• Title/Summary/Keyword: Field coil

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Investigation of Acoustic Emission Signals in Racetrack Superconducting Field Winding Coils (레이스트랙형 초전도계자코일의 AE 신호 특성평가)

  • Sohn, M.H.;Baik, S.K.;Ko, R.K.;Lee, E.Y.;Bae, J.H.;Kwon, Y.K.;Ryu, K.S.
    • Proceedings of the KIEE Conference
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    • 1998.07a
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    • pp.186-188
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    • 1998
  • Acoustic emission monitoring on two racetrack superconducting field winding coil was performed during excitation and quenches to diagnose the integrity of the field winding coils. Two field windings were not impregnated with epoxy The results confirm that the acoustic emission signals are mainly due to conductor motions which cause premature quenching of the winding. The quench current of modified racetrack type field winding coil (Type B) are more higher than that of conventional field winding coil (Type A).

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Estimation of joint and index dissipation in HTS tape (고온초전도 선재의 접합 및 인덱스손실 평가)

  • 김정호;임준형;장석헌;김규태;주진호;최세용;나완수;강형구;고태국
    • Proceedings of the Korea Institute of Applied Superconductivity and Cryogenics Conference
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    • 2003.10a
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    • pp.59-62
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    • 2003
  • We fabricated two HTS closed coils by using resistive-joint method and the joint resistance of the coil was estimated by field decay technique at 77 K. In addition, we used the Runge-kutta method for the numerical analysis to estimate the decay properties. The joint resistances were evaluated as a function of critical current of HTS closed coil and external field strength of excitation coil. It was observed that joint resistance was independent of critical current and external field strength. It was estimated that joint resistance was 8.0$\times$10$^{-9}$ $\Omega$ to 11.9$\times$10$^{-9}$ $\Omega$ for coils of contact length for 7 cm.

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Analysis of mechanical characteristics of superconducting field coil for 17 MW class high temperature superconducting synchronous motor

  • Kim, J.H.;Park, S.I.;Im, S.H.;Kim, H.M.
    • Progress in Superconductivity and Cryogenics
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    • v.15 no.3
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    • pp.13-19
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    • 2013
  • Superconducting field coils using a high-temperature superconducting (HTS) wires with high current density generate high magnetic field of 2 to 5 [T] and electromagnetic force (Lorentz force) acting on the superconducting field coils also become a very strong from the point of view of a mechanical characteristics. Because mechanical stress caused by these powerful electromagnetic force is one of the factors which worsens the critical current performance and structural characteristics of HTS wire, the mechanical stress analysis should be performed when designing the superconducting field coils. In this paper, as part of structural design of superconducting field coils for 17 MW class superconducting ship propulsion motor, mechanical stress acting on the superconducting field coils was analyzed and structural safety was also determined by the coupling analysis system that is consists of commercial electromagnetic field analysis program and structural analysis program.

Design of 1 MW High-temperature Superconducting Motor with Water-cooled Armature (수냉식 전기자로 구성된 1 MW 고온초전도 동기모터의 설계)

  • Baik, S.K.;Lee, J.D.;Kim, S.H.;Lee, E.Y.;Sohn, M.H.;Kwon, Y.K.;Moon, T.S.;Park, H.J.;Kim, Y.C.;Lee, J.Y.;Hong, J.P.
    • Proceedings of the KIEE Conference
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    • 2005.07b
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    • pp.1258-1260
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    • 2005
  • Superconducting synchronous motors and generators have the field coil composed of superconductor with almost zero resistance at superconducting state. Therefore, co or loss at the conventional field coil is eliminated and the superconducting machine gets higher efficiency. The armature coil of the superconducting machine is composed of cower wire and supported by non-magnetic material such as FRP(Fiber Reinforced Plastic). Although a fully-superconducting machine with superconducting armature coil has been researched, it was not developed toward industrial application because of AC transporting loss and difficulty in construction of the cooling structure and so on. This paper contains the design procedure of a 1 MW superconducting synchronous motor using high-temperature superconductor only for the field coil. Especially, the armature coil is designed by water-cooling in order to dissipate Joule heat easily. Moreover, 3-dimensional electromagnetic design is conducted to get a proper design result and reduce design errors from 2-dimensional approach.

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Analysis of Magnetic Field Application Effect on Fault Current Limiting Characteristics of a Flux-lock Type SFCL

  • Lim, Sung-Hun
    • Transactions on Electrical and Electronic Materials
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    • v.9 no.6
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    • pp.255-259
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    • 2008
  • The magnetic field application effect on resistance of a high-$T_c$ superconducting (HTSC) element comprising a flux-lock type superconducting fault current limiter (SFCL) was investigated. The YBCO thin film, which was etched into a meander line using a lithography, was used as a current limiting element of the flux-lock type SFCL. To increase the magnetic field applied into HTSC element, the capacitor was connected in series with a solenoid-type magnetic field coil installed in the third winding of the flux-lock type SFCL. There was no magnetic field application effect on the resistance of HTSC element despite the application of larger magnetic field into the HTSC element when a fault happened. The resistance of HTSC element, on the contrary, started to decrease at the point of four periods from a fault instant although the amplitude of the applied magnetic field increased.

An Optimization of Inductive Coil Design for Thixoforging and Its Experimental Study (반용융 단조를 위한 유도가열용 코일설계의 최적화 및 실험적 연구)

  • Jung, Hong-Kyu;Kim, Nam-Seok;Kang, Chung-Gil
    • Journal of Korea Foundry Society
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    • v.19 no.5
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    • pp.393-402
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    • 1999
  • The reheating of the billet in the semi-solid state as quickly and homogeneously as possible is one of the most important aspects. From this point of view, an optimal design of the induction coil is necessary. The objective of inductive coil designsi a uniform induction heating over the length of the billet. The effect of coil length, diameter, the gap between coil surface and billet and axial position of the billet on temperature distribution of billet has been investigated. These design parameters have an important effectiveness on the electro-magnetic field. Therefore, in this study an optimal coil design to minimize electromagnetic ed effect will be proposed by defining the relationship between billet length and coil length. In particular, key point in induction heating process is focussed on optimizing the coil design with regard to the size of the heating billet and the frequency of induction heating system. After demonstrating the suitability of an optimal coil design through the FEM simulation of the induction heating process, the results of the coil design are also applied to the reheating process to obtain a fine globular microstructure. Its considered that the reheating conditions of aluminum alloys for thixoforging and a new CAE model of the induction heating process are very useful for thixoforging practitioners including induction heating ones.

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Design of 2-Axis Magnetic Field Source for in Vivo Experiments at Extremely Low Frequency (생체 실험용 2-축(軸) 극저주파 자기장 발생 장치의 설계)

  • Kim, Jeong-Ho;Gimm, Youn-Myoung
    • Proceedings of the Korea Electromagnetic Engineering Society Conference
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    • 2003.11a
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    • pp.13-17
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    • 2003
  • In this paper, the design parameters for the magnetic field source at extremely low frequency are proposed. This facility can be used for in vivo experiments with small animals to investigate biological response to the driving magnetic fields. In case that the exposed animals are motionless, the animals may be affected by the directivity of driving field. To avoid this effect, a 2-axis ELF magnetic field driving apparatus was designed, The optimum location and number of turns of each coil were obtained by numerical analysis. Applying these data to the MATLAB code (for computation), the magnetic field distribution was obtained. The calculation result for a well-designed facility showed that the space in which the amplitude of the magnetic field lies within the 95% of the magnetic field distribution was more than 60% of each axis length.

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Double-Excitation Type Single Sheet Tester for the Measurement of the Magnetic Characteristics of the Electrical Steel Sheets (전기강판의 자기특성 측정을 위한 2방향 여자 형 Single Sheet tester 개발)

  • Kim, Hong Jung;Koh, Chang Seop;Hong, Sun-Ki;Shin, Pan Seok
    • The Transactions of the Korean Institute of Electrical Engineers B
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    • v.54 no.10
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    • pp.461-469
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    • 2005
  • In this paper, a double-excitation type single sheet tester is developed to measure the magnetic characteristics of the electrical steel sheets. The developed system has the uniform magnetic field area of 20$\times$20mm$^{2}$, and can be applied to the measurement of the magnetic characteristics of the Non-oriented and Grain oriented electrical steel sheets. In the developed system, the magnetic flux density and magnetic field intensity are measured by using B-coil and H-coil, respectively. The B-coil has 1 turn search coil for each direction, and H-coil has 640 and 640 turns for rolling direction and transverse direction on the Im thickness Glass-Epoxy basement, respectively. Through experiments, it Is shown that the system can measure the magnetic characteristics up to 1.87 of magnetic flux density in the rolling direction in case of the Grain oriented electrical steel sheet. The measured results are compared with those measured in Okayama university, .Japan.

Design of an Electromagnetically-driven Micromirror Through the Coupled Physics Analyses (복합장 해석에 의한 전자력 구동방식의 마이크로미러 설계)

  • Han, Seung-Oh;Kim, Byoung-Min;Pak, Jung-Ho
    • The Transactions of The Korean Institute of Electrical Engineers
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    • v.59 no.2
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    • pp.380-384
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    • 2010
  • A micromirror for a laser display system actuated by the electromagnetic force induced by the surface coil and the permanent magnet was designed and analyzed through the coupled physics analyses incorporating the electromagnetics, mechanics, and electrothermal analysis because the mechanical rotation of the micromirror is driven by the electromagnetic driving force. The proposed micromirror has two torsion beams to sustain the mirror plate which has surface coils on the top and the two permanent magnets exists on both sides of the micromirror for an external magnetic field source. The designed micromirror has the resonant frequency of 3.82kHz. When the magnetic field of the permanent magnet is 0.4T, the coil has 4 turns, and the current density of coil is 3.6A/$mm^2$, the estimated z axis displacement of the mirror plate edge is 0.23mm which corresponds to the rotation angle of $14.2^{\circ}$. When considering the joule heating in the current-carrying coil, the maximum temperature of the mirror plate is obtained as 300.045K, which induces the negligible changes in the rotation angle and the resistance of the coil.

A study on the SMES component modeling using PSCAD/EMTDC (PSCAD/EMTDC를 이용한 SMES Component modeling에 관한 연구)

  • Kim, Jin-Gun;Kim, Jae-Ho;Jung, Hee-Yeol;Park, Min-Won;Yu, In-Keun
    • Proceedings of the KIEE Conference
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    • 2007.07a
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    • pp.1998-1999
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    • 2007
  • Before applying the HTS(High Temperature Superconductor) power devices to a real utility network, system analysis should be carried out by some simulation tools. PSCAD/EMTDC simulation tool is one of the most popularized useful analysis tools for electrical power system. Unfortunately the model component for HTS coil is not provided in PSCAD/EMTDC simulation tool. In this paper, EMTDC model component for HTS coil has been developed considering real characteristics of HTS coil like critical current, temperature and magnetic field. The developed model component of HTS coil could be used for power system application. Using the developed model component for HTS coil, we can easily do the simulation of HTS power devices application test in utility with the various inductance, quench current, inner magnetic field, and temperature values, for instances; SMES(Superconducting Magnetic Energy Storage) system, superconducting motor, transformer, and FCL(Fault Current Limiter)

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