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JPH05267725A - Superconducting magnet - Google Patents

Superconducting magnet

Info

Publication number
JPH05267725A
JPH05267725A JP4062808A JP6280892A JPH05267725A JP H05267725 A JPH05267725 A JP H05267725A JP 4062808 A JP4062808 A JP 4062808A JP 6280892 A JP6280892 A JP 6280892A JP H05267725 A JPH05267725 A JP H05267725A
Authority
JP
Japan
Prior art keywords
superconducting coil
shield plate
superconducting
superconducting magnet
magnetic field
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
JP4062808A
Other languages
Japanese (ja)
Inventor
Tadashi Tokumasu
正 徳増
Takashi Hanai
隆 花井
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
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 filed Critical Toshiba Corp
Priority to JP4062808A priority Critical patent/JPH05267725A/en
Publication of JPH05267725A publication Critical patent/JPH05267725A/en
Pending legal-status Critical Current

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  • Superconductor Devices And Manufacturing Methods Thereof (AREA)
  • Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)

Abstract

PURPOSE:To stably cool a superconducting magnet by a method wherein, when the superconducting magnet receives an external fluctuating magnetic field, the quantity of evaporation of helium, caused by the relative vibration generated between a shield plate and a superconducting coil by an induced current, is reduced. CONSTITUTION:Pertaining to the shielding plate 2 of a superconducting magnet, the part opposing to a superconducting coil 1 is composed of the material of high conductivity, and other part is composed of the material of low conductivity. The magnetic shield effect against the superconducting coil 1 is unchanged in the above-mentioned constitution, but the electromagnetic force of the whole shield plate 2 is decreased, its rigity is increased, and relative vibration is suppressed.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は超電導磁石の構成に関す
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to the construction of superconducting magnets.

【0002】[0002]

【従来の技術】従来の超電導磁石について図4、図5を
参照して説明する。
2. Description of the Related Art A conventional superconducting magnet will be described with reference to FIGS.

【0003】超電導磁石は、超電導コイル1、シールド
板2、真空容器3から構成されている。超電導コイル1
は、超電導導体のコイルを金属の容器に入れたもので、
この容器内は超電導体を冷却するための液体ヘリウムが
満たされている。
The superconducting magnet comprises a superconducting coil 1, a shield plate 2 and a vacuum container 3. Superconducting coil 1
Is a superconducting coil placed in a metal container.
The container is filled with liquid helium for cooling the superconductor.

【0004】さらに、超電導コイル1を安定して超電導
状態に保つためには、超電導コイル1内で発生する熱お
よび外部から超電導コイル1内へ侵入する熱を極力減ら
すことが必要である。これは一つには超電導導体を冷却
する液体ヘリウムは熱容量が小さいため、侵入熱・熱発
生が大きくなると蒸発による液体ヘリウムの消費量が多
くなり、超電導導体の安定的な冷却が行えなくなるから
である。このように冷却が不十分になったり、超電導コ
イル内部での熱発生したりすることによって超電導導体
の温度が上昇し、臨海温度を越えると超電導導体が常電
導状態に転移し、超電導磁石として機能が失われてしま
う。
Further, in order to stably maintain the superconducting coil 1 in a superconducting state, it is necessary to reduce heat generated in the superconducting coil 1 and heat entering the superconducting coil 1 from the outside as much as possible. This is partly because the liquid helium that cools the superconducting conductor has a small heat capacity, so if the amount of intrusion heat / heat generation increases, the amount of liquid helium consumed by evaporation will increase and stable cooling of the superconducting conductor will not be possible. is there. In this way, the temperature of the superconducting conductor rises due to insufficient cooling or heat generation inside the superconducting coil, and when the temperature exceeds the critical temperature, the superconducting conductor changes to the normal conducting state and functions as a superconducting magnet. Will be lost.

【0005】このため、超電導コイル1は、低熱伝導材
からなるコイル支持材4で真空容器3に固定されてい
る。また、対流伝熱を防ぐために、真空容器内は真空に
保持され、さらに輻射電熱を減らすために常温の真空容
器3の壁と超電導コイル1との間には液体窒素などで冷
却されるシールド板2が設置されている。
Therefore, the superconducting coil 1 is fixed to the vacuum container 3 by the coil supporting member 4 made of a low heat conductive material. Further, in order to prevent convective heat transfer, the inside of the vacuum container is kept vacuum, and in order to reduce radiant heat, a shield plate cooled between the wall of the vacuum container 3 at room temperature and the superconducting coil 1 by liquid nitrogen or the like. 2 are installed.

【0006】超電導コイル1に横方向5(矢印)から変
動磁界が作用する場合、この外部からの変動磁界によっ
て超電導コイル1の金属容器および超電導導体に誘導電
流が流れて発熱することを防ぐため、従来、真空容器3
およびシールド板2を導電率の高い材料で構成し、真空
容器3およびシールド板2に誘導電流を発生させること
により、その反作用磁界で変動磁界をシールドすること
が行われている。
When a fluctuating magnetic field acts on the superconducting coil 1 from the lateral direction 5 (arrow), in order to prevent the fluctuating magnetic field from the outside from causing an induced current to flow in the metal container and the superconducting conductor of the superconducting coil 1 to generate heat, Conventionally, vacuum container 3
Further, the shield plate 2 is made of a material having a high conductivity, and an inductive current is generated in the vacuum container 3 and the shield plate 2 to shield the fluctuating magnetic field with the reaction magnetic field.

【0007】[0007]

【発明が解決しようとする課題】しかしこのような構成
では、真空容器およびシールド板に流れる誘導電流は、
超電導コイルのつくる磁界との相互作用によって電磁力
が生じて真空容器の壁やシールド板を振動させる。真空
容器壁の振動はさらにコイル支持材4を介してシールド
板2や超電導コイル1に伝わり、これらを振動させる。
これらの振動により、シールド板2と超電導コイル1と
の間に相対振動が発生する。
However, in such a structure, the induced current flowing through the vacuum container and the shield plate is
An electromagnetic force is generated by the interaction with the magnetic field created by the superconducting coil, causing the wall of the vacuum container and the shield plate to vibrate. The vibration of the vacuum vessel wall is further transmitted to the shield plate 2 and the superconducting coil 1 via the coil supporting member 4 and vibrates them.
Due to these vibrations, relative vibration is generated between the shield plate 2 and the superconducting coil 1.

【0008】この相対振動により、超電導コイルのつく
る直流磁界の中で、導電性の板が振動することになり、
そこに誘導電流が誘起される。さらに、この誘導電流が
つくる変動磁界が超電導コイルに達することにより、そ
の変動磁界の影響で超電導コイルの金属容器・超電導導
体に発熱が生じ、超電導コイル1を冷却している液体ヘ
リウムの消費量が多くなって、安定的な超電導導体の冷
却ができなくなるという問題がある。
Due to this relative vibration, the conductive plate vibrates in the DC magnetic field created by the superconducting coil.
An induced current is induced there. Further, when the fluctuating magnetic field generated by the induced current reaches the superconducting coil, heat is generated in the metal container / superconducting conductor of the superconducting coil due to the influence of the fluctuating magnetic field, and the consumption of liquid helium cooling the superconducting coil 1 is reduced. There is a problem that the number of the superconducting conductors cannot be stably cooled due to the increase in the number.

【0009】本発明は変動磁界を受ける超電導磁石にお
いて、液体ヘリウムで冷却されている超電導コイルの金
属容器・超電導導体の発熱を減少させて、超電導導体を
安定的に冷却し、超電導磁石としての安定性を向上させ
ることを目的とする。
According to the present invention, in a superconducting magnet subjected to a fluctuating magnetic field, the heat generation of the metal container and the superconducting conductor of the superconducting coil cooled by liquid helium is reduced to stably cool the superconducting conductor and stabilize as a superconducting magnet. The purpose is to improve sex.

【0010】[0010]

【課題を解決するための手段】このため本発明では、超
電導磁石のシールド板のうち超電導コイルと対向する部
分のみを導電率の高い材料で構成し、その他の部分につ
いては導電率の低い材料で構成する。
Therefore, in the present invention, only the portion of the shield plate of the superconducting magnet facing the superconducting coil is made of a material having a high conductivity, and the other portions are made of a material having a low conductivity. Constitute.

【0011】[0011]

【作用】シールド板の超電導コイルと対向する部分の導
電率が高いため、超電導コイルに侵入しようとする変動
磁界はこの部分に誘起される誘導電流でシールドされ、
外部からの変動磁界は超電導コイルには達しない。
[Function] Since the portion of the shield plate facing the superconducting coil has a high conductivity, the fluctuating magnetic field attempting to enter the superconducting coil is shielded by the induced current induced in this portion,
The fluctuating magnetic field from the outside does not reach the superconducting coil.

【0012】一方、その他の部分は導電率の低い材料で
形成しているため、従来この部分に誘起されていた誘導
電流はほとんど発生せず、従ってこの部分での電磁力も
大幅に低減する。また、従来は導電性の高い材料として
銅やアルミを用いていたためシールド板の剛性を高める
ことが困難であったが、本発明ではシールド板の剛性に
大きく寄与する中央部分に高強度材を使用できるため、
シールド板の剛性を高める効果もあり、電磁力・剛性の
両面からシールド板の振動を減少することができる。
On the other hand, since the other portions are formed of a material having a low conductivity, the induced current which has been conventionally induced in this portion is hardly generated, and therefore the electromagnetic force in this portion is also significantly reduced. Further, conventionally, it was difficult to increase the rigidity of the shield plate because copper or aluminum was used as the material having high conductivity, but in the present invention, a high-strength material is used in the central portion that greatly contributes to the rigidity of the shield plate. Because you can
It also has the effect of increasing the rigidity of the shield plate, and can reduce the vibration of the shield plate from both aspects of electromagnetic force and rigidity.

【0013】さらに、真空容器の振動が伝わることなど
によって、シールド板と超電導コイルが相対振動した場
合でも、シールド板の一部が導電率の低い材料で構成さ
れているため、誘起される誘導電流の流れる流路が制限
され、シールド板の誘導電流が低減され、またこの誘導
電流がつくる変動磁界が超電導コイルに達する量も低減
できる。
Further, even if the shield plate and the superconducting coil vibrate relative to each other due to the transmission of the vibration of the vacuum container, a part of the shield plate is made of a material having a low electric conductivity, so that an induced current is induced. Is restricted, the induced current in the shield plate is reduced, and the amount of the variable magnetic field generated by the induced current reaching the superconducting coil can be reduced.

【0014】[0014]

【実施例】本発明について図1、図2に示す実施例に基
づいて説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described based on the embodiments shown in FIGS.

【0015】真空容器3内に設けるシールド2は、超電
導コイル1と対向する部分2aは銅またはアルミの導電率
の高い材料で、その他の部分2bは高強度ステンレス材の
ような導電率が低く、剛性の高い材料で構成する。な
お、実施例では外部からの変動磁界が5の方向から加わ
るものとして、変動磁界の侵入してくる方向にのみ導電
率の高い材料を用いているが、外部からの変動磁界がそ
の他の方向から侵入する場合や、複数の方向から侵入す
る場合にはそれに応じて超電導コイル1と対向する部分
2aを設定するものとする。
In the shield 2 provided in the vacuum container 3, the portion 2a facing the superconducting coil 1 is made of copper or aluminum having a high electric conductivity, and the other portion 2b has a low electric conductivity such as high strength stainless steel. Constructed of highly rigid material. It should be noted that in the embodiment, a material having a high conductivity is used only in the direction in which the fluctuating magnetic field enters, assuming that the fluctuating magnetic field from the outside is applied from the direction 5, but the fluctuating magnetic field from the outside is applied from other directions. When intruding or intruding from multiple directions, the portion facing the superconducting coil 1 accordingly.
2a shall be set.

【0016】また、本実施例では導電率の高い材料と導
電率の低い材料を接合部8で接合するようにしている
が、製造上の便宜のために、例えばシールド板2全体を
導電率の低い材料で構成し、超電導コイル1と対向する
部分2aにのみ導電率の高い材料を導電率の低い材料に重
ねて設置するようにしても作用・効果は変わらない。
Further, in this embodiment, the material having a high conductivity and the material having a low conductivity are joined at the joint portion 8. However, for convenience of manufacturing, for example, the entire shield plate 2 is made of a material having a conductivity. Even if the material is made of a low material and the material having high conductivity is placed only on the portion 2a facing the superconducting coil 1 so as to overlap the material having low conductivity, the operation and effect are not changed.

【0017】前述したようにシールド板2のうち超電導
コイル1と対向する部分2aは導電率の高い材料で構成し
ているので、超電導コイル1に侵入しようとする外部変
動磁界はシールド板2でシールドされる。
As described above, since the portion 2a of the shield plate 2 facing the superconducting coil 1 is made of a material having a high conductivity, the external fluctuating magnetic field trying to enter the superconducting coil 1 is shielded by the shield plate 2. To be done.

【0018】また、シールド板2の超電導コイルと対向
しないその他の部分2bは導電率の低い材料で構成してい
るため、シールド板全体としての誘導電流・電磁力が低
減され、振動を低減できる。さらにその他の部分2bには
高強度材を使用しているのでシールド板2全体としての
剛性も高くなり、従ってその点からも振動が抑制され
る。
Further, since the other portion 2b of the shield plate 2 which does not face the superconducting coil is made of a material having a low electric conductivity, the induced current and electromagnetic force of the shield plate as a whole are reduced and vibration can be reduced. Further, since the high strength material is used for the other portion 2b, the rigidity of the shield plate 2 as a whole is increased, and therefore vibration is suppressed also from that point.

【0019】さらに、超電導コイル1とシールド板2が
相対振動した場合にも、超電導コイル1のつくる磁界に
よって誘起される誘導電流の流路が制限されるために、
誘導電流およびそれによって生じる変動磁界も低減され
る。
Further, even when the superconducting coil 1 and the shield plate 2 vibrate relative to each other, the flow path of the induced current induced by the magnetic field generated by the superconducting coil 1 is limited,
The induced current and the varying magnetic field produced thereby are also reduced.

【0020】本発明により、シールド板と超電導コイル
の相対振動によって超電導コイルに誘導電流が発生し、
超電導コイル内での発熱となることを抑制することがで
きる。本発明の他の実施例として図3に示すものについ
て説明する。
According to the present invention, an induced current is generated in the superconducting coil by the relative vibration of the shield plate and the superconducting coil,
It is possible to suppress heat generation in the superconducting coil. Another embodiment of the present invention will be described with reference to FIG.

【0021】シールド板2のうち超電導コイル1に対向
しない部分2bの導電率の低い材料の上に、誘導電流の流
路とならないように櫛形の形状にした良熱伝導材6を設
置する。
A comb-shaped good heat conductive material 6 is provided on a material having a low electric conductivity in a portion 2b of the shield plate 2 which does not face the superconducting coil 1 so as not to serve as a flow path for an induced current.

【0022】これは一般に、導電率の低い材料は熱伝導
率が低いため、シールド板2の該当部分の冷却が十分で
なく、超電導コイル1への輻射伝熱が増加するのを防止
するため良熱伝導材を追加したものである。この場合、
超電導コイルと対向する部分2aの導電率の高い材料と、
この良熱伝導材6とで閉ループ形成されると誘導電流の
流路となって効果が低減するため、閉ループが形成され
ないように良熱伝導材6を櫛形に設置することにより発
明の効果を低減することなく超電導コイル1への輻射伝
熱の増加を防止することになる。なお、一般に導電率の
高い材料は熱伝導率も大きいため、良熱伝導材6と導電
率の高い材料を同一材料として一体化することも可能で
ある。
In general, since a material having a low electric conductivity has a low thermal conductivity, the corresponding portion of the shield plate 2 is not sufficiently cooled and radiative heat transfer to the superconducting coil 1 is prevented from increasing. This is the addition of a heat conductive material. in this case,
A material having a high conductivity of the portion 2a facing the superconducting coil,
If a closed loop is formed with the good thermal conductive material 6, the effect becomes a flow path of an induced current, and the effect is reduced. Therefore, the effect of the invention is reduced by installing the good thermal conductive material 6 in a comb shape so that the closed loop is not formed. Without doing so, an increase in radiant heat transfer to the superconducting coil 1 can be prevented. Generally, a material having a high electrical conductivity also has a high thermal conductivity, so that the good thermal conductive material 6 and the material having a high electrical conductivity can be integrated as the same material.

【0023】[0023]

【発明の効果】本発明により、外部からの変動磁界によ
ってシールド板に誘起される誘導電流が低減され、シー
ルド板全体としての電磁力が減少し、またシールド板の
剛性が高められることによってシールド板や超電導コイ
ルの振動が低減できる。さらにシールド板と超電導コイ
ルが相対振動した場合にも、誘導電流の流路を制限する
ことによって誘導電流およびそれによって生じる変動磁
界を低減し、超電導コイル内での発熱を抑制して超電導
導体を安定的に冷却して、安全性の高い超電導磁石を提
供できる。
According to the present invention, the induced current induced in the shield plate by the fluctuating magnetic field from the outside is reduced, the electromagnetic force of the shield plate as a whole is reduced, and the rigidity of the shield plate is enhanced, whereby the shield plate is increased. Vibration of the superconducting coil can be reduced. Even when the shield plate and the superconducting coil oscillate relative to each other, the flow path of the induced current is limited to reduce the induced current and the fluctuating magnetic field generated by it, thereby suppressing heat generation in the superconducting coil and stabilizing the superconducting conductor. It is possible to provide a highly safe superconducting magnet by cooling the material.

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

【図1】本発明による超電導磁石の断面図である。FIG. 1 is a sectional view of a superconducting magnet according to the present invention.

【図2】図1の部分詳細による磁気シールド作用説明図
である。
FIG. 2 is an explanatory view of a magnetic shield action according to a detail of FIG.

【図3】本発明の他の実施例によるシールド板の斜視図
である。
FIG. 3 is a perspective view of a shield plate according to another embodiment of the present invention.

【図4】従来例の超電導磁石の斜視図である。FIG. 4 is a perspective view of a conventional superconducting magnet.

【図5】図4のVーV線矢視図である。5 is a view taken along the line VV of FIG.

【符号の説明】[Explanation of symbols]

1…超電導コイル 2…シールド板 2a…超電導コイルと対向する部分 2b…超電導コイルと対向しない部分 3…真空容器 5…外部からの変動磁界の侵入方向 6…良熱伝導材 7…接合部 DESCRIPTION OF SYMBOLS 1 ... Superconducting coil 2 ... Shield plate 2a ... Portion facing the superconducting coil 2b ... Portion not facing the superconducting coil 3 ... Vacuum container 5 ... Direction of influx of fluctuating magnetic field from the outside 6 ... Good thermal conductive material 7 ... Joined portion

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】 真空容器、シールド板、超電導コイルか
ら成る超電導磁石において、 前記シールド板を、超電導コイルと対向する部分を導電
率の高い材料で、他の部分をこれより導電率の低い材料
で形成したことを特徴とする超電導磁石。
1. A superconducting magnet comprising a vacuum container, a shield plate, and a superconducting coil, wherein the shield plate is made of a material having a high electrical conductivity at a portion facing the superconducting coil and a material having a lower electrical conductivity than the other portion. A superconducting magnet characterized by being formed.
【請求項2】 導電率の低い材料として高剛性の高強度
ステンレス材料を用いた請求項1記載の超電導磁石。
2. The superconducting magnet according to claim 1, wherein a high-strength and high-strength stainless material is used as the material having a low electric conductivity.
【請求項3】 シールド板の導電率の低い材料の上に、
誘導電流の流路を形成しないような形状の良熱伝導材を
形成した請求項1又は請求項2記載の超電導磁石。
3. A material having a low electrical conductivity for the shield plate,
The superconducting magnet according to claim 1 or 2, wherein a good heat conductive material having a shape that does not form a flow path of an induced current is formed.
JP4062808A 1992-03-19 1992-03-19 Superconducting magnet Pending JPH05267725A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP4062808A JPH05267725A (en) 1992-03-19 1992-03-19 Superconducting magnet

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP4062808A JPH05267725A (en) 1992-03-19 1992-03-19 Superconducting magnet

Publications (1)

Publication Number Publication Date
JPH05267725A true JPH05267725A (en) 1993-10-15

Family

ID=13211014

Family Applications (1)

Application Number Title Priority Date Filing Date
JP4062808A Pending JPH05267725A (en) 1992-03-19 1992-03-19 Superconducting magnet

Country Status (1)

Country Link
JP (1) JPH05267725A (en)

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