• 제목/요약/키워드: YBCO bulk

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The recent investigation and engineering application of YBCO bulk materials

  • Hong, Z;Jiang, Y;Viznichenko, R V;Coombs, T A
    • 한국초전도ㆍ저온공학회논문지
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    • 제10권2호
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    • pp.1-11
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    • 2008
  • The application of bulk superconducting materials to electrical power systems is very attractive because bulk high temperature superconductors offer excellent electromagnetic properties. In recent years there has been significant progresses in the research and fabrication of superconducting bulk materials. Numerous efforts have been made worldwide to make bulk YBCO as a replacement of the conventional magnets to produce larger magnetic field and hence to improve the device performance in electrical power applications. This paper gives a comprehensive review of different applications of bulk HTS materials, concentrating in three areas including superconducting bearing, superconducting motors and high field magnets. The advantages of applying superconducting material into each application are analysed. The status of current research in each section is summarized and examples are given to demonstrate how YBCO bulk materials can benefit the design of electrical devices. Several numerical models which calculate the electromagnetic properties of bulk superconductors are introduced and finally the article concludes with a review on the studies of the demagnetisation effect in superconducting bulk magnets which is extremely relevant to applying superconducting technology to rotating machines.

Fabrication of a large grain YBCO bulk superconductor by homo-seeding melt growth method

  • Lee, Hee-Gyoun
    • 한국초전도ㆍ저온공학회논문지
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    • 제24권3호
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    • pp.35-40
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    • 2022
  • To fabricate large grain YBCO bulk superconductors by melt process, Sm123 single crystal with a high melting point are mostly used as seeds. However, it also uses Y123 film deposited on MgO single crystal substrate. This study investigated the growth behavior of the Y123 grain during a melt process when single grain YBCO bulk was used as a seed. Single grain Y123 bulk was grown when the seed size was small. When the seed size was relatively large, multiple grains were grown but the grains were still large. Y123 seed crystal was completely decomposed during high temperature anneal at 1040℃ and new Y123 crystals were nucleated during a slow cooling stage below a peritectic temperature. Thereafter, newly formed Y123 crystals from the seed area are thought to grow into the Y1.8 powder compact. The crystallographic orientations of newly nucleated Y123 grains are independent of the crystallographic orientation of Y123 seed. It is thought that the crystallographic orientation of newly nucleated Y123 crystal can be controlled by using Y211-free Y123 single crystal as a seed of homo-seeding melt growth.

대면적 YBCO 고온 초전도 벌크 자석 및 조작기 개발 (Development of Large-sized YBCO High Temperature Superconductor Bulk Magnets and Actuator)

  • 한상철;박병준;정세용;한영희;이종원
    • 한국전기전자재료학회논문지
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    • 제28권7호
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    • pp.450-455
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    • 2015
  • For the practical application of a YBCO superconductor bulk, the superconductor bulk magnet with high magnetic field on a large area surface should be fabricated. To make this, YBCO single crystal bulks with fine $Y_2BaCuO_5$(Y211) particles have been prepared by the top-seed melt growth(TSMG) method with $YBa_2Cu_3O_x$, $Y_2O_3$, and $CeO_2$ mixing precursor. By using $Y_2O_3$ instead of $Y_2BaCuO_5$ as precursor, the manufacturing process became simpler and more economical. The microstructures, trapped field and critical current density of the various conditioned YBCO bulks have been observed, analyzed and measured. The different characteristic values of the several samples have been analyzed from the viewpoint of their microstructures. We have developed a $8{\times}12cm$ size superconductor bulk magnet, up to 3 T class, by using the 4 T class-high field superconducting magnetizer and confirmed the applicability of the transmission level circuit breakers by measuring the strength and speed of the superconductor bulk magnet actuator.

YBCO 초전도체 Bulk 소재에 대한 자기적 특성 (Magnetic Properties of YBCO Superconductor Bulk Materials)

  • 이상헌
    • 한국전기전자재료학회논문지
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    • 제33권2호
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    • pp.147-150
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    • 2020
  • Relatively pure YBCO was first synthesized by heating a mixture of metal carbonates at temperatures between 1,000 and 1,300 K, resulting in the reaction: 4BaCO3+Y2(CO3)3+6CuCO3+(1/2-x)O2 → 2YBa2Cu3O7-x+1/3CO2. Modern syntheses of YBCO use the corresponding oxides and nitrates. The superconducting properties of YBa2Cu3O7-x are sensitive to the value of x, i.e., its oxygen content. Only those materials with 0≤x≤0.65 are superconducting below Tc, and when x ~ 0.07, the material superconducts at the highest temperature, i.e., 95 K, or in the highest magnetic fields, i.e., 120 T and 250 T when B is perpendicular and parallel to the CuO2 planes, respectively. In addition to being sensitive to the stoichiometry of oxygen, the properties of YBCO are influenced by the crystallization methods applied. YBCO is a crystalline material, and the best superconductive properties are obtained when crystal grain boundaries are aligned by careful control of annealing and quenching temperature rates. However, these alternative methods still require careful sintering to produce a quality product. New possibilities have arisen since the discovery of trifluoroacetic acid, a source of fluorine that prevents the formation of undesired barium carbonate (BaCO3). This route lowers the temperature necessary to obtain the correct phase at around 700℃. This, together with the lack of dependence on vacuum, makes this method a very promising way to achieve a scalable YBCO bulk.

Bi/CNT 화합물과 Resin/CNT를 보강한 YBCO 초전도체의 기계적, 자기적 특성 변화 (Mechanical and Magnetic Properties of YBCO Superconductor with Bi/CNT Composite and Resin/CNT Impregnation)

  • 오원석;장건익;한영희;성태현
    • Progress in Superconductivity
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    • 제9권1호
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    • pp.107-110
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    • 2007
  • Bi/CNT composite and resin/CNT were chosen to improve the mechanical properties of $YBa_2Cu_3O_7$(YBCO) superconductor. In order to elucidate the effects of Bi/CNT composite and resin/CNT in YBCO superconductors, melt texture superconductor were impregnated by mixed compound of Bi and CNT into the artificial holes parallel to the c-axis, which were drilled on the YBCO superconductor. Various amount of Bi/CNT and resin/CNT were impregnated to YBCO superconductor with different holes diameters. Typical artificial holes diameters were 0.5, 0.7, and 1.0 mm respectively. Result of three-point bending test measurement, the bending strength with resin/CNT impregnation was improved up to 59.64 MPa as compared with 50.79 MPa of resin/CNT free bulk. Resin/CNT impregnation has been found to be one of the effective ways in improving the mechanical properties of bulk superconductor.

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고온초전도자석 충전용 히터트리거 스위칭 시스템에 관한 연구 (A Study on the Heater-Triggered Switching System for Charging of a HTS Magnet)

  • 배덕권;안민철;최석진;김영식;김호민;이찬주;윤용수;이상진;신철기
    • 한국초전도저온공학회:학술대회논문집
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    • 한국초전도저온공학회 2001년도 학술대회 논문집
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    • pp.76-79
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    • 2001
  • The heater-triggered switching system for charging of a high temperature superconductor(HTS) is prepared by simulation and investigated its characteristic by experiment. heater-triggered switching system consists of two nickel-chrome alloy heater, an electromagnet and YBCO bulk HTS. There are three important parameters to generate the pumping-current in this system. The timing sequential control of two heters and electromagnet is an important factor to generate pumping-current in the YBCO bulk HTS. Thermal analysis of the switching part in YBCO bulk HTS according to the heater input current was carried out. Electromagnet of 0.6[T] and DC heater input current of 2.3[A] were optimally derived. In this experiment, the maximum pumping current is reaches about 12[A].

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고온초전도 벌크 베어링을 사용한 유도 전동기의 특성 시험 (Performance Tests of an Induction Motor with Hexahedron HTS Bulk Bearing)

  • 임형우;이광윤;박명진;차귀수;이지광
    • 대한전기학회논문지:전기기기및에너지변환시스템부문B
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    • 제52권6호
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    • pp.286-290
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    • 2003
  • The high temperature superconducting bulk can be used as the bearing of induction motors. This paper presents the fabrication and test results of an induction motor with superconducting bearings using HTS bulks. The bearing had eight hexahedron type YBCO bulks. Height, width and thickness of the HTS bulk were 30mm, 30mm and 10mm, respectively. Single phase induction motor was used to drive the shaft made of aluminum and the rotor of a conventional induction motor. To estimate the performance of the HTS bulk magnetic bearing, no load test, load test and Impact test were carried out. Load tests were performed by using air resistance caused by the shaft-mounted thin cylinder with buckets. Impact tests by axial direction and vertical direction impact showed that the vibration of the shaft gradually decayed. The induction motor with HTS bulk magnetic bearing rotated silently and smoothly throughout the tests. According to the test results, conventional bearings can be replaced with superconducting magnetic bearings made of HTS bulks.

단결정 Y1.5Ba2Cu3O7-y 벌크 초전도체의 냉각효율에 대한 인공 구멍의 효과 (Effects of artificial holes on the cooling efficiency of single grain Y1.5Ba2Cu3O7-y bulk superconductors)

  • 김광모;박순동;전병혁;고태국;김찬중
    • 한국초전도ㆍ저온공학회논문지
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    • 제14권3호
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    • pp.1-4
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    • 2012
  • Effects of artificial holes on the cooling efficiency of single grain YBCO bulk superconductors were studied. Single grain YBCO bulk superconductors without artificial holes, with six 2.4 mm holes and six holes filled with Bi-Pb-Cd-Sn metal solder were fabricated by a top-seeded melt growth process for powder compacts with/without holes. Simulation for the cooling rate to a liquid nitrogen temperature (77 K) of YBCO samples was carried out using a finite element method (FEM) and the results are compared with the actual cooling rates of samples in liquid nitrogen. The simulated cooling times for the YBCO sample without holes, with six holes and with six holes filled with the metal solder were 80, 47 and 75 sec. respectively, which are similar to the actual cooling times of 84, 52 and 78 sec. estimated for the same samples cooled in liquid nitrogen. The shorter cooling time of the sample with artificial holes are attributed to the increased surface areas associated with the presence of artificial holes. The metal filling into the holes did not give any remarkable effect on the cooling efficiency.