JPS62232106A - Superconducting electromagnet - Google Patents
Superconducting electromagnetInfo
- Publication number
- JPS62232106A JPS62232106A JP7607786A JP7607786A JPS62232106A JP S62232106 A JPS62232106 A JP S62232106A JP 7607786 A JP7607786 A JP 7607786A JP 7607786 A JP7607786 A JP 7607786A JP S62232106 A JPS62232106 A JP S62232106A
- Authority
- JP
- Japan
- Prior art keywords
- hole
- electromagnet
- magnetic field
- pipe
- cryostat
- 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
Links
- 239000000463 material Substances 0.000 claims abstract description 6
- 230000002093 peripheral effect Effects 0.000 claims description 6
- 239000013078 crystal Substances 0.000 description 6
- 230000000694 effects Effects 0.000 description 3
- 238000010899 nucleation Methods 0.000 description 2
- VYPSYNLAJGMNEJ-UHFFFAOYSA-N Silicium dioxide Chemical compound O=[Si]=O VYPSYNLAJGMNEJ-UHFFFAOYSA-N 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 238000002425 crystallisation Methods 0.000 description 1
- 230000008025 crystallization Effects 0.000 description 1
- 230000008020 evaporation Effects 0.000 description 1
- 238000001704 evaporation Methods 0.000 description 1
- 230000004907 flux Effects 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 238000003780 insertion Methods 0.000 description 1
- 230000037431 insertion Effects 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 238000000034 method Methods 0.000 description 1
- 231100000989 no adverse effect Toxicity 0.000 description 1
- 239000003507 refrigerant Substances 0.000 description 1
- 230000000007 visual effect Effects 0.000 description 1
Landscapes
- Magnetic Resonance Imaging Apparatus (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〕
この発明は、高磁場発生用の超電導電磁石、詳しくは、
対象物に対する磁場の印加を容易にするため、鞍形のコ
イルを採用し、クライオスタットを含めた全体の端面視
形状を略半円形又はU字形となした電磁石の改善策に関
する。[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a superconducting electromagnet for generating a high magnetic field, specifically,
The present invention relates to an improvement in an electromagnet that employs a saddle-shaped coil and has a generally semicircular or U-shaped end view including the cryostat in order to facilitate the application of a magnetic field to an object.
周知のソレノイド型コイルを使って、磁場印加対象物(
以下では単に対象物と云う)に磁場を印加する方法は、
?「磁石の使用制限がきつく、また、発生磁場を効率良
く利用し得ないケースも生じてくることから、本発明者
等は、その問題解決策として、馬に鞍を跨がせるように
して対象物の周りに配置でき、また、−軸方向に長い対
象物であっても1台の電磁石による磁場の印加が行え、
しかも、常に磁束密度の最も高い磁場空間部に対象物を
おくことのできる超電導磁石を開発して最近特許出願し
た。その電磁石を第3図及び第5図(こ示す。A well-known solenoid coil is used to apply a magnetic field to the object (
The method of applying a magnetic field to an object (hereinafter referred to simply as an object) is as follows:
? ``There are strict restrictions on the use of magnets, and there are cases where the generated magnetic field cannot be used efficiently, so as a solution to this problem, the inventors of the present invention designed the object by having the horse straddle the saddle. It can be placed around objects, and a single electromagnet can apply a magnetic field even to objects that are long in the -axis direction.
Furthermore, they have recently applied for a patent for a superconducting magnet that allows objects to be placed in the magnetic field space where the magnetic flux density is highest. The electromagnet is shown in FIGS. 3 and 5.
第3図の電磁石は、第4図に示すように、端面視が略半
円形のベース板1上に鞍形のコイル2を跨がせ、これを
、内容器3が断熱層4を介して外容器5に囲まれた構造
の端面1M、1賂半円形のクライオスタットb内に、コ
イル冷却用寒剤(一般には液体ヘリウム)と共に収納し
た構造である。As shown in FIG. 4, the electromagnet shown in FIG. It has a structure in which a cryostat (generally liquid helium) for cooling the coil is housed in a semicircular cryostat b with an end face 1M surrounded by an outer container 5.
一方、第5図の電磁石は、鞍形コイルを跨がせるベース
板1を端面視U字形となし、このベース板上に定置され
る鞍形コイルを、ベース板と同様に端面視がU字形をな
すクライオスタット6内に寒剤と共に収めた構造である
。なお、いずれの電磁石も、内容器3の曲率半径の小さ
い側の周壁3aは、ベース板1によって形成しであるが
、ベース板と相似形の他の壁材で形成してその上にベー
ス板を跨がせて固定することもある。On the other hand, in the electromagnet shown in FIG. 5, the base plate 1 that straddles the saddle-shaped coil has a U-shape when viewed from the end, and the saddle-shaped coil placed on the base plate has a U-shape when viewed from the end like the base plate. It has a structure in which it is housed together with a cryogen in a cryostat 6 that forms a In both electromagnets, the peripheral wall 3a of the inner container 3 on the side with a smaller radius of curvature is formed by the base plate 1, but it is formed from another wall material having a similar shape to the base plate, and a base plate is placed on top of it. Sometimes it is fixed by straddling it.
上述の電磁石は、クライオスタットの外壁部に生じた四
部7内に対象物Aを配置して磁場を印加するが、電磁石
を図のように横向きに使用する際には、その上部側から
、一方、電磁石を図の状態から端面が水平になるように
90°回転させて縦向きに使用する際にはその正面側か
ら(いずれも図のX点側から)対象物を観察しようとし
ても、観察点が電磁石に遮えぎられているため、それが
できず、目視やTVカメラ等による磁場の印加状況観測
等に支障をきたすと云う問題がありた。In the above-mentioned electromagnet, a magnetic field is applied by placing the object A within the four parts 7 formed on the outer wall of the cryostat, but when the electromagnet is used horizontally as shown in the figure, from the upper side, When the electromagnet is rotated 90 degrees from the state shown in the figure so that the end face is horizontal and used vertically, even if you try to observe the object from the front side (in both cases from the X point side in the figure), the observation point Since the magnetic field is blocked by the electromagnet, this cannot be done, which poses a problem in that it interferes with visual observation or observation of the applied state of the magnetic field using a TV camera or the like.
この発明は、か\る問題点を解決することを目的として
いる。This invention aims to solve these problems.
この発明は、上述の問題点を無く丁ため、鞍形コイルを
使用し、さらにクライオスタットを含めた全体の端面視
形状を略半円形又はU字形となした上述の超電導電磁石
に対し、コイル線材の存在しない電磁石中央部に、磁場
の印加部をクライオスタットの外壁の途中に開放させる
貫通孔を設け、その孔を透して対象物を電磁石の周囲か
ら観察し得るようにしたのである。In order to eliminate the above-mentioned problems, the present invention uses a saddle-shaped coil and has a substantially semicircular or U-shaped end view shape as a whole including the cryostat. In the center of the electromagnet, which does not exist, a through hole was provided to allow the magnetic field application part to be opened halfway through the outer wall of the cryostat, allowing the object to be observed from around the electromagnet through the hole.
第1図及び第2図に、この発明の超電導電磁石の一例を
示す。この電磁石は、鞍形コイル2を跨がせるベース板
とクライオスタット6とを端面規格半円形に形成した第
3図の電磁石を改善したものであって、貫通孔8は、コ
イル線材の存在しない電磁石中央部に、一端が外容器5
の曲率半径の小さい周壁5aから四部7に開放し、他端
が外容器5の曲率半径の大きい周壁5bから四部7とは
反対側にある空間に開放する向きに設けられている。FIGS. 1 and 2 show an example of a superconducting electromagnet of the present invention. This electromagnet is an improved version of the electromagnet shown in FIG. 3 in which the base plate that straddles the saddle-shaped coil 2 and the cryostat 6 are formed into semicircular end faces. In the center, one end is the outer container 5
The peripheral wall 5a having a small radius of curvature opens to the fourth part 7, and the other end opens from the peripheral wall 5b of the outer container 5 having a large radius of curvature to a space on the opposite side to the fourth part 7.
上記貫通孔8は、周壁5a、5b間にパイプ9を気密に
固定し、そのパイプの途中に内容器3のバイブ挿入穴縁
部を気密に接続する構造として作り出してもよいが、こ
の場合、パイプ9のみを介して寒剤を収納した内容器3
の内室が大気に接し、外部熱の侵入による寒剤の蒸発損
失が増加するので、図のように、パイプ9の外周に、内
容器3の周壁3a、3bに対して気密に固定されるパイ
プ10を配置し、両パイプ9.10間に、断熱層4に連
続した断熱層4′を介在するのが望ましい。The through hole 8 may be created by airtightly fixing the pipe 9 between the peripheral walls 5a and 5b, and airtightly connecting the edge of the vibrator insertion hole of the inner container 3 in the middle of the pipe, but in this case, Inner container 3 containing cryogen only through pipe 9
Since the inner chamber of the inner chamber is in contact with the atmosphere and the evaporation loss of the refrigerant increases due to the intrusion of external heat, the pipe is fixed airtight to the outer circumference of the pipe 9 to the peripheral walls 3a and 3b of the inner container 3, as shown in the figure. 10, and a heat insulating layer 4' continuous to the heat insulating layer 4 is preferably interposed between both pipes 9 and 10.
なお、貫通孔8の形状は特に限定されない。対象物の大
きさ、形状に照らして観察し易い形状に丁ればよい。Note that the shape of the through hole 8 is not particularly limited. It is sufficient if the shape is easy to observe in light of the size and shape of the object.
第5図の電磁石に対しても同一構造を採用して貫通孔を
設けることができるので、その実施例は特に挙げない。Since the same structure can be adopted for the electromagnet shown in FIG. 5 and a through hole can be provided therein, a specific example thereof will not be mentioned.
以上、述べたように、この発明の電磁石は、コイル線材
の存在しない中央部に貫通孔を設けたので、対象物に対
する磁場の印加状況を観察しながら、印加制御等を行う
ことが可能になると云う効果が得られ、その効果により
、単結晶成長装置等では、特に多大の利点がもたらされ
る。As mentioned above, since the electromagnet of the present invention has a through hole in the central part where the coil wire is not present, it is possible to control the magnetic field application while observing the application status of the magnetic field to the object. The above effect can be obtained, and this effect brings particularly great advantages to single crystal growth apparatuses and the like.
即ち、単結晶製造時には、結晶成長炉内の融解した結晶
材料に磁場を印加して、その材料の対誠をなくてことが
行われているが、この単結晶成長時のように種付けが必
要な場合、或いは成長状況の観察が必要な場合には、目
視やTVカメラによる内部観察が必須である。しかしな
がら、7に磁石に貫通孔がなければ、その観察を行えな
いケークが生じてくる。また、単結晶成長装置の場合、
石英ガラス等で構成される結晶炉の内部を、電磁石に邪
魔されない斜め外側からは目視したり、TVカメラで観
察したりてることが考えられるが、斜視像は歪みがでる
ため、正確な種付けや磁場の印加制御に悪影響を及ばず
。In other words, when producing a single crystal, a magnetic field is applied to the molten crystal material in a crystal growth furnace to eliminate the polarity of the material, but seeding is required as in the case of single crystal growth. In such cases, or when it is necessary to observe the growth status, internal observation with the naked eye or a TV camera is essential. However, if the magnet 7 does not have a through hole, there will be cases where observation cannot be performed. In addition, in the case of single crystal growth equipment,
It is conceivable that the inside of a crystallization furnace made of quartz glass or the like can be visually observed from an oblique outside where it is not disturbed by electromagnets, or observed with a TV camera, but since the oblique image is distorted, it is difficult to ensure accurate seeding. No adverse effect on magnetic field application control.
これに対し、この発明の電磁石を使用でれば、磁場印加
部を貫通孔を透して直角方向から観察でき、上述の如き
不都合が一掃される。On the other hand, if the electromagnet of the present invention is used, the magnetic field applying section can be observed from the perpendicular direction through the through hole, and the above-mentioned disadvantages can be eliminated.
第11QIは、この発明の超電導電磁石の一例を示す断
面図、第2図はその平面図、第3図乃至第6図は、本出
願人が先(こ特許出願した電磁石の断面図とそのコイル
の斜視図である。11QI is a sectional view showing an example of the superconducting electromagnet of the present invention, FIG. 2 is a plan view thereof, and FIGS. FIG.
Claims (1)
形コイルを跨がせ、このコイルを、断熱層を介して外容
器に囲まれた内容器の周壁の一部が上記ベース板又はそ
れと相似形の壁材によつて形成される端面視略半円形又
はU字形のクライオスタット内に収納した超電導電磁石
において、コイル線材の存在しない電磁石中央部に、磁
場の印加部をクライオスタットの外壁の途中に開放させ
る貫通孔を設けたことを特徴とする超電導電磁石。A saddle-shaped coil is placed over a base plate having a substantially semicircular or U-shaped end view, and this coil is surrounded by an outer container via a heat insulating layer, and a part of the peripheral wall of the inner container is connected to the base plate. Alternatively, in a superconducting electromagnet housed in a cryostat that is approximately semicircular or U-shaped in end view and formed by wall materials of a similar shape, the magnetic field application part is placed in the center of the electromagnet where no coil wire is present, and the magnetic field application part is placed on the outer wall of the cryostat. A superconducting electromagnet characterized by having a through hole that opens in the middle.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7607786A JPS62232106A (en) | 1986-03-31 | 1986-03-31 | Superconducting electromagnet |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP7607786A JPS62232106A (en) | 1986-03-31 | 1986-03-31 | Superconducting electromagnet |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS62232106A true JPS62232106A (en) | 1987-10-12 |
Family
ID=13594744
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP7607786A Pending JPS62232106A (en) | 1986-03-31 | 1986-03-31 | Superconducting electromagnet |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS62232106A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2017098504A (en) * | 2015-11-27 | 2017-06-01 | 株式会社東芝 | High-temperature superconducting coil, high-temperature superconducting magnet, and method of manufacturing high-temperature superconducting coil |
-
1986
- 1986-03-31 JP JP7607786A patent/JPS62232106A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2017098504A (en) * | 2015-11-27 | 2017-06-01 | 株式会社東芝 | High-temperature superconducting coil, high-temperature superconducting magnet, and method of manufacturing high-temperature superconducting coil |
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