JPS637663B2 - - Google Patents

Info

Publication number
JPS637663B2
JPS637663B2 JP56117676A JP11767681A JPS637663B2 JP S637663 B2 JPS637663 B2 JP S637663B2 JP 56117676 A JP56117676 A JP 56117676A JP 11767681 A JP11767681 A JP 11767681A JP S637663 B2 JPS637663 B2 JP S637663B2
Authority
JP
Japan
Prior art keywords
superconducting
strands
adjacent
superconductor
abutting portions
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired
Application number
JP56117676A
Other languages
Japanese (ja)
Other versions
JPS5819812A (en
Inventor
Susumu Shimamoto
Kyoshi Yoshida
Hiroshi Takada
Tomoaki Sato
Takeshi Yamagiwa
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Ltd
Original Assignee
Hitachi Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP56117676A priority Critical patent/JPS5819812A/en
Publication of JPS5819812A publication Critical patent/JPS5819812A/en
Publication of JPS637663B2 publication Critical patent/JPS637663B2/ja
Granted legal-status Critical Current

Links

Classifications

    • 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
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

Landscapes

  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【発明の詳細な説明】 本発明は超電導々体に係り、特に核融合装置等
の超電導コイルに採用される超電導々体に関す
る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a superconductor, and particularly to a superconductor employed in a superconducting coil of a nuclear fusion device or the like.

一般に核融合装置のトロイダル磁場コイル等、
大容量の超電導々体の構成は、極低温における超
電導状態において本来の通電を可能とする超電導
素線と、安定化材と呼ばれ、超電導素線の電磁力
及び極低温から常電導範囲の不安定な要素をこの
安定化材(通常は硬銅線でできている導体)に転
流し安定化する役目をはたす導体とから成り立つ
ている。
Generally, toroidal magnetic field coils of nuclear fusion devices, etc.
A large-capacity superconducting conductor consists of a superconducting wire that enables the original conduction of electricity in a superconducting state at cryogenic temperatures, and a stabilizing material, which is used to control the electromagnetic force of the superconducting wire and the resistance between the cryogenic and normal conductivity ranges. It consists of a conductor that serves to commutate and stabilize the stabilizing element to this stabilizing material (a conductor usually made of hard copper wire).

このような構成の超電導々体で大型の超電導コ
イルを製作する場合には、通常、超電導素線の長
さには製作上制限があるので巻線途中で接続しな
ければならない。
When manufacturing a large-sized superconducting coil using a superconducting conductor having such a configuration, the length of the superconducting strands is usually limited in terms of manufacturing, so the connection must be made midway through the winding.

従来、この超電導素線の接続としては、超電導
素線の側面同志を比較的長距離にわたつて重ね合
わせたり、あるいは超電導素線の接続端部同志を
ろう付等により接合して行なうものがあつた。し
かしながら、前者には超電導素線寸法が接続部で
大きくならざるを得ないし、十分な機械的強度も
得られない。また、後者には電気抵抗値が高くな
つてしまうという欠点があつた。特に超電導素線
の寸法が大きくなつてしまうことは、機器の構造
に制限を加えてしまい、また、電気抵抗値が高く
なるということはそのまま損失の増大につながつ
て冷却媒体(液体ヘリウム)消費量が増す故、機
器の運転コストの上昇を招くのみならず、超電導
の本旨である低損失という特徴すら失う嫌いがあ
る。
Conventionally, these superconducting wires have been connected by overlapping the sides of the superconducting wires over a relatively long distance, or by joining the connecting ends of the superconducting wires by brazing, etc. Ta. However, in the former case, the dimensions of the superconducting strands must be increased at the connection portion, and sufficient mechanical strength cannot be obtained. Furthermore, the latter had the disadvantage of high electrical resistance. In particular, increasing the dimensions of superconducting strands imposes restrictions on the structure of devices, and increasing electrical resistance directly leads to increased loss and consumption of cooling medium (liquid helium). This increases not only the operating cost of the equipment but also the loss of the low loss characteristic of superconductivity.

本発明は上述の点に鑑み成されたもので、その
目的とするところは、超電導素線の寸法を大きく
することなく、かつ、電気抵抗値を非常に小さく
することのできる超電導々体を提供するにある。
The present invention has been made in view of the above-mentioned points, and its purpose is to provide a superconductor that can reduce the electrical resistance value to a very small value without increasing the dimensions of the superconducting wire. There is something to do.

本発明は少なくとも1個所で突合わされてなる
超電導素線を複数重ね合わせてなる超電導々体に
おいて、相隣接する前記超電導素線の突合わせ部
を互いにずらし、相隣接する超電導素線同志の突
合わせ部間でラツピング部が形成されることによ
り所期の目的を達成するようになしたものであ
る。
The present invention provides a superconducting body formed by overlapping a plurality of superconducting strands that are butted at at least one place, by shifting the abutting portions of the adjacent superconducting strands from each other, and abutting the adjacent superconducting strands. The intended purpose is achieved by forming wrapping parts between the parts.

以下、図面の実施例に基づいて本発明を詳細に
説明する。
Hereinafter, the present invention will be explained in detail based on embodiments shown in the drawings.

第1図、第2図、及び第3図に本発明の超電導
導体1の一実施例を示す。
An embodiment of the superconducting conductor 1 of the present invention is shown in FIGS. 1, 2, and 3.

該図に示す如く、通常超電導々体1は、超電導
素線2の長さに製作上制限があるため、超電導素
線2の途中少なくとも1個所で分割されたものを
その分割部端部同志を突合わせ、突合わせ部3を
形成し、この超電導素線2を複数(実施例では5
本)重ね合わせて並列に並べ、その周囲を超電導
状態を安定させるための安定化材(通常は硬銅
線)4で覆つて構成している。そして、本実施例
では重ね合わせられた方向に相隣接する超電導素
線2の突合わせ部3を軸方向にずらし、しかも段
階的にずらすことにより、相隣接する超電導素線
2同志の突合わせ部3間でラツピング部から形成
されている(第1図参照)。また、並列に並んで
いる超電導素線2の突合わせ部3は同一位置とし
ている(第3図参照)。
As shown in the figure, since there is a manufacturing limit to the length of the superconducting wire 2 in the superconducting conductor 1, the superconducting wire 2 is usually split at at least one point in the middle, and the ends of the split portions are joined together. The butt portions 3 are formed, and a plurality of superconducting strands 2 (in the example, 5
They are stacked and arranged in parallel, and their surroundings are covered with a stabilizing material (usually hard copper wire) 4 to stabilize the superconducting state. In this embodiment, the abutting portions 3 of the superconducting strands 2 adjacent to each other in the overlapping direction are shifted in the axial direction, and the abutting portions 3 of the superconducting strands 2 that are adjacent to each other are shifted in stages. It is formed from a wrapping part between three parts (see Fig. 1). Furthermore, the butt portions 3 of the superconducting wires 2 arranged in parallel are located at the same position (see FIG. 3).

このような本実施例の構成とすることにより、
相隣接する超電導素線2の突合わせ部3をずらす
ことにより、各超電導素線2の相隣接する超電導
素線2同志の突合わせ部3間ではラツピング部が
形成されることになるため、電流の流れは第4図
に示す如く、各超電導素線2間のラツピング部を
通して行なわれることにより、非常に広い面積に
わたり電流の超電導素線2間の移動となり、電気
抵抗値は非常に小さくなつていることがわかる。
また、本実施例のようにすると、超電導素線2の
1本の突合わせ部3は重ね合わさつていないた
め、超電導素線の寸法が大きくなることはない
(このことは第1図において、超電導素線2の寸
法に変化のないことでもわかる)。尚、超電導素
線2の機械的強度は、安定化材3同志の接続部に
ろう付などを適用することで十分大きくできるこ
とは言うまでもない。
By having the configuration of this embodiment as described above,
By shifting the abutting portions 3 of phase-adjacent superconducting strands 2, a wrapping portion is formed between the abutting portions 3 of phase-adjacent superconducting strands 2 of each superconducting strand 2, so that the current As shown in Fig. 4, the current flows through the wrapping portion between each superconducting strand 2, so that the current moves between the superconducting strands 2 over a very wide area, and the electrical resistance value becomes very small. I know that there is.
Furthermore, in this embodiment, since the butt portions 3 of the superconducting wires 2 are not overlapped, the dimensions of the superconducting wires do not increase (this can be seen in FIG. 1). This can also be seen from the fact that there is no change in the dimensions of the superconducting wire 2). It goes without saying that the mechanical strength of the superconducting strands 2 can be sufficiently increased by applying brazing or the like to the joints between the stabilizing members 3.

第5図、及び第6図に本発明の他の実施例を示
す。
Other embodiments of the present invention are shown in FIGS. 5 and 6.

該図に示す実施例は、内部に冷却媒体流路5a
を有する安定化材5の周囲に超電導素線2を巻回
して超電導々体1を形成するものであるが、本実
施例でも相隣接する超電導素線2の突合わせ部3
をずらして巻回し、相隣接する超電導素線2同志
の突合わせ部3間でラツピング部を形成するよう
にしたものである。
The embodiment shown in the figure has a cooling medium flow path 5a inside.
The superconductor 1 is formed by winding the superconducting wires 2 around the stabilizing material 5 having
The superconducting strands 2 are wound in a staggered manner to form a wrapping portion between the abutting portions 3 of adjacent superconducting strands 2.

このような本実施例の構成であつても、その効
果は上述した実施例と全く同様である。
Even with this configuration of this embodiment, the effect is exactly the same as that of the embodiment described above.

以上説明した本発明の超電導々体によれば、少
なくとも1個所で突合わされてなる超電導素線を
複数重ね合わせてなる超電導々体において、相隣
接する前記超電導素線の突合わせ部を互いにずら
し、相隣接する超電導素線同志の突合わせ部間で
ラツピング部が形成されるようにしたものである
から、1本の超電導素線の接合部では重ね合うこ
とはないので、その寸法が大きくなることはな
く、相隣接している超電導素線間の突合わせ部に
形成されるラツピング部を介して電流が流れるこ
ととなり電気抵抗値も非常に小さくでき、此種超
電導導体に採用する場合には有効である。
According to the superconducting body of the present invention described above, in the superconducting body formed by stacking a plurality of superconducting strands abutted at at least one place, the abutting portions of the adjacent superconducting strands are shifted from each other, Since a wrapping part is formed between the abutting parts of adjacent superconducting strands, the joining parts of one superconducting strand will not overlap, so the size will not increase. Instead, current flows through the wrapping part formed at the butt part between adjacent superconducting strands, and the electrical resistance value can be extremely small, making it effective when used in this kind of superconducting conductor. be.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の超電導々体の一実施例を示す
断面図、第2図はその―断面図、第3図は第
2図の―断面図、第4図は本発明の超電導々
体における電流流通路を示す図、第5図は本発明
の他の実施例を示し第2図に相当する図、第6図
は第5図の正面図である。 1……超電導々体、2……超電導素線、3……
突合わせ部、4,5……安定化材。
FIG. 1 is a sectional view showing an embodiment of the superconductor of the present invention, FIG. 2 is a sectional view thereof, FIG. 3 is a sectional view of FIG. 2, and FIG. 4 is a sectional view of the superconductor of the present invention. FIG. 5 is a diagram showing another embodiment of the present invention and corresponds to FIG. 2, and FIG. 6 is a front view of FIG. 5. 1... superconducting conductor, 2... superconducting wire, 3...
Butt part, 4, 5... Stabilizing material.

Claims (1)

【特許請求の範囲】 1 少なくとも1個所で突合わされてなる超電導
素線を複数重ね合わせて成る超電導々体におい
て、相隣接する前記超電導素線の突合わせ部を互
いにずらし、相隣接する超電導素線同志の突合わ
せ部間でラツピング部を形成したことを特徴とす
る超電導々体。 2 前記超電導素線は複数重ね合わせた状態で、
その周囲を安定化材で囲まれていることを特徴と
する特許請求の範囲第1項記載の超電導々体。 3 内部に冷却媒体が通る冷却媒体流路を有する
安定化材の周囲に、前記超電導素線を巻回してな
ることを特徴とする特許請求の範囲第1項記載の
超電導々体。
[Scope of Claims] 1. In a superconductor formed by stacking a plurality of superconducting strands abutted at at least one place, the abutting portions of the adjacent superconducting strands are shifted from each other, and the adjacent superconducting strands are stacked together. A superconductor characterized in that a wrapping portion is formed between abutting portions of comrades. 2. The superconducting strands are in a state where they are stacked one on top of the other,
A superconducting conductor according to claim 1, wherein the superconducting conductor is surrounded by a stabilizing material. 3. The superconducting conductor according to claim 1, wherein the superconducting wire is wound around a stabilizing material having a cooling medium flow path through which a cooling medium passes.
JP56117676A 1981-07-29 1981-07-29 Superconductive conductor Granted JPS5819812A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56117676A JPS5819812A (en) 1981-07-29 1981-07-29 Superconductive conductor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56117676A JPS5819812A (en) 1981-07-29 1981-07-29 Superconductive conductor

Publications (2)

Publication Number Publication Date
JPS5819812A JPS5819812A (en) 1983-02-05
JPS637663B2 true JPS637663B2 (en) 1988-02-17

Family

ID=14717525

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56117676A Granted JPS5819812A (en) 1981-07-29 1981-07-29 Superconductive conductor

Country Status (1)

Country Link
JP (1) JPS5819812A (en)

Also Published As

Publication number Publication date
JPS5819812A (en) 1983-02-05

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