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    • 1. 发明专利
    • Superconducting cable and magnet using the same
    • 超级电缆和磁铁使用它
    • JP2010262933A
    • 2010-11-18
    • JP2010143230
    • 2010-06-23
    • Toshiba Corp株式会社東芝
    • HAMASHIMA KOTAROONO MICHITAKATAKANO HIROHISA
    • H01B12/08H01F6/00H01F6/06
    • Y02E40/641
    • PROBLEM TO BE SOLVED: To provide a superconducting cable for a large current, having sufficient cable performance with high stability and little loss, and to provide a magnet that uses the cable. SOLUTION: The superconducting cable includes a core 1 in the center; and superconducting element wires 2, 3, 4, 5, 6 disposed at the periphery of the core 1 as three or more coaxial layers. In each layer, the superconducting element wires are twisted together. The superconducting element wires are twisted at shorter pitches than or equal to those of the innermost layer in all the layers except for the innermost layer. Superconducting element wires coated with a conductive material and normal superconducting element wires are arranged alternately, in each layer of the superconducting element wires. COPYRIGHT: (C)2011,JPO&INPIT
    • 要解决的问题:提供一种用于大电流的超导电缆,具有足够的电缆性能,具有高稳定性和少损耗,并提供使用电缆的磁体。

      解决方案:超导电缆包括中心的芯1; 以及设置在芯体1的周边的三根或更多个同轴层的超导元件线2,3,4,5,6。 在每层中,超导元件线被绞合在一起。 超导元件线以除了最内层以外的所有层中的最内层的间隔更短的间距被扭曲。 涂覆有导电材料和正常超导元件导线的超导元件线在超导元件线的每一层中交替布置。 版权所有(C)2011,JPO&INPIT

    • 3. 发明专利
    • MAGNETIC-FIELD CORRECTING COIL
    • JPS63239803A
    • 1988-10-05
    • JP28342086
    • 1986-11-28
    • TOSHIBA CORP
    • HAMASHIMA KOTARO
    • G01R33/3875A61B5/055A61B10/00H01F7/20
    • PURPOSE:To obtain high uniform magnetic-field distribution by symmetrically arranging first and second coil groups, holding a plane in space, mounting first-fourth saddle-shaped coils to each coil group and forming these coils under specific conditions. CONSTITUTION:First and second coil groups 1, 2 having the same constitution are disposed symmetrically into space organized of X, Y and Z axes, holding XY planes. The coil group 1 has first-fourth saddle-shaped coils 11-14. The saddle-shaped coils 11, 13 and 12, 14 are constructed and disposed symmetrically, holding a Z axis respectively, the length of the arcuate sections of separate saddle-shaped coil is brought to length where angles facing both ends of these arcuate sections from the Z axis are at 90 deg., and angles where straight lines facing the arcuate sections of each saddle-shaped coil from an origin forms with the Z axis are set at one of the angles of aperture to the Z axis from the origin represented by Z/r satisfying respective formula shown by the values of cylindrical coordinates (r, phi, Z). The same applies to the coil group 2. Accord ingly, a magnetic field proportional to (X -Y ), an error of which is reduced extremely, is generated selectively, thus acquiring uniform magnetic field distribu tion.
    • 4. 发明专利
    • MAGNETIC FIELD CORRECTING COIL
    • JPS63136505A
    • 1988-06-08
    • JP28264786
    • 1986-11-27
    • TOSHIBA CORP
    • HAMASHIMA KOTARO
    • G01R33/3875A61B5/055A61B10/00H01F7/20
    • PURPOSE:To obtain a uniform high magnetic field distribution by setting angles of first to fourth saddle-shaped coils from an origin with respect to the circular arc parts of the coils to specific angles. CONSTITUTION:First to fourth saddle-shaped coils having circular-arc parts bent around Z-axis of X-, Y-and Z-axes crossing perpendicularly to each other are provided. The first, second and the third, fourth coils are disposed symmetrically through an X-Y plane, and the first, third and the second, fourth coils are disposed symmetrically through the Z-axis. When the lengths of the circular- arcs of the first to fourth coils are set to the lengths that the angles of the coils from the Z-axis to the both ends of the circular-arc parts are 120 deg. and the angle of the linear line from the origin to the circular-arc parts of the first to fourth coils with respect to the Z-axis is represented by the value of cylindrical coordinates (r, phi, z) for indicating the circular-arc part, it is set to one of the opening angles from the origin represented by Z/r for satisfying the equations with respect to the Z-axis. Thus, a magnetic field proportional to the specific sole function can be accurately generated to obtain a uniform high magnetic field distribution.
    • 8. 发明专利
    • SUPERCONDUCTIVE CONDUCTOR
    • JPH04370609A
    • 1992-12-24
    • JP14644191
    • 1991-06-19
    • TOSHIBA CORP
    • HAMASHIMA KOTARO
    • H01B12/12H01F6/06
    • PURPOSE:To prevent quenching by forming a superconductive coil by winding many superconductive wires on the outside circumference of a circular or elliptic hollow pipe and by inhibiting frictional heating between the superconductive wires and the pipe, and between the superconductive wires. CONSTITUTION:A superconductive conductor 3 is formed by winding superconductive wires 2, in moderate numbers, formed by twisting many superconductive strands on the outside circumference of a hollow pipe 1. The pipe 1 is formed in circular or elliptic shape by using stainless steel. an aluminium alloy, a copper alloy, ceramics etc. Therefore, the conductive wires 2 are pressed to the surface of the pipe 1 and will not float from the surface, and has no acute end portion. Thus, no gap is generated between tire conductive wires 2. This prevents quenching without generating heating caused by sliding the conductive wires 2 over the surface of the pipe even if the conductor 3 is excited, or without generating frictional heating between the conductive wires 2.
    • 9. 发明专利
    • SUPERCONDUCTING CONDUCTOR
    • JPH02126519A
    • 1990-05-15
    • JP27931088
    • 1988-11-07
    • TOSHIBA CORP
    • HAMASHIMA KOTARO
    • C22C27/02H01B12/10H01F6/06
    • PURPOSE:To reduce AC loss by winding a metal tape or a fine line with pictures around the external circumference of a superconducting wire and bundling and twisting a large number of wound wires to constitute a cable and putting this cable in a tube of stainless steel, etc., and then, heat-treating the tube to form an intermetallic compound superconductor. CONSTITUTION:A fine line 2 or a tape 21 is wound with appropriate pitches lp around the external circumference of a superconducting wire 1 made up of a material constituting Nb3Sn. The superconducting wires around which a fine line or a tape is wound are bundled in an appropriate number and twisted together. The cable is put in a tube made of stainless steel, etc., and then, molded in a prescribed dimension, and then, made into a cable-in-conduit type superconducting conductor through heat-treatment for formation of Nb3Sn, etc. The section between wires is electrically connected through the fine line or the tape by winding it with appropriate pitches around the external circumference of the superconducting wire as above. Thereby, the resistance between the wires increases with the result that AC loss due to a fluctuating magnetic field can be reduced, too.
    • 10. 发明专利
    • PLASMA ACCELERATOR
    • JPS64284A
    • 1989-01-05
    • JP14647587
    • 1987-06-12
    • TOSHIBA CORP
    • FUJIWARA NAOYOSHIHAMASHIMA KOTARONINOMIYA MASAHARUYOSHIDA MASAO
    • C23F4/00
    • PURPOSE:To widen the control range of a plasma speed by adopting the control by Lorentz force and the control by ion energy using high frequencies to accelerate the plasma. CONSTITUTION:A DC voltage is impressed between a pair of accelerating electrodes 1a and 1b by an accelerating power supply 2. A high-frequency power supply 7 is connected to a wafer base 5 which supports a wafer to serve as a target and a high-frequency voltage is impressed between the wafer base 5 and the electrodes 1a, 1b. The plasma 8 flows between the electrodes 1a and 1b and is accelerated toward the wafer base 5. Current (j) flows between the electrodes 1a and 1b and the magnetic field generated by a magnetic field generating means is generated at a specific angle to the current (j) as shown by an arrow B. The Lorentz force F, therefore, acts toward the wafer base 5. The size thereof is determined by jXB. The acceleration of the plasma 8 is executed by controlling the voltage of the accelerating power supply 2.