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JPH01111400A - Magnetic shielding structure body - Google Patents

Magnetic shielding structure body

Info

Publication number
JPH01111400A
JPH01111400A JP62268091A JP26809187A JPH01111400A JP H01111400 A JPH01111400 A JP H01111400A JP 62268091 A JP62268091 A JP 62268091A JP 26809187 A JP26809187 A JP 26809187A JP H01111400 A JPH01111400 A JP H01111400A
Authority
JP
Japan
Prior art keywords
magnetic
layer
substance
shielding
magnetic flux
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
JP62268091A
Other languages
Japanese (ja)
Inventor
Akihiro Matsuzaki
明博 松崎
Osamu Masuko
増子 修
Hiroshi Otsubo
宏 大坪
Yutaka Oka
裕 岡
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.)
JFE Steel Corp
Original Assignee
Kawasaki Steel 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 Kawasaki Steel Corp filed Critical Kawasaki Steel Corp
Priority to JP62268091A priority Critical patent/JPH01111400A/en
Publication of JPH01111400A publication Critical patent/JPH01111400A/en
Pending legal-status Critical Current

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  • Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

PURPOSE:To enhance magnetic shielding performance against an external magnetic field and its change by a method wherein an inner layer composed of a paramagnetic substance, an intermediate layer composed of a substance whose maximum resistivity value is specified and an outer layer composed of the paramagnetic substance are provided. CONSTITUTION:This body is constituted by the following at least three layers: an inner layer 11 composed of a paramagnetic substance, an intermediate layer 12 composed of a substance whose maximum resistivity value is 100 or less; an outer layer 13 composed of the paramagnetic substance. That is, in order to make the inner magnetic flux independent of the outer magnetic flux and to avoid their mutual interference, a shielding layer composed of the paramagnetic substance is divided into two inner and outer layers 11, 13; in order to reduce their mutual interference of the magnetic flux between the two inner and outer layers 11, 13, the substance whose maximum resistivity value is 100 or less is used for the intermediate layer 12 sandwiched between the two inner and outer layers 11, 13. By this setup, an excellent magnetic shielding effect can be realized.

Description

【発明の詳細な説明】 [産業上の利用性!!?] 本発明は、Fii場の漏洩防止と同時に外部磁場の変化
を磁気シールドする必要のある機器、例えば核磁気共鳴
断層撮影装置(以下NMR−CT)等のために用いて好
適な磁気シールド構造体に関する。
[Detailed description of the invention] [Industrial applicability! ! ? ] The present invention provides a magnetic shield structure suitable for use in equipment that requires magnetic shielding from changes in external magnetic fields at the same time as preventing Fii field leakage, such as nuclear magnetic resonance tomography equipment (hereinafter referred to as NMR-CT). Regarding.

[従来の技術] NMR−CT等の磁気シールドは、純鉄あるいは珪素鋼
等の高透磁率材料の単一層からなる磁気シールド構造体
にて、シールド対象機器を囲うのが通例である。
[Prior Art] In magnetic shielding for NMR-CT and the like, it is customary to surround equipment to be shielded with a magnetic shielding structure made of a single layer of high magnetic permeability material such as pure iron or silicon steel.

従来、上記磁気シールド構造体における磁気シールド性
能を向上する試みは1例えば特開昭80−208418
号公報に記載される如く、そのシールド材料の製造方法
を改善することにて実施されている。
Conventionally, there have been attempts to improve the magnetic shielding performance of the above-mentioned magnetic shielding structure, for example, in JP-A-80-208418.
As described in the above publication, this method has been implemented by improving the manufacturing method of the shielding material.

[発明が解決しようとする問題点1 しかしながら、単一層からなる磁気シールド構造体にあ
っては、たとえ透磁率の高い磁気シールド性に優れたシ
ールド材料を用いても、磁束の僅かな遍洩を避けること
ができず、内部のシールド対象機器への影響を完全に遮
断することは不可能である。
[Problem to be Solved by the Invention 1] However, in a magnetic shielding structure made of a single layer, even if a shielding material with high magnetic permeability and excellent magnetic shielding properties is used, it is difficult to prevent even slight leakage of magnetic flux. This is unavoidable, and it is impossible to completely block out the influence on internal shielded equipment.

このことは、例えばNMR−CTのように微小振!!!
I磁場を発生させるシールド対象機器に対して、極めて
大きな影響を及ぼし、それらの機器の作動精度(測定精
度等)の低下を招く。
This means that, for example, in NMR-CT, minute vibrations! ! !
This has an extremely large effect on shielded equipment that generates the I magnetic field, leading to a decrease in the operational accuracy (measurement accuracy, etc.) of those equipment.

本発明は、外部磁場およびその変化に対する磁気シール
ド性を確実に向上することを目的とする。
An object of the present invention is to reliably improve magnetic shielding properties against external magnetic fields and changes thereof.

[問題点を解決するための手段] 本発明は、磁場の影響を遮弊するために設けられる磁気
シールド構造体において、常磁性体からなる内層、最大
比透磁率が100以下の物質からなる中間層、および常
磁性体からなる外層の少なくとも3層を有してなるよう
にしたものである。
[Means for Solving the Problems] The present invention provides a magnetic shield structure provided for shielding the influence of a magnetic field, which includes an inner layer made of a paramagnetic material and an intermediate layer made of a material having a maximum relative magnetic permeability of 100 or less. It has at least three layers: a magnetic layer and an outer layer made of a paramagnetic material.

[作用] 本発明者らの考察によれば、従来の単一層からなる磁気
シールド構造体では、外部磁束と内部磁束が同一のシー
ルド材料を流れるために磁束同士の相互干渉を生じ、そ
の磁気シールド効果が十分でない。
[Function] According to the inventors' considerations, in a conventional single-layer magnetic shield structure, since the external magnetic flux and the internal magnetic flux flow through the same shield material, mutual interference occurs between the magnetic fluxes, and the magnetic shield The effect is not sufficient.

そこで、木発明者らは、上記内外の磁束同士の相互干渉
を防止するため実験を重ねた結果、その相互干渉はシー
ルド構造体の構造の改良により低減できるものであるこ
とを見出した。
As a result of repeated experiments to prevent the mutual interference between the internal and external magnetic fluxes, the inventors discovered that the mutual interference can be reduced by improving the structure of the shield structure.

すなわち、内外の磁束が独立し相互干渉を生じないよう
にするため、常磁性体からなるシールド層を内外の2F
3に分離し、さらにそれら内外2層間における磁束同士
の相互干渉を低減させるため、それら内外2層に挟まれ
る中間層に最大比透ra IEが 100以下の物質を
設けることにより、優れた磁気シールド効果を実現でき
ることを認めた・ 〔実施例〕 本発明の3層構造からなる磁気シールド構造体の磁気シ
ールド効果および中間層材料に備えるべき適正な透磁率
を確認するため、以下の実験を行なった。
In other words, in order to ensure that the magnetic fluxes inside and outside are independent and do not interfere with each other, a shield layer made of paramagnetic material is placed between the inside and outside 2F.
In order to further reduce the mutual interference between the magnetic flux between the two layers, an excellent magnetic shield is achieved by providing a material with a maximum relative permeability ra IE of 100 or less in the intermediate layer sandwiched between the two layers. [Example] In order to confirm the magnetic shielding effect of the magnetic shielding structure consisting of the three-layer structure of the present invention and the appropriate magnetic permeability that should be provided for the intermediate layer material, the following experiment was conducted. .

実験装置として用いた磁気シールド構造体10は第1図
の如くであり、内層シールド体11、外層シールド体1
2、中間層シールド体13の3層にて構成した。
The magnetic shielding structure 10 used as an experimental device is as shown in FIG.
2. Constructed of three layers: intermediate layer shield body 13.

磁気シールド構造体10の大きさは約2mX2mであり
、内層および外層のシールド材料としては純鉄を用い、
中間層を形成するシールド材料の最大比′r透磁率を種
々変化させた。
The size of the magnetic shield structure 10 is approximately 2 m x 2 m, and pure iron is used as the shielding material for the inner and outer layers.
The maximum ratio 'r magnetic permeability of the shielding material forming the intermediate layer was varied.

また、磁気シールド構造体10の内外のそれぞれに、内
部磁場発生装置(定常磁場)14および磁束測定計15
、ならびに外部磁場発生装2!(定常・交番磁場)およ
び磁束測定計17を段設した。
In addition, an internal magnetic field generator (steady magnetic field) 14 and a magnetic flux measuring meter 15 are provided inside and outside the magnetic shielding structure 10, respectively.
, as well as external magnetic field generator 2! (steady/alternating magnetic field) and magnetic flux measuring meters 17 were installed in stages.

まず外部磁場の内部への漏洩を調べるために、外部に交
番磁場を発生させ内部への影響を調べた。ここで、外部
磁場としては0.5 、2 、10Gauβの3水準と
しそれぞれ±30%の交番磁場(周期1秒)を発生させ
た。また、内部磁場としては30 Gauβの定常磁場
を発生させた。結果を第2図に示す、すなわち、第2図
は外部交番磁場を付与した時の内部における磁束変化率
(内部磁場30 Gauβ)を示し、中間層のシールド
材料の最大比透磁率が100以下の場合に1層構造体に
比べて磁気シールド性が著しく向上する。またその磁気
シールド効果は交番磁場の平均が0.5 、2 、10
Gauβのいずれであっても同様である。したがって、
本発明の実施において、中間層のシールド材料としては
非磁性材料または空隙を設けるのみでも十分な磁気シー
ルド効果を得ることができる。
First, in order to investigate the leakage of external magnetic fields into the interior, an alternating magnetic field was generated externally and the influence on the interior was investigated. Here, the external magnetic field was set to three levels: 0.5, 2, and 10 Gauβ, and an alternating magnetic field (period: 1 second) of ±30% was generated. Furthermore, a steady magnetic field of 30 Gauβ was generated as an internal magnetic field. The results are shown in Figure 2. That is, Figure 2 shows the internal magnetic flux change rate (internal magnetic field 30 Gauβ) when an external alternating magnetic field is applied. In this case, magnetic shielding properties are significantly improved compared to a single layer structure. In addition, the magnetic shielding effect is such that the average of the alternating magnetic field is 0.5, 2, 10
The same applies to any of Gauβ. therefore,
In carrying out the present invention, a sufficient magnetic shielding effect can be obtained by simply providing a non-magnetic material or a gap as the shielding material for the intermediate layer.

なお、第2図の縦軸の磁束変化率は、純鉄による1層構
造体の場合の磁束変化幅を 100とした時の比である
The magnetic flux change rate on the vertical axis in FIG. 2 is a ratio when the magnetic flux change width in the case of a single layer structure made of pure iron is set to 100.

次に、内部磁場の外部への漏洩度を第3図に示す、ここ
で、外部磁場としては I Gauβの定常磁場を発生
させた。すなわち、第3図は内部磁場を付与した時の外
部における漏洩磁束(外部磁場I Gauβ)を示し1
本発明の磁気シールド構造体10によれば1層構造体に
比べて磁気シールド性を格段に向りできることが認めら
れる。なお、第3図の縦軸の漏洩磁束比は、純鉄による
1層構造体の場合の漏洩磁束を 100とした時の比で
ある。
Next, the degree of leakage of the internal magnetic field to the outside is shown in FIG. 3, where a steady magnetic field of I Gauβ was generated as the external magnetic field. That is, Figure 3 shows the leakage magnetic flux (external magnetic field I Gauβ) outside when an internal magnetic field is applied.
According to the magnetic shield structure 10 of the present invention, it is recognized that magnetic shielding properties can be improved significantly compared to a single layer structure. Note that the leakage magnetic flux ratio on the vertical axis in FIG. 3 is the ratio when the leakage magnetic flux in the case of a single layer structure made of pure iron is set to 100.

表1は外部交番磁場の内部への漏洩度を、1層シールド
構造体(従来例および比較例)と3層シールド構造体(
本発明例)のそれぞれについて実験した結果である。3
M!シールド構造体によれば、1層シールド4m造体に
比べて著しく優れた磁気シールド性能が得られることが
認められる。
Table 1 shows the degree of leakage of the external alternating magnetic field into the interior of the one-layer shield structure (conventional example and comparative example) and the three-layer shield structure (
These are the results of experiments for each of the invention examples). 3
M! According to the shield structure, it is recognized that a significantly superior magnetic shielding performance can be obtained compared to a 4-m single-layer shield structure.

したがって1本発明によれば1例えばNMR−CT等の
ような装置の測定精度を高めることができ、またそれら
装置の設置にあたって周辺環境への磁気的配慮が軽減で
きる。
Therefore, according to the present invention, it is possible to improve the measurement accuracy of devices such as NMR-CT, and to reduce magnetic considerations to the surrounding environment when installing these devices.

なお1本発明の磁気シールド構造体は、常磁性体からな
る内層、最大比透磁率が100以下の物質からなる中間
層、および常磁性体からなる外層の少なくとも3I5を
宥するものであればよく、それら各層の内外に他の層を
備えた4層以上からなるものであってもよむ蔦。
Note that the magnetic shielding structure of the present invention only needs to satisfy at least 3I5 of an inner layer made of a paramagnetic material, an intermediate layer made of a substance with a maximum relative magnetic permeability of 100 or less, and an outer layer made of a paramagnetic material. , even if it consists of four or more layers with other layers inside and outside each layer.

〔発明の効果〕〔Effect of the invention〕

以上のように1本発明によれば、外部磁場およびその変
化に対する磁気シールド性を確実に向上することができ
る。
As described above, according to one aspect of the present invention, magnetic shielding properties against external magnetic fields and changes thereof can be reliably improved.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明装置の一例を示す模式図、第2図は外部
交番磁場を付与した時の内部における磁束変化率を示す
線図、第3図は内油磁場を付与した時の外部における漏
洩磁束を□示す線図である。 10・・・磁気シールド構造体。 11・・・内層シールド体。 12・・・外層シールド体。 13・・・中間層シールド体。 代理人 弁理士  塩 川 修 治 第1 図 第2図 中間層、oFtの最大比透磁率
Figure 1 is a schematic diagram showing an example of the device of the present invention, Figure 2 is a diagram showing the internal magnetic flux change rate when an external alternating magnetic field is applied, and Figure 3 is a diagram showing the external magnetic flux rate when an internal oil magnetic field is applied. It is a diagram showing leakage magnetic flux. 10...Magnetic shield structure. 11... Inner layer shield body. 12...Outer layer shield body. 13...Middle layer shield body. Agent Patent Attorney Osamu Shiokawa Figure 1 Figure 2 Intermediate layer, maximum relative permeability of oFt

Claims (1)

【特許請求の範囲】[Claims] (1)磁場の影響を遮弊するために設けられる磁気シー
ルド構造体において、常磁性体からなる内層、最大比透
磁率が100以下の物質からなる中間層、および常磁性
体からなる外層の少なくとも3層を有してなることを特
徴とする磁気シールド構造体。
(1) In a magnetic shield structure provided to block the influence of a magnetic field, at least an inner layer made of a paramagnetic material, an intermediate layer made of a substance with a maximum relative magnetic permeability of 100 or less, and an outer layer made of a paramagnetic material. A magnetic shielding structure comprising three layers.
JP62268091A 1987-10-26 1987-10-26 Magnetic shielding structure body Pending JPH01111400A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62268091A JPH01111400A (en) 1987-10-26 1987-10-26 Magnetic shielding structure body

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62268091A JPH01111400A (en) 1987-10-26 1987-10-26 Magnetic shielding structure body

Publications (1)

Publication Number Publication Date
JPH01111400A true JPH01111400A (en) 1989-04-28

Family

ID=17453764

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62268091A Pending JPH01111400A (en) 1987-10-26 1987-10-26 Magnetic shielding structure body

Country Status (1)

Country Link
JP (1) JPH01111400A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011030539A1 (en) * 2009-09-11 2011-03-17 パナソニック株式会社 Electromagnetic induction coil unit and electromagnetic induction device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2011030539A1 (en) * 2009-09-11 2011-03-17 パナソニック株式会社 Electromagnetic induction coil unit and electromagnetic induction device

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