JPH05135944A - Superconducting apparatus - Google Patents

Superconducting apparatus

Info

Publication number
JPH05135944A
JPH05135944A JP29694891A JP29694891A JPH05135944A JP H05135944 A JPH05135944 A JP H05135944A JP 29694891 A JP29694891 A JP 29694891A JP 29694891 A JP29694891 A JP 29694891A JP H05135944 A JPH05135944 A JP H05135944A
Authority
JP
Japan
Prior art keywords
connection terminal
wire
current
superconducting
superconductor
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.)
Pending
Application number
JP29694891A
Other languages
Japanese (ja)
Inventor
Mamoru Shimada
守 嶋田
Masayuki Hoshino
昌幸 星野
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP29694891A priority Critical patent/JPH05135944A/en
Publication of JPH05135944A publication Critical patent/JPH05135944A/en
Pending legal-status Critical Current

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  • Superconductors And Manufacturing Methods Therefor (AREA)

Abstract

PURPOSE:To increase the current capacitance of the joint of a current lead connection terminal and a superconductor wire by comprising the connection terminal having a spiral zone and the superconductor wire which connects it so as to short-circuit the turn of the spiral zone. CONSTITUTION:An extremely fine multicore superconducting wire having several ten thousand superconductor filaments of a diameter of 1mum or less is used as a superconductor wire 1, and every filament is surrounded by CuNi of relatively high electric resistance. Every element wire is kept surfaced with a CuNi layer. This superconductor wire is a plural-order strand and is connected by twist back to the strand one level before in the connection terminal 6. The connection terminal 6 is wounded in a spiral form. This constitution makes current shunt gradually from the connection terminal 6 to the superconductor wire 1 by the effect of the inductance of the connection terminal's spiral zone. This can provide a superconducting apparatus having a joint of high current capacitance and low loss of heat generation and the like.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は超電導装置に係り、特に
超電導コイル等から引出された超電導線と電流供給リー
ド等を接続する構造に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a superconducting device, and more particularly to a structure for connecting a superconducting wire drawn from a superconducting coil or the like with a current supply lead.

【0002】[0002]

【従来の技術】極低温下にある超電導コイルには銅板な
どで構成された電流リードにより常温空間にある電源か
ら電流を供給する。つまり、図5に示すように超電導線
1と電流リード2との接続部を容器3内の極低温雰囲気
中、あるいは液体ヘリウム4などの冷媒の中に設ける。
このとき、接続部での発熱による超電導線の常電導状態
への転移(クエンチ)を防ぐため、接続部を長く取るこ
とによって接続抵抗を低くおさえている。
2. Description of the Related Art A superconducting coil at a cryogenic temperature is supplied with current from a power source in a room temperature space by a current lead made of a copper plate or the like. That is, as shown in FIG. 5, the connection between the superconducting wire 1 and the current lead 2 is provided in a cryogenic atmosphere in the container 3 or in a coolant such as liquid helium 4.
At this time, in order to prevent the transition (quenching) of the superconducting wire to the normal conducting state due to heat generation at the connection portion, the connection resistance is kept low by making the connection portion long.

【0003】[0003]

【発明が解決しようとする課題】しかし、超電導コイル
に交流電流のように、電流の変化率が大きい電流を通電
する場合には接続部全体において電流が電流リードから
超電導線に徐々に分流していかず、電流リードの先端ま
で比較的大きな電流が流れ、そこでの発熱により超電導
線が加熱され超電導状態から、常電導状態へと転移(ク
エンチ)する可能性がある。本発明の目的は、電流リー
ドの接続端子と超電導線の接続部の電流容量が大きく発
熱が少ない超電導装置を提供することにある。
However, when a current having a large rate of change in current, such as an alternating current, is applied to the superconducting coil, the current is gradually shunted from the current lead to the superconducting wire in the entire connecting portion. However, a relatively large current flows to the tip of the current lead, and the heat generated therein may heat the superconducting wire, causing a transition (quenching) from the superconducting state to the normal conducting state. An object of the present invention is to provide a superconducting device that has a large current capacity at a connecting portion of a current lead and a connecting portion of a superconducting wire and little heat generation.

【0004】[0004]

【課題を解決するための手段】本発明の超電導装置は、
螺旋状に巻かれた接続端子の各ターンを短絡するように
超電導コイル等からの超電導線を接続した構成とする。
The superconducting device of the present invention comprises:
A superconducting wire from a superconducting coil or the like is connected so that each turn of the spirally wound connection terminal is short-circuited.

【0005】[0005]

【作用】このような構成にすると、接続端子の螺旋状部
分によってインダクタンスが生じ、電流が良好に超電導
線へ分流するようになる。
With this structure, an inductance is generated by the spiral portion of the connection terminal, and the current is shunted to the superconducting wire in a good condition.

【0006】[0006]

【実施例】以下、本発明の一実施例を図面によって説明
する。
DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS An embodiment of the present invention will be described below with reference to the drawings.

【0007】図1は、本実施例の要部を示す図である。
超電導線1としては直径1μm以下の超電導フィラメン
トを数万本持つ極細多芯超電導線を用いる。また、交流
通電時の損失を低減するために各フィラメントは電気抵
抗の比較的高いCuNiによって囲む。また、素線間に
結合電流が流れるのを防ぐために、各素線の表面にもC
uNiの層を設けておく。この超電導線は複数次の撚線
であり、本実施例では接続端子6において一つ前のレベ
ルの撚線まで撚り戻して接続している。接続端子6は螺
旋状に巻かれている。また、本実施例では接続端子6の
各ターンは離れているが、絶縁物等で各ターンを絶縁し
てもよい。
FIG. 1 is a diagram showing a main part of this embodiment.
As the superconducting wire 1, an ultrafine multicore superconducting wire having tens of thousands of superconducting filaments having a diameter of 1 μm or less is used. Also, each filament is surrounded by CuNi, which has a relatively high electric resistance, in order to reduce the loss during AC energization. In addition, in order to prevent the coupling current from flowing between the wires, C is also applied to the surface of each wire.
A layer of uNi is provided. This superconducting wire is a twisted wire of a plurality of orders, and in this embodiment, the connection terminal 6 is twisted back to the previous level of twisted wire and connected. The connection terminal 6 is spirally wound. In addition, although each turn of the connection terminal 6 is separated in this embodiment, each turn may be insulated by an insulator or the like.

【0008】本実施例のような構成にすると、接続端子
の螺旋状部分のインダクタンスの効果によって電流が接
続端子6から超電導線1に徐々に分流していく。このこ
とを接続部の等価回路を表わす図2を用いて説明する。
この図において、Lcuは接続端子のインダクタンス、R
cuは接続端子の抵抗、Lscは超電導線のインダクタン
ス、Rcon1,Rcon2は接続抵抗である。このとき、Rco
n1,Rcon2に流れる電流をそれぞれI1,I2とすれば
With the structure of this embodiment, the current is gradually shunted from the connection terminal 6 to the superconducting wire 1 by the effect of the inductance of the spiral portion of the connection terminal. This will be described with reference to FIG. 2 showing an equivalent circuit of the connection portion.
In this figure, Lcu is the inductance of the connection terminal, R
cu is the resistance of the connection terminal, Lsc is the inductance of the superconducting wire, and Rcon1 and Rcon2 are the connection resistances. At this time, Rco
If the currents flowing through n1 and Rcon2 are I1 and I2 respectively,

【0009】[0009]

【数1】 [Equation 1]

【0010】つまり、この場合には電流が超電導線に徐
々に分流していくことになる。これに対し、50Hz等の
交流を通電する場合には、インダクタンスを考慮する必
要がある。一般的にインダクタンスは細い線材の方が大
きい。従って、交流を通電する場合には細い線材つまり
超電導線の方へは流れにくいことになる。これは、上式
でLsc>Lcuであることに対応する。 また、本実施例においては、超電導線1が対称的に接続
端子6に接続されているため、超電導線1の各撚線にお
ける分流のアンバランスがなくなる。また、一般的に交
流電流を通電した場合の表皮厚さδxは次式によって与
えられる。
That is, in this case, the current is gradually shunted to the superconducting wire. On the other hand, when energizing an alternating current of 50 Hz, it is necessary to consider the inductance. Generally, the inductance of a thin wire is larger. Therefore, when alternating current is applied, it is difficult for the thin wire, that is, the superconducting wire, to flow. This corresponds to Lsc> Lcu in the above equation. Further, in the present embodiment, since the superconducting wire 1 is symmetrically connected to the connection terminal 6, there is no imbalance of the shunt current in each twisted wire of the superconducting wire 1. Further, generally, the skin depth δx when an alternating current is applied is given by the following equation.

【0011】[0011]

【数2】 ただし、ω:角周波数、μ:透磁率、σ:電気伝導度[Equation 2] Where ω: angular frequency, μ: permeability, σ: electrical conductivity

【0012】極低温において接続端子に交流電流を通電
する場合の表皮厚さδxを求めると約1mmとなる。従っ
て接続端子の厚さが2mm以上の場合には、接続端子の見
かけの抵抗が増加し発熱が大きくなる。そのため、中実
の導体を用いても、交流を通電する場合には表皮効果に
よって中央部にはほとんど電流が流れない。しかし、本
実施例における接続端子6では中空の銅パイプを用い
る。そのため、通電時に無駄になる部分が少ない。この
ようにして、本実施例によれば、交流通電時の発熱が小
さい接続端子を構成することができる。 (他の実施例)
The skin thickness δx when an alternating current is applied to the connection terminal at an extremely low temperature is about 1 mm. Therefore, when the thickness of the connection terminal is 2 mm or more, the apparent resistance of the connection terminal increases and heat generation increases. Therefore, even when a solid conductor is used, almost no current flows in the central portion due to the skin effect when an alternating current is applied. However, a hollow copper pipe is used for the connection terminal 6 in this embodiment. Therefore, there are few parts that are wasted when energized. In this way, according to the present embodiment, it is possible to configure the connection terminal that generates less heat when an alternating current is applied. (Other embodiments)

【0013】図3は、本発明の他の実施例の要部を示す
図である。接続端子7は銅の棒に螺旋状の溝を加工した
ものである。この実施例においても超電導線1を接続端
子7において一つ前のレベルの撚線まで撚り戻して接続
している。
FIG. 3 is a diagram showing a main part of another embodiment of the present invention. The connection terminal 7 is a copper rod processed with a spiral groove. Also in this embodiment, the superconducting wire 1 is untwisted to the previous stranded wire at the connection terminal 7 and connected.

【0014】超電導線1が対称的に接続端子7に接続さ
れているため、超電導線1の各撚線における分流のアン
バランスがなくなる。また、本実施例における接続端子
7は、銅の棒に螺旋状に溝を加工するだけでよいので製
作性がよい。
Since the superconducting wire 1 is symmetrically connected to the connecting terminal 7, there is no imbalance of the shunt current in each twisted wire of the superconducting wire 1. Further, the connection terminal 7 in the present embodiment has good manufacturability because it is only necessary to spirally form a groove on a copper rod.

【0015】図4は、本発明のさらに他の実施例におけ
る電流供給端子を示す図である。接続端子8は銅のパイ
プに螺旋状に溝を加工したものである。本実施例では溝
が比較的多いため、銅のパイプのなかに補強用のFRP
等の補強用筒9を挿入している。ただし、溝の本数や長
さによっては補強用筒9は銅のパイプの中の一部のみに
入れる、あるいは不用となる。また、本実施例では溝に
は特にスペーサー等は入れていないが、加工上FRP等
の絶縁物を詰めることも有り得る。本実施例では超電導
線1が対称的に接続端子に接続されているため、超電導
線1の各撚線における分流のアンバランスがなくなる。
また、銅パイプを用いているため表皮効果による無駄な
部分が少ない。
FIG. 4 is a diagram showing a current supply terminal in still another embodiment of the present invention. The connection terminal 8 is a copper pipe in which a groove is spirally processed. In this embodiment, since there are relatively many grooves, the FRP for reinforcement is provided in the copper pipe.
The reinforcing cylinder 9 is inserted. However, depending on the number and length of the grooves, the reinforcing cylinder 9 may be put in only a part of the copper pipe, or may be unnecessary. Further, in the present embodiment, the groove is not particularly provided with a spacer or the like, but an insulator such as FRP may be filled for processing. In this embodiment, since the superconducting wire 1 is symmetrically connected to the connection terminals, the imbalance of the shunt current in each twisted wire of the superconducting wire 1 is eliminated.
Also, since a copper pipe is used, there is little wasteful part due to the skin effect.

【0016】[0016]

【発明の効果】以上説明したように、本発明によれば電
流容量が大きく発熱等の損失が少ない接続部を持つ超電
導装置を提供することができる。
As described above, according to the present invention, it is possible to provide a superconducting device having a connection portion having a large current capacity and a small loss such as heat generation.

【図面の簡単な説明】[Brief description of drawings]

【図1】本発明の第一の実施例の超電導装置の接続部を
示す図。
FIG. 1 is a diagram showing a connecting portion of a superconducting device according to a first embodiment of the present invention.

【図2】本発明の超電導装置における接続部の電気的な
等価回路を示す図。
FIG. 2 is a diagram showing an electrical equivalent circuit of a connection portion in the superconducting device of the present invention.

【図3】本発明の第二の実施例の超電導装置の接続部を
示す図。
FIG. 3 is a diagram showing a connecting portion of a superconducting device according to a second embodiment of the present invention.

【図4】本発明の第三の実施例の超電導装置の接続部を
示す図。
FIG. 4 is a diagram showing a connecting portion of a superconducting device of a third embodiment of the present invention.

【図5】従来の超電導装置における接続部を示す図。FIG. 5 is a view showing a connecting portion in a conventional superconducting device.

【符号の説明】[Explanation of symbols]

1…超電導線 2…電流リード 3…容器 4…液体ヘリウム 5…超電導コイル 6,7,8…接続端子 9…補強円筒 1 ... Superconducting wire 2 ... Current lead 3 ... Container 4 ... Liquid helium 5 ... Superconducting coil 6, 7, 8 ... Connection terminal 9 ... Reinforcing cylinder

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 螺旋状部を有する接続端子と、前記螺旋
状部のターンを短絡するように接続された超電導線とを
備えたことを特徴とする超電導装置。
1. A superconducting device comprising: a connection terminal having a spiral portion; and a superconducting wire connected so as to short-circuit the turns of the spiral portion.
JP29694891A 1991-11-13 1991-11-13 Superconducting apparatus Pending JPH05135944A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP29694891A JPH05135944A (en) 1991-11-13 1991-11-13 Superconducting apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP29694891A JPH05135944A (en) 1991-11-13 1991-11-13 Superconducting apparatus

Publications (1)

Publication Number Publication Date
JPH05135944A true JPH05135944A (en) 1993-06-01

Family

ID=17840258

Family Applications (1)

Application Number Title Priority Date Filing Date
JP29694891A Pending JPH05135944A (en) 1991-11-13 1991-11-13 Superconducting apparatus

Country Status (1)

Country Link
JP (1) JPH05135944A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102751069A (en) * 2012-07-30 2012-10-24 西部超导材料科技股份有限公司 Low-resistance multi-core NbTi/Cu superconducting magnet coil inner joint and preparation method

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN102751069A (en) * 2012-07-30 2012-10-24 西部超导材料科技股份有限公司 Low-resistance multi-core NbTi/Cu superconducting magnet coil inner joint and preparation method

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