JPH06260335A - High temperature superconducting magnet - Google Patents
High temperature superconducting magnetInfo
- Publication number
- JPH06260335A JPH06260335A JP7093593A JP7093593A JPH06260335A JP H06260335 A JPH06260335 A JP H06260335A JP 7093593 A JP7093593 A JP 7093593A JP 7093593 A JP7093593 A JP 7093593A JP H06260335 A JPH06260335 A JP H06260335A
- Authority
- JP
- Japan
- Prior art keywords
- coil
- magnetic field
- sectional area
- temperature superconducting
- cross
- 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.)
- Pending
Links
Landscapes
- Superconductors And Manufacturing Methods Therefor (AREA)
Abstract
(57)【要約】
【目的】 パンケーキ型高温超電導コイルにおいて、よ
り高い電流を流して高磁場を得る。
【構成】 パンケーキ状コイルを積層してなる高温超電
導マグネットにおいて、該マグネット軸方向両端部のコ
イルを構成する導体の断面積を、同中間部のコイルを構
成する導体の断面積に比べて大きくした。コイル軸方向
両端部のコイル導体断面積を増加させることで、ここに
より高い電流を流し、結果的にコイル全体の電流量を高
め、高磁場を得る。(57) [Abstract] [Purpose] In a pancake type high temperature superconducting coil, a higher magnetic field is applied to obtain a high magnetic field. [Composition] In a high-temperature superconducting magnet formed by stacking pancake-shaped coils, a cross-sectional area of a conductor forming a coil at both ends of the magnet in the axial direction is made larger than a cross-sectional area of a conductor forming a coil in the middle portion. did. By increasing the coil conductor cross-sectional area at both ends in the coil axial direction, a higher current is caused to flow therethrough, and as a result, the amount of current in the entire coil is increased and a high magnetic field is obtained.
Description
【0001】[0001]
【産業上の利用分野】本発明は、高温超電導線材を用い
たマグネット関するものである。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnet using a high temperature superconducting wire.
【0002】[0002]
【従来の技術】高温超電導マグネットのコイル巻回方法
としては、ソレノイド状に巻回するものと、図2に示す
ように、高温超電導テープを同心状に巻回したパンケー
キコイル1を銅ボビン2に装着して積層し、ジョイント
3により各コイル間を接続したものがある。2. Description of the Related Art As a coil winding method for a high temperature superconducting magnet, a coil is wound in a solenoid shape, and as shown in FIG. There is one in which the coils are connected to each other by a joint 3 and the coils are attached to each other.
【0003】[0003]
【発明が解決しようとする課題】ここで、パンケーキコ
イルにおけるコイル全体の磁束密度分布を考えた場合、
磁場のコイル軸方向成分は、図3に示すようにクリアボ
ア5の中心付近で最大となり(BM )、磁場のコイル径
方向成分BR はコイル軸方向両端部で最大となる。尚、
BO は中心磁場である。ところで、Bi系線材などでは
図4のグラフに示すように、臨界電流IC の異方性が大
きく、磁場のコイル径方向成分でIC が大きく低下す
る。従って、軸方向両端部のコイルで全体のIC は決ま
り、これを上げるにはコイルのターン数をかせぐため、
パンケーキコイルの積層枚数を増加するしかなく、多量
の線材が必要であるといった問題があった。Here, when considering the magnetic flux density distribution of the entire pancake coil,
Coil axis direction component of the magnetic field is maximum near the center of the Kuriaboa 5 as shown in FIG. 3 (B M), the coil radial component B R of the magnetic field is maximized in the coil axis direction end portions. still,
B O is the central magnetic field. By the way, as shown in the graph of FIG. 4, in a Bi-based wire or the like, the anisotropy of the critical current I C is large, and I C is greatly reduced by the coil radial component of the magnetic field. Therefore, the total I C is determined by the coils at both ends in the axial direction, and in order to raise this, the number of turns of the coil is earned.
There is a problem that a large number of wire rods are required because there is no choice but to increase the number of laminated pancake coils.
【0004】[0004]
【課題を解決するための手段】本発明は、上記の課題を
解決するためになされたものであって、その特徴は、パ
ンケーキ状コイルを積層してなる高温超電導マグネット
において、該マグネット軸方向両端部のコイルを構成す
る導体の断面積を、同中間部のコイルを構成する導体の
断面積に比べて大きくしたことにある。The present invention has been made to solve the above-mentioned problems, and is characterized by a high-temperature superconducting magnet formed by stacking pancake-shaped coils in the axial direction of the magnet. The cross-sectional area of the conductors forming the coils at both ends is made larger than the cross-sectional area of the conductors forming the coil in the middle portion.
【0005】[0005]
【作用】前述の従来の構成は、積層されたパンケーキコ
イルの導体がいずれも同じ断面積をもっていたため、コ
イル全体に流せる電流がコイル軸方向両端部のコイルの
IC で規制されていた。本発明マグネットは、コイル軸
方向両端部のコイル導体断面積を増加させることで、こ
こにより高い電流を流し、結果的にコイル全体の電流量
を高め、高磁場を得るものである。両端部の導体断面積
を増加させる手段として、例えばテープ線を2枚重ねた
バンドル線を用いることなどが考えられる。この場合、
両端部のコイルにかかる垂直磁場で線材1枚分のIC は
低下しても、2枚分の合計でIC は高くできるため、コ
イル全体に流せる電流量を大きくすることができる。
又、バンドル線の線材枚数は、径方向磁場の大きさに応
じて適宜選択すれば、線材量の節約を効率的に行える。In the above-mentioned conventional structure, since the conductors of the laminated pancake coils have the same cross-sectional area, the current that can flow through the entire coil is regulated by the coils I C at both ends in the coil axial direction. The magnet of the present invention increases the cross-sectional area of the coil conductor at both ends in the axial direction of the coil, thereby allowing a higher current to flow therethrough, consequently increasing the current amount of the entire coil and obtaining a high magnetic field. As a means for increasing the conductor cross-sectional area at both ends, for example, it is conceivable to use a bundle wire in which two tape wires are stacked. in this case,
Also the I C of the wire rod 1 sheet of a vertical magnetic field applied to the coil at both ends decreases, because I C can be increased by the sum of the two sheets, it is possible to increase the amount of current that can be flowed across the coil.
Further, if the number of wire rods of the bundled wire is appropriately selected according to the magnitude of the radial magnetic field, the amount of wire rods can be efficiently saved.
【0006】[0006]
【実施例】以下、本発明の実施例を比較例と併せて説明
する。図1はマグネットを示す概略図で、図示のよう
に、10枚のパンケーキコイル1を銅ボビン2に装着し
て積層したものである。各パンケーキコイルは、同図上
からNo1,No2…と数え、No10まである。この
ようなコイルを2段の冷却ステージを持つ冷凍機で冷却
し、次の条件にて通電を行い、発生できる磁場を測定し
た。尚、比較例として全て1枚の導体からなるパンケー
キコイルを20枚積層したものについても同様に通電を
行ってみた。EXAMPLES Examples of the present invention will be described below together with comparative examples. FIG. 1 is a schematic diagram showing a magnet. As shown, ten pancake coils 1 are mounted on a copper bobbin 2 and laminated. Each pancake coil is numbered from No. 1, No. 2 ... Such a coil was cooled by a refrigerator having two cooling stages, energized under the following conditions, and the generated magnetic field was measured. As a comparative example, the same electricity was applied to a stack of 20 pancake coils each made of a single conductor.
【0007】 (実施例条件) 導体:0.24×2.7mm幅 Bi系銀シーステープ電線 61多芯線 パンケーキコイル:積層枚数10枚 No1,2,9,10は二枚重ねのバンドル線使用。 No3〜8は1枚の導体 コイル寸法:内径40φ,外径100φ,高さ100m
m 通電電流:40A 発生磁場:1.2T(21Kにおいて)(Conditions for Example) Conductor: 0.24 × 2.7 mm width Bi-based silver sheath tape electric wire 61 Multi-core wire Pancake coil: 10 sheets laminated No. 1, 2, 9 and 10 use two bundled bundle wires. No3 to 8 are one conductor Coil dimensions: Inner diameter 40φ, Outer diameter 100φ, Height 100m
m Energizing current: 40A Magnetic field generated: 1.2T (at 21K)
【0008】 (比較例条件) 導体:0.24×2.7mm幅 Bi系銀シーステープ電線 61多芯線 パンケーキコイル:積層枚数20枚 全て1枚の導体 コイル寸法:内径40φ,外径100φ,高さ200m
m 通電電流:20A 発生磁場:1.2T(21Kにおいて)(Conditions for Comparative Example) Conductor: 0.24 × 2.7 mm width Bi-based silver sheath tape electric wire 61 Multi-core wire Pancake coil: 20 sheets of laminated layers All one conductor Coil dimensions: Inner diameter 40φ, Outer diameter 100φ, 200m height
m Energizing current: 20A Magnetic field generated: 1.2T (at 21K)
【0009】その結果、比較例は実施例に対してコイル
体積は2倍で、線材使用量も2倍あり、本発明実施例は
同じ磁場を発生するのに線材使用量を少なくできること
が確認された。As a result, the coil volume of the comparative example is twice as large as that of the embodiment, and the amount of wire used is also twice that of the embodiment. It is confirmed that the embodiment of the present invention can reduce the amount of wire used for generating the same magnetic field. It was
【0010】尚、前記実施例では、2枚のバンドル線を
用いているが、コイル軸方向両端部の導体断面積を増大
させる構造として、中間部のコイルに用いるテープ線材
と厚さが同じで、幅が2倍のものを両端部に用いてもよ
い。In the above embodiment, two bundle wires are used. However, as a structure for increasing the conductor cross-sectional area at both ends in the axial direction of the coil, the thickness is the same as that of the tape wire used for the coil in the middle part. , The width may be doubled at both ends.
【0011】[0011]
【発明の効果】以上説明したように、本発明超電導マグ
ネットによれば、コンパクトでありながら高い磁場を発
生することができる。従って、リニアモータ,電気自動
車等の移動型SC機器や高磁界(15T以上)を要求さ
れるマグネットなどに有効利用することが期待される。As described above, according to the superconducting magnet of the present invention, it is possible to generate a high magnetic field while being compact. Therefore, it is expected to be effectively used for mobile SC devices such as linear motors and electric vehicles and magnets that require a high magnetic field (15T or more).
【図1】超電導マグネットの概略図である。FIG. 1 is a schematic view of a superconducting magnet.
【図2】従来のパンケーキ型マグネットを示す概略図で
ある。FIG. 2 is a schematic view showing a conventional pancake magnet.
【図3】パンケーキ型コイルに発生する磁束密度分布の
説明図である。FIG. 3 is an explanatory diagram of a magnetic flux density distribution generated in a pancake coil.
【図4】超電導電流密度と印加磁場の関係を示すグラフ
である。FIG. 4 is a graph showing the relationship between superconducting current density and applied magnetic field.
1 パンケーキコイル 2 銅ボビン 3 ジョイント 4 巻き枠 5 クリアボア 1 Pancake coil 2 Copper bobbin 3 Joint 4 Reel 5 Clear bore
Claims (1)
超電導マグネットにおいて、該マグネット軸方向両端部
のコイルを構成する導体の断面積を、同中間部のコイル
を構成する導体の断面積に比べて大きくしたことを特徴
とする高温超電導マグネット。1. In a high-temperature superconducting magnet formed by stacking pancake-shaped coils, a cross-sectional area of a conductor forming a coil at both ends of the magnet in an axial direction is compared with a cross-sectional area of a conductor forming a coil at an intermediate portion of the magnet. High temperature superconducting magnet characterized by being made larger.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7093593A JPH06260335A (en) | 1993-03-05 | 1993-03-05 | High temperature superconducting magnet |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7093593A JPH06260335A (en) | 1993-03-05 | 1993-03-05 | High temperature superconducting magnet |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH06260335A true JPH06260335A (en) | 1994-09-16 |
Family
ID=13445868
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP7093593A Pending JPH06260335A (en) | 1993-03-05 | 1993-03-05 | High temperature superconducting magnet |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH06260335A (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006313923A (en) * | 2006-06-26 | 2006-11-16 | Toshiba Corp | High temperature superconducting coil and high temperature superconducting magnet using the same |
KR100720057B1 (en) * | 2005-07-06 | 2007-05-18 | 학교법인 한국산업기술대학 | Superconducting Magnet for Permanent Current and Manufacturing Method |
JP2014216411A (en) * | 2013-04-24 | 2014-11-17 | 株式会社フジクラ | Oxide superconducting coil and superconducting apparatus including the same |
CN108766709A (en) * | 2018-06-13 | 2018-11-06 | 苏州新材料研究所有限公司 | High-temperature superconductor inside coil and preparation method thereof |
-
1993
- 1993-03-05 JP JP7093593A patent/JPH06260335A/en active Pending
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
KR100720057B1 (en) * | 2005-07-06 | 2007-05-18 | 학교법인 한국산업기술대학 | Superconducting Magnet for Permanent Current and Manufacturing Method |
JP2006313923A (en) * | 2006-06-26 | 2006-11-16 | Toshiba Corp | High temperature superconducting coil and high temperature superconducting magnet using the same |
JP4719090B2 (en) * | 2006-06-26 | 2011-07-06 | 株式会社東芝 | High temperature superconducting coil and high temperature superconducting magnet using the same |
JP2014216411A (en) * | 2013-04-24 | 2014-11-17 | 株式会社フジクラ | Oxide superconducting coil and superconducting apparatus including the same |
CN108766709A (en) * | 2018-06-13 | 2018-11-06 | 苏州新材料研究所有限公司 | High-temperature superconductor inside coil and preparation method thereof |
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