• 제목/요약/키워드: High-Tc Superconductors

검색결과 55건 처리시간 0.018초

순차적 순환배열을 이용한 고온초전도 배열 안테나 설계 및 특성해석 (Design and Characterization of HTS antenna array with sequential rotation array)

  • 정동철;황종선;김영민;최효상
    • 한국전기전자재료학회:학술대회논문집
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    • 한국전기전자재료학회 2006년도 영호남 합동 학술대회 및 춘계학술대회 논문집 센서 박막 기술교육
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    • pp.77-81
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    • 2006
  • We report the performance of a four-element, 11.67 GHz, high-Tc superconducting (HTS) microstrip antenna array with corporate feed network and circular polarization for direct broadcasting satellite (DBS) system. Our array antennas were designed and built on a 0.5 mm thick MgO substrate. To compare the superconducting antennas with normal conducting counterpart, One antenna pattern was fabricated from gold thin film, and a second pattern was fabricated from $YBa_2Cu_3O_{7-x}$ (YBCO) superconducting thin film. To improve the axial ratio of circularly polarized arrays, sequential rotation technique were used. Efficiency, radiation pattern, return loss and bandwidth were measured for both antennas at room temperature and at cryogenic temperature. The array produced good circular polarization, and the gain of the array at 77 K, relative to a copper array at room temperature was approximately 1.54 dB. The measured return loss of our HTS antenna array was 35.79 dB at the resonant frequency of 11.67 GHz and The total effective bandwidth was about 3.4 %. The results showed that high-temperature superconductors, when used in microstrip arrays, improved the efficiency of the HTS antenna array for circularly polarization.

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BSCCO 플라즈마 용사피막의 부분용융열처리 후 어닐링 시간에 따른 초전도 특성 (Characteristics of Plasma Sprayed BSCCO Superconductor Coatings with Annealing Time After Partial Melt Process)

  • 박정식;이선홍;박경채
    • 한국재료학회지
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    • 제24권2호
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    • pp.116-122
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    • 2014
  • $Bi_2Sr_2CaCu_2O_x$(Bi-2212) and $Bi_2Sr_2Ca_2Cu_3O_y$(Bi-2223) high-Tc superconductors(HTS) have been manufactured by plasma spraying, partial melt process(PMP) and annealing treatment(AT). A Bi-2212/2223 HTS coating layer was synthesized through the peritectic reaction between a 0212 oxide coating layer and 2001 oxide coating layer by the PMP-AT process. The 2212 HTS layer consists of whiskers grown in the diffusion direction. The Bi-2223 phase and secondary phase in the Bi-2212 layer were observed. The secondary phase was distributed uniformly over the whole layer. As annealing time goes on, the Bi-2212 phase decreases with mis-orientation and irregular shape, but the Bi-2223 phase increases because a new Bi-2223 phase is formed inside the pre-existing Bi-2212 crystals, and because of the nucleation of a Bi-2223 phase at the edge of Bi-2212 crystals by diffusion of Ca and Cu-O bilayers. In this study the spray coated layer showed superconducting transitions with an onset Tc of about both 115 K, and 50 K. There were two steps. Step 1 at 115 K is due to the diamagnetism of the Bi-2223 phase and step 2 at 50 K is due to the diamagnetism of the Bi-2212 phase.

성형 압력변화에 따른 고온초전도체 $Y_1Ba_2Cu_3O_7-\delta$ (Structural and electrical property studies dependent on the molding pressure in high-Tc superconductor $Y_1Ba_2Cu_3O_7-\delta$)

  • 김채옥;박정수;이교운
    • E2M - 전기 전자와 첨단 소재
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    • 제9권1호
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    • pp.18-23
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    • 1996
  • The molding pressure is also one of the important parameters in the preparation of HTSC materials by the solid state reaction method. In the present study, changes in structural, electrical and microstructural proper-ties with the molding pressure in YiB $a_{2}$C $u_{3}$ $O_{70{\delta}}$ superconductors have been performed. The investigated molding pressures were 0.5*10$^{3}$ N/c $m^{2}$, 1*10$^{3}$ N/c $m^{2}$, 2*10$^{3}$ n/c $m^{2}$ and 4*10$^{3}$ N/c $m^{2}$. As the molding pressure increased, the anisotropy of the crystal structure decreased and the grains have been grown preferentially in a c-axis direction. Since the size of the grain becomes larger with the decrease of the porosity, denser textures are formed. The results indicated that the critical current density is improved resulting from the enhanced densification due to higher molding pressure. When the molding pressure was between 1*10$^{3}$ N/c $m^{2}$ and 2*10$^{3}$ N/c $m^{2}$, while it did not affect the oxygen deficiency and Tc, the increase of the molding pressure affects remarkably on grain size and densification of the $Y_{1}$B $a_{2}$C $u_{3}$ $O_{7-{\delta}}$. When the molding pressure is larger than 2*10$^{3}$ N/c $m^{2}$, electrical proper-ties are independent on the molding pressure..

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수송전류에 따른 Bi-2223 선재의 전기적 열화 (The Electrical De연세대학교 전기전자공학과gradation Rate of a Bi-2223 wires by the Various Transferred Current)

  • 배덕권;이상진;배준한;고태국;박경엽
    • 대한전기학회:학술대회논문집
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    • 대한전기학회 2002년도 하계학술대회 논문집 B
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    • pp.831-834
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    • 2002
  • Several companies in the world are marketing superconducting wires, films and bulks. High-Tc superconducting systems using these superconductors are begun to commercialize. For the successful realization or commercialization of superconducting system used Bi-2223 wires, the database on the degradation of critical current is essentially needed. In this paper, the electrical degradation of a Bi-2223 wires is measured. The electrical degradation rate was measured after the certain time of continuous current transportation. Specimens have the length of 190cm and double-pancakes coil have the length of 10m were tested. Tested Bi-2223 wires are commercialized product has 115A of Ic. When the transportation current was 95% of Ie, the degradation of Ic was appeared after 5 hours of transportation time. When the transferred current is enough larger than Ic, Bi-2223 double pancake is damaged seriously.

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부유대역용융성장법을 이용한 (Nd/Y)-Ba-Cu-O계 초전도체의 미세구조 (Microstructure of the (Nd/Y)-Ba-Cu-O superconductors by floating zone melt growth process)

  • 김소정
    • 한국결정성장학회지
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    • 제13권2호
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    • pp.83-87
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    • 2003
  • 부유대역용융성장법을 이용한 $(Nd/Y)_{1.8}Ba_{}2.4Cu_{3.4}O_{7-x}$[이하 (Nd/Y)1.8]계 고온초전도체를 대기 중에서 용융성장실험을 하였다. 용융성장에 사용된 (Nd/Y)1.8 시편은 rubber 몰드를 이용해 냉간정수압성형(CIP) 과정을 거쳐 길이방향 원통 형상으로 제조되었다. 용융성장 된 (Nd/Y)1.8 초전도체는 SEM, TEM 그리고 SQUID magnetometer를 이용해 미세구조 및 초전도특성을을 평가하였다. 특히 용융성장 된 (Nd/Y)1.8 초전도체의 SEM에 의한 미세구조 관측 결과 초전도상인 (Nd/Y)123 matrix 내에 비초전도상인 (Nd/Y)211 inclusions이 균질하게 분포되어 있는 것이 관측되었다. 또한 용융성장 된 (Nd/Y)1.8 초전도체는 90K에서 임계온도가 시작되어 77K 이상의 온도에서 포화되는 특성을 보였다.