• KIEE International Transactions on Electrophysics and Applications
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• v.3C no.6
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• pp.211-215
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• 2003

Alternating current (AC) losses of two Bi-2223 ([Bi, Pb] : Sr : Ca : Cu :O = 2:2:2:3) tapes [one untwisted (Tape I, twist-pitch of $\infty$ mm) and the other with a twist-pitch of 8mm (Tape II) ] were measured and compared. These samples, produced by the powder-in-tube (PIT) method, are multi-filamentary and have a Ag/Au and Ag matrix, respectively. Susceptibility measurements were conducted while cooling in a magnetic field. Flux loss measurements were conducted as a function of ramping rate, frequency and field direction. The AC flux loss increases as the twist-pitch of the tapes decreased, in agreement with the Norris Equation.

• Proceedings of the KIEE Conference
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• 1996.07c
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• pp.1660-1662
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• 1996

Superconducting current lead is one of the promising applications of the oxide high-Tc superconductors, because they have the advantage of decreasing heat conduction to low temperature region, comparing with a conventional cooper alloy lead. High critical current density is a key factor for the applications such as current lead. $(Bi,Pb)_{2}Sr_{2}Ca_{2}Cu_{3}O_{x}$ high Tc superconductor hase been investigated in terms of critical current density. Bi-2223 superconducting current lead made by CIP and solid state sintering process. Bi-2223 current lead that heat treated at $836\;^{\circ}C$ for 240 h in 1/13 $PO_2$ had over $500\;A/cm^2$ of critical current density at 77K. We knew that the superconducting properties of tube type current leads were better than rods type of them. And we investigated the relation of Bi-2223 formation and heat treatment condition by XRD and SEM analysis.

• 한국초전도학회:학술대회논문집
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• v.10
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• pp.65-65
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• 2000

Microwave response of intrinsic Josephson junctions in mesa structure formed on HgI2-intercalated Bi2Sr2CaCu2O8+x single crystals was studied in a wide range of microwave frequency. With irradiation of 73${\sim}$76 GHz microwave, the supercurrent branch becomes resistive above a certain onset microwave power. At low current bias, the current-voltage characteristics show linear behavior, while at high current bias, the resistive branch splits into multiple sub-branches. The voltage spacing between neighboring sub-branches increase with the microwave power and the total number of sub-branches is almost identical to the number of intrinsic Josephson junctions in the mesa. All the experimental results suggest that each sub-branch represents a specific mode of collective motion of Josephson vortices generated by the microwave irradiation. With irradiation of microwave of microwave of frequency lower than 20 GHz, on the other hand, no branch splitting was observed and the current-voltage characteristics exhibited complex behavior at hlgh blas currents. This result can be explained in terms of incoherent motion of Josephson vortices generated by non-uniform microwave irradiation.

• Proceedings of the KIEE Conference
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• 2006.10a
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• pp.44-45
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• 2006

We have fabricated superconductor ceramics by chemical process. A high Tc superconductor with a nominal composition of ${Bi_2}{Sr_2}{Ca_2}{Cu_3}{O_y}$ was prepared by the organic metal salts method. Experimental results suggest that the intermediate phase formed before the formation of the superconductorphase may be the most important factor. The relation between electromagnetic properties of Bi HTS and external applied magnetic field was studied. The electrical resistance of the superconductor was increased by the application of the external magnetic field. But the increase in the electrical resistance continues even after the removal of the magnetic field. The reason is as followsthe magnetic flux due to the external magnetic field penetrates through the superconductor and the penetrated magnetic flux is trapped after the removal of the magnetic flux.

• 한국초전도학회:학술대회논문집
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• v.16
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• pp.85-85
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• 2006

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2004.07b
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• pp.1218-1221
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• 2004

Bi2212 superconducting thin films fabricated by using the ion Beam Sputtering Method. As a result, although the composition of Bi2212 was set up, the phase of Bi2201, Bi2212 and Bi2223 was formed. The formation area of these stable phases is indicated as inclined line in the direction of the right lower end from the Arrhenius plot of the substrate temperature-oxidation gas pressure, and are distributed in very small area. The activation energy for the phase transformation from the Bi2201 to the Bi2212 is estimated in terms of the Avrami equation.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 1992.05a
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• pp.58-63
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• 1992

Effects of the second sintering process on the superconducting characteristics of the (Bi, Pb)SrCaCuO system have been studied. It was found that the optimal calcining temperature of mixed powder may be proper to 820$^{\circ}C$ and the optimal sintering temperture was determined on 845$^{\circ}C$. The 2212 phases transitioned the 2223 phasses during the sintring process and zero resistance was attained at 108 K for the samples sintered for 264 hr. The 2223 phases changed into the 2212 phases and nonsuperconducting phases by the second grinding process. And the 2223 phases did not recover easily by the second sintering process.

• Journal of the Korean institute of surface engineering
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• v.39 no.2
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• pp.57-63
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• 2006

In this study, In-base solder was applied to the interface between $Bi_2Sr_2Ca_1Cu_2O_x(Bi_{2212})$ superconductor and Cu-Ni shunt metal at the temperature lower than $150^{\circ}C$. Most of the cases, $Bi_{2212}$ superconductor was precoated with Ag by electroplating in order to improve the contact properties of the solder layer. When the superconductor was directly soldered on to the superconductor, the solder was easily separated without external force. The shear strength of the contact between superconductor and shunt metal increased from 69.2 kgf to 74.4 kgf and 80.1 kgf, as the current density of the Ag electroplating was changed from 63 mA to 96 mA and 126 mA, respectively. The contact strength also increased to 49.9 kgf and 69.2 kgf when thickness of the electroplated Ag layer increased to $5{\mu}m$ and $10{\mu}m$, reapectively.

• Superconductivity and Cryogenics
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• v.1 no.2
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• pp.14-20
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• 1999

초전도 재료는 선재의 형태로 가공하면 송전선이나 변압기, 발전기 그리고 전력 저장장치 등에 사용되어 전력계통의 효율을 극대화시킬 수 있는 재료로서 실제 응용 기기의 개발을 위해 많은 연구가 수행되고 있다. 더우기 1980년대 후반에 개발된 고온초전도 산화물 재료는 액체질수의 비등점인 77K 이상에서 초전도현상을 나타내어 초전도 현상의 응용에 대한 기대를 고조시켜 이에 대한 연구를 더욱 활성화시키고 있다. 초전도선재 연구는 그간 PIT(Powder in Tube) 공정을 이용한 Ag/Bi-2223(Ag/$Bi_2Sr_2Ca_2Cu_3O$) 선재가 높은 전기적 성질과 장선 가공상의 잇점으로 인해 많은 연구와 성과가 있었다. 그러나 Ag/Bi-2223선재는 강한 자기장 하에서 통전 능력이 현저하게 저하되는 성질 때문에 높은 자기장하에서 사용하기 위해서는 사용온도를 액체질소온도보다 상당히 낮은 20K 부근까지 낮추어야 한다는 점 때문에 전력기기 개발에 제한이 따르는 단점이 있다. 이에 반해 최근에 개발된 금속/YBCO 박막 복합선재는 높은 전기적 특성 이외에 특히 높은 자장에서도 통전 능력의 저하가 적어 제한 없이 전력기기의 모든 분야에 사용할 수 있는 특징이 있다. 따라서 1993년에 일본에서 Ni 금속기판에 물리적 증착방법으로 YBCO($YiBa_2Cu_3O$) 박막을 증착시킨 선재제조에 성공하고 있어 1996년에 Oak Ridge National Laboratories (ORNL)에서 Rolling Assisted Biaxially Textured Substrate (RaBiTS) 라는 집합조직을 형성시킨 금속기판이 개발되어 연속적인 가공의 가능성이 확인된 후 이의 특성향상 및 가공기술 개발을 위한 많은 연구가 수행되고 이다. 이 글에서는 이제 까지 개발된 금속기판을 사용한 YBCO계 초전도 박막형 선재의 제조기술 중에서 최근 가장 가능성 있는 것으로 평가되는 RABiTS 방법을 위주로 그 외에 IBAD와 ISD 방법에 관하여 소개하고 현재까지의 개발현황 및 앞으로의 전망에 대하여 간략하게 기술하고자 한다.

• Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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• 2002.07a
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• pp.94-97
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• 2002

BSCCO (2223) compound which has the highest temperature of transition to the superconducting state in the homologous series considered is synthesized by SHS. The method exploits self-sustaining solid-flame combustion reactions which develop very high internal material temperatures over short periods. This report introduces the SHS method and its advantages and discusses its application in the synthesis of superconducting materials.