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JPS6142403B2 - - Google Patents
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JPS6142403B2 - - Google Patents

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Publication number
JPS6142403B2
JPS6142403B2 JP55123015A JP12301580A JPS6142403B2 JP S6142403 B2 JPS6142403 B2 JP S6142403B2 JP 55123015 A JP55123015 A JP 55123015A JP 12301580 A JP12301580 A JP 12301580A JP S6142403 B2 JPS6142403 B2 JP S6142403B2
Authority
JP
Japan
Prior art keywords
superconducting
spacer
insulating plate
spacers
coil
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
JP55123015A
Other languages
Japanese (ja)
Other versions
JPS5748205A (en
Inventor
Tooru Saima
Mutsuhiko Yamaji
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co Ltd
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 Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP55123015A priority Critical patent/JPS5748205A/en
Publication of JPS5748205A publication Critical patent/JPS5748205A/en
Publication of JPS6142403B2 publication Critical patent/JPS6142403B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F6/00Superconducting magnets; Superconducting coils

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Containers, Films, And Cooling For Superconductive Devices (AREA)

Description

【発明の詳細な説明】 本発明は超電導磁気浮上車等に使用される超電
導磁石に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a superconducting magnet used in a superconducting magnetically levitated vehicle or the like.

近年、超電導磁気浮上車に関する研究開発は著
しい進歩を示し、それに使用される超電導電磁石
も強力・大容量・軽量小形化ときびしい要求を満
足すべく改良が続けられて来ている。しかし強
力・大容量化に伴い超電導電磁石のアンペアター
ンはどんどん増加し、その電磁力は想像を越える
大きな力となつて来ている。このために例えば
800KATのレーストラツク状(長円状)超電導コ
イルを使用したものでは、そのコイルの対向長辺
部間に26ton/mもの電磁反撥力が作用するよう
になり、この反撥力をいかにして受け止めてコイ
ルを安定的に固定させるかが超電導電磁石の製作
上大きな技術課題となつて来た。このコイルの安
定固定を失敗すると超電導電磁石は超電導状態を
維持できなくなつて、クエンチ現象に結びついて
行くようになつてしまうのである。
In recent years, research and development regarding superconducting magnetic levitation vehicles has shown remarkable progress, and the superconducting electromagnets used therein have continued to be improved in order to meet the strict requirements of greater strength, larger capacity, lighter weight, and smaller size. However, as superconducting electromagnets become more powerful and have a larger capacity, the ampere-turns of superconducting electromagnets are increasing rapidly, and the electromagnetic force is becoming more powerful than we can imagine. For this, for example
When using an 800 KAT racetrack-shaped (elliptic) superconducting coil, an electromagnetic repulsive force of 26 tons/m acts between the opposing long sides of the coil, and the question is how to absorb this repulsive force. Stably fixing the coil has become a major technical issue in the production of superconducting electromagnets. If this coil is not stably fixed, the superconducting electromagnet will no longer be able to maintain its superconducting state, leading to the quench phenomenon.

ここで、現在計画されている超電導電磁石の一
例を第1及び第2図により述べると、図中1はレ
ーストラツク状に構成した断面稍々扁平形の内槽
で、これは図示していないが熱伝達の少ない荷重
支持材と真空及び特殊断熱材により外槽内部に断
熱支持して収納する。またその上下対向長辺部相
互は結合材2により結合して変形を阻止してい
る。3は上記内槽1内部にその長円状に亘つて収
納された超電導コイルで、これはモールド等の手
段で一体化成形して固化固定することで剛性を有
する構造とすることが普通であり、こうした超電
導コイル3にこの長手方向に適当間隔を存して
FRP等の絶縁板を被嵌させて、その外周にスペ
ーサ5を囲設し、このスペーサ5により該コイル
3を内槽1内に固定保持している。なお、内槽1
及びスペーサ5等は分割しないと超電導コイル3
の収納ができないことから、縦又は横にそれぞれ
2分割して構成し、超電導コイル3にかぶせるよ
うにして溶接等により結合して組立てることを考
えている。また、図示省略したが超電導電磁石を
構成する上で必要な各種機器・配管等が組込まれ
ることは当然である。しかして上記内槽1を前述
の如く外槽内部に断熱支持して極めて低い熱侵入
量におさえた状態とすると共に、その内槽1内部
に液体ヘリウムを満たすことで、超電導コイル3
を極低温を冷却し、これにて超電導状態を保持し
て、励磁により永久電流を得るようにしている。
なお、その励磁の際に液体ヘリウムが内槽1内全
域を満たすべく流動できるように、又熱侵入によ
り気化したヘリウムガスが上昇して行ける様に、
上記スペーサ5には孔6を形成しておく。
Here, an example of a currently planned superconducting electromagnet will be described with reference to Figures 1 and 2. In the figure, 1 is an inner tank with a racetrack-like structure and a slightly flat cross section, which is not shown in the figure. It is insulated and stored inside the outer tank using a load support material with low heat transfer, vacuum and special heat insulating material. Further, the upper and lower opposing long sides are connected to each other by a bonding material 2 to prevent deformation. Reference numeral 3 denotes a superconducting coil housed inside the inner tank 1 in an elliptical shape, and this is usually formed into a rigid structure by integrally molding and solidifying it by means such as molding. , such superconducting coils 3 are provided with appropriate intervals in the longitudinal direction.
An insulating plate such as FRP is fitted, and a spacer 5 is placed around the outer periphery of the insulating plate, and the coil 3 is fixedly held in the inner tank 1 by the spacer 5. In addition, inner tank 1
If the spacer 5 etc. are not divided, the superconducting coil 3
Since it is not possible to store the superconducting coil 3, we are considering constructing it by dividing it into two parts vertically or horizontally, and assembling them by covering the superconducting coil 3 and joining them by welding or the like. Further, although not shown in the drawings, it is a matter of course that various equipment, piping, etc. necessary for configuring the superconducting electromagnet are incorporated. As described above, the inner tank 1 is insulated and supported inside the outer tank to suppress the amount of heat intrusion to an extremely low level, and the inner tank 1 is filled with liquid helium, so that the superconducting coil 3
The superconducting state is maintained by cooling the superconductor to an extremely low temperature, and a persistent current is obtained by excitation.
In addition, so that the liquid helium can flow to fill the entire area inside the inner tank 1 during the excitation, and so that the helium gas vaporized by heat penetration can rise.
A hole 6 is formed in the spacer 5.

こうした上記構成の超電導電磁石の場合、スペ
ーサ5による超電導コイル3の固定保持が十分で
ないと、該コイル3がガタを生じたり励磁による
電磁反撥力や何等かの加振などにより変形・移動
したりして、超電導状態がくずれ、クエンチ現像
に発展してしまう問題が生じる。このため、超電
導電磁石の製作上コイルの安定固定が大きな技術
課題となるのである。
In the case of a superconducting electromagnet having the above structure, if the spacer 5 does not sufficiently hold the superconducting coil 3 fixedly, the coil 3 may become loose or deformed or moved due to electromagnetic repulsion due to excitation or some kind of vibration. As a result, the superconducting state collapses, leading to a problem of quench development. For this reason, stably fixing the coil is a major technical challenge when manufacturing superconducting electromagnets.

本発明は上記事情に鑑みなされたもので、その
目的とする処は、超電導コイルを内槽内部に極め
確実に安定固定できて、該コイルの変形移動を完
全に防止し、非常に安定した高励磁能力を保有し
得て超電導磁気浮上車等に最適となる超電導電磁
石を提供しようとすることにある。
The present invention has been made in view of the above circumstances, and its purpose is to fix a superconducting coil extremely reliably and stably inside the inner tank, completely prevent deformation and movement of the coil, and achieve a very stable high-speed The object of the present invention is to provide a superconducting electromagnet that has excitation ability and is optimal for superconducting magnetic levitation vehicles and the like.

以下この発明の一実施例を第3図及び第5図に
より説明する。なお、ここでは要部のみを図示
し、その他は第1図、第2図と同様であるので簡
略化のため図示省略する。
An embodiment of the present invention will be described below with reference to FIGS. 3 and 5. Note that only the main parts are shown here, and the rest are the same as those in FIGS. 1 and 2, so illustrations are omitted for the sake of simplification.

第3図は第2図と同じ断面で超電導コイル絶縁
板、スペーサの関係を示し、第4図は絶縁板の形
状を示し、第5図はスペーサと絶縁板を密着させ
る為に工具により予圧縮力をあたえる為の方法を
示しており、3Aで示す超電導コイルは前記同様
モールド等で一体化成形により固化固定されてレ
ーストラツク状とされ、この超電導コイル3Aの
長手方向に間隔を存した断面部の周囲にFRP等
の絶縁板4A,4B,4C,4Dを配し、その外
周に上下2分割構造のスペーサ5A,5Bを囲設
し、これにて超電導コイル3Aに金属製スペーサ
5A,5Bが直接当つて超電導線の表面を傷つけ
て短絡したりするのを該絶縁板で防止していると
共に、励磁やクエンチを生じた時に短絡を生じな
い様にするために絶縁機能を持たせるのに十分な
クリーページをかせぐようにしている。
Figure 3 shows the relationship between the superconducting coil insulating plate and the spacer in the same cross section as Figure 2, Figure 4 shows the shape of the insulating plate, and Figure 5 shows pre-compression using a tool to make the spacer and insulating plate stick together. The superconducting coil 3A shown in FIG. Insulating plates 4A, 4B, 4C, and 4D such as FRP are placed around the outer periphery of the insulating plates 4A, 4B, 4C, and 4D, and spacers 5A and 5B that are divided into upper and lower halves are placed around the outer periphery of the superconducting coil 3A. The insulating plate prevents the surface of the superconducting wire from being damaged and short-circuited by direct contact with the superconducting wire, and also has sufficient insulation to prevent short-circuiting when excitation or quenching occurs. I am trying to earn a lot of creepage.

ここで、上下の絶縁板4A,4Bは第4図に示
す様に両側にフランジ11,11を有する断面
形状とされ、しかもその溝が中央部が浅く両端方
に行くに従い深くなるテーパー状溝とされてい
る。即ち、スペーサ5A,5Bと対向する溝内底
面が高い中央部9とこれから両端側に漸次低くな
るテーパー面10,10とからなる山形面とされ
ている。これにて絶縁板4A,4Bは両側フラン
ジ11,11によりスペーサ5A,5Bをはさみ
こんでずれを防ぎながら該絶縁板自体としては中
央が厚く端部に行くにしたがつて薄くなる構造と
なつている。こうした上下絶縁板4A,4B及び
両側絶縁板4C,4Dをかこんで上下2分割のス
ペーサ5A,5Bが囲設されているが、この上下
スペーサ5A,5Bには外周中央に大形の溝7
A,7Bが設けられ、それに近い所に孔6A,6
Aが配され、更に両側端方にも孔6B,6Bが配
され、これら溝及び孔により弾性変形可能な構造
とされて、互に予圧縮力を与えられた状態で溶接
ビート8A,8Bにより結合される。なお、スペ
ーサに予圧縮力をあたえる締付け工具12は上下
弓形状部材12A,12Bとこれらを締め上げる
ボルト13A,13Bとからなるもので、上下弓
形状部材12A,12Bでスペーサ5A,5Bを
弾性変形せしめる様に締め付けて該スペーサ5
A,5Bが絶縁板4A,4Bの溝内山形底面に完
全に密着するようにして溶接結合する。その工具
12の上下弓形状部材12A,12Bのスペーサ
5A,5Bに圧接する位置は絶縁板4A,4Bの
両端近傍上とするように工夫されている。その結
合したスペーサ5A,5Bの外側には図示しない
が2分割構造の内槽をかぶせて溶接接合し、更に
はその内槽を外槽内部に断熱支持して収納するこ
とで、超電導電磁石を組立て構成している。
Here, the upper and lower insulating plates 4A and 4B have a cross-sectional shape having flanges 11 and 11 on both sides as shown in FIG. has been done. That is, the inner bottom surface of the groove facing the spacers 5A, 5B is a chevron-shaped surface consisting of a high central portion 9 and tapered surfaces 10, 10 that gradually become lower from there toward both ends. In this way, the insulating plates 4A and 4B have spacers 5A and 5B sandwiched between the flanges 11 and 11 on both sides to prevent displacement, while the insulating plates themselves have a structure that is thick in the center and becomes thinner toward the ends. There is. Spacers 5A and 5B divided into upper and lower halves are provided surrounding the upper and lower insulating plates 4A and 4B and the both side insulating plates 4C and 4D.
A, 7B are provided, and holes 6A, 6 are provided near them.
A is arranged, and holes 6B, 6B are also arranged at both ends, and these grooves and holes form a structure that can be elastically deformed. be combined. The tightening tool 12 that applies pre-compression force to the spacer is made up of upper and lower arch-shaped members 12A, 12B and bolts 13A, 13B that tighten these members, and the upper and lower arch-shaped members 12A, 12B elastically deform the spacers 5A, 5B. Tighten the spacer 5
A and 5B are welded together so that they are completely in close contact with the chevron-shaped bottom surfaces of the insulating plates 4A and 4B. The positions where the upper and lower arch-shaped members 12A, 12B of the tool 12 come into pressure contact with the spacers 5A, 5B are designed to be near both ends of the insulating plates 4A, 4B. A superconducting electromagnet is assembled by covering the outside of the combined spacers 5A and 5B with a two-part inner tank (not shown) and welding them together, and then storing the inner tank with insulation support inside the outer tank. It consists of

而して本発明の機能について説明すると、スペ
ーサ5A,5Bの孔6A,6Bは超電導コイル3
Aを冷却する為に内槽内に注入された液体ヘリウ
ム及び冷却作用を行い気化したガスヘリウムの通
路となるが、その孔以外にもかなり大形の溝7
A,7Bが上下に配されている為に液体ヘリウム
の流入とガスヘリウムの流出が更に円滑となる。
又内槽を必要に応じてスペーサ5A,5Bの溝7
A,7Bと対向する所で分割した場合バツキング
プレートの取付スペースとしても流用出来るなど
機能的にも極めて好都合となる。
To explain the function of the present invention, the holes 6A and 6B of the spacers 5A and 5B are connected to the superconducting coil 3.
In addition to the hole, there is a fairly large groove 7 that serves as a passage for the liquid helium injected into the inner tank to cool A and the gas helium vaporized by the cooling effect.
Since A and 7B are arranged one above the other, the inflow of liquid helium and the outflow of gas helium become smoother.
In addition, the grooves 7 of the spacers 5A and 5B can be used as needed for the inner tank.
If it is divided at the location facing A and 7B, it will be extremely convenient from a functional point of view, as it can also be used as a mounting space for a backing plate.

ここで絶縁板4A,4Bのスペーサ5A,5B
と接する部分が山形面に構成されているので、中
央部は接するが両端部は若干の間隙を生じる。こ
の間隙はスペーサ5A,5Bの弾性と予圧縮をあ
たえる力により算出される量により決定しておく
ことで、工具12の上下弓形状部材12A,12
B及びボルト13A,13Bにより上下スペーサ
5A,5Bの外周両端隅角部付近に押力を加える
と、スペーサ5A,5Bが溝7A,7Bと孔6A
との間を結ぶ部分で弾性変形により彎曲したかな
り強いばね構造となつて、そのスペーサ5A,5
Bの内周面が絶縁板4A,4Bの溝内山形状底面
にそつて彎曲し密着するようになる。なお、その
際締付け工具12によりあたえられた押付力は、
超電導コイル3Aに作用する電磁力とほぼ同等以
上の力になる様にすれば、超電導コイル3Aに電
磁力が作用してもスペーサ5A,5Bに対し遊間
が生じる事は無くなり、こうした予圧縮力をかけ
た状態で8A,8Bの溶接を行いばスペーサ5
A,5Bによる超電導コイル3Aの固定保持が良
好となる。この時絶縁板4A,4Bの山形面のテ
ーパー角度は計算により或る程度推定出来るが、
最終的には実験にて確認をした値を使う事が必要
で、予圧縮力が電磁力より若干低い所で該絶縁板
4A,4Bの山形面とスペーサ5A,5Bが接触
しはじめる様にすると良好な結果を得る事が出来
る。この様に構成されたスペーサ5A,5Bの外
周に内槽が2分割にてかぶせられて締付け溶接接
合されることで、超電導コイル3Aは内槽内に於
いてスペーサ5A,5Bにより極めて安定した状
態で固定され、大きな電磁力を受けても変形や移
動する事が完全に防止され、安定した大容量の超
電導磁石を得る事が可能となる。
Here, spacers 5A and 5B of insulating plates 4A and 4B
Since the part in contact with is formed into a chevron-shaped surface, the center part contacts, but there is a slight gap at both ends. By determining this gap based on the amount calculated from the elasticity of the spacers 5A and 5B and the force that applies precompression, the upper and lower arch-shaped members 12A and 12 of the tool 12
When a pressing force is applied to the corners of both ends of the outer periphery of the upper and lower spacers 5A, 5B using B and the bolts 13A, 13B, the spacers 5A, 5B close to the grooves 7A, 7B and the hole 6A.
The spacers 5A, 5 form a fairly strong spring structure that is curved due to elastic deformation at the part connecting the spacers 5A, 5.
The inner circumferential surface of B is curved along the groove-inner mountain-shaped bottom surfaces of the insulating plates 4A and 4B, and comes into close contact. In addition, the pressing force applied by the tightening tool 12 at that time is
If the force is made to be approximately equal to or greater than the electromagnetic force acting on the superconducting coil 3A, even if the electromagnetic force acts on the superconducting coil 3A, there will be no gap between the spacers 5A and 5B, and such precompression force can be reduced. If you weld 8A and 8B with the spacer 5
The superconducting coil 3A is better fixed and held by A and 5B. At this time, the taper angle of the chevron-shaped surfaces of the insulating plates 4A and 4B can be estimated to some extent by calculation, but
In the end, it is necessary to use the values confirmed through experiments, so that the chevron-shaped surfaces of the insulating plates 4A, 4B and the spacers 5A, 5B begin to come into contact at a point where the precompression force is slightly lower than the electromagnetic force. Good results can be obtained. By covering the outer periphery of the spacers 5A and 5B configured in this manner with the inner tank divided into two parts and joining them by tightening and welding, the superconducting coil 3A is kept in an extremely stable state within the inner tank by the spacers 5A and 5B. This completely prevents deformation or movement even when subjected to large electromagnetic force, making it possible to obtain a stable, large-capacity superconducting magnet.

なお本発明の別の実施例として第6図に示す構
造のものも同じ効果を得る事が出来る。このスペ
ーサ5Cは図示しないが絶縁板と対向する内周面
が平滑で高い中央部14とこれから両端隅角方に
行くに従い低くなるテーパー面15A,15Bと
からなる山形面とされており、この場合絶縁板側
の溝内底面は平坦で良く、作用としては上記実施
例と全く同じ効果を得る事が可能である。又上記
テーパー面15A,15Bは円弧で構成されても
良く、すべてNC加工等によれば極めて容易に加
工する事が可能である。
It should be noted that another embodiment of the present invention having the structure shown in FIG. 6 can also achieve the same effect. Although not shown, the inner circumferential surface of this spacer 5C facing the insulating plate is a chevron-shaped surface consisting of a smooth and high central portion 14 and tapered surfaces 15A and 15B that become lower toward both end corners. The bottom surface of the groove on the insulating plate side may be flat, and it is possible to obtain exactly the same effect as in the above embodiment. Further, the tapered surfaces 15A and 15B may be formed of circular arcs, and can be processed extremely easily by NC processing or the like.

又その他の実施例としては2分割スペーサ5
A,5Bの互の結合を溶接ビード8A,8Bで行
う代りに、該スペーサ5A,5Bを図示しないが
相互に重ね合わせ適正な予圧縮力をあたえた上で
リーマー加工しピンを押し込んで固定してもよ
く、上記同様の効果を得ることが可能である。
In addition, as another embodiment, a two-part spacer 5
Instead of joining A and 5B with weld beads 8A and 8B, the spacers 5A and 5B are stacked on top of each other and given an appropriate precompression force (not shown), then reamed and fixed by pushing in a pin. It is also possible to obtain the same effect as above.

本発明は以上詳述した如くなしたから、超電導
コイルを内槽内部にスペーサにより極めて確実に
安定固定することができ、超電導状況を阻害する
ようなコイルの変形・移動を完全に防止できて、
非常に安定した高励磁能力を保有し得て超電導磁
気浮上車等に最適となるものである。
Since the present invention is made as described in detail above, the superconducting coil can be very reliably and stably fixed inside the inner tank with the spacer, and the deformation and movement of the coil that would impede the superconducting state can be completely prevented.
It has extremely stable and high excitation ability, making it ideal for superconducting magnetic levitation vehicles and the like.

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

第1図は現在計画されている超電導電磁石のレ
ーストラツク状内槽主要構造を示す一部断面した
側面図、第2図は第1図の―線に沿う拡大断
面図、第3図乃至第5図は本発明の一実施例を示
すもので、第3図はスペーサと超電導コイル断面
との関係説明図、第4図は絶縁板の斜視図、第5
図はスペーサを組付ける際に予圧縮力を与える工
具の使用例を示す説明図、第6図は本発明の他の
実施例を示す片側分割スペーサのみの正面図であ
る。 1……内槽、2……結合材、3,3A……超電
導コイル、4,4A,4B,4C,4D……絶縁
材、5,5A,5B,5C……スペーサ、6,6
A,6B……孔、7A,7B……溝、8A,8B
……溶接ビード、9,14……山形面の中央部、
10,15A,15B……山形面の両側テーパー
面、11……フランジ。
Figure 1 is a partially sectional side view showing the main structure of the racetrack-shaped inner tank of the currently planned superconducting electromagnet, Figure 2 is an enlarged sectional view taken along the - line in Figure 1, and Figures 3 to 5. The drawings show one embodiment of the present invention, in which Fig. 3 is an explanatory diagram of the relationship between the spacer and the cross section of the superconducting coil, Fig. 4 is a perspective view of the insulating plate, and Fig. 5
The figure is an explanatory diagram showing an example of the use of a tool that applies a precompression force when assembling a spacer, and FIG. 6 is a front view of only one side split spacer showing another embodiment of the present invention. 1... Inner tank, 2... Binding material, 3, 3A... Superconducting coil, 4, 4A, 4B, 4C, 4D... Insulating material, 5, 5A, 5B, 5C... Spacer, 6, 6
A, 6B...hole, 7A, 7B...groove, 8A, 8B
...Welding bead, 9,14...Central part of chevron surface,
10, 15A, 15B... Tapered surfaces on both sides of the chevron-shaped surface, 11... Flange.

Claims (1)

【特許請求の範囲】[Claims] 1 超電導磁気浮上車等に使用される超電導電磁
石において、モールド等により固化固定した超電
導コイルの周囲に絶縁板を配し、その絶縁板の外
周に各々溝・孔等の組合せにより弾性変形可能と
した2分割構造のスペーサを囲設し、且つ絶縁板
と分割スペーサとの対向面のどちらか一方に中央
が高く両側隅角部方に行くに従い低くなる山形面
を形成し、この山形面により生じる両側隅角部方
の空隙が無くなるように上記分割スペーサに予圧
縮力をもたせて相互に溶接又はピン等で結合して
超電導コイルの変形・移動を阻止して構成したこ
とを特徴とする超電導磁石。
1. In superconducting electromagnets used in superconducting magnetic levitation vehicles, etc., an insulating plate is placed around a superconducting coil that is solidified and fixed using a mold, etc., and each insulating plate is made elastically deformable by a combination of grooves, holes, etc. on the outer periphery of the insulating plate. A spacer with a two-part structure is enclosed, and a chevron-shaped surface is formed on one of the facing surfaces of the insulating plate and the divided spacer, and the center is high and becomes lower toward both corners. A superconducting magnet characterized in that the divided spacers are provided with a precompression force so as to eliminate voids at the corners, and are connected to each other by welding or pins to prevent deformation and movement of the superconducting coil.
JP55123015A 1980-09-05 1980-09-05 Superconductive electromagnet Granted JPS5748205A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP55123015A JPS5748205A (en) 1980-09-05 1980-09-05 Superconductive electromagnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP55123015A JPS5748205A (en) 1980-09-05 1980-09-05 Superconductive electromagnet

Publications (2)

Publication Number Publication Date
JPS5748205A JPS5748205A (en) 1982-03-19
JPS6142403B2 true JPS6142403B2 (en) 1986-09-20

Family

ID=14850118

Family Applications (1)

Application Number Title Priority Date Filing Date
JP55123015A Granted JPS5748205A (en) 1980-09-05 1980-09-05 Superconductive electromagnet

Country Status (1)

Country Link
JP (1) JPS5748205A (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63150475A (en) * 1986-12-12 1988-06-23 Honda Motor Co Ltd Shoe structure in swash plate type hydraulic equipment
JP2859427B2 (en) * 1990-11-21 1999-02-17 株式会社東芝 Superconducting coil device
JP4153725B2 (en) 2002-05-22 2008-09-24 ユニ・チャーム株式会社 Pants-type diapers

Also Published As

Publication number Publication date
JPS5748205A (en) 1982-03-19

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