• 대한의용생체공학회:의공학회지
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• 제23권4호
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• pp.287-293
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• 2002

시변 자계를 이용하여 비접촉적인 방법으로 신경을 자극하기 위해서는 신경자극코일에 대용량 전류 펄스를 순시적으로 인가해야만 한다. 신경자극코일에 인가하는 전류 펄스의 주파수를 증가할수록 신경자극코일에 전력을 공급하는 전력공급기의 용량이 커지게 되고 신경자극코일에 발생하는 열량도 커지는 문제가 발생한다. 본 논문에서는 이러한 문제를 완화하기 위해 새로운 형태의 신경자극코일을 제안하였다. 신경자극코일에 강자성체 구조물을 부착하여 자계 거울 효과를 내게 하면 신경자극코일의 효율이 증가하게 된다. 다양한 형태의 신경자극코일에 대해 자계 거울 효과를 유한요소법으로 분석하였고 몇 종류의 신경자극코일에 대해 실험한 결과를 제시하였다.

• 한국자기학회지
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• 제24권6호
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• pp.171-178
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• 2014

전자기를 이용하여 배관의 비파괴검사를 적용하는 방법 중 하나인 Remote Field Eddy Current Testing (RFECT)는 큰 마찰력이 발생하고 잔류자화성분이 남는 Magnetic Flux Leakage (MFL) 방식과 외벽의 결함을 측정하는데 곤란한 일반 Eddy Current Testing (ECT) 방식의 단점들을 보완할 수 있는 기법으로 50여 년 전부터 다양한 기관에서 연구되어왔다. 그러나 배관 내에서 발생하는 와전류와 자기장에 대한 연구와 RFECT Exciter Coil의 설계에 대한 논의가 부족한 실정이다. 본 논문에서는 유한요소법을 이용한 전자기 해석을 통해 배관 내에서 발생하는 와전류와 자기장의 분포를 확인하고 변수 변화에 따른 영향을 분석하였다. 또한 Exciter Coil에 대한 최적 설계 알고리즘을 제시하고, 결함 형상과 기타 변수 변화가 결함신호에 미치는 영향을 확인하였다.

• 전기학회논문지P
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• 제58권1호
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• pp.85-89
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• 2009

We investigated the quench characteristics in accordance with increase of turns number of trigger coil and shunt resistance of matrix-type superconducting fault current limiter (SFCL) with $2{\times}3$ array. The matrix-type SFCL consists of the trigger part to apply magnetic field and the current-limiting part to limit fault current. The fault current limiting characteristics according to the increase of magnetic field and applied voltage were nearly same. This is because the application of magnetic field hasn't an affect on total impedance of the SFCL. When turns number of a reactor increased, the voltage difference between two superconducting units in the current-limiting part according was decreased. The resistance difference generated in two superconducting units was also decreased. Therefore, we confirmed that the differences of the critical behaviors between superconducting units were reduced by application of magnetic field. By this results, we could decide the optimum turns number of reactor to apply magnetic field.

• 한국전자파학회지:전자파기술
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• 제5권4호
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• pp.64-70
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• 1994

전력주파수 자기장 , 펄수 자기장 및 감쇠진동 자기장 내성평가에 대한 규격이 국제전기기술위원회(IEC)에 서 재정되어 전기.전자제품들의 자기장내성에 대한평가가 이루어질 전망이다. 이를 위해 본 연구에서는 IEC규격에서 정하고있는 자기장 내성평가용 유도코일인 정사각형 코일$1m\times1m$, 직사각형 코일 $1m\times2.6m$와 코일사이의 간격이 0.8m 및 0.6m인 이중 정사각형 코일 $1m\times1m$에 대한 자기장의 세기 및 균일도를 계산하여 IEC규격에서 규정한 유도코일의 유호 시험평가 영역을 도출하였다.

• 대한전기학회:학술대회논문집
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• 대한전기학회 2007년도 Techno-Fair 및 추계학술대회 논문집 전기물성,응용부문
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• pp.210-211
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• 2007

Once high current flows through the vacuum interrupter, eddy current occurs due to the time-varying axial magnetic field caused by the current(AC) and it causes a decrease in axial magnetic field generated by current flowing through coil electrode. but if there are slots on contact electrode it is possible to increase the amplitude of axial magnetic field by reducing the influence of eddy current. there has been many studies about the number of slot of the contact electrode[1][2][3]. In this paper, in addition to these previous results we deal with the influence of the length and width of the slots on axial magnetic field at the mid-gap plane in 4 segment coil type vacuum interrupter by using 3D finite element method software.

• Journal of electromagnetic engineering and science
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• 제8권1호
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• pp.23-27
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• 2008

Magnetic coupling delivering wireless power in capsular endoscope(CE) is described in this paper. The characteristic of the magnetic flux linkage coil which generates the induced electromotive force(emf) under the magnetic field was analyzed. With the analyzed results, a magnetic flux linkage coil system was developed and tested. It was confirmed that the magnetic flux linkage coil system could supply more than 50 mW power at 125 kHz without changing the structure of conventional CE.

• 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.

• 전기학회논문지
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• 제57권2호
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• pp.314-319
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• 2008

In this paper, the electric field distribution induced inside the brain during Transcranial Magnetic Stimulation(TMS) has been thoroughly investigated in terms of tissue heterogeneity and anisotropy as well as different head models. To achieve this, first, an elaborate head model consisting of seven major parts of the head has been built based on the Magnetic Resonance(MR) image data. Then the Finite Element Method(FEM) has been used to evaluate the electric field distribution under different head models or three different conductivity conditions when the head model has been exposed to a time varying magnetic field achieved by utilizing the Figure-Of-Eight(FOE) stimulation coil. The results show that the magnitude as well as the distribution of the induced field is significantly affected by the degree of geometrical asymmetry of head models and conductivity conditions with respect to the center of the FOE coil.

• Journal of Electrical Engineering and information Science
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• 제2권6호
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• pp.95-105
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• 1997

In this paper, we have studied about design and fabrication of the actively shielded superconducting MRI magnet. Nonlinear optimization methods are usually used to find optimum coil configurations. However the selection of initial coil configurations is very difficult. In case bad initial data are used, it is even impossible to find optimum coil configurations which satisfy predefined constraints. We have developed computer optimization program which consists of two steps. Initial coil configurations are easily selected through linear optimization in the first step and optimum coil configurations are found through nonlinear optimization in the second step. We have also studied about superconducting shim coils to cancel error fields caused by coil fabrication errors. Many researchers published design concepts of shim coil. However all these studies are for shim coil design using filamentary coils with single turn, Shim coils with multi-turns should be used to produce enough field strength to cancel error fields. We have developed computer program for the design of shim coils which have proper thickness and length. An actively shielded superconducting MRI magnet with a small warm bore was fabricated and four sets of superconducting shim coils were equipped. The magnetic field distributions were measured and field correction was carried out using shim coils.

• Progress in Superconductivity
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• 제5권2호
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• pp.128-131
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• 2004

The resistive superconducting fault current limiters (SFCLs) are very attractive devices for the electric power network. But they have some serious problems when the YBCO thin films were used for the current limiting materials due to the in homogeneities caused by manufacturing process. When the YBCO films have some inhomogeneities, simultaneous quenches are difficult to achieve when the fault current limiting units are connected in series for increasing operating voltage ratings. Magnetic field application is one of the prospective way of inducing simultaneous quenches far the series-connected resistive FCL components. Magnetic field was typically generated by the fault current thorough a coil, which is connected to components of the fault current limiter in series, leaving the problem, which provides significant inductance to the power line and suppresses critical current density of the superconducting components. In this article we investigated the possible application of the protective current transformer (p-CT), which is available current source to the magnetic coil. This system inductively coupled to the circuit, therefore, remarkably reducing impedance to the circuit. The current by the protective current transformer was directly fed to the coil, generating magnetic field large enough to reduce critical current density of the components. This successfully induced simultaneous quenches of the series-connected resistive FCL components.