0.25PNN-0.25PZN](ferroelectric) - x[$(Ni_{0.9}Zn_{0.1})Fe_2O_4$](ferrite) in which x varies as 0, 0.1, 0.2, 0.4, 0.6, 0.8, 1.0 were prepared by conventional ceramic process. The presence of two phases (ferroelectric phase with large grain and ferrite phase with small grain) in the particulate ceramic composites was confirmed by XRD, SEM and EDX. The ferroelectric and magnetic properties of the composites were studied by measuring the P-E and M-H hysterisis loop on the composite composition (x=0, 0.1, 0.2, 1), they were strongly affects of the phase content in composite. The magnetoelectric votage was measured as a function of DC magnetic field and the maximum magnetoelectric voltage coefficient of 14 mV/cm Oe was observed in x=0.2(80 mol% ferroelectric and 20 mol% ferrite phase).

Effect of Permeability and Piezomagnetic Coefficient on Magnetostrictive/Piezoelectric Laminate Composite

  • Wu, Zhiyi;Wen, Yumei;Li, Ping;Yang, Jin;Dai, Xianzhi
    • Journal of Magnetics
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    • 제16권2호
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    • pp.157-160
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    • 2011
  • The magnetostrictive material is magnetized in magnetic field and produces a nonuniform demagnetizing field inside and outside it. The demagnetization is decided by the permeability of magnetostrictive material and its size. The magnetoelectric performances are determined by the synthesis of the applied and demagnetizing fields. An analytical model is proposed to predict the magnetoelectric voltage coefficient (MEVC) of magnetostrictive/piezoelectric laminate composite using equivalent circuit method, in which the nonuniform demagnetizing field is taken into account. The theoretical and experimental results indicate that the MEVC is positively connected with the permeability and the piezomagnetic coefficient of magnetostrictive material. To obtain the maximum MEVC, both the permeability and the piezomagnetic coefficient of magnetostrictive material should be taken into account in selecting the suitable magnetostrictive material.

자기전기복합체의 비공진 및 공진 상태에서의 자기전기 결합 특성 평가 방법 (Demonstration of Magnetoelectric Coupling Measurement at Off-Resonance and Resonance Conditions in Magnetoelectric Composites)

  • ;류정호
    • 한국전기전자재료학회논문지
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    • 제35권4호
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    • pp.333-341
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    • 2022
  • 자기전기복합체(magnetoelectric, ME compositie)는 자왜재료와 압전재료의 결합현상을 이용하는 재료로서 지난 20여 년간 이론적, 실험적으로 많은 연구가 진행되어 왔다. 자기전기복합체의 출력특성은 구성하는 소재, 계면층, 복합체의 형상, 자기장하 진동모드 등의 많은 구성요소의 최적화를 통하여 급속히 향상되고 있다. 하지만 자기전기복합체의 자기전기 결합 특성 평가는 대부분의 연구들에서 구체적인 방법을 제시하지 않아 어떻게 측정한 것인지가 불명확한 경우가 많다. 본 논문에서는 자기전기복합체의 비공진, 공진상황에서 자기전기 전압계수를 어떻게 측정할 수 있는지에 대한 자세한 방법을 소개한다. 평가를 위한 샘플로서 대칭적인 구조를 가지는 Gelfenol/PMN-PZT/Gelfenol 자기전기복합체를 제조하였다. 압전 재료로는 이방성의 (011) 32 모드의 PMN-PZT 압전 단결정과 자왜재료로는 Galfenol 합금을 사용하여 에폭시로 접착하였다. 컴퓨터 인터페이스로 자동화된 자기전기 전압특성 측정 시스템의 구성을 우선 설명하고, 자기전기 결합특성의 측정 방법을 단계별로 설명한다. 본 튜토리얼 논문에서는 자기전기결합 특성과 특성평가방법을 이해하고자 하는 연구자들에게 도움이 될 수 있는 평가방법의 원리와 절차를 제공하고자 하였다.

자기센서용 Ni-PZT-Ni, Co, Fe 적층구조 소자의 ME 특성 (Magnetoelectric Characteristics on Layered Ni-PZT-Ni, Co, Fe Composites for Magnetic Field Sensor)

  • 류지구;전성즙
    • 한국전기전자재료학회논문지
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    • 제28권2호
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    • pp.92-98
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    • 2015
  • The magnetoelectric characteristics on layered Ni-PZT-Ni, Co, Fe composites by epoxy bonding for magnetic field sensor were investigated in the low-frequency range. The ME coefficient of Ni-PZT-Ni, Ni-PZT-Co and Ni-PZT-Fe composites reaches a maximum of $200mV/cm{\cdot}Oe$ at $H_{dc}=110$ Oe, $106mV/cm{\cdot}Oe$ at $H_{dc}=90$ Oe and $87mV/cm{\cdot}Oe$ at $H_{dc}=160$ Oe, respectively. A trend of ME charateristics on Ni-PZT-Co, Ni-PZT-Fe composites was similar to that of Ni-PZT-Ni composites. The ME output voltage shows linearly proportional to ac field $H_{ac}$ and is about 0~150 mV at $H_{ac}$=0~7 Oe and f=110 Hz in the typical Ni-PZT-Ni sample. The frequency shift effect due to the load resistance $R_L$ shows that the frequency range for magnetic field sensor application can be modulated with appropriate load resistance $R_L$. This sample will allow for a low-magnetic ac field sensor in the low-frequency (near f=110 Hz).