JPS5855649B2 - Superconducting coil manufacturing method - Google Patents
Superconducting coil manufacturing methodInfo
- Publication number
- JPS5855649B2 JPS5855649B2 JP51123145A JP12314576A JPS5855649B2 JP S5855649 B2 JPS5855649 B2 JP S5855649B2 JP 51123145 A JP51123145 A JP 51123145A JP 12314576 A JP12314576 A JP 12314576A JP S5855649 B2 JPS5855649 B2 JP S5855649B2
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- Prior art keywords
- superconducting
- coil
- base material
- metal base
- conducting metal
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- Heat Treatment Of Nonferrous Metals Or Alloys (AREA)
- Coil Winding Methods And Apparatuses (AREA)
Description
【発明の詳細な説明】
この発明は核融合装置、エネルギ蓄積装置等に使用され
る大形の超電導コイルの製造方法に関するものである。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a method for manufacturing large-sized superconducting coils used in nuclear fusion devices, energy storage devices, and the like.
エネルギ蓄積装置や核融合炉用の磁界発生装置の構成要
素として超電導コイルの使用が考えられているが、超電
導コイルの大きさはギガジュール(GJ = 109J
)以上の巨大なものである。The use of superconducting coils as a component of energy storage devices and magnetic field generators for fusion reactors is being considered, but the size of superconducting coils is gigajoule (GJ = 109J).
) or more.
第1図は大形超電導コイルの一種であるパンケーキ形超
電導コイルの一部破断斜視図で、この超電導コイル1は
、超電導線2をターン間スペーサ3を介して巻回したパ
ンケーキコイル100を複数個、層間スペーサ4を介し
て巻枠5内に積重ねて固定した構成を有し、超電導線2
はターン間・層間の両方ともターン間スペーサ3および
層間スペーサ4によって電気的に絶縁され、かつ層間ス
ペーサ4により、液体ヘリウムなどの冷却媒体が流され
る間隙6が形成される。FIG. 1 is a partially cutaway perspective view of a pancake-shaped superconducting coil, which is a type of large-sized superconducting coil. It has a structure in which a plurality of superconducting wires 2 are stacked and fixed in a winding frame 5 via interlayer spacers 4.
Both the turns and layers are electrically insulated by interturn spacers 3 and interlayer spacers 4, and interlayer spacers 4 form gaps 6 through which a cooling medium such as liquid helium flows.
この間隙6は超電導線2の表面に発生した冷却媒体の気
泡を逃がす役割と、冷却媒体を供給する役割をもつ。This gap 6 has the role of allowing air bubbles of the cooling medium generated on the surface of the superconducting wire 2 to escape, and the role of supplying the cooling medium.
第2図は大形超電導コイルの一種であるディスク形超電
導コイルの断面図で、この超電導コイル1では、金属ま
たは絶縁物よりなる板状の保持部材7の両側面に複数個
のコイル溝8を設け、そのコイル溝に超電導線2を収納
して形成される超電導ディスク200を複数個重ねて、
ボルト9及びナツト10で締付けて組立てられている。FIG. 2 is a cross-sectional view of a disk-shaped superconducting coil, which is a type of large superconducting coil. In this superconducting coil 1, a plurality of coil grooves 8 are formed on both sides of a plate-shaped holding member 7 made of metal or an insulator. A plurality of superconducting disks 200 formed by storing superconducting wires 2 in the coil grooves are stacked,
It is assembled by tightening bolts 9 and nuts 10.
ディスク形超電導コイル1は、第1図のパンケーキ形超
電導コイルと同様の第3図aに示す円形コイル1、第3
図すに示すレーストラック形コイル1、あるいは第3図
CのD形コイル1である。The disk-shaped superconducting coil 1 includes a circular coil 1 shown in FIG. 3a, similar to the pancake-shaped superconducting coil shown in FIG.
This is the racetrack coil 1 shown in the figure or the D-type coil 1 shown in FIG. 3C.
これら大形超電導コイルに使用される大電流容量の超電
導線2として最適と考えられるものは、ソルダ方式超電
導線である。A solder type superconducting wire is considered to be optimal as the large current capacity superconducting wire 2 used in these large superconducting coils.
第4図aおよびbはソルダ方式超電導線の斜視図で、常
電導金属基材11に切られた溝12に複数本の超電導素
線13の集合体14がソルダ(pbSn等の金属性接着
物)15によって固着されて横取されている。FIGS. 4a and 4b are perspective views of a solder-type superconducting wire, in which an aggregate 14 of a plurality of superconducting strands 13 is placed in a groove 12 cut in a normal-conducting metal base material 11 with solder (a metallic adhesive such as pbSn). ) 15 and has been usurped.
常電導金属基材11は、極低温(例えば液体ヘリウム温
度4.2 K )で電気抵抗率の小さい銅やアルミであ
り、現在銅がよく使用されている。The normally conductive metal base material 11 is made of copper or aluminum, which has low electrical resistivity at extremely low temperatures (for example, liquid helium temperature of 4.2 K), and copper is currently often used.
常電導素線13は、Nb Ti+ Nb3Snなどの
超電導体そのものでもよいが、超電導体に銅やアルミを
被覆したもの、銅などの常電導金属の中に複数本の超電
導フィラメントが埋め込まれた極細多芯超電導線、ある
いは上記超電導フィラメントがツイストされて常電導金
属の中に埋め込まれた極細多芯ツイスト超電導線でも良
い。The normal conductive wire 13 may be a superconductor itself such as NbTi+Nb3Sn, but it may also be a superconductor coated with copper or aluminum, or an ultra-fine multilayer wire in which multiple superconducting filaments are embedded in a normal conductive metal such as copper. It may be a core superconducting wire or an ultrafine multicore twisted superconducting wire in which the superconducting filament is twisted and embedded in a normal conducting metal.
超電導素線の集合体14は例えば第5図aに斜視図で示
すような、断面同一円周上に超電導素線13が配置され
た中空の撚り線を圧延することによって、第5図すに示
すような扁平な集合体14を容易に得ることができる。The superconducting strand assembly 14 is produced by rolling a hollow stranded wire in which the superconducting strands 13 are arranged on the same circumference in cross section, as shown in the perspective view in FIG. 5a, for example. A flat aggregate 14 as shown can be easily obtained.
上記の集合体14は帯状撚線であるが、帯状撚線の代り
に帯状編組線でもよい。Although the above-mentioned aggregate 14 is a band-shaped twisted wire, a band-shaped braided wire may be used instead of the band-shaped twisted wire.
なお、第4図の超電導線2には溝12が設けられている
が、溝のない平角の常電導金属基材11の側面に超電導
素線集合体14をソルダで固着した超電導線であっても
使用することができる。Although the superconducting wire 2 in FIG. 4 is provided with grooves 12, it is a superconducting wire in which a superconducting strand assembly 14 is fixed with solder to the side surface of a rectangular normal-conducting metal substrate 11 without grooves. can also be used.
次に従来の超電導コイルの製造方法について述べる。Next, a conventional method for manufacturing superconducting coils will be described.
常電導金属基材11の溝12に超電導素線13をソルダ
15で固着することによって製作された超電導線2を、
第3図に示す形状に巻回して超電導コイル1を形成する
。A superconducting wire 2 manufactured by fixing a superconducting wire 13 to a groove 12 of a normal conducting metal base material 11 with a solder 15,
The superconducting coil 1 is formed by winding it into the shape shown in FIG.
コイル巻回のときの超電導線の曲げは、第1図のパンケ
ーキ形超電導コイルではフラット・ワイズ、第2図のデ
ィスク形超電導コイルではエッヂ゛・ワイズである。The bending of the superconducting wire during coil winding is flat-wise in the pancake-shaped superconducting coil shown in FIG. 1, and edge-wise in the disk-shaped superconducting coil shown in FIG.
エネルギ蓄積装置や核融合炉に使用される超電導コイル
1はギガジュール以上のエネルギをもつ巨大なものであ
り、これに巻回される超電導線2は大電流、例えば3万
アンペア、を通電することのできる大きい寸法、例えば
外側寸法10朋×6011t11t、をもつものである
。The superconducting coil 1 used in energy storage devices and nuclear fusion reactors is gigantic and has an energy of gigajoules or more, and the superconducting wire 2 wound around it is capable of carrying a large current, for example, 30,000 amperes. It has large dimensions such as outer dimensions of 10 mm x 6,011 mm and 11 mm.
このように大きい寸法の超電導線2を第3図のような形
状に巻回する場合、コイルの最少曲げ半径を例えば1m
とすると、フラット・ワイズで0.5%、エッヂ・ワイ
ズで3%の歪みが超電導線2に発生する。When winding such a large superconducting wire 2 in the shape shown in Figure 3, the minimum bending radius of the coil should be set to, for example, 1 m.
Then, a strain of 0.5% flat-wise and 3% edge-wise occurs in the superconducting wire 2.
特にエッヂ・ワイズ曲げの場合の歪みは大きい。Especially in the case of edgewise bending, the distortion is large.
このコイル巻回時の超電導線の歪みは、超電導線2の基
本的構成要素である超電導素線13のもつ超電流容量を
大巾に低下させ、結果として超電導コイル1のつくる磁
界を設計値より大巾に低下させることがある。This distortion of the superconducting wire during coil winding greatly reduces the supercurrent capacity of the superconducting wire 13, which is a basic component of the superconducting wire 2, and as a result, the magnetic field created by the superconducting coil 1 is lower than the design value. It can be significantly reduced.
特に超電導体がNb3Sn等の化合物である場合には超
電導特性の低下は著しい。In particular, when the superconductor is a compound such as Nb3Sn, the deterioration of superconducting properties is significant.
第6図は上記のような従来の超電導コイルの製造方法の
欠点を除去するためになされた先行技術の超電導コイル
の製造方法の一実施例で、第6図aのように常電導金属
基材11をコイル形状に曲げて、・例えば、第2図の板
状の保持部材7に設けられたコイル溝8に固定してから
のち、第6図すに示すように超電導素線集合体14を常
電導金属基材11の溝12にソルダで固着することによ
ってディスク形超電導コイル1を形成する。FIG. 6 shows an example of a prior art method for manufacturing a superconducting coil, which was made to eliminate the drawbacks of the conventional method for manufacturing a superconducting coil, as shown in FIG. 6a. 11 into a coil shape and fixing it, for example, in the coil groove 8 provided in the plate-shaped holding member 7 shown in FIG. 2, the superconducting strand assembly 14 is bent as shown in FIG. A disk-shaped superconducting coil 1 is formed by fixing it in the groove 12 of the normal-conducting metal base material 11 with solder.
このようにこの先行技術によれば超電導素線13が常電
導金属基材11に固着された後の巻回によって生ずる歪
みを発生させることが有り得ないから、超電導特性の低
下のない超電導コイルを提供することができる。In this way, according to this prior art, it is impossible to generate distortion caused by winding the superconducting wire 13 after it is fixed to the normal conductive metal base material 11, so that a superconducting coil without deterioration of superconducting properties is provided. can do.
尚、上記の超電導コイルでは、常電導金属基材11をコ
イル形状に成形してのち超電導素線集合体14を固着し
たが、常電導基材11をほぼコイル形状に曲げて超電導
素線集合体14を固着して作成した超電導線2をその後
完全にコイル形状にして超電導コイルを形成することも
できる。In the above superconducting coil, the normal conducting metal base material 11 is formed into a coil shape and then the superconducting strand assembly 14 is fixed, but the superconducting strand assembly 14 is fixed by bending the normal conducting base material 11 into a substantially coil shape. The superconducting wire 2 created by fixing the superconducting wires 14 can then be completely shaped into a coil to form a superconducting coil.
この場合、超電導線2の曲げによる歪みはほとんど生じ
ないOまた、この方法によれば、第4図すのように常電
導基材11の両面に超電導素線集合体14を固着するこ
ともできるし、第1図のパンケーキ形超電導コイルも製
作することができる。In this case, almost no distortion occurs due to bending of the superconducting wire 2. Also, according to this method, the superconducting wire assembly 14 can be fixed to both sides of the normal conducting base material 11 as shown in FIG. However, the pancake-shaped superconducting coil shown in FIG. 1 can also be manufactured.
上記のような先行技術の超電導コイルの製造方法によっ
て、従来技術により製造された超電導コイルにおける超
電導電流容量の低下を防ぐことはできる。By the method of manufacturing a superconducting coil of the prior art as described above, it is possible to prevent a decrease in superconducting current capacity in a superconducting coil manufactured by the prior art.
しかし、先行技術の超電導コイルの製造方法においては
、常電導金属基材11をコイル形状または略コイル形状
に曲げて超電導素線集合体14を固着して超電導線2を
作成しているので、常電導金属基材11は曲げ加工を受
けて加工硬化しており、その結果、常電導金属基材11
の抵抗率は増加する。However, in the prior art superconducting coil manufacturing method, the superconducting wire 2 is created by bending the normal conducting metal base material 11 into a coil shape or a substantially coil shape and fixing the superconducting strand assembly 14. The conductive metal base material 11 is subjected to bending and work hardened, and as a result, the normal conductive metal base material 11
The resistivity of increases.
常電導金属基材11の抵抗率ρ(Ω−CrrL)が増加
すると、超電導線2の安定化電流
が低下する。When the resistivity ρ (Ω-CrrL) of the normal conductive metal base material 11 increases, the stabilized current of the superconducting wire 2 decreases.
ここで、A (cit )は常電導金属基材の断面積、
5(CII′L)は超電導線が冷却媒体に接する部分の
冷却ペリメータ、ηは超電導線の冷却率、q(W/i)
は超電導線表面における臨界熱流束である。Here, A (cit) is the cross-sectional area of the normally conducting metal base material,
5 (CII'L) is the cooling perimeter of the part where the superconducting wire is in contact with the cooling medium, η is the cooling rate of the superconducting wire, q (W/i)
is the critical heat flux at the surface of the superconducting wire.
エネルギ蓄積装置や核融合炉用の大形超電導コイルで、
は超電導コイルの設計電流Idを安定化電流Irより若
干低くするのが通常かつ正統的な設計法である。Large superconducting coils for energy storage devices and fusion reactors.
The normal and orthodox design method is to make the design current Id of the superconducting coil slightly lower than the stabilizing current Ir.
したかって、安定化電流Irの低下をもたらす常電導金
属基材の抵抗率ρの増加は好ましくない。Therefore, an increase in the resistivity ρ of the normally conducting metal base material that causes a decrease in the stabilizing current Ir is not preferable.
例えば、加工度3%と10%の場合の常電導金属基材と
しての銅の抵抗率ρは約120%と約160%となり、
安定化電流はそれぞれ約90%と約70%に低下する。For example, the resistivity ρ of copper as a normal conductive metal base material when the working degree is 3% and 10% is approximately 120% and approximately 160%,
The stabilizing current drops to about 90% and about 70%, respectively.
さらに、常電導金属基材の曲げ半径を小さくして加工度
が大きくなると、銅の抵抗率ρはさらに増加し、安定化
電流はさらに低下する。Furthermore, when the bending radius of the normally conducting metal base material is made smaller and the degree of working is increased, the resistivity ρ of copper further increases and the stabilized current further decreases.
以上のことは銅についてであるが、アルミや他の常電導
金属基材についても同様のことが成り立つ0
このように、先行技術の超電導コイル製造方法には、常
電導金属基材の抵抗率ρを増加させ、その結果、超電導
線の安定化電流ね低下させるという欠点があった。Although the above applies to copper, the same holds true for aluminum and other normal conducting metal substrates. In this way, the prior art method for manufacturing superconducting coils requires that the resistivity ρ of the normal conducting metal substrate This has the disadvantage that the stabilizing current of the superconducting wire is decreased as a result.
この発明は上記のような先行技術の欠点を除去するため
になされたもので、コイル形状または略コイル形状に曲
げられた常電導金属基材11を熱処理することにより、
エネルギ蓄積装置や核融合炉に使用される安定化電流の
低下のない大形超電導コイルを提供し得るものである。This invention was made in order to eliminate the drawbacks of the prior art as described above, and by heat-treating the normal conductive metal base material 11 bent into a coil shape or approximately coil shape,
It is possible to provide a large superconducting coil for use in energy storage devices and nuclear fusion reactors that does not cause a drop in stabilizing current.
この発明の超電導コイルの製造方法の一実施例は、第6
図aのように常電導金属基材11をコイル形状に曲げて
、例えば、第2図の板状の保持部材1に設けられたコイ
ル溝8に固定してからのち、熱処理を施こすことによっ
て常電導金属基材11の抵抗率ρを曲げ加工前の抵抗率
にまで低め、第6図すに示すように超電導素線集合体1
4を常電導金属基材11の溝12にソルダで固着するこ
とによってディスク形超電導コイル1を形成する。One embodiment of the method for manufacturing a superconducting coil of this invention is the sixth embodiment of the method for manufacturing a superconducting coil.
By bending the normal conductive metal base material 11 into a coil shape as shown in Figure a, fixing it in the coil groove 8 provided in the plate-shaped holding member 1 shown in Figure 2, for example, and then subjecting it to heat treatment. The resistivity ρ of the normal conductive metal base material 11 is lowered to the resistivity before bending, and the superconducting wire assembly 1 is made as shown in FIG.
The disk-shaped superconducting coil 1 is formed by fixing the coil 4 to the groove 12 of the normal-conducting metal base material 11 with solder.
常電導金属基材11の熱処理は、常電導金属基材11ば
例えば銅の場合、真空炉内で熱処理温度400ないし5
00°C1熱処理時間0.5ないし2時間の条件で通常
実施されるが、上記条件に限定されるものではない。When the normal conductive metal base material 11 is made of copper, for example, the heat treatment of the normal conductive metal base material 11 is carried out in a vacuum furnace at a heat treatment temperature of 400 to 500.
The heat treatment is usually performed at 00° C. for 0.5 to 2 hours, but is not limited to the above conditions.
このように本発明によれば、超電導素線13が常電導金
属基材11に固着された後の巻回によって超電導素線1
3に生ずる歪みを発生させることが有り得ないだけでな
く、常電導金属基材11の曲げによって生ずる歪みをも
又除去することができるので、超電導線の曲げ半径に制
約されることなく、超電導通電容量および安定化電流の
低下のない超電導コイルを提供することができる。As described above, according to the present invention, the superconducting strand 13 is fixed to the normal conducting metal base material 11 by winding.
Not only is it impossible to generate the distortion caused by the bending of the normal conducting metal base material 11, but also the distortion caused by bending the normal conducting metal base material 11 can be removed. A superconducting coil without a decrease in capacity and stabilizing current can be provided.
尚、上記の超電導コイルは、常電導金属基材11をコイ
ル形状に成形してのち、常電導金属基材11を固定した
保持部材7を熱処理して、超電導素線集合体14を固着
したが、常電導金属基材11をほぼコイル形状に曲げて
熱処理したのち、その常電導金属基材11をコイル形状
に巻回して超電導素線集合体14を固着して超電導コイ
ルを形成することもできる。In addition, in the above superconducting coil, the normal conducting metal base material 11 is formed into a coil shape, and then the holding member 7 to which the normal conducting metal base material 11 is fixed is heat-treated to fix the superconducting strand assembly 14. It is also possible to form a superconducting coil by bending the normal conducting metal base material 11 into a substantially coil shape and heat-treating it, and then winding the normal conducting metal base material 11 into a coil shape and fixing the superconducting strand assembly 14. .
この場合、常電導金属基材11のみを熱処理すればよい
ので、熱処理装置を簡便化することができるという利点
がある。In this case, since it is only necessary to heat treat the normal conductive metal base material 11, there is an advantage that the heat treatment apparatus can be simplified.
さらに、この発明の超電導コイルの製造方法の他の実施
例では、常電導金属基材11をほぼコイル形状に曲げて
熱処理して、その常電導金属基材11の表面に超電導素
線集合体14を固着するか、あるいは超電導素線を巻回
して固着するかして作成した超電導線2をその後完全に
コイル形状にして超電導コイルを形成することもできる
。Furthermore, in another embodiment of the method for manufacturing a superconducting coil according to the present invention, the normal conducting metal base material 11 is bent into a substantially coil shape and heat treated, and the superconducting strand aggregates 14 are formed on the surface of the normal conducting metal base material 11. A superconducting wire 2 created by fixing a superconducting wire or winding and fixing a superconducting strand can then be completely formed into a coil shape to form a superconducting coil.
この場合、超電導線2の曲げによる歪みはほとんど生じ
ない。In this case, almost no distortion occurs due to bending of the superconducting wire 2.
また、この方法によれば、第4図すのように常電導金属
基材11の両辺に超電導素線集合体14を固着すること
もできるし、第1図のパンケーキ形超電導コイルをも製
作することもできる。Furthermore, according to this method, the superconducting wire assembly 14 can be fixed to both sides of the normal conducting metal base material 11 as shown in Fig. 4, and the pancake-shaped superconducting coil shown in Fig. 1 can also be manufactured. You can also.
以上のように、この発明によれば、常電導金属基材をコ
イル形状または略コイル形状に巻回して熱処理を施こし
てのち、超電導素線を固着するので、超電導線の曲げ半
径に制約されることなく、超電導電流容量と安定化電流
の低下のない大形超電導コイルを製造することができる
。As described above, according to the present invention, the superconducting wire is fixed after the normal conducting metal base material is wound into a coil shape or a substantially coil shape and heat treated, so that the bending radius of the superconducting wire is not a constraint. Therefore, it is possible to manufacture a large superconducting coil without deterioration in superconducting current capacity and stabilizing current.
第1図はパンケーキ形超電導コイルの一部破断図、第2
図はディスク形超電導コイルの断面図、第3図は超電導
コイル形状を示す斜視図、第4図は従来のソルダ方式超
電導線として完成した状態を示す斜視図、第5図は撚線
および帯状撚線を示す斜視図、第6図は先行技術の超電
導コイル製造法の一実施例である。
図において、1は超電導コイル、2は超電導線、11は
常電導金属基材、12は溝、13は超電導素線、14は
超電導素線集合体、15はソルダである。
なお、図中、同一符号は同一、又は相当部分を示す。Figure 1 is a partially cutaway view of a pancake-shaped superconducting coil, Figure 2
Figure 3 is a cross-sectional view of a disk-shaped superconducting coil, Figure 3 is a perspective view showing the shape of the superconducting coil, Figure 4 is a perspective view showing the completed state as a conventional solder type superconducting wire, and Figure 5 is a stranded wire and strip-shaped twisted wire. A perspective view showing lines, FIG. 6, is one embodiment of a prior art method of manufacturing superconducting coils. In the figure, 1 is a superconducting coil, 2 is a superconducting wire, 11 is a normal conducting metal base material, 12 is a groove, 13 is a superconducting wire, 14 is a superconducting wire assembly, and 15 is a solder. In addition, in the figures, the same reference numerals indicate the same or equivalent parts.
Claims (1)
コイル形状に巻回された常電導金属基材を熱処理する工
程、この熱処理された常電導金属基材の表面に超電導素
線をソルダで固着する工程を備えてなる常電導コイルの
製造方法。 2 常電導金属基材を略コイル形状に曲げる工程、この
略コイル形状に曲げられた常電導金属基材を熱処理する
工程、この熱処理された常電導金属基材をコイル形状に
巻回する工程、このコイル形状に巻回された常電導金属
基材の表面に超電導素線をソルダで固着する工程を備え
てなる超電導コイルの製造方法。 3 常電導金属基材を略コイル形状に曲げる工程、この
略コイル形状に曲げられた常電導金属基材を熱処理する
工程、この熱処理された常電導金属基材の表面に超電導
素線をソルダで固着して略コイル形状の超電導線を形成
する工程、この略コイル形状の超電導線をコイル形状に
巻回する工程を備えてなる超電導コイルの製造方法。[Claims] 1. A step of winding a normal conducting metal base material into a coil shape, a step of heat treating the normal conducting metal base material wound into a coil shape, and a surface of the heat treated normal conducting metal base material. A method for manufacturing a normal conductive coil, which comprises the step of fixing superconducting wires with solder. 2. A step of bending the normal conducting metal base material into a substantially coil shape, a step of heat treating the normal conducting metal base material bent into the substantially coil shape, a step of winding the heat treated normal conducting metal base material into a coil shape, A method for manufacturing a superconducting coil comprising the step of fixing a superconducting wire with solder to the surface of a normal-conducting metal base material wound into a coil shape. 3. A step of bending a normal conducting metal base material into a substantially coil shape, a step of heat treating the normal conducting metal base material bent into a substantially coil shape, and a step of applying a superconducting wire to the surface of the heat treated normal conducting metal base material with solder. A method for manufacturing a superconducting coil comprising the steps of fixing to form a substantially coil-shaped superconducting wire, and winding the substantially coil-shaped superconducting wire into a coil shape.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51123145A JPS5855649B2 (en) | 1976-10-13 | 1976-10-13 | Superconducting coil manufacturing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP51123145A JPS5855649B2 (en) | 1976-10-13 | 1976-10-13 | Superconducting coil manufacturing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5347797A JPS5347797A (en) | 1978-04-28 |
| JPS5855649B2 true JPS5855649B2 (en) | 1983-12-10 |
Family
ID=14853297
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP51123145A Expired JPS5855649B2 (en) | 1976-10-13 | 1976-10-13 | Superconducting coil manufacturing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS5855649B2 (en) |
-
1976
- 1976-10-13 JP JP51123145A patent/JPS5855649B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5347797A (en) | 1978-04-28 |
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