JPH02184003A - Magnetic field generator for mri - Google Patents
Magnetic field generator for mriInfo
- Publication number
- JPH02184003A JPH02184003A JP1004392A JP439289A JPH02184003A JP H02184003 A JPH02184003 A JP H02184003A JP 1004392 A JP1004392 A JP 1004392A JP 439289 A JP439289 A JP 439289A JP H02184003 A JPH02184003 A JP H02184003A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- shaped
- magnetic
- magnetic pole
- plate
- 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
Links
- 230000005415 magnetization Effects 0.000 claims description 5
- 230000004907 flux Effects 0.000 abstract description 13
- 230000003068 static effect Effects 0.000 abstract description 3
- 239000000470 constituent Substances 0.000 abstract 2
- 239000000126 substance Substances 0.000 abstract 1
- XEEYBQQBJWHFJM-UHFFFAOYSA-N Iron Chemical compound [Fe] XEEYBQQBJWHFJM-UHFFFAOYSA-N 0.000 description 5
- 230000000694 effects Effects 0.000 description 3
- 229910052742 iron Inorganic materials 0.000 description 3
- 239000000463 material Substances 0.000 description 3
- 230000007423 decrease Effects 0.000 description 2
- 230000003247 decreasing effect Effects 0.000 description 2
- 238000009434 installation Methods 0.000 description 2
- 238000005481 NMR spectroscopy Methods 0.000 description 1
- 229910052779 Neodymium Inorganic materials 0.000 description 1
- 229910052777 Praseodymium Inorganic materials 0.000 description 1
- 229910000828 alnico Inorganic materials 0.000 description 1
- 239000010941 cobalt Substances 0.000 description 1
- 229910017052 cobalt Inorganic materials 0.000 description 1
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 description 1
- 238000010276 construction Methods 0.000 description 1
- 238000005516 engineering process Methods 0.000 description 1
- 239000000696 magnetic material Substances 0.000 description 1
- 230000002093 peripheral effect Effects 0.000 description 1
- 230000035699 permeability Effects 0.000 description 1
- 229910052761 rare earth metal Inorganic materials 0.000 description 1
- 150000002910 rare earth metals Chemical class 0.000 description 1
- 230000001846 repelling effect Effects 0.000 description 1
- 238000003325 tomography Methods 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
Landscapes
- Magnetic Resonance Imaging Apparatus (AREA)
Abstract
Description
【発明の詳細な説明】
利用産業分野
この発明は、対象物の断面イメージを得て組織の性質ま
で描き出すことのできる医療用核磁気共鳴断層撮影装置
(以下MRIという)等に用いられる永久磁石を使用し
た磁界発生装置に係り、複数の柱状継鉄で支持される一
対の板状継鉄が長方形からなる構成において、板状継鉄
の長辺側と短辺側とで、漏洩磁束量が異なり空隙内の磁
界均一度が低下するのを、短辺側に空隙を介して対向す
る一対の磁界調整用磁石を配置して防止したMRI用磁
界発生装置に関する。[Detailed Description of the Invention] Field of Application This invention relates to a permanent magnet used in medical nuclear magnetic resonance tomography equipment (hereinafter referred to as MRI), etc., which can obtain cross-sectional images of objects and depict the properties of tissues. Regarding the magnetic field generator used, in a configuration where a pair of plate yokes supported by multiple columnar yokes are rectangular, the amount of leakage magnetic flux is different between the long side and short side of the plate yoke. The present invention relates to a magnetic field generation device for MRI in which a pair of magnetic field adjustment magnets are disposed on the short side facing each other with a gap interposed therebetween to prevent the magnetic field uniformity within the gap from decreasing.
背景技術
MHIに用いる磁界発生装置として、第4図に示す如く
、装置の小型化を達成するために、通常、Fe−B−R
系磁石を用いた一対の永久磁石構成体(IXI)の各々
の一方端に磁極片(2X2)を固着して対向させ、他方
端を後述する継鉄(3)にて連結し、磁極片(2X2)
間の空隙(4)内に、静磁界を発生させる構成が知られ
ている。BACKGROUND ART As shown in FIG. 4, as a magnetic field generating device used in MHI, in order to achieve miniaturization of the device, Fe-B-R is usually used.
A magnetic pole piece (2X2) is fixed to one end of each of a pair of permanent magnet structures (IXI) using system magnets, facing each other, and the other end is connected with a yoke (3) described later to form a magnetic pole piece ( 2X2)
A configuration is known in which a static magnetic field is generated in the air gap (4) between the two.
磁極片(2X2)には、空隙(4)内における磁界分布
の均一度を向上するために、周辺部に環状突起(5)を
設けである。The magnetic pole piece (2X2) is provided with an annular protrusion (5) at its periphery in order to improve the uniformity of the magnetic field distribution within the air gap (4).
永久磁石構成体(IXI)を磁気的に結合している継鉄
(3)は、特に、開口部の幅を大きくとり、奥行きを狭
くすることにより、被検者への圧迫感を軽減し、かつ既
設の病院等への搬入を容易にするため、一対の長方形の
板状継鉄(3aX3a)を所要空隙を形成する所定長さ
の4本の柱状継鉄(3b)で結合した構成からなる。The yoke (3) that magnetically couples the permanent magnet structure (IXI) has a wide opening and a narrow depth to reduce the feeling of pressure on the subject. In addition, in order to facilitate transportation to existing hospitals, etc., it consists of a pair of rectangular plate yokes (3a x 3a) connected by four columnar yokes (3b) of a predetermined length that form the required gap. .
上記構成からなるMRI用磁界発生装置(以下磁界発生
装置という)において、空隙(4)は被検者の一部また
は全部が挿入できるだけの広さが必要であり、しかも鮮
明な断層イメージを得るためには、通常空隙(4)内に
0.5〜10kGでがっ1xlO−’以下の精度を有す
る安定した強力な均一磁界を形成することが要求される
。In the magnetic field generator for MRI (hereinafter referred to as the magnetic field generator) having the above configuration, the gap (4) must be wide enough to allow part or all of the subject to be inserted, and in order to obtain a clear tomographic image. Generally, it is required to form a stable and strong uniform magnetic field in the air gap (4) with a precision of 0.5 to 10 kG and less than 1×1O−'.
従来技術の問題点
第4図に示す磁界発生装置は、板状継鉄(3aX3a)
が長方形のため、その長辺側と短辺側とで、磁極片(2
)(2)及び永久磁石構成体(IXI)からの漏洩磁束
量が異なり、すなわち、短辺側への漏洩磁束量が多いた
め、空隙(4)内における磁界均一度が低下する問題が
あった。Problems with the prior art The magnetic field generator shown in Fig. 4 is a plate-shaped yoke (3a x 3a).
Since it is rectangular, the long side and short side of the magnetic pole piece (2
) (2) and the permanent magnet structure (IXI) are different, that is, there is a large amount of leakage magnetic flux toward the short side, so there was a problem that the uniformity of the magnetic field in the air gap (4) decreased. .
そこで、磁極片(2X2)及び永久磁石構成体(IXI
)からの漏洩磁束量の違いに基づく磁界均一度の低下を
解消するために、出願人の一人はすでに、継鉄の内面に
漏洩磁束反発用磁石を配置する手段(実開昭61−88
210号公報)、長方形板状継鉄の長辺側に、磁極片に
近接して磁束シャント板を配置する手段(実開昭62−
101205号公報)、長方形板状継鉄の長辺側に、磁
性薄板を当接配置する手段(実開昭62−101206
号公報)、磁極片の環状突起部の所要位置に、磁界調整
片を着設する手段(実開昭62−112106号公報)
、長方形板状継鉄の短辺側対向面の磁束発生量を大とし
た永久磁石を配置する手段(実開昭62−112107
号公報)を提案している。Therefore, the magnetic pole pieces (2X2) and the permanent magnet structure (IXI
), one of the applicants has already proposed a means of arranging leakage flux repelling magnets on the inner surface of the yoke (Utility Model Application No. 61-88).
No. 210), means for arranging a magnetic flux shunt plate on the long side of a rectangular plate-shaped yoke in close proximity to a magnetic pole piece (Utility Model Application No. 62-
101205), means for placing a magnetic thin plate in contact with the long side of a rectangular plate-shaped yoke (Utility Model Application No. 62-101206)
(Japanese Utility Model Publication No. 112106/1983), a means for attaching a magnetic field adjustment piece to a desired position of an annular protrusion of a magnetic pole piece (Japanese Utility Model Publication No. 112106/1983)
, Means for arranging permanent magnets that generate a large amount of magnetic flux on the opposing surfaces of the short sides of rectangular plate-shaped yoke (Utility Model Application No. 62-112107)
(No. Publication).
ところが、上記技術だけでは、断層イメージの鮮明度向
上および装置の小型軽量化など、現在、磁界発生装置に
要求されている諸条件を十分満足することはできない。However, the above-mentioned technology alone cannot sufficiently satisfy the various conditions currently required of magnetic field generating devices, such as improving the clarity of tomographic images and reducing the size and weight of devices.
発明の目的
この発明は、上記現状に鑑み提案するもので、板状継鉄
の長辺側と短辺側とで、漏洩磁束量が異なり空隙内の磁
界均一度が低下するのを解決し、長方形板状継鉄を用い
た磁界発生装置の長所を活かして、断層イメージの鮮明
度向上および装置の小型軽量化を可能にする構成からな
る磁界発生装置の提供を目的とする。Purpose of the Invention The present invention is proposed in view of the above-mentioned current situation, and solves the problem that the amount of leakage magnetic flux is different between the long side and the short side of a plate-shaped yoke, and the uniformity of the magnetic field in the air gap decreases. The object of the present invention is to provide a magnetic field generator having a configuration that makes it possible to improve the clarity of tomographic images and to reduce the size and weight of the device by taking advantage of the advantages of a magnetic field generator using a rectangular plate-shaped yoke.
発明の概要
この発明は、磁界発生装置において、板状継鉄の長辺側
と短辺側との漏洩磁束量の相違の解消を目的に種々検討
した結果、板状継鉄の短辺側に空隙を介して対向させた
特定構成の一対の磁界調整用磁石を設けることにより、
漏洩磁束を減少させ得ることを知見し、この発明を完成
したものである。Summary of the Invention As a result of various studies aimed at eliminating the difference in the amount of leakage magnetic flux between the long side and the short side of a plate-shaped yoke in a magnetic field generation device, the present invention has been developed. By providing a pair of magnetic field adjustment magnets with a specific configuration facing each other with an air gap,
This invention was completed based on the discovery that leakage magnetic flux could be reduced.
すなわち、この発明は、
複数の柱状継鉄を間隔部材として空隙を形成し、かつ磁
気的に接続して対向配置する一対の長方形板状継鉄と、
板状継鉄の各対向面に着設した永久磁石構成体と、該磁
石構成体各対向面に設けた周辺部に環状突起を有する磁
極片とから構成し、該空隙に磁界を発生するMRI用磁
界発生装置において、
対向する磁極片間の中央部で、かつ磁極片の環状突起よ
り外側で長方形板状継鉄の各短辺側に、対の磁界調整用
磁石を磁化方向が前記一対の永久磁石と逆向きとなるよ
うに設けたことを特徴とするMRI用磁界発生装置であ
る。That is, the present invention includes: a pair of rectangular plate yokes that are magnetically connected and arranged to face each other, with a plurality of columnar yokes forming a gap as spacing members;
An MRI device comprising a permanent magnet structure attached to each opposing surface of a plate-shaped yoke, and a magnetic pole piece having an annular projection on the periphery provided on each opposing surface of the magnet structure, and generating a magnetic field in the air gap. In the magnetic field generating device for magnetic field generation, a pair of magnetic field adjustment magnets are installed on each short side of the rectangular plate-shaped yoke at the center between the opposing magnetic pole pieces and outside the annular protrusion of the magnetic pole piece. This is a magnetic field generating device for MRI, characterized in that it is provided in a direction opposite to that of a permanent magnet.
発明の構成
この発明において、磁気回路は、複数の柱状継鉄を間隔
部材として空隙を形成し、かつ磁気的に接続して対向配
置する一対の長方形板状継鉄と、板状継鉄の各え1向面
に着設した永久磁石構成体と、該永久磁石構成体の各対
向面に設けた周辺部に環状突起を有する磁極片とからな
る構成であり、永久磁石の磁気特性、形状寸法、継鉄の
形状寸法及び所要空隙の大きさ等に応じて、構築手段や
その位置等を適宜選定することが望ましい。Structure of the Invention In the present invention, a magnetic circuit includes a pair of rectangular plate-shaped yokes that are magnetically connected and arranged to face each other, with a plurality of columnar yokes forming a gap as spacing members, and each of the plate-shaped yokes. The structure consists of a permanent magnet structure attached to one facing surface, and a magnetic pole piece having an annular projection on the peripheral part provided on each opposing surface of the permanent magnet structure, and the magnetic properties and shape and dimensions of the permanent magnet are It is desirable to appropriately select the construction means, their position, etc., depending on the shape and dimensions of the yoke, the size of the required gap, etc.
この発明において、磁極片は、円板状の電磁軟鉄、純鉄
等の公知の高透磁率磁性材からなり、例えば、磁極片中
央部に、断面台形状の凸状突起を設けたり、磁極片の所
要位置に磁界調整片を着設するなど、磁束を所要空隙に
集中させがつ均一度を向上させる手段を適宜選定するこ
とができる。In this invention, the magnetic pole piece is made of a known high permeability magnetic material such as disc-shaped electromagnetic soft iron or pure iron. It is possible to appropriately select means for concentrating the magnetic flux in a required gap and improving uniformity, such as attaching a magnetic field adjusting piece at a required position.
かかる磁気回路に用いる磁石構成体の永久磁石は、フェ
ライト磁石、アルニコ系磁石、希土類コバルト系磁石が
使用できるが、特に、RとしてNdやPrを中心とする
資源的に豊富な軽希土類を用い、B、 Feを主成分と
して30MGOe以上の極めて高いエネルギー積を示す
、Fe−B−R系永久磁石を使用することにより、著し
く小型化することができる。As the permanent magnet of the magnet structure used in such a magnetic circuit, ferrite magnets, alnico magnets, and rare earth cobalt magnets can be used, but in particular, as R, light rare earths, which are rich in resources, mainly Nd and Pr, are used. By using a Fe--B--R permanent magnet, which is mainly composed of B and Fe and exhibits an extremely high energy product of 30 MGOe or more, it is possible to significantly reduce the size.
さらに、この発明において、継鉄は長方形板状継鉄と柱
状継鉄から構成されるが、長方形板状継鉄の短辺(L)
と長辺(W)との比率W/Lは、被検者の大きさ、設置
場所の広さ、搬送の作業性等を考慮して、通常1.5〜
2.5とする。また、磁極片直径(D)と短辺(L)と
の比率D/Lは、被検者の大きさ、磁界均一度等を考慮
して、通常0.6〜1.0とする。Furthermore, in this invention, the yoke is composed of a rectangular plate-shaped yoke and a columnar yoke, but the short side (L) of the rectangular plate-shaped yoke
The ratio W/L between the long side (W) and the long side (W) is usually 1.5 to 1.5, taking into account the size of the patient, the size of the installation location, the workability of transportation, etc.
Set it to 2.5. Further, the ratio D/L of the pole piece diameter (D) to the short side (L) is usually set to 0.6 to 1.0 in consideration of the size of the subject, magnetic field uniformity, etc.
柱状継鉄は、磁路形成に必要な有効断面積、機械的強度
、組立て安さ、磁気的なバランス等を考慮して選定する
が、通常4本が好ましい。The columnar yokes are selected in consideration of the effective cross-sectional area necessary for forming the magnetic path, mechanical strength, ease of assembly, magnetic balance, etc., and four pieces are usually preferred.
この発明の特徴である磁界調整用磁石は、対向する磁極
片間の中央部で、かつ磁極片の環状突起より外側の長方
形板状継鉄の各短辺側に、一対の磁界調整用磁石を磁化
方向が一対の永久磁石構成体と逆向きとなるように設け
るが、形状は、実施例に示す棒状に限定されず、要求さ
れる磁界均一度の他、加工性、取付は安さ等を考慮して
選定され、磁極片に沿う如き湾曲状、屈曲状となして調
整用磁界を磁極部周辺に均一に作用させるのも良く、ま
た一体物で構成されていなくても良い。The magnetic field adjusting magnet, which is a feature of this invention, is provided with a pair of magnetic field adjusting magnets on each short side of a rectangular plate-shaped yoke in the center between the opposing magnetic pole pieces and outside the annular protrusion of the magnetic pole piece. Although it is provided so that the magnetization direction is opposite to that of the pair of permanent magnet components, the shape is not limited to the rod shape shown in the example, and consideration is given to the required magnetic field uniformity, workability, and low installation cost. It is also possible to select a curved or bent shape along the magnetic pole piece so that the adjusting magnetic field acts uniformly around the magnetic pole part, and it does not have to be constructed as a single piece.
具体的に説明すると、複数の磁石にて磁界調整用磁石を
構成する場合、磁極面に、板状磁極片を着設して磁束の
均−化及び機械的強度の向上を計ることができる。さら
に、複数の磁石を隙間を開は板状磁極片で支持して分割
配置することも可能である。Specifically, when a magnetic field adjusting magnet is configured with a plurality of magnets, a plate-shaped magnetic pole piece can be attached to the magnetic pole surface to equalize the magnetic flux and improve mechanical strength. Furthermore, it is also possible to separate and arrange a plurality of magnets by supporting them with plate-shaped magnetic pole pieces with gaps between them.
また、磁極片に沿う如き湾曲状、屈曲状の磁界調整用磁
石と同様の効果を、棒状の磁界調整用磁石で得るため、
複数の磁石のうち磁極片がら遠い位置の調整用磁石寸法
を大きくしたり、より高磁力の磁石とする等の手段が採
用できる。In addition, in order to obtain the same effect as a curved or bent magnetic field adjusting magnet along a magnetic pole piece, with a bar-shaped magnetic field adjusting magnet,
Among the plurality of magnets, it is possible to adopt measures such as increasing the size of the adjusting magnet at a position far from the magnetic pole piece, or using a magnet with higher magnetic force.
磁界調整用磁石の幅(磁化方向の寸法)、厚さ(長方形
板状継鉄の長辺と平行方向の寸法)、長さ(長方形板状
継鉄の短辺と平行方向の寸法)は磁界調整用磁石の磁気
特性、空隙の大きさ、磁界強度等を考慮して選定する。The width (dimension in the magnetization direction), thickness (dimension parallel to the long side of the rectangular plate yoke), and length (dimension parallel to the short side of the rectangular plate yoke) of the magnetic field adjustment magnet are determined by the magnetic field. Select the adjusting magnet by considering its magnetic properties, air gap size, magnetic field strength, etc.
磁界調整用磁石の材質は、磁界発生源となる永久磁石構
成体の材質と同様にする必要はなく、要求される磁界強
度、磁界均一度等を考慮して公知の磁石のいずれも使用
可能である。The material of the magnetic field adjustment magnet does not need to be the same as the material of the permanent magnet component that is the magnetic field generation source; any known magnet can be used, taking into account the required magnetic field strength, magnetic field uniformity, etc. be.
発明の好ましい実施態様
第1図aはこの発明の一実施例を示す磁界発生装置の縦
断面図であり、b図は横断面図である。Preferred Embodiment of the Invention FIG. 1a is a longitudinal sectional view of a magnetic field generating device showing an embodiment of the invention, and FIG. 1b is a horizontal sectional view.
この発明による磁界発生装置は、第1図に示す如く、所
要空隙を形成するため、長方形の板状継鉄(3a)の四
隅に所定長さの4本の柱状継鉄(3b)を立設し、さら
に4本の柱状継鉄(3b)先端部にもう一枚の板状継鉄
(3a)を貫通固着して継鉄(3)が構成されている。As shown in Fig. 1, the magnetic field generator according to the present invention has four columnar yokes (3b) of a predetermined length erected at the four corners of a rectangular plate-shaped yoke (3a) in order to form the required air gap. In addition, another plate-like yoke (3a) is penetrated and fixed to the tips of the four columnar yokes (3b) to form a yoke (3).
Fe−B−R系磁石を用いた一タτjの永久磁石構成体
(1)(1)を、前記継鉄(3)の板状継鉄(3a)(
3a)の対向面に固着、さらに各々の磁極面に磁極片(
2X2)を固着して対向させ磁気的に結合し、磁極片(
2X2)間の空隙(4)内に静磁界を発生させる。A permanent magnet structure (1) (1) using a Fe-B-R magnet of one ta τj is attached to the plate-shaped yoke (3a) (
3a), and a magnetic pole piece (
2
A static magnetic field is generated in the air gap (4) between 2×2).
また、磁極片(2X2)には、空隙(4)内における磁
界分布の均一度を向上するために、周辺部に環状突起(
5)を設けである。In addition, the magnetic pole piece (2X2) has an annular projection (
5) is provided.
第1図の実施例に用いた磁界調整用磁石(6X6)は、
棒状の一体物からなり、前記空隙(4)中、対向する磁
極片(2X2)間の中央部で、かつ磁極片(2X2)の
環状突起(5)(5)より外側の板状継鉄(3a)の各
短辺側に配置しである。The magnetic field adjusting magnet (6x6) used in the example of Fig. 1 is as follows:
A plate-shaped yoke (consisting of a rod-shaped integral body) located in the center between the opposing magnetic pole pieces (2X2) in the gap (4) and outside the annular projections (5) (5) of the magnetic pole pieces (2X2). 3a) are arranged on each short side.
この棒状の磁界調整用磁石(6X6)は、その磁化方向
が空隙(4)内の発生磁界と平行し、一対の永久磁石構
成体(IXI)の磁化方向とは逆向きとなるように設け
られている。This bar-shaped magnetic field adjustment magnet (6x6) is provided so that its magnetization direction is parallel to the magnetic field generated in the air gap (4) and opposite to the magnetization direction of the pair of permanent magnet structures (IXI). ing.
発明の効果
前記構成の磁界発生装置に磁界調整用磁石(6X6)を
配置したことにより、以下の効果が得られる。Effects of the Invention By arranging the magnetic field adjusting magnet (6×6) in the magnetic field generator having the above configuration, the following effects can be obtained.
■磁界調整用磁石(6X6)の配置により、空隙(4)
中央部で外周方向、換言すれば、空隙(4)の水平方向
、図中左右方向に広がるように湾曲する磁束線を抑制し
て、一対の磁極片(2X2)間に形成される磁束線の殆
どを直線的にすることができる。■ Due to the arrangement of the magnetic field adjustment magnets (6x6), the air gap (4)
The magnetic flux lines formed between the pair of magnetic pole pieces (2X2) are suppressed in the central part by suppressing the magnetic flux lines that curve in the outer circumferential direction, in other words, in the horizontal direction of the air gap (4), and in the horizontal direction in the figure. Most can be made straight.
■磁界調整用磁石(6X6)を各長方形板状継鉄(3a
)の短辺側に配置することにより、板状継鉄(3a)の
形状に起因する磁界均一度の低下を防止する。■ Magnetic field adjustment magnets (6x6) are attached to each rectangular plate yoke (3a
) is arranged on the short side of the plate-shaped yoke (3a) to prevent a decrease in magnetic field uniformity caused by the shape of the plate-shaped yoke (3a).
■空隙(4)内の軸上磁界均一度とともに磁界強度が向
上するため、断層イメージの鮮明度向上及び磁界発生装
置の小型軽量化を達成できる。(2) Since the axial magnetic field uniformity and the magnetic field strength within the air gap (4) are improved, it is possible to improve the clarity of the tomographic image and to make the magnetic field generator smaller and lighter.
実施例
第1図と同様構成の磁界発生装置に、(BH)max3
5MGOeを有するFe−B−R系永久磁石を用い、棒
状の磁界調整用磁石を各長方形板状継鉄の短辺側に配置
し、周辺部に環状突起を設けた磁極片の直径を1100
mm、一対の磁極片間距離(空隙)500mmに設定し
、空隙内の磁界を測定した。Embodiment A magnetic field generator having the same configuration as in FIG.
Using Fe-B-R permanent magnets with 5 MGOe, bar-shaped magnetic field adjustment magnets were placed on the short side of each rectangular plate-shaped yoke, and the diameter of the magnetic pole pieces with annular protrusions on the periphery was 1100 mm.
mm, and the distance between a pair of magnetic pole pieces (air gap) was set to 500 mm, and the magnetic field within the air gap was measured.
空隙中心から半径175mm内の磁界均一度及び磁界強
度は、
磁界均一度;40ppm 第2図参照磁界強度;2.
OkG
であった。The magnetic field uniformity and magnetic field strength within a radius of 175 mm from the center of the air gap are: Magnetic field uniformity: 40 ppm See Figure 2 Magnetic field strength: 2.
It was OkG.
また、磁界調整用磁石を使用しない以外は全てこの発明
の装置と同一条件の従来の装置の空隙内の磁界を測定し
た結果、
磁界均一度;60ppm 第3図参照磁界強度;2.
OkG
であった。In addition, as a result of measuring the magnetic field in the air gap of a conventional device under the same conditions as the device of the present invention except that no magnetic field adjustment magnet is used, the following results were obtained: Magnetic field uniformity: 60 ppm See Figure 3. Magnetic field strength: 2.
It was OkG.
継鉄及び磁界調整用磁石の構成は下記のとおりである。The configuration of the yoke and the magnetic field adjustment magnet is as follows.
圧立形豊仄藍迭
短辺(L);1200mm、
長辺(W);1950皿亀
厚5mT);130mm
匪兄置駿里風互
材質;Fe−B−R系磁石、
磁気特性;(BH)max 35MGOe輻(1);
30皿m
mさ(w);1200mm、
厚さ(t);20mm、
水平対向距離;1200mmShort side (L): 1200mm, long side (W): 1950, countersunk thickness 5mT); 130mm Material: Fe-B-R magnet, magnetic properties: ( BH) max 35MGOe convergence (1);
30 dishes mm Width (w): 1200mm, Thickness (t): 20mm, Horizontal opposing distance: 1200mm
第1図aはこの発明の一実施例を示す磁界発生装置の縦
断面図であり、b図は横断面図である。
第2図と第3図は磁界発生装置の空隙中心部の磁界均一
度を示すグラフであり、第2図はこの発明装置の場合、
第3図は従来装置の場合を示す。
第4図は従来の磁界発生装置を示す正面図である。
1・・・永久磁石構成体、2・・・磁極片、3・・・継
鉄、3a・・・板状継鉄、3b・・・柱状継鉄、4・・
・空隙、5・・・環状突起部、6・・・磁界調整用磁石
。FIG. 1a is a longitudinal cross-sectional view of a magnetic field generating device showing an embodiment of the present invention, and FIG. 1b is a cross-sectional view. FIGS. 2 and 3 are graphs showing the magnetic field uniformity at the center of the air gap of the magnetic field generator, and FIG.
FIG. 3 shows the case of a conventional device. FIG. 4 is a front view showing a conventional magnetic field generating device. DESCRIPTION OF SYMBOLS 1... Permanent magnet structure, 2... Magnetic pole piece, 3... Yoke, 3a... Plate yoke, 3b... Column yoke, 4...
- Gap, 5... Annular protrusion, 6... Magnetic field adjustment magnet.
Claims (1)
気的に接続して対向配置する一対の長方形板状継鉄と、
板状継鉄の各対向面に着設した永久磁石構成体と、該磁
石構成体の各対向面に設けた周辺部に環状突起を有する
磁極片とから構成し、該空隙に磁界を発生するMRI用
磁界発生装置において、 対向する磁極片間の中央部で、かつ磁極片の環状突起よ
り外側で長方形板状継鉄の各短辺側に、一対の磁界調整
用磁石を磁化方向が前記一対の永久磁石と逆向きとなる
ように設けたことを特徴とするMRI用磁界発生装置。[Scope of Claims] 1. A pair of rectangular plate-shaped yokes that form a gap using a plurality of columnar yokes as spacing members, and are magnetically connected and arranged to face each other;
Consists of a permanent magnet structure attached to each opposing surface of a plate-shaped yoke, and a magnetic pole piece having an annular protrusion on the periphery provided on each opposing surface of the magnet structure, and generates a magnetic field in the air gap. In a magnetic field generation device for MRI, a pair of magnetic field adjustment magnets are installed on each short side of a rectangular plate-shaped yoke at the center between opposing magnetic pole pieces and outside the annular protrusion of the magnetic pole pieces, and the magnetization direction is set to the pair of magnetic field adjustment magnets. 1. A magnetic field generator for MRI, characterized in that the magnetic field generator is provided in a direction opposite to that of a permanent magnet.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1004392A JP2726857B2 (en) | 1989-01-10 | 1989-01-10 | Magnetic field generator for MRI |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP1004392A JP2726857B2 (en) | 1989-01-10 | 1989-01-10 | Magnetic field generator for MRI |
Publications (2)
Publication Number | Publication Date |
---|---|
JPH02184003A true JPH02184003A (en) | 1990-07-18 |
JP2726857B2 JP2726857B2 (en) | 1998-03-11 |
Family
ID=11583084
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP1004392A Expired - Fee Related JP2726857B2 (en) | 1989-01-10 | 1989-01-10 | Magnetic field generator for MRI |
Country Status (1)
Country | Link |
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JP (1) | JP2726857B2 (en) |
Cited By (4)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1542244A3 (en) * | 2003-12-10 | 2008-01-02 | Shin-Etsu Chemical Co., Ltd. | Magnetic circuit with opposing permanent magnets and method for adjusting magnetic field thereof |
WO2008145167A1 (en) * | 2007-05-31 | 2008-12-04 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Magnet arrangement for generating an nmr-compatible homogeneous permanent magnetic field |
CN104051122A (en) * | 2014-06-12 | 2014-09-17 | 包头市稀宝博为医疗系统有限公司 | Magnet device used for magnetic resonance imaging and measuring equipment of magnet device |
CN104051121A (en) * | 2014-06-04 | 2014-09-17 | 中国科学院金属研究所 | Method for establishing adjustable static magnetic field by adopting permanent magnets |
-
1989
- 1989-01-10 JP JP1004392A patent/JP2726857B2/en not_active Expired - Fee Related
Cited By (5)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1542244A3 (en) * | 2003-12-10 | 2008-01-02 | Shin-Etsu Chemical Co., Ltd. | Magnetic circuit with opposing permanent magnets and method for adjusting magnetic field thereof |
WO2008145167A1 (en) * | 2007-05-31 | 2008-12-04 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Magnet arrangement for generating an nmr-compatible homogeneous permanent magnetic field |
US8390289B2 (en) | 2007-05-31 | 2013-03-05 | Fraunhofer-Gesellschaft zur Förderung der angewandten Forschung e.V. | Magnet arrangement for generating an NMR-compatible homogeneous permanent magnetic field |
CN104051121A (en) * | 2014-06-04 | 2014-09-17 | 中国科学院金属研究所 | Method for establishing adjustable static magnetic field by adopting permanent magnets |
CN104051122A (en) * | 2014-06-12 | 2014-09-17 | 包头市稀宝博为医疗系统有限公司 | Magnet device used for magnetic resonance imaging and measuring equipment of magnet device |
Also Published As
Publication number | Publication date |
---|---|
JP2726857B2 (en) | 1998-03-11 |
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