JPH087682A - Method for producing Nb3Sn compound superconducting wire - Google Patents

Method for producing Nb3Sn compound superconducting wire

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Publication number
JPH087682A
JPH087682A JP6160690A JP16069094A JPH087682A JP H087682 A JPH087682 A JP H087682A JP 6160690 A JP6160690 A JP 6160690A JP 16069094 A JP16069094 A JP 16069094A JP H087682 A JPH087682 A JP H087682A
Authority
JP
Japan
Prior art keywords
layer
wire
composite
thermal diffusion
metal material
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
JP6160690A
Other languages
Japanese (ja)
Inventor
Tomonori Yamada
知礼 山田
Kinya Ogawa
欽也 小川
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 JP6160690A priority Critical patent/JPH087682A/en
Publication of JPH087682A publication Critical patent/JPH087682A/en
Pending 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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  • Wire Processing (AREA)
  • Superconductors And Manufacturing Methods Therefor (AREA)

Abstract

(57)【要約】 【目的】 超電導特性に優れたNb3 Sn系化合物超電
導線を製造する。 【構成】 Cu−Sn系合金基体中にNbフィラメント
を多数本配列させた複合素線上に、Sn層5、及びSn
より高融点でSnと非反応性の金属材層を順次形成して
複合線材となし、この複合線材に熱拡散処理を施してC
u−Sn系合金基体中にNb3 Snフィラメントを生成
させる。 【効果】 高融点でSnと非反応性の金属材層6が、複
合素線上の溶融Snを保持するので、Snの熱拡散処理
を高温短時間で行うことができる。従って基体中に空孔
が生成したりせず、超電導特性に優れたNb3 Sn系化
合物超電導線が得られる。
(57) [Summary] [Purpose] To produce Nb 3 Sn-based compound superconducting wire with excellent superconducting properties. [Structure] A Sn layer 5 and Sn are formed on a composite element wire in which a large number of Nb filaments are arranged in a Cu-Sn alloy substrate.
A metal wire layer having a higher melting point and non-reactive with Sn is sequentially formed to form a composite wire, and the composite wire is subjected to thermal diffusion treatment to form C
During u-Sn-based alloy substrate to produce Nb 3 Sn filaments. [Effect] Since the metal material layer 6 having a high melting point and not reacting with Sn holds the molten Sn on the composite wire, the thermal diffusion treatment of Sn can be performed at a high temperature in a short time. Therefore, voids are not formed in the substrate, and an Nb 3 Sn-based compound superconducting wire having excellent superconducting properties can be obtained.

Description

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

【0001】[0001]

【産業上の利用分野】本発明は、超電導特性に優れた、
Nb3 Sn系化合物超電導線の製造方法に関する。
BACKGROUND OF THE INVENTION The present invention has excellent superconducting properties,
The present invention relates to a method for producing a Nb 3 Sn-based compound superconducting wire.

【0002】[0002]

【従来の技術】化合物超電導線はCu又はCu合金基体
中にNb3 Sn、Nb3 Al、V3 Ga等の超電導フィ
ラメントが多数本複合された超電導線である。この化合
物超電導線はNb3 Sn等の超電導体相が脆い為、次の
ようにして製造される。即ち、Cu−Sn系合金基体中
にNb金属の棒材を多数本埋込んで一次ビレットを組立
て、これに中間焼鈍と縮径加工を施して所定形状の線状
体とし、この線状体をCu−Sn系合金パイプ内に多数
本整列充填して二次ビレットを組立て、これに中間焼鈍
と縮径加工を施してCu−Sn系合金基体中にNbフィ
ラメントが複合された複合素線を作製する。次に、この
複合素線に 700〜800 ℃の温度で熱拡散処理を施して、
前記Nbフィラメントを前記基体及びパイプ中のSnと
反応させてNb3 Snフィラメントに形成する。
2. Description of the Related Art A compound superconducting wire is a superconducting wire in which a large number of superconducting filaments such as Nb 3 Sn, Nb 3 Al and V 3 Ga are compounded in a Cu or Cu alloy substrate. This compound superconducting wire is manufactured as follows because the superconductor phase such as Nb 3 Sn is fragile. That is, a large number of Nb metal rods are embedded in a Cu-Sn alloy substrate to assemble a primary billet, which is then annealed and reduced in diameter to form a linear body having a predetermined shape. A large number of Cu-Sn alloy pipes are aligned and filled to assemble a secondary billet, which is then annealed and reduced in diameter to produce a composite element wire in which Nb filaments are compounded in a Cu-Sn alloy substrate. To do. Next, this composite wire is subjected to thermal diffusion treatment at a temperature of 700 to 800 ° C,
The Nb filaments are reacted with Sn in the substrate and pipe to form Nb 3 Sn filaments.

【0003】前述の製造方法では、基体又はパイプを構
成するCu−Sn系合金のSn濃度が高い程、生成する
Nb3 Sn化合物は化学量論組成に近くなり、得られる
超電導線の超電導特性が向上する。しかし、前記Cu−
Sn系合金のSn濃度を高くするとビレットの加工硬化
が大きくなり、特にSnが固溶限を超えて含有される
と、中間焼鈍を多数回入れても伸線加工時に割れが生じ
た。この為Cu−Sn系合金中のSn量は固溶限以下に
抑えざるを得ず、従ってSnの量が不足して十分に高い
超電導特性が得られなかった。又中間焼鈍はNb3 Sn
相が生成しない低い温度で施す為長時間を要し、生産性
を著しく害した。
[0003] In the above manufacturing method, the higher the Sn concentration of the Cu-Sn-based alloy constituting the substrate or pipe, resulting Nb 3 Sn compound is close to the stoichiometric composition, superconducting properties of the resulting superconducting wire improves. However, the Cu-
When the Sn concentration of the Sn-based alloy is increased, the work hardening of the billet becomes large, and especially when Sn is contained in excess of the solid solution limit, cracking occurred during wire drawing even if the intermediate annealing was performed many times. For this reason, the amount of Sn in the Cu-Sn alloy has to be suppressed below the solid solution limit. Therefore, the amount of Sn is insufficient and a sufficiently high superconducting property cannot be obtained. In addition, the intermediate annealing is Nb 3 Sn
Since it was applied at a low temperature at which no phase was formed, it took a long time and markedly impaired the productivity.

【0004】[0004]

【発明が解決しようとする課題】そこで、基体及びパイ
プに、加工性の良い低Sn濃度のCu−Sn系合金を用
いて中間焼鈍の回数を減らし、Snの不足分は、複合素
線上にSnをめっきして補給する外部拡散法が開発され
た。この外部拡散法では、熱拡散処理をいきなり700℃
以上の高温度で施すとSnめっき層やSnリッチのCu
−Sn系化合物が溶落し、不足して所望の超電導特性が
得られなかった。そこで、熱拡散処理を、先ずSnの融
点未満の温度でCu−Sn系合金基体中にSn層を拡散
させ、次いで 300℃前後の温度でSnの拡散を促進し、
最後に 700℃以上の高温でNb3 Sn相を反応生成させ
るという3段階に分けて施す方法(特公昭62-62003号)
が提案された。しかし、このように熱拡散処理を低温度
から徐々に行う方法では、CuとSn原子の拡散速度が
異なることから、Cu−Sn系合金基体中にカーケンダ
ル効果による空孔(以下カーケンダル空孔と略記する)
が生じた。この空孔は超電導線の歪み感受性を大きくし
て、超電導特性を低下させ又不安定にした。このカーケ
ンダル空孔の発生防止策として、複合線材を 0.3mmφ以
下に細くしてSnの拡散時間を短縮する方法が提案され
た。この方法では、二次ビレットの組立てに際し、細い
複合線材を整列充填するのに大変な手間を要した。
Therefore, the number of intermediate annealings is reduced by using a Cu-Sn type alloy having a low Sn concentration with good workability for the substrate and the pipe. An outdiffusion method has been developed to plate and replenish. In this external diffusion method, the thermal diffusion process is suddenly performed at 700 ° C.
When applied at the above high temperature, Sn plating layer and Sn rich Cu
The -Sn-based compound was burned out and insufficient, and desired superconducting properties were not obtained. Therefore, a thermal diffusion treatment is carried out by first diffusing the Sn layer in the Cu—Sn alloy base at a temperature lower than the melting point of Sn, and then promoting the diffusion of Sn at a temperature of around 300 ° C.
Finally, a method in which the Nb 3 Sn phase is formed by reaction at a high temperature of 700 ° C or higher in three steps (Japanese Patent Publication No. 62-62003).
Was proposed. However, in such a method in which the thermal diffusion treatment is gradually performed from a low temperature, since the diffusion rates of Cu and Sn atoms are different, holes in the Cu—Sn alloy substrate due to the Kirkendall effect (hereinafter abbreviated as Kirkendall holes). Do)
Occurred. These vacancies increased the strain sensitivity of the superconducting wire, deteriorating the superconducting property and making it unstable. As a measure for preventing the occurrence of Kirkendall pores, a method has been proposed in which the composite wire is thinned to 0.3 mm or less to shorten the Sn diffusion time. According to this method, it takes a great deal of time to align and fill the thin composite wire rod when assembling the secondary billet.

【0005】この他、カーケンダル空孔の発生防止策と
して、複合素線上にSn層とCu層を順次形成する方法
が提案された(特開平1-232613号)。この方法は、外周
のCu層に溶融Sn層を保持させて高温で熱拡散処理を
行い、熱拡散処理時間を短縮するものである。しかし、
この方法ではSnがCu層に固溶して消費される為、そ
の分Sn層を厚くめっきすることになり、その結果熱拡
散処理時間が長くなって、カーケンダル空孔が生じてし
まうという前述の場合と同じ問題が起きた。
In addition, as a measure for preventing the occurrence of Kirkendall vacancies, a method has been proposed in which an Sn layer and a Cu layer are sequentially formed on a composite wire (Japanese Patent Laid-Open No. 1-261313). In this method, a molten Sn layer is held on the outer Cu layer and a thermal diffusion process is performed at a high temperature to shorten the thermal diffusion process time. But,
In this method, Sn is solid-dissolved in the Cu layer and consumed, so that the Sn layer is plated thicker by that amount, resulting in a longer thermal diffusion treatment time and Kirkendall vacancies. I had the same problem.

【0006】[0006]

【課題を解決するための手段】本発明はこのような状況
の中で鋭意研究を行いなされたもので、超電導特性に優
れたNb3 Sn系化合物超電導線の製造方法を提供する
ことを目的とする。即ち、本発明は、Cu−Sn系合金
基体中にNbフィラメントを多数本配列させた複合素線
上に、Sn層、及びSnより高融点でSnと非反応性の
金属材層を順次形成して複合線材となし、この複合線材
に熱拡散処理を施してCu−Sn系合金基体中にNb3
Snフィラメントを生成させることを特徴とする。
DISCLOSURE OF THE INVENTION The present invention has been earnestly studied under such circumstances, and an object thereof is to provide a method for producing an Nb 3 Sn compound superconducting wire having excellent superconducting properties. To do. That is, according to the present invention, a Sn layer and a metal material layer having a higher melting point than Sn and non-reactive with Sn are sequentially formed on a composite wire in which a large number of Nb filaments are arranged in a Cu—Sn alloy base. The composite wire is formed into a composite wire, and the composite wire is subjected to a heat diffusion treatment to form Nb 3 in the Cu—Sn alloy substrate.
It is characterized by producing Sn filaments.

【0007】本発明において、Snより高融点でSnと
非反応性の金属材層とは、熱拡散処理をSnの融点(232
℃) より高温で行っても、内側の溶融Snを均一な形状
に保持し且つ固溶や化合物形成によりSnを消費しない
金属材層である。具体的には、Cr、Ni、Zn、A
g、Co、Fe、Pd、Pt、Au等の純金属材、Ag
−Pd系、Ag−Sb系、Ag−Se系、Au−Ni
系、Au−Co系、Cu−Zn系、Cu−Sn系、Zn
−Sn系、Ni−Sn系、Co−Sn系等の合金材であ
る。前記金属材層は、Sn層を挟んで、Nbフィラメン
トを配列したCu−Sn系合金基体と合体させたとき、
Sn層のSnがNbフィラメントを配列したCu−Sn
系合金基体の方へ優先的に拡散する金属材層である。金
属材層がCu−Sn系合金等の場合はSnを飽和状態又
は飽和状態に近い量含有させておく。前記金属材層は、
融点が高い為溶融Sn層を均一形状に保持でき且つSn
と非反応性の為Sn層を薄くでき、従って熱拡散処理時
間が短縮されてカーケンダル空孔が形成されない。本発
明において、Sn層と金属材層を複合素線上に形成する
には、電気めっき、無電解めっき、溶融めっき等の厚さ
を均一に形成できる任意の方法が適用できる。前記Sn
含有合金材は、Snが拡散通過可能な為、Sn層と交互
に多層に形成することもできる。金属材層にCrを用い
る場合、Cr層は電気絶縁性の為、絶縁被覆層としての
機能を併せ持つ。そこで、超電導線を、エナメル被覆等
の処理を省略して撚合わせることも可能となる。
In the present invention, the metal material layer having a higher melting point than Sn and non-reactive with Sn is subjected to the thermal diffusion treatment by the melting point of Sn (232
Even if the temperature is higher than (.degree. C.), it is a metal material layer that keeps the molten Sn inside the uniform shape and does not consume Sn due to solid solution or compound formation. Specifically, Cr, Ni, Zn, A
Pure metal materials such as g, Co, Fe, Pd, Pt, Au, Ag
-Pd system, Ag-Sb system, Ag-Se system, Au-Ni
System, Au-Co system, Cu-Zn system, Cu-Sn system, Zn
It is an alloy material such as -Sn system, Ni-Sn system, Co-Sn system. When the metal material layer is combined with a Cu—Sn based alloy substrate in which Nb filaments are arranged with the Sn layer interposed therebetween,
Cu-Sn in which Sn of Sn layer has Nb filaments arranged
The metal material layer preferentially diffuses toward the base alloy base. When the metal material layer is a Cu-Sn alloy or the like, Sn is contained in a saturated state or in an amount close to the saturated state. The metal material layer is
Since the melting point is high, the molten Sn layer can be maintained in a uniform shape and Sn
And the Sn layer can be made thin because it is non-reactive, and therefore the thermal diffusion treatment time is shortened and Kirkendall vacancies are not formed. In the present invention, in order to form the Sn layer and the metal material layer on the composite wire, any method capable of forming a uniform thickness such as electroplating, electroless plating, and hot dipping can be applied. The Sn
Since the contained alloy material allows Sn to diffuse and pass therethrough, it can be formed in multiple layers alternately with the Sn layers. When Cr is used for the metal material layer, the Cr layer also has a function as an insulating coating layer because it is electrically insulating. Therefore, the superconducting wire can be twisted without the need for enamel coating or the like.

【0008】以下に、本発明方法の途中工程で作製され
る複合線材の熱拡散処理前後の構成を図を参照して説明
する。図1イは金属材層にNiを用いた複合線材の熱拡
散処理前の横断面図である。安定化銅線1の周囲にNb
の拡散バリヤが配され、その周囲に、Nb/ブロンズ
(Cu−Sn系合金)複合層3、ブロンズシース(パイ
プ)層4、Sn層5、Niの金属材層6が順次形成され
ている。図1ロは前記複合線材の熱拡散処理後の横断面
図である。図で7は、Nb/ブロンズ複合層3のNbフ
ィラメントがNb3 Snフィラメントに形成されたNb
3 Sn含有ブロンズ層である。このNb3 Sn含有ブロ
ンズ層7の周囲に、低Sn化したブロンズシース層4と
Sn層5の合体層8が形成され、更にその周囲にNiの
金属材層6が位置している。
The structure before and after the thermal diffusion treatment of the composite wire produced in the intermediate step of the method of the present invention will be described below with reference to the drawings. FIG. 1A is a transverse cross-sectional view of a composite wire using Ni for the metal material layer before the thermal diffusion treatment. Nb around the stabilized copper wire 1
Of the diffusion barrier, and the Nb / bronze (Cu—Sn alloy) composite layer 3, the bronze sheath (pipe) layer 4, the Sn layer 5, and the Ni metal material layer 6 are sequentially formed around the diffusion barrier. FIG. 1B is a cross-sectional view of the composite wire after the thermal diffusion treatment. In FIG. 7, Nb filaments of the Nb / bronze composite layer 3 are Nb 3 Sn filaments formed into Nb 3 Sn filaments.
3 Sn-containing bronze layer. Around the Nb 3 Sn-containing bronze layer 7, a united layer 8 of the bronze sheath layer 4 and the Sn layer 5 having a low Sn content is formed, and a Ni metal layer 6 is located around the united layer 8.

【0009】図2イは、金属材層にブロンズを用いた複
合線材の熱拡散処理前の横断面図である。最外層にブロ
ンズの金属材層9が形成されている他は、図1イに示し
たものと同じである。図2ロは熱拡散処理後の横断面図
である。最外層にブロンズの金属材層9が形成されてい
る他は、図1ロに示したものと同じである。
FIG. 2A is a cross-sectional view of a composite wire using bronze as a metal material layer before heat diffusion treatment. It is the same as that shown in FIG. 1A except that the bronze metal material layer 9 is formed on the outermost layer. FIG. 2B is a cross-sectional view after the thermal diffusion process. It is the same as that shown in FIG. 1B except that the bronze metal material layer 9 is formed on the outermost layer.

【0010】本発明において、複合線材全体に含有され
るSn量は、16wt%以上において十分なSn量が供給さ
れて超電導特性に優れた、ストイキオメトリ(Nb−25
at%Sn)に近いNb3 Sn相が形成される。従って、
複合線材全体に含有されるSnの量は16wt%以上である
ことが望ましい。
In the present invention, when the total amount of Sn contained in the composite wire is 16 wt% or more, a sufficient amount of Sn is supplied, and the stoichiometry (Nb-25) is excellent in superconducting properties.
A Nb 3 Sn phase close to at% Sn) is formed. Therefore,
The amount of Sn contained in the entire composite wire is preferably 16 wt% or more.

【0011】又複合素線上に形成するSn層の厚さtと
Snより高融点でSnと非反応性の金属材層の厚さTの
比〔t/T〕が1未満では金属材層が過剰に厚くなり不
経済である。又10を超えては前記金属材層の溶融Snの
保持効果が低下する。従って、複合線材のSn層の厚さ
tとSnより高融点でSnと非反応性の金属材層の厚さ
Tの比〔t/T〕は1以上、10以下であることが望まし
い。
If the ratio [t / T] of the thickness t of the Sn layer formed on the composite wire to the thickness T of the metal material layer having a higher melting point than Sn and not reacting with Sn is less than 1, the metal material layer is It becomes uneconomical because it becomes excessively thick. On the other hand, if it exceeds 10, the effect of retaining the molten Sn of the metal material layer decreases. Therefore, it is preferable that the ratio [t / T] of the thickness t of the Sn layer of the composite wire and the thickness T of the metal material layer having a higher melting point than Sn and not reacting with Sn is 1 or more and 10 or less.

【0012】本発明は、Cu−Sn系合金基体又はNb
フィラメントにTi、Ta、Ha、Ga等の元素を微量
含有させた場合にも同様の効果が得られる。又中心部に
Cu又はAl等の安定化材をNbやTa等のバリヤ層を
介在させて複合したNb3 Sn系化合物超電導線に適用
しても同様の効果が得られる。
The present invention is based on a Cu--Sn alloy substrate or Nb.
Similar effects can be obtained when the filament contains a trace amount of elements such as Ti, Ta, Ha, and Ga. The stabilizing material of Nb and Ta same effect by applying a barrier layer to Nb 3 Sn compound superconducting wire in complex with the interposition of such as Cu or Al can be obtained in the center.

【0013】本発明において、熱拡散処理は、通常、S
n層をCu−Sn系合金基体中に拡散させる低温処理と
前記基体中のSnをNbと反応させてNb3 Sn相を形
成する高温処理に分けて行われる。低温処理もSnの融
点以上の温度で短時間行うことにより、カーケンダル空
孔の発生を抑えることができる。もしカーケンダル空孔
が発生しても、その量は僅かであり、高温処理前に軽圧
延して消滅させることができる。
In the present invention, the thermal diffusion treatment is usually S
The n layer and low-temperature treatment to diffuse into the Cu-Sn-based alloy substrate of Sn in the substrate is reacted with Nb is performed by dividing into high-temperature treatment for forming a Nb 3 Sn phase. Generation of Kirkendall vacancies can be suppressed by performing low-temperature treatment for a short time at a temperature equal to or higher than the melting point of Sn. If Kirkendall vacancies occur, the amount is small and can be eliminated by light rolling before the high temperature treatment.

【0014】[0014]

【作用】本発明では、Nb3 Sn系化合物超電導線を外
部拡散法で製造する際に、複合素線上の溶融Snを、高
融点でSnと非反応性の金属材層で保持するので、Sn
の熱拡散処理を高温短時間で行うことができる。従って
基体中に空孔が生成したりせず、超電導特性に優れたN
3 Sn系化合物超電導線を製造できる。
In the present invention, when the Nb 3 Sn compound superconducting wire is manufactured by the external diffusion method, the molten Sn on the composite wire is held by the metal material layer having a high melting point and not reacting with Sn.
The heat diffusion treatment can be performed at high temperature in a short time. Therefore, no pores are formed in the substrate, and N having excellent superconducting properties is obtained.
A b 3 Sn-based compound superconducting wire can be manufactured.

【0015】[0015]

【実施例】以下に本発明を実施例により詳細に説明す
る。 (実施例1)外径45.3mmφのブロンズ(Cu−14.3wt%
Sn−0.2 wt%Ti系合金)棒材に6.0 mmφの貫通孔を
等間隔に19本あけ、この貫通孔に外径5.8 mmφのNb線
材を挿入し、ブロンズ棒材の前後端にブロンズ製蓋を電
子ビーム溶接により真空封止して被せて1次ビレットを
作製した。次にこの1次ビレットを熱間押出しし、この
押出材に伸線加工と中間焼鈍を繰返し施して、対辺長さ
1mmの六角線を作製した。この六角線を1次ビレットと
同じ組成の外径45mmφ、内径38mmφのブロンズ製パイプ
に充填して2次ビレットを作製した。前記ブロンズ製パ
イプの中心部分には安定化材となす直径20mmφの無酸素
銅棒を外周にNb箔を巻いて配置した。この2次ビレッ
トを1次ビレットと同じ方法により 0.7mmφの複合素線
に加工した。次にこの複合素線上にSn層とNi層を順
次電気めっきして複合線材を作製した。Sn層とNi層
は厚さを種々に変化させた。次にこの複合線材に1回目
の熱拡散処理を 450℃で50時間施した。熱拡散処理後、
組織観察をした。Sn層のSnがブロンズ基体内に 100
μm程度均一に拡散していた。Sn層の溶落はなかっ
た。Nbフィラメントはブロンズ基体内に直線状に等間
隔に位置しており、乱れは見られなかった。ブロンズ基
体内にカーケンダル空孔が少量観察された。次にこの線
材に断面減少率5%の伸線加工を施して、線材の外径を
整え又線材内部のカーケンダル空孔を消滅させた。次い
で2回目の熱拡散処理を 695℃で40時間施してNb3
n系化合物超電導線を製造した。
The present invention will be described below in detail with reference to examples. (Example 1) Bronze with an outer diameter of 45.3 mmφ (Cu-14.3 wt%
Sn-0.2 wt% Ti-based alloy) 19 holes with 6.0 mmφ through holes at regular intervals, insert Nb wire with 5.8 mmφ outside diameter into these holes, and bronze lids at the front and rear ends of the bronze rod. Was vacuum-sealed by electron beam welding and covered to prepare a primary billet. Next, this primary billet was hot extruded, and this extruded material was repeatedly subjected to wire drawing and intermediate annealing to produce a hexagonal wire having an opposite side length of 1 mm. This hexagonal wire was filled into a bronze pipe having the same composition as the primary billet and having an outer diameter of 45 mmφ and an inner diameter of 38 mmφ to produce a secondary billet. At the center of the bronze pipe, an oxygen-free copper rod having a diameter of 20 mm, which serves as a stabilizing material, was arranged by winding Nb foil on the outer circumference. This secondary billet was processed into a composite wire of 0.7 mmφ by the same method as the primary billet. Next, a Sn layer and a Ni layer were sequentially electroplated on this composite wire to prepare a composite wire. The thicknesses of the Sn layer and the Ni layer were variously changed. Next, this composite wire was subjected to the first thermal diffusion treatment at 450 ° C. for 50 hours. After thermal diffusion treatment,
The tissue was observed. Sn of Sn layer is 100 in the bronze substrate.
It was diffused uniformly by about μm. There was no burnout of the Sn layer. The Nb filaments were linearly positioned in the bronze substrate at equal intervals, and no turbulence was observed. A small amount of Kirkendall pores were observed in the bronze substrate. Next, this wire rod was subjected to wire drawing at a cross-section reduction rate of 5% to adjust the outer diameter of the wire rod and eliminate Kirkendall pores inside the wire rod. Then, the second thermal diffusion treatment was performed at 695 ° C for 40 hours to obtain Nb 3 S.
An n-based compound superconducting wire was manufactured.

【0016】(実施例2)実施例1において、複合素線
上にSn層及びCu−10wt%Sn合金層を順次電気めっ
きして複合線材とした他は、実施例1と同じ方法により
Nb3 Sn系化合物超電導線を製造した。
Example 2 Nb 3 Sn was prepared by the same method as in Example 1 except that the Sn layer and the Cu-10 wt% Sn alloy layer were sequentially electroplated on the composite wire to form a composite wire. A compound superconducting wire was manufactured.

【0017】(比較例1)実施例1において、複合素線
にSn層を8μm厚さに、その上にCu層を 1.5μm厚
さにめっきした他は、実施例1と同じ方法によりNb3
Sn系化合物超電導線を製造した。
(Comparative Example 1) Nb 3 was prepared in the same manner as in Example 1 except that a Sn layer was plated on the composite wire to a thickness of 8 μm and a Cu layer was plated thereon to a thickness of 1.5 μm.
An Sn-based compound superconducting wire was manufactured.

【0018】(比較例2)実施例1において、複合素線
にSn層を14μm厚さに、その上にCu層を 2.5μm厚
さにめっきし、1回目の熱拡散処理を 450℃で 100時間
施した他は、実施例1と同じ方法によりNb3 Sn系化
合物超電導線を製造した。
(Comparative Example 2) In Example 1, an Sn layer was plated on the composite wire to a thickness of 14 μm, and a Cu layer was plated thereon to a thickness of 2.5 μm, and the first thermal diffusion treatment was performed at 450 ° C. for 100 minutes. An Nb 3 Sn-based compound superconducting wire was manufactured by the same method as in Example 1 except that the time was applied.

【0019】(比較例3)実施例1において、複合素線
にSn層のみを8μm厚さに形成した他は、実施例1と
同じ方法によりNb3 Sn系化合物超電導線を製造し
た。
(Comparative Example 3) A Nb 3 Sn-based compound superconducting wire was manufactured in the same manner as in Example 1, except that only the Sn layer was formed to a thickness of 8 μm on the composite element wire.

【0020】(比較例4)実施例1において、複合素線
にSn層のみを8μm厚さに形成して複合線材となし、
この複合線材にSnの融点未満の 200℃の温度で60時
間、次に 300℃の温度で50時間、最後に 695℃の温度で
40時間の加熱条件で熱拡散処理を施した他は、実施例1
と同じ方法によりNb3 Sn系化合物超電導線を製造し
た。
(Comparative Example 4) In Example 1, only a Sn layer was formed on the composite wire to a thickness of 8 μm to form a composite wire.
This composite wire is heated at a temperature of 200 ° C below the melting point of Sn for 60 hours, then at 300 ° C for 50 hours, and finally at 695 ° C.
Example 1 except that the heat diffusion treatment was performed under heating conditions for 40 hours
A Nb 3 Sn-based compound superconducting wire was manufactured by the same method as described above.

【0021】得られた各々のNb3 Sn系化合物超電導
線について、臨界電流(Ic)を測定した。又断面を観
察してSnの溶落有無、カーケンダル空孔の有無を調べ
た。結果を表1に示す。
The critical current (Ic) was measured for each of the obtained Nb 3 Sn-based compound superconducting wires. Also, the cross section was observed to examine the presence or absence of Sn burn-out and the presence or absence of Kirkendall pores. The results are shown in Table 1.

【0022】[0022]

【表1】 [Table 1]

【0023】表1より明らかなように、本発明方法品
(No.1〜10) はいずれもIcが高く、Snの溶落がなく
断面形状に優れ、カーケンダル空孔は小さいか、又は少
なかった。尚、No.2はSnの平均濃度が16wt%を下回っ
た為Icが若干低下した。No.6はSn層の厚さに対して
金属材層(Ni層)がやや厚過ぎて不経済であったが、
特性上問題なかった。No.7は金属材層(Ni層)が薄く
Sn層の保持力が弱くなり断面がやや変形し、Icも幾
分低下した。但し、実用上問題ない程度であった。
As is clear from Table 1, all the products of the method of the present invention (Nos. 1 to 10) had high Ic, no Sn burn-through, excellent cross-sectional shape, and small or few Kirkendall pores. . Incidentally, in No. 2, the average Sn concentration was below 16 wt%, so that Ic was slightly lowered. No. 6 was uneconomical because the metal material layer (Ni layer) was slightly thicker than the Sn layer thickness,
There was no problem in terms of characteristics. In No. 7, the metal material layer (Ni layer) was thin, the coercive force of the Sn layer was weakened, the cross-section was slightly deformed, and Ic was also slightly lowered. However, there was no problem in practical use.

【0024】これに対し、比較例品のNo.11 はSn層上
にCu層を形成した為、Sn層がCu層に消費されてS
nが不足し、Icが低下した。No.12 はSn層を厚く形
成したので、熱拡散処理時間が長くなり、カーケンダル
空孔が多量に発生し、軽圧下後も残存してIcを低下さ
せた。No.13 は高融点金属材層を用いず、しかも始めか
ら 450℃の温度で熱拡散処理を施した為、Sn層が溶落
しNb3 Snフィラメントが露出してIcが著しく低下
した。No.14 は熱拡散処理をSnの融点未満の低温から
始めたので、Sn層の溶落は防止できたが、カーケンダ
ル空孔が多量に発生し、軽圧下後も残存してIcが低下
した。
On the other hand, in No. 11 of the comparative example, since the Cu layer was formed on the Sn layer, the Sn layer was consumed by the Cu layer and S
n was insufficient and Ic was lowered. In No. 12, since the Sn layer was formed thickly, the heat diffusion treatment time became long, a large number of Kirkendall vacancies were generated, and it remained even after light pressure reduction to lower Ic. In No. 13, the high melting point metal material layer was not used, and since the thermal diffusion treatment was performed at a temperature of 450 ° C. from the beginning, the Sn layer was burned out, the Nb 3 Sn filament was exposed, and the Ic was significantly lowered. In No. 14, the thermal diffusion treatment was started at a temperature lower than the melting point of Sn, so the burnout of the Sn layer could be prevented, but a large number of Kirkendall vacancies were generated and the Ic was reduced even after the pressure was reduced. .

【0025】[0025]

【効果】以上述べたように、本発明によれば、高融点で
Snと非反応性の金属材層が、複合素線上の溶融Snを
保持するので、Snの熱拡散処理を高温短時間で行うこ
とができる。又熱拡散処理を高温短時間で行うので、基
体中の空孔の成長も抑えられて、超電導特性に優れたN
3 Sn系化合物超電導線が得られる。
As described above, according to the present invention, since the metal material layer having a high melting point and non-reactive with Sn holds the molten Sn on the composite wire, the thermal diffusion treatment of Sn can be performed at high temperature in a short time. It can be carried out. Further, since the thermal diffusion treatment is carried out at a high temperature in a short time, the growth of holes in the substrate can be suppressed, and N having excellent superconducting characteristics can be obtained.
A b 3 Sn-based compound superconducting wire is obtained.

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

【図1】本発明における複合線材の熱拡散処理前後の態
様を示す横断面図である。
FIG. 1 is a cross-sectional view showing aspects of a composite wire according to the present invention before and after thermal diffusion treatment.

【図2】本発明における複合線材の熱拡散処理前後の他
の態様を示す横断面図である。
FIG. 2 is a cross-sectional view showing another embodiment before and after the thermal diffusion treatment of the composite wire according to the present invention.

【符号の説明】[Explanation of symbols]

1──安定化銅線 2──Nb箔 3──Nb/ブロンズ複合層 4──ブロンズシース層 5──Sn層 6──Niの金属材層 7──Nb3 Sn含有ブロンズ層 8──ブロンズシース層とSn層の合体層 9──ブロンズの金属材層1--Stabilized copper wire 2 --Nb foil 3 --Nb / bronze composite layer 4 --Bronze sheath layer 5 --Sn layer 6 --Ni metal material layer 7 --Nb 3 Sn-containing bronze layer 8- -Bronze sheath layer and Sn layer combined layer 9 --- Bronze metal material layer

─────────────────────────────────────────────────────
─────────────────────────────────────────────────── ───

【手続補正書】[Procedure amendment]

【提出日】平成7年3月24日[Submission date] March 24, 1995

【手続補正1】[Procedure Amendment 1]

【補正対象書類名】明細書[Document name to be amended] Statement

【補正対象項目名】全文[Correction target item name] Full text

【補正方法】変更[Correction method] Change

【補正内容】[Correction content]

【書類名】 明細書[Document name] Statement

【発明の名称】 Nb3 Sn系化合物超電導線の製造方
Title: Method for producing Nb 3 Sn compound superconducting wire

【特許請求の範囲】[Claims]

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

【0001】[0001]

【産業上の利用分野】本発明は、超電導特性に優れた、
Nb3 Sn系化合物超電導線の製造方法に関する。
BACKGROUND OF THE INVENTION The present invention has excellent superconducting properties,
The present invention relates to a method for producing a Nb 3 Sn-based compound superconducting wire.

【0002】[0002]

【従来の技術】化合物超電導線はCu又はCu合金基体
中にNb3 Sn、Nb3 Al、V3 Ga等の超電導フィ
ラメントが多数本複合された超電導線である。この化合
物超電導線はNb3 Sn等の超電導体相が脆い為、次の
ようにして製造される。即ち、Cu−Sn系合金基体中
にNb金属の棒材を多数本埋込んで一次ビレットを組立
て、これに中間焼鈍と縮径加工を施して所定形状の線状
体とし、この線状体をCu−Sn系合金パイプ内に多数
本整列充填して二次ビレットを組立て、これに中間焼鈍
と縮径加工を施してCu−Sn系合金基体中にNbフィ
ラメントが複合された複合素線を作製する。次に、この
複合素線に 700〜800 ℃の温度で熱拡散処理を施して、
前記Nbフィラメントを前記基体及びパイプ中のSnと
反応させてNb3 Snフィラメントに形成する。
2. Description of the Related Art A compound superconducting wire is a superconducting wire in which a large number of superconducting filaments such as Nb 3 Sn, Nb 3 Al and V 3 Ga are compounded in a Cu or Cu alloy substrate. This compound superconducting wire is manufactured as follows because the superconductor phase such as Nb 3 Sn is fragile. That is, a large number of Nb metal rods are embedded in a Cu-Sn alloy substrate to assemble a primary billet, which is then annealed and reduced in diameter to form a linear body having a predetermined shape. A large number of Cu-Sn alloy pipes are aligned and filled to assemble a secondary billet, which is then annealed and reduced in diameter to produce a composite element wire in which Nb filaments are compounded in a Cu-Sn alloy substrate. To do. Next, this composite wire is subjected to thermal diffusion treatment at a temperature of 700 to 800 ° C,
The Nb filaments are reacted with Sn in the substrate and pipe to form Nb 3 Sn filaments.

【0003】前述の製造方法では、基体又はパイプを構
成するCu−Sn系合金のSn濃度が高い程、生成する
Nb3 Sn化合物は化学量論組成に近くなり、得られる
超電導線の超電導特性が向上する。しかし、前記Cu−
Sn系合金のSn濃度を高くするとビレットの加工硬化
が大きくなり、特にSnが固溶限を超えて含有される
と、中間焼鈍を多数回入れても伸線加工時に割れが生じ
た。この為Cu−Sn系合金中のSn量は固溶限以下に
抑えざるを得ず、従ってSnの量が不足して十分に高い
超電導特性が得られなかった。又中間焼鈍はNb3 Sn
相が生成しない低い温度で施す為長時間を要し、生産性
を著しく害した。
[0003] In the above manufacturing method, the higher the Sn concentration of the Cu-Sn-based alloy constituting the substrate or pipe, resulting Nb 3 Sn compound is close to the stoichiometric composition, superconducting properties of the resulting superconducting wire improves. However, the Cu-
When the Sn concentration of the Sn-based alloy is increased, the work hardening of the billet becomes large, and especially when Sn is contained in excess of the solid solution limit, cracking occurred during wire drawing even if the intermediate annealing was performed many times. For this reason, the amount of Sn in the Cu-Sn alloy has to be suppressed below the solid solution limit. Therefore, the amount of Sn is insufficient and a sufficiently high superconducting property cannot be obtained. In addition, the intermediate annealing is Nb 3 Sn
Since it was applied at a low temperature at which no phase was formed, it took a long time and markedly impaired the productivity.

【0004】[0004]

【発明が解決しようとする課題】そこで、基体及びパイ
プに、加工性の良い低Sn濃度のCu−Sn系合金を用
いて中間焼鈍の回数を減らし、Snの不足分は、複合素
線上にSnをめっきして補給する外部拡散法が開発され
た。この外部拡散法では、熱拡散処理をいきなり700℃
以上の高温度で施すとSnめっき層やSnリッチのCu
−Sn系化合物が溶落し、不足して所望の超電導特性が
得られなかった。そこで、熱拡散処理を、先ずSnの融
点未満の温度でCu−Sn系合金基体中にSn層を拡散
させ、次いで 300℃前後の温度でSnの拡散を促進し、
最後に 700℃以上の高温でNb3 Sn相を反応生成させ
るという3段階に分けて施す方法(特公昭62-62003号)
が提案された。しかし、このように熱拡散処理を低温度
から徐々に行う方法では、CuとSn原子の拡散速度が
異なることから、Cu−Sn系合金基体中にカーケンダ
ル効果による空孔(以下カーケンダル空孔と略記する)
が生じた。この空孔は超電導線の歪み感受性を大きくし
て、超電導特性を低下させ又不安定にした。このカーケ
ンダル空孔の発生防止策として、複合線材を 0.3mmφ以
下に細くしてSnの拡散時間を短縮する方法が提案され
た。この方法では、二次ビレットの組立てに際し、細い
複合線材を整列充填するのに大変な手間を要した。
Therefore, the number of intermediate annealings is reduced by using a Cu-Sn type alloy having a low Sn concentration with good workability for the substrate and the pipe. An outdiffusion method has been developed to plate and replenish. In this external diffusion method, the thermal diffusion process is suddenly performed at 700 ° C.
When applied at the above high temperature, Sn plating layer and Sn rich Cu
The -Sn-based compound was burned out and insufficient, and desired superconducting properties were not obtained. Therefore, a thermal diffusion treatment is carried out by first diffusing the Sn layer in the Cu—Sn alloy base at a temperature lower than the melting point of Sn, and then promoting the diffusion of Sn at a temperature of around 300 ° C.
Finally, a method in which the Nb 3 Sn phase is formed by reaction at a high temperature of 700 ° C or higher in three steps (Japanese Patent Publication No. 62-62003).
Was proposed. However, in such a method in which the thermal diffusion treatment is gradually performed from a low temperature, since the diffusion rates of Cu and Sn atoms are different, holes in the Cu—Sn alloy substrate due to the Kirkendall effect (hereinafter abbreviated as Kirkendall holes). Do)
Occurred. These vacancies increased the strain sensitivity of the superconducting wire, deteriorating the superconducting property and making it unstable. As a measure for preventing the occurrence of Kirkendall pores, a method has been proposed in which the composite wire is thinned to 0.3 mm or less to shorten the Sn diffusion time. According to this method, it takes a great deal of time to align and fill the thin composite wire rod when assembling the secondary billet.

【0005】この他、カーケンダル空孔の発生防止策と
して、複合素線上にSn層とCu層を順次形成する方法
が提案された(特開平1-232613号)。この方法は、外周
のCu層に溶融Sn層を保持させて高温で熱拡散処理を
行い、熱拡散処理時間を短縮するものである。しかし、
この方法ではSnがCu層に固溶して消費される為、そ
の分Sn層を厚くめっきすることになり、その結果熱拡
散処理時間が長くなって、カーケンダル空孔が生じてし
まうという前述の場合と同じ問題が起きた。
In addition, as a measure for preventing the occurrence of Kirkendall vacancies, a method has been proposed in which an Sn layer and a Cu layer are sequentially formed on a composite wire (Japanese Patent Laid-Open No. 1-261313). In this method, a molten Sn layer is held on the outer Cu layer and a thermal diffusion process is performed at a high temperature to shorten the thermal diffusion process time. But,
In this method, Sn is solid-dissolved in the Cu layer and consumed, so that the Sn layer is plated thicker by that amount, resulting in a longer thermal diffusion treatment time and Kirkendall vacancies. I had the same problem.

【0006】[0006]

【課題を解決するための手段】本発明はこのような状況
の中で鋭意研究を行いなされたもので、超電導特性に優
れたNb3 Sn系化合物超電導線の製造方法を提供する
ことを目的とする。即ち、本発明は、Cu−Sn系合金
基体中にNbフィラメントを多数本配列させた複合素線
上に、Sn層、及びSnより高融点の金属材層を順次形
成して複合線材となし、この複合線材に熱拡散処理を施
してCu−Sn系合金基体中にNb3 Snフィラメント
を生成させるNb3 Sn系化合物超電導線の製造方法で
あって、前記金属材層は、Sn層のSnがNbフィラメ
ントを配列したCu−Sn系合金基体の方へ優先的に拡
散する金属材層であることを特徴とするNb3 Sn系化
合物超電導線の製造方法である。
DISCLOSURE OF THE INVENTION The present invention has been earnestly studied under such circumstances, and an object thereof is to provide a method for producing an Nb 3 Sn compound superconducting wire having excellent superconducting properties. To do. That is, according to the present invention, a Sn wire and a metal material layer having a higher melting point than Sn are sequentially formed on a composite wire in which a large number of Nb filaments are arranged in a Cu-Sn alloy base to form a composite wire. a method of manufacturing a composite wire in Nb 3 Sn compound superconducting wire to produce Nb 3 Sn filaments is subjected to thermal diffusion treatment in the Cu-Sn-based alloy substrate, the metal material layer, Sn of the Sn layer is Nb a method for producing a Nb 3 Sn compound superconducting wire which is a metal material layer to diffuse preferentially towards the Cu-Sn-based alloy substrate having an array of filaments.

【0007】本発明において、金属材層とは、熱拡散処
理をSnの融点(232℃) より高温で行っても、内側の溶
融Snを均一な形状に保持し且つ固溶や化合物形成によ
りSnを消費しない金属材層である。具体的には、C
r、Ni、Zn、Ag、Co、Fe、Pd、Pt、Au
等の純金属材、Ag−Pd系、Ag−Sb系、Ag−S
e系、Au−Ni系、Au−Co系、Cu−Zn系、C
u−Sn系、Zn−Sn系、Ni−Sn系、Co−Sn
系等の合金材である。前記金属材層は、Sn層を挟ん
で、Nbフィラメントを配列したCu−Sn系合金基体
と合体させたとき、Sn層のSnがNbフィラメントを
配列したCu−Sn系合金基体の方へ優先的に拡散する
金属材層である。金属材層がCu−Sn系合金等の場合
はSnを飽和状態又は飽和状態に近い量含有させてお
く。前記金属材層は、融点が高い為溶融Sn層を均一形
状に保持でき、又Sn層を消費せず、更にSn層のSn
がNbフィラメントを配列したCu−Sn系合金基体の
方へ優先的に拡散するものなので、Sn層を薄くでき
る。従って熱拡散処理時間が短縮されてカーケンダル空
孔が形成されない。本発明において、Sn層と金属材層
を複合素線上に形成するには、電気めっき、無電解めっ
き、溶融めっき等の厚さを均一に形成できる任意の方法
が適用できる。前記Sn含有合金材は、Snが拡散通過
可能な為、Sn層と交互に多層に形成することもでき
る。金属材層にCrを用いる場合、Cr層は電気絶縁性
の為、絶縁被覆層としての機能を併せ持つ。そこで、超
電導線を、エナメル被覆等の処理を省略して撚合わせる
ことも可能となる。
In the present invention, the metallic material layer means that even if the thermal diffusion treatment is carried out at a temperature higher than the melting point of Sn (232 ° C.), the inner molten Sn is kept in a uniform shape and is formed by solid solution or compound formation. Is a metal material layer that does not consume. Specifically, C
r, Ni, Zn, Ag, Co, Fe, Pd, Pt, Au
Pure metal materials such as Ag-Pd system, Ag-Sb system, Ag-S
e type, Au-Ni type, Au-Co type, Cu-Zn type, C
u-Sn system, Zn-Sn system, Ni-Sn system, Co-Sn
It is an alloy material such as series. When the metal material layer is combined with a Cu—Sn based alloy base body in which Nb filaments are arranged with the Sn layer interposed therebetween, Sn in the Sn layer is preferentially directed to the Cu—Sn base alloy base body in which Nb filaments are arranged. It is a metal material layer that diffuses into the. When the metal material layer is a Cu-Sn alloy or the like, Sn is contained in a saturated state or in an amount close to the saturated state. Since the metal material layer has a high melting point, the molten Sn layer can be held in a uniform shape, and the Sn layer is not consumed.
Is preferentially diffused toward the Cu-Sn based alloy substrate in which Nb filaments are arranged, so that the Sn layer can be thinned. Therefore, the thermal diffusion treatment time is shortened and Kirkendall vacancies are not formed. In the present invention, in order to form the Sn layer and the metal material layer on the composite wire, any method capable of forming a uniform thickness such as electroplating, electroless plating, and hot dipping can be applied. Since the Sn-containing alloy material allows Sn to diffuse and pass therethrough, it can be formed in multiple layers alternately with the Sn layers. When Cr is used for the metal material layer, the Cr layer also has a function as an insulating coating layer because it is electrically insulating. Therefore, the superconducting wire can be twisted without the need for enamel coating or the like.

【0008】以下に、本発明方法の途中工程で作製され
る複合線材の熱拡散処理前後の構成を図を参照して説明
する。図1イは金属材層にNiを用いた複合線材の熱拡
散処理前の横断面図である。安定化銅線1の周囲にNb
の拡散バリヤが配され、その周囲に、Nb/ブロンズ
(Cu−Sn系合金)複合層3、ブロンズシース(パイ
プ)層4、Sn層5、Niの金属材層6が順次形成され
ている。図1ロは前記複合線材の熱拡散処理後の横断面
図である。図で7は、Nb/ブロンズ複合層3のNbフ
ィラメントがNb3 Snフィラメントに形成されたNb
3 Sn含有ブロンズ層である。このNb3 Sn含有ブロ
ンズ層7の周囲に、低Sn化したブロンズシース層4と
Sn層5の合体層8が形成され、更にその周囲にNiの
金属材層6が位置している。
The structure before and after the thermal diffusion treatment of the composite wire produced in the intermediate step of the method of the present invention will be described below with reference to the drawings. FIG. 1A is a transverse cross-sectional view of a composite wire using Ni for the metal material layer before the thermal diffusion treatment. Nb around the stabilized copper wire 1
Of the diffusion barrier, and the Nb / bronze (Cu—Sn alloy) composite layer 3, the bronze sheath (pipe) layer 4, the Sn layer 5, and the Ni metal material layer 6 are sequentially formed around the diffusion barrier. FIG. 1B is a cross-sectional view of the composite wire after the thermal diffusion treatment. In FIG. 7, Nb filaments of the Nb / bronze composite layer 3 are Nb 3 Sn filaments formed into Nb 3 Sn filaments.
3 Sn-containing bronze layer. Around the Nb 3 Sn-containing bronze layer 7, a united layer 8 of the bronze sheath layer 4 and the Sn layer 5 having a low Sn content is formed, and a Ni metal layer 6 is located around the united layer 8.

【0009】図2イは、金属材層にブロンズを用いた複
合線材の熱拡散処理前の横断面図である。最外層にブロ
ンズの金属材層9が形成されている他は、図1イに示し
たものと同じである。図2ロは熱拡散処理後の横断面図
である。最外層にブロンズの金属材層9が形成されてい
る他は、図1ロに示したものと同じである。
FIG. 2A is a cross-sectional view of a composite wire using bronze as a metal material layer before heat diffusion treatment. It is the same as that shown in FIG. 1A except that the bronze metal material layer 9 is formed on the outermost layer. FIG. 2B is a cross-sectional view after the thermal diffusion process. It is the same as that shown in FIG. 1B except that the bronze metal material layer 9 is formed on the outermost layer.

【0010】本発明において、複合線材全体に含有され
るSn量は、16wt%以上において十分なSn量が供給さ
れて超電導特性に優れた、ストイキオメトリ(Nb−25
at%Sn)に近いNb3 Sn相が形成される。従って、
複合線材全体に含有されるSnの量は16wt%以上である
ことが望ましい。
In the present invention, when the total amount of Sn contained in the composite wire is 16 wt% or more, a sufficient amount of Sn is supplied, and the stoichiometry (Nb-25) is excellent in superconducting properties.
A Nb 3 Sn phase close to at% Sn) is formed. Therefore,
The amount of Sn contained in the entire composite wire is preferably 16 wt% or more.

【0011】又複合素線上に形成するSn層の厚さtと
前記金属材層の厚さTの比〔t/T〕が1未満では金属
材層が過剰に厚くなり不経済である。又10を超えては前
記金属材層の溶融Snの保持効果が低下する。従って、
複合線材のSn層の厚さtと前記金属材層の厚さTの比
〔t/T〕は1以上、10以下であることが望ましい。
If the ratio [t / T] of the thickness t of the Sn layer formed on the composite wire and the thickness T of the metal material layer is less than 1, the metal material layer becomes excessively thick, which is uneconomical. On the other hand, if it exceeds 10, the effect of retaining the molten Sn of the metal material layer decreases. Therefore,
The ratio [t / T] of the thickness t of the Sn layer of the composite wire and the thickness T of the metal layer is preferably 1 or more and 10 or less.

【0012】本発明は、Cu−Sn系合金基体又はNb
フィラメントにTi、Ta、Ha、Ga等の元素を微量
含有させた場合にも同様の効果が得られる。又中心部に
Cu又はAl等の安定化材をNbやTa等のバリヤ層を
介在させて複合したNb3 Sn系化合物超電導線に適用
しても同様の効果が得られる。
The present invention is based on a Cu--Sn alloy substrate or Nb.
Similar effects can be obtained when the filament contains a trace amount of elements such as Ti, Ta, Ha, and Ga. The stabilizing material of Nb and Ta same effect by applying a barrier layer to Nb 3 Sn compound superconducting wire in complex with the interposition of such as Cu or Al can be obtained in the center.

【0013】本発明において、熱拡散処理は、通常、S
n層をCu−Sn系合金基体中に拡散させる低温処理と
前記基体中のSnをNbと反応させてNb3 Sn相を形
成する高温処理に分けて行われる。低温処理もSnの融
点以上の温度で短時間行うことにより、カーケンダル空
孔の発生を抑えることができる。もしカーケンダル空孔
が発生しても、その量は僅かであり、高温処理前に軽圧
延して消滅させることができる。
In the present invention, the thermal diffusion treatment is usually S
The n layer and low-temperature treatment to diffuse into the Cu-Sn-based alloy substrate of Sn in the substrate is reacted with Nb is performed by dividing into high-temperature treatment for forming a Nb 3 Sn phase. Generation of Kirkendall vacancies can be suppressed by performing low-temperature treatment for a short time at a temperature equal to or higher than the melting point of Sn. If Kirkendall vacancies occur, the amount is small and can be eliminated by light rolling before the high temperature treatment.

【0014】[0014]

【作用】本発明では、Nb3 Sn系化合物超電導線を外
部拡散法で製造する際に、複合素線上の溶融Snを、S
nより高融点で、Snを消費せず、Sn層のSnがNb
フィラメントを配列したCu−Sn系合金基体の方へ優
先的に拡散する金属材層で保持するので、Snの熱拡散
処理を高温短時間で行うことができる。従って基体中に
空孔が生成したりせず、超電導特性に優れたNb3 Sn
系化合物超電導線を製造できる。
In the present invention, when the Nb 3 Sn compound superconducting wire is produced by the external diffusion method, the molten Sn on the composite wire is
The melting point is higher than n, Sn is not consumed, and Sn in the Sn layer is Nb.
Since the metal material layer preferentially diffuses toward the Cu—Sn alloy base body in which the filaments are arranged, the thermal diffusion treatment of Sn can be performed at high temperature in a short time. Therefore, no holes are formed in the substrate, and Nb 3 Sn excellent in superconducting properties is obtained.
A system compound superconducting wire can be manufactured.

【0015】[0015]

【実施例】以下に本発明を実施例により詳細に説明す
る。 (実施例1)外径45.3mmφのブロンズ(Cu−14.3wt%
Sn−0.2 wt%Ti系合金)棒材に6.0 mmφの貫通孔を
等間隔に19本あけ、この貫通孔に外径5.8 mmφのNb線
材を挿入し、ブロンズ棒材の前後端にブロンズ製蓋を電
子ビーム溶接により真空封止して被せて1次ビレットを
作製した。次にこの1次ビレットを熱間押出しし、この
押出材に伸線加工と中間焼鈍を繰返し施して、対辺長さ
1mmの六角線を作製した。この六角線を1次ビレットと
同じ組成の外径45mmφ、内径38mmφのブロンズ製パイプ
に充填して2次ビレットを作製した。前記ブロンズ製パ
イプの中心部分には安定化材となす直径20mmφの無酸素
銅棒を外周にNb箔を巻いて配置した。この2次ビレッ
トを1次ビレットと同じ方法により 0.7mmφの複合素線
に加工した。次にこの複合素線上にSn層とNi層を順
次電気めっきして複合線材を作製した。Sn層とNi層
は厚さを種々に変化させた。次にこの複合線材に1回目
の熱拡散処理を 450℃で50時間施した。熱拡散処理後、
組織観察をした。Sn層のSnがブロンズ基体内に 100
μm程度均一に拡散していた。Sn層の溶落はなかっ
た。Nbフィラメントはブロンズ基体内に直線状に等間
隔に位置しており、乱れは見られなかった。ブロンズ基
体内にカーケンダル空孔が少量観察された。次にこの線
材に断面減少率5%の伸線加工を施して、線材の外径を
整え又線材内部のカーケンダル空孔を消滅させた。次い
で2回目の熱拡散処理を 695℃で40時間施してNb3
n系化合物超電導線を製造した。
The present invention will be described below in detail with reference to examples. (Example 1) Bronze with an outer diameter of 45.3 mmφ (Cu-14.3 wt%
Sn-0.2 wt% Ti-based alloy) 19 holes with 6.0 mmφ through holes at regular intervals, insert Nb wire with 5.8 mmφ outside diameter into these holes, and bronze lids at the front and rear ends of the bronze rod. Was vacuum-sealed by electron beam welding and covered to prepare a primary billet. Next, this primary billet was hot extruded, and this extruded material was repeatedly subjected to wire drawing and intermediate annealing to produce a hexagonal wire having an opposite side length of 1 mm. This hexagonal wire was filled into a bronze pipe having the same composition as the primary billet and having an outer diameter of 45 mmφ and an inner diameter of 38 mmφ to produce a secondary billet. At the center of the bronze pipe, an oxygen-free copper rod having a diameter of 20 mm, which serves as a stabilizing material, was arranged by winding Nb foil on the outer circumference. This secondary billet was processed into a composite wire of 0.7 mmφ by the same method as the primary billet. Next, a Sn layer and a Ni layer were sequentially electroplated on this composite wire to prepare a composite wire. The thicknesses of the Sn layer and the Ni layer were variously changed. Next, this composite wire was subjected to the first thermal diffusion treatment at 450 ° C. for 50 hours. After thermal diffusion treatment,
The tissue was observed. Sn of Sn layer is 100 in the bronze substrate.
It was diffused uniformly by about μm. There was no burnout of the Sn layer. The Nb filaments were linearly positioned in the bronze substrate at equal intervals, and no turbulence was observed. A small amount of Kirkendall pores were observed in the bronze substrate. Next, this wire rod was subjected to wire drawing at a cross-section reduction rate of 5% to adjust the outer diameter of the wire rod and eliminate Kirkendall pores inside the wire rod. Then, the second thermal diffusion treatment was performed at 695 ° C for 40 hours to obtain Nb 3 S.
An n-based compound superconducting wire was manufactured.

【0016】(実施例2)実施例1において、複合素線
上にSn層及びCu−10wt%Sn合金層を順次電気めっ
きして複合線材とした他は、実施例1と同じ方法により
Nb3 Sn系化合物超電導線を製造した。
Example 2 Nb 3 Sn was prepared by the same method as in Example 1 except that the Sn layer and the Cu-10 wt% Sn alloy layer were sequentially electroplated on the composite wire to form a composite wire. A compound superconducting wire was manufactured.

【0017】(比較例1)実施例1において、複合素線
にSn層を8μm厚さに、その上にCu層を 1.5μm厚
さにめっきした他は、実施例1と同じ方法によりNb3
Sn系化合物超電導線を製造した。
(Comparative Example 1) Nb 3 was prepared in the same manner as in Example 1 except that a Sn layer was plated on the composite wire to a thickness of 8 μm and a Cu layer was plated thereon to a thickness of 1.5 μm.
An Sn-based compound superconducting wire was manufactured.

【0018】(比較例2)実施例1において、複合素線
にSn層を14μm厚さに、その上にCu層を 2.5μm厚
さにめっきし、1回目の熱拡散処理を 450℃で 100時間
施した他は、実施例1と同じ方法によりNb3 Sn系化
合物超電導線を製造した。
(Comparative Example 2) In Example 1, an Sn layer was plated on the composite wire to a thickness of 14 μm, and a Cu layer was plated thereon to a thickness of 2.5 μm, and the first thermal diffusion treatment was performed at 450 ° C. for 100 minutes. An Nb 3 Sn-based compound superconducting wire was manufactured by the same method as in Example 1 except that the time was applied.

【0019】(比較例3)実施例1において、複合素線
にSn層のみを8μm厚さに形成した他は、実施例1と
同じ方法によりNb3 Sn系化合物超電導線を製造し
た。
(Comparative Example 3) A Nb 3 Sn-based compound superconducting wire was manufactured in the same manner as in Example 1, except that only the Sn layer was formed to a thickness of 8 μm on the composite element wire.

【0020】(比較例4)実施例1において、複合素線
にSn層のみを8μm厚さに形成して複合線材となし、
この複合線材にSnの融点未満の 200℃の温度で60時
間、次に 300℃の温度で50時間、最後に 695℃の温度で
40時間の加熱条件で熱拡散処理を施した他は、実施例1
と同じ方法によりNb3 Sn系化合物超電導線を製造し
た。
(Comparative Example 4) In Example 1, only a Sn layer was formed on the composite wire to a thickness of 8 μm to form a composite wire.
This composite wire is heated at a temperature of 200 ° C below the melting point of Sn for 60 hours, then at 300 ° C for 50 hours, and finally at 695 ° C.
Example 1 except that the heat diffusion treatment was performed under heating conditions for 40 hours
A Nb 3 Sn-based compound superconducting wire was manufactured by the same method as described above.

【0021】得られた各々のNb3 Sn系化合物超電導
線について、臨界電流(Ic)を測定した。又断面を観
察してSnの溶落有無、カーケンダル空孔の有無を調べ
た。結果を表1に示す。
The critical current (Ic) was measured for each of the obtained Nb 3 Sn-based compound superconducting wires. Also, the cross section was observed to examine the presence or absence of Sn burn-out and the presence or absence of Kirkendall pores. The results are shown in Table 1.

【0022】[0022]

【表1】 [Table 1]

【0023】表1より明らかなように、本発明方法品
(No.1〜10) はいずれもIcが高く、Snの溶落がなく
断面形状に優れ、カーケンダル空孔は小さいか、又は少
なかった。尚、No.2はSnの平均濃度が16wt%を下回っ
た為Icが若干低下した。No.6はSn層の厚さに対して
金属材層(Ni層)がやや厚過ぎて不経済であったが、
特性上問題なかった。No.7は金属材層(Ni層)が薄く
Sn層の保持力が弱くなり断面がやや変形し、Icも幾
分低下した。但し、実用上問題ない程度であった。
As is clear from Table 1, all the products of the method of the present invention (Nos. 1 to 10) had high Ic, no Sn burn-through, excellent cross-sectional shape, and small or few Kirkendall pores. . Incidentally, in No. 2, the average Sn concentration was below 16 wt%, so that Ic was slightly lowered. No. 6 was uneconomical because the metal material layer (Ni layer) was slightly thicker than the Sn layer thickness,
There was no problem in terms of characteristics. In No. 7, the metal material layer (Ni layer) was thin, the coercive force of the Sn layer was weakened, the cross-section was slightly deformed, and Ic was also slightly lowered. However, there was no problem in practical use.

【0024】これに対し、比較例品のNo.11 はSn層上
にCu層を形成した為、Sn層がCu層に消費されてS
nが不足し、Icが低下した。No.12 はSn層を厚く形
成したので、熱拡散処理時間が長くなり、カーケンダル
空孔が多量に発生し、軽圧下後も残存してIcを低下さ
せた。No.13 は高融点金属材層を用いず、しかも始めか
ら 450℃の温度で熱拡散処理を施した為、Sn層が溶落
しNb3 Snフィラメントが露出してIcが著しく低下
した。No.14 は熱拡散処理をSnの融点未満の低温から
始めたので、Sn層の溶落は防止できたが、カーケンダ
ル空孔が多量に発生し、軽圧下後も残存してIcが低下
した。
On the other hand, in No. 11 of the comparative example, since the Cu layer was formed on the Sn layer, the Sn layer was consumed by the Cu layer and S
n was insufficient and Ic was lowered. In No. 12, since the Sn layer was formed thickly, the heat diffusion treatment time became long, a large number of Kirkendall vacancies were generated, and it remained even after light pressure reduction to lower Ic. In No. 13, the high melting point metal material layer was not used, and since the thermal diffusion treatment was performed at a temperature of 450 ° C. from the beginning, the Sn layer was burned out, the Nb 3 Sn filament was exposed, and the Ic was significantly lowered. In No. 14, the thermal diffusion treatment was started at a temperature lower than the melting point of Sn, so the burnout of the Sn layer could be prevented, but a large number of Kirkendall vacancies were generated and the Ic was reduced even after the pressure was reduced. .

【0025】[0025]

【効果】以上に述べたように、本発明によれば、Snよ
り高融点で、Snを消費せず、しかもSn層のSnがN
bフィラメントを配列したCu−Sn系合金基体の方へ
優先的に拡散する金属材層が、複合素線上の溶融Snを
保持するので、Snの熱拡散処理を高温短時間で行うこ
とができる。又熱拡散処理を高温短時間で行うので、基
体中の空孔の成長も抑えられて、超電導特性に優れたN
3 Sn系化合物超電導線が得られる。
As described above, according to the present invention, the melting point of Sn is higher than Sn, Sn is not consumed, and Sn in the Sn layer is N.
Since the metal material layer preferentially diffusing toward the Cu—Sn alloy base body in which the b filaments are arranged holds the molten Sn on the composite wire, the thermal diffusion treatment of Sn can be performed at a high temperature in a short time. Further, since the thermal diffusion treatment is carried out at a high temperature in a short time, the growth of holes in the substrate can be suppressed, and N having excellent superconducting characteristics can be obtained.
A b 3 Sn-based compound superconducting wire is obtained.

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

【図1】本発明における複合線材の熱拡散処理前後の態
様を示す横断面図である。
FIG. 1 is a cross-sectional view showing aspects of a composite wire according to the present invention before and after thermal diffusion treatment.

【図2】本発明における複合線材の熱拡散処理前後の他
の態様を示す横断面図である。
FIG. 2 is a cross-sectional view showing another embodiment before and after the thermal diffusion treatment of the composite wire according to the present invention.

【符号の説明】 1──安定化銅線 2──Nb箔 3──Nb/ブロンズ複合層 4──ブロンズシース層 5──Sn層 6──Niの金属材層 7──Nb3 Sn含有ブロンズ層 8──ブロンズシース層とSn層の合体層 9──ブロンズの金属材層[Explanation of Codes] 1--Stabilized copper wire 2 --Nb foil 3 --Nb / bronze composite layer 4 --Bronze sheath layer 5 --Sn layer 6 --Ni metal material layer 7 --Nb 3 Sn Contained bronze layer 8 --- Coalescing layer of bronze sheath layer and Sn layer 9 --- Metal material layer of bronze

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】 Cu−Sn系合金基体中にNbフィラメ
ントを多数本配列させた複合素線上に、Sn層、及びS
nより高融点でSnと非反応性の金属材層を順次形成し
て複合線材となし、この複合線材に熱拡散処理を施して
Cu−Sn系合金基体中にNb3 Snフィラメントを生
成させることを特徴とするNb3 Sn系化合物超電導線
の製造方法。
1. An Sn layer and an S layer are formed on a composite element wire in which a large number of Nb filaments are arranged in a Cu—Sn based alloy substrate.
A metal wire layer having a melting point higher than n and non-reactive with Sn is sequentially formed to form a composite wire, and the composite wire is subjected to a thermal diffusion treatment to form an Nb 3 Sn filament in a Cu-Sn alloy base. A method for producing a Nb 3 Sn-based compound superconducting wire, comprising:
【請求項2】 Snより高融点でSnと非反応性の金属
材層がCr、Ni、Zn、Ag、Co、Fe、Pd、P
t、Au等の純金属材、又はAg−Pd系、Ag−Sb
系、Ag−Se系、Au−Ni系、Au−Co系、Cu
−Zn系、Cu−Sn系、Zn−Sn系、Ni−Sn
系、Co−Sn系等の合金材から構成されていることを
特徴とする請求項1記載のNb3 Sn系化合物超電導線
の製造方法。
2. A metal material layer having a higher melting point than Sn and not reacting with Sn is Cr, Ni, Zn, Ag, Co, Fe, Pd, P.
Pure metal materials such as t and Au, or Ag-Pd-based, Ag-Sb
System, Ag-Se system, Au-Ni system, Au-Co system, Cu
-Zn system, Cu-Sn system, Zn-Sn system, Ni-Sn
System, method according to claim 1 Nb 3 Sn compound superconducting wire according to, characterized in that it is composed of an alloy material of Co-Sn system, etc..
JP6160690A 1994-06-20 1994-06-20 Method for producing Nb3Sn compound superconducting wire Pending JPH087682A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP6160690A JPH087682A (en) 1994-06-20 1994-06-20 Method for producing Nb3Sn compound superconducting wire

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP6160690A JPH087682A (en) 1994-06-20 1994-06-20 Method for producing Nb3Sn compound superconducting wire

Publications (1)

Publication Number Publication Date
JPH087682A true JPH087682A (en) 1996-01-12

Family

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP6160690A Pending JPH087682A (en) 1994-06-20 1994-06-20 Method for producing Nb3Sn compound superconducting wire

Country Status (1)

Country Link
JP (1) JPH087682A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007165152A (en) * 2005-12-14 2007-06-28 Hitachi Cable Ltd Core wire for Nb3Sn superconducting wire, Nb3Sn superconducting wire, and manufacturing method thereof

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007165152A (en) * 2005-12-14 2007-06-28 Hitachi Cable Ltd Core wire for Nb3Sn superconducting wire, Nb3Sn superconducting wire, and manufacturing method thereof

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