JPH01109290A - Magnetic shield apparatus - Google Patents

Magnetic shield apparatus

Info

Publication number
JPH01109290A
JPH01109290A JP62265372A JP26537287A JPH01109290A JP H01109290 A JPH01109290 A JP H01109290A JP 62265372 A JP62265372 A JP 62265372A JP 26537287 A JP26537287 A JP 26537287A JP H01109290 A JPH01109290 A JP H01109290A
Authority
JP
Japan
Prior art keywords
magnetic field
magnetic
electromagnets
coil
lower parts
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
JP62265372A
Other languages
Japanese (ja)
Inventor
Yasuhiro Wada
康弘 和田
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.)
Asahi Chemical Industry Co Ltd
Original Assignee
Asahi Chemical Industry 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 Asahi Chemical Industry Co Ltd filed Critical Asahi Chemical Industry Co Ltd
Priority to JP62265372A priority Critical patent/JPH01109290A/en
Publication of JPH01109290A publication Critical patent/JPH01109290A/en
Pending legal-status Critical Current

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  • Details Of Measuring And Other Instruments (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)
  • Shielding Devices Or Components To Electric Or Magnetic Fields (AREA)

Abstract

PURPOSE: To reduce the weight of an entire device by providing a magnetic shielding member made of a ferromagnetic body in parallel with the direction of magnetic field and by surrounding the periphery of a magnetic field to be shielded and providing a plane coil vertical to the direction of magnetic field and at both edges of the magnetic field to be shielded. CONSTITUTION: A plane coil 3 is arranged within a plane that is vertical to the axial core of electromagnets 1A and 1B at the upper and lower parts of the electromagnets 1A and 1B. A current for forming a magnetic field for canceling a magnetic field that is formed at the upper and lower parts of the electromagnets 1A and 1B by the electromagnets 1A and 1B is allowed to flow to the coil 3, thus shielding the leaked magnetic field at the upper and lower parts of the electromagnets 1A and 1B. Also, the coil 3 forms a magnetic field that is in parallel with the magnetic shield member 2B near the coil 3. The magnetic field increases the number of magnetic force lines passing through the inside of the member 2B and further increases magnetic shielding effect.

Description

【発明の詳細な説明】 産業上の利用分野 本発明は、例えば空心型電磁石を利用した核磁気共鳴診
断装置などの磁気利用装置において、その漏洩磁界を効
果的に遮断する装置(:関する。
DETAILED DESCRIPTION OF THE INVENTION Field of Industrial Application The present invention relates to a device (: for example) for effectively blocking leakage magnetic fields in a magnetic field utilization device such as a nuclear magnetic resonance diagnostic device using an air-core electromagnet.

従来の技術 例えば常電導型核磁気共鳴診断装置は撮像に必要な・静
磁界を空心型常電導磁石によって得ている。
Conventional technology, for example, a normal conducting nuclear magnetic resonance diagnostic apparatus uses an air-core normal conducting magnet to obtain the static magnetic field necessary for imaging.

空心型常電導磁石はその中心部に磁界を形成するのと同
時にその周辺にも磁界(以下、漏洩磁界と称す)を形成
する。漏洩磁界は核磁気共鳴診断装置の周辺(:ある機
器に悪影響を及ぼして周辺機器の誤動作や動作の停止を
招く場合がある。例えばペースメーカーは、強い磁界の
中C:置かれると、その機能が停止する。そこで、常電
導型核磁気共鳴診断装置には漏洩磁界を遮断するシール
ドの機能が必要C:なる。
An air-core normally conducting magnet forms a magnetic field at its center and at the same time forms a magnetic field (hereinafter referred to as a leakage magnetic field) around the center. Leakage magnetic fields may have an adverse effect on certain devices around nuclear magnetic resonance diagnostic equipment, causing peripheral equipment to malfunction or stop working.For example, if a pacemaker is placed in a strong magnetic field, its functions may be affected. Therefore, the normal conduction type nuclear magnetic resonance diagnostic apparatus requires a shield function to block the leakage magnetic field.

第ダ図において、核磁気共鳴診断装置の空心型の電磁石
rA、IBはそれらの共通軸芯で上下C;所定の間隔を
以て対向して配設されている。傾斜磁場発生手段、高周
波信号送受信手段などの関連装置は省略され図示されな
い。鉄などの強磁性体の材料よりなる磁気シールド部材
2A、2Bが電磁石IA、1B等の装置全体の周囲を囲
繞して設けられている。
In Fig. D, air-core electromagnets rA and IB of a nuclear magnetic resonance diagnostic apparatus are disposed facing each other with a predetermined interval above and below C; about their common axis. Related devices such as gradient magnetic field generating means and high frequency signal transmitting/receiving means are omitted and not shown. Magnetic shield members 2A and 2B made of a ferromagnetic material such as iron are provided to surround the entire device including electromagnets IA and 1B.

発明が解決しようとする問題点 第ダ図C:おいて、磁気シールド部材2A、2BC:よ
って電磁石外側の磁力線は電磁石IA、IBの軸芯に寄
せられた形の曲線になる。要素すれば、その軸芯に垂直
な方向、すなわち側方の磁気シールド部材2人の左右外
方には磁力線が少なく、漏洩磁界が遮断されている。一
方、その軸芯シュ平行な方向すなわち上方及び下方の磁
気シールド部材2人の上下方向には磁力線が残貿する傾
向となり、それらの磁力線は上方及び下方の磁気シール
ド部材2Bζ:はぼ垂直に投射されるので、これらによ
って遮断されがたく、漏洩磁界を所定のレベル(1弱め
ることが困難であった。これを少しでも低減するために
磁気シールド部材の−厚さを厚くしたりしているが、そ
の重量増加の割シーは磁気シールド効果の増加は小さい
(例えば厚さを二倍−二シても磁気シールド効果は二倍
にならない。。磁気シールド部材の重量増加は例えば核
磁気共鳴診断装置全体の重量増加を招来し、病院など(
;設置する際に大きな障害になることがある。
Problems to be Solved by the Invention In Figure C, the lines of magnetic force outside the electromagnets form a curved line centered around the axes of the electromagnets IA and IB. Specifically, there are few lines of magnetic force in the direction perpendicular to the axis, that is, on the left and right sides of the two lateral magnetic shield members, and leakage magnetic fields are blocked. On the other hand, lines of magnetic force tend to remain in the direction parallel to the axis, that is, in the vertical direction of the two upper and lower magnetic shield members, and these lines of magnetic force are projected almost perpendicularly to the upper and lower magnetic shield members 2Bζ. Therefore, it is difficult to be blocked by these, and it is difficult to weaken the leakage magnetic field to a predetermined level (1. However, the increase in the weight of the magnetic shielding member is small, but the increase in the magnetic shielding effect is small (for example, even if the thickness is doubled, the magnetic shielding effect will not be doubled.) This may lead to an increase in overall weight, such as in hospitals (
;It may become a major obstacle during installation.

問題を解決するための手段 本発明は、強磁性体よりなる磁気シールド部材が磁界方
向に平行(;且つシールドすべき磁界の周囲を囲繞して
設けられ、平面コイルが磁界方向に垂直に且つシールド
すべき磁界の両端に配設されていることを特徴とする磁
気シールド装置である。
Means for Solving the Problems The present invention provides a magnetic shield member made of a ferromagnetic material that is provided parallel to the direction of the magnetic field (and surrounding the magnetic field to be shielded), and a planar coil that is perpendicular to the direction of the magnetic field and that surrounds the magnetic field to be shielded. This is a magnetic shielding device characterized in that it is disposed at both ends of a magnetic field to be generated.

強磁性体とは、磁界中におかれたときに磁化する性質の
大きなものであり、例えば鉄系の材料である。
A ferromagnetic material is a material that has a strong property of becoming magnetized when placed in a magnetic field, and is, for example, an iron-based material.

作用 電磁石IA、IBの軸芯方向に平行に設けられている磁
気シールド部材は、その長手方向が磁力線と長い区間に
亘って平行しているので、磁界l:垂直な方向の漏洩磁
界を効果的に遮断する。一方、磁界方向に垂直嬬二設け
られている平面コイルは、磁界に平行な方向の漏洩磁界
をキャンセルして、結果的に漏洩磁界を遮断する。
The magnetic shielding member, which is provided parallel to the axial direction of the working electromagnets IA and IB, has its longitudinal direction parallel to the lines of magnetic force over a long section, so that the magnetic field l: effectively reduces the leakage magnetic field in the perpendicular direction. cut off. On the other hand, the two planar coils provided perpendicularly to the direction of the magnetic field cancel out the leakage magnetic field in the direction parallel to the magnetic field, thereby blocking the leakage magnetic field.

実施例 ■ 第7図e:示す実施例シ:おいて、°題磁石IA、
IBの上方及び下方に装置される磁気シールド部材2B
は円盤状の形状をしているが、中央部に孔があるような
ドーナツ状の形状であってもよい。
Example ■ Fig. 7 e: Example shown: In the case of the title magnet IA,
Magnetic shielding member 2B installed above and below IB
Although it has a disk-like shape, it may also have a donut-like shape with a hole in the center.

この形状寸法の主な決定要因は、例えば核磁気共鳴診断
装置の場合、必要とされる電磁石IA、IBの内部の磁
界均一性である。平面コイル3は電磁石IA、IBの上
方及び下方で、電磁石IA。
The main determining factor for this geometry is, for example in the case of a nuclear magnetic resonance diagnostic apparatus, the required magnetic field homogeneity inside the electromagnets IA, IB. The planar coil 3 is located above and below the electromagnets IA and IB.

1Bの軸芯1二垂直な平面内に配置されている。平面コ
イル3の形状は磁気シールド部材2Bの形状シ:合わせ
ることが望ましいが、若干ずれていても差し支えない。
The axis 1 of 1B is arranged in two perpendicular planes. It is desirable that the shape of the planar coil 3 match the shape of the magnetic shielding member 2B, but there is no problem even if the shape is slightly deviated.

平面コイル36:は、電磁石IA。Planar coil 36: is electromagnet IA.

lBがその上方及び下方で形成する磁界を打ち消すよう
な磁界を形成するような電流を流してやる。
A current is applied to create a magnetic field that cancels the magnetic field created by IB above and below it.

こうすること(:より電磁石IA、IBの上方及び下方
での漏洩磁界は遮断される。また平面コイル3はその近
傍i二磁気シールド部材2Bと平行に磁界を形成する。
By doing this, leakage magnetic fields above and below the electromagnets IA and IB are blocked.Furthermore, the planar coil 3 forms a magnetic field parallel to the magnetic shielding member 2B in its vicinity.

この磁界は磁気シールド部材2Bの内部を通過する磁力
線の数を増やし、磁気シール、ド効果をさらに増加する
This magnetic field increases the number of lines of magnetic force passing through the inside of the magnetic shielding member 2B, further increasing the magnetic shielding effect.

■ 第2図に実施例を示す。平面コイル3は磁気シール
ド部材2Bの電磁石IA、IB側、すなわち内側4:配
置される。平面コイル3に流す電流は■の場合と逆方向
(磁流してやる。この方向は■の場合と同じく磁気シー
ルド部材2Bの内側の磁力線の数を増加する方向である
。磁気シールド部材2Bが■と同様にその内部を通過す
る磁力線の数を増加し、結果的に磁気シールド効果を増
加して漏洩磁界を遮断することができる。但し、平面コ
イル3単体が電磁石IA%IBの軸芯上C:形成する磁
界は電磁石IA、IBの漏洩磁界と同じ方向なので磁界
を打ち消す効果はなく、そのため得られる磁気シールド
効果は■の場合よりも劣る。
■ Fig. 2 shows an example. The planar coil 3 is arranged on the electromagnet IA, IB side of the magnetic shielding member 2B, that is, on the inside 4:. The current flowing through the planar coil 3 is in the opposite direction (magnetic flow) to that in the case (■). This direction is the direction that increases the number of magnetic lines of force inside the magnetic shielding member 2B as in the case (■). Similarly, it is possible to increase the number of magnetic lines of force passing through the inside, and as a result, increase the magnetic shielding effect and block the leakage magnetic field.However, the planar coil 3 alone is located above the axis of the electromagnet IA%IB: Since the formed magnetic field is in the same direction as the leakage magnetic field of the electromagnets IA and IB, there is no effect of canceling the magnetic field, and therefore the obtained magnetic shielding effect is inferior to the case (2).

■ 第3図に実施例を示す。平面コイル3は■■と同様
礪;配置されている。その形状は円環形状が望ましいが
、必ずしも円環形状である必要はなく、例えば磁気シー
ルド部材2人を電磁石lA、IBの軸芯方向からみた形
状に合わせた形でよい。平面コイル3に■と同様4:゛
磁流を流してやる。こうすること4二より電磁石IA、
IBの上方及び下方での漏洩磁界は打ち消される。
■ Fig. 3 shows an example. The planar coil 3 is arranged in the same manner as in ■■. The shape is preferably an annular shape, but it does not necessarily have to be an annular shape; for example, the shape of the two magnetic shielding members may be matched to the shape seen from the axial direction of the electromagnets IA and IB. 4: Let a magnetic current flow through the planar coil 3 in the same way as in ■. By doing this 42, the electromagnet IA,
The leakage fields above and below the IB are canceled out.

効果 本発明は、磁気シールド部材と平面コイルの協同作用(
;よって磁気シールド効果が顕著であり、例えば核磁気
共鳴診断装置において漏洩磁界を効果的に遮断すること
C=よって系外へ漏洩磁界悪影響を著減し、装置全体重
量を軽減できることからして病院などの建造物の構成材
に掛ける負担も小さくて済む効果を有する。
Effect The present invention has a cooperative effect (
Therefore, the magnetic shielding effect is remarkable, and for example, in nuclear magnetic resonance diagnostic equipment, leakage magnetic fields can be effectively blocked. Therefore, the negative effects of leakage magnetic fields outside the system can be significantly reduced, and the overall weight of the equipment can be reduced, making it suitable for hospitals. This has the effect of reducing the burden placed on the constituent materials of buildings such as.

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

第7図は本発明の実施例の模式断面図、第2図は別の実
施例の模式断面図、第3図は更に別の模式断面図、第9
図は従来の磁気シールド装置の1例を示す模式断面図で
ある。 1−・・電磁石、2・・・磁気シールド部材、3・・・
平面コイル 特許出願人 旭化成工業株式会社 第1図 第2図 第3図
FIG. 7 is a schematic sectional view of an embodiment of the present invention, FIG. 2 is a schematic sectional view of another embodiment, FIG. 3 is yet another schematic sectional view, and FIG.
The figure is a schematic cross-sectional view showing an example of a conventional magnetic shielding device. 1-...Electromagnet, 2...Magnetic shielding member, 3...
Planar coil patent applicant Asahi Kasei Industries, Ltd. Figure 1 Figure 2 Figure 3

Claims (1)

【特許請求の範囲】[Claims]  強磁性体よりなる磁気シールド部材が磁界方向に平行
に且つシールドすべき磁界の周囲を囲繞して設けられ、
平面コイルが磁界方向に垂直に且つシールドすべき磁界
の両端に配設されていることを特徴とする磁気シールド
装置。
A magnetic shielding member made of a ferromagnetic material is provided parallel to the direction of the magnetic field and surrounding the magnetic field to be shielded,
A magnetic shielding device characterized in that planar coils are arranged perpendicular to the direction of the magnetic field and at both ends of the magnetic field to be shielded.
JP62265372A 1987-10-22 1987-10-22 Magnetic shield apparatus Pending JPH01109290A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62265372A JPH01109290A (en) 1987-10-22 1987-10-22 Magnetic shield apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62265372A JPH01109290A (en) 1987-10-22 1987-10-22 Magnetic shield apparatus

Publications (1)

Publication Number Publication Date
JPH01109290A true JPH01109290A (en) 1989-04-26

Family

ID=17416265

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62265372A Pending JPH01109290A (en) 1987-10-22 1987-10-22 Magnetic shield apparatus

Country Status (1)

Country Link
JP (1) JPH01109290A (en)

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