JP3302773B2 - electromagnet - Google Patents

electromagnet

Info

Publication number
JP3302773B2
JP3302773B2 JP09696793A JP9696793A JP3302773B2 JP 3302773 B2 JP3302773 B2 JP 3302773B2 JP 09696793 A JP09696793 A JP 09696793A JP 9696793 A JP9696793 A JP 9696793A JP 3302773 B2 JP3302773 B2 JP 3302773B2
Authority
JP
Japan
Prior art keywords
coil
tape
electromagnet
magnetic field
coils
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 - Fee Related
Application number
JP09696793A
Other languages
Japanese (ja)
Other versions
JPH06290939A (en
Inventor
一正 戸叶
浩明 熊倉
仁 北口
弘 前田
淳一 下山
成明 富田
克己 野村
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Hitachi Cable Ltd
National Institute for Materials Science
Original Assignee
Hitachi Cable Ltd
National Institute for Materials Science
Priority date (The priority date 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 date listed.)
Filing date
Publication date
Application filed by Hitachi Cable Ltd, National Institute for Materials Science filed Critical Hitachi Cable Ltd
Priority to JP09696793A priority Critical patent/JP3302773B2/en
Publication of JPH06290939A publication Critical patent/JPH06290939A/en
Application granted granted Critical
Publication of JP3302773B2 publication Critical patent/JP3302773B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

Classifications

    • YGENERAL 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
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E40/00Technologies for an efficient electrical power generation, transmission or distribution
    • Y02E40/60Superconducting electric elements or equipment; Power systems integrating superconducting elements or equipment

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  • Superconductors And Manufacturing Methods Therefor (AREA)

Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は、電磁石、特に酸化物超
電導体を用いた超電導電磁石に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electromagnet, and more particularly to a superconducting magnet using an oxide superconductor.

【0002】[0002]

【従来の技術】近年、液体窒素温度以上で超電導転移を
示す酸化物超電導体が次々と発見され、線材やテープ材
等への加工することにより様々な応用が試みられてい
る。酸化物超電導線材を利用した超電導電磁石は代表的
な応用例であり、従来の金属系線材に比べ高い転移温度
を持つことから液体窒素温度で作動する超電導コイル、
さらに20K以下の温度では従来材より高い臨界磁界を
示すことから強磁界発生用ハイブリッドコイルの内層コ
イルとしての応用が期待されている。
2. Description of the Related Art In recent years, oxide superconductors showing a superconducting transition at a temperature of liquid nitrogen or higher have been found one after another, and various applications have been attempted by processing them into wires, tapes and the like. A superconducting magnet using an oxide superconducting wire is a typical application example, and since it has a higher transition temperature than conventional metal-based wires, a superconducting coil that operates at liquid nitrogen temperature,
Further, since the critical magnetic field is higher than that of the conventional material at a temperature of 20 K or less, application of the hybrid coil for generating a strong magnetic field as an inner layer coil is expected.

【0003】最近、酸化物超電導線材による電磁石用コ
イルの作製が盛んに行われるようになっており、酸化物
超電導線材の製造方法としては、金属シース法、ドクタ
ーブレード法、ディップコート法等が知られている。と
ころが酸化物超電導体はセラミックスであるため非常に
脆くて破断しやすい。このため、酸化物超電導体を用い
たコイルでは、一般に、曲げ歪みを低減するため薄いテ
ープ状の形態をした線材が用いられることが多い。ま
た、さらに歪みを少なくするために、線材を巻回してコ
イル状に成形してから熱処理を行う、いわゆるワインド
・アンド・リアクト法により作製されている。
[0003] Recently, the production of coils for electromagnets using an oxide superconducting wire has been actively performed, and as a method for producing an oxide superconducting wire, a metal sheath method, a doctor blade method, a dip coating method and the like are known. Have been. However, since oxide superconductors are ceramics, they are very brittle and easily broken. For this reason, in a coil using an oxide superconductor, generally, a wire in the form of a thin tape is often used in order to reduce bending strain. In order to further reduce the distortion, the wire is wound and formed into a coil shape and then heat-treated, that is, a so-called wind and react method is used.

【0004】このとき用いられるコイルの形態として、
テープ状線材をロール状に巻固めた、いわゆるパンケー
キコイルがある。パンケーキコイルは成形が比較的容易
なため、脆い酸化物超電導線材を利用したコイルには適
した形態である。
The form of the coil used at this time is as follows:
There is a so-called pancake coil in which a tape-shaped wire is wound into a roll. Since the pancake coil is relatively easy to mold, it is a form suitable for a coil using a brittle oxide superconducting wire.

【0005】ところが、パンケーキコイルはコイル中心
軸方向の発生磁界分布が急峻、即ちコイル中心軸方向の
中心位置から離れるにしたがって発生磁界が急激に減少
する。このため広範囲の均一磁界を発生させるために
は、多数のパンケーキコイルをコイル中心軸方向にパン
ケーキコイル間の間隙ができるだけ小さくなるように積
層しなければならない。これはコイル積層・組み込み工
程を非常に困難なものにしている。
However, in a pancake coil, the generated magnetic field distribution in the direction of the coil central axis is steep, that is, the generated magnetic field decreases rapidly as the distance from the center position in the coil central axis direction increases. Therefore, in order to generate a uniform magnetic field over a wide range, a large number of pancake coils must be stacked in the direction of the coil center axis so that the gap between the pancake coils is as small as possible. This makes the coil lamination and assembly process very difficult.

【0006】特にドクターブレード法、ディップコート
法で作製した酸化物超電導線材では、製造工程上、テー
プの超電導層部分より幅の広い銀基体が必要であるた
め、コイル導体部分の実質間隙を5mm未満に小さくす
ることは非常に困難であり、パンケーキコイルを積層し
た場合コイル中心軸方向の発生磁界分布が不均一になっ
てしまうという問題があった。
Particularly, in the case of an oxide superconducting wire produced by a doctor blade method or a dip coating method, a silver substrate wider than the superconducting layer portion of the tape is required in the manufacturing process, so that the substantial gap of the coil conductor portion is less than 5 mm. It is very difficult to make the size smaller, and there is a problem that when the pancake coils are stacked, the generated magnetic field distribution in the direction of the coil center axis becomes non-uniform.

【0007】[0007]

【発明が解決しようとする課題】本発明は、テープ状形
態を持つ脆い線材で電磁石用に外径が小さいコイルを作
製する際、コイル軸方向の磁界分布が急峻でないコイ
ル、さらに、積層した場合にコイル間の中心軸方向の間
隙が広くても積層コイルの軸方向の磁界分布が均一であ
るようなコイルを提供するものである。
SUMMARY OF THE INVENTION The present invention relates to a method for manufacturing a coil having a small outer diameter for an electromagnet made of a brittle wire having a tape-like form and having a non-steep magnetic field distribution in the coil axis direction, Another object of the present invention is to provide a coil in which the axial magnetic field distribution of the laminated coil is uniform even if the gap in the central axis direction between the coils is wide.

【0008】[0008]

【課題を解決するための手段】本発明は、テープ状の導
体が巻回されてなるコイル構造であって、隣接したテー
プは少なくともその一部が重なっており、かつ、コイル
の軸方向にずれた構成をしているコイル構造を有する電
磁石を提供するものである。
According to the present invention, there is provided a coil structure in which a tape-shaped conductor is wound, wherein at least a part of adjacent tapes overlaps, and the tape is displaced in the axial direction of the coil. An object of the present invention is to provide an electromagnet having a coil structure configured as described above.

【0009】本発明の1実施態様を、図1にしたがって
説明する。図1において、テープ状の導体が、1つの軸
の周囲に巻回されている。このテープは、一周ごとに一
部分は重なっているが、軸方向にずれている。このずれ
は、中央から周囲に向かって常に一定方向である必要は
なく、図において一旦下方向にずれた後で、上方向にず
れていてもよい。また、部分的にずれのない巻回があっ
てもよい。
One embodiment of the present invention will be described with reference to FIG. In FIG. 1, a tape-shaped conductor is wound around one axis. This tape partially overlaps every circumference, but is shifted in the axial direction. This shift need not always be in a fixed direction from the center to the periphery, but may be shifted downward once in the drawing and then shifted upward. Further, there may be a winding in which there is no partial displacement.

【0010】本発明のコイル構造を軸方向に2個以上積
層する場合は、その効果がさらに増大するので好まし
い。例えば、図2に示すように、同じずれ構造を有する
コイルを積層する場合は、軸に垂直にみたときにコイル
の一部分が重なるように中心軸方向に積層することがで
きるので、特に好ましい。
When two or more coil structures of the present invention are laminated in the axial direction, the effect is further increased, which is preferable. For example, as shown in FIG. 2, it is particularly preferable to stack coils having the same misalignment structure, since the coils can be stacked in the central axis direction such that a part of the coils overlaps when viewed perpendicularly to the axis.

【0011】複数のコイルを積層する場合は、各コイル
の導電路を直列に接続するのが好ましい。
When a plurality of coils are stacked, it is preferable to connect the conductive paths of each coil in series.

【0012】このとき用いるテープ状導体は、テープ幅
に対して厚みのある導体では螺旋に巻いた効果が小さ
く、また螺旋形状に固定したときの強度も得にくい。こ
のためテープ状の導体の幅と厚みの比は100:1以上
であることが好ましい。
The tape-shaped conductor used at this time has a small effect of being wound spirally when the conductor has a thickness relative to the tape width, and it is difficult to obtain strength when fixed in a spiral shape. For this reason, the ratio of the width to the thickness of the tape-shaped conductor is preferably 100: 1 or more.

【0013】高効率で強磁界を発生する電磁石用コイル
のテープ状導体には超電導導体を用いることが望まし
い。特に臨界温度が高く、高い密度で電流が通電できる
テープ長手方向に結晶のc軸が配向したBi系酸化物超
電導体と銀の複合体が望ましい。
It is desirable to use a superconducting conductor for the tape-like conductor of the coil for the electromagnet which generates a strong magnetic field with high efficiency. In particular, a composite of a Bi-based oxide superconductor and silver in which the c-axis of the crystal is oriented in the longitudinal direction of the tape, which has a high critical temperature and allows current to flow at a high density, is desirable.

【0014】[0014]

【実施例】【Example】

実施例1 Bi2 Sr2 Ca1 Cu2y (yは酸素量)仮焼粉末
と有機溶媒、バインダーを含むスラリーに銀テープを送
り込むことにより、幅25mm、厚さ50μmの銀テー
プの両面にそれぞれ幅20mm、約50μmの酸化物層
をディップコートした。このテープをパンケーキコイル
状に巻き、脱媒した後、溶融凝固処理を行った。溶融凝
固処理過程は、約300℃/hで892℃まで昇温、5
分保持し、5℃/hで835℃まで徐冷後835℃で1
時間保持し、室温まで空冷した。酸化物超電導体からB
i成分の揮発を防ぐため、試料をBi−Al−O粉上に
載置し、準密閉容器中で溶融凝固処理を行った。
Example 1 A silver tape was fed into a slurry containing Bi 2 Sr 2 Ca 1 Cu 2 O y (y is the amount of oxygen), a calcined powder, an organic solvent and a binder, so that the silver tape was 25 mm wide and 50 μm thick. An oxide layer having a width of 20 mm and a thickness of about 50 μm was dip-coated. This tape was wound in a pancake coil shape, and after the solvent was removed, a melt-solidification treatment was performed. The melting and solidification process is performed by raising the temperature to 892 ° C. at about 300 ° C./h, 5
And slowly cooled to 835 ° C at 5 ° C / h,
It was kept for a while and cooled to room temperature. From oxide superconductor to B
In order to prevent volatilization of the i component, the sample was placed on Bi-Al-O powder and subjected to a melt-solidification treatment in a semi-closed container.

【0015】溶融凝固処理後、超電導層の厚みは15μ
mであり、この超電導層は酸化物超電導体の結晶のc軸
がテープ長手方向に垂直に配向していた。絶縁処理し、
巻締めた後、コイル中心部および外周部を引き出すこと
により図1に示すようなコイル形状にした。下部を樹脂
で固定、ワックス含浸後、上部を樹脂で固定した。この
一つのコイルのテープ長は6m、内径は16mm、外径
は45mmであった。このように作製したコイルの中心
軸上の発生磁界分布を図3に白丸で示す。
After the melt-solidification treatment, the superconducting layer has a thickness of 15 μm.
m, and in this superconducting layer, the c-axis of the crystal of the oxide superconductor was oriented perpendicular to the longitudinal direction of the tape. Insulated,
After the coiling, the coil was formed into a coil shape as shown in FIG. The lower part was fixed with resin, and after wax impregnation, the upper part was fixed with resin. The tape length of this one coil was 6 m, the inner diameter was 16 mm, and the outer diameter was 45 mm. The generated magnetic field distribution on the central axis of the coil thus manufactured is shown by white circles in FIG.

【0016】実施例2 実施例1で作製したコイルを図2に示すようにコイル大
径部とコイル小径部が重なるように5段積層させ一体化
し、各コイルの導電路が直列に接続したときの発生磁界
分布を図4に白丸で示す。
Example 2 As shown in FIG. 2, when the coil manufactured in Example 1 was laminated and integrated into five stages such that the large-diameter portion of the coil and the small-diameter portion of the coil overlapped, the conductive paths of each coil were connected in series. Are shown by white circles in FIG.

【0017】比較例 実施例1と同様にして作成した酸化物超電導体テープ
を、絶縁処理した後、巻締め、テープをずらすことなく
下部を樹脂で固定、ワックス含浸後、上部を樹脂で固定
し、パンケーキコイルを作製した。
COMPARATIVE EXAMPLE The oxide superconductor tape produced in the same manner as in Example 1 was subjected to an insulation treatment, then wound, fixed with a resin without displacing the tape, and impregnated with wax. Then, a pancake coil was produced.

【0018】このように作製したコイルの中心軸上の発
生磁界分布を図3に黒丸で示す。またこのように作製し
たコイルを5段積層させ一体化し、各コイルの導電路を
直列に接続したときの発生磁界分布を図4に黒丸で示
す。このときのコイル間の超電導層の間隔は5mmであ
った。
The generated magnetic field distribution on the central axis of the coil manufactured in this manner is shown by a black circle in FIG. In addition, the magnetic field distribution generated when the coils thus manufactured are stacked and integrated in five stages and the conductive paths of each coil are connected in series is shown by a black circle in FIG. At this time, the interval between the superconducting layers between the coils was 5 mm.

【0019】図3より、テープをずらして巻いたコイル
はテープをずらさないコイルに比べ中心軸方向に非常に
滑らかな発生磁界分布を示すことが分かる。また図4よ
り、積層した場合でも、テープをずらさないコイルでは
中心軸方向に磁界に分布が不均一になるのに対し、テー
プをずらして巻いたコイルは非常に均一な発生磁界分布
を示すことが分かる。
FIG. 3 shows that the coil wound with the tape shifted has a much smoother distribution of the generated magnetic field in the direction of the center axis than the coil without the tape shifted. From Fig. 4, it can be seen from Fig. 4 that even when the coils are stacked, the distribution of the magnetic field in the direction of the central axis is non-uniform for the coil that does not displace the tape, whereas the coil that is wound with the displaced tape exhibits a very uniform generated magnetic field distribution. I understand.

【0020】[0020]

【発明の効果】本発明の電磁石は、コイル中心軸方向の
発生磁界分布が非常に滑らかになる。このコイル構造を
積層して一体化する場合は、各単コイルの発生磁界分布
が非常に滑らかなため、積層軸方向に広い範囲の非常に
均一な発生磁界が得られる。
According to the electromagnet of the present invention, the generated magnetic field distribution in the direction of the center axis of the coil becomes very smooth. When the coil structures are stacked and integrated, the generated magnetic field distribution of each single coil is extremely smooth, so that a very uniform generated magnetic field can be obtained over a wide range in the stacking axis direction.

【図面の簡単な説明】[Brief description of the drawings]

【図1】本発明のコイルの1実施態様を示す外形図FIG. 1 is an external view showing one embodiment of a coil of the present invention.

【図2】本発明のコイルを5段に積層した場合の1実施
態様を示す断面図
FIG. 2 is a cross-sectional view showing one embodiment in which the coils of the present invention are stacked in five stages.

【図3】実施例1のコイルの中心軸における発生磁界分
布図
FIG. 3 is a distribution diagram of a generated magnetic field around a central axis of the coil according to the first embodiment.

【図4】実施例2のコイルの中心軸における発生磁界分
布図
FIG. 4 is a distribution diagram of a generated magnetic field at a central axis of the coil of the second embodiment.

フロントページの続き (72)発明者 北口 仁 茨城県つくば市千現1丁目2番1号 科 学技術庁金属材料技術研究所筑波支所内 (72)発明者 前田 弘 茨城県つくば市千現1丁目2番1号 科 学技術庁金属材料技術研究所筑波支所内 (72)発明者 下山 淳一 東京都墨田区押上2−12−7−321 (72)発明者 富田 成明 神奈川県横浜市神奈川区羽沢町1150番地 旭硝子株式会社 中央研究所内 (72)発明者 野村 克己 茨城県土浦市木田余町3550番地 日立電 線株式会社アドバンスリサーチセンタ内 (56)参考文献 実開 昭60−141104(JP,U) (58)調査した分野(Int.Cl.7,DB名) H01F 6/00 - 6/06 Continuing on the front page (72) Inventor Jin Kitaguchi 1-2-1 Sengen, Tsukuba, Ibaraki Pref., National Institute of Science and Technology Tsukuba Branch (72) Inventor Hiroshi Maeda 1-2-1, Sengen, Tsukuba, Ibaraki 1 Tsukuba Branch, National Institute for Metals Sciences, Science and Technology Agency (72) Inventor Junichi Shimoyama 2-12-7-321 Oshiage, Sumida-ku, Tokyo (72) Inventor Shigeaki Tomita 1150 Hazawacho, Kanagawa-ku, Yokohama-shi, Kanagawa Address Asahi Glass Co., Ltd. Central Research Laboratory (72) Inventor Katsumi Nomura 3550 Kida Yomachi, Tsuchiura City, Ibaraki Pref. Hitachi Cable Co., Ltd. Advanced Research Center (56) References Reference: Shokai Sho 60-141104 (JP, U) ) Surveyed field (Int.Cl. 7 , DB name) H01F 6/00-6/06

Claims (6)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】テープ状の導体が巻回されてなるコイル構
造であって、隣接したテープは少なくともその一部が重
なっており、かつ、コイルの軸方向にずれた構成をして
いるコイル構造を有する電磁石。
1. A coil structure in which a tape-shaped conductor is wound, wherein at least a part of adjacent tapes overlaps, and the coil structure is shifted in the axial direction of the coil. An electromagnet.
【請求項2】請求項1のコイル構造を軸方向に2個以上
積層した電磁石。
2. An electromagnet in which two or more coil structures according to claim 1 are laminated in the axial direction.
【請求項3】隣接するコイル構造の少なくとも一部分
が、軸に垂直方向にみて重なっている請求項2の電磁
石。
3. The electromagnet of claim 2, wherein at least a portion of adjacent coil structures overlap in a direction perpendicular to the axis.
【請求項4】各コイル構造が直列に接続されている請求
項2または請求項3の電磁石。
4. The electromagnet according to claim 2, wherein each coil structure is connected in series.
【請求項5】テープ状の導体の幅と厚みの比が100:
1以上である請求項1〜4いずれか1の電磁石。
5. A tape-shaped conductor having a ratio of width to thickness of 100:
The electromagnet according to any one of claims 1 to 4, wherein the number is one or more.
【請求項6】導体が、テープ長手方向に結晶のc軸が配
向したBi系酸化物超電導体と銀の複合体である請求項
1〜5いずれか1の電磁石。
6. The electromagnet according to claim 1, wherein the conductor is a composite of silver and a Bi-based oxide superconductor in which the c-axis of the crystal is oriented in the longitudinal direction of the tape.
JP09696793A 1993-03-31 1993-03-31 electromagnet Expired - Fee Related JP3302773B2 (en)

Priority Applications (1)

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JP09696793A JP3302773B2 (en) 1993-03-31 1993-03-31 electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP09696793A JP3302773B2 (en) 1993-03-31 1993-03-31 electromagnet

Publications (2)

Publication Number Publication Date
JPH06290939A JPH06290939A (en) 1994-10-18
JP3302773B2 true JP3302773B2 (en) 2002-07-15

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