JP2859953B2 - Superconducting device and permanent current switch used for the superconducting device - Google Patents
Superconducting device and permanent current switch used for the superconducting deviceInfo
- Publication number
- JP2859953B2 JP2859953B2 JP31416290A JP31416290A JP2859953B2 JP 2859953 B2 JP2859953 B2 JP 2859953B2 JP 31416290 A JP31416290 A JP 31416290A JP 31416290 A JP31416290 A JP 31416290A JP 2859953 B2 JP2859953 B2 JP 2859953B2
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- superconducting
- resistance
- permanent current
- wire
- current switch
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Description
【発明の詳細な説明】 〔産業上の利用分野〕 本発明は超電導装置及び該超電導装置に使用する永久
電流スイツチに係り、特に超電導コイルと永久電流スイ
ツチの接続に関する。Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a superconducting device and a permanent current switch used for the superconducting device, and more particularly to a connection between a superconducting coil and a permanent current switch.
核磁気共鳴装置(MRI)等に使用する超電導コイル装
置は、超電導コイルを永久電流(循環電流)モードで使
用するために該超電導コイルと並列に永久電流スイツチ
が接続される。この永久電流スイツチは、形状,重量及
び操作(制御)性等の観点から、超電導材の外周に比抵
抗が大きいマトリツクス層が形成された超電導線と該超
電導線を加熱するヒータとを備え、ヒータによつて超電
導線の温度を制御して該超電導線を超電導状態(オン状
態)または常電導状態(オフ状態)とする構成である。In a superconducting coil device used for a nuclear magnetic resonance apparatus (MRI) or the like, a permanent current switch is connected in parallel with the superconducting coil to use the superconducting coil in a permanent current (circulating current) mode. This permanent current switch is provided with a superconducting wire having a matrix layer having a large specific resistance formed on the outer periphery of a superconducting material and a heater for heating the superconducting wire from the viewpoints of shape, weight and operability (control). Thus, the temperature of the superconducting wire is controlled to bring the superconducting wire into a superconducting state (on state) or a normal conducting state (off state).
第7図は、このような超電導装置の電気的接続(配
置)構成を示している。冷却容器1に充填された液体ヘ
リウム2に浸された超電導コイル3には、励磁電源4か
ら励磁電流が供給される。給電時には、超電導コイル3
と並列に接続された永久電流スイツチ5をオフ状態とす
るために、該永久電流スイツチ5を制御するヒータ6に
制御電源7から電流を供給し、超電導線8を加熱して常
電導状態にする。そして、超電導コイル3に流れている
励磁電流を永久電流スイツチ5を介して循環する永久電
流とするためには、ヒータ6への給電を止めて超電導線
8を周囲の液体ヘリウム2で冷却して超電導状態にし、
該永久電流スイツチ5をオン状態にする。FIG. 7 shows an electrical connection (arrangement) configuration of such a superconducting device. An excitation current is supplied from an excitation power supply 4 to the superconducting coil 3 immersed in the liquid helium 2 filled in the cooling container 1. When power is supplied, the superconducting coil 3
A current is supplied from a control power supply 7 to a heater 6 for controlling the permanent current switch 5, which is connected in parallel with the superconducting current switch 5, and the superconducting wire 8 is heated to a normal conduction state. . Then, in order to make the exciting current flowing in the superconducting coil 3 a permanent current circulating through the permanent current switch 5, the power supply to the heater 6 is stopped and the superconducting wire 8 is cooled by the surrounding liquid helium 2. Into superconducting state,
The permanent current switch 5 is turned on.
永久電流スイッチ5は好ましいオン/オフ機能を実現
するために、該永久電流スイツチ5を構成する超電導線
8には、NbTi合金線を超電導材として使用し、オフ状態
で大きい抵抗値を得るために、例えばCuNi合金等の比抵
抗の大きい金属をマトリツクスとする極細多心線が用い
られている。The permanent current switch 5 uses a NbTi alloy wire as a superconducting material for the superconducting wire 8 constituting the permanent current switch 5 in order to realize a preferable on / off function. For example, an ultrafine multifilamentary wire having a matrix made of a metal having a large specific resistance such as a CuNi alloy is used.
しかしながら、比抵抗の大きいマトリツクスを用いた
超電導線は、CuやAl等のように比抵抗の小さい金属をマ
トリツクスとする超電導コイル用の超電導線に較べて電
磁気的に不安定であり、超電導状態での通電許容電流が
小さい。このために、超電導コイル3に対して複数個の
永久電流スイツチ5を並列接続して大きな永久電流を確
保することが行われている。そして、複数個の永久電流
スイツチ5に均等に電流を分流すために、励磁用電流線
との間に低抵抗体を介在させた接続を行うことが提案さ
れている。However, a superconducting wire using a matrix having a large specific resistance is electromagnetically unstable compared to a superconducting wire for a superconducting coil using a metal having a small specific resistance, such as Cu or Al, in the superconducting state. Is small. For this reason, a large permanent current is secured by connecting a plurality of permanent current switches 5 to the superconducting coil 3 in parallel. Then, in order to distribute the current evenly to the plurality of permanent current switches 5, it has been proposed to make a connection with a low resistance element between the excitation current line and the excitation current line.
この種の超電導装置及び永久電流スイツチは、特開昭
61−269301号公報及び特開平1−102905号公報に開示さ
れている。This type of superconducting device and permanent current switch is disclosed in
It is disclosed in JP-A-61-269301 and JP-A-1-102905.
しかしながら、この種の従来の超電導装置及び永久電
流スイツチは、永久電流スイツチの超電導線と低抵抗体
との接続部において、CuNi合金マトリツクス層の抵抗に
よるジュール発熱が原因で、しばしば、該超電導線が超
電導状態から常電導状態に転移してしまう問題があつ
た。However, this type of conventional superconducting device and the persistent current switch often have a problem in that the superconducting wire is often connected to the superconducting wire of the persistent current switch and the low-resistance body due to the Joule heat generated by the resistance of the CuNi alloy matrix layer. There was a problem that a transition from a superconducting state to a normal conducting state occurred.
従って、本発明の目的は、超電導コイルと永久電流ス
イツチとの並列接続を仲介する低抵抗体と永久電流スイ
ツチの接続部の接続抵抗値を小さくして大きな永久電流
を安定に流すことができる超電導装置及び永久電流スイ
ツチを提供することにある。Accordingly, an object of the present invention is to provide a superconducting coil that can flow a large permanent current stably by reducing the connection resistance value of the connection portion between the low-resistance body and the permanent current switch that mediates the parallel connection of the superconducting coil and the permanent current switch. It is to provide a device and a permanent current switch.
この目的を達成するために、第1の発明は、超電導コ
イルと、超電導材の外周に比抵抗が大きいマトリツクス
層が形成された超電導線と該超電導線を加熱する加熱手
段とを備えた永久電流スイツチと、前記超電導コイルと
永久電流スイツチとの並列接続を仲介する低抵抗体を備
えた超電導装置において、前記永久電流スイツチは、前
記マトリツクス層外に露出した超電導材部分を前記低抵
抗体に接続することを特徴とし、 第2の発明は、超電導材の外周に比抵抗が大きいマト
リツクス層が形成された超電導線と該超電導線を加熱す
るヒータと前記超電導線を延長して口出し線部とした永
久電流スイツチにおいて、前記口出し線部の接続部分の
超電導材をマトリツクス層外に露出させたことを特徴と
する。In order to achieve this object, a first invention provides a permanent current comprising a superconducting coil, a superconducting wire having a matrix layer having a large specific resistance formed on the outer periphery of a superconducting material, and a heating means for heating the superconducting wire. In a superconducting device including a switch and a low-resistance element that mediates a parallel connection of the superconducting coil and the persistent current switch, the permanent current switch connects a superconducting material portion exposed outside the matrix layer to the low-resistance body. The second invention is characterized in that a superconducting wire in which a matrix layer having a large specific resistance is formed on the outer periphery of a superconducting material, a heater for heating the superconducting wire, and the superconducting wire are extended to form a lead wire portion. In the permanent current switch, a superconducting material at a connection portion of the lead wire portion is exposed outside the matrix layer.
永久電流スイツチと低抵抗体との接続部分には比抵抗
が大きいマトリツクス層が介在しないので接続抵抗が小
さくなり、接続抵抗のジユール発熱による常電導状態転
移がなくなる。Since a matrix layer having a large specific resistance is not interposed at the connection portion between the permanent current switch and the low-resistance body, the connection resistance is reduced, and the transition of the normal conduction state due to the double heat generation of the connection resistance is eliminated.
超電導コイルに複数個の永久電流スイツチを並列した
超電導装置では、各永久電流スイツチに均等に電流を分
配するために、前述したように、低抵抗体を仲介してお
り、その抵抗値が1/107Ω程度あるので、回路抵抗が零
の永久電流モードとはならない。永久電流の減衰時定数
は、超電導コイルのインダクタンスLと循環回路の抵抗
Rの比L/Rで決まる。超電導コイルでの永久電流モード
持続必要時間は20時間程度で十分であり、前記低抵抗体
の抵抗値が減衰時定数に及ぼす影響は問題にならない程
度である。In a superconducting device in which a plurality of permanent current switches are arranged in parallel with a superconducting coil, as described above, a low-resistance element is interposed as described above in order to distribute current evenly to each of the permanent current switches. Since it is about 10 7 Ω, it does not become the permanent current mode with zero circuit resistance. The decay time constant of the permanent current is determined by the ratio L / R of the inductance L of the superconducting coil and the resistance R of the circulation circuit. The duration required for the permanent current mode in the superconducting coil is about 20 hours, which is sufficient, and the effect of the resistance value of the low-resistance body on the decay time constant is not significant.
しかしながら、発明者等が種々の実験を行つた結果、
該抵抗が永久電流スイツチの超電導線の接続部分に集中
しているために、大きな永久電流を流すと、そのジユー
ル発熱のために該永久電流スイツチの超電導線が超電導
状態から常電導状態に転移して永久電流モードを維持す
ることができなくなる事態が発生することが分かつた。However, as a result of various experiments performed by the inventors,
Since the resistance is concentrated at the connection portion of the superconducting wire of the permanent current switch, when a large permanent current is applied, the superconducting wire of the permanent current switch changes from the superconducting state to the normal conducting state due to the heat generated by the module. It has been found that a situation in which the permanent current mode cannot be maintained occurs.
永久電流スイツチの超電導線は、比較的高抵抗のCuNi
合金をマトリツクスとするNbTi極細多心線であるので、
安定性のマージンが極めて小さく、超電導コイルの超電
導線として使用されるCuマトリツクスNbTi極細多心線の
場合の1/10以下の熱エネルギーで超電導状態から常電導
状態に転移してしまうことが分かつた。The superconducting wire of the persistent current switch is made of CuNi with relatively high resistance.
Since it is an NbTi extra-fine multi-core wire using an alloy as a matrix,
The margin of stability is extremely small, and it has been found that the transition from the superconducting state to the normal conducting state is made with less than 1/10 of the heat energy of the Cu matrix NbTi ultra-fine multi-core wire used as the superconducting wire of the superconducting coil. .
従つて本発明の各実施例は、低抵抗体に対する永久電
流スイツチの超電導線の接続部の接続抵抗が極力小さく
なるように工夫されている。Therefore, each embodiment of the present invention is devised so that the connection resistance of the connection portion of the superconducting wire of the permanent current switch to the low resistance body is minimized.
超電導線同志の接続は、接続抵抗の観点からは接続抵
抗値が零の超電導接続が理想的であるが、多数のNbTi極
細多心線同志を加締め圧着で接続したり、スポツト溶接
接続する構成は、電磁気的及び機械的に不安定な接続部
となる。従つて、本発明は、超電導コイルに対する永久
電流スイツチの超電導線の接続部には低抵抗体を介在さ
せ、然も、永久電流スイツチの超電導線の高抵抗マトリ
ツクスが介在されて接続抵抗値が増えないように、該高
抵抗マトリツクスを除去して該超電導線のNbTi極細多心
線を露出させて低抵抗体に接続するようにしている。た
だ、裸のNbTi極細多心線を低抵抗体に良好な状態で直接
接続することが困難であるので、低抵抗のスリーブを介
在させたり、比抵抗が小さいCuマトリツクス超電導線を
介在させたりしている。低抵抗体に対する超電導線の好
ましい接続抵抗値の許容最大値は、該超電導コイルが動
作状態にあるときの温度4.2Kにおいて、1/109Ω程度で
ある。Ideally, superconducting connections with a connection resistance value of zero are ideal for the connection of superconducting wires.However, many NbTi ultra-fine multi-core wires are connected by crimping or spot welding. Is a connection that is electromagnetically and mechanically unstable. Therefore, according to the present invention, the connection portion of the superconducting wire of the permanent current switch to the superconducting coil is provided with a low-resistance body, and the connection resistance value is increased due to the high resistance matrix of the superconducting wire of the permanent current switch. To avoid this, the high-resistance matrix is removed to expose the ultra-fine NbTi multifilamentary wire of the superconducting wire and connect it to a low-resistance body. However, it is difficult to directly connect bare NbTi ultrafine multifilamentary wires to a low-resistance body in good condition.Therefore, a low-resistance sleeve is interposed, or a Cu matrix superconducting wire with low specific resistance is interposed. ing. The allowable maximum value of the preferable connection resistance value of the superconducting wire with respect to the low-resistance body is about 1/10 9 Ω at a temperature of 4.2 K when the superconducting coil is in an operating state.
低抵抗のスリーブには無酸素銅を使用し、接続部の電
磁気的安定性向上と電磁力に対する機械的補強機能をも
たせる。また、スリーブ内の超電導線の充填率が低いと
接続(圧接)状態が不安定になるので、AgやCuの粉末や
繊維を充填して堅固な接続状態が得られるようにすると
よい。Oxygen-free copper is used for the low-resistance sleeve to improve the electromagnetic stability of the connection and provide mechanical reinforcement against electromagnetic forces. If the filling rate of the superconducting wire in the sleeve is low, the connection (pressure welding) state becomes unstable. Therefore, it is preferable that a solid connection state is obtained by filling with Ag or Cu powder or fiber.
また、永久電流スイツチにおける超電導線の常電導状
態への転移は、その口出し線部で発生する場合が多い。
超電導線が無誘導巻きされた永久電流スイツチであつて
も、電磁力に対する固定が不十分である場合に発生す
る。永久電流スイツチ内部の巻線部はエポキシ樹脂含浸
等により堅固に固定されるが、口出し線部は自由な状態
であるので該部分が常電導状態に転移し易い。このよう
な部分をなくして安定した超電導状態を維持するために
は、低抵抗体,永久電流スイツチ(口出し線)及び接続
部を一体的に支持する支持体を設け、エポキシ樹脂含浸
(充填)や縛り付け等による固定を行うことが好まし
い。Further, the transition of the superconducting wire to the normal conducting state in the permanent current switch often occurs at the lead wire portion.
Even if the superconducting wire is a permanent current switch that is non-inductively wound, it occurs when the fixation to the electromagnetic force is insufficient. The winding inside the permanent current switch is firmly fixed by epoxy resin impregnation or the like, but since the lead wire is in a free state, the part easily transitions to a normal conduction state. In order to eliminate such parts and maintain a stable superconducting state, a low-resistance body, a persistent current switch (lead wire) and a support that integrally supports the connection portion are provided, and epoxy resin impregnation (filling) or the like is performed. It is preferable to perform fixing by binding or the like.
次に、永久電流スイツチ用超電導線のクエンチ電流の
値を該超電導線の接続構成を変えて測定・評価した結果
を説明する。測定した超電導線は、外径が0.4mmで、直
径が約10μmのNbTi極細線を1171本纏めてCu−30%Ni合
金マトリツクス中に埋設したものである。Next, the results of measurement and evaluation of the quench current value of the superconducting wire for a permanent current switch by changing the connection configuration of the superconducting wire will be described. The measured superconducting wire is one in which 1171 ultrafine NbTi wires having an outer diameter of 0.4 mm and a diameter of about 10 μm are bundled together and embedded in a Cu-30% Ni alloy matrix.
該超電導線は測定のためにヘアピン状にしてその両端
部を低抵抗体(Cu線)に接続し、液体ヘリウム中に浸し
て4.2Kの温度で外部磁界の大きさを変えながら、クエン
チ電流を測定した。測定試料(I)は永久電流スイツチ
用超電導線をそのままCu線に半田付け接続したもの、測
定試料(II)は永久電流スイツチ用超電導線の両端部の
マトリツクスを除去してNbTi極細多心線を露出させ、該
露出部にCuスリーブを加締固定(接続)し、該Cuスリー
ブをCu線に半田付け接続したものである。各測定試料
(I),(II)は、それぞれ、10本ずつ同一方法で測定
及び評価して、そのバラツキ状態も併せて測定した。The superconducting wire is made into a hairpin shape for measurement, and both ends are connected to a low-resistance body (Cu wire), immersed in liquid helium and changing the magnitude of the external magnetic field at a temperature of 4.2 K to reduce the quench current. It was measured. For the measurement sample (I), the superconducting wire for the permanent current switch was soldered and connected to the Cu wire as it was. For the measurement sample (II), the matrix at both ends of the superconducting wire for the permanent current switch was removed to form an NbTi ultrafine multi-core wire. It is exposed, a Cu sleeve is crimped and fixed (connected) to the exposed portion, and the Cu sleeve is connected by soldering to a Cu wire. Each of the measurement samples (I) and (II) was measured and evaluated by the same method for 10 samples each, and the variation was also measured.
第8図は該測定結果を示している。領域(I)は測定
試料(I)の10本の超電導線の測定値の最大値と最小値
(分布範囲)であり、領域(II)は測定試料(II)の10
本の超電導線の測定値の最大値と最小値(分布範囲)で
ある。測定試料(II)のクエンチ電流の値は、測定試料
(I)のクエンチ電流の値よりも大きいことが分かる。
測定試料(I)の常電導転移は接続部から発生してお
り、接続部の接続抵抗によるジユール発熱で超電導線が
加熱されてクエンチ電流を低下させている、と考えられ
る。このような測定結果を見ると、接続構造を工夫する
ことにより、1Tの外部磁界において従来の1.7倍の電流
を安定に流すことができることが分かる。FIG. 8 shows the measurement results. The region (I) is the maximum and minimum values (distribution range) of the measured values of the ten superconducting wires of the measurement sample (I), and the region (II) is the 10th of the measurement sample (II).
These are the maximum value and the minimum value (distribution range) of the measured values of the superconducting wires. It can be seen that the value of the quench current of the measurement sample (II) is larger than the value of the quench current of the measurement sample (I).
It is considered that the normal conduction transition of the measurement sample (I) occurred from the connection part, and the superconducting wire was heated by the Joule heat generated by the connection resistance of the connection part, thereby reducing the quench current. From these measurement results, it can be seen that by devising the connection structure, a current 1.7 times larger than that of the conventional device can be stably passed in an external magnetic field of 1T.
以下、本発明の実施例を図面を参照して具体的に説明
する。Hereinafter, embodiments of the present invention will be specifically described with reference to the drawings.
第1図は本発明になる超電導コイル装置の主要構成要
素の配置を示している。FIG. 1 shows an arrangement of main components of a superconducting coil device according to the present invention.
超電導コイル3の両端の口出し線3a,3bは低抵抗体9,1
0に半田付けにより接続される。励磁電源4から該超電
導コイル3の励磁電流を供給するための励磁用電流線1
1,12もこの低抵抗体9,10に半田付けで接続される。超電
導コイル3に対して並列回路を構成するために3個の永
久電流スイツチ5a,5b,5cが前記低抵抗体9,10間に並列接
続される。The lead wires 3a, 3b at both ends of the superconducting coil 3 are low-resistance bodies 9, 1
Connected to 0 by soldering. An exciting current line 1 for supplying an exciting current of the superconducting coil 3 from an exciting power supply 4
1, 12 are also connected to the low-resistance elements 9, 10 by soldering. In order to form a parallel circuit with the superconducting coil 3, three permanent current switches 5a, 5b, 5c are connected in parallel between the low-resistance elements 9, 10.
各永久電流スイツチ5a〜5cは、前述した永久電流スイ
ツチ5と同様な構成であり、それぞれ、NbTi合金線の超
電導体とCuNi合金のマトリツクスを使用した極細多心線
の超電導線8と、該超電導線8を加熱するヒータ(図示
せず)とを備え、各永久電流スイツチ5a〜5cはそれぞれ
の口出し線部8a,8bを前記低抵抗体9,10に接続する構成
である。各接続部は同様な接続構成であり、各口出し線
部8a,8bの接続部分のマトリツクスを硝酸で溶解除去し
てNbTi合金の極細多心線を露出させ、該露出部分にCuス
リーブ13,14を被せて圧着接続し、該Cuスリーブ13,14を
低抵抗体9,10に半田付けで接続する構成である。Each of the permanent current switches 5a to 5c has the same configuration as the above-described permanent current switch 5, and includes a superconducting wire 8 of an ultrafine multicore wire using a superconductor of an NbTi alloy wire and a matrix of a CuNi alloy. A heater (not shown) for heating the wire 8 is provided, and each of the permanent current switches 5a to 5c connects the lead wire portions 8a and 8b to the low resistance elements 9 and 10, respectively. Each connection part has the same connection configuration, and the matrix at the connection part of each lead wire part 8a, 8b is dissolved and removed with nitric acid to expose the ultrafine multifilamentary wire of the NbTi alloy, and the Cu sleeves 13, 14 are exposed on the exposed part. And the Cu sleeves 13 and 14 are connected to the low-resistance elements 9 and 10 by soldering.
第2図(a),(b)は、該接続部の接続構造の一部
を詳細に示したものである。永久電流スイツチ5の超電
導線8の延長部分である口出し線部8aは、NbTi合金の極
細多心線8cとこれを埋設するCuNi合金のマトリツクス8d
から成り、接続部分となる先端部のCuNi合金マトリツク
ス8dが除去されて極細多心線8cが露出される。Cuスリー
ブ13は極細多心線8cのこの露出部分に被せて圧着接続さ
れ、該Cuスリーブ13が低抵抗体9に半田付け19で接続さ
れている。2 (a) and 2 (b) show a part of the connection structure of the connection part in detail. The lead wire portion 8a, which is an extension of the superconducting wire 8 of the persistent current switch 5, is composed of an NbTi alloy ultra-fine multi-core wire 8c and a CuNi alloy matrix 8d in which it is embedded.
, And the CuNi alloy matrix 8d at the distal end serving as a connection portion is removed, and the ultrafine multi-core wire 8c is exposed. The Cu sleeve 13 is press-fitted over this exposed portion of the ultrafine multi-core wire 8c, and the Cu sleeve 13 is connected to the low-resistance body 9 by soldering 19.
5個の永久電流スイツチ5を並列接続した従来の超電
導コイル装置で、5個のスイツチ5がオフ状態にあると
きの合成抵抗を100Ω(1個の抵抗値を500Ω)とし、オ
ン状態にあるときの許容電流を686A(1個の定格電流を
137.5A)とする特性を、本実施例では3個の永久電流ス
イツチ5a〜5cで得ることができた。すなわち、1個の永
久電流スイツチ5で228.7Aの定格電流が得られ、オフ状
態で300Ωの抵抗値が得られた。これは、各永久電流ス
イツチ5a〜5cの超電導線8の口出し線部8a,8bと低抵抗
体9,10の接続抵抗が減少して許容電流が増加することに
より実現したものである。In a conventional superconducting coil device in which five permanent current switches 5 are connected in parallel, the combined resistance when the five switches 5 are in the off state is 100Ω (one resistance value is 500Ω), and when the five switches 5 are in the on state. Current of 686A (one rated current
In this example, the characteristic of 137.5 A) could be obtained with three permanent current switches 5a to 5c. That is, a rated current of 228.7 A was obtained with one permanent current switch 5, and a resistance value of 300Ω was obtained in the off state. This is realized by reducing the connection resistance between the lead wires 8a, 8b of the superconducting wire 8 of each of the permanent current switches 5a to 5c and the low-resistance bodies 9, 10 and increasing the allowable current.
そしてこのような構成の超電導コイル装置によれば、
永久電流スイツチ5の数が減少すると共に該永久電流ス
イツチ5における超電導線8を短くすることができるの
で、超電導コイル装置内での配置所要スペース,重量,
製造コストが低減すると共に、冷却用の液体ヘリウムの
蒸発量を低減して運転コストを低減することができる。And according to the superconducting coil device having such a configuration,
Since the number of the permanent current switches 5 can be reduced and the superconducting wires 8 in the permanent current switches 5 can be shortened, the required space, weight, and weight in the superconducting coil device can be reduced.
The manufacturing cost can be reduced, and the amount of evaporation of the liquid helium for cooling can be reduced to reduce the operating cost.
第3図は永久電流スイツチ5a〜5cの各口出し線部8a,8
bを、NbTi合金の極細多心線をCuマトリツクス中に埋設
した低抵抗の超電導線20,21を介して低抵抗体9,10に半
田付け接続した超電導コイル装置を示している。FIG. 3 shows the respective lead wires 8a, 8 of the permanent current switches 5a to 5c.
FIG. 1B shows a superconducting coil device in which b is connected by soldering to low-resistance members 9 and 10 via low-resistance superconducting wires 20 and 21 in which ultrafine multi-core wires of an NbTi alloy are embedded in Cu matrix.
この実施例で、永久電流スイツチ5a〜5cにおける超電
導線8の各口出し線部8a,8bと仲介用超電導線20,21との
接続は、接続部分のマトリツクスを除去してNbTi合金の
極細多心線を露出させ、該露出部分を重ね合わせた状態
でCuスリーブ13,14を被せて圧着接続する構成である。In this embodiment, the connection between the lead wires 8a, 8b of the superconducting wire 8 and the intermediary superconducting wires 20, 21 in the permanent current switches 5a to 5c is performed by removing the matrix at the connection portion and making the NbTi alloy extra fine multi-core. The configuration is such that the wires are exposed, the Cu sleeves 13 and 14 are covered with the exposed portions overlapped, and pressure-bonded.
第4図(a)〜(e)は、該接続部の接続プロセスを
詳細に示している。永久電流スイツチ5の超電導線8の
延長部分である口出し線部8aで接続部分となる先端部の
CuNi合金マトリツクス8dが除去されて極細多心線8cが露
出され、同様に、仲介用超電導線20の接続部分となる先
端部のCuマトリツクス20dも除去されて極細多心線20cが
露出され、極細多心線8c,20cの該露出部分を重ね合わせ
た状態でCuスリーブ13を被せて圧着接続される。そし
て、仲介用超電導線20の他端部分はCuマトリツクス20d
を付けたままの状態で低抵抗体9に半田付け接続され
る。4 (a) to 4 (e) show the connection process of the connection section in detail. The leading end portion serving as a connection portion at the lead wire portion 8a which is an extension portion of the superconducting wire 8 of the permanent current switch 5
The CuNi alloy matrix 8d is removed to expose the ultrafine multifilamentary wire 8c.Similarly, the Cu matrix 20d at the distal end serving as a connection portion of the intermediary superconducting wire 20 is also removed to expose the ultrafine multifilamentary wire 20c. With the exposed portions of the multicore wires 8c and 20c overlapped with each other, a Cu sleeve 13 is put on and connected by crimping. The other end of the intermediary superconducting wire 20 is a Cu matrix 20d.
Is connected to the low-resistance body 9 by soldering.
この実施例は、Cuスリーブ13内の極細多心線の充填率
が大幅に向上して極細多心線同志の超電導接続が安定
し、永久電流スイツチ5a〜5c間のクエンチ電流のバラツ
キが低減する利点がある。In this embodiment, the filling rate of the ultrafine multifilamentary wires in the Cu sleeve 13 is greatly improved, the superconducting connection between the ultrafine multifilamentary wires is stabilized, and the variation of the quench current between the permanent current switches 5a to 5c is reduced. There are advantages.
第5図(a),(b)は、永久電流スイツチ用超電導
線と仲介用超電導線との接続の他の実施例を示してい
る。FIGS. 5 (a) and 5 (b) show another embodiment of the connection between the superconducting wire for permanent current switch and the superconducting wire for mediation.
永久電流スイツチ5の超電導線8は、通常、線材製法
上の制約から、Cu−30%Ni合金をマトリツクスとするNb
Ti極細多心線8cを中心にしてその周りにCu−30%Ni合金
層8dが存在する構成である。例えば、外径が0.46mmの超
電導線では、外周部分のCu−30%Ni合金層8cの厚さは約
0.03mmである。The superconducting wire 8 of the permanent current switch 5 is usually made of Nb with a matrix of Cu-30% Ni alloy due to restrictions on the wire rod manufacturing method.
The structure is such that a Cu-30% Ni alloy layer 8d exists around the Ti ultrafine multi-core wire 8c. For example, for a superconducting wire having an outer diameter of 0.46 mm, the thickness of the Cu-30% Ni alloy
0.03 mm.
このような超電導線8の口出し線部8aにNbTi合金の極
細多心線をCuマトリツクス中に埋設した仲介用超電導線
をそのまま長さ300mmにわたつて半田付け接続したもの
を液体ヘリウムに浸して冷却した状態で、その接続抵抗
値を測定すると、8/108Ωもの接続抵抗があり、この接
続抵抗値の大部分は外周部分のCu−30%Ni合金層8dによ
るものである。A superconducting superconducting wire in which an NbTi alloy ultrafine multifilamentary wire is buried in Cu matrix in the lead wire portion 8a of such a superconducting wire 8 is directly connected by soldering over a length of 300 mm and immersed in liquid helium for cooling. When the connection resistance is measured in this state, the connection resistance is as high as 8/10 8 Ω, and most of the connection resistance is due to the Cu-30% Ni alloy layer 8d in the outer peripheral portion.
この実施例は、このようなCu−30%Ni合金層8dによる
接続抵抗の増加を抑えたもので、永久電流スイツチ用超
電導線8の口出し線部8aにおける長さ450mの半田付け接
続端部の前記Cu−30%Ni合金層8dを硝酸にて溶解除去
し、該接続端部に2本のCuマトリツクス極細多心線構造
の仲介用超電導線20a,20bを長さ450mmにわたつて半田付
け接続したものである。In this embodiment, an increase in connection resistance due to such a Cu-30% Ni alloy layer 8d is suppressed, and a 450 m long soldering connection end portion at a lead wire portion 8a of a superconducting wire 8 for permanent current switch 8 is used. The Cu-30% Ni alloy layer 8d is dissolved and removed with nitric acid, and two Cu matrix superconducting superconducting wires 20a, 20b having a length of 450 mm are soldered to the connection end portions over a length of 450 mm. It was done.
この接続部の電気抵抗を温度4.2Kで測定したところ、
9/1010Ωであり、永久電流スイツチ8のクエンチ電流に
影響しない値であることが分かつた。この接続抵抗値
は、他の実施例における接続抵抗値よりも劣る値である
が、接続構造が極めて単純であり、信頼性の高い接続部
が得られる利点がある。When the electrical resistance of this connection was measured at a temperature of 4.2K,
9/10 10 Ω, which is a value that does not affect the quench current of the permanent current switch 8. Although this connection resistance value is inferior to the connection resistance values in the other embodiments, there is an advantage that the connection structure is extremely simple and a highly reliable connection portion can be obtained.
このような超電導コイル装置における永久電流スイツ
チの特性を安定させるには、電磁力によつて口出し線部
あるいは仲介用超電導線が振動しないようにすることが
好ましいことは前述した通りである。As described above, in order to stabilize the characteristics of the permanent current switch in such a superconducting coil device, it is preferable to prevent the lead wire portion or the intermediate superconducting wire from vibrating due to the electromagnetic force.
第6図は、口出し線部及び仲介用超電導線を堅固に保
持して、振動に起因するクエンチの発生を防止した実施
例である。低抵抗体と永久電流スイツチの接続構成は、
第3図を参照して前述した実施例と同一である。2個の
低抵抗体9,10の間に配置された永久電流スイツチ5a〜5c
とその各口出し線部8a,8b及び仲介用超電導線20,21更に
は両線を圧着接続するCuスリーブ13,14を、これらに沿
わせて絶縁状態で配置したステンレス製の支持板22に縛
り付け又は樹脂含浸あるいは充填等の固定材23により、
絶縁状態に一体的に固着している。FIG. 6 shows an embodiment in which the lead wire portion and the intermediary superconducting wire are firmly held to prevent the occurrence of quench due to vibration. The connection configuration of the low resistance element and the permanent current switch is
This is the same as the embodiment described above with reference to FIG. Permanent current switches 5a to 5c arranged between two low-resistance elements 9 and 10
And the lead wires 8a and 8b and the intermediate superconducting wires 20 and 21 and the Cu sleeves 13 and 14 for crimp-connecting both wires are tied to a stainless steel support plate 22 arranged in an insulated state along these lines. Or by a fixing material 23 such as resin impregnation or filling,
They are integrally fixed in an insulating state.
本発明は、永久電流スイツチと低抵抗体との接続部分
には比抵抗が大きいマトリツクス層が介在しないので、
接続抵抗が小さくなり該接続抵抗のジユール発熱による
影響が少なくなり、大きな永久電流を安定に流すことが
できる超電導装置及び永久電流スイツチを提供すること
ができる。According to the present invention, since a matrix layer having a large specific resistance is not interposed at a connection portion between the permanent current switch and the low-resistance body,
It is possible to provide a superconducting device and a permanent current switch capable of stably supplying a large permanent current by reducing the connection resistance and reducing the influence of the connection resistance due to the joule heat.
第1図〜第6図は本発明の実施例を示すもので、第1図
はその一実施例である超電導コイル装置の主要構成要素
配置図、第2図(a),(b)は低抵抗体と永久電流ス
イツチの接続部の詳細を示す縦断側面図とそのB−B断
面図、第3図は他の実施例である超電導コイル装置の主
要構成要素配置図、第4図(a)〜(e)は永久電流ス
イツチ口出し線部と仲介超電導線の接続工程図、第5図
(a),(b)は永久電流スイツチ用超電導線と仲介用
超電導線との接続の他の実施例を示す縦断側面図と縦断
正面図、第6図は更に他の実施例である超電導コイル装
置の主要構成要素配置図である。 第7図は従来の超電導コイル装置の主要構成要素配置図
である。 第8図は接続抵抗特性図である。 3……超電導コイル、3a,3b……口出し線、5a〜5c……
永久電流スイツチ、8a,8b……口出し線部、8c……NbTi
合金の極細多心線、8d……CuNi合金のマトリツクス、9,
10……低抵抗体、13,14……Cuスリーブ、19……半田付
け。1 to 6 show an embodiment of the present invention. FIG. 1 is a layout diagram of main components of a superconducting coil device as one embodiment of the present invention, and FIGS. FIG. 3 (a) is a longitudinal sectional side view showing details of a connection portion between a resistor and a permanent current switch and a BB sectional view thereof. FIG. 3 is a layout diagram of main components of a superconducting coil device as another embodiment, 5 (e) to 5 (e) are diagrams showing a process of connecting a permanent current switch lead wire portion and an intermediate superconducting wire, and FIGS. 5 (a) and 5 (b) show another embodiment of connection between a permanent current switch superconducting wire and an intermediate superconducting wire. FIG. 6 is a layout view of main components of a superconducting coil device according to still another embodiment. FIG. 7 is an arrangement diagram of main components of a conventional superconducting coil device. FIG. 8 is a connection resistance characteristic diagram. 3. Superconducting coil, 3a, 3b Lead wire, 5a to 5c
Permanent current switch, 8a, 8b ... Lead wire, 8c ... NbTi
Ultra fine multi-core wire of alloy, 8d …… Matrix of CuNi alloy, 9,
10 ... Low resistance, 13,14 ... Cu sleeve, 19 ... Soldering.
Claims (7)
が大きいマトリックス層が形成された超電導線と該超電
導線を加熱する加熱手段とを備えた永久電流スイッチ
と、前記超電導コイルと永久電流スイッチとの並列接続
を仲介する低抵抗体を備えた超電導装置において、 前記永久電流スイッチは、前記マトリックス層外に露出
した超電導材部分が前記低抵抗体されたことを特徴とす
る超電導装置。1. A permanent current switch comprising a superconducting coil, a superconducting wire having a matrix layer having a large specific resistance formed on the outer periphery of a superconducting material, and heating means for heating the superconducting wire. A superconducting device including a low-resistance element that mediates a parallel connection with a switch, wherein the permanent current switch is configured such that a superconducting material portion exposed outside the matrix layer is the low-resistance element.
は、前記超電導材露出部分が低抵抗材スリーブを介して
前記低抵抗体に接続されたことを特徴とする超電導装
置。2. The superconducting device according to claim 1, wherein the permanent current switch has the exposed portion of the superconducting material connected to the low-resistance body via a low-resistance material sleeve.
超電導材露出部に圧着接続されると共に前記低抵抗体に
半田付け接続されたことを特徴とする超電導装置。3. The superconducting device according to claim 2, wherein the low-resistance sleeve is connected to the exposed portion of the superconducting material by crimping and soldered to the low-resistance body.
と前記低抵抗スリーブの間に充填材を充填した状態で該
低抵抗スリーブを加締接続したことを特徴とする超電導
装置。4. The superconducting device according to claim 3, wherein said low-resistance sleeve is crimped in a state where a filler is filled between said superconducting material exposed portion and said low-resistance sleeve.
電流スイッチとその接続部を一体的に固定したことを特
徴とする超電導装置。5. The superconducting device according to claim 1, wherein the low resistance element, the permanent current switch, and a connection portion thereof are integrally fixed.
いて、前記接続部の接続抵抗値を4.2Kにおいて1/109Ω
以下にしたことを特徴とする超電導装置。6. The semiconductor device according to claim 1, wherein the connection resistance of said connection portion is 1/10 9 Ω at 4.2 K.
A superconducting device characterized by the following.
クス層が形成された超電導線と該超電導線を加熱するヒ
ータとを備え、前記超電導線を延長して口出し線部とし
た永久電流スイッチにおいて、前記口出し線部の接続部
分の超電導材を前記マトリックス層から露出させたこと
を特徴とする永久電流スイッチ。7. A permanent current switch comprising a superconducting wire in which a matrix layer having a large specific resistance is formed on the outer periphery of a superconducting material, and a heater for heating the superconducting wire, wherein the superconducting wire is extended to form a lead wire portion. A permanent current switch wherein a superconducting material at a connection portion of the lead wire portion is exposed from the matrix layer.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31416290A JP2859953B2 (en) | 1990-11-21 | 1990-11-21 | Superconducting device and permanent current switch used for the superconducting device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP31416290A JP2859953B2 (en) | 1990-11-21 | 1990-11-21 | Superconducting device and permanent current switch used for the superconducting device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH04186806A JPH04186806A (en) | 1992-07-03 |
| JP2859953B2 true JP2859953B2 (en) | 1999-02-24 |
Family
ID=18049991
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP31416290A Expired - Lifetime JP2859953B2 (en) | 1990-11-21 | 1990-11-21 | Superconducting device and permanent current switch used for the superconducting device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2859953B2 (en) |
Families Citing this family (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE19720397A1 (en) * | 1997-05-15 | 1999-04-01 | Magnet Motor Gmbh | Superconducting high current switch |
| JP5356663B2 (en) * | 2007-06-27 | 2013-12-04 | 東海旅客鉄道株式会社 | Semiconductor switch and permanent current switch system |
| JP6862382B2 (en) * | 2018-03-07 | 2021-04-21 | 株式会社東芝 | High-temperature superconducting magnet device, its operation control device and method |
-
1990
- 1990-11-21 JP JP31416290A patent/JP2859953B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH04186806A (en) | 1992-07-03 |
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