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JPS58186914A - Superconductive magnet apparatus - Google Patents

Superconductive magnet apparatus

Info

Publication number
JPS58186914A
JPS58186914A JP57070753A JP7075382A JPS58186914A JP S58186914 A JPS58186914 A JP S58186914A JP 57070753 A JP57070753 A JP 57070753A JP 7075382 A JP7075382 A JP 7075382A JP S58186914 A JPS58186914 A JP S58186914A
Authority
JP
Japan
Prior art keywords
reinforcing member
superconducting
aluminium
helium container
superconductive 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.)
Pending
Application number
JP57070753A
Other languages
Japanese (ja)
Inventor
Hirohisa Takano
高野 広久
Kazunari Nakamoto
一成 中本
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp, Tokyo Shibaura Electric Co Ltd filed Critical Toshiba Corp
Priority to JP57070753A priority Critical patent/JPS58186914A/en
Publication of JPS58186914A publication Critical patent/JPS58186914A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F6/00Superconducting magnets; Superconducting coils
    • H01F6/06Coils, e.g. winding, insulating, terminating or casing arrangements therefor

Landscapes

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

Abstract

PURPOSE:To firmly hold a superconductive coil within a helium container while cooling process and ease an electromagnetic force working on a super-conductive coil by arranging a reinforcing member consisting of aluminium or aluminium alloy having a line expansion coefficient larger than that of copper at the outside of superconductive coil mainly consisting of copper and accommodating it within the helium container. CONSTITUTION:The figure shows a sectional view. 2 indicates a helium container, and the outside of superconductive coil 1 is surrounded by a reinforcing member 8 consisting of aluminium or aluminum alloy through a spacer 7 consisting of an insulator. Moreover, cotters 5, 6 may be inserted between the superconductive coil 1 and reinforcing member 8 in place of the spacer 7. The helium container 2 itself may be formed with aluminium or aluminium alloy and the cotters 5 and 6 may be inserted as the reinforcing members 8. In case the reinforcing member 8 is formed by aluminium or aluminium alloy, contraction of reinforming member 8 consisting of aluminium or aluminium alloy is more distinctive than that of copper. A shrinkage fit allowance is given rather than forming clearance between the superconductive coil 1 and the reinforcing member 8 and thereby the superconductive coil 1 and helium container 2 can be combined more stringly.

Description

【発明の詳細な説明】 〔発明cD技術分野〕 本発明は超電導;イルに作用する電磁カミ軽減したWi
電導マグネット装置に関する。
[Detailed Description of the Invention] [Technical Field of the Invention] The present invention is directed to superconducting;
This invention relates to a conductive magnet device.

〔発明の技術的背景〕[Technical background of the invention]

第1図扛超電導マダネット装置の一例【示す図で1扛超
電導導体を巻回して構成し友超電導コイルである。この
コイル1轄液体ヘリウムを収納丁ゐヘリウム容器2内に
収納している。1友ヘリウム容b2は真空容器3内に収
納している。そしてヘリウム容器2と貞9容器3との間
會真9に保ち真空断熱を行なうようにしてい−る。
Fig. 1 An example of a superconducting Madanet device [In the figure shown, one superconducting conductor is wound to form a superconducting coil. This coil 1 liquid helium is stored in a helium container 2. A helium container b2 is housed in a vacuum container 3. The space between the helium container 2 and the helium container 3 is maintained at 9 and vacuum insulation is provided.

またこのへリウム答麹1と真9容器Sと0間にはふく射
熱の浸入管防ぐためふく射シールド411獣している。
In addition, there is a radiation shield 411 between the helium reaction koji 1 and the true 9 containers S and 0 to prevent radiant heat from entering the tube.

このような補H,〇超電導コイルに毅て、近時鳥い轟場
を要X畜れ、それによって大きな電磁力が作用すめため
に超電導コイル1自身ではそO機械的強度を保てなくな
p、へシウム容−1にも電磁力の一部を伝達し超電導コ
イル1にかかる応力t@滅する試みがなされている。第
2図はこのような構成の超電導=イに〇−例の要部を示
す断面図でヘリウム客器1と超電導=イル1との間にク
ナビ状KIIt形し良絶縁物より構成されるコツター5
.6を挿入する。すなわちコツター5【ヘリウム容器1
0内壁に配置し、このブック−5と超電導コイル1とO
関にコツター61挿入して超電導コイル1に作用す墨電
磁力をヘリウム容器1に効率よく伝達しようとするもの
である。
In order to maintain the strength of such superconducting coils, the superconducting coil 1 has recently been exposed to a very strong field, and due to the large electromagnetic force acting on it, the superconducting coil 1 itself cannot maintain its mechanical strength. Attempts have been made to transmit part of the electromagnetic force to the hesium capacitor 1 to eliminate the stress t@ applied to the superconducting coil 1. Figure 2 is a cross-sectional view showing the main parts of a superconductor with such a configuration. 5
.. Insert 6. In other words, Cottater 5 [Helium container 1
This book-5, superconducting coil 1 and O
This is intended to efficiently transmit black electromagnetic force acting on the superconducting coil 1 to the helium container 1 by inserting a colander 61 into the superconducting coil 1.

〔背景技術の問題点〕[Problems with background technology]

しかしながらこのような40で轄ヘリクム寝aXはステ
ンレス鋼からな)、超電導コイル1の超電導体の主成分
扛銅である丸め、その熱膨張係数の差によって低温まで
冷却する場合、例えtf300Kから4.2 K ”1
で冷却する場合、両者の間にコツター6の1九た自込み
代1以上のスキマ【生じ、超電導コイルIKかかる電磁
力tヘリウム@器2へ伝達できなくなる。このために超
IIL導コイルIK過大な応力がかか9、場合によって
は超電導導体の破壊につながる。さらにこのような状況
で超電導導体に1gcm力が作用した場合、導体間に動
at生じ、その発熱作用勢のために所要の定格磁場音発
生できなくなる可能性がある。
However, when the superconducting coil 1 is made of copper (the main component of the superconductor of the superconducting coil 1 is copper), when cooling to a low temperature due to the difference in coefficient of thermal expansion, even if the superconducting coil 1 is cooled to a low temperature from 300 K to 4. 2K”1
When cooling the superconducting coil IK, a gap of 1 or more is generated between the two, and the electromagnetic force applied to the superconducting coil IK cannot be transmitted to the helium reactor 2. This imposes excessive stress on the super-IIL conductor IK, 9 which may lead to destruction of the superconductor. Furthermore, if a force of 1 gcm is applied to the superconducting conductor in such a situation, movement will occur between the conductors, and due to the heat generation force, there is a possibility that the required rated magnetic field sound cannot be generated.

〔発明の目的〕[Purpose of the invention]

本発明は上虻の事情に鑑みてなされたもので超電導コイ
ルとヘリウム容器との間にアル電又はアルミ合金からな
る補強部材を介挿して両者を強固に結合し、それによっ
て、超電導コイルに作用する電磁力V*滅することがで
きる超電導マグネット装置管提供すること【目的とする
奄のである。
The present invention was made in view of the above-mentioned circumstances, and a reinforcing member made of aluminum or aluminum alloy is inserted between the superconducting coil and the helium container to firmly connect the two, thereby acting on the superconducting coil. The objective is to provide a superconducting magnet device tube that can eliminate the electromagnetic force V*.

〔発明の値要〕[Value of invention]

すなわち本発明は超IIE導コイルの外周【アルミ又は
アルミ合金からなる補強部材で囲繞してヘリウム客器に
保持することt%黴とするものである。
That is, the present invention is to surround the outer periphery of a super IIE conductive coil with a reinforcing member made of aluminum or an aluminum alloy and to hold it in a helium container.

〔発明の実施例〕[Embodiments of the invention]

以下本発明の一実施例を第3図、第4図を参照して詳細
に説明する。第311Iは断面図で図中1は超電導コイ
ル、2はヘリウム容器である。
An embodiment of the present invention will be described in detail below with reference to FIGS. 3 and 4. 311I is a cross-sectional view, in which 1 is a superconducting coil and 2 is a helium container.

そして超電導コイル1の外側に絶縁物より構成されるス
ペーサ1(介して、アル櫂又はアルミ合金よりなる補強
部材8で囲繞する。仁の補強部材8は円形のリング状の
ものでもよいし、非円形のコイル周li!It−嶺う部
材でも良い。壜た第4図に示すようにスペーサ10かわ
砂に超電導コイル1と補強部材8と0間にコツター5.
6【挿入するようにしてもよい、11えヘリウム客器1
自体tアルン又はアルミ合金より構成して補強部材8t
−兼ねるようにし、このヘリウム客器兼補強部材と超電
導=イル1との間に第4図に示すように;イタ−5,6
を挿入してもよい。
The superconducting coil 1 is surrounded by a reinforcing member 8 made of an aluminum paddle or an aluminum alloy through a spacer 1 made of an insulating material on the outside of the superconducting coil 1. A member that extends around the circumference of the circular coil may also be used.As shown in FIG.
6 [You may insert 11 helium container 1
Reinforcement member 8t made of aluminum alloy or aluminum alloy
- As shown in FIG.
may be inserted.

#!5図はアルミニウム、銅、ステンレス銅むm*張係
数を示す図て、横軸扛温度(絶対鯨)ty5し縦軸が*
*張率を示す。第5図において各材料の線膨張率の大き
さはアル1=ウム〉銅〉ステンレス−のIIIKなる。
#! Figure 5 shows the tensile modulus of aluminum, copper, and stainless steel.
*Indicates tensile strength. In FIG. 5, the coefficient of linear expansion of each material is IIIK for aluminum, copper, and stainless steel.

一方M114 :1イh1、ヘリウム容器2などは製作
時室温で組立てられ、実際に超電導コ、イルとして使用
する九めに1111c第抵抗に−v口にする場合に社液
体ヘリウムーii&腋4.2に箇で冷却しなけれはなら
ない。この時の熱収縮率Δ1はそOi!温から4.2に
迄の温度差41間における部材、の平均線膨張係数αか
ら次の1)式で与えられる。
On the other hand, M114: 1 h1, helium container 2, etc. are assembled at room temperature during manufacture, and when the 1111c resistor is used as a superconducting coil, liquid helium II & armpit 4.2 are used. It must be cooled in stages. The heat shrinkage rate Δ1 at this time is Oi! It is given by the following equation 1) from the average linear expansion coefficient α of the member during the temperature difference 41 from 4.2 to 4.2.

Δj;αXΔT  川・・川・ 1) すなわち、補強部材8′tアルミまたはアルミ合金とす
ることによって、銅に比ベアル<tたはアルミ合金から
なる補強部材8の縮み量の方が大きい。すなわち、超電
導コイル1と補強部材80間にスキiを生じるどころか
1焼睡はめ代1會与え、より9M向に超電導コイル1と
ヘリウム容器2とt結合させることができる。また絹5
図から明らかなように従来の一−ステンレスーの組み合
わせでは中心倒に位置する主に銅からなる超電導コイル
の方が外匈のステンレス鋼からなるヘリウム容−2より
も大きく縮むために、その間にスキマを生ずることは明
らかである。!7tアル建又にアルミ合金以外にも銅に
比して、よpat張係数の大きい材料はあるが、製作性
、経済性、強度等の点でアルミ又はアルミ合金が最奄好
ましい。
Δj;αXΔT River···························· 1) That is, by making the reinforcing member 8't aluminum or aluminum alloy, the amount of shrinkage of the reinforcing member 8 made of aluminum alloy or bearing <t is larger than that of copper. In other words, instead of creating a gap between the superconducting coil 1 and the reinforcing member 80, a 1-coin allowance is provided, and the superconducting coil 1 and the helium container 2 can be coupled in the 9M direction. Also silk 5
As is clear from the figure, in the conventional 1-stainless steel combination, the superconducting coil located in the center and made mainly of copper shrinks more than the helium container made of stainless steel on the outside, so there is no gap between them. It is clear that this will occur. ! Although there are materials other than 7t aluminum and aluminum alloys that have a higher tensile modulus than copper, aluminum or aluminum alloys are most preferred in terms of manufacturability, economy, strength, etc.

なお本発明社上記実施例に隈定されるものではなく、た
とえばコイル1の全周にアルミ又はアルき合金からなる
補強部材8t一般社ず、その一部にアに7又扛アルミ合
金を用いその他の部分に他の部材1組み合わせて超電導
コイに1を補強するようにしてもよい。
It should be noted that the present invention is not limited to the above-mentioned embodiments; for example, the reinforcing member 8t made of aluminum or aluminum alloy is generally used around the entire circumference of the coil 1, and a part of the reinforcing member is made of a seven-pronged aluminum alloy. Other parts may be combined with other members 1 to reinforce the superconducting coil.

〔発明の効果〕〔Effect of the invention〕

以上のように本発明は主に銅からなる超電導コイルの外
側に、銅よシも線膨侵率の大きいアルミ又はアルミ合金
からなる補強部材【配置し、これ七ヘリクムs*rc収
納するようにし喪ので冷却時に超電導コイル【ヘリクム
容器Kll実に保持でIiそれによって超電導コイルに
作用する電磁力t@滅することができる超電導マグネッ
トfi!直を提供することかで龜る。
As described above, the present invention places a reinforcing member made of aluminum or aluminum alloy, which has a higher coefficient of linear expansion than copper, on the outside of a superconducting coil mainly made of copper, and stores the reinforcing member of seven helium s*rc. When the superconducting coil is cooled down, the superconducting coil can be held in place by the superconducting magnet, which can eliminate the electromagnetic force acting on the superconducting coil! It is difficult to provide direct service.

纂1図は従来の超電導マグネット装置の一例に不すll
l!IT面図、第2図は従来の超電導マグネット装置の
要部1示す図、1llN3図扛本発明の一笑一例會示す
断面図、第4図に本発明の他の実施例の要部を示す図、
第5図探合材料の線II#張率を示す図である。
Figure 1 is an example of a conventional superconducting magnet device.
l! IT plan view, FIG. 2 is a view showing the main part 1 of a conventional superconducting magnet device, 1llN3 is a sectional view showing an example of the present invention, and FIG. 4 is a view showing the main part of another embodiment of the present invention. ,
FIG. 5 is a diagram showing the line II# elongation of the probe material.

1・・・超電導コイル、1・・・ヘリウム!!器、3・
・・)?!!器、4・・・−く射シールド、5.6・・
・コツ/−1フー8.スペーサ、8・・・補強部材。
1...Superconducting coil, 1...Helium! ! Vessel, 3.
...)? ! ! Vessel, 4... - Shooting shield, 5.6...
・Tips/-1 Fu 8. Spacer, 8... reinforcing member.

出願人代理人  弁理士 鈴 江 武 彦第1図 第2図 第3図 第4図Applicant's agent: Patent attorney Takehiko Suzue Figure 1 Figure 2 Figure 3 Figure 4

Claims (1)

【特許請求の範囲】 (υ ヘリウム容器内に超電導導体會巻謙した超電導コ
イルを収納し良もOKお−て、麺電導プイルの外側を絶
縁物!介してアルR重えはアル建合金から′&る補強部
材でsIl&シて上記ヘリウム容器に保持すること10
徽とする超電導マグネット装置。 (乃 特許請求の範囲第1項記載のものにおいて、補強
部材管円形のリング状KIit形し、この補強部材と超
電導ツイルと0間に絶縁材!介挿したことt特徴とする
超電導!!ネット装置。 (a)  特許請求の範囲第2項記載OもOにおいて、
クサビ状の絶縁材を補強部材と超電導;イルとの間に挿
入したことt時機と丁ゐ超電導!グネット装置。 (4%軒請求O範WA第1項1九は第2項記載のものに
おいて、アル電又はアル電金金からな心ヘリウム容it
楠強部材とすることt%黴と丁4超電導マグネット装置
[Claims] (υ It is OK to store a superconducting coil with a superconducting conductor in a helium container, and the outside of the noodle conductive pool is insulated! Hold it in the helium container with the reinforcing member 10.
A superconducting magnet device. (No. The superconducting net characterized in that the reinforcing member tube is shaped like a circular ring, and an insulating material is inserted between the reinforcing member, the superconducting twill, and the superconducting twill. Apparatus. (a) O described in claim 2 also includes:
A wedge-shaped insulating material was inserted between the reinforcing member and the superconducting wire. Gnet device. (Article 1, 19 of the 4% Claims WA applies to the thing described in Paragraph 2, where the heart helium capacity is
A superconducting magnet device with t% mold and 4 superconducting magnets made of Kusunoki materials.
JP57070753A 1982-04-27 1982-04-27 Superconductive magnet apparatus Pending JPS58186914A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57070753A JPS58186914A (en) 1982-04-27 1982-04-27 Superconductive magnet apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57070753A JPS58186914A (en) 1982-04-27 1982-04-27 Superconductive magnet apparatus

Publications (1)

Publication Number Publication Date
JPS58186914A true JPS58186914A (en) 1983-11-01

Family

ID=13440582

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57070753A Pending JPS58186914A (en) 1982-04-27 1982-04-27 Superconductive magnet apparatus

Country Status (1)

Country Link
JP (1) JPS58186914A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0200867A3 (en) * 1985-05-10 1988-01-07 Kernforschungszentrum Karlsruhe Gmbh Dismantable structure for the mutual strutting of two constructional elements at a low temperature
WO2007135459A1 (en) * 2006-05-22 2007-11-29 Siemens Magnet Technology Limited Improved magnetic formers

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58148808A (en) * 1982-02-16 1983-09-05 デグツサ・アクチエンゲゼルシヤフト Bactericide

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS58148808A (en) * 1982-02-16 1983-09-05 デグツサ・アクチエンゲゼルシヤフト Bactericide

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0200867A3 (en) * 1985-05-10 1988-01-07 Kernforschungszentrum Karlsruhe Gmbh Dismantable structure for the mutual strutting of two constructional elements at a low temperature
WO2007135459A1 (en) * 2006-05-22 2007-11-29 Siemens Magnet Technology Limited Improved magnetic formers

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