• 제목/요약/키워드: magneto-impedance effect

검색결과 29건 처리시간 0.023초

Magnetic Properties and Magnetoimpedance Effect in Mumetal Thin Films

  • Cho, Wan-Shik;Yoon, Tae-Sick;Lee, Heebok;Kim, Chong-Oh
    • Journal of Magnetics
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    • 제6권1호
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    • pp.9-12
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    • 2001
  • The dependence of the magnetoimpedance effect (MI) on magnetic properties has been investigated in mumetal thin films prepared by rf magnetron sputtering. Coercivity of thin films prepared at 400 W was about 0.4 Oe, and the magnetic anisotropy field of films deposited under a uniaxial magnetic field decreased with increasing film thickness. The saturation magnetization of mumetal films increased with rising input power and thickness and was smaller than that of permalloy films. Transverse incremental Permeability (TPR) of films of 1$\mu m$ thick increased with increasing effective permeability. The magneto impedance ratio (MIR) was proportional to TPR in films 1$\mu m$ thick but in spite of lower effective permeability at higher thicknesses, MIR increased due to skin effect. The height of the double peaks in the MIR curves decreased with decreasing anisotropy and thickness. The maximum MIR value for a 4$\mu m$ thick 75% at 36.5 MHz.

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Annealing Effect of Local Anisotropy Field in Amorphous Co66Fe4Ni1B14Si15 Ribbon

  • Kim, C.G.;Jeong, M.H.;Jeong, M.H.;Yoon, S.S.;Yu, S.C.
    • Journal of Magnetics
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    • 제3권4호
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    • pp.123-126
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    • 1998
  • The magneto-impedance (MI) has been measured in the annealed Co66Fe4Ni1B14Si15 amorphous ribbon for the evaluation of anisotropy field. MI at the frequency of 10 MHz is related to the transverse permeability from rotational magnetization depending on the local anisotropy field. MI varies sensitively with the annealing temperature, reflecting the change of anisotropy field distribution. The local anisotropy fields evaluated from MI Profiles are discussed in terms of the magnetic softness and microstructural change by the annealing.

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아몰퍼스리본을 이용한 미안더타입 자계센서 (Meander type magnetic field sensors using amorphous ribbon)

  • K. H. Shin;J. Hur;G. Sa-Gong;Kim, Y.;J. Cho
    • 한국자기학회:학술대회 개요집
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    • 한국자기학회 2002년도 동계연구발표회 논문개요집
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    • pp.230-231
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    • 2002
  • 고주파전류가 통전되고 있는 연자성체에 외부자계가 인가되면 자성체의 표피효과(Skin effect)에 의해서 임피던스가 변화하게 된다. 따라서 고주파의 정전류를 통전시키면 자성체의 양단에서 전압의 크기는 외부에서 인가되는 자계에 따라 변화하게 되는데, 이 때의 전압을 자계로 환산함으로써 자계의 검출이 가능하다. 이러한 현상을 이용하여 자계를 검출하는 소자를 자기임피던스 센서(Magneto-Impedance sensor)라고 한다$^{1.2}$ . 자기임피던스 센서는 주로 연자성이 우수한 아몰퍼스 자성체를 이용하여 구성되고, 구조가 간단하며, 극히 우수한 자계 검출능력을 나타내므로, 차세대의 고감도 자계센서로서 주목을 받고 있다. (중략)

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이식형 중이 청각보조기를 위한 진동 트랜스듀서의 설계 (Design of Vibrating Transducer for Implantable Middle Ear Hearing Aid)

  • 박형욱
    • 대한의용생체공학회:의공학회지
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    • 제17권4호
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    • pp.535-544
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    • 1996
  • In this paper, we analyzed the coil-magnet type vibrating transducer for the implantable middle ear hearing aid which is appropriate for patient's hearing level, and an experimental transducer system is designed For the objective and quantitative analysis of the transducer, a theoretical equivalent model containing coil, magneto and inner ear is developed To perform effective evaluation of the transducer, a transforming ratio Tr is introduced and its range that is suitable for practical implantable middle ear hearing device is foun4 The result of applying physical parameters of ear system to the proposed analytical model shows that frequency response of the coil magrlet type vibrator is predominantly governed by resistive impedance of the coil rather than inertia effect of the magnet and the inner parameters. In addition, we realized an experimental middle ear hearing aid system to show the theoretical validity of designed system and this will provide the basis of the development for actually implantable system.

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Microstructure and Magnetic Characteristics of Mn-doped Finemet Nanocomposites

  • Le, Anh-Tuan;Kim, Chong-Oh;Chau Nguyen;Tho Nguyen Duc;Hoa Nguyen Quang;Lee, Hee-Bok
    • Journal of Magnetics
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    • 제11권1호
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    • pp.30-35
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    • 2006
  • A thorough study about the influences of Mn substitution for Fe on the microstructure and magnetic characteristics of $Fe_{73.5-x}Mn-{x}Si_{13.5}B_{9}Nb_{3}Cu_1$ (x = 1, 3, 5) alloys prepared by the melt-spinning technique has been performed. Nanocomposites composed of nanoscale $(Fe,Mn)_{3}Si$ magnetic phase embedded in an amorphous matrix were obtained by annealing their amorphous alloys at $535^{\circ}C$ for 1 hour. The addition of Mn causes a slight increase in the mean grain size. The Curie temperatures of the initial amorphous phase and of the nanocrystals phase decreased, while the Curie temperature of the remaining amorphous phase remained nearly constant with increasing Mn content. Soft magnetic properties of the crystallized samples have been significantly improved by a proper thermal treatment. Accordingly, the giant magnetoimpedance effect is observed and ascribed to the increase of the magnetic permeability, and the decrease of the coercivity of the samples. The increased magnetic permeability is resulted from a decrease in the magnetocrystalline anisotropy and saturation magnetostriction.

Ultra Low Field Sensor Using GMI Effect in NiFe/Cu Wires

  • Kollu, Pratap;Kim, Doung-Young;Kim, Cheol-Gi
    • Journal of Magnetics
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    • 제12권1호
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    • pp.35-39
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    • 2007
  • A highly sensitive magnetic sensor using the Giant MagnetoImpedance effect has been developed. The sensor performance is studied and estimated. The sensor circuitry consists of a square wave generator (driving source), a sensing element in a form of composite wire of a 25 $\mu$m copper core electrodeposited with a thin layer of soft magnetic material ($Ni_{80}Fe_{20}$), and two amplifier stages for improving the gain, switching mechanism, scaler circuit, an AC power source driving the permeability of the magnetic coating layer of the sensing element into a dynamic state, and a signal pickup LC circuit formed by a pickup coil and an capacitor. Experimental studies on sensor have been carried out to investigate the key parameters in relation to the sensor sensitivity and resolution. The results showed that for high sensitivity and resolution, the frequency and magnitude of the ac driving current through the sensing element each has an optimum value, the resonance frequency of the signal pickup LC circuit should be equal to or twice as the driving frequency on the sensing element, and the anisotropy of the magnetic coating layer of the sensing wire element should be longitudinal.

온도에 따른 비정질 금속$Co_{66}Fe_4Ni_1B_{14}Si_{15}$ 의 자기 임피던스 효과 (Temperature Dependence of Magnetoimpedance Effect in Amorphous $Co_{66}Fe_4Ni_1B_{14}Si_{15}$)

  • 김용국;김택기;김성일;이희복
    • 한국자기학회지
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    • 제8권1호
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    • pp.21-26
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    • 1998
  • 온도에 따른 비정질 금속 Co66Fe4Ni1B14Si15의 자기 임피던스의 변화를 저온 장치를 써서 시료의 온도를 10K∼300K까지 변화시키면서 측정하였다. 이때, 시료에 겉어준 교류전류를 10mA로 고정시키고 주파수를 100KHz에서 10MHz 까지 변화시켰다. MIR (Magneto-Impedance Ratio)은 온도가 증가함에 따라 급격히 증가하였으며, MIR(T)≡MIR(0)exp(cT2)의 관계식으로 나타났다. 상온에서 측정한 MIR 값은 측정 주파수내에서 10K에서의 값보다 2∼3배 크게 나타났다. 이 결과는 MI 온도 효과를 이용한 온도 센서로서의 가능성을 제시한다. MIR 곡선의 모양은 온도의 증가에 따라 큰 변화가 없었으며 MIR은 주파수 증가에 따라 커지면서 MIR 곡선의 모양이 퍼지는 전형적인 경향을 나타냈다.

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AFM Study and Magnetic Properties of Nanocrystalline Fe73.5-xCrxSi13.5B9Nb3Au1 (x=1~5) Alloys

  • Le, Anh-Than;Chau Nguyen;Cuong Nguyen Duy;The Ngo Duc;Kim, Chong-Oh;Rhee, Jang-Roh;Lee, Hee-Bok
    • Journal of Magnetics
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    • 제11권1호
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    • pp.43-50
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    • 2006
  • In this paper, the influences of microstructural and surface morphological developments on the soft magnetic properties and giant magneto-impedance (GMI) effect of the $Fe_{73.5-x}Cr_{x}Si_{13.5}B_{9}Nb_{3}Au_1$ (x = 1, 2, 3, 4, 5) alloys have been presented. It was found that the Cr addition slightly decreased the mean grain size of $\alpha-Fe(Si)$ grains. AFM results indicate a large variation of surface morphology of density and size of protrusions along the ribbon plane due to microstructural changes caused by thermal annealing with increasing Cr content. Ultrasoft magnetic properties of the nanocrystallized samples were noticeably enhanced by properly heat treatments at $T_a=540^{\circ}C$ such as an increase of the magnetic permeability and the decrease of coercivity, which is likely due to the formation of nanoscale $\alpha-Fe(Si)$ phase which reduced the magnetoelastic anisotropy of samples. Accordingly, the GMI effect was observed in the annealed samples. The correlation between the microstructure, surface morphology, and soft magnetic properties were explained by nucleation and growth model.

New Classes of LC Resonators for Magnetic Sensor Device Using a Glass-Coated Amorphous CO83.2B3.3Si5.9Mn7.6 Microwire

  • Kim, Yong-Seok;Yu, Seong-Cho;Hwang, Myung-Joo;Lee, Hee-Bok
    • Journal of Magnetics
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    • 제10권3호
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    • pp.122-127
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    • 2005
  • New classes of LC resonators for micro magnetic sensor device were proposed and fabricated. The first type LC resonator (Type I) consists of a small piece of microwire and two cylindrical electrodes at the end of the microwire without direct contact to its ferromagnetic core. In type I resonator the ferromagnetic core of the microwire and cylindrical electrodes act as an inductor and two capacitors respectively to form a LC circuit. The second type LC resonator (Type II) consists of a solenoidal micro-inductor with a bundle of soft magnetic microwires as a core. The solenoidal micro-inductors fabricated by MEMS technique were $500\sim1,000\;\mu{m}$ in length with $10\sim20$ turns. A capacitor is connected in parallel to the micro-inductor to form a LC circuit. A tiny glass coated $CO_{83.2}B_{3.3}Si_{5.9}Mn_{7.6}$ microwire was fabricated by a glass-coated melt spinning technique. A supergiant magneto-impedance effect was found in a type I resonator as much as 400,000% by precise tuning frequency at around 518.51 MHz. In type II resonator the changes of inductance as a function of external magnetic field in micro-inductors with properly annealed microwire cores were varied as much as 370%. The phase angle between current and voltage was also strongly dependent on the magnetic field. The drastic increments of magnetoimpedance at near the resonance frequency were observed in both types of LC resonators. Accordingly, the sudden change of the phase angle, as large as $180^{\circ}C$, evidenced the occurrence of the resonance at a given external magnetic field.