• Title/Summary/Keyword: Superconductor bulk

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Magnetic levitation properties of single- and multi-grain YBCO bulk superconductors

  • Kim, C.J.;Yang, A.Y.;Lee, S.H.;Jun, B.H.
    • Progress in Superconductivity and Cryogenics
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    • v.24 no.3
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    • pp.52-56
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    • 2022
  • Single-grain (c-normal or c-parallel) and multi-grain YBCO superconductors were prepared by a melt growth process with/without seeding. The magnetic levitation force and trapped magnetic field at liquid N2 temperature (77 K) of the YBCO superconductors were investigated. Samples for the levitation force measurement were zero-field cooled (ZFC) to 77 K, and samples for trapped field measurement were field-cooled (FC) using Nd magnets. As for the magnetic levitation force, the c-normal, single grain sample showed the largest value, whereas the multi-grain sample showed the lowest value. The trapped magnetic field of the c-normal and c-parallel single-grain samples was 4-5 times that of the multi-grain sample. In addition, as the external magnetic field (the number of magnets) increased, the both properties increased proportionally. These results were explained in terms of the orientation dependence of the levitation forces and the magnetic field trapping capability of the YBCO superconductor.

Enhanced superconducting properties of MgB2 by doping the carbon quantum dots

  • K.C., Chung;S.H., Jang;Y.S., Oh;S.H., Kang
    • Progress in Superconductivity and Cryogenics
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    • v.24 no.4
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    • pp.55-58
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    • 2022
  • Carbon-based doping to MgB2 superconductor is the simplest approach to enhance the critical current densities under magnetic fields. Carbon quantum dots is synthesized in this work as a carbon provider to MgB2 superconductors. Polyvinyl Pyrrolidone is pyrolyzed and dispersed in dimethylfomamide solvent as a dopant to the mixture of Mg and B powders. Doped MgB2 bulk samples clearly show the decrease of a-axis lattice constant, grain refinements, and broadening of FWHM of diffraction peaks compared to un-doped MgB2 possibly due to the carbon substitution and/or boron vacancy at the boron site in MgB2 lattice. Also, high-field Jc for the doped MgB2 is enhanced significantly with the crossover about 3 T at 5 & 20 K when increasing the doping of carbon quantum dots.

Mechanical Properties of YBCO Superconductors with Impregnation Materials (보강재를 첨가한 YBCO 초전도체의 기계적강도 변화)

  • Lee, Nam-Il;Jang, Gun-Eik;Lee, Sang-Heon;Kim, Chan-Jung
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 2006.06a
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    • pp.247-248
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    • 2006
  • Bulk YBCO 초전도체는 top-seeded melt-growth 방법으로 제조되었다. YBCO bulk는 Epoxy resin과 $AgNO_3$를 보강해 초전도체의 기계적 강도를 향상하고자 하였다. Epoxy resin은 보강 재료인 STYCAST 2850-FT와 경화제인 CATALYST 24LV 를 100:5 비율로 혼합하여 제조한 후 mould에 넣고 $66^{\circ}C$에서 2시간 열처리 하였다 (rotary pump로 진공 분위기 조성). $AgNO_3$$350^{\circ}C$에서 2시간, $450^{\circ}C$에서 1시간 열처리 하여 Ag와 $NO_3$의 분리 후 YBCO bulk에 Ag가 보강되도록 하였다. Epoxy resin 과 분리된 Ag는 YBCO bluk의 crack과 void에 침투되는 것을 SEM과 광학현미경을 통해 관찰할 수 있었다. Three point bending test를 이용하여 보강 전후의 YBCO bulk의 기계적 강도를 측정하였다. 보강 후의 YBCO bluk의 기계적 강도는 보강 전에 비해 향상된 결과를 확인할 수 있었고, Epoxy resin과 $AgNO_3$를 보강한 YBCO는 기계적 강도 향상에 높은 신뢰성을 보이고 있다.

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The fabrication of bulk magnet stacked with HTS tapes for the magnetic levitation

  • Park, Insung;Kim, Gwantae;Kim, Kyeongdeok;Sim, Kideok;Ha, Hongsoo
    • Progress in Superconductivity and Cryogenics
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    • v.24 no.3
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    • pp.47-51
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    • 2022
  • With the innovative development of bio, pharmaceutical, and semiconductor technologies, it is essential to demand a next-generation transfer system that minimizes dust and vibrations generated during the manufacturing process. In order to develop dust-free and non-contact transfer systems, the high temperature superconductor (HTS) bulks have been applied as a magnet for levitation. However, sintered HTS bulk magnets are limited in their applications due to their relatively low critical current density (Jc) of several kA/cm2 and low mechanical properties as a ceramic material. In addition, during cooling to cryogenic temperatures repeatedly, cracks and damage may occur by thermal shock. On the other hand, the bulk magnets made by stacked HTS tapes have various advantages, such as relatively high mechanical properties by alternate stacking of the metal and ceramic layer, high magnetic levitation performance by using coated conductors with high Jc of several MA/cm2, consistent superconducting properties, miniaturization, light-weight, etc. In this study, we tried to fabricate HTS tapes stacked bulk magnets with 60 mm × 60 mm area and various numbers of HTS tape stacked layers for magnetic levitation. In order to examine the levitation forces of bulk magnets stacked with HTS tapes from 1 to 16 layers, specialized force measurement apparatus was made and adapted to measure the levitation force. By increasing the number of HTS tapes stacked layers, the levitation force of bulk magnet become larger. 16 HTS tapes stacked bulk magnets show promising levitation force of about 23.5 N, 6.538 kPa at 10 mm of levitated distance from NdFeB permanent magnet.

Stiffness Evaluation of High Temperature Superconductor Bearing Stiffness for 10 kWh Superconductor Flywheel Energy Storage System (10 kWh급 초전도 플라이휠 베어링의 강성 평가)

  • Park, B.J.;Jung, S.Y.;Lee, J.P.;Park, B.C.;Kim, C.H.;Han, S.C.;Du, S.G.;Sung, T.H.;Han, Y.H.
    • Progress in Superconductivity
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    • v.11 no.1
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    • pp.57-61
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    • 2009
  • A superconductor flywheel energy storage(SFES) system is mainly act an electro-mechanical battery which transfers mechanical energy into electrical form and vice versa. SFES system consists of a pair of non-contacting High Temperature Superconductor (HTS) bearings with a very low frictional loss. But it is essential to design an efficient HTS bearing considering with rotor dynamic properties through correct calculation of stiffness in order to support a huge composite flywheel rotor with high energy storage density. Static properties of HTS bearings provide data to solve problems which may occur easily in a running system. Since stiffness to counter vibration is the main parameter in designing an HTS bearing system, we investigate HTS bearing magnetic force through static properties between the Permanent Magnet(PM) and HTS. We measured axial / radial stiffness and found bearing stiffness can be easily changed by activated vibration direction between PM and HTS bulk. These results are used to determine the optimal design for a 10 kWh SFES.

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Preparation and Its Properties of YBCO Superconductor Induced by Seeds

  • Shan, Y.Q.;Soh, D.W.;Fan, Z.G.;Men, M.F.;Wang, W.H.;Zhao, Z.X.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1998.06a
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    • pp.371-373
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    • 1998
  • The SmBa$_2$Cu$_3$O$\sub$x/ single crystals were used as seeds to induced YBCO growth in MTG process. As the result, the large bulk oriented YBCO superconductors were prepared with dimension of plane 21mm and 32mm in diameter and 10mm in height. The typical Jc value of the sample is 6.5${\times}$10$^4$A/$\textrm{cm}^2$ and its flux float force is 4.6N/$\textrm{cm}^2$. The oxygen absorption in large bulk textured YBCO samples in pure oxygen was studied at several constant temperatures. It can be divided into two steps: a chemical reaction step and a diffusion step.

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Preparation and Its Properties of YBCO Superconductor Induced by Seeds

  • Shan, Y.Q.;Soh, D.W.;Fan, Z.G.;Men, M.F.;Wang, W.H.;Zhao, Z.X.
    • Proceedings of the Korean Institute of Electrical and Electronic Material Engineers Conference
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    • 1998.06a
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    • pp.491-493
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    • 1998
  • The SmBa$_2$Cu$_3$O$\sub$x/ single crystals were used as seeds to induced YBCO growth in MTG process. As the result, the large bulk oriented YBCO superconductors were prepared with dimension of plane 21mm and 32mm in diameter and 10mm in height. The typical Jc value of the sample is 6.5${\times}$10$^4$A/$\textrm{cm}^2$ and its flux float force is 4.6N/$\textrm{cm}^2$. The oxygen absorption in large bulk textured YBCO samples in pure oxygen was studied at several constant temperatures. It can be divided into two steps: a chemical reaction step and a diffusion step.

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Feasible waste liquid treatment from electroless nickel-plating by intense magnetic field of HTS bulk magnets

  • Oka, T.;Furusawa, M.;Sudo, K.;Dadiel, L.;Sakai, N.;Seki, H.;Miryala, M.;Murakami, M.;Nakano, T.;Ooizumi, M.;Yokoyama, K.;Tsujimura, M.
    • Progress in Superconductivity and Cryogenics
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    • v.23 no.3
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    • pp.37-40
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    • 2021
  • Nickel (Ni) is a kind of the rare earth resources. Since Ni-containing waste is drained after several plating operations in the factories, the effective recycling technique has been expected to be introduced. An actual magnetic separation technique using HTS bulk magnet generating the strong magnetic field has succeeded in collecting the paramagnetic slurry containing Ni-sulphate coarse crystals which were fabricated from the Ni-plating waste. The Ni compound in the collected slurry was identified as NiSO4/6H2O, showing slight differences in the particle size and magnetic susceptibility between the samples attracted and not-attract to the magnetic pole. This preferential extraction suggests us a novel recycling method of Ni resource because the compound is capable of recycling back to the plating processes as a raw material.