JPS6347086B2 - - Google Patents
Info
- Publication number
- JPS6347086B2 JPS6347086B2 JP55166357A JP16635780A JPS6347086B2 JP S6347086 B2 JPS6347086 B2 JP S6347086B2 JP 55166357 A JP55166357 A JP 55166357A JP 16635780 A JP16635780 A JP 16635780A JP S6347086 B2 JPS6347086 B2 JP S6347086B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting wire
- wire
- diffusion
- niobium
- copper
- 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
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Classifications
-
- Y—GENERAL 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
- Y02—TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
- Y02E—REDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
- Y02E40/00—Technologies for an efficient electrical power generation, transmission or distribution
- Y02E40/60—Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment
Landscapes
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
本発明は溶質金属を未反応複合超電導線に拡散
処理によつて供給し化合物超電導線を製造する方
法の改良に関するものである。
従来溶質金属を拡散処理法によつて未反応複合
超電導線に供給するにおいて、次の如き欠点を有
するものであつた。即ち化合物超電導線の1例と
してNb3Sn超電導線を製造する方法について詳述
すると、第1図に示す如く銅マトリツクス1に複
数本のニオブ2を埋込み減面加工を行つて最終形
状となした後、これにスズメツキ3を施し、加熱
によつてスズ3を銅1内に拡散処理を行つて、ニ
オブとの界面にNb3Sn化合物超電導体4を形成せ
しめているものである。
又別の方法として第2図に示す如く銅粉とニオ
ブ粉とをアーク溶解炉などにより溶解し、これを
凝固後、減面加工を行つて最終形状となした後、
これにスズメツキ3を施し、加熱によつてスズ3
を銅の内に拡散処理を行つてニオブとの界面に
Nb3Sn化合物超電導体4を形成せしめているもの
である。
これらの方法を通常In―Situ法とよんでいるも
のである。
然しながら上記の方法による場合には、拡散に
よつて5〜20μm2の大きさのカーケンダルボイド
(Kirkendall Void)6が多数分散して形成する
ため化合物超電導体の脆性を助長し、耐張力性及
び耐屈曲性を著しく阻害する。また、スズとニオ
ブとの反応によつてNb3Sn層の結晶粒径を小さく
且つ層厚を厚くするためには拡散温度を750℃以
下に制御する必要があるが、所定の時間内にて反
応を終了させるにはスズの拡散距離(深さ)に大
きく制限をうけ線外径として0.3mmが限界とされ
ている。換言すれば0.3mmφ以上の太径の導体は
えられないというものであつた。更にメツキ層が
低融点物質であるため最終の焼鈍において長手方
向の直径変化が大きく巻付作業が困難であつた。
このように従来の方法においてはスズを拡散せ
しめた後、更にNb3Snを形成させるまで全く加工
処理を施されないため、スズと銅或はニオブとの
拡散速度の相違によるKirkendall Voidが発生し
てもこれを除去する手段を行つていないものであ
つた。
本発明はかかる欠点を改善せんとして鋭意研究
を行つた結果、カーケンダルボイドを消失せし
め、機械的強度並に耐屈曲性に優れた化合物超電
導体をうる方法を見出したものである。即ち本発
明方法は溶質金属例えばSn、Gaを未反応複合超
電導線の表層部から拡散処理により供給して化合
物超電導線を製造する方法において、銅又は銅合
金とニオブとの複合体を減面加工する第1工程
と、溶質金属のメツキを施して拡散熱処理を行う
第2工程と、5〜80%の減面加工を行う第3工程
と、第2工程と第3工程とを繰り返し行う第4工
程と、拡散焼鈍を行う第5工程とよりなることを
特徴とするものである。
なお上記において未反応複合超電導線の表層部
とは、通常外表面を指示するものであるが、該複
合超電導線が中空体よりなる場合には、この円孔
部表面をも含めていう。
本発明の製造工程の1例を図面により説明す
る。第3図に示す如く、銅1及びニオブ2とを従
来方法と同様にして複合し、減面加工後最終形状
に至る前にスズメツキ3を施し、このスズを拡散
させるに必要な温度250〜450℃にて5〜50時間焼
鈍し、ブロンズマトリツクス5にニオブ2が埋込
まれた未反応複合超電導線8とする。この超電導
線8にダイス引き或は圧延等によつて5〜80%の
減面加工を行つて最終形状とする。
なおその形状としては丸線、第4図の如き角
線、第5図の如きスムースボデイ撚線10、第6
図の如き成形撚線11、など如何なる形状のもの
でもよい。次いでNb3Sn化合物超電導体をうるに
必要な温度500〜800℃にて、10〜100時間拡散焼
鈍し、ブロンズ5とニオブ2との界面にNb3Sn層
4を形成して本発明化合物超電導線9をうるもの
である。
なお、上記において銅及びニオブの未反応複合
超電導線を製造する過程において銅及びニオブが
稀薄合金であつたり、又酸素、水素などの不純物
を含有しても差支えない。又スズメツキを施す工
程においてもスズにカリウムなどの元素が混入し
ていても差支えない。
更に電流容量の大きい導体をうるには、第7図
に示す如くブロンズマトリツクス5とニオブ2と
の未反応複合超電導線8をタンタルなどの拡散バ
リヤ12で包被し、安定化銅1の中に埋込むこと
によつて得られるものである。
而して本発明方法においてスズメツキを施した
未反応複合超電導線を焼鈍後加工する理由につい
て説明すると次の如くである。
(1) スズが銅中に拡散する過程で発生するカーケ
ンダルボイドを小さく分散せしめ実用上問題と
ならない大きさのものとする。
(2) ブロンズマトリツクスに歪エネルギーを蓄積
させることによりNb3Snを形成させる最終拡散
熱処理工程においてSnの拡散を助長すると共
にNb3Sn核を微細にすることが出来る。
(3) 導体の最終形状を任意なものにすることが出
来る。
(4) スズメツキを施した未反応複合超電導線を焼
鈍し、ブロンズマトリツクス複合体による過程
において導体形状の変形分を矯正することがで
きる。
なお本発明方法は溶質金属としてSn、Gaのよ
うな単一物質のほかSnの次にGaを拡散させる多
重拡散やSn―Mg合金、Ga―Zn合金などの合金
拡散にも適用できる。
次に本発明の実施例について説明する。
実施例
銅粉末とニオブ粉末とを重量%で65:35の比率
を配合し圧縮後アーク溶解炉により溶製し、100
mmφ×180mmのインゴツトをえた。このインゴ
ツトを450゜において2時間加熱後熱間押出しを行
い15mmφ×800mmの押出棒とした。この押出棒
を冷間減面加工によつて0.3mmφの線材とした。
この線材の一部を使用し、約10μmの厚さにス
ズメツキを施し、400℃において24時間焼鈍した
後、ダイス引きによつて0.22mmφの線径となし、
750℃において50時間拡散熱処理を行つて本発明
化合物超電導線をえた。
又本発明化合物超電導線と比較するために上記
の0.3mmφ複合線をダイス引きによつて0.22mmφ
まで伸線後約7μmの等価厚さのスズメツキを施
し、750℃において50時間拡散熱処理を行つて従
来の化合物超電導線をえた。
而して本発明超電導線及び従来超電導線につい
て夫々金属組織、機械特性及び電気特性を測定し
た結果は第1表に示す如くであつた。
The present invention relates to an improvement in a method for producing a compound superconducting wire by supplying solute metal to an unreacted composite superconducting wire through a diffusion process. Conventionally, supplying a solute metal to an unreacted composite superconducting wire by a diffusion treatment method has had the following drawbacks. Specifically, the method for manufacturing a Nb 3 Sn superconducting wire as an example of a compound superconducting wire will be described in detail. As shown in Figure 1, a plurality of niobium 2 is embedded in a copper matrix 1 and subjected to area reduction processing to obtain the final shape. Thereafter, tin plating 3 is applied to this, and tin 3 is diffused into copper 1 by heating to form a Nb 3 Sn compound superconductor 4 at the interface with niobium. As another method, as shown in Figure 2, copper powder and niobium powder are melted in an arc melting furnace or the like, solidified, and then subjected to area reduction processing to form the final shape.
Apply tin 3 to this and heat it to make tin 3
is diffused into the copper and at the interface with niobium.
This is what forms the Nb 3 Sn compound superconductor 4. These methods are usually called in-situ methods. However, in the case of the above method, a large number of Kirkendall voids 6 with a size of 5 to 20 μm 2 are dispersed and formed due to diffusion, which promotes the brittleness of the compound superconductor and deteriorates the tensile strength and Significantly reduces bending resistance. Furthermore, in order to reduce the crystal grain size and increase the layer thickness of the Nb 3 Sn layer through the reaction between tin and niobium, it is necessary to control the diffusion temperature to 750°C or less, but within a specified time. In order to complete the reaction, the diffusion distance (depth) of tin is greatly limited, and the outer diameter of the wire is limited to 0.3 mm. In other words, it was impossible to obtain a conductor with a diameter larger than 0.3 mmφ. Furthermore, since the plating layer is a low melting point material, the diameter change in the longitudinal direction is large in the final annealing, making the winding operation difficult. In this way, in the conventional method, after tin is diffused, no further processing is performed until Nb 3 Sn is formed, so Kirkendall Void occurs due to the difference in diffusion rate between tin and copper or niobium. However, no measures had been taken to remove this. As a result of extensive research aimed at improving these drawbacks, the present invention has discovered a method for eliminating Kirkendall voids and producing a compound superconductor with excellent mechanical strength and bending resistance. That is, the method of the present invention is a method for producing a compound superconducting wire by supplying solute metals such as Sn and Ga from the surface layer of an unreacted composite superconducting wire through a diffusion process, in which a composite of copper or a copper alloy and niobium is subjected to an area-reducing process. a second step of plating with solute metal and performing diffusion heat treatment; a third step of reducing the area by 5 to 80%; and a fourth step of repeating the second and third steps. and a fifth step of performing diffusion annealing. Note that in the above, the surface layer portion of the unreacted composite superconducting wire usually refers to the outer surface, but when the composite superconducting wire is made of a hollow body, it also includes the surface of this circular hole. An example of the manufacturing process of the present invention will be explained with reference to the drawings. As shown in Fig. 3, copper 1 and niobium 2 are composited in the same manner as in the conventional method, and after surface reduction processing and before reaching the final shape, tin plating 3 is applied, and the temperature required to diffuse the tin is 250 to 450. C. for 5 to 50 hours to obtain an unreacted composite superconducting wire 8 in which niobium 2 is embedded in the bronze matrix 5. This superconducting wire 8 is subjected to a surface reduction process of 5 to 80% by die drawing or rolling to obtain a final shape. The shapes include round wire, square wire as shown in Fig. 4, smooth body stranded wire 10 as shown in Fig. 5, and
It may be of any shape, such as a shaped stranded wire 11 as shown in the figure. Next, the Nb 3 Sn compound superconductor is diffusion annealed at a temperature of 500 to 800° C. for 10 to 100 hours to form a Nb 3 Sn layer 4 at the interface between the bronze 5 and the niobium 2, thereby forming the inventive compound superconductor. This is the one that obtains line 9. In addition, in the process of manufacturing the unreacted composite superconducting wire of copper and niobium in the above, copper and niobium may be a dilute alloy or may contain impurities such as oxygen and hydrogen. Also, there is no problem even if an element such as potassium is mixed into the tin in the tin plating process. In order to obtain a conductor with an even larger current capacity, as shown in FIG. This can be obtained by embedding it in The reason why the unreacted composite superconducting wire that has been subjected to tin plating is processed after annealing in the method of the present invention will be explained as follows. (1) Kirkendall voids, which are generated during the process of tin diffusion into copper, are made small and dispersed to a size that does not pose a practical problem. (2) In the final diffusion heat treatment step in which Nb 3 Sn is formed by accumulating strain energy in the bronze matrix, diffusion of Sn can be promoted and Nb 3 Sn nuclei can be made fine. (3) The final shape of the conductor can be made into any desired shape. (4) By annealing the unreacted composite superconducting wire that has been tin-plated, it is possible to correct the deformation of the conductor shape during the bronze matrix composite process. The method of the present invention can be applied not only to single substances such as Sn and Ga as solute metals, but also to multiple diffusion in which Ga is diffused after Sn, and alloy diffusion such as Sn--Mg alloy and Ga--Zn alloy. Next, examples of the present invention will be described. Example Copper powder and niobium powder were mixed in a weight percent ratio of 65:35, compressed, and then melted in an arc melting furnace.
An ingot of mmφ×180mm was obtained. This ingot was heated at 450° for 2 hours and then hot extruded to obtain an extruded rod of 15 mmφ×800 mm. This extruded rod was made into a wire rod with a diameter of 0.3 mm by cold area reduction processing. Using a part of this wire, tin plate it to a thickness of about 10μm, annealing it at 400℃ for 24 hours, and then cutting it into a wire diameter of 0.22mmφ by die drawing.
Diffusion heat treatment was performed at 750°C for 50 hours to obtain a superconducting wire of the compound of the present invention. In addition, for comparison with the compound superconducting wire of the present invention, the above 0.3 mmφ composite wire was cut into 0.22 mmφ by die drawing.
After drawing the wire to 7 μm, the wire was plated to an equivalent thickness of approximately 7 μm, and diffusion heat treatment was performed at 750°C for 50 hours to obtain a conventional compound superconducting wire. Table 1 shows the results of measuring the metal structure, mechanical properties, and electrical properties of the superconducting wire of the present invention and the conventional superconducting wire.
【表】
上表より明らかの如く本発明方法による化合物
超電導線は従来方法による化合物超電導線に比し
てボイドサイズが著しく小さく且つ分散してい
る。又Nb3Snの結晶粒径が微細化し且つ層厚が厚
いものがえられる。更に線材圧力、耐曲げ特性、
及び臨界電流密度が著しく向上することが認めら
れた。
以上詳述した如く本発明方法によれば次の如き
効果を有するものである。
(1) カーケンダルボイドを消失し未反応複合超電
導線の機械的強度並に耐屈曲性を著しく改善す
る。
(2) 臨界電流密度が高く且つ電流容量の大きさを
超電導線をうることが出来る。
(3) 減面率を最高80%にて加工するため導体形状
を変更することができるため、導体として撚線
成形撚線、テープなどその形状に限定する必要
はない。[Table] As is clear from the above table, the void size of the compound superconducting wire produced by the method of the present invention is significantly smaller and more dispersed than that of the compound superconducting wire produced by the conventional method. In addition, Nb 3 Sn has a fine grain size and a thick layer. Furthermore, wire pressure, bending resistance,
It was observed that the critical current density and the critical current density were significantly improved. As detailed above, the method of the present invention has the following effects. (1) Eliminating Kirkendall voids and significantly improving the mechanical strength and bending resistance of unreacted composite superconducting wires. (2) Superconducting wires with high critical current density and large current capacity can be obtained. (3) Since the shape of the conductor can be changed as it is processed with a maximum area reduction rate of 80%, there is no need to limit the shape of the conductor to stranded wire forming, stranded wire, tape, etc.
第1図及び第2図は従来の化合物超電導線の製
造方法の1例を示す製造工程説明図、第3図は本
発明による化合物超電導線の製造方法の1例を示
す製造工程説明図、第4図、第5図及び第6図は
未反応複合超電導線の形状の1例を示す断面図、
第7図は大電流容量の未反応複合超電導線の1例
を示すものであり、Aは丸線断面図、Bは丸線A
を圧延した角線断面図である。
1…銅マトリツクス、2…ニオブ、3…スズメ
ツキ、4…Nb3Sn化合物超電導体、5…ブロンズ
マトリツクス、6…カーケンダルボイド、7…従
来の未反応複合超電導線、8…本発明未反応複合
超電線、9…本発明化合物複合超電導線、10…
スムースボデイ撚線、11…成形撚線、12…拡
散バリヤー。
1 and 2 are manufacturing process explanatory diagrams showing one example of a conventional method for manufacturing a compound superconducting wire, FIG. 3 are manufacturing process explanatory diagrams showing an example of a manufacturing method for a compound superconducting wire according to the present invention, 4, 5 and 6 are cross-sectional views showing an example of the shape of an unreacted composite superconducting wire,
Figure 7 shows an example of an unreacted composite superconducting wire with a large current capacity, where A is a cross-sectional view of the round wire, and B is a cross-sectional view of the round wire A.
FIG. 1... Copper matrix, 2... Niobium, 3... Suzmetsuki, 4... Nb 3 Sn compound superconductor, 5... Bronze matrix, 6... Kirkendall void, 7... Conventional unreacted composite superconducting wire, 8... Unreacted of the present invention Composite superconducting wire, 9...Compound superconducting wire of the present invention, 10...
Smooth body stranded wire, 11... Molded stranded wire, 12... Diffusion barrier.
Claims (1)
拡散処理により供給して化合物超電導線を製造す
る方法において、銅又は銅合金とニオブとの複合
体を減面加工する第1工程と、溶質金属のメツキ
を施して拡散熱処理を行う第2工程と、5〜80%
の減面加工を行う第3工程と、第2工程と第3工
程とを繰り返し行う第4工程と拡散焼鈍を行う第
5工程とよりなることを特徴とする化合物超電導
線の製造方法。1. In a method for producing a compound superconducting wire by supplying solute metal from the surface layer of an unreacted composite superconducting wire by diffusion treatment, a first step of reducing the area of a composite of copper or copper alloy and niobium; The second step is plating and diffusion heat treatment, and 5 to 80%
A method for manufacturing a compound superconducting wire, comprising: a third step of performing surface reduction processing; a fourth step of repeatedly performing the second and third steps; and a fifth step of performing diffusion annealing.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55166357A JPS5790814A (en) | 1980-11-26 | 1980-11-26 | Method of producing compound superconductive wire |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP55166357A JPS5790814A (en) | 1980-11-26 | 1980-11-26 | Method of producing compound superconductive wire |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5790814A JPS5790814A (en) | 1982-06-05 |
| JPS6347086B2 true JPS6347086B2 (en) | 1988-09-20 |
Family
ID=15829880
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP55166357A Granted JPS5790814A (en) | 1980-11-26 | 1980-11-26 | Method of producing compound superconductive wire |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5790814A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6051013U (en) * | 1983-09-14 | 1985-04-10 | 伊藤鉄工有限会社 | Inner formwork for concrete pipe formwork |
| JPH02103813A (en) * | 1988-10-13 | 1990-04-16 | Fujikura Ltd | Compound superconducting wire and manufacture thereof |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS4896093A (en) * | 1972-03-21 | 1973-12-08 | ||
| JPS49115696A (en) * | 1973-03-07 | 1974-11-05 | ||
| JPS5631509B2 (en) * | 1973-06-26 | 1981-07-22 |
-
1980
- 1980-11-26 JP JP55166357A patent/JPS5790814A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5790814A (en) | 1982-06-05 |
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