• 제목/요약/키워드: Magnetization current

검색결과 249건 처리시간 0.027초

Analysis of AC losses in HTS coils by temperature variations

  • Kim, Yungil;Lee, Ji-Kwang;Lee, Seyeon;Kim, Woo-Seok;Lee, Siyoung;Choi, Kyeongdal
    • 한국초전도ㆍ저온공학회논문지
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    • 제20권4호
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    • pp.50-54
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    • 2018
  • We analyzed the temperature dependency of the AC losses in high temperature superconducting (HTS) coils. In the case of a short sample of an HTS tape, the magnetization loss at 4.2 K could be higher than the one at 77 K for a same transport current. It happens when the perpendicular magnetic field is above a certain magnitude. The AC loss characteristics of solenoidal coils have been analyzed at the temperatures of 65 K and 77 K. They were categorized by the aspect ratios. The operating current of a solenoid was normally set about 70 % of the critical current. An HTS solenoid with the same operating current of 77 K causes larger AC losses at 65 K in the most cases of the HTS solenoids. We also analyzed the AC loss characteristics due to the temperature variations for three types of superconducting magnetic energy storages. Two of them were solenoidal types and the other was toroidal type. The results showed the tendency for the coils to have higher AC losses at lower temperature with the same operating currents and scenarios.

자속구속형 초전도 사고전류제한기의 사고각에 따른 철심의 포화특성 (Saturation Characteristic of Iron Core Dependent on Fault Angle in a Flux-Lock Type SFCL)

  • 김재철;임성훈
    • 조명전기설비학회논문지
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    • 제21권10호
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    • pp.29-34
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    • 2007
  • 본 논문에서는 사고각에 따른 자속구속형 초전도 사고전류제한기의 사고전류제한 특성을 분석하였다. 이를 위해 자화가지를 포함한 등가회로로부터 사고각에 따른 자속구속형 초전도 사고전류제한기의 철심내부자속을 유도하였으며 사고전류에 미치는 영향을 분석하였다. 사고전류제한 실험을 통해, 철심의 포화와 관련한 여자전류를 유도하였으며 사고각에 따른 변화를 분석하였다. 사고전에는 발생되지 않았지만 사고가 발생함과 동시에 여자전류크기가 증가하였으며 특히, 자속구속형 초전도 사고전류제한기를 가극결선한 경우가 감극결선한 경우보다 보다 크게 증가되는 것을 확인할 수 있었다. 등가회로로부터 분석한 결과와 실험결과는 일치되는 것을 확인할 수 있었다.

SQUID 센서 기반의 극저자장 자기공명 장치를 위한 사전자화코일 전류구동장치 개발 (Development of Prepolarization Coil Current Driver in SQUID Sensor-based Ultra Low-field Magnetic Resonance Apparatuses)

  • 황성민;김기웅;강찬석;이성주;이용호
    • Progress in Superconductivity
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    • 제13권2호
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    • pp.105-110
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    • 2011
  • SQUID sensor-based ultra low-field magnetic resonance apparatus with ${\mu}T$-level measurement field requires a strong prepolarization magnetic field ($B_p$) to magnetize its sample and obtain magnetic resonance signal with a high signal-to-noise ratio. This $B_p$ needs to be ramped down very quickly so that it does not interfere with signal acquisition which must take place before the sample magnetization relaxes off. A MOSFET switch-based $B_p$ coil driver has current ramp-down time ($t_{rd}$) that increases with $B_p$ current, which makes it unsuitable for driving high-field $B_p$ coil made of superconducting material. An energy cycling-type current driver has been developed for such a coil. This driver contains a storage capacitor inside a switch in IGBT-diode bridge configuration, which can manipulate how the capacitor is connected between the $B_p$ coil and its current source. The implemented circuit with 1.2 kV-tolerant devices was capable of driving 32 A current into a thick copper-wire solenoid $B_p$ coil with a 182 mm inner diameter, 0.23 H inductance, and 5.4 mT/A magnetic field-to-current ratio. The measured trd was 7.6 ms with a 160 ${\mu}F$ storage capacitor. trd was dependent only on the inductance of the coil and the capacitance of the driver capacitor. This driver is scalable to significantly higher current of superconducting $B_p$ coils without the $t_{rd}$ becoming unacceptably long with higher $B_p$ current.

여자전류에 따른 저온초전도전원장치의 3차원 정자계 유한요소 시뮬레이션 (3-D Magnetostatic Finite Element Simulation of a Low-Tc Superconducting Power Supply with Respect to the Excitation Current)

  • 배덕권;김호민;이찬주;윤영수;이상진
    • 대한전기학회논문지:전기기기및에너지변환시스템부문B
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    • 제51권7호
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    • pp.364-369
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    • 2002
  • In this paper, 3-D magnetostatic finite element simulation of a rotux type Low-Tc superconducing (LTS) superconducting power supply, finite element method, cryogenic system, superconducting foil by generated magnetic flux from the rotating pole. The magnetic flux density on the superconducting foil caused by two exciters is therefore sufficiently greater than its critical magnetic flux density and it is an essential point in LTS power supply design. To establish the sufficient flux path of this machine, ferromagnetic materials is used in this power supply. When ferromagnetic materials is used at extremely low temperature, its characteristic of magnetization differs to that at room temperature. For this reason, special consideration is needed in the magnetic analysis of cryogenic systems. When the excitation current is 10A, the normal spot appears on superconducting foil. The results of this analysis are calculated and compared with the experimental results. The linkage flux due to the excitation current of 10, 20, 30, 40 and 50A are respectively $1.30{\times}10-4$, $2.67{\times}10-4$, $5.08{\times}10-4$ and $6.15{\times}10-4Wb$.

고온 초전도체 $Y_{1-x}Yb_xBa_2Cu_3FyOy$의 자기적 성질에 관한 연구 (A study on the magnetic properties of high Tc superconductor $Y_{1-x}Yb_xBa_2Cu_3FyOy$)

  • 김재욱;김채옥
    • E2M - 전기 전자와 첨단 소재
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    • 제9권6호
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    • pp.578-583
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    • 1996
  • The magnetic properties have been investigated for the system of $Y_{1-x}$Yb$_{x}$Ba$_{2}$Cu$_{3}$F$_{y}$O$_{y}$ with x=0.0, 0.1, 0.2, 0.3, 0.4 and 0.5. In the magnetic hysteresis measurements, the values of the magnetic critical current densities are in the range of 10$^{4}$-10$^{5}$ A/cm$^{2}$ at the maximum external field 1.4 T. The upper critical field is over 100 T. The critical current density is estimated by the magnetization width .DELTA.M through the Bean critical state model. As the field strength is increased, the .DELTA.M diminishes slowly. The .DELTA.M for the fluorinated sample also decreases slowly with increasing field. It is considered that the large J, value results from this type is due to enhanced pinning center in grain boundary.y.ary.y.

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Flux pinning and critical current density in $TiO_2$-doped $MgB_2$ superconductor

  • 강지훈;박정수;박진우;이영백
    • 한국진공학회:학술대회논문집
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    • 한국진공학회 2010년도 제39회 하계학술대회 초록집
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    • pp.172-172
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    • 2010
  • $MgB_2$ doped with $TiO_2$ was prepared by the in-situ solid state reaction to study the effects of $TiO_2$ dopant on the flux pinning behavior of $MgB_2$ superconductor. From the field-cooled and the zero-field-cooled temperature dependences of magnetization, the realms of vortex-glass and vortex-liquid states of $TiO_2$-doped $MgB_2$ were determined in the H-T diagram (the temperature dependence of upper critical magnetic field and irreversibility line). The critical current density was estimated from the width of hysteresis loops in the framework of Beam's model at different temperatures. The results indicate that nano-scale $TiO_2$ inclusions play a role of the effective pinning centers and lead to the enhanced upper critical field and critical current density. It is suggested that the grain-boundary pinning mechanism is realized in $TiO_2$-doped $MgB_2$ superconductor.

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Spin-polarized Current Switching of Co/Cu/Py Pac-man type II Spin-valve

  • Lyle, Andrew;Hong, Yang-Ki;Choi, Byoung-Chul;Abo, Gavin;Bae, Seok;Jalli, Jeevan;Lee, Jae-Jin;Park, Mun-Hyoun;Syslo, Ryan
    • Journal of Magnetics
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    • 제15권3호
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    • pp.103-107
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    • 2010
  • We investigated spin-polarized current switching of Pac-man type II (PM-II) nanoelements in Pac-man shaped nanoscale spin-valves (Co/Cu/Py) using micromagnetic simulations. The effects of slot angle and antiferromagnetic (AFM) layer were simulated to obtain optimum switching in less than 2 ns. At a critical slot angle of $105^{\circ}$, the lowest current density for anti-parallel to parallel (AP-P) switching was observed due to no vortex or antivortex formation during the magnetic reversal process. All other slot angles for AP-P formed a vortex or antivortex during the magnetization reversal process. Additionally, a vortex or anti-vortex formed for all slot angles for parallel to anti-parallel (P-AP) switching. The addition of an AFM layer caused the current density to decrease significantly for AP-P and P-AP at slot angles less than $90^{\circ}$. However, at slot angles greater than $90^{\circ}$, the current density tended to decrease by less amounts or actually increased slightly as shape anisotropy became more dominant. This allowed ultra-fast switching with 5.05 and $5.65{\times}10^8\;A/cm^2$ current densities for AP-P and P-AP, respectively, at a slot angle of $105^{\circ}$.

강자성체박막의 회전에 따른 자기저항의 변화 (Magnetoresistance Variation for Rotation in Ferromagnetic Thin Films)

  • 양기원;박상철
    • 한국안광학회지
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    • 제11권3호
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    • pp.225-229
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    • 2006
  • 강자성체인 철과 니켈의 박막에서 전류와 자기장이 이루는 각도의 변화에 따른 자기저항의 변화를 관찰하였다. 경사각에 따른 PMR과 NMR의 크기가 같은 ${\phi}_{mix}$의 변화는 전류에 수직한 자기장의 성분과 평행한 자기장의 성분이 같게 되는 각도에서 자기저항 루프의 역전이 되는 것을 이용하면 ${\phi}_{mix}=tan^{-1}(1+tan{\theta})$와 같이 구해진다. 위 관계식은 실험치와 잘 일치함을 보여준다. 반면에 철박막의 경우에는 니켈박막과 자화축이 다르게 나타나서 ${\phi}_{mix}$가 위 식으로 주어진 관계와 일치하지 않는다.

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Mechanically Driven Decomposition of Intermetallics

  • Kwon, Young-Soon;Kim, Hyun-Sik;Gerasimov, Konstantin B.
    • 한국분말재료학회지
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    • 제9권6호
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    • pp.422-432
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    • 2002
  • Mechanically driven decomposition of intermetallics during mechanical milling(MM 1 was investigated. This process for Fe-Ce and Fe-Sn system was studied using conventional XRD, DSC, magnetization and alternative current susceptibility measurements. Mechanical alloying and milling form products of the following composition (in sequence of increasing Gecontent): $\alpha$(${\alpha}_1$) bcc solid solution, $\alpha$+$\beta$-phase ($Fe_{2-x}Ge$), $\beta$-phase, $\beta$+FeGe(B20), FeGE(B20), FeGe(B20)+$FeGe_2$,$FeGe_2$,$FeGe_2$+Ge, Ge. Incongruently melting intermetallics $Fe_6Ge_5$ and $Fe_2Ge_3$ decompose under milling. $Fe_6Ge_5$ produces mixture of $\hat{a}$-phase and FeGe(B20), $Fe_2Ge_3$ produces mixture of FeGe(B20) and $FeGe_2$ phases. These facts are in good agreement with the model that implies local melting as a mechanism of new phase for-mation during medchanical alloying. Stability of FeGe(B20) phase, which is also incongruently melting compound, is explained as a result of highest density of this phase in Fe-Ge system. Under mechanical milling (MM) in planetary ball mill, FeSn intermetallic decomposes with formation $Fe_5Sn_3$ and $FeSn_2$ phases, which have the biggest density among the phases of Fe-Sn system. If decomposition degree of FeSn is relatively small(<60%), milled powder shows superparamagnetic behavior at room temperature. For this case, magnetization curves can be fitted by superposition of two Langevin functions. particle sizes for ferromagnetic $Fe_5Sn_3$ phase determined from fitting parameters are in good agreement with crystalline sizes determined from XRD data and remiain approximately chageless during MM. The decomposition of FeSn is attributed to the effects of local temperature and local pressure produced by ball collisions.

영구자석을 이용한 전단모드 MR 댐퍼 설계 및 해석 (Design and Analysis of Magneto-Rheological Damper Using Permanent Magnet)

  • 김완호;칼루반 수레쉬;박진하;최상민;박춘용;강제원;최승복
    • 한국소음진동공학회논문집
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    • 제26권4호
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    • pp.443-448
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    • 2016
  • A novel Permanent Magnet based Magneto Rheological (PM-MR) damper is proposed in this paper. The principle of proposed MR damper is achieved by designing a linearly varying magnetization area with-respect to the movable permanent magnetic based piston setup. Nowadays, commercially available MR damper uses electromagnetic coils for generating the variable magnetic fields corresponding to the variable damping force. The amount of magnetic field produced by the electromagnetic coils are depends on the biasing current of voltage source. The key enabling concept of the proposed MR damper is to replace the electromagnetic coils and the voltage sources by utilizing the variable area based permanent magnetic piston setup. The proposed unique design structure of PM-MR damper has an increasing shear mode damping force with the piston movement in both jounce and rebound motion. In this research, analytical model of the proposed structure is derived and the structural design of proposed concept is verified using numerical CAD tool. As a result, the damping force is increase when piston movement in both jounce and rebound motion.