• 한국초전도ㆍ저온공학회논문지
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• 제15권4호
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• pp.26-29
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• 2013

Smart fault current controller (SFCC) proposed in our previous work consists of a power converter, a high temperature superconducting (HTS) DC reactor, thyristors, and a control unit [1]. SFCC can limit and control the current by adjusting firing angles of thyristors when a fault occurs. SFCC has complex structure because the HTS DC reactor generates the loss under AC. To use the DC reactor under AC, rectifier that consists of four thyristors is needed and it increases internal resistance of SFCC. For this reason, authors propose a hybrid type superconducting fault current limiter (SFCL). The hybrid type SFCL proposed in this paper consists of a non-inductive superconducting coil and two thyristors. To verify the feasibility of the proposed hybrid type SFCL, simulations about the interaction of the superconducting coil and thyristors are conducted when fault current flows in the superconducting coil. Authors expect that the hybrid type SFCL can control the magnitude of the fault current by adjusting the firing angles of thyristors after the superconducting coil limits the fault current at first peak.

• 한국자기학회지
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• 제14권6호
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• pp.232-235
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• 2004

아날로그 형태의 신호를 전송하기에 적합한 특성을 보이는 선형 GMR(giant magnetoresistance) 아이솔레이터를 모델링하여 입력전류에 따른 출력전압과 전류를 조사하였다. GMR 아이솔레이터를 자기적 부분과 전기적 부분으로 나누고 선택된 스핀밸브 소자의 MR(magnetoresistance) 결과를 대입하여 출력전압을 구할 수 있는 순서도를 설정하였다. 자기적 모델링으로는 평판 코일의 3차원 모델을 FEM방법으로 해석하여 입력전류에 의해 생성되는 자장의 세기를 구하였으며, 여기에서 자기코어층이 있는 경우 50% 이상 더 커지는 결과를 얻었다. 그리고 아이솔레이터의 출력전압파형을 계산한 결과 입력 코일 전류에 따른 궤환 코일 전류가 $I_{out}$ = $I_{in}$ -5 mA의 선형함수와 비교시 평균 $\pm$0.25 mA 이내의 차이로 근사한 값으로 계산되었다. 또한 입력되는 코일 전류가 구형파일 때, 출력전압의 반응시간과 파형을 계산하였으며, 이때 최저전압에서 최대 전압까지 상승 및 하강하는 시간은 연산증폭 기의 slew rate가 0.3 V/${\mu}\textrm{s}$ 일 때, 최저전압에서 최대 전압까지 상승 및 하강하는 시간은 6 ${\mu}\textrm{s}$였다.

• 한국초전도저온공학회:학술대회논문집
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• 한국초전도저온공학회 2003년도 학술대회 논문집
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• pp.239-241
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• 2003

When superconductors are combined with normal conductor as a parallel electric circuit, imbalance of the applied current is happened. For the accurate parameters of the circuit, it is needed to measure the current of the circuit under LN2 condition. In this case, the measurement using Rogowski coil, which is not that affected by changing temperature, can be a method. In this study, using 2 Rogowski coil, the measurement of current was conducted under the condition that is room and LN2 temperature respectively.

• 한국초전도ㆍ저온공학회논문지
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• 제14권3호
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• pp.33-37
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• 2012

An HTS racetrack-type coil without turn-to-turn insulation was characterized by critical current, sudden discharge, and over-current tests with respect to external pressures applied to the straight sections of the coil. The thermal stability of the non-insulated HTS racetrack-type coil was remarkably enhanced with increasing external pressure applied to the straight sections of racetrack-type coil. Furthermore, over-current test results confirmed that the non-insulated HTS racetrack-type coil with increased turn-to-turn thermal contact has the potential to be manufactured into field coils of HTS wind turbine generators with highly enhanced thermal and electrical stabilities.

• 전기학회논문지
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• 제56권6호
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• pp.1035-1038
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• 2007

We designed and manufactured a 1.8T high temperature superconducting(HTS) insert coil for a NMR magnet operated at 4.2 K. Suitable HTS superconductor and HTS coil were carefully designed and developed. We have selected multi-filamentary Bi2223 conductor fabricated by American Superconductor Corporation(AMSC). The selected conductor consists of Bi2223 filaments of 55, silver stabilizer and stainless steel reinforcement tapes. Therefore, it shows good hoop strength as well as compression tolerance. The conductor has a tape cross-section of 0.31mm x 4.8mm. the Bi2223 conductor shows large anisotropy of critical current. The critical current of conductor in magnetic field parallel to the flat surface are much higher than that in magnetic field perpendicular. The HTS coil has an inner diameter of 78 mm, an outer diameter of 127 mm and a coil length of 600 mm. In this paper, the detailed design, fabrication and test results on the HTS insert coil are presented.

• 한국산학기술학회논문지
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• 제17권5호
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• pp.717-722
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• 2016

본 논문은 고장발생 초기 고장전류의 크기에 따라 피크전류제한 기능을 갖도록 하나의 철심에 기존 1차 코일과 2차 코일이 병렬로 연결된 초전도 소자 1과 추가적인 철심을 사용하여 3차 권선에 초전도 소자 2가 연결된 자기결합형 초전도한류기를 제안하였다. 이중 철심을 이용하여 코일 1과 코일 2간 병렬로 연결한 자기결합형 초전도한류기가 고장발생시 피크전류를 초전도 소자 1만이 분담하는 것을 확인할 수 있었다. 그 이유는 초기 사고전류의 순간적인 요소가 커서 초전도 소자 1이 ?치되어 작동하였으나, 코일 3에 흐르는 전류가 임계전류를 초과하지 않았고, 이로 인해 초전도 소자 2가 ?치되어 작동하지 않았기 때문이다. 사고 시 피크전류를 순차적인 초전도 소자로 제한하기 위해서는 코일 1이 낮은 자기인덕턴스 값을 갖고 있으면서도 코일 2보다 코일 3이 보다 높은 자기인덕턴스 값을 갖도록 설계해야 할 것이다. 또한, 고장 발생 초기 사고전류의 크기를 결정하는 고장조건 중의 하나인 1차 코일과 2차 코일간의 권선비가 0.25일 때 두 SFCL의 전류제한 및 회복특성에 대한 검증을 선로단락실험을 통해 분석되었다. 이 단락실험의 분석결과, 가극결선인 경우가 감극결선한 경우보다도 전류제한 및 회복특성이 더욱 우수함을 확인할 수 있었다.

• 한국정밀공학회:학술대회논문집
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• 한국정밀공학회 2005년도 춘계학술대회 논문집
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• pp.1788-1792
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• 2005

Eddy current sensor is representative instrument measuring gap to base metal and sensing trouble in base metal. The existing eddy current sensor works as measuring variance of sensor coil's inductance. But, sensor coil have phenomenon that not only inductance but also real resistance varies in real action. Conductivity and Permeability are main variable in sensor coil's varying impedance(inductance, real resistance). By searching relationship between conductivity-permeability and sensor coil's impedance, eddy current sensor gain advantage of elevation of accuracy, removal of alignment to each base metal, and continuous sensing to varying base metal.

• 센서학회지
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• 제19권6호
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• pp.475-482
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• 2010

Rogowski coil which detects magnetic flux on current changes. It is used for digital integration with watt-hour meter's current sensor, because, Rogowski coil has non-cored or non-magnetic core structure, so that, it cannot be saturated magnetically. This is a study for inventing accurate electric current sensors that have been applied on multi-layer ceramic substrate. We have confirmed its properties from each different layer's materials and pattern sizes by MWS 3D Electromagnetic field analysis program. And, after sensor manufacturing on multi-layer ceramic substrate, we confirmed its sensing quality is reliable as accurate electric current sensor for watt-hour meter.

• 대한전기학회논문지
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• 제43권7호
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• pp.1050-1060
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• 1994

This paper is a study on the computer simulation of the characteristics of the superconducting fault current limiter. Input variable parameters are apparent power, load resistance value, line resistance value and so on. Initial fault current 2 times larger than the trigger current is required to reduce the switching time of SFCL. The propagation velocity increases abruptly, the transport current is several times larger than the ciritical current. In this paper, the switching time is calculated to be 323$\mu$ sec, and the initial fault current is 19 times larger than the critical current. Because the trigger coils are bifilar winding, they have little impedance in superconducting state. After fault occurred, the limiting coil acts as a superconducting reactor and the trigger coils quench at a critical current. Without the SFCL in the circuit, fault current after the load impedence is shorted might be increased to 1100A. The fault current is, therefore, successfully limited by the superconducting limiting coil to 100A determined by the coil inductance.

• 한국초전도ㆍ저온공학회논문지
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• 제17권2호
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• pp.41-44
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• 2015

Critical current of high-temperature superconducting (HTS) coil is influenced by its own self magnetic field. Direction and density distribution of the magnetic field around the coil are fixed after the shape of the coil is decided. If the entire part of the HTS tape has homogeneous $I_c$ distribution characteristic, quench would be initiated in fixed location on the coil. However, the actual HTS tape has inhomogeneous $I_c$ distribution along the length. If the $I_c$ distribution of the HTS tape is known, we can expect the spot within the HTS coil that has the highest probability to initiate the quench. In this paper, $I_c$ distribution within the HTS coil under self-field effect is simulated by MATLAB. In the simulation procedure, $I_c$ distribution of the entire part of the HTS tape is assume d to follow Gaussian-distribution by central limit theorem. The HTS coil model is divided into several segments, and the critical current of each segment is calculated based on the-generalized Kim model. Single pancake model is simulated and self-field of HTS coil is calculated by Biot-Savart's law. As a result of simulation, quench-initiating spot in the actual HTS coil can be predicted statistically. And that statistical analysis can help detect or protect the quench of the HTS coil.