• Title/Summary/Keyword: Giant Magneto-Impedance

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Giant Magnetoimpedance in C067Fe4Mo1.5Si16.5B11 Metallic Glass Ribbon

  • Kuzminski, M.;Nesteruk, K.;Lachowicz, H.K.;Krzyzewski, A.;Yu, Seong-Cho;Lee, Hee-Bok;Kim, Cheol-Gi
    • Journal of Magnetics
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    • v.9 no.2
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    • pp.47-51
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    • 2004
  • Giant magneto-impedance (GMI) effect in zero-magnetostrictive Co-based amorphous ribbons samples in their as-quenched and stress-released states as well as with intentionally induced magnetic anisotropy were investigated. Magnetic and impedance properties of the samples exhibiting different anisotropy were compared and the optimum operation conditions for the studied samples from the view-point of their utilization as a sensor element have been determined. A design of a model of magnetic field sensor and characteristics of the constructed prototype are presented.

Magnetic Sensor Using Giant Magneto-Impedance Effect (거대자기임피던스 효과를 이용한 자기 센서)

  • Choi, Kyoo-Nam
    • The Journal of the Korea institute of electronic communication sciences
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    • v.12 no.6
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    • pp.1057-1064
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    • 2017
  • High sensitivity magnetic sensor having foreign metal detection capability is proposed utilizing giant magneto-impedance effect. Strip sensor showed the increasing output voltage when the external magnetic field was applied along with strip from strip grounding point, although the initial DC voltage varied depending on the pointing direction of strip sensor. Proposed sensor was able to eliminate more than half of background noise using active noise filter to achive high sensitivity, and it showed the capability to detect magnetized foreign metal object independent of ambient electro-magnetic noise and earth magnet. In case of ferrous sphere, the metal detection up to 0.8mm diameter was experimentally demonstrated at 5mm distance from strip sensor.

Angle Sensors Based on Oblique Giant Magneto Impedance Devices

  • Kim, Do-Hun;Na, Ji-Won;Jeung, Won-Young
    • Journal of Magnetics
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    • v.14 no.1
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    • pp.42-46
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    • 2009
  • The measurement of external magnetic field orientation using Giant Magneto Impedance (GMI) sensors has been performed. A soft magnetic alloy of $Co_{30}Fe_{34}Ni_{36}$ was electroplated on a Si wafer with a CoFeNi seed layer. V-shaped microwire patterns were formed using a conventional photolithography process. An external magnetic field was generated by a rectangular AlNiCo permanent magnet. The reference direction was defined as the external magnetic field direction oriented in the middle of 2 GMI devices. As the orientation of the magnetic field deviated from the reference direction, variation in the field component along each device introduced voltage changes. It was found that, by taking the voltage difference between the left and right arms of the Vshaped device, the nonlinearity of each device could be significantly reduced. The fabricated angle sensor had a linear range of approximately $70^{\circ}$ and an overall sensitivity of approximately 10 mV.

Super-giant Magneto-Impedance Effect of a LC-resonator Using a Glass-Coated Amorphous Microwire

  • Lee, Heebok;Kim, Yong-Seok;Yu, Seong-Cho
    • Journal of Magnetics
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    • v.7 no.4
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    • pp.160-164
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    • 2002
  • A new discovery of the super-giant magneto-impedance (SGMI) effect was found out in a LC-resonator consisted of a glass-coated amorphous $CO_{83.2}B_{3.3}Si_{5.9}Mn_{7.6}$ microwire. The measurement was carried out at high frequency range from 100 MHz up to 1 GHz of an ac-current flowing along the wire and at varying axial dcmagnetic field in its range of $\pm$120 Oe. The wires, about 16${\mu}m$ in diameter, were fabricated by a glass-coated melt spinning technique. The shape of the impedance curves plotted vs. a dc-field is changing dramatically with the frequency. The phase angle was also strongly dependent on this field. The external dc-magnetic field changes the circumferential permeability as well as the penetration depth, both in turn change the impedance of the sample. The drastic increments of SGMI at high frequency can be understood in terms of the LC-resonance phenomena. The sudden change of the phase angle, as large as $180^{\circ}$ evidenced the occurrence of the resonance at a given intensity of the external dc-field. The maximum ratio of SGMI reached in the experiment by precise tuning frequency equals 450,000% at the frequency of around 551.9075 MHz.