Recent Progress in Compact, Robust, and Superior Field-Tolerant QMG Current Leads Using RE–Ba–Cu–O Bulk Superconductors

High-temperature superconducting (HTS) bulk materials of RE-Ba-Cu-O (RE: Y or rare-earth elements) exhibit excellent Jc properties, even at 77 K, leading to current leads with large current capacity and superior magnetic field tolerance. The thermal conductivity of HTS bulk materials is two orders of magnitude smaller than that of the conventional current lead material of copper, and Dy-Ba-Cu-O has particularly low thermal conductivity in the RE-Ba-Cu-O family. Unlike HTS wires, HTS bulks have no metal sheath such as silver or silver alloys with high thermal conductivity, resulting in the reduction of heat leak through the current lead, even in the compact size. Although they are a kind of brittle ceramic or oxide, HTS bulks can be transformed into robust current leads by reinforcing them with the support cover made of glass-fiber-reinforced plastics with low thermal conductivity and high strength. In addition to excellent mechanical stress tolerance, HTS bulk current leads also have a robust structure that minimizes thermal stress, which was experimentally demonstrated by a rapid cooling test to liquid nitrogen over 100 cycles. Due to distinctive advantages such as compactness, robustness, and superior field tolerance, more than 500 pieces of HTS bulk current leads have been successfully provided so far.

[1]  T. Sonobe,et al.  Low-Temperature Operation of a Bulk HTSC Staggered Array Undulator , 2012, IEEE Transactions on Applied Superconductivity.

[2]  Tomoyuki Haishi,et al.  Development of a magnetic resonance microscope using a high Tc bulk superconducting magnet , 2011 .

[3]  Mitsuru Sawamura,et al.  Processing and properties of QMG materials , 1994 .

[4]  Force Density of Magnetic Bearings Using Superconducting Coils and Bulk Superconductors , 2008 .

[5]  Takashi Nakamura,et al.  Experimental evaluation of the magnetization process in a high Tc bulk superconducting magnet using magnetic resonance imaging , 2013 .

[6]  H. Teshima,et al.  Low-Thermal-Conductive$rm DyBaCuO$Bulk Superconductor for Current Lead Application , 2006, IEEE Transactions on Applied Superconductivity.

[7]  M. Morita,et al.  Critical current of Y-Ba-Cu-O bulk current leads , 2004, IEEE Transactions on Applied Superconductivity.

[8]  Materials processing and machine applications of bulk HTS , 2010 .

[9]  M. Miki,et al.  An axial gap-type HTS bulk synchronous motor excited by pulsed-field magnetization with vortex-type armature copper windings , 2005, IEEE Transactions on Applied Superconductivity.

[10]  M. Murakami,et al.  Processing and superconducting properties of high-Jc bulk YBaCuO prepared by melt process☆ , 1990 .

[11]  N. Nishijima,et al.  Development of a Palm-sized Miniature Superconducting Bulk Magnet , 2012 .

[12]  M. Murakami,et al.  Magnetic Separator for Water Treatment Using Superconducting Bulk Magnets , 2002 .

[13]  Hideo Kitamura,et al.  Magnetic characterization for cryogenic permanent-magnet undulators: a first result. , 2007, Journal of synchrotron radiation.

[14]  H. Nakao,et al.  Development of a low heat leak current-lead system , 2004, IEEE Transactions on Applied Superconductivity.