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JPH0479083B2 - - Google Patents
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JPH0479083B2 - - Google Patents

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Publication number
JPH0479083B2
JPH0479083B2 JP58125967A JP12596783A JPH0479083B2 JP H0479083 B2 JPH0479083 B2 JP H0479083B2 JP 58125967 A JP58125967 A JP 58125967A JP 12596783 A JP12596783 A JP 12596783A JP H0479083 B2 JPH0479083 B2 JP H0479083B2
Authority
JP
Japan
Prior art keywords
wire
superconducting
current
switch
wires
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 - Lifetime
Application number
JP58125967A
Other languages
Japanese (ja)
Other versions
JPS6017804A (en
Inventor
Takuya Suzuki
Yoshinori Nagasu
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.)
Furukawa Electric Co Ltd
Mitsubishi Electric Corp
Original Assignee
Furukawa Electric Co Ltd
Mitsubishi Electric 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 Furukawa Electric Co Ltd, Mitsubishi Electric Corp filed Critical Furukawa Electric Co Ltd
Priority to JP58125967A priority Critical patent/JPS6017804A/en
Publication of JPS6017804A publication Critical patent/JPS6017804A/en
Publication of JPH0479083B2 publication Critical patent/JPH0479083B2/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

  • Containers, Films, And Cooling For Superconductive Devices (AREA)
  • Non-Insulated Conductors (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

[産業上の利用分野] 本考案は、超電導マグネツト等に使用される永
久電流スイツチ用超電導線の改良に関する。 [従来の技術および課題] 一般にスイツチ用線材は、超電導から常電導に
遷移したとき、線材の電気抵抗値が高いほどスイ
ツチ特性として優れている。従つて、安定化材は
使用せずマトリツクスとして高電気抵抗金属、例
えばCuNiが使用されている。 スイツチ用線材は、超電導マグネツトの電源を
切り、永久電流モードに切換える際、マグネツト
コイルの始端と終端とを接続し、コイルを閉回路
にするために使用するものであり、所定の磁場に
達するまではスイツチを常電導状態にしておき、
磁場が到達後にスイツチを常電導から超電導に切
り換え、電源を切る。超電導状態になつたスイツ
チ用線材で閉回路になつたコイルには、永久電流
が流れ、磁界を維持できる。主な用途としては、
NMR磁気浮上用マグネツト等の電源を切離して
熱侵入を防ぎ、長時間磁場を保持する目的のマグ
ネツトが挙げられる。スイツチの特性は、コイル
の定格電流では安定に超電導でなければならな
い。一方、励磁時は熱で常電導状態になつている
必要がある。スイツチには、常電導の電気抵抗値
が高くSNの応答性が良好であることが必要で
あり、線材に要求される特性もまたIQ(クエンチ
電流)が高くかつ安定していること、同時に常電
導時の電気抵抗が高いこと(9−1CuNiより7−
3CuNiの方がよい)である。 ここで「クエンチ」とは、超電導コイルに電流
を流して磁界を発生する際、電磁力による導体の
移動等により局部的に発熱し、常電導領域の芽が
発生し、このようにして発生した常電導部分が急
速に伝搬して臨界電流(IC)より小さい電流で、
突然超電導状態から常電導状態に転移する現象で
ある。このように転移する際の電流値をクエンチ
電流値(IQ値)という。なお、前記臨界電流
(IC)は短尺試料(超電導線)に電流を流した際
に10-12Ωcmの電気抵抗を生じる電流として定義
される。 また、スイツチ用超電導線としては、細線化し
た素線を撚線構造にしたもの、または素線を平角
形状に成型したものが用いられている。また、一
般に超電導線の特性として臨界電流密度(Jc)を
改善するために素線に熱処理を施している。ただ
し、スイツチ用線材の特性はJcのみで決定される
ものではなく前記クエンチ電流値によつて判断し
ているものであり、この値が高いほど良好なスイ
ツチ用線材として認められている。 しかしながら、前述したような撚線構造にした
場合にはその占有率が低くなるため、例えば素線
の特性が優れていても、スイツチ用線材として十
分な性能を得ることができない。なお、占有率を
向上するために巻線後エポキシ樹脂等を含浸せし
めても、線の動きによるマグネツトのクエンチが
起こり易く、撚線による巻線としての欠点を有す
る。また、クエンチ電流は線材の表面積によつて
左右されるため、前述のように平角形状に成型し
た場合には、細線の撚線と等価のクエンチ電流値
を得ることができない。さらに、熱処理を施す場
合には、Jcを著しく向上することが困難な線材を
対象としてJcを高めようとして熱処理を行うた
め、クエンチ電流値は逆に低くなり、特性を阻害
する。 本発明は、上記従来の問題点を解決するために
なされたもので、優れたクエンチ電流値を有する
永久電流スイツチ用超電導線を提供しようとする
ものである。 [課題を解決するための手段] 本発明は、高電気抵抗金属からなるマトリツク
ス内に多数本のNbTi合金のフイラメントを埋込
んだ素線を電気絶縁銅線と共に複数本撚合せてな
る撚線を平角状成型撚線としたことを特徴とする
永久電流スイツチ用超電導線である。 前記高電気抵抗金属としては、例えばCuNi等
を用いることができる。 前記素線としては、例えば375℃〜450℃にて4
〜8日間熱処理を行つた後、10〜30%の冷間加工
を施してなるものを用いることが望ましい。前記
熱処理温度を限定した理由は、375℃未満にする
と熱処理の効果が十分に達成されず一方450℃を
越えるとクエンチ電流値(IQ値)が低下する恐れ
があるからである。 前記電気絶縁銅線は、超電導素線と共に撚り合
わされる銅線に電気絶縁被覆を施して前記超電銅
素線が常電銅状態に転移する時(スイツチをオフ
にした時)に前記超電銅素線から前記銅線にバイ
パスするのを防止するもので、前記超電導素線が
局部的な常電導状態に転移した時に発生した熱を
前記電気絶縁銅線を通して逃散させるという意味
において、安定化材としての役割の一部を担つて
いるものである。このような電気絶縁銅線として
例えば綿巻銅線、ホルマール銅線等を用いること
ができる。例えば綿巻銅線、ホルマール銅線等を
用いることができる。 [作用] 本発明によれば、高電気抵抗金属からなるマト
リツクス内に多数本のNbTi合金のフイラメント
を埋込んだ素線を安定化材として作用する電気絶
縁銅線と共に複数本撚合せことによつて、外部か
らのなんらかの影響により前記素線が局部的に超
電導状態から常電導状態に転移した場合でも、発
生した熱を前記電気絶縁銅線を通して逃散させる
ことができ、速やかに超電導状態に戻すこことが
可能となる。 また、クエンチ電流値(IQ値)の向上は素線の
細線化や等価断面積を小さくすることにより達成
される。本発明では、前記撚合せ撚線を平角状成
型撚線とすることによつて、線積率を向上できる
と共に、巻線としての密度も向上できる。 したがつて、超電導状態から常電導状態に転移
した場合でも、速やかに超電導状態に戻すここと
が可能となること、平角状成型撚線として線積率
を向上できると共に、巻線としての密度も向上で
きること、によつて高いIQ値を有する永久電流ス
イツチ用超電導線を得ることができる。 また、素線として375℃〜450℃にて4〜8日間
熱処理を行つた後、10〜30%の冷間加工を施して
なる物を用いれば、さらに高いIQ値を有する永久
電流スイツチ用超電導線を得ることができる。 [実施例] 以下、本発明の実施例を詳細に説明する。 実施例 まず、CuNi比1.6、フイラメント数4000芯の
CuNi−NbTi素線を420℃×6日間熱処理した
後、20%の冷間加工を行つて0.76mmφの素線を
作製した。つづいて、前記素線5本と綿巻き銅線
2本とを成形加工により撚合せた後、平角状に加
工して断面が1.2×2.5mmのフイラメント数4000
芯×5本の平角状成型撚線による超電導線を製造
した。 参照例 実施例と同様な素線を7本成形加工により撚合
せた後、平角状に加工して断面が1.2×2.5mmのフ
イラメント数4000芯×7本の平角状成型撚線によ
る超電導線を製造した。 比較例 断面が1.3×2.6mmの平角状超電導素線線
(CuNi比1.6、フイラメント数28000芯のCuNi−
NbTi単線)を実施例と同様に420℃×6日間熱
処理した後、20%の冷間加工を行つて超電導線を
製造した。 得られた本実施例、参照例および比較例の超電
導線を巻線加工して円筒状コイルにし、超電導磁
石により発生された磁束密度1.5テスラ(T)の
磁場中に設置した後、前記コイルに流す電流を漸
次増加させて超電導状態から常電導状態に転移す
る際の電流値(クエンチ電流値;IQ値)を測定し
た。
[Industrial Application Field] The present invention relates to improvements in superconducting wires for persistent current switches used in superconducting magnets and the like. [Prior Art and Problems] Generally, when a wire for a switch transitions from superconductivity to normal conductivity, the higher the electrical resistance value of the wire, the better the switch characteristics. Therefore, no stabilizing material is used, and a high electrical resistance metal such as CuNi is used as the matrix. The switch wire is used to connect the starting and ending ends of the magnet coil to create a closed circuit when the superconducting magnet is turned off and switched to persistent current mode, and it reaches a predetermined magnetic field. Keep the switch in normal conductivity until
After the magnetic field arrives, switch from normal conductivity to superconductivity and turn off the power. A persistent current flows through the coil, which has become a closed circuit due to the switch wire becoming superconducting, and is able to maintain a magnetic field. The main uses are:
Examples of such magnets include NMR magnetic levitation magnets, which are used to disconnect the power supply to prevent heat intrusion and maintain a magnetic field for a long time. The characteristics of the switch must be stable superconductivity at the coil's rated current. On the other hand, during excitation, it must be in a normal conductive state due to heat. The switch must have a high normal conductivity electrical resistance and good SN response, and the wire must also have a high IQ (quench current) and be stable. High electrical resistance during normal conduction (7-1 CuNi)
3CuNi is better). Here, "quench" means that when a current is passed through a superconducting coil to generate a magnetic field, heat is generated locally due to the movement of the conductor due to electromagnetic force, and the buds of the normal conductive region are generated. The normally conducting part propagates rapidly and with a current smaller than the critical current (I C ),
This is a phenomenon in which a superconducting state suddenly transitions to a normal conducting state. The current value during this transition is called the quench current value ( IQ value). Note that the critical current (I C ) is defined as a current that produces an electrical resistance of 10 -12 Ωcm when a current is passed through a short sample (superconducting wire). Further, as superconducting wires for switches, wires made of thin wires made into a twisted wire structure, or wires molded into a rectangular shape are used. Furthermore, in order to improve the critical current density (Jc), which is a characteristic of superconducting wires, the strands are generally heat treated. However, the characteristics of the switch wire are determined not only by Jc but also by the quench current value, and the higher this value, the better the switch wire is recognized. However, in the case of the above-described stranded wire structure, the occupancy rate is low, so that even if the strands have excellent characteristics, for example, sufficient performance as a wire for a switch cannot be obtained. Incidentally, even if the wire is impregnated with epoxy resin or the like after winding in order to improve the occupancy rate, the magnet is likely to be quenched due to the movement of the wire, which is a disadvantage of winding with twisted wire. Furthermore, since the quench current depends on the surface area of the wire, when the wire is formed into a rectangular shape as described above, it is not possible to obtain a quench current value equivalent to that of a thin stranded wire. Furthermore, when heat treatment is performed, the quench current value becomes low and the characteristics are impaired because the heat treatment is performed in an attempt to increase the Jc of a wire material for which it is difficult to significantly improve the Jc. The present invention was made in order to solve the above-mentioned conventional problems, and aims to provide a superconducting wire for persistent current switch having an excellent quench current value. [Means for Solving the Problem] The present invention provides a stranded wire in which a plurality of strands of NbTi alloy filament embedded in a matrix made of a high electrical resistance metal are twisted together with an electrically insulated copper wire. This is a superconducting wire for a persistent current switch, which is characterized by being a rectangular shaped stranded wire. As the high electrical resistance metal, for example, CuNi or the like can be used. For example, the wire may be heated at 375°C to 450°C
It is desirable to use a material that has been heat treated for ~8 days and then subjected to 10 to 30% cold working. The reason for limiting the heat treatment temperature is that if the heat treatment temperature is lower than 375°C, the effect of the heat treatment will not be fully achieved, whereas if it exceeds 450°C, the quench current value ( IQ value) may decrease. The electrically insulated copper wire is provided with an electrically insulating coating on the copper wire that is twisted together with the superconducting strands, so that when the superconducting copper strands transition to a normal copper state (when the switch is turned off), the superconductor Stabilization in the sense that it prevents bypass from the copper wire to the copper wire, and dissipates heat generated when the superconducting wire locally transitions to a normal conductive state through the electrically insulated copper wire. It plays a part in its role as a material. As such an electrically insulated copper wire, for example, a cotton-wound copper wire, a formal copper wire, etc. can be used. For example, cotton-wound copper wire, formal copper wire, etc. can be used. [Function] According to the present invention, a plurality of wires each having a large number of NbTi alloy filaments embedded in a matrix made of a high electrical resistance metal are twisted together with electrically insulated copper wires acting as a stabilizing material. Therefore, even if the wire locally transitions from a superconducting state to a normal conducting state due to some external influence, the generated heat can be dissipated through the electrically insulated copper wire, and the wire can quickly return to a superconducting state. becomes possible. Furthermore, the quench current value ( IQ value) can be improved by making the wire thinner and reducing the equivalent cross-sectional area. In the present invention, by forming the twisted strands into rectangular shaped strands, it is possible to improve the wire area ratio and also improve the density as a winding wire. Therefore, even when the superconducting state transitions to the normal conducting state, it is possible to quickly return to the superconducting state, and the wire area factor can be improved as a rectangular shaped stranded wire, and the density as a winding wire can also be improved. By improving the IQ value, it is possible to obtain a superconducting wire for a persistent current switch having a high IQ value. In addition, if the wire is heat-treated at 375°C to 450°C for 4 to 8 days and then subjected to 10 to 30% cold working, it can be used for persistent current switches with even higher IQ values. Superconducting wire can be obtained. [Examples] Examples of the present invention will be described in detail below. Example First, the CuNi ratio is 1.6 and the number of filaments is 4000.
After heat treating the CuNi-NbTi wire at 420°C for 6 days, cold working was performed by 20% to produce a wire with a diameter of 0.76 mm. Next, the five strands of wire and the two cotton-wrapped copper wires were twisted together by forming, and then processed into a rectangular shape, resulting in 4000 filaments with a cross section of 1.2 x 2.5 mm.
A superconducting wire made of rectangular molded stranded wire with 5 cores was manufactured. Reference example Seven strands similar to those in the example were twisted together by forming process, and then processed into a rectangular shape to produce a superconducting wire made of 7 rectangular shaped stranded wires with a cross section of 1.2 x 2.5 mm and 4000 filaments x 7. Manufactured. Comparative example Rectangular superconducting wire with a cross section of 1.3 x 2.6 mm (CuNi ratio 1.6, number of filaments 28000 CuNi−
NbTi single wire) was heat treated at 420°C for 6 days in the same manner as in the example, and then subjected to 20% cold working to produce a superconducting wire. The obtained superconducting wires of this example, reference example, and comparative example were wound into a cylindrical coil and placed in a magnetic field with a magnetic flux density of 1.5 Tesla (T) generated by a superconducting magnet. The current value (quench current value; IQ value) at the time of transition from the superconducting state to the normal conducting state was measured by gradually increasing the applied current.

【表】 前記第1表から明らかなように素線と綿巻き銅
線を撚合せ、平角状成型撚線とした本実施例の超
電導線導線は、比較例の同超電同線はもとより素
線のみを撚合せて平角状成型撚線とした参照例の
同超電導線に比べてIQ値(素線1本当り)が高
く、スイツチ用線材としてより安定であることが
わかる。 [発明の効果] 以上詳述したように、本発明によればクエンチ
電流値が著しく向上された永久電流スイツチ用超
電導線を提供することができる。
[Table] As is clear from Table 1, the superconducting wire of this example, which is made by twisting bare wires and cotton-wound copper wires and forming a rectangular stranded wire, is not only the superconducting wire of the comparative example, but also the plain wire. It can be seen that the IQ value (per strand) is higher than that of the reference superconducting wire, which is a rectangular shaped stranded wire made by twisting only the wires together, and is more stable as a wire for switches. [Effects of the Invention] As detailed above, according to the present invention, it is possible to provide a superconducting wire for a persistent current switch in which the quench current value is significantly improved.

Claims (1)

【特許請求の範囲】 1 高電気抵抗金属からなるマトリツクス内に多
数本のNbTi合金のフイラメントを埋込んだ素線
を電気絶縁銅線と共に複数本撚合せてなる撚線を
平角状成型撚線としたことを特徴とする永久電流
スイツチ用超電導線。 2 素線として375℃〜450℃にて4〜8日間熱処
理を行つた後、10〜30%の冷間加工を施してなる
ものを用いたことを特徴とする特許請求の範囲第
1項記載の永久電流スイツチ用超電導線。
[Claims] 1. A stranded wire made by twisting together a plurality of strands of NbTi alloy filaments embedded in a matrix made of a high electrical resistance metal together with an electrically insulated copper wire is called a rectangular shaped stranded wire. A superconducting wire for persistent current switches. 2. Claim 1, characterized in that the wire is heat treated at 375°C to 450°C for 4 to 8 days and then subjected to 10 to 30% cold working. superconducting wire for persistent current switches.
JP58125967A 1983-07-11 1983-07-11 Superconductive wire for permanent current switch Granted JPS6017804A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58125967A JPS6017804A (en) 1983-07-11 1983-07-11 Superconductive wire for permanent current switch

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58125967A JPS6017804A (en) 1983-07-11 1983-07-11 Superconductive wire for permanent current switch

Publications (2)

Publication Number Publication Date
JPS6017804A JPS6017804A (en) 1985-01-29
JPH0479083B2 true JPH0479083B2 (en) 1992-12-15

Family

ID=14923405

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58125967A Granted JPS6017804A (en) 1983-07-11 1983-07-11 Superconductive wire for permanent current switch

Country Status (1)

Country Link
JP (1) JPS6017804A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE3623609C1 (en) * 1986-07-12 1988-01-21 Didier Werke Ag Gas purging device
JPS6356963U (en) * 1986-09-30 1988-04-16
JPH0613254Y2 (en) * 1988-08-03 1994-04-06 川崎炉材株式会社 Molten metal agitator

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6020856B2 (en) * 1977-03-11 1985-05-24 古河電気工業株式会社 Stabilized composite superconducting cable and its manufacturing method
JPS55136408A (en) * 1979-04-12 1980-10-24 Furukawa Electric Co Ltd Method of manufacturing superconductive wire
JPS56112012A (en) * 1980-02-12 1981-09-04 Furukawa Electric Co Ltd Superconductive twisted wire
JPS60810U (en) * 1983-06-16 1985-01-07 昭和電線電纜株式会社 Superconducting stranded wire for persistent current switch

Also Published As

Publication number Publication date
JPS6017804A (en) 1985-01-29

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