JPS62183752A - Uniform magnetic field magnet for nuclear magnetic resonancediagnostic apparatus - Google Patents

Uniform magnetic field magnet for nuclear magnetic resonancediagnostic apparatus

Info

Publication number
JPS62183752A
JPS62183752A JP61025340A JP2534086A JPS62183752A JP S62183752 A JPS62183752 A JP S62183752A JP 61025340 A JP61025340 A JP 61025340A JP 2534086 A JP2534086 A JP 2534086A JP S62183752 A JPS62183752 A JP S62183752A
Authority
JP
Japan
Prior art keywords
magnetic field
uniform magnetic
correction
magnet
uniform
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.)
Granted
Application number
JP61025340A
Other languages
Japanese (ja)
Other versions
JPH043218B2 (en
Inventor
春雄 小野
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric 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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP61025340A priority Critical patent/JPS62183752A/en
Publication of JPS62183752A publication Critical patent/JPS62183752A/en
Publication of JPH043218B2 publication Critical patent/JPH043218B2/ja
Granted legal-status Critical Current

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  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の属する技術分野〕 不発明は、核磁気共鳴診断装置(以下NMR−CTと略
称する)用均−磁場マグネット、ことに均一磁場補正用
コイルの構造配置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Technical field to which the invention pertains] The present invention relates to a uniform magnetic field magnet for a nuclear magnetic resonance diagnostic apparatus (hereinafter abbreviated as NMR-CT), and particularly to a structural arrangement of a uniform magnetic field correction coil.

〔従来技術とその問題点〕[Prior art and its problems]

第1図は従来技術の一例を示す永久磁石形均−磁場マグ
ネットの側断面図であり、直径りなる円板状の一対の永
久磁石2A 、2Bが方形筒状に形成された継鉄5の内
壁面に平行かつ同心状に固定されており、永久磁石2A
、2Bそれぞれには直径りが永久磁石のそれに等しい円
板状の補正極6A、3Bが密接配置され、さらに補正極
3A、3Bの周縁部にはそれぞれ反永久磁石側に突出し
た三角形断面を有する環状突起4A 、4Bが設けられ
て一対の磁極iA、1Bが形成され、一対の磁極1A、
iB間の間隙の中央部の直径400m+n程度のエリア
内に磁場の強さが0,05ないし0.3 T、磁場の強
さの均一度が数1QPPM以下の均一磁場10を発生す
るよう構成されている。
FIG. 1 is a side cross-sectional view of a permanent magnet-type uniform magnetic field magnet showing an example of the prior art, in which a pair of disk-shaped permanent magnets 2A and 2B with diameters are arranged in a yoke 5 formed into a rectangular cylindrical shape. It is fixed parallel and concentrically to the inner wall surface, and has a permanent magnet of 2A.
, 2B are closely arranged with disk-shaped correction poles 6A and 3B whose diameter is equal to that of the permanent magnet, and furthermore, the peripheral edges of the correction poles 3A and 3B each have a triangular cross section protruding toward the side opposite to the permanent magnet. Annular protrusions 4A and 4B are provided to form a pair of magnetic poles iA and 1B, and a pair of magnetic poles 1A and 1B are formed.
It is configured to generate a uniform magnetic field 10 with a magnetic field strength of 0.05 to 0.3 T and a uniformity of the magnetic field strength of several QPPM or less in an area with a diameter of about 400 m + n at the center of the gap between the iBs. ing.

前述のように構成された均一磁場マグネットにおいては
、永久磁石2A、2Bの磁化の強さが局部的に異なるこ
とによって生ずる均一磁場の乱れは強磁性材からなる補
正極によって均等化され、また磁極1A、 1Bの側方
に漏れる漏れ磁界は環状突起4A 、4Bによって抑制
されて、均一磁場10の均一度をかなシ高めることがで
きる。しかしながら磁場の均一度110PPM程度にま
で高めるためには磁極1A、iBの直径りが非常に大き
くなるという問題がめるために、一対の磁極1A、iB
間に均一磁場微調整用の一対の補正コイル6A 、6B
t−設けることによシ、直径りの増大を抑制しつつ磁場
の均一度を高めるよう構成したものが知られている。し
かしながら、従来装置においては一対の補正コイル6を
環状突起4A、4B間の間隙中に突出した位置に配して
いるために、均一磁場10内に人体を搬入するに必要な
間隙長ルが補正コイル6A、6Bによって制約され、そ
の結果一対の磁石2A 、2B間の磁石間距離Hが必然
的に増大する。均一磁場10の均一度を110PP程度
に高度に保持するためには、磁極1人、1Bの直径りを
磁石間距離Hの2倍以上とすることが必要であり、補正
コイル6を設けたために磁石間距離Hが増大すると、磁
極直径りが増大して永久磁石2A、2Bの総発生磁束量
および高価な永久磁石材の部用量の増大、ならびに継鉄
5の磁路長の増大を招くとともに、総発生磁束量の増大
によって継鉄5の断面積が増大するなどの悪循環を生じ
、その結果、舊−磁場マグネットが大形かつ高重量化す
るという欠点があり、その改善が求められている。
In the uniform magnetic field magnet configured as described above, disturbances in the uniform magnetic field caused by locally different magnetization strengths of the permanent magnets 2A and 2B are equalized by the correction pole made of ferromagnetic material, and the magnetic pole The leakage magnetic field leaking to the sides of 1A and 1B is suppressed by the annular protrusions 4A and 4B, and the uniformity of the uniform magnetic field 10 can be greatly improved. However, in order to increase the uniformity of the magnetic field to about 110 PPM, the diameter of the magnetic poles 1A and iB becomes very large.
A pair of correction coils 6A and 6B for fine adjustment of the uniform magnetic field are installed between them.
A structure is known in which the uniformity of the magnetic field is increased while suppressing an increase in diameter by providing a magnetic field. However, in the conventional device, since the pair of correction coils 6 are disposed in a protruding position in the gap between the annular protrusions 4A and 4B, the gap length required to bring the human body into the uniform magnetic field 10 is corrected. This is restricted by the coils 6A and 6B, and as a result, the distance H between the pair of magnets 2A and 2B inevitably increases. In order to maintain the uniformity of the uniform magnetic field 10 at a high level of about 110PP, it is necessary to make the diameter of each magnetic pole 1B more than twice the distance H between the magnets, and by providing the correction coil 6. As the distance H between the magnets increases, the magnetic pole diameter increases, resulting in an increase in the total amount of magnetic flux generated by the permanent magnets 2A and 2B, an increase in the amount of expensive permanent magnet material, and an increase in the magnetic path length of the yoke 5. , an increase in the total amount of generated magnetic flux causes a vicious cycle such as an increase in the cross-sectional area of the yoke 5, and as a result, there is a drawback that the magnetic field magnet becomes larger and heavier, and there is a need to improve this problem. .

〔発明の目的〕[Purpose of the invention]

本発明は前述の状況に鑑みてなされたもので、補正コイ
ルを配したことによる磁石間距離の増大が排除され、し
たがって磁場の均一度が高く小形、@量かつ安価な核磁
気共鳴診断装置用均一磁場マグネットを提供することを
目的とする。
The present invention has been made in view of the above-mentioned situation, and eliminates the increase in the distance between the magnets due to the arrangement of correction coils, and therefore has a high degree of uniformity of the magnetic field, and is suitable for use in small, small, and inexpensive nuclear magnetic resonance diagnostic equipment. The purpose is to provide a uniform magnetic field magnet.

〔発明の要点〕[Key points of the invention]

本発明の目的は、補正コイルを環状突起によって包囲さ
れた補正極の凹所に配役可能な大きさに形成して前記凹
所を補正コイルの設置スペースとして利用するよう構成
したことにより達成されたものである。
The object of the present invention has been achieved by forming a correction coil to a size that allows it to be placed in a recess of a correction pole surrounded by an annular projection, and using the recess as an installation space for the correction coil. It is something.

〔発明の実施例〕[Embodiments of the invention]

以下本発明を実施例技基づいて説明する。 The present invention will be explained below based on examples.

第1図は本発明の実施例を示す概略側断面図、第2図は
第1図におけるA−A方向の水平断面図である。図にお
いて、方形筒状に形成された継鉄5の内壁面に平行かつ
同心状に固定された円板状の永久磁石2A 、2Bおよ
び補正極3A 、3Bからなる一対の磁極1A、1Bに
は、三角形断面を有する環状突起4A 、4Bによって
それぞれ包囲された補正極3A、、Bの凹所7内に、円
板状の補正コイル16A、16Bが配されておシ、一対
の補正コイル16の外径を磁極IA、1Bの直径りよシ
小さく形成することによって凹所7を補正コイル1(S
A、16Bの設置スペースとして利用することが可能と
なり、補正コイル16A、16Bが環状突起4A 、4
B間の間隙中に突出するのを回避できる。したがって、
環状突起間の間隙を人体の搬入に必要な間隙長りとする
ことができるので、補正コイルを配したことによる磁石
間距離Hの増大を完全に排除することができる。
FIG. 1 is a schematic side sectional view showing an embodiment of the present invention, and FIG. 2 is a horizontal sectional view taken along the line A--A in FIG. In the figure, a pair of magnetic poles 1A and 1B consisting of disk-shaped permanent magnets 2A and 2B and correction poles 3A and 3B are fixed concentrically and parallel to the inner wall surface of a rectangular yoke 5. , disk-shaped correction coils 16A, 16B are disposed in the recesses 7 of the correction poles 3A, 3A, 4B surrounded by annular protrusions 4A, 4B each having a triangular cross section. By forming the outer diameter smaller than the diameter of the magnetic poles IA and 1B, the recess 7 is
A, 16B can be used as the installation space, and the correction coils 16A, 16B can be used as the installation space for the annular projections 4A, 4.
It is possible to avoid protruding into the gap between B. therefore,
Since the gap between the annular protrusions can be set to a length necessary for carrying in a human body, an increase in the distance H between the magnets due to the provision of the correction coil can be completely eliminated.

前述のように構成された均一磁場マグネットにおいては
、補正コイルに流す電流を制御することによシ均−磁場
10の均一度を微調整でき、したがって磁場の均一度を
高められるとともに、磁石間距離Hを磁極lA、 1B
によって決まる最適寸法とすることができるので、磁石
間距離Hの増大に伴って生ずる磁極面積、永久磁石材の
使用量。
In the uniform magnetic field magnet configured as described above, the uniformity of the uniform magnetic field 10 can be finely adjusted by controlling the current flowing through the correction coil, thereby increasing the uniformity of the magnetic field and increasing the distance between the magnets. H as magnetic pole 1A, 1B
As the distance H between the magnets increases, the magnetic pole area and the amount of permanent magnet material used can be set to the optimum size determined by the following.

総発生磁束量、断鉄断面積、断鉄の磁路長などの増大要
因をすべて排除することができる。
It is possible to eliminate all increasing factors such as the total amount of magnetic flux generated, the cross-sectional area of the iron section, and the magnetic path length of the iron section.

第3図は本発明の異なる実施例を示す補正コイルの配置
説明図であシ、第2図に対応する部分を示したものであ
る。図において、補正コイルを長丸状の4個の分割コイ
ル26,27.28.29で構成し、磁極1Bの凹所内
に4個のコイルを井桁状に組み合わせた状態で配設した
点が前述の実施例と異なっておシ、4個の補正コイル2
6,27.28.29に流す電流の向きおよび大きさを
個々に制御することKよシ、均一磁場10の磁場の均一
度をよシ木目細かく制御することができもなお、補正コ
イルの形状1寸法、数などは磁極1A、iBによって発
生する磁場の不均一性を勘案してその補正に好適な条件
を選択すべきことはいうまでもないことである。
FIG. 3 is an explanatory diagram of the arrangement of a correction coil showing a different embodiment of the present invention, and shows a portion corresponding to FIG. 2. In the figure, the correction coil is composed of four divided coils 26, 27, 28, and 29 in an oblong shape, and the four coils are arranged in a parallel cross shape in the recess of the magnetic pole 1B as described above. In contrast to the embodiment, four correction coils 2 are used.
6, 27, 28, and 29, it is possible to control the uniformity of the magnetic field of the uniform magnetic field 10 more precisely, but it is also possible to control the shape of the correction coil. It goes without saying that the dimensions, number, etc. should be selected in consideration of the non-uniformity of the magnetic field generated by the magnetic poles 1A and iB, and conditions suitable for correction thereof should be selected.

また、前述の各実施例においては永久磁石形均−磁場マ
グネットへの適用例について説明した力ζ電磁石形均−
磁場マグネットへの適用も前述の説明に基づいて容易に
実施することができる。
In addition, in each of the above-mentioned embodiments, the force ζ electromagnet type uniformity magnet described with respect to an example of application to a permanent magnet type uniform magnetic field magnet.
Application to magnetic field magnets can also be easily implemented based on the above explanation.

〔発明の効果〕〔Effect of the invention〕

本発明は前述のように、補正コイルを環状突起で包囲さ
れた補正極の凹所に収納し得る大きさに形成し、凹所を
補正コイルの設置スペースに利用するよう構成した。そ
の結果、従来技術において補正コイルを環状突起間の間
隙中に突設したことによシ問題となった磁石間距離の増
大が回避され磁石間距離の増大に伴なって生ずる磁極面
積、総磁束発生蓋、永久磁石材の使用量の増大が阻止さ
れ、一対の磁極を小形、軽量かつ安価に形成することが
可能になシ、また磁石間距離の増大が継鉄の断面積およ
び磁路長の増大に及ぼす影響も排除され、したがって小
形化、軽量化された核磁気共鳴診断装置用均一磁場マグ
ネットを提供することができる。また補正コイルによる
磁場の強さの均一度の向上効果が得られ、かつ小形、軽
量化されることによシ設置場所への運搬、搬入の容易化
、ならびに設置場所の省スペース化などにも貢献するこ
とかできる。
As described above, the present invention is configured such that the correction coil is formed in a size that can be accommodated in the recess of the correction pole surrounded by the annular protrusion, and the recess is used as the installation space for the correction coil. As a result, the problem of increasing the distance between the magnets due to the correction coil protruding into the gap between the annular protrusions in the prior art is avoided, and the magnetic pole area and total magnetic flux that occur with the increase in the distance between the magnets can be avoided. This prevents an increase in the amount of permanent magnet material used, making it possible to form a pair of magnetic poles in a small, lightweight, and inexpensive manner.In addition, an increase in the distance between the magnets reduces the cross-sectional area of the yoke and the length of the magnetic path. The influence on the increase in the magnetic field is also eliminated, so that it is possible to provide a uniform magnetic field magnet for a nuclear magnetic resonance diagnostic apparatus that is smaller and lighter in weight. In addition, the correction coil improves the uniformity of the magnetic field strength, and its small size and weight make it easier to transport and bring in to the installation site, as well as save space at the installation site. I can make a contribution.

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

第1図は本発明の実施例を示す概略側断面図、第2図は
第1図におけるA−A方向の水平断面図、第6図は異な
る実施例を示す補正コイルの配置説明図、第4図は従来
の永久磁石形均−磁場マグネットの概略側断面図である
。 iA、1B・・・磁極、2A、2B・・・永久磁石、6
A、5B・・・補正極、4A、4B・・・環状突起、5
・・・継鉄、6.6A 、6B・・・補正コイル、7・
・・凹所、16.16A、16B・・・補正コイル、1
0・・・均一磁場、26,27,28,29・・・補正
コイル(分j・     ・  ・。  ・−l・・、
′」グ第2図 第3図 A +−一 第4図
FIG. 1 is a schematic side sectional view showing an embodiment of the present invention, FIG. 2 is a horizontal sectional view taken along the line A-A in FIG. FIG. 4 is a schematic side sectional view of a conventional permanent magnet type uniform magnetic field magnet. iA, 1B...Magnetic pole, 2A, 2B...Permanent magnet, 6
A, 5B... Correction pole, 4A, 4B... Annular projection, 5
...Yoke, 6.6A, 6B...Correction coil, 7.
...Recess, 16.16A, 16B...Correction coil, 1
0... Uniform magnetic field, 26, 27, 28, 29... Correction coil (minute j... ・-l...,
Figure 2 Figure 3 A +-1 Figure 4

Claims (1)

【特許請求の範囲】[Claims] 1)均一磁場空間を隔てて互いに平行かつ同心状に継鉄
に支持された一対の円板状の磁石と、この磁石それぞれ
の表面に密接して配され円板状の周縁部に反磁石側に突
出した環状突起を有する均一磁場の補正極とを備えたも
のにおいて、均一磁場調整用の補正コイルが前記環状突
起で包囲された前記補正極の凹所それぞれに配されたこ
とを特徴とする核磁気共鳴診断装置用均一磁場マグネッ
ト。
1) A pair of disc-shaped magnets supported by a yoke in parallel and concentrically with each other across a uniform magnetic field space, and a counter-magnet side arranged closely on the surface of each magnet and on the peripheral edge of the disc-shaped part. and a correction pole for a uniform magnetic field having an annular protrusion projecting therein, characterized in that a correction coil for adjusting the uniform magnetic field is disposed in each recess of the correction pole surrounded by the annular protrusion. Uniform magnetic field magnet for nuclear magnetic resonance diagnostic equipment.
JP61025340A 1986-02-07 1986-02-07 Uniform magnetic field magnet for nuclear magnetic resonancediagnostic apparatus Granted JPS62183752A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61025340A JPS62183752A (en) 1986-02-07 1986-02-07 Uniform magnetic field magnet for nuclear magnetic resonancediagnostic apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61025340A JPS62183752A (en) 1986-02-07 1986-02-07 Uniform magnetic field magnet for nuclear magnetic resonancediagnostic apparatus

Publications (2)

Publication Number Publication Date
JPS62183752A true JPS62183752A (en) 1987-08-12
JPH043218B2 JPH043218B2 (en) 1992-01-22

Family

ID=12163175

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61025340A Granted JPS62183752A (en) 1986-02-07 1986-02-07 Uniform magnetic field magnet for nuclear magnetic resonancediagnostic apparatus

Country Status (1)

Country Link
JP (1) JPS62183752A (en)

Also Published As

Publication number Publication date
JPH043218B2 (en) 1992-01-22

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