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JP2004335160A - Current leads for superconducting devices - Google Patents

Current leads for superconducting devices Download PDF

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Publication number
JP2004335160A
JP2004335160A JP2003126134A JP2003126134A JP2004335160A JP 2004335160 A JP2004335160 A JP 2004335160A JP 2003126134 A JP2003126134 A JP 2003126134A JP 2003126134 A JP2003126134 A JP 2003126134A JP 2004335160 A JP2004335160 A JP 2004335160A
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superconducting
current
current lead
temperature side
lead
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JP4599807B2 (en
Inventor
Takaaki Bono
敬昭 坊野
Akira Tomioka
章 富岡
Yasutaka Sanuki
育孝 讃岐
Masayuki Konno
雅行 今野
Hidemi Hayashi
秀美 林
Kanichi Terazono
完一 寺薗
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Fuji Electric Co Ltd
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Fuji Electric Systems Co Ltd
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    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
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    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

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Abstract

<P>PROBLEM TO BE SOLVED: To obtain a stably operable current lead in which degradation of conductive capacity and local heating can be evaded even if it is installed in the vicinity of a superconductive coil. <P>SOLUTION: In the current lead 1 consisting of a room-temperature side lead 7 using a conductive metal material and a low-temperature side lead 8 using a parallel connection body of a plurality of unit conductors 4 made of tape-shaped oxide superconductive wires, the plurality of unit conductors 4 are buried in grooves of a support member 5 with their wide faces directed in the same direction to make up a low-temperature side current path, and the unit conductors 4 are arranged so as to receive a generated magnetic field of the superconductive coil 2 in parallel with the wide faces and are to be connected to the superconductive coil 2. <P>COPYRIGHT: (C)2005,JPO&NCIPI

Description

【0001】
【発明の属する技術分野】
本発明は、超電導エネルギー貯蔵用超電導コイルや超電導限流器、超電導ケーブル、超電導発電機、超電導変圧器などの超電導装置において、室温にある電源から極低温に冷却された超電導機器へと電力を供給する電流リードに関する。
【0002】
【従来の技術】
超電導コイルは、物性研究用装置や磁気共鳴装置などに利用されており、磁気浮上列車や核融合用磁気閉じ込め装置等にも応用されつつある。しかしながら、超電導コイルは極低温中に置かれて使用され、室温に置かれた電源より電力を供給して運転されるので、電力を供給する電流リードを介して極低温域に侵入する熱を抑えることが重要課題となっている。すなわち、冷媒としてしばしば用いられる液体ヘリウムは、1リットルの値段が約1000円にもなる高価な液体であり、また、1Wの侵入熱により蒸発した液体ヘリウムを冷凍機により再液化するために必要な冷凍機入力は、理想的な条件においても約400W、実際には約1000Wに達する。したがって、電流リードを介しての侵入熱が多いと、液体ヘリウムの購入等に伴うコストが上昇するばかりでなく、再液化に用いる冷凍機が大型化、大容量化するので、超電導装置の利点である小型化、少電力化を実現させるには、電流リードの低熱侵入化が重要課題となる。
【0003】
このため、各種の超電導装置の開発に際し、その実用化の可能性を左右するものとして低熱侵入の電流リードの開発が進められ、いわゆる高温超電導材料の発見に伴い、これを低温側の電流経路に用いた高温超電導電流リードが開発されてきている。
図2は、従来の高温超電導電流リードを用いた超電導磁石装置の縦断面図である。極低温容器3の内部に超電導コイル2が収納され、図示しない液体ヘリウム等の冷媒により冷却されている。超電導コイル2には室温部に配された図示しない電源より電力を供給するための一対の電流リード1が組込まれている。この電流リード1は、いわゆる高温超電導電流リードで、良導電性金属材料を電流経路とする室温側リード7と高温超電導材料を電流経路とする低温側リード8との直列接続体により構成されている。図3は、図2に組み込まれた電流リード1のY−Y断面図、すなわち高温超電導材料を電流経路とする低温側リード8の断面図である(例えば、特許文献1、あるいは特許文献2を参照)。図3に見られるように、低温側リード8は、銀シース型のテープ状高温超電導線材からなる複数本のユニット導体4Aを円筒状の支持部材6の表面に幅広面が円筒座標系の周方向と平行になるように配置して構成されている。ユニット導体4Aとして用いられているテープ状高温超電導線材の臨界電流値は磁界の影響を受け、特に幅広面に垂直方向の磁界を受けると臨界電流値が著しく低下する。このため、上記のごとくユニット導体4Aを配列することによって、電流リード1で生じる自己磁界の方向と幅広面とを平行にし、垂直方向の磁界成分を少なくして臨界電流値の低下を抑えている。なお、室温側リード7には、良導電性金属材料である銅線を複数本束ねて構成した銅製リードがしばしば用いられる。
【0004】
【特許文献1】
特開平10−188691号公報
【特許文献2】
特開平11−260162号公報
【0005】
【発明が解決しようとする課題】
上記のように従来の高温超電導電流リードでは、円筒状の支持部材の表面に複数のテープ状高温超電導線材を幅広面が円筒座標系の周方向と平行になるように配置して低温側リードを構成し、自己磁界による臨界電流値の低下を抑えている。しかしながら、このように構成した高温超電導電流リードにおいても、例えば図2に示したごとく超電導コイル2に接続して用いれば、超電導コイル2の発生する磁界の影響を受けて不具合が生じる危険性がある。すなわち、図2に示したごとき超電導コイル2においては、コイルの内側に、例えば図中の上方向への磁界が生じ、コイルの外側にその逆方向、例えば図中の下方向への磁界が生じ、コイルの巻線の上端、下端には径方向の磁界が生じる。したがって、図2に示されたごとく配置された電流リード1の低温側リード8には、図3に矢印付き細線で示したごとき超電導コイル2からの磁界が加わることとなる。このため、図3中にAで示した領域の近傍(領域A)に配されたユニット導体4Aのテープ状高温超電導線材は、超電導コイル2からの磁界を幅広面に平行に受け、図3中にBで示した領域の近傍(領域B)に配されたユニット導体4Aのテープ状高温超電導線材は、超電導コイル2からの磁界を垂直に受けることとなる。既に述べたように、テープ状高温超電導線材においては、幅広面に垂直方向の磁界を受けると臨界電流値が著しく低下するので、領域Aのユニット導体4Aは超電導コイル2からの磁界の影響を受けないが、領域Bのユニット導体4Aは超電導コイル2からの磁界により臨界電流値が著しく低下する。このため、領域Aのユニット導体4Aには電流が多く流れ、領域Bのユニット導体4Aにはあまり流れないという偏流が生じることとなる。このように偏流が生じると、電流リードとしての通電容量が低下するばかりでなく、室温側リード7との接続部の接続抵抗による発熱にバラツキが生じ、局部的な加熱を引起す危険性がある。
【0006】
本発明は、上記のごとき従来技術の問題点を考慮してなされたもので、テープ状高温超電導線材からなる複数のユニット導体を用いて構成される低温側リードが超電導コイルの近傍に設置されるものにおいても、複数のユニット導体間の偏流の発生が防止され、かつ通電容量の低下や接続抵抗による局部的加熱が回避され、安定して運転できる超電導装置用電流リードを提供することにある。
【0007】
【課題を解決するための手段】
上記の目的を達成するために、本発明においては、
極低温に冷却された超電導機器に室温にある電源より電力を供給する超電導装置用電流リードで、室温側電流経路と低温側電流経路との直列接続体よりなり、室温側電流経路が良導電性金属材料により構成され、低温側電流経路がテープ状酸化物超電導線よりなる複数本のユニット導体の並列接続体により構成された超電導装置用電流リードにおいて、
(1)上記の複数本のユニット導体のテープ状酸化物超電導線を、幅広面を同一方向に向けて配置することとし、
(2)超電導コイルに電力を供給する超電導装置用電流リードにおいては、複数本のユニット導体のテープ状酸化物超電導線が、その幅広面を超電導コイルの半径方向に略一致するように配置して組込むこととする。
【0008】
(3)また、上記の(1)、(2)において、低温側電流経路を構成する複数本のユニット導体を、低熱伝導性金属材料よりなる支持部材に設けられた溝中に埋設することとし、さらに、
(4)ユニット導体を、外表面に金属薄膜を形成した支持部材の溝中に、金属薄膜を介してはんだ付け接続することとする。
上記(1)のごとく電流リードを構成すれば、ユニット導体のテープ状酸化物超電導線の幅広面が超電導機器の発生磁界に平行となるように配して組込むことによって、超電導機器の発生磁界によるテープ状酸化物超電導線の臨界電流の低下が抑えられ、ユニット導体間の偏流を生じることなく、各ユニット導体に均等に電流が流れることとなる。例えば、超電導コイルに電力を供給する超電導装置用電流リードにおいては、上記の(2)のごとく配置して組込むことにより、テープ状酸化物超電導線の臨界電流の低下が抑えられ、偏流を生じることなく各ユニット導体に均等に電流が流れることとなる。
【0009】
また、上記の(3)のごとくユニット導体を支持部材の溝中に埋設すれば、磁界との相互作用により働く電磁力が安定に支持されるとともに、万が一何らかの要因によりテープ状酸化物超電導線がクエンチ(常伝導遷移)を生じても、電流が支持部材にバイパスして通流するので破損が回避される。なお、支持部材は低熱伝導性金属材料によって形成されているので、本支持部材を介しての侵入熱は微量に抑えられる。特に、上記の(4)のごとくとすれば、支持部材がはんだ付けの困難なステンレスやチタン等の金属材料で形成されている場合においても、ユニット導体と支持部材とを電気的にも、また機械的にも強力に接合することができるので、電磁力の支持とクエンチ時の電流バイパスが安定して行われる。
【0010】
【発明の実施の形態】
以下、本発明の実施の形態を例を挙げて詳しく説明する。なお、本発明は、この実施例に制限されるものではなく、同一の基本理念に基づく構成に広く適用される。
図1は、本発明の実施例の構成図で、(a)は、本発明の超電導装置用電流リードを組込んだ超電導磁石装置の縦断面図、(b)は、(a)に示された超電導装置用電流リードの低温側電流経路のX−X面の断面図である。図1(a)に見られるように、本超電導磁石装置においては、極低温容器3の内部に超電導コイル2が収納され、その超電導コイル2へ図示しない電源から電力を供給する電流リード1が組込まれている。電流リード1は、電流経路が良導電性金属材料により構成された室温側リード7と、電流経路がテープ状酸化物超電導線よりなるユニット導体4で構成された低温側リード8との直列接続体として構成されている。このうち、低温側リード8は、図1(b)に見られるように、複数本の銀シース型のテープ状酸化物超電導線からなるユニット導体4をステンレス材料よりなる支持部材5の溝中に埋設し、はんだ付け接続して構成されており、本構成の低温側リード8の特徴は、複数のユニット導体4が幅広面を同一方向に向けて配列されていることにある。また、図1(a)に示した超電導磁石装置の特徴は、上記の電流リード1が、低温側リード8のユニット導体4の幅広面を超電導コイル2の半径方向とほぼ一致するように配置して組込まれていることにある。
【0011】
したがって、本装置では、電流リード1の低温側リード8が超電導コイル2に近接して配置されているが、超電導コイル2の発生する磁界の方向は低温側リード8のユニット導体4の幅広面と平行な方向になるため、ユニット導体4のテープ状酸化物超電導線の臨界電流の低下は微小に抑えられる。また、複数のユニット導体4に加わる磁界の強さはほぼ同一となるので、各ユニット導体4にほぼ均等に電流が流れ、偏流を生じる恐れはない。したがって、従来の電流リードに見られたような、外部磁界による低温側リードのユニット導体間の通電電流の偏流に起因する通電容量の低下や局部的加熱を生じることなく、安定して使用することができる。
【0012】
なお、上記の低温側リード8のユニット導体4が埋設されている支持部材5は、電磁力等のユニット導体4に加わる力を支持する役割を果す。したがって、剛性の高いステンレス材料により構成すれば効果的に支持され、特に図1(b)に示したごとく溝中にユニット導体4を埋設すれば、より効果的に支持される。また、ステンレス材料は低熱伝導性の材料であるため、支持部材を介しての侵入熱を微小に抑えることができる。
また、支持部材5は、何らかの要因でユニット導体4のテープ状酸化物超電導線がクエンチを生じた際には、安全を確保するために電流をバイパスして流す役割を持つ。このため、本実施例の構成では、銀シース型のテープ状酸化物超電導線からなるユニット導体4と支持部材5とをはんだ付け接続して電気的にも良好に接着している。なお、このステンレス材料やチタン等の金属材料のように直接はんだ付けをすることが困難な材料からなる支持部材5を用いる場合には、あらかじめその接着面に銅や銅合金の薄膜を形成し、その薄膜面とユニット導体4とをはんだ付けして構成することによって、強固な接着が得られる。
【0013】
【発明の効果】
以上述べたように、本発明によれば、
極低温に冷却された超電導機器に室温にある電源より電力を供給する超電導装置用電流リードを、
(1)請求項1に記載のごとく構成することとしたので、低温側リードを構成するユニット導体のテープ状酸化物超電導線の幅広面が超電導機器の発生磁界に平行となるように配して組込むことによって、超電導機器の発生磁界によるテープ状酸化物超電導線の臨界電流の低下が抑えられることとなったので、複数のユニット導体間の偏流の発生が防止され、かつ通電容量の低下や接続抵抗による局部的加熱が回避され、安定して運転できる超電導装置用電流リードが得られることとなった。
【0014】
(2)また、請求項2のごとく構成すれば、超電導コイルを用いる超電導機器用として特に好適な超電導装置用電流リードが得られる。
(3)また、請求項3のごとく構成すれば、低温側リードを構成するユニット導体に加わる電磁力が安定に支持されるとともに、万が一何らかの要因によりテープ状酸化物超電導線がクエンチを生じても、電流が支持部材にバイパスして破損が回避されるので、通電容量の低下や接続抵抗による局部的加熱が回避され、安定して運転できる超電導装置用電流リードとして好適である。
(4)また、請求項4のごとく構成すれば、ユニット導体と支持部材とが電気的、機械的にも強力に接合され、電磁力の支持とクエンチ時の電流バイパスが安定して行われるので、通電容量の低下や接続抵抗による局部的加熱が回避され、安定して運転できる超電導装置用電流リードとしてより好適である。
【図面の簡単な説明】
【図1】(a)は、本発明の超電導装置用電流リードを組込んだ超電導磁石装置の縦断面図、(b)は、(a)に示された超電導装置用電流リードの低温側電流経路のX−X面の断面図
【図2】従来の高温超電導電流リードを用いた超電導磁石装置の縦断面図
【図3】図2に組み込まれた電流リードのY−Y断面での断面図
【符号の説明】
1 電流リード
2 超電導コイル
3 極低温容器
4 ユニット導体
5 支持部材
7 室温側リード
8 低温側リード
[0001]
TECHNICAL FIELD OF THE INVENTION
The present invention provides a superconducting coil for storing superconducting energy, a superconducting current limiter, a superconducting cable, a superconducting generator, a superconducting transformer, and the like, in which power is supplied from a room temperature power supply to a cryogenically cooled superconducting device. Current lead.
[0002]
[Prior art]
Superconducting coils are used in physical property research equipment, magnetic resonance equipment, and the like, and are also being applied to magnetic levitation trains, magnetic confinement equipment for nuclear fusion, and the like. However, since the superconducting coil is used in a cryogenic temperature and is operated by supplying power from a power source placed at room temperature, heat entering the cryogenic region through a current lead for supplying power is suppressed. Is an important issue. That is, liquid helium, which is often used as a refrigerant, is an expensive liquid for which the price of one liter is as high as about 1,000 yen, and is necessary for re-liquefying liquid helium evaporated by the invasion heat of 1 W by a refrigerator. The refrigerator input reaches about 400 W even under ideal conditions, and actually reaches about 1000 W. Therefore, if there is a large amount of heat penetrating through the current lead, not only does the cost associated with the purchase of liquid helium, etc. rise, but also the refrigerator used for reliquefaction becomes large-sized and large-capacity. In order to realize certain miniaturization and low power consumption, it is important to reduce the heat penetration of the current leads.
[0003]
For this reason, in the development of various superconducting devices, the development of current leads with low heat penetration has been promoted as a factor in determining the possibility of their practical application.With the discovery of a so-called high-temperature superconducting material, this was transferred to the current path on the low-temperature side. High temperature superconducting current leads used have been developed.
FIG. 2 is a longitudinal sectional view of a conventional superconducting magnet device using a high-temperature superconducting current lead. The superconducting coil 2 is housed inside the cryogenic vessel 3 and is cooled by a coolant such as liquid helium (not shown). The superconducting coil 2 incorporates a pair of current leads 1 for supplying power from a power source (not shown) disposed at a room temperature portion. The current lead 1 is a so-called high-temperature superconducting current lead, and is formed by a series connection of a room-temperature-side lead 7 using a good conductive metal material as a current path and a low-temperature side lead 8 using a high-temperature superconducting material as a current path. . FIG. 3 is a sectional view taken along line YY of the current lead 1 incorporated in FIG. 2, that is, a sectional view of a low-temperature side lead 8 using a high-temperature superconducting material as a current path (for example, see Patent Document 1 or Patent Document 2). reference). As shown in FIG. 3, the low-temperature side lead 8 is composed of a plurality of unit conductors 4A made of a silver-sheathed tape-shaped high-temperature superconducting wire, and a wide surface formed on the surface of a cylindrical support member 6 in a circumferential direction of a cylindrical coordinate system. It is arranged so as to be in parallel with. The critical current value of the tape-shaped high-temperature superconducting wire used as the unit conductor 4A is affected by a magnetic field. Particularly, when a magnetic field is applied in a direction perpendicular to a wide surface, the critical current value is significantly reduced. For this reason, by arranging the unit conductors 4A as described above, the direction of the self-magnetic field generated in the current lead 1 is made parallel to the wide surface, and the magnetic field component in the vertical direction is reduced to suppress a decrease in the critical current value. . Note that a copper lead formed by bundling a plurality of copper wires made of a good conductive metal material is often used as the room temperature side lead 7.
[0004]
[Patent Document 1]
Japanese Patent Laid-Open No. Hei 10-188691 [Patent Document 2]
JP-A-11-260162
[Problems to be solved by the invention]
As described above, in the conventional high-temperature superconducting current lead, a plurality of tape-shaped high-temperature superconducting wires are arranged on the surface of the cylindrical support member such that the wide surface is parallel to the circumferential direction of the cylindrical coordinate system, and the low-temperature side lead is disposed. With this configuration, a decrease in the critical current value due to the self-magnetic field is suppressed. However, even in the high-temperature superconducting current lead configured as described above, if it is used by being connected to the superconducting coil 2 as shown in FIG. 2, for example, there is a risk that a malfunction may occur due to the influence of the magnetic field generated by the superconducting coil 2. . That is, in the superconducting coil 2 as shown in FIG. 2, a magnetic field is generated inside the coil, for example, in the upward direction in the figure, and a magnetic field in the opposite direction, for example, downward in the figure, is generated outside the coil. A radial magnetic field is generated at the upper and lower ends of the coil winding. Accordingly, a magnetic field from the superconducting coil 2 as shown by a thin line with an arrow in FIG. 3 is applied to the low-temperature side lead 8 of the current lead 1 arranged as shown in FIG. For this reason, the tape-shaped high-temperature superconducting wire of the unit conductor 4A arranged in the vicinity (region A) of the region indicated by A in FIG. 3 receives the magnetic field from the superconducting coil 2 in parallel to the wide surface, and 2B, the tape-shaped high-temperature superconducting wire of the unit conductor 4A disposed in the vicinity (region B) of the unit conductor receives the magnetic field from the superconducting coil 2 vertically. As described above, in a tape-shaped high-temperature superconducting wire, when a magnetic field is applied in a direction perpendicular to the wide surface, the critical current value is significantly reduced. Therefore, the unit conductor 4A in the region A is affected by the magnetic field from the superconducting coil 2. However, the critical current value of the unit conductor 4A in the region B is significantly reduced due to the magnetic field from the superconducting coil 2. For this reason, a large current flows through the unit conductor 4A in the region A, and a small current flows through the unit conductor 4A in the region B. If such a drift occurs, not only does the current carrying capacity of the current lead decrease, but also the heat generated by the connection resistance of the connection with the room-temperature-side lead 7 varies, which may cause local heating. .
[0006]
The present invention has been made in consideration of the problems of the related art as described above, and a low-temperature side lead configured using a plurality of unit conductors made of a tape-like high-temperature superconducting wire is installed near a superconducting coil. Also, it is an object of the present invention to provide a current lead for a superconducting device that can stably operate by preventing the occurrence of a drift between a plurality of unit conductors, avoiding a decrease in current carrying capacity and avoiding local heating due to connection resistance.
[0007]
[Means for Solving the Problems]
In order to achieve the above object, in the present invention,
A current lead for a superconducting device that supplies power from a power supply at room temperature to a superconducting device cooled to cryogenic temperature. It consists of a series connection of a room temperature side current path and a low temperature side current path. In a current lead for a superconducting device, which is constituted by a metal material, and a low-temperature side current path is constituted by a parallel connection body of a plurality of unit conductors formed of a tape-shaped oxide superconducting wire,
(1) The tape-shaped oxide superconducting wires of the plurality of unit conductors are arranged with their wide surfaces facing in the same direction,
(2) In a current lead for a superconducting device for supplying power to a superconducting coil, a tape-shaped oxide superconducting wire of a plurality of unit conductors is arranged such that a wide surface thereof substantially coincides with a radial direction of the superconducting coil. It shall be incorporated.
[0008]
(3) In the above (1) and (2), a plurality of unit conductors constituting a low-temperature side current path are embedded in a groove provided in a support member made of a low heat conductive metal material. ,further,
(4) The unit conductor is connected to the groove of the support member having the metal thin film formed on the outer surface by soldering via the metal thin film.
If the current lead is configured as in the above (1), the wide surface of the tape-shaped oxide superconducting wire of the unit conductor is arranged and incorporated so as to be parallel to the magnetic field generated by the superconducting device, so that the magnetic field generated by the superconducting device is reduced. The reduction in the critical current of the tape-shaped oxide superconducting wire is suppressed, and the current flows evenly through each unit conductor without causing drift between the unit conductors. For example, in a current lead for a superconducting device that supplies power to a superconducting coil, by arranging and incorporating as described in (2) above, a decrease in the critical current of the tape-shaped oxide superconducting wire is suppressed, and a drift occurs. Therefore, current flows evenly through each unit conductor.
[0009]
If the unit conductor is buried in the groove of the support member as described in (3) above, the electromagnetic force acting due to the interaction with the magnetic field is stably supported, and the tape-shaped oxide superconducting wire is inadvertently generated by some factor. Even if a quench (normal conduction transition) occurs, the current is bypassed to the support member to avoid damage. Since the support member is made of a low thermal conductive metal material, the amount of heat penetrating through the support member can be suppressed to a small amount. In particular, according to the above (4), even when the support member is formed of a metal material such as stainless steel or titanium which is difficult to be soldered, the unit conductor and the support member can be electrically connected to each other. Since mechanically strong bonding can be performed, the electromagnetic force is supported and the current bypass at the time of quench is performed stably.
[0010]
BEST MODE FOR CARRYING OUT THE INVENTION
Hereinafter, embodiments of the present invention will be described in detail with reference to examples. The present invention is not limited to this embodiment, but is widely applied to configurations based on the same basic philosophy.
1A and 1B are configuration diagrams of an embodiment of the present invention, in which FIG. 1A is a longitudinal sectional view of a superconducting magnet device incorporating a current lead for a superconducting device of the present invention, and FIG. It is sectional drawing of the XX plane of the low-temperature side current path of the current lead for superconducting devices which was used. As shown in FIG. 1A, in the present superconducting magnet device, a superconducting coil 2 is housed inside a cryogenic vessel 3, and a current lead 1 for supplying power to the superconducting coil 2 from a power source (not shown) is incorporated. Have been. The current lead 1 is a series connection of a room-temperature-side lead 7 whose current path is made of a good conductive metal material and a low-temperature side lead 8 whose current path is made of a unit conductor 4 made of a tape-shaped oxide superconducting wire. It is configured as Among them, the low-temperature side lead 8 has a unit conductor 4 composed of a plurality of silver-sheathed tape-shaped oxide superconducting wires in a groove of a support member 5 made of a stainless material, as shown in FIG. The low-temperature side lead 8 of this configuration is buried and connected by soldering. A feature of the low-temperature side lead 8 is that a plurality of unit conductors 4 are arranged with their wide surfaces facing in the same direction. The superconducting magnet device shown in FIG. 1A is characterized in that the current lead 1 is arranged such that the wide surface of the unit conductor 4 of the low-temperature side lead 8 substantially matches the radial direction of the superconducting coil 2. It is built in.
[0011]
Therefore, in the present device, the low-temperature side lead 8 of the current lead 1 is arranged close to the superconducting coil 2, but the direction of the magnetic field generated by the superconducting coil 2 is different from the wide surface of the unit conductor 4 of the low-temperature side lead 8. Since the directions are parallel to each other, a decrease in the critical current of the tape-shaped oxide superconducting wire of the unit conductor 4 can be suppressed to a small extent. Further, since the strengths of the magnetic fields applied to the plurality of unit conductors 4 are substantially the same, current flows almost uniformly in each unit conductor 4 and there is no possibility that a drift occurs. Therefore, it must be used stably without causing a decrease in current carrying capacity or local heating caused by the current flowing between the unit conductors of the low-temperature side lead due to an external magnetic field, as seen in conventional current leads. Can be.
[0012]
The support member 5 in which the unit conductor 4 of the low-temperature side lead 8 is embedded serves to support a force applied to the unit conductor 4 such as an electromagnetic force. Therefore, when the unit conductor 4 is made of a highly rigid stainless steel material, it is effectively supported. In particular, when the unit conductor 4 is embedded in the groove as shown in FIG. In addition, since the stainless steel material is a material having low thermal conductivity, heat entering through the support member can be suppressed to a very small level.
When the tape-shaped oxide superconducting wire of the unit conductor 4 is quenched for some reason, the support member 5 has a role of bypassing an electric current to ensure safety. For this reason, in the configuration of the present embodiment, the unit conductor 4 composed of a silver-sheathed tape-shaped oxide superconducting wire and the supporting member 5 are connected by soldering and are electrically well bonded. When using a support member 5 made of a material that is difficult to directly solder, such as a stainless steel material or a metal material such as titanium, a thin film of copper or a copper alloy is formed on the bonding surface in advance, By forming the thin film surface and the unit conductor 4 by soldering, strong adhesion can be obtained.
[0013]
【The invention's effect】
As described above, according to the present invention,
A current lead for a superconducting device that supplies power from a power supply at room temperature to a superconducting device cooled to cryogenic temperature,
(1) Since it is configured as described in claim 1, the wide surface of the tape-shaped oxide superconducting wire of the unit conductor constituting the low-temperature side lead is arranged so as to be parallel to the magnetic field generated by the superconducting device. By incorporating, the reduction of the critical current of the tape-shaped oxide superconducting wire due to the magnetic field generated by the superconducting device is suppressed, so that the occurrence of drift between the plurality of unit conductors is prevented, and the reduction of the current carrying capacity and connection Local heating due to resistance is avoided, and a current lead for a superconducting device that can operate stably can be obtained.
[0014]
(2) According to the second aspect, a current lead for a superconducting device particularly suitable for a superconducting device using a superconducting coil can be obtained.
(3) Further, according to the present invention, the electromagnetic force applied to the unit conductor constituting the low-temperature side lead is stably supported, and even if the tape-shaped oxide superconducting wire is quenched by some factor. In addition, since the current is bypassed to the support member to avoid breakage, local heating due to a reduction in current carrying capacity and connection resistance is avoided, and the current lead is suitable for a superconducting device that can operate stably.
(4) Further, according to the present invention, the unit conductor and the support member are strongly joined electrically and mechanically, and the support of the electromagnetic force and the current bypass at the time of quench are performed stably. In addition, the present invention is more suitable as a current lead for a superconducting device that can be operated stably while avoiding a decrease in current-carrying capacity and local heating due to connection resistance.
[Brief description of the drawings]
1A is a longitudinal sectional view of a superconducting magnet device incorporating a current lead for a superconducting device of the present invention, and FIG. 1B is a low-temperature side current of the current lead for a superconducting device shown in FIG. FIG. 2 is a longitudinal sectional view of a superconducting magnet device using a conventional high-temperature superconducting current lead. FIG. 3 is a sectional view of a current lead incorporated in FIG. [Explanation of symbols]
DESCRIPTION OF SYMBOLS 1 Current lead 2 Superconducting coil 3 Cryogenic container 4 Unit conductor 5 Support member 7 Room temperature side lead 8 Low temperature side lead

Claims (4)

極低温に冷却された超電導機器に室温にある電源より電力を供給する超電導装置用電流リードで、室温側電流経路と低温側電流経路との直列接続体よりなり、室温側電流経路が良導電性金属材料により構成され、低温側電流経路がテープ状酸化物超電導線よりなる複数本のユニット導体の並列接続体により構成された超電導装置用電流リードにおいて、
複数本のユニット導体のテープ状酸化物超電導線が幅広面を同一方向に向けて配置されていることを特徴とする超電導装置用電流リード。
A current lead for a superconducting device that supplies power from a power supply at room temperature to a superconducting device cooled to cryogenic temperature. It consists of a series connection of a room temperature side current path and a low temperature side current path. In a current lead for a superconducting device, which is constituted by a metal material, and a low-temperature side current path is constituted by a parallel connection body of a plurality of unit conductors formed of a tape-shaped oxide superconducting wire,
A current lead for a superconducting device, wherein a plurality of tape-shaped oxide superconducting wires of unit conductors are arranged with their wide faces facing in the same direction.
超電導コイルに電力を供給する超電導装置用電流リードで、複数本のユニット導体のテープ状酸化物超電導線が、その幅広面を前記ソレノイド型超電導コイルの半径方向に略一致するように配置して組込まれていることを特徴とする請求項1に記載の超電導装置用電流リード。A superconducting device current lead for supplying power to the superconducting coil, in which tape-shaped oxide superconducting wires of a plurality of unit conductors are arranged and arranged such that the wide surface thereof substantially coincides with the radial direction of the solenoid type superconducting coil. The current lead for a superconducting device according to claim 1, wherein the current lead is provided. 低温側電流経路を構成する複数本のユニット導体が、低熱伝導性金属材料よりなる支持部材に設けられた溝中に埋設されていることを特徴とする請求項1または2に記載の超電導装置用電流リード。3. The superconducting device according to claim 1, wherein a plurality of unit conductors constituting a low-temperature side current path are buried in a groove provided in a support member made of a low thermal conductive metal material. Current lead. 前記ユニット導体が、外表面に金属薄膜を形成した支持部材の溝中に、金属薄膜を介してはんだ付け接続されていることを特徴とする請求項3に記載の超電導装置用電流リード。The current lead for a superconducting device according to claim 3, wherein the unit conductor is soldered and connected via a metal thin film in a groove of a support member having a metal thin film formed on an outer surface.
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JP2008251564A (en) * 2007-03-29 2008-10-16 Kyushu Univ High temperature superconducting current leads and methods for increasing critical current density
JP2009212028A (en) * 2008-03-06 2009-09-17 Fuji Electric Systems Co Ltd Superconducting current lead
JP2009211899A (en) * 2008-03-04 2009-09-17 Fuji Electric Systems Co Ltd Superconductive current lead and method of manufacturing the same
JP2009230913A (en) * 2008-03-19 2009-10-08 Swcc Showa Cable Systems Co Ltd Oxide superconductive current lead
JP2009259520A (en) * 2008-04-15 2009-11-05 Fuji Electric Systems Co Ltd Superconductive current lead
JP2012028041A (en) * 2010-07-20 2012-02-09 Sumitomo Heavy Ind Ltd Superconducting current lead
JP2012064323A (en) * 2010-09-14 2012-03-29 Swcc Showa Cable Systems Co Ltd Superconductive current lead
JP2013187405A (en) * 2012-03-08 2013-09-19 Toshiba Corp Connection conductor of superconductive magnet apparatus and superconductive magnet apparatus

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JP2008251564A (en) * 2007-03-29 2008-10-16 Kyushu Univ High temperature superconducting current leads and methods for increasing critical current density
JP2009211899A (en) * 2008-03-04 2009-09-17 Fuji Electric Systems Co Ltd Superconductive current lead and method of manufacturing the same
JP2009212028A (en) * 2008-03-06 2009-09-17 Fuji Electric Systems Co Ltd Superconducting current lead
JP2009230913A (en) * 2008-03-19 2009-10-08 Swcc Showa Cable Systems Co Ltd Oxide superconductive current lead
JP2009259520A (en) * 2008-04-15 2009-11-05 Fuji Electric Systems Co Ltd Superconductive current lead
JP2012028041A (en) * 2010-07-20 2012-02-09 Sumitomo Heavy Ind Ltd Superconducting current lead
JP2012064323A (en) * 2010-09-14 2012-03-29 Swcc Showa Cable Systems Co Ltd Superconductive current lead
JP2013187405A (en) * 2012-03-08 2013-09-19 Toshiba Corp Connection conductor of superconductive magnet apparatus and superconductive magnet apparatus

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