JPH0745991A - Superconducting magnetic shielding structure - Google Patents
Superconducting magnetic shielding structureInfo
- Publication number
- JPH0745991A JPH0745991A JP5192395A JP19239593A JPH0745991A JP H0745991 A JPH0745991 A JP H0745991A JP 5192395 A JP5192395 A JP 5192395A JP 19239593 A JP19239593 A JP 19239593A JP H0745991 A JPH0745991 A JP H0745991A
- Authority
- JP
- Japan
- Prior art keywords
- cylindrical
- superconductor
- magnetic field
- superconducting
- permeability
- 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
Abstract
Description
【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。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 minute magnetic field measurement such as biomagnetic field measurement and precision physical measurement, and EB exposure of semiconductor manufacturing equipment. Regarding 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を筒状構造物とし、これを
臨界温度以下に冷却して超電導状態に転移させ、筒状構
造物の内部空間を磁気シールドするものである。こうし
た筒状構造物は、筒の中心軸に平行な磁場に対する遮蔽
効率は良いが、中心軸に垂直な磁場に対する遮蔽効率は
良くないため、筒の内径に対して長さを長くしなければ
ならず、人間が入れる程度の直径で所望の低磁場空間を
得る場合には、とくに問題となる。これを解決するため
に、従来、特開平4−218998号公報において、図
5に示すように、超電導材料からなる筒状超電導体1内
に、筒状超電導体1の長手方向に沿って、開口を有する
筒状高透磁率体2を筒状超電導体1の内壁と間隔をもっ
て配設する方式を提案している。これによれば、筒状超
電導体1の長手軸上の中心方向に減衰分布を示す侵入磁
界に対して、筒状高透磁率体2内に磁気誘導が生じ、そ
の結果、侵入磁界が磁気的に短絡し、筒状超電導体1内
部に侵入する磁界を減少させるものである。2. Description of the Related Art A magnetic shield structure using a superconductor is a magnetic shield structure utilizing the Meissner effect that magnetic field lines cannot enter the inside of the superconductor. For example, a material having the Meissner effect is formed into a tubular structure, This is cooled to below the critical temperature and transformed into a superconducting state to magnetically shield the internal space of the cylindrical structure. Such a cylindrical structure has good shielding efficiency against a magnetic field parallel to the central axis of the cylinder, but has poor shielding efficiency against a magnetic field perpendicular to the central axis. Therefore, the length must be increased relative to the inner diameter of the cylinder. However, when a desired low magnetic field space is obtained with a diameter that humans can enter, it becomes a particular problem. In order to solve this, in Japanese Patent Laid-Open No. 4-218998, conventionally, as shown in FIG. 5, an opening is formed in a tubular superconductor 1 made of a superconducting material along the longitudinal direction of the tubular superconductor 1. It proposes a method of arranging the cylindrical high-permeability body 2 having a space with the inner wall of the cylindrical superconductor 1. According to this, magnetic induction occurs in the cylindrical high-permeability body 2 with respect to the intruding magnetic field showing the attenuation distribution in the central direction on the longitudinal axis of the cylindrical superconductor 1, and as a result, the intruding magnetic field is magnetically induced. To reduce the magnetic field penetrating inside the tubular superconductor 1.
【0003】[0003]
【発明が解決しようとする課題】しかしながら、上記従
来の方式においては、筒状超電導体1の開口部に筒状高
透磁率体2を配設するため、開口部を利用して人間が出
入りする場合には筒状高透磁率体2が障害となり、その
分だけ筒状シールド体1の内径を大きく、従って所望の
低磁場空間を得るには長さも長くしなければならないと
いう問題を有している。However, in the above-mentioned conventional method, the cylindrical high-permeability body 2 is arranged in the opening of the cylindrical superconductor 1, so that a person can enter and leave using the opening. In this case, the cylindrical high-permeability body 2 becomes an obstacle, and the inner diameter of the cylindrical shield body 1 is correspondingly increased, so that the length must be increased to obtain a desired low magnetic field space. There is.
【0004】本発明は上記問題を解決するものであっ
て、筒状超電導体の軸方向および軸に垂直方向からの侵
入磁界に対するを磁気遮蔽効率を向上させるとともに、
筒状超電導体の開口部の広さを確保しつつ長さを短くす
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。The present invention solves the above problems and improves the magnetic shielding efficiency against the magnetic field penetrating from the axial direction of the cylindrical superconductor and the direction perpendicular to the axis.
An object of the present invention is to provide a superconducting magnetic shield structure capable of shortening the length of the tubular superconductor while ensuring the width of the opening.
【0005】[0005]
【課題を解決するための手段】そのために、本発明の超
電導磁気シールド構造物は、超電導材料からなる筒状超
電導体11の開口部または最も磁場の低い部分の少なく
とも一つの部分に、筒状超電導体11の外周に高透磁率
材料からなる筒状高透磁率体12、13が配設されてな
ることを特徴とする。なお、前記筒状高透磁率体13
は、多重中空筒状からなるようにしてもよい。ここで上
記構成に付加した番号は、本発明の理解を容易にするた
めに図面と対比させるためのもので、これにより本発明
の構成が何ら限定されるものではない。To this end, the superconducting magnetic shield structure of the present invention is provided with a cylindrical superconducting material in at least one of the opening or the lowest magnetic field portion of the cylindrical superconductor 11 made of a superconducting material. It is characterized in that cylindrical high magnetic permeability bodies 12 and 13 made of a high magnetic permeability material are arranged on the outer periphery of the body 11. The cylindrical high magnetic permeability body 13
May have a multiple hollow cylindrical shape. The numbers added to the above configuration are for comparison with the drawings to facilitate understanding of the present invention, and the configuration of the present invention is not limited thereby.
【0006】[0006]
【作用】本発明においては、例えば図1から図4に示す
ように、筒状超電導体11の軸方向からの外部磁気は筒
状超電導体11と筒状高透磁率体12、13によって遮
蔽され、また軸に垂直方向の外部磁気は主として筒状高
透磁率体12、13によって遮蔽される。In the present invention, as shown in FIGS. 1 to 4, for example, the external magnetism from the axial direction of the tubular superconductor 11 is shielded by the tubular superconductor 11 and the tubular high-permeability bodies 12, 13. Also, external magnetism in the direction perpendicular to the axis is mainly shielded by the cylindrical high magnetic permeability bodies 12 and 13.
【0007】[0007]
【実施例】以下、本発明の実施例を図面を参照しつつ説
明する。図1から図4は本発明の超電導磁気シールド構
造物の各実施例を示し、それぞれ図(A)は軸方向断面
図、図(B)は図(A)のB−B線に沿って矢印方向に
見た断面図である。Embodiments of the present invention will be described below with reference to the drawings. 1 to 4 show each embodiment of the superconducting magnetic shield structure of the present invention. FIG. 1A is an axial sectional view, and FIG. 1B is an arrow along line BB in FIG. 1A. It is sectional drawing seen in the direction.
【0008】図1の実施例においては、超電導材料から
なる筒状超電導体11の開口部にまたがるように、筒状
超電導体11の外周と間隔をおいて高透磁率材料からな
る筒状高透磁率体12が配設されている。超電導材料と
しては、極低温で超電導体となる周知の材料が使用さ
れ、高透磁率材料としてはパーマロイ、珪素鋼板など周
知の材料が使用される。In the embodiment of FIG. 1, a cylindrical high-permeability material made of a high-permeability material is formed at a distance from the outer periphery of the cylindrical superconductor 11 so as to extend over the opening of the cylindrical superconductor 11 made of a superconducting material. A magnetic susceptibility body 12 is provided. A well-known material that becomes a superconductor at an extremely low temperature is used as the superconducting material, and a well-known material such as permalloy or a silicon steel sheet is used as the high magnetic permeability material.
【0009】図2の実施例においては、筒状超電導体1
1の開口部にまたがるように、筒状超電導体11の外周
と間隔をおいて、高透磁率材料からなる中空二重の筒状
高透磁率体13が配設されている。中空二重の筒状高透
磁率体13は、内筒13a、外筒13b、内筒13aと
外筒13b間に固定されるスペーサ部材13cからな
る。なお、二重筒に限定されるものではなく、三重筒以
上でもよい。In the embodiment of FIG. 2, the tubular superconductor 1
A hollow double cylindrical high-permeability body 13 made of a high-permeability material is arranged at a distance from the outer periphery of the cylindrical superconductor 11 so as to straddle the opening 1. The hollow double tubular high magnetic permeability body 13 includes an inner cylinder 13a, an outer cylinder 13b, and a spacer member 13c fixed between the inner cylinder 13a and the outer cylinder 13b. The cylinder is not limited to the double cylinder, but may be a triple cylinder or more.
【0010】図3の実施例においては、筒状超電導体1
1の内部の最も磁場の低い部分の外周に間隔をおいて、
図1と同様の筒状高透磁率体12を配設した例を示し、
図4の実施例においては、筒状超電導体11の内部の最
も磁場の低い部分の外周に間隔をおいて、図2と同様の
中空二重の筒状高透磁率体13を配設した例を示してい
る。なお、本発明は上記実施例に限定されるものではな
く、図1の構成と図3または図4の構成を組み合わせる
方式や、或いは図2の構成と図3または図4の構成を組
み合わせる方式が挙げられる。In the embodiment of FIG. 3, the cylindrical superconductor 1
A space is placed around the lowest magnetic field inside 1
An example in which a cylindrical high magnetic permeability body 12 similar to that shown in FIG.
In the embodiment of FIG. 4, an example in which a hollow double cylindrical high magnetic permeability body 13 similar to that of FIG. 2 is arranged at an outer circumference of a portion having the lowest magnetic field inside the cylindrical superconductor 11. Is shown. The present invention is not limited to the above embodiment, and a method of combining the configuration of FIG. 1 and the configuration of FIG. 3 or 4 or a method of combining the configuration of FIG. 2 and the configuration of FIG. Can be mentioned.
【0011】上記構成により、筒状超電導体11の軸方
向からの外部磁気は筒状超電導体11と筒状高透磁率体
12、13によって遮蔽され、また軸に垂直方向の外部
磁気は主として筒状高透磁率体12、13によって遮蔽
される。With the above structure, the external magnetism in the axial direction of the tubular superconductor 11 is shielded by the tubular superconductor 11 and the tubular high-permeability bodies 12 and 13, and the external magnetism perpendicular to the axis is mainly in the tubular form. Are shielded by the high magnetic permeability bodies 12, 13.
【0012】[0012]
【発明の効果】以上の説明から明らかなように本発明に
よれば、筒状超電導体の軸方向および軸に垂直方向から
の侵入磁界に対するを磁気遮蔽効率を向上させるととも
に、筒状超電導体の開口部の広さを確保しつつ長さを短
くすることができる。As is apparent from the above description, according to the present invention, the magnetic shielding efficiency against the intruding magnetic field from the axial direction and the direction perpendicular to the axis of the tubular superconductor is improved, and the tubular superconductor The length can be shortened while ensuring the width of the opening.
【図1】本発明の超電導磁気シールド構造物の1実施例
を示し、図(A)は垂直断面図、図(B)は図(A)の
B−B線に沿って矢印方向に見た断面図である。1A and 1B show an embodiment of a superconducting magnetic shield structure of the present invention, FIG. 1A is a vertical sectional view, and FIG. 1B is seen in a direction of an arrow along line BB in FIG. 1A. FIG.
【図2】本発明の超電導磁気シールド構造物の他の実施
例を示し、図(A)は垂直断面図、図(B)は図(A)
のB−B線に沿って矢印方向に見た断面図である。2A and 2B show another embodiment of the superconducting magnetic shield structure of the present invention, in which FIG. 2A is a vertical sectional view and FIG.
FIG. 4 is a sectional view taken along line BB in FIG.
【図3】本発明の超電導磁気シールド構造物の他の実施
例を示し、図(A)は垂直断面図、図(B)は図(A)
のB−B線に沿って矢印方向に見た断面図である。3A and 3B show another embodiment of the superconducting magnetic shield structure of the present invention, FIG. 3A is a vertical sectional view, and FIG.
FIG. 4 is a sectional view taken along line BB in FIG.
【図4】本発明の超電導磁気シールド構造物の他の実施
例を示し、図(A)は垂直断面図、図(B)は図(A)
のB−B線に沿って矢印方向に見た断面図である。FIG. 4 shows another embodiment of the superconducting magnetic shield structure of the present invention, where FIG. 4A is a vertical sectional view and FIG.
FIG. 4 is a sectional view taken along line BB in FIG.
【図5】従来の超電導磁気シールド構造物の例を示す断
面図である。FIG. 5 is a sectional view showing an example of a conventional superconducting magnetic shield structure.
11…筒状超電導体、12…筒状高透磁率体 13…中空二重の筒状高透磁率体 11 ... Cylindrical superconductor, 12 ... Cylindrical high magnetic permeability body 13 ... Hollow double cylindrical high magnetic permeability body
フロントページの続き (72)発明者 澁谷紳一 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 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Front page continued (72) Shinichi Shibuya, 1-3-2 Shibaura, Minato-ku, Tokyo Shimizu Construction Co., Ltd. (72) Sumio Mukaiyama, 1-3-2 Shibaura, Minato-ku, Tokyo Shimizu Construction Co., Ltd.
Claims (2)
または最も磁場の低い部分の少なくとも一つの部分に、
筒状超電導体の外周に高透磁率材料からなる筒状高透磁
率体が配設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 tubular superconductor made of a superconducting material, at least at least one of an opening or a portion having the lowest magnetic field,
A superconducting magnetic shield structure characterized in that a cylindrical high-permeability body made of a high-permeability material is arranged around the outer periphery of the cylindrical superconductor.
なることを特徴とする請求項1に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 cylindrical high-permeability body has a multi-hollow cylindrical shape.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5192395A JPH0745991A (en) | 1993-08-03 | 1993-08-03 | Superconducting magnetic shielding structure |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP5192395A JPH0745991A (en) | 1993-08-03 | 1993-08-03 | Superconducting magnetic shielding structure |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0745991A true JPH0745991A (en) | 1995-02-14 |
Family
ID=16290599
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP5192395A Pending JPH0745991A (en) | 1993-08-03 | 1993-08-03 | Superconducting magnetic shielding structure |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0745991A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013077698A (en) * | 2011-09-30 | 2013-04-25 | Seiko Epson Corp | Magnetic shield |
-
1993
- 1993-08-03 JP JP5192395A patent/JPH0745991A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2013077698A (en) * | 2011-09-30 | 2013-04-25 | Seiko Epson Corp | Magnetic shield |
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