JPH07147496A - Superconductive magnetic shielding structure - Google Patents

Superconductive magnetic shielding structure

Info

Publication number
JPH07147496A
JPH07147496A JP5339120A JP33912093A JPH07147496A JP H07147496 A JPH07147496 A JP H07147496A JP 5339120 A JP5339120 A JP 5339120A JP 33912093 A JP33912093 A JP 33912093A JP H07147496 A JPH07147496 A JP H07147496A
Authority
JP
Japan
Prior art keywords
magnetic shield
superconducting
shield structure
opening
main body
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
JP5339120A
Other languages
Japanese (ja)
Inventor
Shinichi Shibuya
紳一 渋谷
Noboru Ishikawa
登 石川
Sumio Mukoyama
澄夫 向山
Masahiro Kojima
正大 小嶋
Hideetsu Haseyama
秀悦 長谷山
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.)
Shimizu Construction Co Ltd
Dowa Holdings Co Ltd
Shimizu Corp
Original Assignee
Shimizu Construction Co Ltd
Shimizu Corp
Dowa Mining 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 Shimizu Construction Co Ltd, Shimizu Corp, Dowa Mining Co Ltd filed Critical Shimizu Construction Co Ltd
Priority to JP5339120A priority Critical patent/JPH07147496A/en
Publication of JPH07147496A publication Critical patent/JPH07147496A/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)
  • Measuring Magnetic Variables (AREA)

Abstract

PURPOSE:To enable a superconductive magnetic shielding structure to shield an object contained in it from the influence of a magnetic field which penetrates through an opening and to be set compact in structure as a whole by a method wherein a superconductive case of circular or square tube is superconductively joined to the opening of the superconductive magnetic shielding structure. CONSTITUTION:A cylindrical magnetic shield structure main body 1 which is provided with closed upper and lower ends and an opening 4 at its side wall and formed of superconductive material board, a cylindrical case 2 whose upper and lower ends are both open is large in the L/D ratio (L: length, D: diameter) and formed of superconductive material board, and the cylindrical case 2 is superconductively joined to the cylindrical magnetic shield structure main body 1 in one piece with superconductive paste by inserting the one end of the case 2 into the opening 4 of the main body 1. By this setup, a superconductive magnetic shield structure wherein the structure main body l and the case 2 communicate with each other can be obtained. Thus, an external magnetic line of force is indirectly weakened, and an external magnetic field can be prevented from penetrating into a shield structure main body through an opening.

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、生体磁場計測や精密物
理計測等の微小磁場計測,半導体製造装置のEB露光な
どの分野において、比較的大型の磁気シールド空間を作
るための超電導磁気シールド構造物に関するものであ
る。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a superconducting magnetic shield structure for making a relatively large magnetic shield space in the fields of biomagnetic field measurement, minute magnetic field measurement such as precision physical measurement, and EB exposure of semiconductor manufacturing equipment. It is about things.

【0002】[0002]

【従来の技術】超電導体を利用した磁気シールド構造
は、磁力線が超電導体の内部に入り込めないというマイ
スナー効果を利用した磁気シールド構造であり、例えば
マイスナー効果を有する材料で筒状構造物を作製し、こ
れを臨界温度以下に冷却して超電導状態に転移させ、該
構造物の内部空間を磁気シールドするものである。
2. Description of the Related Art A magnetic shield structure using a superconductor is a magnetic shield structure utilizing the Meissner effect that magnetic lines of force cannot enter the inside of the superconductor. For example, a tubular structure is made of a material having the Meissner effect. Then, it is cooled to a temperature below the critical temperature to transform it into a superconducting state, and the internal space of the structure is magnetically shielded.

【0003】しかしながら、このような構造物には、人
の出入りや機材の搬入・搬出のための開口部を設けなけ
ればならず、そうすれば該開口部からの内部への侵入磁
場のため良好な遮蔽効果が得られず、磁気シールド構造
物内部での精密磁気測定が不可能となる。
However, such a structure must be provided with an opening for the entry and exit of people and the loading and unloading of equipment, which is favorable because of the magnetic field penetrating into the interior from the opening. Since no effective shielding effect is obtained, precise magnetic measurement inside the magnetic shield structure becomes impossible.

【0004】そのために、開口径に対して非常に大きな
長さの筒状構造物が必要となり、例えば各方向からの磁
界に対して遮蔽率が10−6倍程度の磁気遮蔽空間を得
るためには、長さが開口径の5倍以上の一方端を閉塞し
た筒状超電導構造物が必要であり、従って大きな空間が
必要となり、しかも作製が困難でコスト高となる等の問
題があった。
Therefore, a cylindrical structure having a very large length with respect to the opening diameter is required. For example, in order to obtain a magnetically shielded space having a shielding rate of about 10 −6 times against a magnetic field from each direction. Requires a cylindrical superconducting structure having one end closed at least 5 times the opening diameter, which requires a large space, and is difficult to manufacture, resulting in high cost.

【0005】また、超電導体によって磁気ノイズの少な
い空間を得るために、超電導体で扉を設けることが難し
いことから、添付の図11に示すような構造が従来から
提案されている。しかしながら、図11に示されるよう
に本来必要としない空間が大きくなり、従って高価な超
電導材料が多量に必要となってコストが上昇し、磁気シ
ールドルームの設置スペースの自由度が低下するという
問題があった。
Further, since it is difficult to provide a door with a superconductor in order to obtain a space with less magnetic noise by the superconductor, a structure as shown in FIG. 11 attached heretofore has been proposed. However, as shown in FIG. 11, the space that is not originally required becomes large, and therefore a large amount of expensive superconducting material is required, resulting in an increase in cost and a reduction in the degree of freedom in the installation space of the magnetic shield room. there were.

【0006】また、本来必要とする磁気遮蔽空間が狭く
なり、広く取ろうとする場合、本来必要としない空間部
分も同じ割合で広く取らなければならず、結局必要とし
ない空間部分の面積が相当大きくなってしまい、構造物
全体をコンパクトにまとめて限られた狭い空間に収納す
ることができないという問題があった。
Further, when the originally required magnetic shield space is narrowed and is intended to be wide, the originally unnecessary space portion must be widened at the same ratio, and the area of the unnecessary space portion is considerably large. However, there is a problem that the entire structure cannot be compactly packed and stored in a limited narrow space.

【0007】[0007]

【発明が解決しようとする課題】本発明は、上記のよう
な従来の諸問題を解決し、人間の出入りや機材の搬入・
搬出用のための開口部から侵入してくる不可避的な磁場
の影響を遮断し、磁気シールド構造物内部において精密
磁気測定が可能な高度な磁気遮蔽空間が実現でき、しか
も該構造物全体をコンパクトにまとめて、限られた狭い
空間の中に該構造物を収納することができる超電導磁気
シールド構造物を提供することを目的とする。
DISCLOSURE OF THE INVENTION The present invention solves the above-mentioned problems of the prior art, and allows humans to move in and out and equipment to be carried in.
By blocking the effect of inevitable magnetic field coming in through the opening for carrying out, it is possible to realize a sophisticated magnetic shielded space that enables precise magnetic measurement inside the magnetic shield structure, and the entire structure is compact. In summary, it is an object of the present invention to provide a superconducting magnetic shield structure capable of housing the structure in a limited narrow space.

【0008】[0008]

【課題を解決するための手段】請求項1の発明は、超電
導材料からなる開口部を有する磁気シールド構造物本体
の該開口部へ、両端開放の超電導材料からなる函体の一
端が超電導結合して該構造物本体と一体化され、内部が
連通されてなることを特徴とする超電導磁気シールド構
造物であり、
According to a first aspect of the present invention, one end of a box made of a superconducting material having both ends opened is superconductingly coupled to the opening of a magnetic shield structure body having an opening made of a superconducting material. Is a superconducting magnetic shield structure, characterized in that it is integrated with the main body of the structure, and the inside is communicated,

【0009】請求項3の発明は、超電導材料からなる開
口部を有する磁気シールド構造物本体の該開口部へ、該
構造物本体の一部を共有して形成された両端開放の超電
導材料からなる函体の一端が超電導結合して該構造物本
体と一体化され、内部が連通されてなることを特徴とす
る超電導磁気シールド構造物を提供するものである。
According to a third aspect of the present invention, the magnetic shield structure main body having an opening made of a superconducting material is formed of a superconducting material having both ends opened, which is formed by sharing a part of the structure main body. A superconducting magnetic shield structure characterized in that one end of a box is superconductingly coupled to be integrated with the main body of the structure, and the inside is communicated.

【0010】上記請求項1の発明においては、函体の形
状が円筒状又は角筒状であることが好ましく、請求項3
の発明においては函体の形状が平面円弧状又は角筒状で
あることが好ましいのである。
In the invention according to claim 1, it is preferable that the box has a cylindrical shape or a rectangular tube shape.
In the invention of (1), it is preferable that the shape of the box is a plane arc shape or a rectangular tube shape.

【0011】[0011]

【作用】次に、本発明を詳細に説明する。請求項1の発
明は、図1及び図2に例示するように、板状の超電導材
料で形成した円筒状あるいは角筒状の上・下端が閉塞さ
れた磁気シールド構造物本体に人間の出入りや機材の搬
入・搬出等用の開口部を設け、該開口部へ両端が開放さ
れ、長さ(L)と開口径(D:円筒状の場合は内径,角
筒状の場合は横幅)の比(L/D)が、好ましくは3以
上の円筒状(図1)又は角筒状(図2)の板状の超電導
材料で形成された函体の一方端を超電導ペースト等によ
り超電導結合させて上記超電導構造物本体と一体化さ
せ、両者内部が連通した超電導磁気シールド構造物であ
る。
Next, the present invention will be described in detail. In the invention of claim 1, as shown in FIG. 1 and FIG. 2, human beings enter and leave the main body of the magnetic shield structure in which the upper and lower ends of a cylindrical or rectangular tube formed of a plate-shaped superconducting material are closed. An opening for loading and unloading of equipment is provided, and both ends are opened to the opening, and the ratio of the length (L) to the opening diameter (D: inner diameter in the case of a cylindrical shape, width in the case of a square tube). (L / D) is preferably 3 or more, and one end of a box formed of a plate-shaped superconducting material having a cylindrical shape (FIG. 1) or a rectangular tube shape (FIG. 2) is superconductingly coupled with a superconducting paste or the like. It is a superconducting magnetic shield structure which is integrated with the superconducting structure body and has the inside communicating with each other.

【0012】上記の超電導磁気シールド構造物を構成す
る磁気シールド構造物本体及び函体の形状は、図1及び
図2に例示した円筒状あるいは角筒状に限定されるもの
ではなく、若干変形されたものでもよく、各部断面の形
状が均一でなくともよいことは勿論である。函体は外部
磁場の侵入を遮蔽し、かつ人間の出入り及び機材の搬入
・搬出等ができれば良いのである。
The shapes of the magnetic shield structure body and the box forming the above-mentioned superconducting magnetic shield structure are not limited to the cylindrical shape or the rectangular tube shape illustrated in FIGS. 1 and 2, but may be slightly modified. Of course, the shape of the cross section of each part may not be uniform. It suffices that the box shields the invasion of external magnetic fields and allows humans to enter and exit and equipment to be carried in and out.

【0013】上記のように構成された超電導磁気シール
ド構造物は、各方向からの外部磁場の侵入を超電導材料
製の構造物本体,函体及び超電導結合部によって遮蔽
し、特に開口部から侵入しようとする磁力線は、超電導
材料製の函体により後述(図10)のようにして遮蔽さ
れ、磁気シールド構造物本体内部は完全に磁気遮蔽され
高度な磁気遮蔽空間が得られるのである。
In the superconducting magnetic shield structure constructed as described above, the intrusion of the external magnetic field from each direction is shielded by the structure body made of the superconducting material, the box body and the superconducting joint portion, and in particular, it should enter through the opening. The magnetic lines of force are shielded by a box made of a superconducting material as described later (FIG. 10), and the inside of the magnetic shield structure main body is completely magnetically shielded to obtain a high-level magnetic shielding space.

【0014】請求項3の発明は、図3及び図5に例示す
るように、板状の超電導材料で形成した円筒状又は角筒
状の上・下端が閉塞された磁気シールド構造物本体に人
間の出入りや機材の搬入・搬出用の開口部を設け、該構
造物本体の一部を共有して形成され、かつ両端が開放さ
れ、長さ(L)(平面円弧状の場合は、円弧の長さ)と
開口部の幅(D)(角筒状又は平面円弧状の場合、共に
断面横幅)の比が大きく、好ましくは3以上の角筒状
(図3)又は平面円弧状(図5)の超電導材料で形成し
た函体の一方端を上記開口部へ超電導ペースト等により
超電導結合させて該構造物本体と一体化させ、両者内部
が連通した超電導磁気シールド構造物である。
In the invention of claim 3, as illustrated in FIGS. 3 and 5, a human being is attached to the main body of the magnetic shield structure in which the upper and lower ends of a cylindrical or rectangular tube formed of a plate-shaped superconducting material are closed. And an opening for loading and unloading of equipment and a part of the main body of the structure are shared, and both ends are open, and the length (L) (in the case of a plane arc shape, an arc shape) The ratio of the length) to the width (D) of the opening (in the case of a rectangular tube shape or a plane arcuate shape, the cross-sectional lateral width is large), preferably 3 or more of a rectangular tube shape (FIG. 3) or a plane arc shape (FIG. ) Is a superconducting magnetic shield structure in which one end of the box formed of the superconducting material is superconductingly coupled to the opening with a superconducting paste or the like to be integrated with the main body of the structure, and the insides of both are connected to each other.

【0015】上記請求項3記載の発明に係る超電導磁気
シールド構造物を構成する磁気シールド構造物本体の形
状は、図3及び図5に例示した円筒状又は角筒状に限定
されるものではなく、多少変形されたものでもよく、函
体の形状も同様に角筒状又は平面円弧状に限定されるも
のでなく、また各部の断面の形状が均一でなくともよい
ことは勿論である。また、外部磁場に対する磁気遮蔽効
果は、上記請求項1の発明の場合と同様である。
The shape of the magnetic shield structure body constituting the superconducting magnetic shield structure according to the third aspect of the invention is not limited to the cylindrical shape or the rectangular tube shape illustrated in FIGS. 3 and 5. Needless to say, the shape of the box body is not limited to the rectangular tube shape or the plane arc shape, and the cross-sectional shape of each part may not be uniform. Further, the magnetic shielding effect against the external magnetic field is similar to that of the invention of claim 1 above.

【0016】図7及び図8は、開口部に函体を連設しな
い超電導磁気シールド構造物に外部磁場が印加された場
合の説明図であり、図7は函体を連設しない超電導磁気
シールド構造物本体の斜視図であり、これに外部磁場
(Hex)が印加された場合の磁力線の侵入状況を示し
たのが図8である。
FIGS. 7 and 8 are explanatory views when an external magnetic field is applied to a superconducting magnetic shield structure in which a box is not continuously provided in the opening, and FIG. 7 is a superconducting magnetic shield in which no box is continuously provided. FIG. 8 is a perspective view of the structure body, and FIG. 8 shows a state of penetration of magnetic force lines when an external magnetic field (Hex) is applied to the structure body.

【0017】即ち、超電導磁気シールド構造物では、マ
イスナー効果により、外部磁場(Hex)は開口部以外
から構造物内部へ侵入することはできずに遮蔽される
が、開口部からの回り込み漏れ磁場により、磁気シール
ド構造物本体内部へ磁力線が侵入し、特に開口部付近で
の減衰率(Htr/Hex)の低下が著しく、該構造物
内部の磁気シールド効果はほとんど認められない。
That is, in the superconducting magnetic shield structure, the external magnetic field (Hex) is shielded by the Meissner effect because the external magnetic field (Hex) cannot enter the structure from the portions other than the opening, but the leakage magnetic field leaks from the opening. The magnetic field lines penetrate into the main body of the magnetic shield structure, and the attenuation rate (Htr / Hex) is remarkably reduced particularly near the opening, and the magnetic shield effect inside the structure is hardly recognized.

【0018】図9及び図10は、開口部に角筒状函体を
超電導結合した超電導磁気シールド構造物に外部磁場が
印加された場合の説明図であり、図9は開口部に角筒状
函体を超電導結合した超電導磁気シールド構造物の斜視
図であり、これに外部磁場(Hex)が印加された場合
の磁力線の侵入状況を示したのが図10である。
FIGS. 9 and 10 are explanatory views when an external magnetic field is applied to a superconducting magnetic shield structure in which a rectangular cylindrical box body is superconductingly coupled to the opening, and FIG. 9 is a rectangular cylindrical shape at the opening. FIG. 10 is a perspective view of a superconducting magnetic shield structure in which a box is superconductingly coupled, and FIG. 10 shows a state of penetration of magnetic force lines when an external magnetic field (Hex) is applied to the superconducting magnetic shield structure.

【0019】即ち、上記同様に超電導磁気シールド構造
物本体,函体及び超電導結合部に外部磁場(Hex)が
印加されても、これを打ち消す超電導電流が切れ目なく
流れて外部磁場(Hex)を遮蔽する。但し、函体の開
口部からは、回り込み漏れ磁場が侵入しようとするが、
函体のL/Dの比が少なくとも3以上の場合には、外部
磁場(Hex)はほぼ完全に遮蔽されるので磁気シール
ド構造物本体内には、高度な磁気遮蔽空間が得られるの
である。次に、本発明の実施例を図により説明する。
That is, even if an external magnetic field (Hex) is applied to the main body of the superconducting magnetic shield structure, the box and the superconducting coupling portion in the same manner as described above, the superconducting electric current that cancels this flow without interruption and shields the external magnetic field (Hex). To do. However, a sneaking magnetic field tries to enter from the opening of the box,
When the L / D ratio of the box is at least 3 or more, the external magnetic field (Hex) is almost completely shielded, so that a high magnetic shielding space can be obtained in the magnetic shield structure body. Next, an embodiment of the present invention will be described with reference to the drawings.

【0020】[0020]

【実施例】【Example】

実施例1 図1は、板状の超電導材料で形成した側壁面に開口部4
を設けた円筒状の上・下端閉塞された磁気シールド構造
物本体1の該開口部4へ両端が開放され、長さ(L)と
開口径(D)の比(L/D)が大きな円筒状の板状超電
導材料で形成された函体2の一方端(本図では左端)を
磁気シールド構造物本体1の開口部4に超電導ペースト
により超電導結合させて該構造物本体1と一体化させ、
該構造物本体1と函体2の内部が連通した超電導磁気シ
ールド構造物である。超電導材料としては、極低温で超
電導性を有する周知の材料が使用できる。
Example 1 FIG. 1 shows an opening 4 on a side wall formed of a plate-shaped superconducting material.
Both ends of the magnetic shield structure main body 1 having closed cylindrical upper and lower ends are provided with the openings 4 and both ends thereof are opened, and the ratio (L / D) of the length (L) to the opening diameter (D) is large. One end (the left end in the figure) formed of a plate-shaped plate-shaped superconducting material is superconductingly coupled to the opening 4 of the magnetic shield structure body 1 with a superconducting paste to be integrated with the structure body 1. ,
This is a superconducting magnetic shield structure in which the structure body 1 and the inside of the box 2 communicate with each other. As the superconducting material, a well-known material having superconductivity at an extremely low temperature can be used.

【0021】実施例2 図2は、板状の超電導材料で形成した側壁面に開口部4
を設けた四角筒状の上・下端閉塞された磁気シールド構
造物本体1の該開口部4へ両端が開放され、長さ(L)
と開口幅(断面横幅)(D)の比(L/D)が大きな四
角筒状の板状超電導材料で形成された函体2の一方端
(本図では左端)を磁気シールド構造物本体1の開口部
4に超電導ペーストにより超電導結合させて、該構造物
本体1と一体化させ、該構造物本体1と函体2の内部が
連通した超電導磁気シールド構造物である。超電導材料
としては、実施例1と同様に極低温で超電導特性を有す
る周知の材料が使用できる。
Example 2 FIG. 2 shows an opening 4 formed on a side wall of a plate-shaped superconducting material.
Both ends are opened to the opening 4 of the main body 1 of the magnetic shield structure which is closed at the upper and lower ends of the rectangular cylindrical shape having a length (L).
And one end (the left end in the figure) of the box body 2 formed of a plate-shaped superconducting material in the shape of a rectangular tube having a large ratio (L / D) of the opening width (cross sectional width) (D) to the magnetic shield structure body 1 It is a superconducting magnetic shield structure in which the opening 4 is superconductingly coupled with a superconducting paste to be integrated with the structure body 1, and the structure body 1 and the inside of the box 2 communicate with each other. As the superconducting material, a known material having superconducting properties at an extremely low temperature can be used as in the first embodiment.

【0022】実施例3 図3は、板状の超電導材料で形成した四角筒状の上・下
端閉塞された磁気シールド構造物本体1のA側壁に開口
部4を設け、該構造物本体1の一部であるA側壁を共有
して形成された両端が開放され、長さ(L)と出入口5
(開口部4と同形同寸法)の横幅(D)の比(L/D)
が大きな超電導材料で形成された函体2の一方端を磁気
シールド構造物本体1の開口部4に超電導ペーストによ
り超電導結合させて、該構造物本体1と一体化させ、該
構造物本体1と函体2の内部が連通した超電導磁気シー
ルド構造物である。図4は、X,Y,Z方向からの矢視
図である。上記函体2は、A側壁とB側壁と上・下壁面
とで形成され高さは構造物本体1と同程度に作製されて
いる。超電導材料としては、上記実施例1,2と同様の
材料板を使用した。
Embodiment 3 FIG. 3 shows an opening 4 is provided in the side wall A of a magnetic shield structure body 1 having a rectangular tubular shape formed of a plate-shaped superconducting material and having its upper and lower ends closed. Both ends formed by sharing the A side wall, which is a part, are opened, and the length (L) and the entrance / exit 5
Ratio (L / D) of lateral width (D) of the same shape and size as the opening 4
With a large superconducting material, one end of the box body 2 is superconductingly coupled to the opening 4 of the magnetic shield structure body 1 with a superconducting paste to be integrated with the structure body 1 and It is a superconducting magnetic shield structure in which the inside of the box 2 communicates. FIG. 4 is a view from the X, Y, and Z directions. The box 2 is formed by the A side wall, the B side wall, and the upper and lower wall surfaces, and is manufactured to have the same height as the structure body 1. As the superconducting material, the same material plate as in Examples 1 and 2 was used.

【0023】実施例4 図5は、超電導磁気シールド構造物の斜視図で、図6は
その平面図であり、本実施例においては、板状の超電導
材料で形成した円筒状の上・下端が閉塞された磁気シー
ルド構造物本体1の側壁に開口部4を設け、該構造物本
体1の一部である平面円弧状の側壁Aを共有して形成さ
れた両端が開放され、平面円弧状の側壁長さ(L)と、
両側壁間の幅(D)との比(L/D)が大きな超電導材
料で形成された平面円弧状の函体2の一方端を、磁気シ
ールド構造物本体1の開口部に超電導ペーストにより超
電導結合させて該構造物本体1と一体化させ、該構造物
本体1と函体2の内部が連通した超電導磁気シールド構
造物である。上記函体2は平面円弧状のA,B側壁と上
・下壁面とで形成され、高さは構造物本体1と同程度に
作製されている。使用する超電導材料としては、上記実
施例1〜3と同様な材料を使用した。
Embodiment 4 FIG. 5 is a perspective view of a superconducting magnetic shield structure, and FIG. 6 is a plan view thereof. In this embodiment, the cylindrical upper and lower ends made of a plate-shaped superconducting material are An opening 4 is provided in the side wall of the closed magnetic shield structure body 1, and both ends formed by sharing the side wall A having a plane arc shape, which is a part of the structure body 1, are opened to form a plane arc shape. Side wall length (L),
Superconducting one end of a planar arc-shaped box body 2 made of a superconducting material having a large ratio (L / D) with a width (D) between both side walls to an opening of the magnetic shield structure body 1 with a superconducting paste. It is a superconducting magnetic shield structure in which the structure body 1 and the inside of the box 2 are connected to each other and integrated with the structure body 1. The box 2 is formed by A and B side walls having a plane arc shape and upper and lower wall surfaces, and is manufactured to have the same height as the structure main body 1. As the superconducting material to be used, the same materials as those in Examples 1 to 3 were used.

【0024】上記実施例1〜4のL/Dが3以上の超電
導磁気シールド構造物を液体窒素(77K)で冷却した
後、該構造物本体1の中心軸に対して平行ならびに垂直
方向に外部から磁場を印加し、磁気遮蔽特性を測定し
た。
After cooling the superconducting magnetic shield structures having L / D of 3 or more in Examples 1 to 4 described above with liquid nitrogen (77K), the superconducting magnetic shield structures were externally parallel and perpendicular to the central axis of the structure main body 1. A magnetic field was applied to measure the magnetic shielding characteristics.

【0025】その結果、各超電導磁気シールド構造物本
体1内部に、滅衰率(Htr/Hex)が10−6倍以
上の遮蔽空間が得られた。
As a result, a shielded space having an extinction ratio (Htr / Hex) of 10 −6 or more was obtained inside each superconducting magnetic shield structure body 1.

【0026】[0026]

【発明の効果】本発明によれば、超電導磁気シールド構
造物本体の開口部に長さ(L)と開口径(D)の比(L
/D)が好ましくは3以上の筒状又は角筒状の超電導函
体を超電導結合させることにより、外部の磁力線は間接
的に弱められ、開口部からの該シールド構造物本体内へ
の外部磁場の侵入が遮蔽でき、高度な遮蔽空間を得るこ
とができる。
According to the present invention, the ratio (L) of the length (L) to the opening diameter (D) is set in the opening of the main body of the superconducting magnetic shield structure.
/ D) is preferably 3 or more in the form of a tubular or rectangular tubular superconducting box, the external magnetic field lines are indirectly weakened and the external magnetic field from the opening into the shield structure body. It is possible to shield the invasion of the air and to obtain a highly shielded space.

【0027】しかも、本発明によれば、構造物全体をコ
ンパクトにまとめて、限られた狭い空間の中に該構造物
を収納することができる。
Moreover, according to the present invention, the entire structure can be compactly packed, and the structure can be housed in a limited narrow space.

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

【図1】本発明に係る円筒状函体を結合した超電導磁気
シールド構造物の一実施例を示す斜視図である。
FIG. 1 is a perspective view showing an embodiment of a superconducting magnetic shield structure in which cylindrical boxes according to the present invention are combined.

【図2】本発明に係る角筒状函体を結合した超電導磁気
シールド構造物の一実施例を示す斜視図である。
FIG. 2 is a perspective view showing an embodiment of a superconducting magnetic shield structure in which rectangular tubular boxes according to the present invention are combined.

【図3】磁気シールド構造物本体の一部を共有した角筒
状の函体を結合した本発明に係る超電導磁気シールド構
造物の一実施例を示す斜視図である。
FIG. 3 is a perspective view showing an embodiment of a superconducting magnetic shield structure according to the present invention, in which a rectangular tubular box body sharing a part of the magnetic shield structure body is coupled.

【図4】図3に示す超電導磁気シールド構造物のX,
Y,Z方向からの矢視図である。
FIG. 4 is a diagram showing X, of the superconducting magnetic shield structure shown in FIG.
It is an arrow view from the Y and Z directions.

【図5】磁気シールド構造物本体の一部を共有した平面
円弧状の函体を結合した本発明に係る超電導磁気シール
ド構造物の一実施例を示す斜視図である。
FIG. 5 is a perspective view showing an embodiment of a superconducting magnetic shield structure according to the present invention, in which planar arc-shaped boxes sharing a part of the magnetic shield structure main body are combined.

【図6】図5に示す超電導磁気シールド構造物の平面図
である。
FIG. 6 is a plan view of the superconducting magnetic shield structure shown in FIG.

【図7】磁気シールド構造物本体の開口部に函体を結合
しない超電導磁気シールド構造物の斜視図である。
FIG. 7 is a perspective view of a superconducting magnetic shield structure in which a box is not coupled to the opening of the magnetic shield structure body.

【図8】図7に示す構造物に外部磁場が印加された場合
の説明的磁力線図である。
8 is an explanatory diagram of magnetic force lines when an external magnetic field is applied to the structure shown in FIG.

【図9】磁気シールド構造物本体の開口部に角筒状函体
を結合した超電導磁気シールド構造物の斜視図である。
FIG. 9 is a perspective view of a superconducting magnetic shield structure in which a rectangular tubular box is coupled to the opening of the magnetic shield structure body.

【図10】図9に示す構造物に外部磁場が印加された場
合の説明的磁力線図である。
FIG. 10 is an explanatory diagram of magnetic force lines when an external magnetic field is applied to the structure shown in FIG.

【図11】従来の磁気シールド構造物の説明的な断面図
である。
FIG. 11 is an explanatory cross-sectional view of a conventional magnetic shield structure.

【符号の説明】[Explanation of symbols]

1−超電導磁気シールド構造物本体 2−函体 3−超電導結合部 4−開口部 5−出入口 6−磁力線 A−共有側壁 B−側壁 D−開口径,又は開口幅 L−函体の長さ イ−超電導磁気シールド空間 ロ−実質的に必要としない空間 1-Superconducting magnetic shield structure main body 2-Box 3-Superconducting coupling section 4-Aperture section 5-Inlet / outlet port 6-Magnetic field line A-Shared side wall B-Side wall D-Opening diameter or opening width L-Box length a − Superconducting magnetic shield space − Space not actually needed

───────────────────────────────────────────────────── フロントページの続き (72)発明者 向山 澄夫 東京都港区芝浦一丁目2番3号 清水建設 株式会社内 (72)発明者 小嶋 正大 東京都千代田区丸の内一丁目8番2号 同 和鉱業株式会社内 (72)発明者 長谷山 秀悦 東京都千代田区丸の内一丁目8番2号 同 和鉱業株式会社内 ─────────────────────────────────────────────────── ─── Continuation of the front page (72) Sumio Mukaiyama, 1-3-2 Shibaura, Minato-ku, Tokyo Shimizu Construction Co., Ltd. (72) Masahiro Kojima 1-2-8, Marunouchi, Chiyoda-ku, Tokyo Dowa Mining Co., Ltd. (72) Inventor Hideetsu Haseyama 1-2-8 Marunouchi, Chiyoda-ku, Tokyo Dowa Mining Co., Ltd.

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】 超電導材料からなる開口部を有する磁気
シールド構造物本体の該開口部へ両端開放の超電導材料
からなる函体の一端が超電導結合して該構造物本体と一
体化され内部が連通されてなることを特徴とする超電導
磁気シールド構造物。
1. A magnetic shield structure body having an opening made of a superconducting material, wherein one end of a box made of a superconducting material whose both ends are open is superconductingly coupled to the opening so as to be integrated with the structure body and communicate with the inside. A superconducting magnetic shield structure characterized by being formed.
【請求項2】 前記函体が円筒状又は角筒状であること
を特徴とする請求項1記載の超電導磁気シールド構造
物。
2. The superconducting magnetic shield structure according to claim 1, wherein the box has a cylindrical shape or a rectangular tube shape.
【請求項3】 超電導材料からなる開口部を有する磁気
シールド構造物本体の該開口部へ該構造物本体の一部を
共有して形成された両端開放の超電導材料からなる函体
の一端が超電導結合して該構造物本体と一体化され内部
が連通されてなることを特徴とする超電導磁気シールド
構造物。
3. A magnetic shield structure main body having an opening made of a superconducting material, wherein one end of a box made of a superconducting material having both ends opened and formed by sharing a part of the structure main body is superconducting. A superconducting magnetic shield structure, characterized in that the superconducting magnetic shield structure is integrated with the structure body and communicates with the inside.
【請求項4】 前記函体が平面円弧状又は角筒状である
ことを特徴とする請求項3記載の超電導磁気シールド構
造物。
4. The superconducting magnetic shield structure according to claim 3, wherein the box has a plane arc shape or a rectangular tube shape.
JP5339120A 1993-11-24 1993-11-24 Superconductive magnetic shielding structure Pending JPH07147496A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5339120A JPH07147496A (en) 1993-11-24 1993-11-24 Superconductive magnetic shielding structure

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5339120A JPH07147496A (en) 1993-11-24 1993-11-24 Superconductive magnetic shielding structure

Publications (1)

Publication Number Publication Date
JPH07147496A true JPH07147496A (en) 1995-06-06

Family

ID=18324442

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5339120A Pending JPH07147496A (en) 1993-11-24 1993-11-24 Superconductive magnetic shielding structure

Country Status (1)

Country Link
JP (1) JPH07147496A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10627456B2 (en) 2017-02-10 2020-04-21 Electronics And Telecommunications Research Institute Magnetic field shielding apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US10627456B2 (en) 2017-02-10 2020-04-21 Electronics And Telecommunications Research Institute Magnetic field shielding apparatus

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