JPS596486B2 - Superconducting coil manufacturing method - Google Patents
Superconducting coil manufacturing methodInfo
- Publication number
- JPS596486B2 JPS596486B2 JP52089638A JP8963877A JPS596486B2 JP S596486 B2 JPS596486 B2 JP S596486B2 JP 52089638 A JP52089638 A JP 52089638A JP 8963877 A JP8963877 A JP 8963877A JP S596486 B2 JPS596486 B2 JP S596486B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting
- coil
- superconducting wire
- wire
- manufacturing
- 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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- Superconductor Devices And Manufacturing Methods Thereof (AREA)
- Manufacturing Cores, Coils, And Magnets (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 nuclear fusion reactors is being considered, but the size of superconducting coils is gigajoule (GJ=109 J) or larger.
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によつ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。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。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1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2
00を複数個重ねて、ボルト9及びナット10で締付け
て組立てられている。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. 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. 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 1 made of metal or an insulator. A superconducting disk 2 formed by providing a coil groove and storing a superconducting wire 2 in the coil groove.
It is assembled by stacking a plurality of 00 and tightening them with 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bに示すレーストラック形コイル1、あるいは第3図
c(7)D形コイル1である。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。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 FIG. b or the D-type coil 1 shown in FIG. 3c (7). 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(Pb−Sn等の金属性接
着物)15によつて固着されて構成されている。FIGS. 4a and 4b are perspective views of solder-type superconducting wires, 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 (metallic material such as Pb-Sn). It is configured to be fixed by an adhesive 15.
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に)で電気抵抗率の小さい銅やアルミニウムで
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 a low electrical resistivity at extremely low temperatures (for example, liquid helium temperature of 4.2), and copper is currently often used.
超電導素線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ニウム
を被覆したもの、銅などの常電導金属の中に複数本の超
電導フイ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イ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
よい。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つて、第5図
b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 wire 13 may be a superconductor itself such as Nb-Ti or Nb3Sn, but it may also be a superconductor coated with copper or aluminum, or an ultra-fine superconductor in which multiple superconducting filaments are embedded in a normal conductive metal such as copper. It may be a multicore superconducting wire or an ultrafine multicore twisted superconducting wire in which the superconducting filament is twisted and embedded in a normal conducting metal. 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 a perspective view in FIG. 5a, for example. A flat aggregate 14 as shown in b 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つて
も使用することができる。Note that although the superconducting wire 2 shown in FIG. 4 is provided with a groove 12, it is a superconducting wire in which a superconducting wire assembly 14 is fixed with solder to the side surface of a rectangular normal-conducting metal substrate 11 without a groove. It 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。常
電導金属基材11の溝12に超電導素線13をソルダ1
5で固着することによつ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。
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ツト・ワイス、第2図のデ
イスク形超電導コイルではエツヂ・ワイスである。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10mf60muをもつものである。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
ラツト・ワイスで0.5(f)、エツヂ・ワイスで3(
:f)の歪みが超電導線2に発生する。Next, a conventional method for manufacturing superconducting coils will be described. Solder 1 superconducting wire 13 into groove 12 of normal conductive metal base material 11
A superconducting coil 1 is formed by winding the superconducting wire 2 manufactured by fixing the superconducting wires 5 into the shape shown in FIG.
The bending of the superconducting wire during coil winding is a flat twist in the pancake-shaped superconducting coil shown in FIG. 1, and an edge twist in the disk-shaped superconducting coil shown in FIG. The superconducting coil 1 used in energy storage devices and nuclear fusion reactors is gigantic and has an energy of more than gigajoules.
The superconducting wire 2 wound around this has large dimensions, for example, outer dimensions of 10 mf and 60 mu, which can carry a large current, for example, 30,000 amperes. When winding such a large superconducting wire 2 into the shape shown in Fig. 3, if the minimum bending radius of the coil is 1 m, for example, 0.5 (f) for a flat weiss and 3 (f) for an edge weiss. (
:f) distortion occurs in the superconducting wire 2.
特にエツヂ・ワイス曲げの場合の歪みは大きい。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のもつ超電導電流容量を大
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。Distortion is particularly large in edge-weiss bending. This distortion of the superconducting wire during coil winding greatly reduces the superconducting current 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。この発明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
れたもので、超電導線2が巻回による変形を受ける際に
、ソルダ15が溶融状態にあるようにして、超電導素線
13に歪みの加わることを避けることにより、エネルギ
蓄積装置や核融合炉に使用される超電導特性の低下のな
い大形超電導コイルを提供し得るものである。In particular, when the superconductor is a compound such as Nb3Sn, the deterioration of superconducting properties is significant. This invention was made in order to eliminate the drawbacks of the conventional method of manufacturing a superconducting coil as described above, and when the superconducting wire 2 is deformed by winding, the solder 15 is in a molten state. By avoiding the addition of strain to the superconducting strands 13, it is possible to provide a large superconducting coil that is used in energy storage devices and nuclear fusion reactors without deteriorating its superconducting properties.
第6図はこの発明の超電導コイルの製造方法の一実施例
を示す。FIG. 6 shows an embodiment of the method for manufacturing a superconducting coil according to the present invention.
線材ドラム16から供給された超電導線2は、コイル巻
型17に巻き取られコイルに成形される。コイル巻型1
7に近接して加熱装置18を設け、超電導線2を加熱し
、その構成要素であるソルダ15を溶融状態に保つたま
まコイル巻型に巻き取られるようにする。このようにす
れば超電導線2が巻回による変形を受けても、その構成
要素である超電導素線13は全く歪みを生じない。何故
ならば、溶融状態にあるソルダ15は全く固着力を失つ
ているため、超電導素線13相互の間、或いは超電導素
線と常電導金属基材11との間は固着されておらず超電
導素線の集合体14は自由に変形できるからである。コ
イル巻型に巻き取られ変形を終えた超電導線は自然冷却
され、又は必要があれば強制冷却を施されてソルダ15
は再び固化し、固着力を回復し元の超電導線の状態にも
どる。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に固着されたまま巻回された場合に生
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。The superconducting wire 2 supplied from the wire drum 16 is wound around a coil former 17 and formed into a coil. Coil winding form 1
A heating device 18 is provided adjacent to the superconducting wire 7 to heat the superconducting wire 2 so that the superconducting wire 2 is wound onto a coil former while keeping the solder 15, which is a component thereof, in a molten state. In this way, even if the superconducting wire 2 is deformed by winding, the superconducting wire 13, which is a component thereof, will not be distorted at all. This is because the solder 15 in a molten state has completely lost its adhesion, so the superconducting wires 13 are not bonded to each other, or the superconducting wires and the normal conductive metal base 11 are not bonded and the superconducting wires are not bonded to each other. This is because the line assembly 14 can be freely deformed. The superconducting wire that has been wound into a coil former and has finished its deformation is cooled naturally or, if necessary, forcedly cooled to solder 15.
solidifies again, regains its adhesion, and returns to its original state as a superconducting wire. As described above, according to the present invention, since it is impossible to generate the distortion that occurs when the superconducting wire 13 is wound while being fixed to the normal conductive metal base material 11, it is possible to create a superconducting coil without deterioration of superconducting properties. can be provided.
なお、第6図では第3図aに示す円形コイルの製造の場
合を示しているが、第3図bのレーストラツクコイル、
第3図COD形コイル、あるいは第1図に示すパンケー
キ形コイルの製造の場合にも発発明をそのまま適用する
ことができる。Although FIG. 6 shows the case of manufacturing the circular coil shown in FIG. 3a, the racetrack coil shown in FIG. 3b,
The invention can be applied as is to the production of the COD type coil shown in FIG. 3 or the pancake type coil shown in FIG.
また、加熱装置としては通常のヒータによる加熱炉でも
良いし、他の誘導加熱装置や超電導線の適当な部分に電
流を通じる通電加熱等の方法が用いられても良いことは
言うまでもない。なお、上記の超電導コイルでは、超電
導線2は加熱装置18を経てコイル巻型17に巻回され
たが、ほぼコイル形状に巻回してのち超電導コイルに形
成することもできる。It goes without saying that the heating device may be a heating furnace using a normal heater, or other induction heating devices or a method such as electrical heating in which a current is passed through an appropriate portion of the superconducting wire. In the above-mentioned superconducting coil, the superconducting wire 2 was passed through the heating device 18 and wound around the coil winding die 17, but the superconducting wire 2 can also be wound into a substantially coil shape and then formed into a superconducting coil.
この方法は特にデイスク形超電導コイルにおいて有効で
ある。以上のようにこの発明によれば、ソルダ方式超電
導線を巻回して成る超電導コイルの製造において、超電
導線が巻回による変形を受ける際に、ソルダが溶融状態
にあるようにしているので、超電導素線に歪みが加わる
ことなく、超電導特性が低下することのない大形超電導
コイルを製造することができる。This method is particularly effective for disk-shaped superconducting coils. As described above, according to the present invention, in manufacturing a superconducting coil formed by winding solder-type superconducting wire, the solder is kept in a molten state when the superconducting wire is deformed by winding, so that the superconducting A large superconducting coil can be manufactured without strain being applied to the strands and without deterioration of superconducting properties.
第1図はパンケーキ形超電導コイルの一部破断図、第2
図はデイ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図はソルダ方式超電導線
の斜視図、第5図は撚線および帯状撚線を示す斜視図、
第6図はこの発明の超電導コイル製造方法の一実施例を
示す図である。Figure 1 is a partially cutaway view of a pancake-shaped superconducting coil, Figure 2
3 is a perspective view showing the shape of the superconducting coil, FIG. 4 is a perspective view of a solder-type superconducting wire, and FIG. 5 is a perspective view showing stranded wires and strip-shaped stranded wires.
FIG. 6 is a diagram showing an embodiment of the superconducting coil manufacturing method of the present invention.
Claims (1)
で固着した超電導線を巻回して成る超電導コイルの製造
方法において、上記超電導線を加熱して上記金属性接着
物を溶融状態にして巻回するようにしたことを特徴とす
る超電導コイルの製造方法。 2 常電導金属基材の表面に超電導素線を金属性接着物
で固着した超電導線を巻回してなる超電導コイルの製造
方法において、上記超電導線を加熱して上記金属性接着
物を溶融状態にして略コイル状に巻回し、その後所定の
コイル形状に成形するようにしたことを特徴とする超電
導コイルの製造方法。[Scope of Claims] 1. A method for manufacturing a superconducting coil comprising winding a superconducting wire in which a superconducting wire is fixed with a metallic adhesive on the surface of a normal-conducting metal base material, wherein the superconducting wire is heated to form the metallic material. A method for manufacturing a superconducting coil, characterized in that the adhesive is wound in a molten state. 2. A method for manufacturing a superconducting coil in which a superconducting wire having a superconducting wire fixed to the surface of a normal-conducting metal base material with a metallic adhesive is wound, the superconducting wire being heated to melt the metallic adhesive. 1. A method for manufacturing a superconducting coil, comprising: winding the superconducting coil into a substantially coil shape, and then forming the coil into a predetermined coil shape.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52089638A JPS596486B2 (en) | 1977-07-25 | 1977-07-25 | Superconducting coil manufacturing method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP52089638A JPS596486B2 (en) | 1977-07-25 | 1977-07-25 | Superconducting coil manufacturing method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS5424595A JPS5424595A (en) | 1979-02-23 |
| JPS596486B2 true JPS596486B2 (en) | 1984-02-13 |
Family
ID=13976303
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP52089638A Expired JPS596486B2 (en) | 1977-07-25 | 1977-07-25 | Superconducting coil manufacturing method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS596486B2 (en) |
-
1977
- 1977-07-25 JP JP52089638A patent/JPS596486B2/en not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS5424595A (en) | 1979-02-23 |
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