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JPS60937B2 - superconducting coil - Google Patents
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JPS60937B2 - superconducting coil - Google Patents

superconducting coil

Info

Publication number
JPS60937B2
JPS60937B2 JP52078890A JP7889077A JPS60937B2 JP S60937 B2 JPS60937 B2 JP S60937B2 JP 52078890 A JP52078890 A JP 52078890A JP 7889077 A JP7889077 A JP 7889077A JP S60937 B2 JPS60937 B2 JP S60937B2
Authority
JP
Japan
Prior art keywords
superconducting
coil
holding member
wires
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
Application number
JP52078890A
Other languages
Japanese (ja)
Other versions
JPS5413293A (en
Inventor
隆 佐藤
泰秀 服部
雅民 岩本
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
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 Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP52078890A priority Critical patent/JPS60937B2/en
Publication of JPS5413293A publication Critical patent/JPS5413293A/en
Publication of JPS60937B2 publication Critical patent/JPS60937B2/en
Expired legal-status Critical Current

Links

Landscapes

  • Containers, Films, And Cooling For Superconductive Devices (AREA)
  • Coils Of Transformers For General Uses (AREA)
  • Transformer Cooling (AREA)

Description

【発明の詳細な説明】 この発明は超電導コイルに関するもので、特にコイル保
持部材に設けられた溝に、断面サイズの小さな超電導素
線を、多数本東にした超電導素線群を巻回して成る超電
導ディスクタイプの超電導コイルに係るものである。
[Detailed Description of the Invention] This invention relates to a superconducting coil, and in particular, it is made by winding a group of superconducting strands, each consisting of a large number of superconducting strands with a small cross-sectional size, in a groove provided in a coil holding member. This relates to a superconducting disk type superconducting coil.

一般に高磁界を発生する装置として、超電導コイルが多
く使用されているが、超電導コイルは通常の電磁石と異
なり、極低温、主として液体ヘリウム温度にまで冷却さ
れる必要があり、さらに、メガ・ジュール以上、特に核
融合装置に使用されるとみられているギガ・ジュール以
上の磁界エネルギーを有する大型超電導コイルにおいて
は、そのコイルによって発生される巨大な電磁力に耐え
る支持構造をいかに構成するかが重要な問題になつてい
る。
Generally, superconducting coils are often used as devices that generate high magnetic fields, but unlike ordinary electromagnets, superconducting coils need to be cooled to extremely low temperatures, mainly liquid helium temperatures, and furthermore, superconducting coils have to be cooled to extremely low temperatures, mainly to the temperature of liquid helium. In particular, for large superconducting coils with magnetic field energies of gigajoules or more that are expected to be used in nuclear fusion devices, it is important to construct a support structure that can withstand the enormous electromagnetic force generated by the coils. It's becoming a problem.

そこで、第1図に示すような構造の超電導コイルが、先
行技術として考えられた。
Therefore, a superconducting coil having a structure as shown in FIG. 1 was considered as a prior art.

この超電導コイルは、金属または絶縁物より成る板状の
コイル保持部材1に、多数のコイル溝2が設けられてお
り、このコイル溝2には超電導線3が収納される。なお
コイル保持部材1のコイル溝2間には超電導線3が次の
ターンに巻上るための斜めに連なる立上り溝(図示せず
)が設けられている。上記コイル保持部材1に設けられ
たコイル溝2に、所定のターン数だけ超電導線3を組み
込み、1個の超電導ディスク4が形成される。そして、
この超電導ディスク4複数個をボルト5およびナット6
で緒付けて組立て、超電導コイル7全体が構成される。
上記コイル構造では超電導線3は第2図に示すような配
置で構成される。
In this superconducting coil, a plate-shaped coil holding member 1 made of metal or an insulator is provided with a large number of coil grooves 2, and superconducting wires 3 are housed in the coil grooves 2. Incidentally, between the coil grooves 2 of the coil holding member 1, there are provided diagonally continuous rising grooves (not shown) for winding the superconducting wire 3 into the next turn. A predetermined number of superconducting wires 3 are assembled into the coil grooves 2 provided in the coil holding member 1 to form one superconducting disk 4. and,
A plurality of these superconducting disks 4 are attached to bolts 5 and nuts 6.
The superconducting coil 7 is assembled as a whole.
In the coil structure described above, the superconducting wire 3 is arranged as shown in FIG.

すなわち、第2図は超電導ディスク4の部分的な拡大斜
視図で、超電導線3は、コイル保持部材1に設けられた
コイル溝2内に、間隔部材3を介して固定され全周冷却
が可能なようになっている。間隔部材3は、コイル保持
部材1が金属の場合には絶縁物または表面に絶縁処理を
施こした金属であり、コイル保持部材1が絶縁物の場合
には絶縁物でも金属でもよい。超電導コイルを以上の様
なディスク構造にすることにより、超電導コイルが発生
する巨大な電磁力にも十分耐え得ることが可能となった
。しかし、超電導コイルの大型化に伴なし、巻回される
超電導線3の断面サイズが大きくなると、第1図及び第
2図に示した全周冷却をもってしても「安定化電流をあ
まり高くとることはできない。大型超電導コイルにおい
ては、コイル運転電流1は安定化電流lr以下に設定す
るという設定方針が通常とられている。
That is, FIG. 2 is a partially enlarged perspective view of the superconducting disk 4, in which the superconducting wire 3 is fixed in the coil groove 2 provided in the coil holding member 1 via the spacing member 3, and can be cooled all around. It looks like this. When the coil holding member 1 is made of metal, the spacing member 3 may be an insulating material or a metal whose surface has been subjected to insulation treatment, and when the coil holding member 1 is made of an insulating material, it may be an insulating material or a metal. By making the superconducting coil have the disk structure described above, it has become possible to sufficiently withstand the huge electromagnetic force generated by the superconducting coil. However, as superconducting coils become larger, the cross-sectional size of the wound superconducting wire 3 becomes larger. This is not possible. In large superconducting coils, a setting policy is usually adopted in which the coil operating current 1 is set to be equal to or less than the stabilizing current lr.

したがってlrを高めるほどコイル電流1を大きくする
ことができ、コイル電流1を大きくするとコイル電流密
度も高くなり、超電導コイルをコンパクト化することが
でき、クラィオスタットのコンパクト化、さらに冷却シ
ステムのコンパクト化にもつながることになる。この安
定化電流lr■は、超電導線の冷却べリメ−夕S(cm
)に依存し、それらにはlr戊ノ亨 【1} なる関係がある。
Therefore, the coil current 1 can be increased as lr is increased, and when the coil current 1 is increased, the coil current density also increases, making it possible to make the superconducting coil more compact, making the cryostat more compact, and further making the cooling system more compact. will also be connected. This stabilizing current lr■ is the cooling beam meter S (cm
), and there is a relationship between them as follows.

この発明は以上の点に鑑み巨大な電磁力にも十分耐え「
しかも冷却べリメータを増大することにより安定化電
流lrを増加せしめ、よりコンパクトな超電導コイルを
提供することを目的とするものである。
In view of the above points, this invention can withstand huge electromagnetic force.
Moreover, by increasing the number of cooling verimeters, the stabilizing current lr is increased, and the purpose is to provide a more compact superconducting coil.

以下、この発明の一実施例を図について説明する。An embodiment of the present invention will be described below with reference to the drawings.

第3図において、9a,9b,9c,9d’9e,……
は超電導秦線、9はこれら超電導素線を多数本東にした
超電導素線群であり、4は「 これら超電導素線群9を
前記コイル保持部材1のコイル溝2内に巻回して成る超
電導ディスクである。また、1川まコイル溝2の関口部
を閉塞する押え部材であり、これは超電導素線群9をコ
イル溝2内に保持する役目をすると同時に、このコイル
溝2内の各超電導素線9a,9b・・…・間は冷却媒体
が流通する冷却媒体流通路ともなるため、コイル保持材
1と押え部材10との間には気密が保たれなけれがなら
ない。巻回する超電導線を上記のような構造することに
より超電導線が受ける冷却面積を著しく増大することが
でき、第m式の関係により安定化電流lrを増加するこ
とが可能となる。
In FIG. 3, 9a, 9b, 9c, 9d'9e,...
is a superconducting wire, 9 is a superconducting strand group made up of a large number of these superconducting strands, and 4 is a superconducting wire group formed by winding these superconducting strands 9 into the coil groove 2 of the coil holding member 1. It is also a holding member that closes the entrance of the coil groove 2, and this serves to hold the superconducting wire group 9 in the coil groove 2, and at the same time Since the space between the superconducting wires 9a, 9b, . . . also serves as a cooling medium flow path through which the cooling medium flows, airtightness must be maintained between the coil holding material 1 and the holding member 10. By structuring the wire as described above, the cooling area that the superconducting wire receives can be significantly increased, and the stabilizing current lr can be increased by the relationship of the mth equation.

このため運転電流も増加することができ「同一空間に同
一磁界を発生する超電導コイル装置の大きさは、第2図
に示して従来タイプの超電導線3で巻回した超電導コイ
ル装置より小さくすることができる。なお、上記超電導
素線9a,9b,9c,….・・はそれぞれ絶縁処理が
施こされていない、いわゆる裸線でもまたは絶縁された
線でもどちらでもよい。
Therefore, the operating current can also be increased, and the size of the superconducting coil device that generates the same magnetic field in the same space should be smaller than the superconducting coil device shown in Figure 2, which is wound with the conventional type of superconducting wire 3. Note that the superconducting strands 9a, 9b, 9c, . . . may be either so-called bare wires without insulation treatment, or insulated wires.

また、上記超電導素線群9は、第3図に示した様な撚線
タイプのものでも、また編組線タイプのものでもよい。
さらに、上記押え都材1川まコイル保持部材1との間に
気密性を保つ必要があるため金属を用いコイル保持部材
1に溶接等で固定される。
Further, the superconducting wire group 9 may be of a twisted wire type as shown in FIG. 3, or may be of a braided wire type.
Further, since it is necessary to maintain airtightness between the presser material 1 and the coil holding member 1, metal is used and fixed to the coil holding member 1 by welding or the like.

このとき、巻回される超電導素線ga,gb・・・・・
・か絶縁処理のない裸線の場合には、コイル保持部材1
及び押え都材10と超電導素線群9との間に絶縁層を入
れ電気絶縁をとる必要がある。ここで、使用される冷却
媒体は液体ヘリウムの一相流でもよいし、または液体ヘ
リウムとヘリウムガスの二相流でもよい。
At this time, the superconducting wires ga, gb...
・In the case of bare wires without insulation treatment, coil holding member 1
Also, it is necessary to insert an insulating layer between the holding material 10 and the superconducting wire group 9 to provide electrical insulation. Here, the cooling medium used may be a one-phase flow of liquid helium or a two-phase flow of liquid helium and helium gas.

以上詳述したように「 この発明ではコイル保持部材に
巻回される超電導線材として、多数の超電導素線を撚線
あるし、は編組線に構成した超電導素線群を用いること
により、各超電導素線間に冷却媒体が流通できるように
なり「冷却べリメータの向上が図られ、超電導コイル装
置のコンパクト化を可能とし、その実用上の効果は大き
い。
As detailed above, ``In this invention, as the superconducting wire wound around the coil holding member, a group of superconducting strands made up of a large number of stranded or braided superconducting strands is used, so that each superconducting Cooling medium can now flow between the wires, improving the cooling verimer and making it possible to make superconducting coil devices more compact, which has great practical effects.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は先行技術の超電導ディスク構造から成る超電導
コイルの縦断面図、第2図は第1図の部分的な拡大斜視
図、第3図は、この発明の一実施例による部分的な拡大
斜視図である。 図において、1はコイル保持部材、2はコイル溝、3は
従来の超電導線、4は超電導ディスク、5はボルト、6
はナット、7は超電導コイル全体、8は間隔部材、ga
,9b,gc・…・・は超電導素線、9は超電導泰線群
、1川ま押え部材である。 なお、図中、同一符号は同一、又は相当部分を示す。第
1図 第2図 第3図
FIG. 1 is a longitudinal cross-sectional view of a superconducting coil having a prior art superconducting disk structure, FIG. 2 is a partially enlarged perspective view of FIG. 1, and FIG. 3 is a partially enlarged perspective view of an embodiment of the present invention. FIG. In the figure, 1 is a coil holding member, 2 is a coil groove, 3 is a conventional superconducting wire, 4 is a superconducting disk, 5 is a bolt, and 6
is a nut, 7 is the entire superconducting coil, 8 is a spacing member, ga
, 9b, gc... are superconducting wires, 9 is a group of superconducting wires, and 1 is a holding member. In addition, in the figures, the same reference numerals indicate the same or equivalent parts. Figure 1 Figure 2 Figure 3

Claims (1)

【特許請求の範囲】[Claims] 1 コイル溝が形成されたコイル保持部材と、上記コイ
ル溝に挿入され多数本の超電導素線を束にしてなる超電
導素線群と、上記コイル溝の開口部を気密に閉塞して上
記超電導素線間に冷却媒体を流通させる冷却媒体通路を
形成する押え部材を備えてなる超電導コイル。
1. A coil holding member in which a coil groove is formed, a group of superconducting strands inserted into the coil groove and formed into a bundle of multiple superconducting strands, and an opening of the coil groove airtightly closed to hold the superconducting element. A superconducting coil comprising a holding member that forms a cooling medium passage for circulating a cooling medium between the wires.
JP52078890A 1977-06-30 1977-06-30 superconducting coil Expired JPS60937B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP52078890A JPS60937B2 (en) 1977-06-30 1977-06-30 superconducting coil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP52078890A JPS60937B2 (en) 1977-06-30 1977-06-30 superconducting coil

Publications (2)

Publication Number Publication Date
JPS5413293A JPS5413293A (en) 1979-01-31
JPS60937B2 true JPS60937B2 (en) 1985-01-11

Family

ID=13674398

Family Applications (1)

Application Number Title Priority Date Filing Date
JP52078890A Expired JPS60937B2 (en) 1977-06-30 1977-06-30 superconducting coil

Country Status (1)

Country Link
JP (1) JPS60937B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5840803A (en) * 1981-09-04 1983-03-09 Hitachi Ltd Superconductive device

Also Published As

Publication number Publication date
JPS5413293A (en) 1979-01-31

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