JPH04298917A - Manufacture of compound superconductor - Google Patents
Manufacture of compound superconductorInfo
- Publication number
- JPH04298917A JPH04298917A JP3064448A JP6444891A JPH04298917A JP H04298917 A JPH04298917 A JP H04298917A JP 3064448 A JP3064448 A JP 3064448A JP 6444891 A JP6444891 A JP 6444891A JP H04298917 A JPH04298917 A JP H04298917A
- Authority
- JP
- Japan
- Prior art keywords
- superconductor
- superconducting
- wire
- compound
- tube
- 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.)
- Withdrawn
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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)
Abstract
Description
【0001】[発明の目的][Object of the invention]
【0002】0002
【産業上の利用分野】本発明は、化合物超電導導体の製
造方法に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a method for producing a compound superconducting conductor.
【0003】0003
【従来の技術】現在、実用化されている超電導導体とし
ては、Nb3 SnやNb3 Al等の化合物系超電導
体を用いたものや、Nb−Ti やNb−Zr 等の合
金系超電導体を用いたものが知られており、送電ケーブ
ルや電力をほとんど消費することなく強磁界の形成が可
能な超電導コイル等への実用化が進められている。上記
したような化合物超電導体を用いた超電導導体の製造方
法としては、ブロンズ法、チューブ法、内部拡散法、ジ
ェリーロール法等が知られている。[Prior Art] Superconductors currently in practical use include those using compound-based superconductors such as Nb3Sn and Nb3Al, and those using alloy-based superconductors such as Nb-Ti and Nb-Zr. This technology is well known, and efforts are being made to put it to practical use in superconducting coils, etc., which can generate strong magnetic fields without consuming power transmission cables or electricity. As methods for manufacturing superconducting conductors using the above-mentioned compound superconductors, the bronze method, tube method, internal diffusion method, jelly roll method, etc. are known.
【0004】例えば、Nbチューブ法を適用した超電導
導体は、例えば以下に示すようにして製造される。超電
導導体として、Nb3 Snマルチ超電導線を例にとる
と、まずNbチューブ内に、 Cu−Sn合金やSn棒
を挿入したCu管を充填すると共に、このNbチューブ
の外周にCuを被覆し、これをスウェージングマシン等
により一体化しながら所定の外径まで減面加工する。次
いで、この素線の多数本をCu管内に挿入し、一体化し
た後に、減面加工を施して所定の線径とする。この後、
Nb3 Snの生成温度で熱処理を施すことによって、
Nbチューブ内のSnを拡散させてNbと反応させ、N
bチューブの表面にNb3 Sn超電導体層を形成する
。For example, a superconducting conductor to which the Nb tube method is applied is manufactured, for example, as shown below. Taking Nb3Sn multi-superconducting wire as an example of a superconducting conductor, first, a Cu tube into which a Cu-Sn alloy or Sn rod is inserted is filled into an Nb tube, and the outer periphery of this Nb tube is coated with Cu. The parts are integrated using a swaging machine, etc., and the area is reduced to a predetermined outer diameter. Next, a large number of these strands are inserted into a Cu tube, integrated, and then subjected to surface reduction processing to obtain a predetermined wire diameter. After this,
By performing heat treatment at the formation temperature of Nb3Sn,
Sn in the Nb tube is diffused and reacted with Nb, and the Nb
b Form a Nb3Sn superconductor layer on the surface of the tube.
【0005】また、Nb3 Sn等を用いた超電導線は
、長手方向の引張り力や曲げ歪が加わった際に、臨界電
流密度等の超電導特性が低下しやすいという欠点を有し
ているが、断面円形の超電導線よりも断面矩形状の超電
導線の方が、上記した変形による超電導特性の低下が少
ないため、超電導コイルを作製するような際には、断面
矩形状の超電導線が一般的に用いられている。このよう
な平角状の超電導線は、上述したNbチューブ法におい
て、化合物超電導体の生成温度による熱処理前に、減面
加工によって所定の線径とした丸線を加圧ローラ等で圧
延することによって、断面形状を正方形や長方形のよう
な矩形状にし、この後に化合物超電導体の生成温度によ
る熱処理を施して得ている。[0005] Furthermore, superconducting wires using Nb3Sn etc. have the disadvantage that superconducting properties such as critical current density tend to deteriorate when longitudinal tensile force or bending strain is applied. A superconducting wire with a rectangular cross section is less likely to deteriorate its superconducting properties due to the above deformation than a superconducting wire with a circular cross section, so superconducting wires with a rectangular cross section are generally used when manufacturing superconducting coils. It is being Such a rectangular superconducting wire is produced in the above-mentioned Nb tube method by rolling a round wire to a predetermined wire diameter through area reduction processing using a pressure roller or the like before heat treatment at the temperature for forming a compound superconductor. , the cross-sectional shape is made into a rectangular shape such as a square or a rectangle, and then heat treatment is performed at the temperature at which a compound superconductor is formed.
【0006】[0006]
【発明が解決しようとする課題】ところで、上述したよ
うな平角状の超電導線では、丸線を断面矩形状に加工す
る際に、図4に示すように、Sn棒1およびCu管2が
順に充填されたNbチューブ3自体も偏平状に変形して
しまう。同図では省略したが、Nb3 Sn等の超電導
体層は、変形したNbチューブ3の内周側に形成される
ため、Nbチューブ3が偏平状に変形すると、磁場に対
する超電導線の臨界電流密度(Jc)に異方性が生じて
しまう。この様子を図5に示す。図5から明らかなよう
に、超電導線の断面の短辺方向に磁場が印加された際の
Jc (図中、△で示す)に比べて、超電導線の断面の
長辺方向に磁場が印加された際のJc (図中、○で示
す)は大幅に低下する。これによって、超電導線を使用
する際の自由度が大幅に制限されている。[Problems to be Solved by the Invention] By the way, in the rectangular superconducting wire as described above, when processing the round wire into a rectangular cross-section, as shown in FIG. The filled Nb tube 3 itself also deforms into a flat shape. Although not shown in the figure, a superconductor layer such as Nb3Sn is formed on the inner circumferential side of the deformed Nb tube 3, so when the Nb tube 3 is deformed into a flat shape, the critical current density of the superconducting wire ( Anisotropy occurs in Jc). This situation is shown in FIG. As is clear from Fig. 5, compared to Jc (indicated by △ in the figure) when a magnetic field is applied in the short side direction of the cross section of the superconducting wire, the magnetic field is applied in the long side direction of the cross section of the superconducting wire. Jc (indicated by ○ in the figure) decreases significantly. This significantly limits the degree of freedom in using superconducting wires.
【0007】また、超電導マグネットを作製する際には
、巻き易さや歪および荷重によるJc の低下を抑制す
るため、平角状超電導線の断面長辺が巻き治具に接する
ように巻回している。すなわち平角状超電導線を、超電
導マグネットが形成する磁場方向に対してJc の低下
が大きい方向に巻回することになる。したがって、所定
の磁場を得るためには、巻数を多くしたり、線径を太く
する等によって対処しなければならないため、大型で重
い超電導マグネットになってしまうという問題があった
。Furthermore, when manufacturing a superconducting magnet, the rectangular superconducting wire is wound so that the long side of the cross section is in contact with a winding jig in order to reduce the ease of winding and to suppress a decrease in Jc due to strain and load. That is, the rectangular superconducting wire is wound in the direction in which the Jc decreases more with respect to the direction of the magnetic field formed by the superconducting magnet. Therefore, in order to obtain a predetermined magnetic field, it is necessary to take measures such as increasing the number of turns or increasing the diameter of the wire, resulting in a large and heavy superconducting magnet.
【0008】本発明は、このような従来技術の課題に対
処するためになされたもので、平角状の超電導導体を作
製する際、超電導素線を変形させることなく、所定の断
面矩形状に容易に加工することを可能にした化合物超電
導導体の製造方法を提供することを目的としている。[0008] The present invention has been made to address the above-mentioned problems of the prior art, and when manufacturing a rectangular superconducting conductor, it is possible to easily shape the superconducting wire into a predetermined rectangular cross-sectional shape without deforming the superconducting wire. The purpose of the present invention is to provide a method for manufacturing a compound superconducting conductor that can be processed into a compound superconducting conductor.
【0009】[発明の構成][Configuration of the invention]
【0010】0010
【課題を解決するための手段と作用】すなわち、本発明
の化合物超電導導体の製造方法は、熱処理により反応し
て化合物超電導体を形成する化合物超電導体材料を含む
多数の素線を、 500℃〜700℃の範囲の温度で加
熱処理されたCu系マトリックス内に埋設する工程と、
前記Cu系マトリックスの外周側に強化銅層を一体化す
る工程と、この一体化された構造体を、所定の外形形状
に冷間加工する工程と、前記加工体に対して、前記化合
物超電導体の生成温度領域での熱処理を施す工程とを有
することを特徴としている。[Means and Effects for Solving the Problems] That is, the method for manufacturing a compound superconducting conductor of the present invention is to heat a large number of wires containing a compound superconductor material that reacts to form a compound superconductor by heat treatment at a temperature of 500°C to embedding in a Cu-based matrix heat-treated at a temperature in the range of 700°C;
A step of integrating a reinforcing copper layer on the outer peripheral side of the Cu-based matrix, a step of cold working this integrated structure into a predetermined external shape, and a step of applying the compound superconductor to the processed body. The method is characterized by comprising a step of performing heat treatment in the formation temperature range.
【0011】本発明に用いられる熱処理により反応して
化合物超電導体を形成する化合物超電導体材料としては
、Nb3 Snの形成材料であるNbとSnや、Nb3
Alの形成材料であるNbとAl等が例示され、例え
ばNbチューブ内にSnやAlを含む材料等を充填する
ことによって超電導体素線が形成される。また、Nbや
SnもしくはAlを別個に素線として用いることも可能
である。[0011] The compound superconductor material that reacts to form a compound superconductor by heat treatment used in the present invention includes Nb and Sn, which are the forming materials of Nb3 Sn, and Nb3
Nb and Al, which are forming materials for Al, are exemplified. For example, a superconductor wire is formed by filling a Nb tube with a material containing Sn or Al. Furthermore, it is also possible to use Nb, Sn, or Al as separate wires.
【0012】このような超電導体素線は、Cu系マトリ
ックス内に埋設される。また、このCu系マトリックス
の外周側には、強化銅層が一体化され、本発明の化合物
超電導導体の原型となる構造体が構成される。ここで、
上記Cu系マトリックスは、 500℃〜 700℃の
温度で加熱処理されたCuからなるものである。このよ
うな加熱処理が施されたCuは、減面加工等の冷間加工
によって軟化現象を起こすため、上記超電導体素線の変
形を防止する上で非常に有効である。上記加熱処理時の
温度が 500℃未満では、上記した軟化現象を十分に
得ることができず、また 700℃を超えると軟化しに
くくなる。加熱処理時の雰囲気は、特に限定されるもの
ではないが、Cuの酸化を防ぐ上で真空または不活性雰
囲気とすることが好ましい。ただし、大気中等の酸化性
雰囲気中において熱処理した際には、その後に酸化層の
除去処理を行えばよい。また、熱処理時間は10時間〜
50時間程度とすることが好ましい。また、上記したC
u系マトリックスの外周側に一体化される強化銅として
は、例えばアルミナ粒子等による粒子分散強化型銅合金
、Cr、Zr、Ti、Zn等による固溶強化型銅合金、
加工硬化させた銅等が例示され、特にアルミナ分散強化
銅が好ましい。このアルミナ分散強化銅は、Cu中にA
l2 O 3 粒子を 1〜 2重量%程度の範囲で分
散させることによって、分散強化させた強化Cu合金で
あり、例えば酸化銅粉末とアルミナ粉末との混合物を還
元焼結させることによって得られる。このアルミナ分散
強化銅は、化合物超電導体の生成温度による熱処理によ
っても、引張り強度の低下が極めて小さく、化合物超電
導導体の強度メンバーとして十分な効果をもたらすと共
に、超電導体素線の変形を防止する上で非常に有効であ
る。[0012] Such superconductor wires are embedded in a Cu-based matrix. Further, a reinforcing copper layer is integrated on the outer peripheral side of this Cu-based matrix, thereby forming a structure that is a prototype of the compound superconducting conductor of the present invention. here,
The Cu-based matrix is made of Cu that has been heat-treated at a temperature of 500°C to 700°C. Cu subjected to such heat treatment causes a softening phenomenon by cold working such as area reduction processing, and is therefore very effective in preventing deformation of the superconductor strands. If the temperature during the heat treatment is less than 500°C, the above-mentioned softening phenomenon cannot be sufficiently obtained, and if it exceeds 700°C, softening becomes difficult. The atmosphere during the heat treatment is not particularly limited, but is preferably a vacuum or an inert atmosphere in order to prevent oxidation of Cu. However, when the heat treatment is performed in an oxidizing atmosphere such as the air, the oxide layer may be removed after that. In addition, the heat treatment time is 10 hours ~
It is preferable to set it as about 50 hours. In addition, the above C
Examples of the reinforced copper integrated on the outer peripheral side of the U-based matrix include particle dispersion strengthened copper alloys using alumina particles, solid solution strengthened copper alloys using Cr, Zr, Ti, Zn, etc.
Examples include work-hardened copper, and alumina dispersion-strengthened copper is particularly preferred. This alumina dispersion strengthened copper has A in Cu.
It is a reinforced Cu alloy that is dispersion-strengthened by dispersing l2O3 particles in a range of about 1 to 2% by weight, and is obtained, for example, by reducing and sintering a mixture of copper oxide powder and alumina powder. This alumina dispersion-strengthened copper exhibits extremely small decrease in tensile strength even when heat treated at the temperature at which compound superconductors are formed, and is effective as a strong member of compound superconducting conductors, as well as preventing deformation of superconductor strands. is very effective.
【0013】本発明の製造方法においては、上記した構
造体に対して冷間にて伸線加工を施し、所定の線径の丸
型線とした後、この丸型線を加圧ローラ等によって圧延
して化合物超電導導体の外形形状を断面矩形状に加工す
る。ここで、上記丸型線に印加された圧力は、最外層の
強化銅層により受け止められ、また内部のCu系マトリ
ックスは伸線加工によって軟化現象を起こしており、マ
トリックス内の超電導体素線の移動が起き易くなってい
ることから、超電導体素線に加わる荷重は分散されると
共に軽減される。したがって、化合物超電導導体自体の
外形形状を断面矩形状に加工しても、超電導体素線の形
状をおおよそ断面円形に維持することができる。In the manufacturing method of the present invention, the above-described structure is subjected to cold wire drawing to form a round wire of a predetermined wire diameter, and then this round wire is drawn using a pressure roller or the like. The external shape of the compound superconducting conductor is processed into a rectangular cross-section by rolling. Here, the pressure applied to the round wire is absorbed by the outermost reinforcing copper layer, and the internal Cu-based matrix is softened by wire drawing, and the superconductor strands in the matrix are softened. Since movement is more likely to occur, the load applied to the superconductor strands is dispersed and reduced. Therefore, even if the external shape of the compound superconducting conductor itself is processed to have a rectangular cross-section, the shape of the superconductor strand can be maintained to have an approximately circular cross-section.
【0014】そして、上記したように外形形状を所定の
断面矩形状に加工した加工体に対して、化合物超電導体
の生成温度領域での熱処理を施すことによって、化合物
超電導体層を形成し、目的とする化合物超電導導体が得
られる。この熱処理条件は、例えばNb3 Snの場合
には 650℃〜 770℃の温度で10時間〜 40
0時間程度、Nb3 Alの場合には 750℃〜 9
50℃の温度で 1時間〜 100時間程度である。[0014] Then, a compound superconductor layer is formed by heat-treating the processed body having a predetermined rectangular cross-sectional shape in the compound superconductor formation temperature range as described above. A compound superconducting conductor is obtained. For example, in the case of Nb3Sn, the heat treatment conditions are 650°C to 770°C for 10 hours to 40°C.
Approximately 0 hours, in the case of Nb3 Al, 750°C ~ 9
The time is about 1 hour to 100 hours at a temperature of 50°C.
【0015】なお、本発明により得られた化合物超電導
導体を熱処理可能な製品へ適用する場合には、本発明の
熱処理をその製品の組立過程で行うようにしてもよい。
例えば、本発明により製造された超電導線を用いて超電
導マグネットを形成するような場合には、コイル用の巻
枠へ熱処理前のものを巻装し、この状態で化合物超電導
体および拡散防止層形成のための熱処理を行うようにし
てもよい。[0015] When the compound superconducting conductor obtained according to the present invention is applied to a heat-treatable product, the heat treatment of the present invention may be performed during the assembly process of the product. For example, when forming a superconducting magnet using a superconducting wire manufactured according to the present invention, the wire before heat treatment is wound around a coil winding frame, and in this state, a compound superconductor and a diffusion prevention layer are formed. Heat treatment may also be performed for this purpose.
【0016】[0016]
【実施例】次に、本発明の化合物超電導導体の製造方法
の実施例について、図面を参照して説明する。EXAMPLES Next, examples of the method for manufacturing a compound superconducting conductor of the present invention will be described with reference to the drawings.
【0017】実施例1
図1および図2は、本発明の一実施例の化合物超電導導
体の製造工程を示す図である。これらの図にしたがって
、この実施例のマルチ超電導線の製造方法を以下に説明
する。Example 1 FIGS. 1 and 2 are diagrams showing the manufacturing process of a compound superconducting conductor according to an example of the present invention. The method for manufacturing the multi-superconducting wire of this example will be described below with reference to these figures.
【0018】まず、純銅からなる管状部材に、大気中に
て 600℃、16時間の加熱処理を施した。次いで、
酸化銅の形成によって黒化した表面を光輝にするため、
さらに 600℃の真空中で熱処理した。このような加
熱処理を施したCu管を、マトリックス構成部材として
使用し、超電導体素線を以下の要領により作製した。First, a tubular member made of pure copper was heat treated at 600° C. for 16 hours in the atmosphere. Then,
In order to brighten the blackened surface due to the formation of copper oxide,
Further, heat treatment was performed in a vacuum at 600°C. The Cu tube subjected to such heat treatment was used as a matrix component, and a superconductor wire was produced in the following manner.
【0019】図1(a)に示すように、Nbチューブ1
1内にSn棒12が充填されたCu管13を挿入した後
、さらにこれを上記加熱処理が施されたCu管14内に
挿入し、一体化して超電導体素線15を作製した。上記
加熱処理が施されたCu管14は、Cuマトリックスの
構成部材となるものである。As shown in FIG. 1(a), an Nb tube 1
After inserting the Cu tube 13 filled with the Sn rods 12 into the Cu tube 14, this was further inserted into the Cu tube 14 which had been subjected to the heat treatment, and the superconductor wire 15 was produced by integrating the Cu tube 13 into the Cu tube 14. The Cu tube 14 subjected to the above heat treatment becomes a constituent member of the Cu matrix.
【0020】次に、図1(b)に示すように、上記超電
導体素線15を多数本束ね、アルミナ分散強化銅( 1
.1wt% Al2 O 3 −Cu)管16内に挿入
した。このアルミナ分散強化銅管16は、目的とする超
電導線の最外層を構成するものである。Next, as shown in FIG. 1(b), a large number of the superconductor wires 15 are bundled and alumina dispersion strengthened copper (1
.. 1wt% Al2O3-Cu) was inserted into the tube 16. This alumina dispersion-strengthened copper tube 16 constitutes the outermost layer of the intended superconducting wire.
【0021】上記多数本の超電導体素線15を挿入した
アルミナ分散強化銅管16を、図2(a)に示すように
、スウェージングマシンによって一体化して、目的とす
る超電導線の原型となる構造体を作製した。この一体化
工程で、上記加熱処理が施されたCu管14はCuマト
リックスを形成する。この後、上記一体化した構造体に
、冷間にて減面加工(伸線加工)を施して、直径1.1
2mmの丸形線17を得た。[0021] The alumina dispersion-strengthened copper tube 16 into which a large number of superconducting wires 15 are inserted is integrated by a swaging machine to form a prototype of the desired superconducting wire, as shown in FIG. 2(a). A structure was created. In this integration step, the Cu tube 14 subjected to the heat treatment forms a Cu matrix. After this, the integrated structure was subjected to a cold area reduction process (wire drawing process) to a diameter of 1.1 mm.
A 2 mm round wire 17 was obtained.
【0022】次に、上記丸形線17を加圧ローラで圧延
し、断面形状が 0.7mm× 1.4mmの長方形と
なるように加工して、図2(b)に示すように平角線1
8を作製した。この平角線18の断面構造を顕微鏡で観
察したところ、図2(b)に示したように、超電導体素
線15の形状はおおよそ丸形を維持していた。これは、
図2(a)に示したように、丸形線17に印加された圧
力(図中、矢印Aで示す)が、機械的強度が大きい最外
層のアルミナ分散強化銅管16に受け止められると共に
、内部のCuマトリックス14は、伸線加工によって軟
化現象を起こしており、マトリックス14内の超電導体
素線15の移動が起き易くなっているためである。Next, the round wire 17 is rolled with a pressure roller and processed to have a rectangular cross-sectional shape of 0.7 mm x 1.4 mm, so as to form a rectangular wire as shown in FIG. 2(b). 1
8 was produced. When the cross-sectional structure of this rectangular wire 18 was observed under a microscope, the shape of the superconductor strand 15 maintained a roughly round shape, as shown in FIG. 2(b). this is,
As shown in FIG. 2(a), the pressure applied to the round wire 17 (indicated by arrow A in the figure) is received by the outermost alumina dispersion-strengthened copper tube 16, which has high mechanical strength. This is because the internal Cu matrix 14 has undergone a softening phenomenon due to the wire drawing process, and the superconductor wires 15 within the matrix 14 are likely to move.
【0023】この後、上記平角線18に、真空中で 7
00℃にて30時間熱処理を施し、Nbチューブ11と
内部のCu管13中を拡散してきたSnとを反応させて
、図2(b)では図示を省略したが、Nbチューブ11
の内周側にNb3 Sn層を形成して、目的とする平角
形の超電導線を得た。[0023] After that, the above rectangular wire 18 is 7
Heat treatment was performed at 00° C. for 30 hours to cause the Nb tube 11 to react with the Sn that had diffused in the internal Cu tube 13. Although not shown in FIG. 2(b), the Nb tube 11
A Nb3Sn layer was formed on the inner peripheral side of the wire to obtain the desired rectangular superconducting wire.
【0024】このようにして得た平角形超電導線の臨界
電流密度を、断面の短辺方向に磁場を印加した状態と長
辺方向に磁場を印加した状態それぞれについて測定した
。その結果を図3に示す。図3から明らかなように、磁
場の印加方向に対する臨界電流密度の異方性が従来の平
角形超電導線(図5参照)に比べて大幅に改善されてい
ることが分かる。例えば、断面の短辺方向に磁場を印加
した状態では、15テスラで 850A/mm2 であ
り、また長辺方向に磁場を印加した状態では、15テス
ラで800A/mm2 であった。また、平角状に加工
する前の丸形線を同様にして作製し、これに同様な熱処
理を施して得た超電導線の臨界電流密度を測定したとこ
ろ、935A/mm2 であった。このことから、超電
導体素線を偏平させることなく平角状に加工することに
よって、臨界電流密度の値自体も丸形超電導線に近い値
が得られることが分かる。The critical current density of the rectangular superconducting wire thus obtained was measured in a state in which a magnetic field was applied in the short side direction of the cross section and in a state in which a magnetic field was applied in the long side direction. The results are shown in FIG. As is clear from FIG. 3, the anisotropy of the critical current density with respect to the direction of magnetic field application is significantly improved compared to the conventional rectangular superconducting wire (see FIG. 5). For example, when a magnetic field was applied in the direction of the short side of the cross section, it was 850 A/mm2 at 15 Tesla, and when the magnetic field was applied in the direction of the long side, it was 800 A/mm2 at 15 Tesla. Further, a round wire before being processed into a rectangular shape was produced in the same manner, and the critical current density of the superconducting wire obtained by subjecting it to the same heat treatment was measured and found to be 935 A/mm2. From this, it can be seen that by processing the superconductor strand into a rectangular shape without flattening it, a critical current density value itself close to that of a round superconducting wire can be obtained.
【0025】[0025]
【発明の効果】以上説明したように、本発明の化合物超
電導導体の製造方法によれば、平角状の超電導導体を作
製する際に、超電導体素線を偏平状に変形させることな
く、所定の断面矩形状に容易に加工することが可能とな
るため、磁場の印加方向に対する臨界電流密度等の超電
導特性の異方性が小さい化合物超電導導体を提供するこ
とが可能となる。これにより、平角状の超電導導体を使
用する際の自由度を大幅に向上させることが可能となる
。[Effects of the Invention] As explained above, according to the method for producing a compound superconducting conductor of the present invention, when producing a rectangular superconducting conductor, a predetermined shape can be obtained without deforming the superconducting wire into a flat shape. Since it can be easily processed into a rectangular cross-sectional shape, it is possible to provide a compound superconducting conductor with small anisotropy in superconducting properties such as critical current density with respect to the direction of application of a magnetic field. This makes it possible to greatly improve the degree of freedom when using rectangular superconducting conductors.
【図1】本発明の一実施例の超電導線の製造工程の一部
を示す断面図である。FIG. 1 is a cross-sectional view showing a part of the manufacturing process of a superconducting wire according to an embodiment of the present invention.
【図2】図1に続く超電導線の製造工程を示す断面図で
ある。FIG. 2 is a cross-sectional view showing the superconducting wire manufacturing process following FIG. 1;
【図3】本発明の一実施例により得た平角形超電導線の
印加磁場方向に対する臨界電流密度を示す図である。FIG. 3 is a diagram showing the critical current density of a rectangular superconducting wire obtained according to an example of the present invention with respect to the direction of an applied magnetic field.
【図4】従来の平角形超電導線の断面構造を示す図であ
る。FIG. 4 is a diagram showing a cross-sectional structure of a conventional rectangular superconducting wire.
【図5】従来の平角形の超電導線の印加磁場方向に対す
る臨界電流密度を示す図である。FIG. 5 is a diagram showing the critical current density of a conventional rectangular superconducting wire with respect to the direction of an applied magnetic field.
11……Nbチューブ
12……Sn棒
13……Cu管
14……Cuマトリックス(加熱処理が施されたCu管
)15……超電導体素線
16……アルミナ分散強化銅管
17……丸形線
18……平角線11...Nb tube 12...Sn rod 13...Cu tube 14...Cu matrix (heat-treated Cu tube) 15...Superconductor wire 16...Alumina dispersion-strengthened copper tube 17...Round shape Line 18...Flat line
Claims (1)
を形成する化合物超電導体材料を含む多数の素線を、
500℃〜 700℃の範囲の温度で加熱処理されたC
u系マトリックス内に埋設する工程と、前記Cu系マト
リックスの外周側に強化銅を一体化する工程と、この一
体化された構造体を、所定の外形形状に冷間加工する工
程と、前記加工体に対して、前記化合物超電導体の生成
温度領域での熱処理を施す工程とを有することを特徴と
する化合物超電導導体の製造方法。Claim 1: A large number of strands containing a compound superconductor material that reacts with heat treatment to form a compound superconductor,
C heat treated at a temperature ranging from 500℃ to 700℃
a step of embedding in a u-based matrix, a step of integrating reinforcing copper on the outer peripheral side of the Cu-based matrix, a step of cold working this integrated structure into a predetermined external shape, and a step of said processing. A method for manufacturing a compound superconducting conductor, comprising the step of subjecting the body to a heat treatment in a temperature range in which the compound superconductor is formed.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3064448A JPH04298917A (en) | 1991-03-28 | 1991-03-28 | Manufacture of compound superconductor |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3064448A JPH04298917A (en) | 1991-03-28 | 1991-03-28 | Manufacture of compound superconductor |
Publications (1)
| Publication Number | Publication Date |
|---|---|
| JPH04298917A true JPH04298917A (en) | 1992-10-22 |
Family
ID=13258548
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3064448A Withdrawn JPH04298917A (en) | 1991-03-28 | 1991-03-28 | Manufacture of compound superconductor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH04298917A (en) |
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2007173102A (en) * | 2005-12-22 | 2007-07-05 | Kobe Steel Ltd | PRECURSOR FOR MAKING Nb3Sn SUPERCONDUCTIVE WIRE ROD AND ITS MANUFACTURING METHOD |
| WO2023013726A1 (en) | 2021-08-06 | 2023-02-09 | 古河電気工業株式会社 | Precursor wire for compound superconducting wire, compound superconducting wire, and rewinding method for compound superconducting wire |
-
1991
- 1991-03-28 JP JP3064448A patent/JPH04298917A/en not_active Withdrawn
Cited By (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2007173102A (en) * | 2005-12-22 | 2007-07-05 | Kobe Steel Ltd | PRECURSOR FOR MAKING Nb3Sn SUPERCONDUCTIVE WIRE ROD AND ITS MANUFACTURING METHOD |
| WO2023013726A1 (en) | 2021-08-06 | 2023-02-09 | 古河電気工業株式会社 | Precursor wire for compound superconducting wire, compound superconducting wire, and rewinding method for compound superconducting wire |
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