• Title/Summary/Keyword: Magnetoelectric (ME)

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Frequency Dependent Magnetoelectric Responses in [0.948 Na0.5K0.5NbO3-0.052 LiSbO3]-[Co1-xZnxFe2O4] Particulate Composites

  • Choi, Moon Hyeok;Noh, Byung Il;Yun, Woosik;Jung, Chaewon;Yang, Su Chul
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.35 no.3
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    • pp.303-307
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    • 2022
  • Magnetoelectric (ME) properties of 3-0 type particulate composites have been investigated with respect to application features for reliable magnetic sensitivity and magnetically-induced output voltage. In order to figure out the magnetoelectric characteristics in the ME composites, frequency dependent ME responses were studied from [0.948 Na0.5K0.5NbO3-0.052 LiSbO3]-[Co1-xZnxFe2O4] (NKNLS)/Co1-xZnxFe2O4 (CZFO, x=0, 0.1, and 0.2). As a result, the maximal αME of 23.15 mV/cm·Oe was achieved from the NKNLS-CZFO (xZn = 0.1) composites at resonance frequency of 315 kHz and Hdc = 0 Oe. From the frequency dependent ME responses, it is clearly described that the self-biased ME composites can be used for applications as both magnetic sensors and energy harvesters, respectively.

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

  • Ryu, Ji-Goo;Jeon, Seong-Jeub
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.28 no.2
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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).

Characteristics of Magnetoelectric Composite with Rosen Type Piezoelectric Transducer Structure (Rosen형 압전 변압기 구조를 적용한 자기-전기 복합체의 특성)

  • Park, Sung Hoon;Yoon, Woon-Ha;Patil, Deepak Rajaram;Ryu, Jungho
    • Journal of the Korean Institute of Electrical and Electronic Material Engineers
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    • v.34 no.6
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    • pp.480-486
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    • 2021
  • Magnetoelectric (ME) composite is composed of a piezoelectric material and a magnetostrictive material. Among various ME structures, 2-2 type layered ME composites are anticipated to be used as high-sensitivity magnetic field sensors and energy harvesting devices especially operating at its resonance modes. Rosen type piezoelectric transducer using piezoelectric material is known to amplify a small electrical input voltage to a large electrical output voltage. The output voltage of these Rosen type piezoelectric transducers can be further enhanced by modifying them into ME composite structures. Herein, we fabricated Rosen type ME composites by sandwiching Rosen type PMN-PZT single crystal between two Ni layers and studied their ME coupling. However, the voltage step-up ratio at the resonance frequency was found to be smaller than the value calculated with αME value. The ATILA FEA (Finite Elements Analysis) simulation results showed that the position of the nodal point was changed with the presence of a magnetostrictive layer. Thus, while designing a Rosen type ME composite with high performance in a resonant driving situation, it is necessary to optimize the position of the nodal point by optimizing the thickness or length of the magnetostrictive layer.

Magnetoelectric Effects in (Bi,La)FeO3-PbTiO3 Ceramics ((Bi,La)FeO3-PbTiO3 세라믹스의 자전효과)

  • Lee Eun Gu;Lee Jong Kook;Jang Woo Yang;Kim Sun Jae;Lee Jae Gab
    • Korean Journal of Materials Research
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    • v.15 no.2
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    • pp.121-125
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    • 2005
  • Magnetoelectric (ME) effects for lanthanum modified $BiFeO_3-PbTiO_3\;(BE-_xPT)$ solid solutions have been investigated. The value of magnetoelectric polarization coefficient, up is 10 times greater than that of $Cr_2O_3$. The results also show that up is due to a linear coupling between polarization and magnetization, and that up is independent of do magnetic bias and ac magnetic field. The ME effect is believed to be significantly enhanced due to breaking of the cycloidal spin state of a long-period spiral spin structure, via randomly distributed charged imperfections.

The Dumb-bell Shaped Magnetostrictive/Piezoelectric Transducer

  • Li, Jianzhong;Wen, Yumei;Li, Ping
    • Journal of Magnetics
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    • v.16 no.4
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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.

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
    • Journal of the Korean Ceramic Society
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    • v.39 no.9
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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.

Enhancement of the Magnetic Flux in Metglas/PZT-Magnetoelectric Integrated 2D Geomagnetic Device

  • Huong Giang, D.T.;Duc, P.A.;Ngoc, N.T.;Hien, N.T.;Duc, N.H.
    • Journal of Magnetics
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    • v.17 no.4
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    • pp.308-315
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    • 2012
  • Experimental investigations of the magnetization, magnetostriction and magnetoelectric (ME) effects were performed on sandwich - type Metglas/PZT/Metglas laminate composites. The results have been analyzed by taking into account the demagnetization contribution. The study has pointed out that the magnetic flux concentration is strongly improved in piezomagnetic laminates with a narrower width leading to a significant enhancement of the ME effects. The piezomagnetic laminates with the optimal area dimension were integrated to form a 2-D geomagnetic device, which simultaneously can precisely detect the strength as well as inclination of the earth's magnetic field. In this case, a magnetic field resolution of better than $10^{-4}$ Oe and an angle precision of ${\pm}0.1^{\circ}$ were determined. This simple and low-cost geomagnetic-field device is promising for various applications.

Magnetic sensor and current sensor using a Magnetoelectric effect (Magnetoelectric 효과를 이용한 전류 및 자기 센서)

  • Lee, Dong-Gun;Lee, Jeong-Hoon
    • Proceedings of the KIEE Conference
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    • 2011.07a
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    • pp.1696-1697
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    • 2011
  • 최근들어 멀티 페로익스(multiferroics)재료를 이용하여 자계(magnetic field)하에서 전기적현상(polarization)을 유기시키는 재료에 대한 관심이 폭발적으로 증가되고 있다. 이는 megnetoelectric 효과(ME 효과)를 이용하는 방법으로, 자기 및 전류센서에 응용함을 위해 크게 각광받고 있으며, 본 연구에서는 자계내에서 자성재료-압전재료의 다층 구조 캔틸레버의 구현을 통해 전기적인 신호로의 변화를 통해 전류 및 자기 센서로의 가능성에 대한 연구를 진행하였다.

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Magnetoelectric Characteristics on Layered Fe78B13Si9/PZT/Fe78B13Si9 Composites for Magnetic Field Sensor (자기센서용 Fe78B13Si9/PZT/Fe78B13Si9 적층구조 소자의 ME 특성)

  • Ryu, Ji-Goo;Jeon, Seong-Jeub
    • Journal of Sensor Science and Technology
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    • v.24 no.3
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    • pp.181-187
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    • 2015
  • The magnetoelectric characteristics on layered $Fe_{78}B_{13}Si_9/PZT$ and $Fe_{78}B_{13}Si_9/PZT/Fe_{78}B_{13}Si_9$($t_m=0.017$, 0.034mm) composites by epoxy bonding for magnetic field sensor were investigated in the low-frequency range and resonance frequency range. The optimal bias magnetic field $H_{dc}$ of these samples was about 23~63 Oe range. The Me coefficient of $Fe_{78}B_{13}Si_9/PZT/Fe_{78}B_{13}Si_9(t_m=0.034mm)$ composites reaches a maximum of $186mV/cm{\cdot}Oe$ at $H_{dc}=63Oe$, f=50 Hz and a maximum of $1280mV/cm{\cdot}Oe$ at $H_{dc}=63Oe$, resonance frequency $f_r=95.5KHz$. The output voltage shows linearity proportional to ac fields $H_{ac}$ and is about U=0~130.6 mV at $H_{ac}=0{\sim}7Oe$, f=50 Hz, U=0~12.4 V at $H_{ac}=0{\sim}10Oe$, $f_r=95.5KHz$(resonance frequency). The optimal frequency(f=50 Hz) of this sample is around the utility ac frequency(f=60 Hz). Therefore, this sample will allow for ac magnetic field sensor at utility frequency and low bias magnetic fields $H_{dc}$.

Enhanced Giant Magnetoelectric Effect in Laminate Composites of FeCuNbSiB/FeNi/PZT

  • Wen, Yumei;Wang, Dong;Li, Ping
    • Journal of Magnetics
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    • v.16 no.4
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    • pp.398-402
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    • 2011
  • A novel laminate composite of FeCuNbSiB/FeNi /PZT is proposed, where FeCuNbSiB has a permeability of around 100000, which is much larger than that of FeNi. The high-permeability FeCuNbSiB was laminated with piezomagnetic FeNi rather than attached to its ends. It is expected that the effect produced by the high permeability will act on the whole of the piezomagnetic layer. While a FeNi layer was laminated with a FeCuNbSiB layer, the strong demagnetization produced by the latter was expected to be imposed on the FeNi layer as well as the applied fields. The distribution of applied fields was altered by the high-permeability material (both bias and ac field) and the field variation positively contributed to the ME effect in piezomagnetic/piezoelectric composites. Thus the ME voltage coefficient along with the field sensitivity were improved.