JPH0313686B2 - - Google Patents

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Publication number
JPH0313686B2
JPH0313686B2 JP56079590A JP7959081A JPH0313686B2 JP H0313686 B2 JPH0313686 B2 JP H0313686B2 JP 56079590 A JP56079590 A JP 56079590A JP 7959081 A JP7959081 A JP 7959081A JP H0313686 B2 JPH0313686 B2 JP H0313686B2
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JP
Japan
Prior art keywords
wire
diameter
composite
plating
alloy
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
JP56079590A
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Japanese (ja)
Other versions
JPS57194404A (en
Inventor
Tsukasa Kono
Yoshimitsu Ikeno
Nobuyuki Sadakata
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.)
Fujikura Ltd
Original Assignee
Fujikura Ltd
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Priority to JP56079590A priority Critical patent/JPS57194404A/en
Publication of JPS57194404A publication Critical patent/JPS57194404A/en
Publication of JPH0313686B2 publication Critical patent/JPH0313686B2/ja
Granted legal-status Critical Current

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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

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  • Superconductors And Manufacturing Methods Therefor (AREA)
  • Non-Insulated Conductors (AREA)

Description

【発明の詳細な説明】 この発明はNb3Sn系の極細多芯超電導線を製造
する方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing an Nb 3 Sn-based ultrafine multifilamentary superconducting wire.

金属間化合物系の超電導材料としては、Nb3Sn
のほか、Nb3Ga,Nb3Ge,Nb3Al,V3Ga等が知
られている。この種の金属間化合物系超電導材料
は一般的に超電導特性の点からは合金系超電導材
料よりも優れているが、その反面加工性、特に展
性や延性が低い問題があり、そのため超電導金属
間化合物の棒材等を加工することは困難であるか
ら、未だ金属間化合物となつていない複合状態で
加工を加え、その加工後に拡散熱処理を加えて金
属間化合物を生成させるのが通常である。
As an intermetallic compound-based superconducting material, Nb 3 Sn
Besides, Nb 3 Ga, Nb 3 Ge, Nb 3 Al, V 3 Ga, etc. are known. This type of intermetallic compound-based superconducting material is generally superior to alloy-based superconducting materials in terms of superconducting properties, but on the other hand, it has problems with workability, particularly low malleability and ductility, and therefore Since it is difficult to process compounds such as rods, it is common to process them in a composite state that has not yet become an intermetallic compound, and then apply diffusion heat treatment after that process to generate an intermetallic compound.

ところで従来の金属間化合物系の極細多芯超電
導線の製造方法について、代表的なNb3Sn系の極
細多芯超電導線の場合を例にとつて説明すると、
従来の方法はブロンズ法とSnメツキ法とに大別
される。前者のブロンズ法は、第1図に示すよう
に、望ましくは10〜15wt%程度のSn濃度を有す
るCu−Sn合金(ブロンズ)の基地1中に多数の
Nbフイラメント2を配して所定の線径の極細多
芯複合線を作り、その後拡散熱処理を施してCu
−Sn合金基地1中のSnを拡散させて多数の
Nb3Snフイラメントを有する極細多芯Nb3Sn系超
電導線を得る方法であり、また後者のSnメツキ
法は第2図に示すように純Cuの基地3中に多数
のNbフイラメント2を配して所定の線径とした
後、Cu基地の外周上にSnメツキ4を施し、その
後拡散熱処理を施して外側のSnメツキ層4から
Cu基地3を介してSnを拡散させて前記同様な極
細多芯Nb3Sn超電導線を製造する方法である。し
かしながら従来のこれらの方法はそれぞれ一長一
短があり、いずれも満足すべきものでないのが実
情である。
By the way, the conventional method for manufacturing intermetallic compound-based ultrafine multicore superconducting wires will be explained using a typical Nb 3 Sn-based ultrafine multicore superconducting wire as an example.
Conventional methods are broadly divided into the bronze method and the Sn plating method. As shown in Fig. 1, the former bronze method involves forming a large number of Cu-Sn alloys (bronze) in a base 1 of Cu-Sn alloy (bronze), which preferably has an Sn concentration of about 10 to 15 wt%.
Nb filament 2 is arranged to make an ultra-fine multicore composite wire with a predetermined wire diameter, and then diffusion heat treatment is applied to Cu.
− Diffusion of Sn in the Sn alloy base 1 to create a large number of
This is a method for obtaining ultrafine multicore Nb 3 Sn superconducting wires having Nb 3 Sn filaments, and the latter Sn plating method involves arranging a large number of Nb filaments 2 in a base 3 of pure Cu, as shown in Figure 2. After adjusting the wire diameter to a predetermined wire diameter, Sn plating 4 is applied on the outer periphery of the Cu base, and then diffusion heat treatment is performed to remove the wire from the outer Sn plating layer 4.
This is a method of manufacturing an ultrafine multicore Nb 3 Sn superconducting wire similar to that described above by diffusing Sn through the Cu base 3. However, each of these conventional methods has advantages and disadvantages, and the reality is that none of them is satisfactory.

すなわち、前者のブロンズ法にあつては比較的
簡単な熱処理でNb3Snを生成させることができ、
しかもSnメツキ処理を必要としない等の長所を
有するが、その反面、縮径加工における加工性に
劣る重大な問題がある。すなわちブロンズ法にお
いては充分な量のNb3Snを生成させるためには
Sn濃度が10〜15%程度と相当に高いCu−Sn合金
を基地として用いる必要があるが、このような
Sn濃度が高いCu−Sn合金では加工硬化がきわめ
て生じ易く、そのため中間焼鈍を頻繁に行なわな
ければならず、特に極細多芯超電導線の製造にお
いては1本のNb芯材の径が数μm程度のフイラメ
ントとなるまで縮径加工を行なわなければならな
いため焼鈍回数が著しく多くなり、そのため作業
工数が著しく多くなつて生産性が著しく低下する
問題がある。これに対し後者のSnメツキ法にあ
つては、基地として加工性が良好な純銅を用いて
いるため縮径加工における焼鈍回数はブロンズ法
と比較して著しく少なくすることが可能である
が、その反面、充分な量のNb3Snを生成させるた
めには相当に厚いSnメツキ層を必要とし、この
ような厚いメツキ層を生成させるためにはメツキ
に相当な長時間を要し、しかもメツキ厚みの制御
が困難となる問題があり、またこの方法では
Nb3Snを生成させるためのSnがNbフイラメント
から相当に離れていて、長い拡散距離を必要とす
るため、Nb3Snの生成効率を高めるためには拡散
熱処理に長時間を要し、しかもその熱処理条件も
種々の工夫をする必要があるほか、熱処理時に外
周上のSnが溶け落ちたり、下側に廻り込んだり
する不都合が生じる。このようなSnメツキ法の
欠点は特に太径の極細多芯Nb3Sn系超電導線を製
造する場合に顕著となる。すなわち線径が太くな
ればそれに伴つて多量のSnを必要とするように
なるためSnメツキ層の厚みを著しく厚くする必
要が生じ、また中心部のNbフイラメントとSnメ
ツキ層との間の距離が大きくなつてSnの拡散移
動すべき距離が長くなり、そのため多量のSnを
長い距離拡散移動させて充分な量のNb3Snを生成
させるためには、通常の拡散熱処理の前に予備熱
処理を必要とし、しかもその予備熱処理を数段階
に行なわなければならない等の不都合が生じる。
そしてまたこのような予備熱処理の間にはSnリ
ツチな脆いCu−Sn系金属間化合物が生成されて
しまつて、特性を低下させるおそれもある。さら
にSnメツキ法の最大の欠点は、後に詳細に説明
するように、最外周に安定化のための純銅を配し
てその内側に拡散障壁(バリヤ)を設ける所謂安
定化銅付きの超電導線の製造に適用できないこと
である。
In other words, in the former bronze method, Nb 3 Sn can be produced by relatively simple heat treatment,
Moreover, it has advantages such as not requiring Sn plating, but on the other hand, it has a serious problem of poor workability in diameter reduction processing. In other words, in the bronze method, in order to generate a sufficient amount of Nb 3 Sn,
It is necessary to use a Cu-Sn alloy with a fairly high Sn concentration of about 10 to 15% as a base;
Work hardening is extremely likely to occur in Cu-Sn alloys with a high Sn concentration, so intermediate annealing must be performed frequently.Especially in the production of ultrafine multifilamentary superconducting wires, the diameter of one Nb core material is approximately several μm. Since diameter reduction processing must be performed until the filament becomes a filament, the number of annealing operations is significantly increased, resulting in a significant increase in the number of work steps and a problem in that productivity is significantly reduced. On the other hand, in the latter Sn plating method, since pure copper with good workability is used as the base, the number of annealing times during diameter reduction processing can be significantly reduced compared to the bronze method. On the other hand, in order to generate a sufficient amount of Nb 3 Sn, a fairly thick Sn plating layer is required, and in order to generate such a thick plating layer, plating requires a considerable amount of time, and the plating thickness is There is a problem that it is difficult to control the
Sn to generate Nb 3 Sn is quite far away from the Nb filament and requires a long diffusion distance. In addition to the need to make various adjustments to the heat treatment conditions, there is also the problem that Sn on the outer periphery melts down or sneaks into the bottom during heat treatment. Such drawbacks of the Sn plating method become particularly noticeable when manufacturing ultrafine multicore Nb 3 Sn superconducting wires with large diameters. In other words, as the wire diameter becomes thicker, a larger amount of Sn is required, so the thickness of the Sn plating layer needs to be significantly thicker, and the distance between the Nb filament in the center and the Sn plating layer increases. As the size increases, the distance that Sn must diffuse and move becomes longer, so in order to diffuse and move a large amount of Sn over a long distance and generate a sufficient amount of Nb 3 Sn, preliminary heat treatment is required before normal diffusion heat treatment. However, there are disadvantages in that the preliminary heat treatment must be carried out in several stages.
Moreover, during such preliminary heat treatment, a brittle Sn-rich Cu-Sn intermetallic compound is generated, which may deteriorate the properties. Furthermore, the biggest drawback of the Sn plating method, as will be explained in detail later, is that it is a superconducting wire with stabilized copper, in which pure copper is placed on the outermost periphery for stabilization and a diffusion barrier is placed inside. This cannot be applied to manufacturing.

上述のような問題を解決するため、本発明者等
は既にブロンズ法とSnメツキ法を組合せた改良
方法を提案している。その改良方法の第1は、前
述のSnメツキ法における純銅基地1(第2図参
照)の代りに10wt%未満の低Sn濃度のCu−Sn合
金基地を用い、その低Sn濃度のCu−Sn合金基地
中に多数のNbフイラメントを配し、所定の線径
まで縮径した後、その外周面にSnメツキを施す
方法である。また第2の改良方法は、第3図に示
すようにCu−Sn合金基地5中に多数のNbフイラ
メント2を配すと共に前記Cu−Sn合金基地5の
周囲に純銅6を配して、所定の線径まで縮径した
後、その外周面にSnメツキ4を施し、その後前
記同様に拡散熱処理を施す方法である。さらに第
3の改良方法は、第4図に示すように従来のブロ
ンズ法と同程度の高Sn濃度のCu−Sn合金基地7
中に多数のNbフイラメント2を配してその高Sn
濃度Cu−Sn合金基地7の周囲に低Sn濃度のCu−
Sn合金基地8を配し、所定の線径まで縮径した
後、その外周面に薄いSnメツキ4を施し、その
後前記同様に拡散熱処理を施す方法である。
In order to solve the above-mentioned problems, the present inventors have already proposed an improved method that combines the bronze method and the Sn plating method. The first improvement method is to use a Cu-Sn alloy base with a low Sn concentration of less than 10wt% in place of the pure copper base 1 (see Figure 2) in the Sn plating method described above, and use the Cu-Sn alloy base with a low Sn concentration of less than 10 wt%. This is a method in which a large number of Nb filaments are arranged in an alloy matrix, the diameter is reduced to a predetermined diameter, and then Sn plating is applied to the outer peripheral surface of the filament. A second improvement method is to arrange a large number of Nb filaments 2 in a Cu-Sn alloy base 5 and to arrange pure copper 6 around the Cu-Sn alloy base 5, as shown in FIG. After reducing the wire diameter to a wire diameter of , Sn plating 4 is applied to the outer circumferential surface of the wire, and then diffusion heat treatment is performed in the same manner as described above. Furthermore, the third improvement method is a Cu-Sn alloy base 7 with a high Sn concentration comparable to that of the conventional bronze method, as shown in Figure 4.
A large number of Nb filaments 2 are placed inside the
A low Sn concentration Cu-
In this method, a Sn alloy base 8 is arranged, the wire diameter is reduced to a predetermined wire diameter, a thin Sn plating 4 is applied to the outer circumferential surface of the wire, and then a diffusion heat treatment is performed in the same manner as described above.

これらの改良方法は、前記ブロンズ法と比較す
れば相対的に縮径加工が容易で縮径加工中の焼鈍
回数が比較的少なくて済み、また前記Snメツキ
法と比較すればSnメツキ工程およびNb3Snの生
成のための熱処理工程が比較的簡単となるが、い
ずれも未だ充分に満足できる程度には至つていな
い。すなわち前記第1の改良方法では基地として
加工性が比較的良好な低Sn濃度のCu−Sn合金を
用い、また第2の改良方法では望ましくは低Sn
濃度のCu−Sn合金基地の外側に加工性が良好な
Cuを被せているため、いずれも前記ブロンズ法
の場合よりは加工性が良好となつて焼鈍回数が少
なくて済むが、ある程度の厚みのSnメツキ層を
形成する必要があり、その場合太径となれば外側
のSnメツキ層中のSnを充分に拡散させるために
はブロンズ法の場合よりも充分な熱処理を行う必
要がある。また第3の改良方法では加工性が劣る
高Sn濃度のCu−Sn合金基地の上に比較的加工性
が良好な低Sn濃度のCu−Sn合金を被せてはいる
が、従来の単なるブロンズ法の場合と比較してわ
ずかしか加工性は良好とならず、したがつて焼鈍
回数もさほど減少しない。
Compared to the bronze method mentioned above, these improved methods are relatively easy to reduce the diameter and require a relatively small number of annealing operations during the diameter reduction process, and compared to the Sn plating method mentioned above, the Sn plating process and the Nb Although the heat treatment process for producing 3Sn is relatively simple, it has not yet reached a fully satisfactory level. That is, in the first improvement method, a low Sn concentration Cu-Sn alloy with relatively good workability is used as the base, and in the second improvement method, a low Sn
The outside of the concentrated Cu-Sn alloy base has good workability.
Since it is covered with Cu, the workability is better than in the case of the bronze method mentioned above, and the number of annealing is reduced, but it is necessary to form a Sn plating layer with a certain thickness, and in that case, it is necessary to form a Sn plating layer with a certain thickness. If so, in order to sufficiently diffuse Sn in the outer Sn plating layer, it is necessary to perform a more sufficient heat treatment than in the case of the bronze method. In addition, in the third improved method, a Cu-Sn alloy base with a high Sn concentration and poor workability is covered with a Cu-Sn alloy with a low Sn concentration that has relatively good workability. The workability is only slightly improved compared to the case of , and therefore the number of annealing times is not significantly reduced.

さらに、前記Snメツキ法、および第1〜第3
の改良方法に共通する欠点として、いずれも所定
の線径まで縮径した後にSnメツキを施して拡散
熱処理を行う関係上、拡散バリヤを伴う安定化銅
付きの極細多芯超電導線の製造には適用できない
問題がある。すなわち、ブロンズ法の場合、従来
から第5図に示すように多数のNbフイラメント
2を配したCu−Sn合金基地1の外側にTaもしく
はNbからなる拡散バリヤ層9を形成し、さらに
その拡散バリヤ層9の外側に無酸素銅からなる安
定化銅層10を形成して、所望の線径まで縮径し
た後拡散熱処理を施すことによつて、安定化のた
めの高純度のCu層を備えた極細多芯超電導線を
製造する方法が知られており、この方法では拡散
バリヤ層の存在によつてSnが外側のCu層に拡散
されないため、そのCu層の純度を高く保つて、
安定化に充分な役割を果たすことができる。しか
しながらSnメツキ法や前記改良法を用いて上述
のような拡散バリヤを伴う安定化銅付きの極細多
芯超電導線を製造しようとしても、拡散バリヤが
存在するため外部からSnを拡散させることは不
可能であり、またバリヤの外側に配した安定化の
ための無酸素銅を汚すことになり、したがつてこ
の型式の極細多芯超電導線の製造はブロンズ法に
限られるのが実情である。また前記各改良方法に
おいては、Snメツキ法の場合と同様に、拡散熱
処理時やその予備処理時等においてSnメツキ層
からSnが溶け落ち、充分な量のNb3Snを生成で
きなくなることもあつた。
Furthermore, the Sn plating method and the first to third
A common drawback of these improvement methods is that they all require Sn plating and diffusion heat treatment after the wire diameter has been reduced to a predetermined diameter, making it difficult to manufacture ultrafine multicore superconducting wires with stabilized copper and diffusion barriers. There are some problems that cannot be applied. That is, in the case of the bronze method, a diffusion barrier layer 9 made of Ta or Nb is conventionally formed on the outside of a Cu-Sn alloy base 1 in which a large number of Nb filaments 2 are arranged, as shown in FIG. A stabilized copper layer 10 made of oxygen-free copper is formed on the outside of the layer 9, and a high purity Cu layer for stabilization is provided by performing diffusion heat treatment after reducing the wire diameter to a desired wire diameter. There is a known method for manufacturing ultrafine multicore superconducting wires, and in this method, Sn is not diffused into the outer Cu layer due to the presence of a diffusion barrier layer, so the purity of the Cu layer is kept high.
It can play a sufficient role in stabilization. However, even if an attempt is made to manufacture an ultrafine multicore superconducting wire with stabilized copper accompanied by a diffusion barrier as described above using the Sn plating method or the improved method described above, it is impossible to diffuse Sn from the outside because of the existence of the diffusion barrier. However, it also contaminates the stabilizing oxygen-free copper placed outside the barrier, so the production of this type of ultrafine multicore superconducting wire is actually limited to the bronze method. In addition, in each of the above improvement methods, as with the Sn plating method, Sn may melt off from the Sn plating layer during diffusion heat treatment or its preliminary treatment, making it impossible to generate a sufficient amount of Nb 3 Sn. Ta.

この発明は以上の事情に鑑みてなされたもの
で、縮径加工時の加工性を良好にして焼鈍回数を
少なくし、しかも拡散熱処理を簡単に行ない得る
ようにし、特に太線径の極細多芯超電導線の製造
に有利とするとともに拡散バリヤを伴う安定化銅
付きのNb3Sn系の超電導線の製造に適した方法を
提供することを目的とするものである。
This invention has been made in view of the above circumstances, and aims to improve workability during diameter reduction processing, reduce the number of annealing operations, and easily perform diffusion heat treatment. The object is to provide a method which is advantageous for the production of wires and is suitable for the production of Nb 3 Sn based superconducting wires with stabilized copper with a diffusion barrier.

すなわち従来のSnメツキ法や前記各改良法に
おいては、特に芯線数の多い極細多芯超電導線を
製造する場合、前述のように複合素線の集合と縮
径(伸線加工)を複数回繰返し、所望の線径、芯
線数とした数、最外周側にSnメツキを施してい
たのに対し、この発明の方法では例えばNb3Sn系
の超電導線を製造する場合最終的な芯線数まで集
合されていない素線段階でSnメツキを施し、最
終的に集合された段階ではその外側にはSnメツ
キを施さないようにしたものである。
In other words, in the conventional Sn plating method and each of the improved methods mentioned above, especially when manufacturing ultrafine multicore superconducting wires with a large number of core wires, assembling the composite strands and reducing the diameter (wire drawing) as described above is repeated multiple times. In contrast, in the method of this invention, for example, when manufacturing Nb 3 Sn superconducting wire, the final number of cores is assembled to the desired wire diameter and number of cores. Sn plating is applied to the strands that are not assembled, and Sn plating is not applied to the outside of the wires when they are finally assembled.

すなわちこの発明の化合物系極細多芯超電導線
の製造方法は、超電導金属間化合物を構成する2
種以上の金属元素Nb,Snの内、Nbからなる一
本以上の芯材を、Snを含有する銅合金もしくは
実質的に銅からなる基地中に配して複合素線を作
り、その複合素線の表面にSnをメツキしてメツ
キ複合線を作り、さらにそのメツキ複合線を複数
本集合し、その集合線の外側にCu層もしくはCu
−Sn合金層を形成するとともにその層の外側に
Snの外側への拡散を防止するための拡散バリヤ
層を形成し、かつその拡散バリヤ層の外周面に安
定化のための純銅層を形成し、所定の線径まで縮
径した後、拡散熱処理を施して超電導金属間化合
物である。Nb3Sn系の極細多芯超電導線を得るも
のである。
In other words, the method for manufacturing a compound-based ultrafine multicore superconducting wire of the present invention involves
Among the metal elements Nb and Sn, one or more core materials made of Nb are placed in a copper alloy containing Sn or a base made essentially of copper to make a composite wire, and the composite wire is Plating Sn on the surface of the wire to create a plating composite wire, then collecting multiple plating composite wires, and adding a Cu layer or Cu layer to the outside of the assembly line.
- Forms a Sn alloy layer and outside of that layer.
A diffusion barrier layer is formed to prevent the diffusion of Sn to the outside, and a pure copper layer is formed on the outer peripheral surface of the diffusion barrier layer for stabilization. After reducing the wire diameter to a predetermined wire diameter, diffusion heat treatment is performed. It is a superconducting intermetallic compound. This is to obtain an Nb 3 Sn-based ultrafine multicore superconducting wire.

以下にこの発明の方法を具体的に説明する。 The method of this invention will be specifically explained below.

先ず第6図Aに示すように棒状、線状材、もし
くは粉末状のNb芯材2をCu−Sn合金もしくは
Cu製の中空パイプ11Aに挿入し、必要に応じ
てスエージング加工、伸線・引抜加工等の縮径加
工を施して、第6図Bに示すようにCu−Sn合金
もしくはCuの基地11にNb芯材2が埋込まれた
複合素線12を作成する。あるいはまた第7図A
に示すようにCu−Sn合金またはCuからなる棒材
11Bに複数の穴13を形成してその各穴13に
棒状、線材状もしくは粉未状のNb芯材2を挿入
し、押出加工、スエージング加工、引抜・伸線加
工等の縮径加工を行つて第7図Bに示すように
Cu−Sn合金もしくはCuの基地11に複数のNb
芯材2が埋込まれた複合素線12′を作成する。
次いで第6図Cもしくは第7図Cに示すように複
合素線12,12′の外側、すなわちCu−Sn合金
もしくはCuからなる基地11の外表面に電気メ
ツキ等により必要な厚みのSnメツキ層13を形
成し、メツキ複合線14を得る。次いでそのメツ
キ複合線14を第6図Dもしくは第7図Dに示す
ように複数本集合してCu−Sn合金もしくはCuか
らなるパイプ11Cに挿入するとともにさらにそ
れを拡散バリヤ層となるべきNbもしくはTaから
なるパイプ16に挿入し、かつその全体を安定化
銅層となるべき無酸素銅パイプ17に挿入し、そ
の後スエージング加工、伸線・引抜加工等の縮径
加工を施して、所望の線径すなわち最終的に得る
べき超電導線の径となるまで縮径し、第6図Eも
しくは第7図Eに示すような極細多芯複合線15
を得る。この極細多芯複合線15は、第8図もし
くは第9図に拡大して示すように、Cu−Sn合金
もしくはCuからなる基地11中に極めて細い多
数のNb芯材(Nbフイラメント)2が間隔を置い
て埋設され、しかも基地11の内部にSnメツキ
層13が網目状に配され、さらにその全体の外側
にはCuもしくはCu−Sn合金からなる層11
C′が、またその層11C′の外側には拡散バリヤ層
16′および安定化銅層17′がそれぞれ形成され
たものとなつている。このようにして極細多芯複
合線15を得た後には、拡散熱処理を施すことに
よつて、基地11の内部のSnメツキ層13から
Snが拡散されて、Nbフイラメント2の周囲に
Nb3Snが生成され、極細多芯超電導線となる。
First, as shown in FIG.
It is inserted into a Cu hollow pipe 11A, and subjected to diameter reduction processing such as swaging, wire drawing and drawing as necessary, to form a Cu-Sn alloy or Cu base 11 as shown in Fig. 6B. A composite wire 12 in which the Nb core material 2 is embedded is created. Or again, Figure 7A
As shown in the figure, a plurality of holes 13 are formed in a bar material 11B made of Cu-Sn alloy or Cu, and a Nb core material 2 in the form of a rod, wire, or powder is inserted into each hole 13, and extrusion processing and rolling are performed. After performing diameter reduction processing such as aging processing, drawing and wire drawing processing, it becomes as shown in Fig. 7B.
Multiple Nb in Cu-Sn alloy or Cu base 11
A composite wire 12' in which the core material 2 is embedded is created.
Next, as shown in FIG. 6C or FIG. 7C, a Sn plating layer of a required thickness is applied to the outside of the composite wires 12, 12', that is, the outside surface of the base 11 made of Cu-Sn alloy or Cu, by electroplating or the like. 13 to obtain a plating composite line 14. Next, as shown in FIG. 6D or FIG. 7D, a plurality of the plated composite wires 14 are assembled and inserted into a pipe 11C made of Cu-Sn alloy or Cu, and are further coated with Nb or Nb to form a diffusion barrier layer. It is inserted into a pipe 16 made of Ta, and the whole is inserted into an oxygen-free copper pipe 17 which is to become a stabilized copper layer, and then subjected to diameter reduction processing such as swaging, wire drawing, and drawing to obtain the desired shape. The diameter is reduced to the wire diameter, that is, the diameter of the superconducting wire to be finally obtained, and the ultrafine multicore composite wire 15 as shown in FIG. 6E or FIG. 7E is produced.
get. As shown in an enlarged view in FIG. 8 or 9, this ultra-fine multifilamentary composite wire 15 has a large number of extremely thin Nb core materials (Nb filaments) 2 arranged at intervals in a base 11 made of Cu-Sn alloy or Cu. Furthermore, a Sn plating layer 13 is arranged in a mesh pattern inside the base 11, and furthermore, a layer 11 made of Cu or Cu-Sn alloy is disposed on the outside of the entire base 11.
C', and a diffusion barrier layer 16' and a stabilizing copper layer 17' are respectively formed outside the layer 11C'. After obtaining the ultrafine multifilamentary composite wire 15 in this way, diffusion heat treatment is performed to remove the Sn plating layer 13 inside the base 11.
Sn is diffused around Nb filament 2.
Nb 3 Sn is generated and becomes an ultrafine multicore superconducting wire.

前述の拡散熱処理は、この発明の方法によれば
従来のブロンズ法における拡散熱処理と同程度の
簡単な処理で充分である。すなわち、極細多芯複
合線の段階において第8図もしくは第9図に示す
ようにSnメツキ層13が基地11の内部に網目
状に配されているため、従来のSnメツキ法や従
来の改良方法の如くSnメツキ層が最外周側に位
置している場合と比較して、主たるSn供給源で
あるSnメツキ層13とNbフイラメント2との間
の距離が著しく短かい。換言すれば、Nb3Snを生
成するためにSnが拡散移動すべき距離が従来の
Snメツキ法と比較して著しく短かく、したがつ
て拡散熱処理時に予備熱処理を施したり、さらに
はその予備熱処理を複数段にわたつて施したりす
る必要がなく、簡単な熱処理で充分な量のNb3Sn
を生成させることができる。このような効果は、
特に太い線径の場合、すなわちNbフイラメント
の数が多い場合に顕著となる。すなわち、従来の
Snメツキ法においては線径が太くなればそれに
伴つて外側のメツキ層と中心部のNbフイラメン
トとの間の距離が大きくなるが、この発明の方法
では線径が太くなつてもNbフイラメント径をほ
とんど同じ細径に仕上げるためそのようなことが
なく、Snの拡散移動距離は常に短かいから、線
径が太い場合でも細い線径の場合と同様に簡単な
熱処理で充分な量のNb3Snを生成させることがで
きる。具体的には、拡散熱処理としては真空中も
しくは不活性ガス雰囲気中において650〜850℃程
度の温度で20〜150時間程度加熱すれば良い。
According to the method of the present invention, the above-mentioned diffusion heat treatment can be as simple as the diffusion heat treatment in the conventional bronze method. In other words, since the Sn plating layer 13 is arranged in a mesh pattern inside the base 11 as shown in FIG. 8 or 9 at the stage of ultra-fine multicore composite wire, the conventional Sn plating method and the conventional improvement method are not possible. The distance between the Sn plating layer 13, which is the main Sn supply source, and the Nb filament 2 is significantly shorter than in the case where the Sn plating layer is located at the outermost circumferential side. In other words, the distance that Sn must diffuse to generate Nb 3 Sn is longer than the conventional distance.
It is significantly shorter than the Sn plating method, and therefore there is no need to perform preheat treatment during diffusion heat treatment or to perform the preheat treatment in multiple stages. 3 Sn
can be generated. Such an effect is
This is particularly noticeable when the wire diameter is large, that is, when the number of Nb filaments is large. In other words, conventional
In the Sn plating method, as the wire diameter increases, the distance between the outer plating layer and the central Nb filament increases, but with the method of this invention, the Nb filament diameter can be maintained even when the wire diameter increases. This does not happen because the wires are finished to almost the same small diameter, and the diffusion migration distance of Sn is always short, so even if the wire is thick, a sufficient amount of Nb 3 Sn can be produced with a simple heat treatment, just like in the case of a thin wire. can be generated. Specifically, the diffusion heat treatment may be performed by heating at a temperature of about 650 to 850° C. for about 20 to 150 hours in a vacuum or an inert gas atmosphere.

なおNb芯材が埋込まれる基地11となるべき
パイプ11A,11Cあるいは棒11Bとしては
前述のようにCuもしくはCu−Sn合金を用いれば
良いが、Nb3Snの生成に必要なSn量はSnメツキ
層から補給されるためCu−Sn合金を用いる場合
でもそのCu−Sn合金は低Sn濃度のもので充分で
ある。したがつて加工性を良好にして縮径加工に
おける中間焼鈍の回数を少なくするためには、
Sn濃度が10wt%未満、より最適には8wt%以下
程度のCu−Sn合金を用いることが望ましい。ま
たこのCu−Sn合金としては小量のPを含有する
もの、すなわちリン青銅を用いることもできる。
As mentioned above, Cu or Cu-Sn alloy may be used for the pipes 11A, 11C or the rod 11B that will become the base 11 in which the Nb core material is embedded, but the amount of Sn required to generate Nb 3 Sn is Since the metal is supplied from the plating layer, even if a Cu-Sn alloy is used, it is sufficient that the Cu-Sn alloy has a low Sn concentration. Therefore, in order to improve workability and reduce the number of intermediate annealing operations during diameter reduction processing,
It is desirable to use a Cu-Sn alloy with a Sn concentration of less than 10 wt%, more optimally about 8 wt% or less. Moreover, as this Cu-Sn alloy, one containing a small amount of P, that is, phosphor bronze can also be used.

ここで、拡散バリヤ層16′は、Snが外側の安
定化銅層17′に拡散してNb3Snの生成効率が低
下したり安定化銅層17′の純度が低下してその
電気抵抗が低下したりすることを防止するに寄与
する。そしてこの拡散バリヤ層16′の内側にCu
層もしくはCu−Sn合金層11C′を配しておくこ
とにより、拡散バリヤ層16′の内周面での
Nb3Snの生成による加工性の劣化を補つて、良好
な加工性を確保することができる。
Here, in the diffusion barrier layer 16', Sn diffuses into the outer stabilizing copper layer 17', reducing the Nb 3 Sn generation efficiency, or reducing the purity of the stabilizing copper layer 17', increasing its electrical resistance. Contributes to preventing deterioration. Then, Cu is deposited on the inside of this diffusion barrier layer 16'.
By disposing the Cu-Sn alloy layer 11C', the diffusion barrier layer 16'
Good workability can be ensured by compensating for the deterioration in workability due to the formation of Nb 3 Sn.

上述の説明において、複合素線を最終的なNb
フイラメント数となるように集合する以前の段階
でも中間的に複合素線を集合させることもでき
る。すなわち、全く集合されていない複合素線
(以下これを一次複合素線と称する)を複数本集
合して二次複合素線を作り、その二次集合素線を
さらに複数本集合して縮径し、最終的なNbフイ
ラメント数を有する極細多芯複合線を得ることが
ある。この場合Snメツキは一次複合素線の段階
もしくは二次複合素線の段階のいずれで行つても
良く、また一次複合素線の段階および二次複合素
線の段階の両段階でSnメツキを施しても良く、
要は最終的なフイラメント数に集合される以前の
段階でSnメツキを行えば良い。
In the above explanation, the composite wire is the final Nb
Composite strands can be assembled intermediately even before they are assembled to the number of filaments. In other words, multiple composite strands that are not assembled at all (hereinafter referred to as primary composite strands) are assembled to create a secondary composite strand, and multiple secondary assembled strands are further assembled to reduce the diameter. However, an ultrafine multifilamentary composite wire with the final number of Nb filaments may be obtained. In this case, Sn plating may be performed either at the stage of the primary composite strand or at the stage of the secondary composite strand, or the Sn plating may be performed at both the stage of the primary composite strand and the stage of the secondary composite strand. It's okay,
In short, Sn plating should be performed at a stage before the final number of filaments is assembled.

例えば第10図Aに示すようにCuもしくはCu
−Sn合金からなるパイプ11AにNb芯材2を挿
入して縮径加工し、第10図Bに示すようにCu
もしくはCu−Sn合金の基地11中にNb芯材2を
配した一次複合素線12Aを得、第10図Cに示
すように一次複合素線12Aの外表面にSnメツ
キ層13を形成した後、そのSnメツキが施され
た一次複合素線12Aを第10図Dに示すように
複数本集合してCuもしくはCu−Sn合金製のパイ
プ11Dに挿入し、縮径加工を施して第10図E
に示すような所望の径の二次複合素線12Bを
得、さらに第10図Fに示すように複数本の二次
複合素線12Bを集合してCuもしくはCu−Sn合
金製のパイプ11Cに挿入するとともに拡散バリ
ヤ層となるべきNbもしくはTaからなるパイプ1
6に挿入し、かつその全体を安定化銅層となるべ
き無酸素銅パイプ17に挿入し、再び縮径加工を
行つて第10図Gに示すような極細多芯複合線1
5を得れば良い。あるいはまた、第10図Bに示
される一次複合素線12Aに対してSnメツキを
施さずに第10図Hに示すように一次複合素線1
2を複数本集合してCuもしくはCu−Sn合金製の
パイプ11Dに挿入し、縮径加工を施して第10
図Iに示すような所望の線径の二次複合素線12
Bを得、その後第10図Jに示すように二次複合
素線12Bの表面にSnメツキ層13′を形成し、
次いで第10図Kに示すようにそのSnメツキが
施された二次複合素線12Bを複数本集合して
CuもしくはCu−Sn合金製のパイプ11Cに挿入
するとともに拡散バリヤ層となるべきNbもしく
はTaからなるパイプ16に挿入し、さらにその
全体を安定化銅層となるべき無酸素銅パイプ17
に挿入し、再び縮径加工を行つて第10図Lに示
すような極細多芯複合線15を得ても良い。さら
には第10図A〜Cに示すように一次複合素線1
2Aの表面にSnメツキ層13を形成した後、第
10図D,Eに示すように集合および縮径加工し
て二次複合素線12Bを得、その後第10図Jに
示すように二次複合素線12Bの表面にもSnメ
ツキ層13′を形成し、その後前記同様に集合お
よび縮径加工しても良い。もちろん最終的な集合
工程以前に2回以上集合および縮径加工を繰返す
場合にも上述の各例に準じてSnメツキを施せば
良い。上述のようにして得られた極細多芯複合線
に対しては、前記同様に拡散熱処理を施せば良
い。
For example, as shown in Figure 10A, Cu or Cu
- The Nb core material 2 is inserted into the pipe 11A made of Sn alloy, the diameter is reduced, and the Cu
Alternatively, after obtaining the primary composite wire 12A in which the Nb core material 2 is arranged in the base 11 of Cu-Sn alloy, and forming the Sn plating layer 13 on the outer surface of the primary composite wire 12A as shown in FIG. 10C, A plurality of the Sn-plated primary composite wires 12A are assembled into a pipe 11D made of Cu or Cu-Sn alloy as shown in FIG. 10D, and the diameter is reduced. E
A secondary composite wire 12B having a desired diameter as shown in FIG. 10F is obtained, and as shown in FIG. Pipe 1 made of Nb or Ta to be inserted and to serve as a diffusion barrier layer
6, and the entirety thereof is inserted into the oxygen-free copper pipe 17 which is to become a stabilized copper layer, and the diameter is reduced again to form the ultra-fine multifilamentary composite wire 1 as shown in FIG. 10G.
All you have to do is get a 5. Alternatively, the primary composite wire 12A shown in FIG. 10B is not plated with Sn, and the primary composite wire 12A shown in FIG. 10H is
A plurality of pipes 2 are assembled and inserted into a pipe 11D made of Cu or Cu-Sn alloy, and the diameter is reduced to form the 10th pipe.
Secondary composite wire 12 of desired wire diameter as shown in Figure I
B was obtained, and then, as shown in FIG. 10J, a Sn plating layer 13' was formed on the surface of the secondary composite wire 12B,
Next, as shown in FIG. 10K, a plurality of the Sn-plated secondary composite wires 12B are assembled.
The oxygen-free copper pipe 17 is inserted into a pipe 11C made of Cu or Cu-Sn alloy and is inserted into a pipe 16 made of Nb or Ta which is to serve as a diffusion barrier layer, and further whose entirety is to be a stabilizing copper layer.
The wire may be inserted into the wire and the diameter reduction process may be performed again to obtain an ultrafine multifilamentary composite wire 15 as shown in FIG. 10L. Furthermore, as shown in FIGS. 10A to 10C, the primary composite wire 1
After forming the Sn plating layer 13 on the surface of the wire 2A, the secondary composite wire 12B is assembled and diameter-reduced as shown in FIG. The Sn plating layer 13' may also be formed on the surface of the composite wire 12B, and then the wires may be assembled and diameter-reduced in the same manner as described above. Of course, even if the assembly and diameter reduction process are repeated two or more times before the final assembly process, Sn plating may be applied in accordance with each of the above-mentioned examples. The ultrafine multifilamentary composite wire obtained as described above may be subjected to diffusion heat treatment in the same manner as described above.

以下にこの発明の実施例を記す。 Examples of this invention are described below.

実施例 1 外径10mm、肉厚1.5mmのSn濃度6wt%のリン青
銅製のパイプに外径6.5mmのNb棒を挿入し、伸線
加工および中間焼鈍を繰返して外径0.75mmの一次
複合素線を得た。この一次複合素線の外周面に電
気メツキにより10μm厚のSnメツキ層を形成した
後、そのSnメツキが施された一次複合素線を91
本集合し、外径10mm、肉厚0.5mmの6wt%Snを含
有するリン青銅製のパイプに挿入し、伸線加工お
よび中間焼鈍を繰返し、外径0.75mmの二次複合素
線を得た。さらにこの二次複合素線の表面に電気
メツキにより10μm厚のSnメツキ層を形成した
後、その二次複合素線を91本集合して外径10mm、
肉厚0.5mmの6wt%Snを含有するリン青銅パイプ
に挿入し、さらにそれを外径12mm、肉厚0.5mmの
Nbパイプに挿入し、その全体を外径17mm、肉厚
2mmの無酸素銅パイプに挿入して、伸線加工およ
び中間焼鈍を繰返して外径1.0mmの安定化銅付き
の8281芯の極細多芯複合線を作成した。次いでこ
の様に800℃×50時間の拡散熱処理を施して安定
化銅付きのNb3Sn系極細多芯超電導線を得た。そ
の超電導線の超電導特性を温度4.2K、外部磁界
100KGの条件で測定したところ、臨界電流値
250Aを得た。この値は、Nb3Snだけの臨界電流
値としてみた場合、3×103A/mm2に相当し、良
好な特性といえる。
Example 1 A Nb rod with an outer diameter of 6.5 mm was inserted into a phosphor bronze pipe with an outer diameter of 10 mm and a wall thickness of 1.5 mm with an Sn concentration of 6 wt%, and wire drawing and intermediate annealing were repeated to create a primary composite with an outer diameter of 0.75 mm. I got a bare wire. After forming a Sn plating layer with a thickness of 10 μm on the outer peripheral surface of this primary composite wire by electroplating, the primary composite wire with the Sn plating was
This assembly was inserted into a phosphor bronze pipe containing 6 wt% Sn with an outer diameter of 10 mm and a wall thickness of 0.5 mm, and wire drawing and intermediate annealing were repeated to obtain a secondary composite wire with an outer diameter of 0.75 mm. . Furthermore, after forming a Sn plating layer with a thickness of 10 μm on the surface of this secondary composite strand by electroplating, 91 secondary composite strands were assembled to form an outer diameter of 10 mm.
Insert it into a phosphor bronze pipe containing 6wt% Sn with a wall thickness of 0.5 mm, and then insert it into a phosphor bronze pipe with an outer diameter of 12 mm and a wall thickness of 0.5 mm.
The whole is inserted into an oxygen-free copper pipe with an outer diameter of 17 mm and a wall thickness of 2 mm, and the wire drawing process and intermediate annealing are repeated. Created a core compound line. Next, diffusion heat treatment was performed at 800°C for 50 hours in this manner to obtain an Nb 3 Sn-based ultrafine multifilamentary superconducting wire with stabilized copper. The superconducting properties of the superconducting wire are measured at a temperature of 4.2K and an external magnetic field.
When measured under the condition of 100KG, the critical current value
Got 250A. This value corresponds to 3×10 3 A/mm 2 when viewed as a critical current value of only Nb 3 Sn, and can be said to be a good characteristic.

実施例 2 外径200mmのCu−Sn合金(Sn3wt%)のビレツ
ト13mmφの穴を91本形成し、各穴に外径12mmの
Nb棒を挿入して押出し用ビレツトを作成した。
そのビレツトを押出し加工した後、伸線加工およ
び中間焼鈍を繰返して外径6.5mmの複合素線を得
た。その複合素線の表面に厚さ160μmのSnメツ
キ層を溶融メツキにより形成した後、外径200mm、
内径160mmの無酸素銅パイプ、外径150mm、内径
140mmのNbパイプ、および外径130mm、内径120mm
のCu−Sn合金(Su3wt%)を重ねた複合パイプ
中に前記の線を217本集合して挿入し、19747芯の
ビレツトを作成した。そのビレツトを押出加工
後、伸線加工および中間焼鈍を繰返して外径2.0
mmの安定化銅付きの極細多芯複合線を得た。その
後755℃×100時間の拡散熱処理を施して安定化銅
付きのNb3Sn系極細多芯超電導線を作成した。こ
の超電導線の超電導特性を温度4.2K、外部磁界
120KGで測定したところ、臨界電流値370Aを得
た。この値はNb3Snだけの臨界電流値に換算すれ
ば1.5×103A/mm2となり、良好な特性であると認
められる。
Example 2 Ninety-one 13 mmφ billet holes of Cu-Sn alloy (Sn3wt%) with an outer diameter of 200 mm were formed, and a hole with an outer diameter of 12 mm was formed in each hole.
A billet for extrusion was created by inserting a Nb rod.
After extruding the billet, wire drawing and intermediate annealing were repeated to obtain a composite wire with an outer diameter of 6.5 mm. After forming a Sn plating layer with a thickness of 160 μm on the surface of the composite wire by melt plating,
Oxygen-free copper pipe with inner diameter 160mm, outer diameter 150mm, inner diameter
140mm Nb pipe, and outer diameter 130mm, inner diameter 120mm
A billet with 19,747 cores was created by inserting a collection of 217 wires into a composite pipe made of stacked Cu-Sn alloys (Su3wt%). After extruding the billet, wire drawing and intermediate annealing are repeated to obtain an outer diameter of 2.0.
An ultrafine multicore composite wire with stabilized copper of mm was obtained. After that, diffusion heat treatment was performed at 755°C for 100 hours to create a Nb 3 Sn-based ultrafine multicore superconducting wire with stabilized copper. The superconducting properties of this superconducting wire are measured at a temperature of 4.2K and an external magnetic field.
When measured at 120KG, a critical current value of 370A was obtained. This value is 1.5×10 3 A/mm 2 when converted to the critical current value of only Nb 3 Sn, which is recognized as having good characteristics.

前述の説明で明らかなようにこの発明の方法
は、最終的に所望の芯線数となるように集合する
以前の段階の複合素線にSn等のメツキを施すも
のであるから、拡散熱処理を行う直前の極細多芯
複合線の段階では、金属間化合物を構成する一方
の金属からなるメツキ層部分が複合線の内部でし
かも前記金属間化合物を構成する他方の金属から
なる芯材フイラメントの極く近傍に位置し、した
がつて拡散により前記金属間化合物を生成するこ
とが容易であるから、拡散熱処理を簡単に行ない
得、しかも太線径の場合でもその径にほとんど影
響されることなく簡単に拡散熱処理を行うことが
でき、また芯材が埋込れる基地は加工性が良好な
銅または低合金濃度の銅合金を使用できるから、
縮径加工中における中間焼鈍の必要回数も従来の
Snメツキ法と同程度に少なくすることができ、
さらには前述のごとく拡散熱処理が簡単で特に予
備熱処理を必要としないため熱処理時にCu−Sn
系金属間化合物等の有害な化合物相を生成するお
それも少なく、またSn等の低融点金属のメツキ
層部分が複合線の内部に位置するため拡散熱処理
時にSn等が溶け落ちしてしまうおそれも少ない
等、各種の効果が得られるものである。
As is clear from the above explanation, in the method of the present invention, the composite strands are plated with Sn or the like before they are assembled to have the desired number of cores, so diffusion heat treatment is performed. In the immediately preceding stage of ultra-fine multicore composite wire, the plating layer made of one of the metals constituting the intermetallic compound is inside the composite wire and at the very edge of the core filament made of the other metal constituting the intermetallic compound. Since the intermetallic compounds are located nearby and it is therefore easy to generate the intermetallic compound by diffusion, diffusion heat treatment can be easily performed, and even in the case of thick wire diameters, the diffusion can be easily performed without being affected by the diameter. Heat treatment can be performed, and the base in which the core material is embedded can be made of copper, which has good workability, or copper alloy with a low alloy concentration.
The required number of intermediate annealing during diameter reduction processing is also lower than conventional
The amount can be reduced to the same level as the Sn plating method.
Furthermore, as mentioned above, diffusion heat treatment is easy and does not require any preliminary heat treatment, so Cu-Sn can be removed during heat treatment.
There is little risk of generating harmful compound phases such as intermetallic compounds, and since the plating layer of low melting point metals such as Sn is located inside the composite wire, there is no risk of Sn etc. melting through during diffusion heat treatment. Various effects can be obtained, such as reducing the amount of water used.

さらにこの発明によれば、拡散バリヤを伴つた
安定化銅付きのNb3Sn系極細多芯超電導線をブロ
ンズ法によらず製造することができ、したがつて
拡散バリヤの存在により安定化銅層にSnが拡散
することを防止して、安定化銅層の電気抵抗の低
下を防止するとともにNb3Sn生成効率の低下を防
止することができ、かつまた芯材を埋込む基地と
して前述のように加工性が良好な銅または低合金
濃度の銅合金を用いるとともに、安定化バリヤ層
の内周にも銅もしくは銅合金を配することによつ
て、加工性が極めて良好となり、そのため縮径加
工が容易で中間焼鈍回数を減らすことができる点
から有利となる。
Furthermore, according to the present invention, it is possible to produce an Nb 3 Sn-based ultrafine multifilamentary superconducting wire with stabilized copper accompanied by a diffusion barrier without using the bronze method, and therefore, due to the presence of the diffusion barrier, the stabilized copper layer By preventing Sn from diffusing into the stabilized copper layer, it is possible to prevent a decrease in electrical resistance of the stabilized copper layer and to prevent a decrease in Nb 3 Sn generation efficiency. By using copper or a copper alloy with a low alloy concentration, which has good workability, and by disposing copper or a copper alloy on the inner periphery of the stabilizing barrier layer, the workability is extremely good, and therefore diameter reduction processing is possible. This is advantageous because it is easy to perform and the number of intermediate annealing can be reduced.

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

第1図は従来のブロンズ法における複合線の断
面図、第2図は従来のSnメツキ法における複合
線の断面図、第3図および第4図はそれぞれ従来
の改良方法における複合線の断面図、第5図は従
来の安定化銅付き複合線の断面図、第6図および
第7図はそれぞれこの発明の方法の一例を段階的
に示すための説明図、第8図は第6図のEに示さ
れる複合線の拡大断面図、第9図は第7図のEに
示される複合線の拡大断面図、第10図は複合素
線の集合および縮径を2回行う場合のこの発明の
方法の例を段階的に示す説明図である。 2……Nb芯材、11……基地、12……複合
素線、12A……一次複合素線、12B……二次
複合素線、13,13′……Snメツキ層、14…
…メツキ複合線、15……極細多芯複合線。
Figure 1 is a cross-sectional view of a composite wire in the conventional bronze method, Figure 2 is a cross-sectional view of a composite wire in the conventional Sn plating method, and Figures 3 and 4 are cross-sectional views of a composite wire in the conventional improved method. , FIG. 5 is a sectional view of a conventional stabilized composite wire with copper, FIGS. 6 and 7 are explanatory diagrams showing step-by-step an example of the method of the present invention, and FIG. 8 is a cross-sectional view of a conventional stabilized composite wire with copper. FIG. 9 is an enlarged sectional view of the composite wire shown in E of FIG. 7, and FIG. 10 is an enlarged sectional view of the composite wire shown in E of FIG. It is an explanatory diagram showing an example of a method step by step. 2...Nb core material, 11...Base, 12...Composite strand, 12A...Primary composite strand, 12B...Secondary composite strand, 13, 13'...Sn plating layer, 14...
...Metsuki compound wire, 15...Extra-fine multicore compound wire.

Claims (1)

【特許請求の範囲】[Claims] 1 Nbからなる一本以上の芯材を、Cu−Sn合金
もしくは実質的にCuからなる基地中に配して複
合素線を作り、その複合素線の表面にSnメツキ
してメツキ複合線を作り、さらにそのメツキ複合
線を複数本集合し、その集合線の外側にCuもし
くはCu−Sn合金層を形成するとともにその外側
にSnの外側への拡散を防止するための拡散バリ
ヤ層を形成し、かつその拡散バリヤ層の外周面に
安定化のための純銅層を形成し、所定の線径まで
縮径した後、拡散熱処理を施して超電導金属間化
合物としてのNb3Snを内部に生成させることを特
徴とする化合物系極細多芯超電導線の製造方法。
1. One or more core materials made of Nb are arranged in a Cu-Sn alloy or a base substantially made of Cu to make a composite wire, and the surface of the composite wire is plated with Sn to form a plated composite wire. Then, a plurality of the plated composite wires are assembled, and a Cu or Cu-Sn alloy layer is formed on the outside of the assembled wire, and a diffusion barrier layer is formed on the outside to prevent Sn from diffusing outward. , and a pure copper layer is formed on the outer circumferential surface of the diffusion barrier layer for stabilization, and after reducing the wire diameter to a predetermined diameter, a diffusion heat treatment is performed to generate Nb 3 Sn as a superconducting intermetallic compound inside. A method for producing a compound-based ultrafine multicore superconducting wire, characterized by the following.
JP56079590A 1981-05-25 1981-05-25 Method of producing compound series extrafine multicore superconductive wire Granted JPS57194404A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56079590A JPS57194404A (en) 1981-05-25 1981-05-25 Method of producing compound series extrafine multicore superconductive wire

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56079590A JPS57194404A (en) 1981-05-25 1981-05-25 Method of producing compound series extrafine multicore superconductive wire

Publications (2)

Publication Number Publication Date
JPS57194404A JPS57194404A (en) 1982-11-30
JPH0313686B2 true JPH0313686B2 (en) 1991-02-25

Family

ID=13694204

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56079590A Granted JPS57194404A (en) 1981-05-25 1981-05-25 Method of producing compound series extrafine multicore superconductive wire

Country Status (1)

Country Link
JP (1) JPS57194404A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61284556A (en) * 1985-06-11 1986-12-15 Fujikura Ltd Production of compound superconductive wire
JP2845905B2 (en) * 1988-10-13 1999-01-13 株式会社フジクラ Compound conducting wire for alternating current
JPH02103813A (en) * 1988-10-13 1990-04-16 Fujikura Ltd Compound superconducting wire and manufacture thereof

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS522599A (en) * 1975-06-24 1977-01-10 Yukio Matsuda Selecting device for documents storage safe
JPS5439594A (en) * 1977-09-02 1979-03-27 Mitsubishi Electric Corp Manufacture for compound system composite superconductor

Also Published As

Publication number Publication date
JPS57194404A (en) 1982-11-30

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