• 한국전기전자재료학회:학술대회논문집
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• 한국전기전자재료학회 2009년도 추계학술대회 논문집
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• pp.214-214
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• 2009

While critical properties of BSCCO wires rely considerably on grid direction upon BSCCO and have very complicated mechanism of generating a superconducting phase, making it difficult to improve properties of wires, YBCO thin-film wires which can be formed in a superconducting phase upon metal board through vapor deposition processing can get excellent direction and reduce manufacturing costs with more flexibility in improving critical properties; thus, they will be suitable for instrument application in the future. Contrary to BSCCO wires for which thick silver alloy covering materials should inevitably be used, moreover, YBCO thin-film wires have an advantage of making thickness and quality of covering materials different by usage. Such a property can be an important element to widen application of wires by presenting possibility of using thin-film wires as superconducting material for fault current limiter as well as for high power current application. In this study we intend to prepare YBCO thin-film wires with different stabilizer layers to analyze current application and current restriction properties by stabilizer layers on the basis of detailed researches on changes in current classification properties below critical value.

• 한국초전도ㆍ저온공학회논문지
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• 제12권1호
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• pp.28-31
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• 2010

A magnetic field calculation method for toroidal type winding which has circular section was developed. At first, the equation for magnetic field by single filament coil was extended using numerical integration to estimate the entire interesting region of solenoid, especially winding region itself. And then, the magnetic field by toroidal arrangement of solenoids was computed with a coordinate transformation of vector fields. The superconducting magnet with toroidal arrangement can be made up of several tens of solenoid type double pancake windings for some applications such as superconducting magnetic energy storage system(SMES). In this system, the field calculation on the high-Tc superconducting(HTS) tape itself is very important because the entire system can be reached to a fault by magnetic stress of conductor or the critical current of superconducting tape can be dramatically reduced under its self field condition. To make matters worse, 3-dimensional analysis is indispensable for this type of magnet and the most of commercial programs with finite element method can be taken too much time for analysis and design. In this paper, a magnetic field calculation method for toroidal type winding with circular section was induced.

• 한국초전도ㆍ저온공학회논문지
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• 제25권4호
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• pp.75-80
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• 2023

Rare earth barium copper oxide (REBCO) materials have shown the possibility of high-temperature superconductor (HTS) magnetic resonance imaging (MRI) magnets due to their elevated transition temperature. While numerous MRI magnet designs have emerged, there is a growing emphasis on estimating the cost before manufacturing. In this paper, we propose two designs of REBCO whole-body MRI magnets: (1) 1.5 T and (2) 3.0 T, the standard center field choices for hospital use, and compare their costs based on conductor usage. The basis topology of the design method is based on discretized solenoids to enhance field homogeneity. Magnetic stress calculation is done to further prove the mechanical feasibility of their construction. Multi-width winding technique and outer notch structure are used to improve critical current characteristic. We apply consistent constraints for current margins, sizes, and field homogeneities to ensure an equal cost comparison. A graph is plotted to show the cost increase with magnetic flux growth. Additionally, we compare our designs to two additional MRI magnet designs from other publications with respect to the cost and magnetic flux, and present the linear relationship between them.

• 새물리
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• 제68권12호
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• pp.1293-1301
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• 2018

시판 중인 고온초전도 GdBCO 박막선재의 기본적인 자기적 특성들을 PPMS-VSM 장비를 이용하여 조사하였다. ZFC m(T) 곡선으로부터 $T_c$ 는 ~93 K였다. m(H) 배경데이터를 제거한 후, GdBCO 초전도층의 알짜 m(H) 데이터를 얻고, ${\Delta}m_{irr}$ 을 구하였다. $H_{irr}(T)$ 곡선은 $H_{irr}=H_{irr}(0)(1-T/T_c)^n$ 관계식과 잘 일치하고, n 값은 1.19이다. GdBCO 박막선재의 $J_c$ 와 H의 $J_c{\propto}{\Delta}M_{irr}{\propto}{\Delta}m_{irr}{\propto}H^{-{\delta}}$ 관계식의 ${\delta}$ 값으로부터 자속 특성을 조사하였다. 독립적인 자속고정효과를 나타내는 ${\delta}{\approx}0$ 인 영역, 상호작용의 집단적인 자속고정효과를 나타내는 ${\delta}{\approx}0.6{\sim}1.2$인 영역, 그리고 로렌츠 힘을 받아 자속들이 자유롭게 움직이는 ${\delta}{\gg}2$ 영역 등으로 구분할 수 있다. ${\delta}{\approx}0$ 특성에서 ${\delta}{\approx}0.6{\sim}1.2$ 특성으로 변화하는 자기장을 $H_1$ 으로, ${\delta}{\approx}0.6{\sim}1.2$ 특성에서 ${\delta}{\gg}2$ 특성으로 전이하는 자기장을 $H_2$ 라 하였다. $H_1$ < H < $H_2$ 영역에서 ${\delta}(T)$ 관계를 구하였고, 온도가 감소함에 따라 ${\delta}$ 값은 점차적으로 줄어들었다.