JPH0464165B2 - - Google Patents
Info
- Publication number
- JPH0464165B2 JPH0464165B2 JP58182749A JP18274983A JPH0464165B2 JP H0464165 B2 JPH0464165 B2 JP H0464165B2 JP 58182749 A JP58182749 A JP 58182749A JP 18274983 A JP18274983 A JP 18274983A JP H0464165 B2 JPH0464165 B2 JP H0464165B2
- Authority
- JP
- Japan
- Prior art keywords
- spacer
- superconducting
- conductor
- turn
- inter
- 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
- 125000006850 spacer group Chemical group 0.000 claims description 58
- 239000004020 conductor Substances 0.000 claims description 39
- 238000004804 winding Methods 0.000 claims description 15
- 229910052734 helium Inorganic materials 0.000 claims description 6
- 239000001307 helium Substances 0.000 claims description 6
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 claims description 6
- 239000002826 coolant Substances 0.000 claims description 4
- 239000007788 liquid Substances 0.000 claims description 4
- 239000002887 superconductor Substances 0.000 claims 1
- 238000001816 cooling Methods 0.000 description 5
- 238000005452 bending Methods 0.000 description 4
- 238000009413 insulation Methods 0.000 description 4
- 230000004927 fusion Effects 0.000 description 3
- 238000010586 diagram Methods 0.000 description 2
- 239000010410 layer Substances 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 230000002093 peripheral effect Effects 0.000 description 2
- 238000003825 pressing Methods 0.000 description 2
- 238000010008 shearing Methods 0.000 description 2
- 230000000994 depressogenic effect Effects 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000010292 electrical insulation Methods 0.000 description 1
- 238000004146 energy storage Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 230000001771 impaired effect Effects 0.000 description 1
- 239000011229 interlayer Substances 0.000 description 1
- 238000010030 laminating Methods 0.000 description 1
- 238000005339 levitation Methods 0.000 description 1
- 239000003507 refrigerant Substances 0.000 description 1
Classifications
-
- 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)
- Coils Of Transformers For General Uses (AREA)
Description
【発明の詳細な説明】
〔発明の技術分野〕
本発明は核融合装置等に使用する超電導磁石に
係り、特に超電導磁石本体を冷却するための流路
を形成するスペーサの改良に関するものである。DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a superconducting magnet used in a nuclear fusion device or the like, and particularly relates to an improvement in a spacer that forms a flow path for cooling a superconducting magnet body.
近年、超電導現象を利用した装置は磁石浮上列
車、エネルギー貯蔵、回転電機、核融合装置等広
い範囲にわたつて採用されつつある。特に核融合
装置は実用化に向けて装置の大型化が著しく、こ
れに使用される大型超電導磁石の開発が必要不可
欠となつている。
In recent years, devices that utilize superconductivity have been widely adopted, such as magnetic levitation trains, energy storage, rotating electric machines, and nuclear fusion devices. In particular, nuclear fusion devices are significantly increasing in size as they move toward practical use, making it essential to develop large superconducting magnets for use in these devices.
一般に超電導状態を作り出すためには、超電導
線材で成形された磁石本体を液体ヘリウムまたは
超臨介ヘリウム等の冷媒によつて極低温に冷却す
る必要がある。このため、超電導磁石本体は通常
真空断熱された容器の中に収納されている。 Generally, in order to create a superconducting state, it is necessary to cool a magnet body made of superconducting wire to an extremely low temperature using a coolant such as liquid helium or superconducting helium. For this reason, the superconducting magnet body is usually housed in a vacuum-insulated container.
ところで従来の超電導磁石としては、超電導導
体を所定回数巻回するとともにその各導体間に複
数個のターン間スペーサを適宜の間隔を存して挿
入して単位コイルを成形し、この単位コイルを複
数個軸方向に積層するとともにその各積層間に複
数個の層間スペーサを適宜の間隔を存して介挿し
た超電導磁石本体を構成し、この超電導磁石本体
を真空断熱された極低温容器内に液体ヘリウム等
の冷媒とともに収納するようにしたものがある。 By the way, conventional superconducting magnets are made by winding a superconducting conductor a predetermined number of times and inserting a plurality of inter-turn spacers at appropriate intervals between each conductor to form a unit coil. A superconducting magnet body is constructed by laminating the individual layers in the axial direction and inserting a plurality of interlayer spacers at appropriate intervals between the laminated layers, and the superconducting magnet body is placed in a cryogenic container with vacuum insulation. Some are designed to be stored together with a refrigerant such as helium.
第1図乃至第3図はかかる超電導磁石におい
て、その基本構成要素となる単位コイルの成形過
程の状態をそれぞれ示すものである。すなわち、
第1図乃至第3図に示すように巻枠1の外周面に
複数個のターン間スペーサ2を適宜の間隔を存し
て配設し、その上に帯状の超電導導体3を巻枠1
を図示矢印方向に回転させて1ターン巻き付け、
次いで超電導導体3を引張つた状態で前述と同様
のターン間スペーサ2を順次挿入しながら巻枠1
を回転させることにより各導体間にターン間スペ
ーサを挿入した単位コイル4を成形している。 FIGS. 1 to 3 each show the state of the forming process of a unit coil, which is a basic component of such a superconducting magnet. That is,
As shown in FIGS. 1 to 3, a plurality of inter-turn spacers 2 are arranged at appropriate intervals on the outer peripheral surface of the winding frame 1, and a strip-shaped superconducting conductor 3 is placed on the outer peripheral surface of the winding frame 1.
Rotate in the direction of the arrow shown and wrap it around for one turn.
Next, with the superconducting conductor 3 in tension, the winding frame 1 is inserted while sequentially inserting the inter-turn spacers 2 similar to those described above.
By rotating the unit coil 4, a unit coil 4 with an inter-turn spacer inserted between each conductor is formed.
この単位コイル4の各導体間に介在するターン
間スペーサ2は各導体間の電気絶縁、電磁力に対
する支持および超電導導体3を冷却する液体ヘリ
ウム等の冷媒流路を形成するためのものである。 The inter-turn spacer 2 interposed between each conductor of the unit coil 4 is used to provide electrical insulation between each conductor, support against electromagnetic force, and form a coolant flow path for liquid helium or the like to cool the superconducting conductor 3.
したがつて、電磁力に対する支持特性を向上さ
せるにはスペーサ率(超電導導体3のターン方向
表面積に対するターン間スペーサ2のターン方向
表面積の割合)を上げればよいが、超電導磁石を
安定に運転するためには前記スペーサ率を下げ冷
却流路を充分にとる必要がある。そこで、通常は
このスペーサ率を50%以下になるようにしてい
る。 Therefore, in order to improve the supporting characteristics against electromagnetic force, it is sufficient to increase the spacer ratio (the ratio of the surface area in the turn direction of the inter-turn spacer 2 to the surface area in the turn direction of the superconducting conductor 3), but in order to operate the superconducting magnet stably, To achieve this, it is necessary to reduce the spacer ratio and provide sufficient cooling channels. Therefore, this spacer ratio is usually set to 50% or less.
しかしこのように単位コイル4の各超電導導体
3間にスペーサ率が50%以下になるようにターン
間スペーサ2を介在させる場合、第2図からも明
らかなようにターン間スペーサ2の導体巻回方向
の長さに対してスペーサ間隔が大きく、しかも各
ターン間におけるスペーサの配置位置が径方に同
一線上に並ばないため、超電導導体3の巻き付け
時にそのターン間に挿入されたターン間スペーサ
2が強く押圧されるとその内側の超電導導体3に
対して曲げ応力、剪断応力を与える結果となる。
このため、超電導導体3の絶縁特性が劣化するば
かりでなく、極端な場合には第3図に点線にて示
すように内側の超電導導体3がスペーサ間に落ち
込み、ターン間絶縁不良を生ずる等の欠点があつ
た。
However, when the inter-turn spacer 2 is interposed between each superconducting conductor 3 of the unit coil 4 so that the spacer ratio is 50% or less, as is clear from Fig. 2, the conductor winding of the inter-turn spacer 2 is Since the spacer interval is large relative to the length in the direction, and the spacer positions between each turn are not aligned in the same line in the radial direction, the inter-turn spacer 2 inserted between the turns when winding the superconducting conductor 3 is If it is strongly pressed, bending stress and shearing stress will be applied to the superconducting conductor 3 inside it.
For this reason, not only will the insulation properties of the superconducting conductor 3 deteriorate, but in extreme cases, the inner superconducting conductor 3 will fall between the spacers as shown by the dotted line in Figure 3, resulting in poor inter-turn insulation. There were flaws.
本発明は上記のような欠点を除去すべくなされ
たもので、その目的は単位コイルのスペーサ率を
下げても超電導導体間に挿入されるターン間スペ
ーサの押圧力による超電導導体の曲げ応力、剪断
応力の発生をなくすことができる堅牢かつ特性に
優れた超電導磁石を提供するにある。
The present invention has been made to eliminate the above-mentioned drawbacks, and its purpose is to reduce the bending stress and shear of the superconducting conductor due to the pressing force of the inter-turn spacer inserted between the superconducting conductors even if the spacer ratio of the unit coil is reduced. It is an object of the present invention to provide a superconducting magnet that is robust and has excellent characteristics and can eliminate the generation of stress.
本発明はかかる目的を達成するため、超電導導
体を同心円状に所定回数巻回し且つ各導体間に複
数個のターン間スペーサを適宜の間隔を存して挿
入してなる単位コイルを基本構成要素とする超電
導磁石本体を真空断熱された容器内に液体ヘリウ
ム等の冷媒とともに収納した超電導磁石におい
て、前記単位コイルを構成する各超電導導体間に
挿入されるターン間スペーサの導体巻回方向長さ
をスペーサ間隔より長くし且つそのスペーサの一
部に切り欠き部を設けてスペーサ率を小さくした
ことを特徴としている。
In order to achieve this object, the present invention uses a unit coil as a basic component, which is formed by winding a superconducting conductor concentrically a predetermined number of times and inserting a plurality of inter-turn spacers at appropriate intervals between each conductor. In a superconducting magnet in which a superconducting magnet main body is housed together with a coolant such as liquid helium in a vacuum-insulated container, the length in the conductor winding direction of the inter-turn spacer inserted between each superconducting conductor constituting the unit coil is defined as the spacer. It is characterized by being longer than the spacer and having a notch in a part of the spacer to reduce the spacer ratio.
以下本発明の一実施例を図面を参照して説明す
る。
An embodiment of the present invention will be described below with reference to the drawings.
第4図は本発明による超電導磁石の基本構成要
素となる単位コイルの部分的な構成例を示すもの
で、その成形手段は第1図の場合と同様なのでそ
の説明を省略し、ここでは異なる点について述べ
る。すなわち、本実施例では第4図a,bに示す
ように超電導導体3が同心円状に所定回数巻回さ
れ且つその各導体間に挿入される複数個のターン
間スペーサ21として、導体巻回方向のスペーサ
長さlがスペーサ間隔pより大きく(l>p)
し、且つその一部を切り欠いてコの字形状のスペ
ーサとしたものである。 FIG. 4 shows an example of a partial configuration of a unit coil which is a basic component of the superconducting magnet according to the present invention.The forming means thereof are the same as in the case of FIG. Let's talk about. That is, in this embodiment, as shown in FIGS. 4a and 4b, a superconducting conductor 3 is wound concentrically a predetermined number of times, and a plurality of inter-turn spacers 21 are inserted between each of the conductors in the direction of conductor winding. The spacer length l is larger than the spacer interval p (l>p)
A part of the spacer is cut out to form a U-shaped spacer.
したがつて、このようなスペーサ長さを有する
コの字形状のターン間スペーサ21を図示する如
く超電導導体3を巻回しながらスペーサ間隔pを
存して挿入していくことにより、内側の超電導導
体3間に挿入されたターン間スペーサ21と外側
の超電導導体3間に挿入されたターン間21とは
その導体巻回方向両端部がラツプするような位置
関係となる。このため、超電導導体3の巻き付け
時に外側のターン間スペーサ21が押圧されても
その内側の超電導導体3に曲げ応力や剪断応力を
生じるようなことがなく、この超電導導体3がそ
の下側のスペーサ間に落ち込むこともないので、
ターン間の絶縁特性が損なわれることがない。ま
た、単にスペーサ長さlをスペーサ間隔pよりも
大きく(l>p)したのではスペーサ率が50%以
上となり、冷却効率の悪いものになつてしまう
が、本実施例では矩形状のスペーサの一部を切り
欠いてコの字形としスペーサ率が50%以下になる
ようにしているので、冷却流路を充分確保するこ
とができ、冷却効率を向上させることができる。 Therefore, by inserting the U-shaped inter-turn spacer 21 having such a spacer length while winding the superconducting conductor 3 with the spacer interval p as shown in the figure, the inner superconducting conductor The inter-turn spacer 21 inserted between the outer superconducting conductors 3 and the inter-turn spacer 21 inserted between the outer superconducting conductors 3 have a positional relationship such that both ends in the winding direction of the conductor overlap. Therefore, even if the outer inter-turn spacer 21 is pressed when the superconducting conductor 3 is wound, bending stress or shearing stress will not be generated in the inner superconducting conductor 3, and this superconducting conductor 3 will be able to move around the lower spacer. I don't get depressed in between,
The insulation properties between turns are not impaired. Furthermore, if the spacer length l is simply made larger than the spacer interval p (l>p), the spacer ratio will be more than 50%, resulting in poor cooling efficiency, but in this example, rectangular spacers are used. Since a portion is cut out to form a U-shape so that the spacer ratio is 50% or less, a sufficient cooling flow path can be secured and cooling efficiency can be improved.
上記実施例ではターン間スペーサ21としてコ
の字形のものを用いる場合について述べたが、第
5図a〜hに示すように矩形状のスペーサの一部
を切り欠いて図示形状のターン間スペーサとして
もよいことは勿論である。要するにスペーサの導
体巻回方向の長さlがスペーサ間隔pの長さより
も大きく、しかもその一部を切り欠いてスペーサ
率が50%以下にできればその形状は如何なるもの
であつてもよい。 In the above embodiment, a U-shaped spacer 21 is used as the inter-turn spacer 21, but as shown in FIG. Of course, this is a good thing. In short, any shape may be used as long as the length l of the spacer in the conductor winding direction is greater than the length of the spacer interval p, and the spacer ratio can be reduced to 50% or less by cutting out a part of the spacer.
以上述べたように本発明によれば、単位コイル
のスペーサ率を下げても超電導導体間に挿入され
るターン間スペーサの押圧力による超電導導体の
曲げ応力、剪断応力の発生をなくすことができる
堅牢かつ特性に優れた超電導磁石が提供できる。
As described above, according to the present invention, even if the spacer ratio of the unit coil is lowered, the bending stress and shear stress of the superconducting conductor due to the pressing force of the inter-turn spacer inserted between the superconducting conductors can be eliminated. Moreover, a superconducting magnet with excellent characteristics can be provided.
第1図乃至第3図は従来の超電導磁石の基本構
成要素となる単位コイルの構成およびその成形過
程の説明図、第4図a,bは本発明の一実施例に
おける単位コイルの一部を示す構成説明図、第5
図a〜hは本発明で用いられるターン間スペーサ
のそれぞれ異なる形状例を示す平面図である。
1……巻枠、21……ターン間スペーサ、3…
…超電導導体、4……単位コイル。
FIGS. 1 to 3 are explanatory diagrams of the structure and forming process of a unit coil, which is a basic component of a conventional superconducting magnet, and FIGS. 4a and 4b show a part of a unit coil in an embodiment of the present invention. Configuration explanatory diagram shown, No. 5
Figures a to h are plan views showing examples of different shapes of inter-turn spacers used in the present invention. 1... winding frame, 21... spacer between turns, 3...
...Superconducting conductor, 4...Unit coil.
Claims (1)
導体間に複数個のターン間スペーサを適宜の間隔
を存して挿入してなる単位コイルを基本構成要素
として超電導磁石本体を構成し、この超電導磁石
本体を真空断熱された容器内に液体ヘリウム等の
冷媒とともに収納した超電導磁石において、前記
単位コイルを構成する超電導導体に挿入されるタ
ーン間スペーサの導体巻回方向長さをスペーサ間
隔より長くし且つそのスペーサの一部に切り欠き
部を設けてスペーサ率を小さくしたことを特徴と
する超電導磁石。1. A superconducting magnet body is constructed with a unit coil as a basic component, which is formed by winding a superconductor concentrically a predetermined number of times and inserting a plurality of inter-turn spacers at appropriate intervals between each conductor. In a superconducting magnet whose magnet body is housed in a vacuum-insulated container together with a coolant such as liquid helium, the length of the inter-turn spacer inserted into the superconducting conductor constituting the unit coil in the conductor winding direction is longer than the spacer interval. A superconducting magnet characterized in that a notch is provided in a part of the spacer to reduce the spacer ratio.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58182749A JPS6074605A (en) | 1983-09-30 | 1983-09-30 | Superconducting magnet |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58182749A JPS6074605A (en) | 1983-09-30 | 1983-09-30 | Superconducting magnet |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6074605A JPS6074605A (en) | 1985-04-26 |
| JPH0464165B2 true JPH0464165B2 (en) | 1992-10-14 |
Family
ID=16123760
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58182749A Granted JPS6074605A (en) | 1983-09-30 | 1983-09-30 | Superconducting magnet |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS6074605A (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE102016206573A1 (en) * | 2016-04-19 | 2017-10-19 | Siemens Aktiengesellschaft | Electric coil winding |
-
1983
- 1983-09-30 JP JP58182749A patent/JPS6074605A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS6074605A (en) | 1985-04-26 |
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