JPH07192547A - Composite multi-core superconducting wire - Google Patents

Composite multi-core superconducting wire

Info

Publication number
JPH07192547A
JPH07192547A JP5332612A JP33261293A JPH07192547A JP H07192547 A JPH07192547 A JP H07192547A JP 5332612 A JP5332612 A JP 5332612A JP 33261293 A JP33261293 A JP 33261293A JP H07192547 A JPH07192547 A JP H07192547A
Authority
JP
Japan
Prior art keywords
matrix
composite
superconducting wire
volume ratio
filament
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
JP5332612A
Other languages
Japanese (ja)
Inventor
Katsunori Wada
克則 和田
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
Original Assignee
Furukawa Electric Co 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 Furukawa Electric Co Ltd filed Critical Furukawa Electric Co Ltd
Priority to JP5332612A priority Critical patent/JPH07192547A/en
Publication of JPH07192547A publication Critical patent/JPH07192547A/en
Pending 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)

Abstract

PURPOSE:To manufacture a composite multiconductor superconductive wire useful to an application wherein a small diameter or light weight is required by specifying the volume ratio of a local matrix to a superconductive filament and the volume ratio of the total of the local matrix to the superconductive filament and a stabilizing matrix. CONSTITUTION:A composite multiconductor superconductive wire 4 is formed which consists of a coexistent part 1, composed of a local matrix, arranged in the outer periphery of each superconductive filament, and a superconductive filament; and a stabilizing matrix 2 arranged in the periphery of the coexistent part 1. The local matrix and the stabilizing matrix 2 are composed of high- purity copper, the volume ratio of the local matrix to the superconductive filament is made 0.35 or less, and the volume ratio of a whole matrix composed of the total of the local matrix to the superconductive filament and the stabilizing matrix 2 is made 1.5 or less. This can provide a composite multiconductor superconductive electric wire 4 capable of coping with application wherein a small diameter or light weight is required.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は高純度銅をマトリックス
とし、多数の超電導フィラメントが埋め込まれた複合多
芯超電導線に関し、更に詳しくは細径化や軽量化が要求
される磁気浮上列車用等の用途に対応できる複合多芯超
電導線に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a composite multifilamentary superconducting wire in which a large number of superconducting filaments are embedded using high-purity copper as a matrix, and more specifically, for a magnetic levitation train in which a diameter reduction and a weight reduction are required. The present invention relates to a composite multifilamentary superconducting wire that can be used for various purposes.

【0002】[0002]

【従来の技術】複合多芯超電導線は純銅や銅合金等をマ
トリックスとして、NbTi等からなる極細超電導フィ
ラメントが多数埋め込まれた構造になっている。交流用
特殊用途に使われる複合多芯超電導線の場合、交流損失
の低減の観点から上記マトリックスに高電気抵抗の銅合
金が使用されることもあるが、それ以外の通常の場合は
電気抵抗や熱抵抗が低い純銅が使われる。これは複合多
芯超電導線の通電時の電気的、熱的安定性を向上させる
ためである。
2. Description of the Related Art A composite multifilamentary superconducting wire has a structure in which a large number of ultrafine superconducting filaments made of NbTi or the like are embedded in a pure copper or copper alloy matrix. In the case of a composite multicore superconducting wire used for a special purpose for alternating current, a copper alloy with high electrical resistance may be used for the above matrix from the viewpoint of reducing AC loss, but in other normal cases, electrical resistance or Pure copper with low thermal resistance is used. This is to improve the electrical and thermal stability of the composite multicore superconducting wire during energization.

【0003】一般に複合多芯超電導線は、各々の超電導
フィラメントがその外周に配置されたローカルマトリッ
クスの中に埋め込まれた共存部と、その共存部の外周や
内周等に配置された安定化マトリックスとからなってい
る。図1を参照しながら説明すると、複合多芯超電導線
4は、超電導フィラメントがローカルマトリックスであ
る純銅に埋め込まれた超電導フィラメント/純銅共存部
1の外周に安定化純銅層2が設けられている。また図1
に示すように、熱的安定性等を向上させるために必要に
応じて安定化純銅芯3が配置される場合もある。
In general, a composite multicore superconducting wire has a coexisting portion in which each superconducting filament is embedded in a local matrix and a stabilizing matrix arranged on the outer or inner periphery of the coexisting portion. It consists of Explaining with reference to FIG. 1, the composite multicore superconducting wire 4 has a stabilized pure copper layer 2 provided on the outer periphery of a superconducting filament / pure copper coexisting portion 1 in which a superconducting filament is embedded in pure copper as a local matrix. See also FIG.
As shown in FIG. 5, a stabilized pure copper core 3 may be arranged as needed in order to improve thermal stability and the like.

【0004】[0004]

【発明が解決しようとする課題】最近、磁気浮上列車用
等に使用される超電導コイルでは、その小型軽量化のた
めに複合多芯超電導線の細径化や軽量化が要求されてい
る。従来、複合多芯超電導線の電気的、熱的安定性を向
上させるためには、複合多芯超電導線におけるマトリッ
クスの体積比を高めることが行われてきたが、マトリッ
クスの体積比を高めると、当然複合多芯超電導線の径が
太くなり、重量も大きくなる問題があった。
Recently, in a superconducting coil used for a magnetic levitation train or the like, it has been required to reduce the diameter and weight of a composite multicore superconducting wire in order to reduce its size and weight. Conventionally, in order to improve the electrical and thermal stability of the composite multi-core superconducting wire, the volume ratio of the matrix in the composite multi-core superconducting wire has been increased, but if the volume ratio of the matrix is increased, Naturally, there was a problem that the diameter of the composite multifilamentary superconducting wire became thick and the weight also became large.

【0005】このためマトリックスである純銅の純度を
高めたり、加工歪みを可能な限り除去する等、マトリッ
クスの電気抵抗、熱抵抗を低めることで、マトリックス
の体積比を低める努力がなされていた。なお通常、マト
リックス(純銅)の電気抵抗は、温度300Kでの抵抗
値を10Kでの抵抗値で割った値(RRRと称される)
で表現され、現状では磁気浮上列車用等の用途には、マ
トリックスの体積比が1.5以下の場合、RRR≧20
0が要求されている。
For this reason, efforts have been made to lower the volume ratio of the matrix by lowering the electrical resistance and thermal resistance of the matrix, such as increasing the purity of pure copper as the matrix and removing processing strain as much as possible. The electrical resistance of the matrix (pure copper) is usually a value obtained by dividing the resistance value at a temperature of 300K by the resistance value at a temperature of 10K (referred to as RRR).
Currently, for applications such as magnetic levitation trains, when the volume ratio of the matrix is 1.5 or less, RRR ≧ 20.
0 is required.

【0006】しかしながら、初期RRRが400程度の
高純度銅を用いて複合多芯超電導線を製造しても、延伸
加工等による加工歪みがマトリックス中に残り、焼鈍を
行ってもRRRが250程度まで低下してしまうことが
避けられない。加えてローカルマトリックスの場合、肉
厚が極めて薄くなっているため、この肉厚がある程度ま
で薄くなると電子の平均自由工程の関係で前記RRRが
250にも至らず、実質的に肉厚(μm)の23.6倍
程度の値にしかならないことが知られている。従って各
々の超電導フィラメントがローカルマトリックスの中に
埋め込まれた共存部においては、該ローカルマトリック
スのRRRは小さいものになってしまう。
However, even if a composite multifilamentary superconducting wire is manufactured by using high-purity copper having an initial RRR of about 400, a processing strain due to a drawing process or the like remains in the matrix, and even if annealing is performed, the RRR is up to about 250. It is inevitable that it will drop. In addition, in the case of the local matrix, the wall thickness is extremely thin. Therefore, when the wall thickness becomes thin to some extent, the RRR does not reach 250 due to the mean free path of electrons, and the wall thickness (μm) is substantially reduced. It is known that the value is only about 23.6 times. Therefore, in the coexistence part where each superconducting filament is embedded in the local matrix, the RRR of the local matrix becomes small.

【0007】従って、例え初期RRRが同程度の高純度
銅を用いて複合多芯超電導線を製造しても、製造後のロ
ーカルマトリックスと安定化マトリックスのRRRは異
ったものになる。従ってその配分比により複合多芯超電
導線を構成するマトリックス全体のRRRが左右される
のである。なお複合多芯超電導線を構成するマトリック
ス全体のRRRとは、理論的にはマトリックスの各部位
の体積分率とその部位でのRRRを掛けた値の総和であ
るが、実際には測定によって求められる値である。複合
多芯超電導線の安定性の観点では、前述したマトリック
ス全体のRRRがなるべく高くなることが望ましいが、
現状ではこのRRRに影響する前記配分比は経験によっ
て決められており、複合多芯超電導線の細径化(軽量
化)とRRRの高いレベルでの両立ができていなかっ
た。
Therefore, even if a composite multicore superconducting wire is manufactured using high-purity copper having an initial RRR of the same level, the RRRs of the local matrix and the stabilizing matrix after manufacture are different. Therefore, the distribution ratio influences the RRR of the entire matrix forming the composite multicore superconducting wire. The RRR of the entire matrix that constitutes the composite multicore superconducting wire is theoretically the sum of the volume fraction of each part of the matrix and the RRR at that part, but it is actually obtained by measurement. It is a value that can be. From the viewpoint of stability of the composite multi-core superconducting wire, it is desirable that the RRR of the entire matrix described above is as high as possible.
At present, the distribution ratio that affects the RRR is determined by experience, and it has not been possible to achieve both a reduction in diameter (weight reduction) of the composite multicore superconducting wire and a high level of RRR.

【0008】[0008]

【課題を解決するための手段】本発明はかかる状況に鑑
み、鋭意研究を行った結果なされたもので、その目的
は、磁気浮上列車用等の用途に対応できるように、複合
多芯超電導線の細径化(軽量化)とRRR(200以
上)の高いレベルでの両立を可能とする複合多芯超電導
線を提供しようとするものである。即ち、各々の超電導
フィラメントの外周に配置されたローカルマトリックス
と超電導フィラメントとからなる共存部と、該共存部の
周囲に配置された安定化マトリックスとからなる複合多
芯超電導線において、前記ローカルマトリックスと前記
安定化マトリックスが高純度銅からなっており、また前
記超電導フィラメントに対する前記ローカルマトリック
スの体積比が0.35以下でかつ前記超電導フィラメン
トに対する、前記ローカルマトリックスと前記安定化マ
トリックスの合計からなるマトリックス全体の体積比が
1.5以下であることを特徴とする複合多芯超電導線で
ある。
SUMMARY OF THE INVENTION The present invention has been made as a result of intensive studies in view of such a situation, and its purpose is to provide a composite multicore superconducting wire so as to be applicable to applications such as magnetic levitation trains. It is an object of the present invention to provide a composite multi-core superconducting wire capable of achieving both a reduction in diameter (reduction in weight) and a high level of RRR (200 or more). That is, in a composite multi-core superconducting wire consisting of a coexisting portion composed of a local matrix and a superconducting filament arranged on the outer periphery of each superconducting filament, and a stabilizing matrix arranged around the coexisting portion, the local matrix is The stabilizing matrix is made of high-purity copper, and the volume ratio of the local matrix to the superconducting filament is 0.35 or less, and the whole matrix composed of the total of the local matrix and the stabilizing matrix to the superconducting filament. Is a composite multifilamentary superconducting wire having a volume ratio of 1.5 or less.

【0009】[0009]

【作用】本発明の複合多芯超電導線は、磁気浮上列車用
等の用途に対応できるように、複合多芯超電導線の細径
化(軽量化)を実現するため、前記ローカルマトリック
スと前記安定化マトリックスの合計からなるマトリック
ス全体の前記超電導フィラメントに対する体積比は1.
5以下となっている。この体積比が1.5を越えると、
複合多芯超電導線が太く重量も大きくなるため、軽量小
型化が求められる磁気浮上列車用等の用途には対応でき
ない。
The composite multifilamentary superconducting wire of the present invention realizes the diameter reduction (weight reduction) of the composite multifilamentary superconducting wire so that it can be used for applications such as magnetic levitation trains. The volume ratio of the entire matrix consisting of the totalized matrix to the superconducting filament is 1.
It is 5 or less. If this volume ratio exceeds 1.5,
Since the composite multifilamentary superconducting wire is thick and heavy, it cannot be applied to applications such as magnetic levitation trains, which are required to be lightweight and compact.

【0010】このようにマトリックス全体と超電導フィ
ラメントの合計の体積比を1.5以下にするという制限
の下では、複合多芯超電導線を構成するマトリックス全
体のRRRを高いレベル(200以上)にすることが難
しい。本発明は、薄肉化してRRRが小さくなったロー
カルマトリックスの体積比を0.35と小さい配分にす
ることで、マトリックス全体のRRRが200以上の複
合多芯超電導線を実現したものである。なおローカルマ
トリックスの体積比は製造上0.2〜0.35であるこ
とが望ましい。0.2以下であると、延伸加工中に超電
導フィラメントが露出する可能性が大きくなるからであ
る。
Under the limitation that the total volume ratio of the entire matrix and the superconducting filament is 1.5 or less, the RRR of the entire matrix constituting the composite multicore superconducting wire is set to a high level (200 or more). Difficult to do. The present invention realizes a composite multifilamentary superconducting wire having an RRR of 200 or more in the entire matrix by reducing the volume ratio of the local matrix having a reduced RRR and a reduced RRR to 0.35. The volume ratio of the local matrix is preferably 0.2 to 0.35 in terms of manufacturing. If it is 0.2 or less, the possibility that the superconducting filament will be exposed during the drawing process increases.

【0011】[0011]

【実施例】次に本発明を実施例により詳細に説明する。
先ずNbTi棒を1次高純度銅シースに挿入し、これを
延伸加工して1次複合素線を作製した。この1次高純度
銅シースを形成する高純度銅の初期(加工前)のRRR
は400であった。この1次素線を2次高純度銅シース
に1550本充填した後、延伸加工と焼鈍をして複合多
芯超電導線(径1.67mm)を製造した。この2次高
純度銅シースを形成する高純度銅の初期(加工前)のR
RRは480であった。
EXAMPLES The present invention will now be described in detail with reference to Examples.
First, a NbTi rod was inserted into a primary high-purity copper sheath, and this was drawn to prepare a primary composite strand. Initial (before processing) RRR of high-purity copper that forms this primary high-purity copper sheath
Was 400. After filling 1550 secondary high-purity copper sheaths with this primary strand, drawing and annealing were performed to produce a composite multicore superconducting wire (diameter 1.67 mm). The initial (before processing) R of the high-purity copper that forms this secondary high-purity copper sheath
The RR was 480.

【0012】製造した複合多芯超電導線の断面を顕微鏡
で観察して、NbTiフィラメントの平均径と、このN
bTiフィラメントに対するローカルマトリックス(上
記1次高純度銅シースが加工された部分である)の体積
比(ローカルマトリックスの体積比と称する)を測定し
た。なお、前記体積比は実質的には複合多芯超電導線の
断面における面積比と同一である。またNbTiフィラ
メントに対する安定化マトリックス(上記2次高純度シ
ースが加工された部分である)の体積比(安定化マトリ
ックスの体積比と称する)を測定した。製造した複合多
芯超電導線は2種類(本発明例と比較例)で、上記2つ
の体積比とその合計値(マトリックス全体の体積比と称
する)、およびNbTiフィラメントの平均径を表1に
示す。
The cross section of the produced composite multifilamentary superconducting wire was observed with a microscope, and the average diameter of the NbTi filaments and the N
The volume ratio (referred to as the volume ratio of the local matrix) of the local matrix (the portion where the primary high-purity copper sheath was processed) to the bTi filament was measured. The volume ratio is substantially the same as the area ratio in the cross section of the composite multicore superconducting wire. Further, the volume ratio of the stabilizing matrix (the portion where the secondary high-purity sheath is processed) to the NbTi filament (referred to as the stabilizing matrix volume ratio) was measured. There are two types of composite multifilamentary superconducting wires produced (inventive example and comparative example), and the above two volume ratios and their total values (referred to as the volume ratio of the entire matrix) and the average diameter of the NbTi filaments are shown in Table 1. .

【0013】[0013]

【表1】 [Table 1]

【0014】製造した複合多芯超電導線のマトリックス
全体のRRRを測定した。結果を表1に併記する。表1
によると、ローカルマトリックスの体積比が0.5であ
る比較例はマトリックス全体のRRRが170となった
のに対し、本発明例では220となり、本発明は高いR
RRが実現したことが判った。
The RRR of the entire matrix of the manufactured composite multifilamentary superconducting wire was measured. The results are also shown in Table 1. Table 1
According to the above, in the comparative example in which the volume ratio of the local matrix is 0.5, the RRR of the whole matrix was 170, while in the example of the present invention, it was 220, and the present invention showed high R
It turned out that RR was realized.

【0015】[0015]

【効果】以上詳述したように、本発明による複合多芯超
電導線は、マトリックス全体の体積比が小さく、細径化
(軽量化)したものであるが、マトリックス全体のRR
Rが200以上と高く、細径化(軽量化)とRRRの高
いレベルでの両立を実現したものである。このため本発
明の複合多芯超電導線は磁気浮上列車用等、細径化と軽
量化が要求される用途に対応できる等、工業上著しい貢
献をなすものである。
As described in detail above, the composite multifilamentary superconducting wire according to the present invention has a small volume ratio of the whole matrix and a small diameter (light weight).
It has a high R of 200 or more, and achieves both a small diameter (light weight) and a high level of RRR. Therefore, the composite multifilamentary superconducting wire of the present invention makes a significant industrial contribution, for example, for magnetic levitation trains and in other applications requiring a smaller diameter and lighter weight.

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

【図1】超電導フィラメントがマトリックスに埋め込ま
れた複合多芯超電導線の一例を示す説明図である。
FIG. 1 is an explanatory diagram showing an example of a composite multicore superconducting wire in which a superconducting filament is embedded in a matrix.

【符号の説明】[Explanation of symbols]

1 超電導フィラメント/純銅共存部 2 安定化純銅層 3 安定化純銅芯 4 複合多芯超電導線 1 Superconducting filament / pure copper coexistence part 2 Stabilized pure copper layer 3 Stabilized pure copper core 4 Composite multi-core superconducting wire

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】 各々の超電導フィラメントの外周に配置
されたローカルマトリックスと超電導フィラメントとか
らなる共存部と、該共存部の周囲に配置された安定化マ
トリックスとからなる複合多芯超電導線において、前記
ローカルマトリックスと前記安定化マトリックスが高純
度銅からなっており、また前記超電導フィラメントに対
する前記ローカルマトリックスの体積比が0.35以下
でかつ前記超電導フィラメントに対する、前記ローカル
マトリックスと前記安定化マトリックスの合計からなる
マトリックス全体の体積比が1.5以下であることを特
徴とする複合多芯超電導線。
1. A composite multi-core superconducting wire comprising a coexisting portion composed of a local matrix and a superconducting filament arranged on the outer periphery of each superconducting filament, and a stabilizing matrix arranged around the coexisting portion, The local matrix and the stabilizing matrix are made of high-purity copper, and the volume ratio of the local matrix to the superconducting filament is 0.35 or less and the total of the local matrix and the stabilizing matrix to the superconducting filament. The composite multicore superconducting wire, wherein the volume ratio of the entire matrix is 1.5 or less.
JP5332612A 1993-12-27 1993-12-27 Composite multi-core superconducting wire Pending JPH07192547A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5332612A JPH07192547A (en) 1993-12-27 1993-12-27 Composite multi-core superconducting wire

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5332612A JPH07192547A (en) 1993-12-27 1993-12-27 Composite multi-core superconducting wire

Publications (1)

Publication Number Publication Date
JPH07192547A true JPH07192547A (en) 1995-07-28

Family

ID=18256897

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5332612A Pending JPH07192547A (en) 1993-12-27 1993-12-27 Composite multi-core superconducting wire

Country Status (1)

Country Link
JP (1) JPH07192547A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008147175A (en) * 2006-11-14 2008-06-26 Furukawa Electric Co Ltd:The NbTi superconducting multi-core wire for pulse and NbTi superconducting molded stranded wire for pulse

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60101813A (en) * 1983-11-08 1985-06-05 昭和電線電纜株式会社 Method of producing superconductive wire
JPH05198224A (en) * 1992-01-20 1993-08-06 Hitachi Cable Ltd Nb-Ti alloy superconducting wire

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS60101813A (en) * 1983-11-08 1985-06-05 昭和電線電纜株式会社 Method of producing superconductive wire
JPH05198224A (en) * 1992-01-20 1993-08-06 Hitachi Cable Ltd Nb-Ti alloy superconducting wire

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2008147175A (en) * 2006-11-14 2008-06-26 Furukawa Electric Co Ltd:The NbTi superconducting multi-core wire for pulse and NbTi superconducting molded stranded wire for pulse

Similar Documents

Publication Publication Date Title
US3910802A (en) Stabilized superconductors
JPH02276111A (en) Compound superconductor and its manufacture
JP2013062239A (en) Nb3Sn SUPERCONDUCTING WIRE AND METHOD FOR MANUFACTURING THE SAME
JP4676699B2 (en) Method for manufacturing superconducting wire
US4094059A (en) Method for producing composite superconductors
JPH07192547A (en) Composite multi-core superconducting wire
JP3754522B2 (en) Nb (3) Sn superconducting wire
JP2876667B2 (en) Aluminum stabilized superconducting wire
JP2008147175A (en) NbTi superconducting multi-core wire for pulse and NbTi superconducting molded stranded wire for pulse
JP2005141968A (en) Compound superconducting wire material and its manufacturing method
JP2742436B2 (en) Method for producing compound superconducting stranded wire
JPH0589726A (en) Nbyi superconductive wire
JP2878390B2 (en) Method of manufacturing Nb (3) Sn superconducting wire for superconducting generator
JPH0982149A (en) Nb3sn superconducting wire excellent in strength and workability
JP2004152677A (en) High-strength superconducting wire rod
JPH04132108A (en) Nb3al superconductor
JP2719155B2 (en) Superconducting stranded wire manufacturing method
JPH0146963B2 (en)
JP2749136B2 (en) Aluminum stabilized superconducting wire
JP3143908B2 (en) Superconducting conductor
JPH08212847A (en) Composite multi-core superconducting wire
JPH09129043A (en) Nb3Al-based multicore superconducting wire
JPH07176222A (en) Nb3X series superconducting wire
JPH02103811A (en) Compound superconducting wire
JPH05182536A (en) Superconductor and stabilizing member used therein