JPH02237101A - Superconducting magnetic-field utilization apparatus - Google Patents
Superconducting magnetic-field utilization apparatusInfo
- Publication number
- JPH02237101A JPH02237101A JP1058410A JP5841089A JPH02237101A JP H02237101 A JPH02237101 A JP H02237101A JP 1058410 A JP1058410 A JP 1058410A JP 5841089 A JP5841089 A JP 5841089A JP H02237101 A JPH02237101 A JP H02237101A
- Authority
- JP
- Japan
- Prior art keywords
- superconducting coils
- superconducting
- pair
- internal support
- 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.)
- Granted
Links
- 238000007789 sealing Methods 0.000 claims description 6
- 230000004907 flux Effects 0.000 claims 1
- 238000000034 method Methods 0.000 abstract description 6
- 230000009545 invasion Effects 0.000 abstract 1
- 239000001307 helium Substances 0.000 description 6
- 229910052734 helium Inorganic materials 0.000 description 6
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 6
- 239000007788 liquid Substances 0.000 description 5
- 230000007935 neutral effect Effects 0.000 description 5
- 230000005494 condensation Effects 0.000 description 3
- 238000009833 condensation Methods 0.000 description 3
- IJGRMHOSHXDMSA-UHFFFAOYSA-N Atomic nitrogen Chemical compound N#N IJGRMHOSHXDMSA-UHFFFAOYSA-N 0.000 description 2
- 230000005469 synchrotron radiation Effects 0.000 description 2
- 238000013459 approach Methods 0.000 description 1
- 239000003795 chemical substances by application Substances 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 230000000694 effects Effects 0.000 description 1
- 238000007710 freezing Methods 0.000 description 1
- 230000008014 freezing Effects 0.000 description 1
- 230000012447 hatching Effects 0.000 description 1
- 238000010438 heat treatment Methods 0.000 description 1
- 230000008595 infiltration Effects 0.000 description 1
- 238000001764 infiltration Methods 0.000 description 1
- 238000012423 maintenance Methods 0.000 description 1
- 238000012986 modification Methods 0.000 description 1
- 230000004048 modification Effects 0.000 description 1
- 229910052757 nitrogen Inorganic materials 0.000 description 1
- 238000000926 separation method Methods 0.000 description 1
Landscapes
- Particle Accelerators (AREA)
- Containers, Films, And Cooling For Superconductive Devices (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は超電導磁場利用装置に関し、特に極低温に維持
した超電導コイルを極低温に保ったまま、磁極間の磁場
利用空間を画定する容器を外部に取り出すことのできる
超電導磁場利用装置に関する.以下、主として放射光を
発生させる電子蓄積リングを例として説明する.
[従来の技術]
電子蓄積リング(SOR)は加速した電子を強磁場中に
閉じ込め、回転運動をさせることによって放射光を発生
させる.この加速電子を閉じこめるための強磁場形成に
超電導マグネットが用いられる.超電導マグネットは、
極低温に冷却された超電導コイルを含む.
第2図に従来の電子蓄積リングの代表的構造を概略的に
示す.上超電導コイル51と下超電導コイル52とはへ
ルムホルツコイル型に同軸に向い合って配置されている
.上超電導コイル51に囲まれな領域内に環状の上磁極
53か配置され、対称的に下超電導コイル52に囲まれ
た領域内に環状の下磁極54が配置されている.両磁極
53、54間に磁場によって周回軌道を描く電子を蓄積
するための環状の真空容器55が配置されている.ヨー
ク57が上超電導コイル51と下超電導コイル52とを
外側から取り囲み、さらに上下から上磁極53、下磁極
54を挾むように延在して磁気回路を形成している.
上超電導コイル51、下超電導コイル52に電流を流す
と両超電導コイル間に強い吸引力が助<,そこで、両超
電導コイルと対抗する物理的な支持構造が必要である.
一方、真空容器55は必要に応じて外部に取り出し、整
備、設定変更等を行う必要がある.まず、上下超電導コ
イル51、52間に働く力を支持するには、両超電導コ
イル51、52間に物理的支持部材を配置するのが好ま
しい.そこで、第3図(A)、(B)、に示すように内
部支持ロッド58a、58bを用いて、上下超電導コイ
ル51、52を少なくとも数箇所で直接連結することが
望ましい.しかし、この構造では真空容器55を外部に
取り出すことができない.真空容器55を外に取り出せ
るようにするには、第4図に示すように、ヨーク57を
水平中立面56で分割することが望ましい.上側の超電
導コイル51とヨーク57aを持上げることにより真空
容器55を取り出すことができる.しかし、この方法で
は超電導コイル51、52の外部支持ロツド59からの
熱の侵入が大きく、ヘリウムの消費量が大きくなる.
このような事情は、電子蓄積装置に瀬らず、超電導磁場
利用装置に広く存在する.
[発明が解決しようとする課題]
以上説明したように、従来技術によれば、1対の超電導
コイル51、52間を物理的に支持すると、磁極53、
54間の真空容器55が容易に取り出せず、真空容器5
5が取り出し易いようにヨーク57を2分し、外部支持
部材59によって各ヨーク57a、57bに超電導コイ
ル51、52を支持すると、外部支持部材59からの熱
侵入が大きくなり、液体ヘリウムの消費が増大する間U
があった。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a superconducting magnetic field utilization device, and in particular to a superconducting coil maintained at an extremely low temperature and a container that defines a magnetic field utilization space between magnetic poles. This article relates to a superconducting magnetic field utilization device that can be taken out to the outside. Below, we will mainly explain an electron storage ring that generates synchrotron radiation as an example. [Prior Art] An electron storage ring (SOR) confines accelerated electrons in a strong magnetic field and generates synchrotron radiation by rotating them. A superconducting magnet is used to create a strong magnetic field to confine these accelerated electrons. Superconducting magnets are
Contains superconducting coils cooled to extremely low temperatures. Figure 2 schematically shows the typical structure of a conventional electron storage ring. The upper superconducting coil 51 and the lower superconducting coil 52 are arranged coaxially and facing each other in a Helmholtz coil type. An annular upper magnetic pole 53 is arranged in an area surrounded by the upper superconducting coil 51, and an annular lower magnetic pole 54 is symmetrically arranged in an area surrounded by the lower superconducting coil 52. An annular vacuum container 55 is disposed between the magnetic poles 53 and 54 to store electrons orbiting in a magnetic field. A yoke 57 surrounds the upper superconducting coil 51 and the lower superconducting coil 52 from the outside, and further extends to sandwich the upper magnetic pole 53 and the lower magnetic pole 54 from above and below, forming a magnetic circuit. When a current is passed through the upper superconducting coil 51 and the lower superconducting coil 52, a strong attractive force is created between the two superconducting coils.Therefore, a physical support structure is required to oppose the two superconducting coils. On the other hand, it is necessary to take the vacuum container 55 out to perform maintenance, change settings, etc., as necessary. First, in order to support the force acting between the upper and lower superconducting coils 51 and 52, it is preferable to arrange a physical support member between both the superconducting coils 51 and 52. Therefore, as shown in FIGS. 3A and 3B, it is desirable to directly connect the upper and lower superconducting coils 51 and 52 at at least several locations using internal support rods 58a and 58b. However, with this structure, the vacuum container 55 cannot be taken out. In order to be able to take out the vacuum container 55, it is desirable to divide the yoke 57 at a horizontal neutral plane 56, as shown in FIG. The vacuum container 55 can be taken out by lifting the upper superconducting coil 51 and yoke 57a. However, in this method, a large amount of heat enters from the external support rod 59 of the superconducting coils 51 and 52, and the amount of helium consumed becomes large. This situation exists not only in electron storage devices, but also in devices that utilize superconducting magnetic fields. [Problems to be Solved by the Invention] As explained above, according to the prior art, when the pair of superconducting coils 51 and 52 are physically supported, the magnetic poles 53,
The vacuum container 55 between the vacuum containers 54 and 54 cannot be easily removed.
If the yoke 57 is divided into two to make it easier to take out the superconducting coils 51 and 52, and the superconducting coils 51 and 52 are supported on each yoke 57a and 57b by the external support member 59, heat infiltration from the external support member 59 increases and the consumption of liquid helium is reduced. While increasing
was there.
本発明の目的は、真空容器の取出しが容易でかつ外部か
ら超電導コイルへの支持部材を熱侵入の小さいものにす
ることができる超電導磁場利用装置を提供することであ
る.
[課題を解決するための手段〕
1対の超電導コイル間に内部支持部材を設け、この内部
支持部材を分割可能な構成とし、さらに各超電導コイル
に対して気密容器を形成できる気密部材を備える.
さらに、内部支持部材を超電導コイルからも分割可能な
構成としてもよい.
第1図(A)、(B)を参照して本発明の基本概念を説
明する.(A》が全体の断面図、(B)が超電導コイル
切離し時の部分断面図である.1対の超電導コイル1、
2が1対の磁極3、4を取り巻き、磁極3、4間に磁場
を発生させる.真空容器5がこの磁場中に置かれ、この
内部で電子を蓄積すること等に磁場を利用する.超電導
コイル1、2は液体ヘリウムを用いて極低温に冷却され
る.但し、極低温冷却用の液体ヘリウム、液体窒素のシ
ステム系統は図示していない.上ヨーク7、下ヨーク8
はそれぞれ上磁極3、下磁極4に連続し、水平中立面6
で互いに接触して磁気回路を横成する.上超電導コイル
1、下超電導コイル2の間には上、下内部支持部材9、
10が設けられ、両超電導コイル1、2に電流を流し、
吸引力が働いた時に、その吸引力に対向して両超電導コ
イル1、2を支持する.この内部支持部材9、106使
用時には極低温になる.これら極低温になる部分を囲ん
でクライオスタットゲース14、15が設けられている
.このクライオスタットケースは両超電導コイル1、2
に対応して上クライオスタットケース部14と下クライ
オスタットゲース部15に分離できる.超電導コイル1
、2はまた位置決め部材16、17によってヨーク7、
8に支持され、その位置を定めている.
クライオスタットケースを分離した時に、内部支持部材
9、10も分離し、さらに上下内部支持部材9、10か
ら張り出した第2シール部材20、21が上、下クライ
オスタットゲース部14、15から張り出しな第1シー
ル部材18、19とそれぞれ係合し、上下別個に気密真
空容器を形成できる.
第1図(B)に上側を示すように、さらに超電導コイル
1を引上げることにより、超電導コイル1と内部支持部
材9も切り離され、内部支持部材9は極低温から分離さ
れる.なお、下側も同様である.
[作用]
まず装置を組立てた使用時は、超電導コイル1、2間に
内部支持部材9、10が挿入されて超電導コイル1、2
間の吸引力に対して物理的支持を与えている.このなめ
超電導コイル1、2とヨークとの間の位置決め部材(外
部支持部材)16、17は熱伝導の小さい断面積の小さ
なもので足りる.このため、外部より極低温部への熱の
流入を低減できる.
上、下ヨーク7、8が分離でき、ヨーク分離と共に上下
超電導コイル1、2も分離できるので真空容器5の取り
出しが容易である.
さらに、内部支持部材9、10が超電導コイル1、2と
の係合を解除できる構成を持つときは、分^【時の極低
温部への熱の流入をさらに低減できる.
[実施例コ
第5、6、7図を参照して、本発明の実施例を説明する
.
第5図は、第1図に示すような超電導磁場利用装置の部
分断面図である.
上磁極3と下磁極4どの間に真空容器5が配置されてい
る.上磁極3、4間を、水平中立面6で接続した上ヨー
ク7と下ヨーク8が磁気回路的に接続している.上、下
ヨーク7、8及び真空容器5を貫いて上、下超電導コイ
ルユニット29、30が配置されている.
上超電導コイル1はコイルゲース23内に密封され、液
体ヘリウムで冷却されている.上下のコイルユニット2
9、30はほぼ対称的な構成を有する.ここでは上側の
コイルユニット29について説明する.コイルケース2
3の上には位置決め部材である外部支持ロッド16aが
収り付けられ上端で上ヨーク7に固定される.コイルケ
ース23の下には内部支持部材である内部支持ロッド9
aが取り付けられ、装置の水平中立面6で下コイルユニ
ット30の内部支持ロッドlOa(図示せず)と接触し
ている.通電時に上下コイル1、2に働く吸引力は内部
支持ロツド9a、10aで受け持ち、外部支持ロヅドi
6aは上コイルユニット29を上ヨーク7に固定するた
めのもので支持力は小さい.
内部支持ロッド9aとコイルケース23との間の係合部
には、コンタクトフィンガ31が設けられている.完全
な係合を達成する前にコンタクトフィンガを介して部分
的な熱的、ないし機械的係合を行う.
コイルゲース23の周囲には熱シールド板25が取り付
けられ、その外側の上クライオスタットケース14から
の熱侵入を小さくする作用をする.1層で図示するが、
温度の異なる複数の層で楕成するのが好ましい.
外部支持ロッド16aの上端には調整機構が取り付けら
れ、コイルケース23を上クライオスタットゲース14
に対し、相対的に上下できる,内部支持ロツド9aには
、第6図の部分拡大図に示すようにシール部材であるバ
ルブプレート20aが取り付けられバネ33でコイルケ
ース23に引き付けられている.上クライオスタットケ
ース14には対応する位置にシール部材であるバルブシ
一ト18aが取り付けられている.バルブグレート20
aとバルブシ一ト18aとが係合すると気密状態を保つ
バルブが構成される.同様に、下側には、バルブプレー
ト40とバルブシ一ト38が設けられ、バルブを構成す
る.上クライオスタットゲース14の下面当接部にはフ
ランジ37が形成され、下クライオスタットケースのフ
ランジとの間でOリングを利用して真空を保つ梢成を有
しているや
図示の場合、内部支持ロツド9aを取り囲むクライオス
タットゲース14は真空容器5に設けた連結用の孔39
に入っている.真空容器に設ける孔39は、例えば第7
図の平面図に示すように均等に分布した6箇所に設ける
.電子は矢印で示す方向から入射し、破線で示す軌道を
回る.この軌道経路上のハッチングで示す領域に各種機
器が設置される.前述の孔39はこのハッチング領域を
避けて決定される.この孔は外縁に対し切欠かれた孔で
もよい.また真空容器の外径を小さくすることが可能な
ら切欠きも孔も不要である.第6図に示すように、支持
ロッド9aの下端面に近い所にヒータと温度センサ27
が取り付けられている.極低温であった内部支持ロッド
9aを外気に露出するとき結露防止のため加熱するため
である.
第5〜7図に示す構成は、磁気回路が上下対称的な構造
で構成され、中央部で上下に分離できる.分離時にも超
電導コイルを極低温に維持できるので、ヘリウムの消費
を節約すると共に真空容器取り付け後の操作開始までの
時間を短縮できる.以下に真空容器5の取出し、組込み
の手順を簡単に説明する.
真空容器5を外部に取出す場合の手順は以下のようであ
る.
1,外部支持ロッド16を上部のn整機構を用いて上側
に引上げる.この操作により内部支持ロッド9aに取り
付けられたバルプグレート20a《第6図》はバルブシ
一ト18aに押し付けられる.これで上クライオスタッ
トゲース14fflに気密真空容器が形成される.
2.外部支持ロッド16aをさらに引上げるとコイルゲ
ース23と内部支持ロツド9aとが分離し、バネ33で
互いに引合う状態になる.すなわち内部支持ロッド9a
が極低温から分講tされる.3.ヒータ27で内部支持
ロッド9a下部を加熱し、室温に戻す.これで外気が触
れても結露しない状態になる.
4,上記操作を下側コイルユニットにも同様の手順で行
う.両バルブグレート20a、40はバルブシ一ト18
a、38と係合し、中間にバッファ空間43を作る.
5.リーク弁35を開き、バッファ空間43を大気圧に
する.
6.上ヨーク7を持上げ真空容器5を取出す.真空容器
を取込む場合の手段は以下のようである.
l.真空容器5を組込む。An object of the present invention is to provide a superconducting magnetic field utilization device in which a vacuum container can be easily taken out and a support member for supporting a superconducting coil from the outside can be made to have a small amount of heat intrusion. [Means for Solving the Problems] An internal support member is provided between a pair of superconducting coils, this internal support member is configured to be divisible, and an airtight member is provided to form an airtight container for each superconducting coil. Furthermore, the internal support member may also be configured to be separable from the superconducting coil. The basic concept of the present invention will be explained with reference to FIGS. 1(A) and 1(B). (A) is an overall cross-sectional view, and (B) is a partial cross-sectional view when the superconducting coils are separated. A pair of superconducting coils 1,
2 surrounds a pair of magnetic poles 3 and 4, and generates a magnetic field between the magnetic poles 3 and 4. A vacuum container 5 is placed in this magnetic field, and the magnetic field is used to accumulate electrons inside the container. Superconducting coils 1 and 2 are cooled to extremely low temperatures using liquid helium. However, the liquid helium and liquid nitrogen systems for cryogenic cooling are not shown. Upper yoke 7, lower yoke 8
are continuous with the upper magnetic pole 3 and the lower magnetic pole 4, respectively, and the horizontal neutral plane 6
contact each other to form a magnetic circuit. Between the upper superconducting coil 1 and the lower superconducting coil 2, there are upper and lower internal support members 9,
10 is provided, current is passed through both superconducting coils 1 and 2,
When an attractive force is applied, both superconducting coils 1 and 2 are supported in opposition to the attractive force. When these internal support members 9 and 106 are used, they become extremely cold. Cryostat gates 14 and 15 are provided surrounding these extremely low temperature parts. This cryostat case has both superconducting coils 1 and 2.
It can be separated into an upper cryostat case part 14 and a lower cryostat case part 15 correspondingly. Superconducting coil 1
, 2 is also connected to the yoke 7 by the positioning members 16, 17.
It is supported by 8 and determines its position. When the cryostat case is separated, the internal support members 9 and 10 are also separated, and the second seal members 20 and 21 that protrude from the upper and lower internal support members 9 and 10 are removed from the first seal members that protrude from the upper and lower cryostat case parts 14 and 15. By engaging with the sealing members 18 and 19, the upper and lower parts can form airtight vacuum containers separately. As shown on the upper side in FIG. 1(B), by further pulling up the superconducting coil 1, the superconducting coil 1 and the internal support member 9 are also separated, and the internal support member 9 is separated from the cryogenic temperature. The same applies to the lower side. [Function] First, when the device is assembled and used, the internal support members 9 and 10 are inserted between the superconducting coils 1 and 2, and the superconducting coils 1 and 2
It provides physical support to the attractive force between the two. The positioning members (external support members) 16 and 17 between the slanted superconducting coils 1 and 2 and the yoke need only have small cross-sectional areas with low thermal conductivity. Therefore, it is possible to reduce the inflow of heat from the outside into the cryogenic part. The upper and lower yokes 7 and 8 can be separated, and the upper and lower superconducting coils 1 and 2 can also be separated together with the yokes, making it easy to take out the vacuum vessel 5. Furthermore, when the internal support members 9 and 10 have a configuration that allows them to be disengaged from the superconducting coils 1 and 2, it is possible to further reduce the inflow of heat into the cryogenic region at the time of . [Embodiment] An embodiment of the present invention will be described with reference to FIGS. 5, 6, and 7. FIG. 5 is a partial cross-sectional view of the superconducting magnetic field utilization device shown in FIG. A vacuum container 5 is placed between the upper magnetic pole 3 and the lower magnetic pole 4. An upper yoke 7 and a lower yoke 8, which are connected by a horizontal neutral plane 6 between the upper magnetic poles 3 and 4, are connected in a magnetic circuit. Upper and lower superconducting coil units 29 and 30 are disposed passing through the upper and lower yokes 7 and 8 and the vacuum vessel 5. The upper superconducting coil 1 is sealed within a coil gate 23 and cooled with liquid helium. Upper and lower coil unit 2
9 and 30 have a nearly symmetrical configuration. Here, the upper coil unit 29 will be explained. coil case 2
An external support rod 16a, which is a positioning member, is housed above 3 and fixed to the upper yoke 7 at its upper end. An internal support rod 9 that is an internal support member is provided below the coil case 23.
a is attached and is in contact with the internal support rod lOa (not shown) of the lower coil unit 30 at the horizontal neutral plane 6 of the device. The attraction force acting on the upper and lower coils 1 and 2 when energized is handled by the internal support rods 9a and 10a, and the external support rod i
6a is for fixing the upper coil unit 29 to the upper yoke 7, and its supporting force is small. A contact finger 31 is provided at the engagement portion between the internal support rod 9a and the coil case 23. Perform partial thermal or mechanical engagement via contact fingers before achieving full engagement. A heat shield plate 25 is attached around the coil gauge 23, and serves to reduce heat intrusion from the upper cryostat case 14 on the outside. Although illustrated in one layer,
It is preferable to form an ellipse with multiple layers at different temperatures. An adjustment mechanism is attached to the upper end of the external support rod 16a to adjust the coil case 23 to the upper cryostat gauge 14.
On the other hand, a valve plate 20a, which is a sealing member, is attached to the internal support rod 9a, which can be moved up and down relatively, as shown in the partially enlarged view of FIG. 6, and is attracted to the coil case 23 by a spring 33. A valve seat 18a, which is a sealing member, is attached to the upper cryostat case 14 at a corresponding position. valve great 20
When a and the valve seat 18a are engaged, a valve that maintains an airtight state is formed. Similarly, a valve plate 40 and a valve seat 38 are provided on the lower side to constitute a valve. A flange 37 is formed on the lower surface abutting part of the upper cryostat case 14, and has a top structure that maintains a vacuum using an O-ring between it and the flange of the lower cryostat case. The cryostat gate 14 surrounding the 9a is connected to a connecting hole 39 provided in the vacuum container 5.
It's in. The hole 39 provided in the vacuum container is, for example, the seventh hole.
They are installed at six evenly distributed locations as shown in the plan view of the figure. Electrons enter from the direction shown by the arrow and orbit in the orbit shown by the dashed line. Various equipment will be installed in the area shown by hatching on this orbit route. The aforementioned hole 39 is determined avoiding this hatched area. This hole may be a hole cut into the outer edge. Furthermore, if it is possible to reduce the outer diameter of the vacuum container, there is no need for notches or holes. As shown in FIG. 6, a heater and a temperature sensor 27 are installed near the lower end surface of the support rod 9a.
is installed. This is to heat the internal support rod 9a, which was at an extremely low temperature, to prevent condensation when it is exposed to the outside air. In the configuration shown in FIGS. 5 to 7, the magnetic circuit has a vertically symmetrical structure, and can be separated into upper and lower parts at the center. The superconducting coil can be maintained at an extremely low temperature even during separation, which saves helium consumption and shortens the time it takes to start operation after installing the vacuum vessel. The procedure for removing and assembling the vacuum container 5 will be briefly explained below. The procedure for taking out the vacuum container 5 to the outside is as follows. 1. Pull the external support rod 16 upward using the adjustment mechanism at the top. By this operation, the valve grating 20a (Fig. 6) attached to the internal support rod 9a is pressed against the valve seat 18a. This forms an airtight vacuum vessel in the upper cryostat gauge 14ffl. 2. When the external support rod 16a is further pulled up, the coil gauge 23 and the internal support rod 9a are separated and pulled together by the spring 33. That is, the internal support rod 9a
will be lectured on from extremely low temperatures. 3. Heat the lower part of the internal support rod 9a with the heater 27 and return it to room temperature. This will prevent condensation even when exposed to outside air. 4. Repeat the above procedure for the lower coil unit as well. Both valve grades 20a and 40 are valve seats 18
a, 38 to create a buffer space 43 in the middle. 5. Open the leak valve 35 and bring the buffer space 43 to atmospheric pressure. 6. Lift the upper yoke 7 and take out the vacuum container 5. The method for importing a vacuum container is as follows. l. Assemble the vacuum container 5.
2.上ヨーク7を下げ、上クライオスタットゲース14
の7ランジ部37を下クライオスタットゲースの7ラン
ジ部と突合わせる.
3.バッファ空間43を真空排気する.4.外部支持口
γド16aを下げ、内部支持ロツド9aに取り付けたコ
ンタクトフィンガ31をコイルゲース32に接触させる
.さらに外部支持ロッド16aを下げるとバルブプレー
ト20aがバルブシ一ト18aから離れる.この際、内
部支持ロツド9aとコイルゲース23はコンタクトフィ
ンガ31を介して部分的に機械的および熱的に接触して
いる.
5.ヒータ27を切ると内部支持ロッド9aはコンタク
トフィンガ31とバネ33を経由して冷却される.温度
センサで温度を検知する
6.内部支持ロッド9aの温度がコイルケース23の温
度に近付いた時点で外部支持ロッド16aを最終位置ま
で押し下げる.
以上説明したように本実施例によれば、低温部と連結し
ている外部支持ロッド16aの荷重は小さいので断面を
小さくでき、外部からの熱侵入の少ない超電導コイルが
できる.内部支持ロッドが上下分割可能で、超電導コイ
ルを上下別個の気密真空容器に収容できるので、磁場利
用のための真空容器を容易に取り出せる。2. Lower the upper yoke 7 and lower the upper cryostat gauge 14.
Butt the 7-lunge part 37 of the lower cryostat gauge with the 7-lunge part of the lower cryostat gauge. 3. The buffer space 43 is evacuated. 4. The external support port γ rod 16a is lowered, and the contact finger 31 attached to the internal support rod 9a is brought into contact with the coil gauge 32. Further lowering the external support rod 16a causes the valve plate 20a to separate from the valve seat 18a. At this time, the internal support rod 9a and the coil gauge 23 are in partial mechanical and thermal contact via the contact fingers 31. 5. When the heater 27 is turned off, the internal support rod 9a is cooled via the contact finger 31 and the spring 33. 6. Detect the temperature with a temperature sensor. When the temperature of the internal support rod 9a approaches the temperature of the coil case 23, the external support rod 16a is pushed down to the final position. As explained above, according to this embodiment, the load on the external support rod 16a connected to the low temperature section is small, so the cross section can be made small, and a superconducting coil with little heat intrusion from the outside can be created. The internal support rod can be divided into upper and lower parts, and the superconducting coils can be housed in separate upper and lower airtight vacuum containers, so the vacuum containers for magnetic field utilization can be easily taken out.
さらに、コイルユニットの上下接合部を大気に露出する
場合、内部支持ロツド9aを極低温部と分離することに
より、内部支持ロッド9aからの熱侵入を小さくできる
.
内部支持ロツド9a端面にヒータを設け、加熱すること
により端面の結露、凍結を防止できる.以上、実施例に
沿って説明したが、本発明はこれらに制限されるもので
はない.たとえば、種々の変形、変更、組み合わせなど
が可能であることは当業者に自明であろう.
[発明の効果]
以上説明したように、本発明によればヨークを分割して
真空容器を容易に外部に取出せる構造としつつ、超電導
コイル間に支持部材を設けて吸引力を支持できる.
真空容器取出し時には、上、下超電導コイルを極低温に
保ったまま、分離された真空気密容器内に上、下超電導
コイルを独立別個に収納できる.Furthermore, when the upper and lower joints of the coil unit are exposed to the atmosphere, by separating the internal support rod 9a from the cryogenic part, it is possible to reduce heat intrusion from the internal support rod 9a. By providing a heater on the end face of the internal support rod 9a and heating it, dew condensation and freezing on the end face can be prevented. Although the embodiments have been described above, the present invention is not limited thereto. For example, it will be obvious to those skilled in the art that various modifications, changes, combinations, etc. are possible. [Effects of the Invention] As explained above, according to the present invention, the vacuum container can be easily taken out by dividing the yoke, and the suction force can be supported by providing a support member between the superconducting coils. When taking out the vacuum container, the upper and lower superconducting coils can be stored independently and separately in a separate vacuum-tight container while keeping the upper and lower superconducting coils at an extremely low temperature.
第1図(A)、(B)は本発明の基本概念を示し、(A
)は使用時の超電導磁場利用装置の模式断面図、(B)
は切M時の模式部分断面図、第2図、第3図(A)、(
B)、第4図は従来技術を説明するための超電導磁場利
用装置の模式断面図、
第5図は本発明の1実施例による超電導磁場利用装置を
示す断面図、
第6図は第5図の部分拡大図、
第7図は第5図に示す真空容器5の平面構造例を示す平
面図である.
図において、
1、2
3、4
7、8
9、10
9a
14、15
16、17
超電導コイル
磁極
真空容器
中立面
ヨーク
支持部材
内部支持ロツド
クライオスタットゲース
位置決め部材
16a
1 8、 19
20、21
29、 30
18a、 38
20a、40
外部支持ロツド
第1シール部材
第2シール部材
コイルケース
熱シールド板
ヒータ及び温度センサ
コイルユニット
コンタクトフィンガ
バネ
リーク弁
フランジ
バルブシ一ト
バルブプレート
孔
バッファ空間
上超電導コイル
下超電導コイル
上磁極
下磁極
真空容器
ヨーク
支持ロッド
復代理人1 (A) and (B) show the basic concept of the present invention, and (A
) is a schematic cross-sectional view of the superconducting magnetic field utilization device in use, (B)
are schematic partial cross-sectional views when cutting M, Fig. 2, Fig. 3 (A), (
B), FIG. 4 is a schematic cross-sectional view of a superconducting magnetic field utilizing device for explaining the prior art, FIG. 5 is a cross-sectional view showing a superconducting magnetic field utilizing device according to an embodiment of the present invention, and FIG. FIG. 7 is a plan view showing an example of the planar structure of the vacuum container 5 shown in FIG. In the figure: 1, 2 3, 4 7, 8 9, 10 9a 14, 15 16, 17 Superconducting coil magnetic pole Vacuum vessel neutral plane Yoke support member Internal support rod Cryostat gauge positioning member 16a 1 8, 19 20, 21 29 , 30 18a, 38 20a, 40 External support rod First sealing member Second sealing member Coil case Heat shield plate Heater and temperature sensor Coil unit Contact finger Spring Leak valve Flange Valve Seat Valve plate Hole Buffer space Upper superconducting coil Lower superconducting Coil upper magnetic pole lower magnetic pole vacuum vessel yoke support rod sub-agent
Claims (2)
器(5)内の少なくとも所定の領域に磁場を形成するた
めの1対の磁極(3、4)とこれら磁極間を磁気的に接
続するヨークとこれら磁極(3、4)を囲んで磁束を発
生するための1対の超電導コイル(1、2)とを有する
超電導磁場利用装置であって、 前記ヨークが各磁極(3、4)に接続する2つの部分(
7、8)に分離可能であり、 1端で前記1対の超電導コイル(1、2)に係合し、他
端で互いに係合して前記超電導コイル間に働く吸引力を
支持する1対の荷重支持部材(9、10)と、 前記1対の荷重支持部材(9、10)の各々とそれに隣
接する前記超電導コイル(1、2)の1方を取り囲む1
対のクライオスタットケース(14、15)であり、互
いに係合して1つの真空容器を作ると共に、別にそれぞ
れが気密シールを形成するための第1シール部材(18
、19)を有する1対のクライオスタットケース(14
、15)と、 前記1対の各荷重支持部材(9、10)の相互に係合す
る端部近傍から外に向かって形成され、前記第1シール
部材と係合して気密シールを形成するための第2シール
部材(20、21)と、 前記第1シール部材(18、19)間に形成され排気系
との接続及び外気のリークを行うための弁部材(35)
と を有する超電導磁場利用装置。(1). A container (5) that defines a space in which a magnetic field is used, a pair of magnetic poles (3, 4) for forming a magnetic field in at least a predetermined region within the container (5), and a yoke that magnetically connects these magnetic poles. and a pair of superconducting coils (1, 2) for generating magnetic flux surrounding these magnetic poles (3, 4), the yoke being connected to each magnetic pole (3, 4). Two parts (
7 and 8), one end of which engages with the pair of superconducting coils (1, 2), and the other end of which engages with each other to support the attraction force acting between the superconducting coils; load supporting members (9, 10); 1 surrounding each of the pair of load supporting members (9, 10) and one of the superconducting coils (1, 2) adjacent thereto;
A pair of cryostat cases (14, 15) that engage each other to form one vacuum vessel, and each separately have a first seal member (18) for forming an airtight seal.
, 19) with a pair of cryostat cases (14
, 15) formed outward from near the mutually engaging ends of each of the pair of load supporting members (9, 10) and engaging with the first sealing member to form an airtight seal. and a valve member (35) formed between the first seal member (18, 19) for connecting with the exhaust system and leaking outside air.
A superconducting magnetic field utilization device having
コイル(1,2)との係合を解除できる構成を有してい
る請求項1記載の超電動磁場利用装置。(2). The superelectric magnetic field utilizing device according to claim 1, wherein the load supporting member (9, 10) has a configuration that allows the engagement with the superconducting coil (1, 2) to be released.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1058410A JP2599988B2 (en) | 1989-03-10 | 1989-03-10 | Superconducting magnetic field utilization device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP1058410A JP2599988B2 (en) | 1989-03-10 | 1989-03-10 | Superconducting magnetic field utilization device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH02237101A true JPH02237101A (en) | 1990-09-19 |
| JP2599988B2 JP2599988B2 (en) | 1997-04-16 |
Family
ID=13083601
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP1058410A Expired - Lifetime JP2599988B2 (en) | 1989-03-10 | 1989-03-10 | Superconducting magnetic field utilization device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP2599988B2 (en) |
Cited By (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2014007150A (en) * | 2012-06-01 | 2014-01-16 | Sumitomo Heavy Ind Ltd | Cyclotron |
| EP2717276A3 (en) * | 2012-10-04 | 2014-09-24 | Tesla Engineering Limited | Magnet apparatus |
| WO2018180154A1 (en) * | 2017-03-28 | 2018-10-04 | 住友重機械工業株式会社 | Air-core-type cyclotron |
-
1989
- 1989-03-10 JP JP1058410A patent/JP2599988B2/en not_active Expired - Lifetime
Cited By (5)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2014007150A (en) * | 2012-06-01 | 2014-01-16 | Sumitomo Heavy Ind Ltd | Cyclotron |
| EP2717276A3 (en) * | 2012-10-04 | 2014-09-24 | Tesla Engineering Limited | Magnet apparatus |
| US9019054B2 (en) | 2012-10-04 | 2015-04-28 | Tesla Engineering Limited | Magnet apparatus |
| US9396856B2 (en) | 2012-10-04 | 2016-07-19 | Tesla Engineering Limited | Magnet apparatus |
| WO2018180154A1 (en) * | 2017-03-28 | 2018-10-04 | 住友重機械工業株式会社 | Air-core-type cyclotron |
Also Published As
| Publication number | Publication date |
|---|---|
| JP2599988B2 (en) | 1997-04-16 |
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