JPH0467327B2 - - Google Patents
Info
- Publication number
- JPH0467327B2 JPH0467327B2 JP5304384A JP5304384A JPH0467327B2 JP H0467327 B2 JPH0467327 B2 JP H0467327B2 JP 5304384 A JP5304384 A JP 5304384A JP 5304384 A JP5304384 A JP 5304384A JP H0467327 B2 JPH0467327 B2 JP H0467327B2
- Authority
- JP
- Japan
- Prior art keywords
- superconducting coil
- coil according
- fluid
- pipes
- wire
- 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 - Lifetime
Links
- 229910052751 metal Inorganic materials 0.000 claims description 16
- 239000002184 metal Substances 0.000 claims description 16
- 239000012530 fluid Substances 0.000 claims description 11
- 238000004804 winding Methods 0.000 claims description 9
- 239000003822 epoxy resin Substances 0.000 claims description 8
- 229920000647 polyepoxide Polymers 0.000 claims description 8
- 239000000463 material Substances 0.000 claims description 3
- 229910000838 Al alloy Inorganic materials 0.000 claims description 2
- 229910000881 Cu alloy Inorganic materials 0.000 claims description 2
- 229910001069 Ti alloy Inorganic materials 0.000 claims description 2
- 230000008018 melting Effects 0.000 claims description 2
- 238000002844 melting Methods 0.000 claims description 2
- 229920002050 silicone resin Polymers 0.000 claims description 2
- 229910000963 austenitic stainless steel Inorganic materials 0.000 claims 1
- 239000004020 conductor Substances 0.000 description 7
- 238000010791 quenching Methods 0.000 description 4
- 238000005470 impregnation Methods 0.000 description 3
- 238000007711 solidification Methods 0.000 description 3
- 230000008023 solidification Effects 0.000 description 3
- 230000006835 compression Effects 0.000 description 2
- 238000007906 compression Methods 0.000 description 2
- 238000010438 heat treatment Methods 0.000 description 2
- 239000011810 insulating material Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000000171 quenching effect Effects 0.000 description 2
- 230000002787 reinforcement Effects 0.000 description 2
- 239000004593 Epoxy Substances 0.000 description 1
- 102100040287 GTP cyclohydrolase 1 feedback regulatory protein Human genes 0.000 description 1
- 101710185324 GTP cyclohydrolase 1 feedback regulatory protein Proteins 0.000 description 1
- 229910000831 Steel Inorganic materials 0.000 description 1
- 230000015271 coagulation Effects 0.000 description 1
- 238000005345 coagulation Methods 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 238000007796 conventional method Methods 0.000 description 1
- 238000009792 diffusion process Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 239000003507 refrigerant Substances 0.000 description 1
- 230000003014 reinforcing effect Effects 0.000 description 1
- 230000006641 stabilisation Effects 0.000 description 1
- 238000011105 stabilization Methods 0.000 description 1
- 239000010959 steel Substances 0.000 description 1
- 239000002887 superconductor Substances 0.000 description 1
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F41/00—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties
- H01F41/02—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets
- H01F41/04—Apparatus or processes specially adapted for manufacturing or assembling magnets, inductances or transformers; Apparatus or processes specially adapted for manufacturing materials characterised by their magnetic properties for manufacturing cores, coils, or magnets for manufacturing coils
- H01F41/048—Superconductive coils
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/06—Coils, e.g. winding, insulating, terminating or casing arrangements therefor
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Manufacturing & Machinery (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Description
本発明は超電導コイルにおいて、クエンチの原
因である電磁力による導体の動きを阻止せんとす
るものである。
従来超電導コイルにおける撚線を固定する方法
としては
(1) 撚線の巻回中に張力を負荷する。
(2) 巻線後外部から補強線にて圧縮する。
(3) 巻線後エポキシ樹脂に含浸する。
(4) 巻線間に熱絶縁物を挿入する。
然しながらこれらの方法によると撚線を固定す
ることが出来ず、その中でも(3)によるエポキシ樹
脂含浸による場合には線材の動きを押えることが
出来うるも含浸後冷却するに伴つて熱収縮を生
じ、このときクラツクを生ずるときに放出される
熱によつてクエンチをおこすものであつた。又冷
媒と超電導線とが直接接触しないため安定化条件
のマージンを大きく選ぶ必要があり、コイルの総
合電流密度を低下せしめているものである。特に
Wind&Reat型コイルにおいては高温部(700℃
近傍)で処理されるため加熱冷却に伴う巻線の伸
び或は縮みが大きくエポキシ含浸のみによつては
巻回巻線の間隔を一定にすることが難しく高均質
なマグネツトをうることが出来難いものであつ
た。
本発明はかかる現状に鑑み鋭意研究を行つた結
果、超電導導体を巻回して形成する超電導コイル
の導体間をより強固に固定してクエンチを防止す
ると共に機械的強度を向上せしめる超電導コイル
を開発したものである。即ち本発明は中空部が真
円以外の形状からなる薄肉の非磁性パイプの外周
に平角成形撚線を巻付けた超電導コイルにおい
て、該中空部に300℃以下で硬化または凝固する
流体を注入し該パイプを膨脹せしめて該撚線を固
定せしめることを特徴とする超電導コイルであ
る。
本発明を図面について説明すると、第1図aに
示す如く薄肉の非磁性金属管1の円周上に導体素
線2を撚合せ、その後第1図bに示す如く該金属
管と導体とを偏平状に圧延成形する。なおこの場
合金属管は僅かな空隙部3を設けておくことが必
要である。
又第2図aに示す如く薄肉の非磁性金属管1を
偏平状に成型した後、該管の外周に導体素線2を
撚合せ成型する。なお、この場合と前記同様金属
管に空隙部を設けておく。
然る後上記の成型撚線のコイル巻を行う、例え
ば円筒型のボビンにコイル巻し、その外周に補強
のためにGFRPの筒を被覆するか或は絶縁材をは
こんで金属ワイヤ例えばSUSなどを巻いて縛り
つける。このとき線材の両端は外側に出し、その
まわりを補強する。
撚線の1端を開口したままにするか或は吸引状
態にして他端から該金属管内に充填流体4を流し
込む該金属管内に流体が満たされたら、片端を封
じて密閉し開口端から圧力をかけて第2図bに示
す如く該管1が膨脹するまで該流体を充填する。
充電後開口端も封口し、300℃以下の温度に加熱
して該流体を硬化又は凝固せしめて、本発明超電
導体をうるものである。
本発明において非磁性金属管としてはオーステ
ナイト系鋼管、チタン合金管、銅合金管、アルミ
合金管などが使用され、その肉厚については流体
の圧入によつて容易に膨脹しうる程度にすること
が必要であるが、該金属管の材質によつて夫々異
にするものである。通常肉厚は0.1〜1.0mm程度に
することが好ましい。又金属管の形状としては断
面が真円以外のものであれば特に限定するもので
はなく要は管内に流体を圧入することにより断面
積が増大する形状であればよい。例えば楕円形、
角形、偏平形のもの又は、第3図に示す如く内面
が楔状のもの又は凹凸部を有するものでもよい。
又金属管内に充填する流体としては該管内に内
圧を付加するための圧力媒体であればよく、熱伝
導性良好にして線膨脹係数が超電導線に近いガス
発生の少い低融点金属、シリコン樹脂、エポキシ
樹脂、ワツクス等が好ましい。
なお、該流体の固化又は凝固温度として300℃
以下と限定したが、その理由は300℃以上にした
場合には固化又は凝固時の温度で超電導特性が劣
化するためである。
次に本発明の実施例について説明する。
実施例
第1図aに示す如き24本のNb芯を有する素線
2を肉厚0.25mmのSUS300管1の外周に撚り合せ、
ターグスヘツドにより圧縮し第1図bに示す如く
中空部3を厚さ方向に沿つて0.2mmを有する偏平
状となし、この成形撚線を用いたソレノイドコイ
ルを2個作製した。この場合何れも巻回後外部を
外径0.8mmφのSUS304線にて緊締した後、700℃
にて3日間拡散熱処理を行つた後室温まで冷却し
て平角状成形撚線をえた。
然る後第2図aに示す如く該コイルの成形撚線
の1端を減圧しながら該SUS管の他端からエポ
キシ樹脂4を注入し、該管内をエポキシ樹脂で満
たした後、減圧していた1端を閉じ、更に6気圧
まで加圧し第2図bに示す如く該管1を膨出せし
め150時間で4時間キユアして本発明超電導コイ
ルをえた。
又本発明コイルと比較するために上記成形撚線
にその外側からエポキシ樹脂を含浸せしめ150℃
にて4時間キユアしてソレノイドコイルを2個作
製した。
斯くして得た本発明超電導コイルと比較例超電
導コイルとについてその性能を試みるために通電
試験を行つた。その結果は第1表に示す通りであ
る。
The present invention aims to prevent the movement of a conductor due to electromagnetic force, which is the cause of quenching, in a superconducting coil. Conventional methods for fixing stranded wires in superconducting coils include (1) applying tension while winding the stranded wires; (2) After winding, compress it from the outside with reinforcing wire. (3) Impregnate with epoxy resin after winding. (4) Insert thermal insulation between the windings. However, with these methods, it is not possible to fix the stranded wire, and among them, in the case of epoxy resin impregnation according to (3), although the movement of the wire can be suppressed, heat shrinkage occurs as the wire is cooled after impregnation. At this time, the quench was caused by the heat released when the crack occurred. Furthermore, since the refrigerant and the superconducting wire do not come into direct contact, it is necessary to select a large margin for the stabilization conditions, which reduces the overall current density of the coil. especially
Wind & Reat type coils have a high temperature section (700℃
Because the magnet wire is processed in the vicinity), the winding expands or contracts significantly as it heats and cools, making it difficult to maintain a constant spacing between the windings by epoxy impregnation alone, making it difficult to obtain a highly homogeneous magnet. It was hot. As a result of intensive research in view of the current situation, the present invention has developed a superconducting coil that is formed by winding a superconducting conductor and that more firmly fixes the conductors between the coils to prevent quenching and improves mechanical strength. It is something. That is, the present invention provides a superconducting coil in which rectangular shaped stranded wire is wound around the outer periphery of a thin non-magnetic pipe whose hollow part has a shape other than a perfect circle, in which a fluid that hardens or solidifies at 300°C or less is injected into the hollow part. The superconducting coil is characterized in that the stranded wires are fixed by expanding the pipe. To explain the present invention with reference to the drawings, conductor wires 2 are twisted around the circumference of a thin non-magnetic metal tube 1 as shown in FIG. 1a, and then the metal tube and the conductor are twisted together as shown in FIG. Roll and form into a flat shape. In this case, it is necessary to provide a small gap 3 in the metal tube. Further, as shown in FIG. 2a, after a thin non-magnetic metal tube 1 is formed into a flat shape, conductor wires 2 are twisted and formed around the outer periphery of the tube. Note that, in this case and similar to the above, a gap is provided in the metal tube. After that, the above-mentioned molded stranded wire is wound into a coil, for example, on a cylindrical bobbin, and the outer periphery is covered with a GFRP tube for reinforcement, or an insulating material is inserted, and a metal wire such as SUS is wrapped around the outer circumference for reinforcement. Wrap something around it and tie it up. At this time, both ends of the wire are brought out to the outside and the area around them is reinforced. Filling fluid 4 is poured into the metal tube from the other end by leaving one end of the stranded wire open or in a suction state. Once the metal tube is filled with fluid, one end is sealed and sealed, and pressure is applied from the open end. The tube 1 is filled with the fluid until it expands as shown in FIG. 2b.
After charging, the open end is also sealed, and the fluid is hardened or solidified by heating to a temperature of 300° C. or lower to obtain the superconductor of the present invention. In the present invention, austenitic steel tubes, titanium alloy tubes, copper alloy tubes, aluminum alloy tubes, etc. are used as the non-magnetic metal tubes, and the wall thickness of the tubes must be such that they can be easily expanded by press-fitting fluid. Although it is necessary, it differs depending on the material of the metal tube. Normally, the wall thickness is preferably about 0.1 to 1.0 mm. Further, the shape of the metal tube is not particularly limited as long as the cross section is other than a perfect circle, and any shape that can increase the cross-sectional area by pressurizing fluid into the tube may be used. For example, an oval
It may be rectangular or flat, or it may have a wedge-shaped inner surface or an uneven surface as shown in FIG. The fluid to be filled in the metal tube may be any pressure medium for adding internal pressure to the tube, such as a low melting point metal or silicone resin that has good thermal conductivity and a coefficient of linear expansion that is close to that of a superconducting wire and generates little gas. , epoxy resin, wax, etc. are preferred. In addition, the solidification or coagulation temperature of the fluid is 300℃.
The reason for this is that if the temperature is 300°C or higher, the superconducting properties will deteriorate at the temperature during solidification or solidification. Next, examples of the present invention will be described. Example A strand 2 having 24 Nb cores as shown in FIG.
The wire was compressed using a tag head to form the hollow portion 3 into a flat shape having a thickness of 0.2 mm in the thickness direction as shown in FIG. In this case, after winding, tighten the outside with SUS304 wire with an outer diameter of 0.8 mmφ, and then heat it to 700℃.
After performing diffusion heat treatment for 3 days, the wire was cooled to room temperature to obtain a rectangular shaped stranded wire. Thereafter, as shown in Figure 2a, while reducing the pressure at one end of the formed stranded wire of the coil, epoxy resin 4 was injected from the other end of the SUS tube to fill the inside of the tube with the epoxy resin, and then the pressure was reduced. One end of the tube was closed, and the tube 1 was further pressurized to 6 atmospheres to bulge out as shown in FIG. In addition, in order to compare with the coil of the present invention, the above molded stranded wire was impregnated with epoxy resin from the outside and heated at 150°C.
After curing for 4 hours, two solenoid coils were produced. An energization test was conducted to test the performance of the superconducting coil of the present invention and the superconducting coil of the comparative example thus obtained. The results are shown in Table 1.
【表】
ンプ
以上詳述した如く本発明によれば超電導線が強
固に固定され電磁力によつて線材が動揺してクエ
ンチをおこすことがない、又金属管内の中空部に
エポキシ樹脂等の絶縁性物質を充填することによ
りパルスマグネツトとして用いる場合安定性が著
しく向上する等顕著な効果を有する。[Table]
As detailed above, according to the present invention, the superconducting wire is firmly fixed, the wire does not sway due to electromagnetic force and does not quench, and the hollow part in the metal tube is filled with an insulating material such as epoxy resin. By doing so, when used as a pulsed magnet, it has remarkable effects such as a marked improvement in stability.
第1図は本発明超電導コイルにおいて、平角成
形撚線の工程を示すものであり、aは圧縮前の断
面図、bは圧縮後の断面図、第2図乃至第4図は
本発明において種々の形状を有する偏平状成形撚
線の膨出状態を示すものでありaは加圧前の偏平
管の断面図、bは加圧膨出後の偏平管断面図であ
る。
1……金属管、2……導体素線、3……空隙
部、4……充填材。
Figure 1 shows the process of rectangular forming stranded wire in the superconducting coil of the present invention, where a is a cross-sectional view before compression, b is a cross-sectional view after compression, and Figures 2 to 4 show various steps in the present invention. Fig. 3 shows a bulged state of a flat-formed stranded wire having the shape of , where a is a cross-sectional view of the flat tube before pressurization, and b is a cross-sectional view of the flat tube after pressurization and expansion. 1...Metal tube, 2...Conductor strand, 3...Gap, 4...Filling material.
Claims (1)
性パイプの外周に平角成形撚線を巻付けたものを
コイル巻きしてなる超電導コイルにおいて、該中
空部に300℃以下で硬化または凝固する流体を注
入し該パイプを膨脹せしめて該撚線を固定せしめ
たことを特徴とする超電導コイル。 2 薄肉非磁性パイプの厚さとして0.1〜1.0mmの
範囲のものを使用することを特徴とする特許請求
の範囲第1項記載の超電導コイル。 3 薄肉非磁性パイプの形状として楕円形、角形
偏平形からなることを特徴とする特許請求の範囲
第1項記載の超電導コイル。 4 薄肉非磁性パイプの材質としてオーステナイ
ト系ステンレス鋼管、チタン合金管、銅合金管、
アルミニウム合金管からなることを特徴とする特
許請求の範囲第1項記載の超電導コイル。 5 300℃以下で硬化或は凝固する流体として低
融点金属例えば鉛、ワツクス、シリコン樹脂、エ
ポキシ樹脂からなることを特徴とする特許請求の
範囲第1項記載の超電導コイル。[Claims] 1. A superconducting coil formed by winding rectangular shaped stranded wire around the outer periphery of a thin non-magnetic pipe whose hollow part has a shape other than a perfect circle, wherein the hollow part is heated to 300°C. A superconducting coil characterized in that the stranded wires are fixed by injecting a fluid that hardens or solidifies below to expand the pipe. 2. The superconducting coil according to claim 1, wherein the thin non-magnetic pipe has a thickness in the range of 0.1 to 1.0 mm. 3. The superconducting coil according to claim 1, wherein the thin non-magnetic pipe has an elliptical shape or a rectangular flat shape. 4 Materials for thin-walled non-magnetic pipes include austenitic stainless steel pipes, titanium alloy pipes, copper alloy pipes,
The superconducting coil according to claim 1, characterized in that it is made of an aluminum alloy tube. 5. The superconducting coil according to claim 1, characterized in that the fluid that hardens or solidifies at 300° C. or lower is made of a low melting point metal such as lead, wax, silicone resin, or epoxy resin.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5304384A JPS60196907A (en) | 1984-03-19 | 1984-03-19 | Superconductive coil |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP5304384A JPS60196907A (en) | 1984-03-19 | 1984-03-19 | Superconductive coil |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS60196907A JPS60196907A (en) | 1985-10-05 |
| JPH0467327B2 true JPH0467327B2 (en) | 1992-10-28 |
Family
ID=12931852
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP5304384A Granted JPS60196907A (en) | 1984-03-19 | 1984-03-19 | Superconductive coil |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS60196907A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP7347323B2 (en) * | 2020-05-18 | 2023-09-20 | トヨタ紡織株式会社 | Armature manufacturing method |
-
1984
- 1984-03-19 JP JP5304384A patent/JPS60196907A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS60196907A (en) | 1985-10-05 |
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