JP3445303B2 - Magnetic field generator for MRI - Google Patents
Magnetic field generator for MRIInfo
- Publication number
- JP3445303B2 JP3445303B2 JP06339793A JP6339793A JP3445303B2 JP 3445303 B2 JP3445303 B2 JP 3445303B2 JP 06339793 A JP06339793 A JP 06339793A JP 6339793 A JP6339793 A JP 6339793A JP 3445303 B2 JP3445303 B2 JP 3445303B2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- magnetic
- mri
- eddy current
- field generator
- 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.)
- Expired - Lifetime
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- Magnetic Resonance Imaging Apparatus (AREA)
Description
【0001】[0001]
【産業上の利用分野】この発明は、医療用磁気共鳴断層
撮影装置等に用いられる磁界発生装置の改良に係り、空
隙を形成して対向する一対の磁極片を有し、特にその周
縁部に設けた突起部の少なくとも表層を積層けい素鋼板
またはソフトフェライトで形成し、空隙内の磁界均一度
を損なうことなく、傾斜磁界コイルによる磁極片内の渦
電流、残磁現象の低減を図り、高速撮像を可能にしたM
RI用磁界発生装置に関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an improvement of a magnetic field generator used in a magnetic resonance tomography apparatus for medical use and the like, and has a pair of magnetic pole pieces opposed to each other with a gap formed therebetween, and particularly in a peripheral portion thereof. At least the surface layer of the protrusions provided is made of laminated silicon steel plate or soft ferrite to reduce the eddy current and remanence phenomenon in the pole piece by the gradient magnetic field coil without impairing the magnetic field uniformity in the air gap. M that enabled imaging
The present invention relates to a magnetic field generator for RI.
【0002】[0002]
【従来の技術】医療用磁気共鳴断層撮影装置(以下MR
Iという)は、強力な磁界を形成する磁界発生装置の空
隙内に、被検者の一部または全部を挿入して、対象物の
断層イメージを得てその組織の性質まで描き出すことが
できる装置である。上記MRI用の磁界発生装置におい
て、空隙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、かつ鮮明な断層イメージを得るため
に、通常、空隙内の撮像視野内には、0.02〜2.0
Tでかつ1×10-4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。2. Description of the Related Art A magnetic resonance tomography apparatus for medical use (hereinafter referred to as MR
(I) is a device capable of inserting a part or all of a subject into a void of a magnetic field generator that forms a strong magnetic field, obtaining a tomographic image of an object, and drawing out even the nature of the tissue. Is. In the above-mentioned magnetic field generator for MRI, the space needs to be wide enough to allow a part or the whole of the subject to be inserted, and in order to obtain a clear tomographic image, normally, the imaging field of view in the space is , 0.02-2.0
It is required to form a stable and strong uniform magnetic field with T and an accuracy of 1 × 10 −4 or less.
【0003】MRIに用いる磁界発生装置として、磁界
発生源にR−Fe−B系磁石を用いた一対の永久磁石構
成体の各々の一方端に磁極片を固着して対向させ、他方
端を継鉄にて連結し、磁極片間の空隙内に、静磁界を発
生させる構成が知られている。磁極片には、空隙内にお
ける磁界分布の均一度を向上させるために、周辺部に環
状突起を設けてあり、通常、電磁軟鉄、純鉄等の磁性材
料を削り出した板状のバルク(一体物)から構成される
(特開昭60−88407号公報)。As a magnetic field generator used for MRI, magnetic pole pieces are fixed to one end of each of a pair of permanent magnet constructions using an R-Fe-B system magnet as a magnetic field generation source to face each other, and the other end is connected. A configuration is known in which a static magnetic field is generated in a gap between magnetic pole pieces by connecting with iron. In order to improve the homogeneity of the magnetic field distribution in the air gap, the pole pieces are provided with annular protrusions on the periphery, and are usually a plate-shaped bulk (integrated) made by cutting out magnetic materials such as electromagnetic soft iron and pure iron. (Japanese Patent Laid-Open No. 60-88407).
【0004】[0004]
【発明が解決しようとする課題】MRIでは、空隙内の
位置情報を得るために、通常X、Y、Zの3方向に対応
する3組のコイル群からなる傾斜磁界コイル(GC)が
各磁極片の近傍に配置され、この傾斜磁界コイルに、パ
ルス電流を通電することによって台形波状に時間変化す
る所望方向の傾斜磁界を発生することができる。In MRI, a gradient magnetic field coil (GC), which is usually composed of three coil groups corresponding to three directions of X, Y, and Z, is used to obtain position information in the air gap. A gradient magnetic field in a desired direction which changes in a trapezoidal wave shape with time can be generated by applying a pulse current to the gradient magnetic field coil which is arranged in the vicinity of the one piece.
【0005】しかし、磁極片の配置は傾斜磁界コイルと
の関係において、渦電流や残留磁気の問題を有してい
る。つまり、MRI用磁界発生装置は、通常均一な磁界
に傾斜磁界を加えることによって核磁気共鳴の信号に位
置情報を与えている。一つの画像を得るためには多数の
パルス状傾斜磁界を加えることが必要である。この傾斜
磁界は傾斜磁界コイルにパルス電流を与えて発生させる
が、その近傍に鉄のような導電率の高い導体があると渦
電流が発生し、傾斜磁界が急峻には立ち上がりにくくな
る。However, the arrangement of the magnetic pole pieces has problems of eddy current and residual magnetism in relation to the gradient magnetic field coil. That is, the magnetic field generator for MRI gives position information to a signal of nuclear magnetic resonance by applying a gradient magnetic field to a normally uniform magnetic field. It is necessary to apply a large number of pulsed gradient magnetic fields to obtain one image. This gradient magnetic field is generated by applying a pulse current to the gradient magnetic field coil, but if a conductor with high conductivity such as iron is present in the vicinity of the gradient magnetic field coil, an eddy current is generated and the gradient magnetic field is hard to rise sharply.
【0006】例えば、高速撮像するためのFSE法(フ
ァーストスピンエコー法)では、傾斜磁界を高速で切り
かえるパルスシーケンスを利用するため、渦電流の発生
が極めて少ない磁界発生装置が必要とされている。For example, in the FSE method (fast spin echo method) for high-speed imaging, a pulse sequence for switching a gradient magnetic field at a high speed is used, so that a magnetic field generator that generates very little eddy current is required.
【0007】この発明は、MRI用磁界発生装置の磁極
片における上記現状に鑑み提案するもので、空隙内の磁
界均一度を低下させることなく、渦電流の発生を低減し
て短時間で傾斜磁界が所定の強度に上昇し、鮮明な画像
を得ることができる構成からなる磁極片の提供を目的と
し、さらに加工、製造が容易で組立て作業性にすぐれた
構成からなる磁極片の提供を目的としている。The present invention is proposed in view of the above-mentioned current situation in the magnetic pole piece of the magnetic field generator for MRI, and reduces the generation of eddy currents without decreasing the magnetic field homogeneity in the air gap and reduces the gradient magnetic field in a short time. For the purpose of providing a magnetic pole piece having a structure capable of obtaining a clear image by increasing the strength of the magnetic pole, and further for providing a magnetic pole piece having a structure that is easy to process and manufacture and has excellent assembling workability. There is.
【0008】[0008]
【課題を解決するための手段】この発明は、渦電流の発
生を低減し、また残磁現象を低減しFSE法などの高速
撮像が可能な構成からなるMRI用磁界発生装置を目的
に種々検討した結果、空隙を形成して対向する一対の磁
極片の表層部をソフトフェライトで形成し、さらに磁極
片の周縁部に設けた突起部の表層をソフトフェライトま
たは積層けい素鋼板で形成することにより、磁界強度お
よび磁界均一度を低下させることなく、傾斜磁界コイル
による渦電流、並びに残磁現象を低減でき、さらに加
工、製造が容易となることを知見した。SUMMARY OF THE INVENTION The present invention is variously studied for the purpose of an MRI magnetic field generator having a structure capable of reducing the generation of eddy currents and reducing the residual magnetism phenomenon and enabling high-speed imaging such as the FSE method. As a result, by forming the air gaps to form the surface layer portions of the pair of pole pieces facing each other with soft ferrite, and further forming the surface layer of the protrusions provided on the peripheral portions of the pole pieces with soft ferrite or laminated silicon steel sheet. It has been found that the eddy current due to the gradient magnetic field coil and the residual magnetism phenomenon can be reduced without lowering the magnetic field strength and the magnetic field homogeneity, and that the processing and manufacturing are easy.
【0009】すなわち、この発明は、磁界発生源と、空
隙を挟んで対向して配置され、各々が対向面の周縁部に
環状突起を形成された一対の磁極片とを有し、該空隙内
に所定の均一磁界を発生させ、傾斜磁界を高速で切りか
えるパルスシーケンスを利用するMRI用磁界発生装置
において、前記各磁極片は、前記環状突起部の内周面及
び前記環状突起部同志の対向面が積層けい素鋼板または
ソフトフェライトの渦電流低減材の層で覆われているこ
とを特徴とするMRI用磁界発生装置である。また、こ
の発明は上記の構成において、前記磁極片の各々は、前
記環状突起部の凹部内の底面が渦電流低減材の層で覆わ
れていることを特徴とするMRI用磁界発生装置であ
る。この発明は、磁極片の周縁突起部及びその近傍の表
層を積層けい素鋼板またはソフトフェライトの渦電流低
減材で形成、中央部に中央突起部を設け、あるいはさら
に周縁突起部及びその近傍以外の中央突起部を含む表層
部をソフトフェライトで形成したことを特徴とするが、
周縁突起部を含む磁極片の主体を軟鉄材などの磁性材ベ
ースで構成し、その上に積層けい素鋼板またはソフトフ
ェライトを積層する構成、すなわち渦電流低減材の層で
覆う構成を採用できる。That is, the present invention has a magnetic field generation source and a pair of magnetic pole pieces which are arranged so as to face each other with a gap therebetween and each of which has an annular protrusion formed on the peripheral edge of the facing surface. To generate a predetermined uniform magnetic field and cut the gradient magnetic field at high speed.
In the magnetic field generator for MRI using the pulse sequence, the inner peripheral surface of the annular protrusion and the opposing surfaces of the annular protrusions are made of laminated silicon steel plate or soft ferrite eddy current reducing material. The magnetic field generator for MRI is characterized in that it is covered with a layer. Further, the present invention is the magnetic field generating apparatus for MRI according to the above-mentioned structure, wherein each of the magnetic pole pieces has a bottom surface in the recess of the annular protrusion covered with a layer of an eddy current reducing material. . According to the present invention, the peripheral protrusion of the pole piece and the surface layer in the vicinity thereof are formed of an eddy current reducing material such as a laminated silicon steel plate or soft ferrite, a central protrusion is provided in the center, or a peripheral protrusion other than the peripheral protrusion is formed. It is characterized in that the surface layer portion including the central protrusion is formed of soft ferrite,
It is possible to adopt a configuration in which the main body of the magnetic pole pieces including the peripheral protrusions is composed of a magnetic material base such as a soft iron material, and a laminated silicon steel plate or soft ferrite is laminated thereon, that is, a structure of covering with an eddy current reducing material layer.
【0010】この発明において、磁気回路には2枚の継
鉄板を4本の柱状継鉄にて対向配置し、各継鉄板の対向
面に磁極片を着設する構成のほか、筒状継鉄内に一対の
永久磁石構成体を対向配置し、一対の永久磁石構成体を
配置しない内周面に複数の補助永久磁石構成体を配置す
るなど種々の構成が採用でき、筒状継鉄の場合、鉄等の
軟質磁性材料が用いられるが、特に鉄、けい素鋼板等の
積層体からなる継鉄を用いることにより渦電流の低減効
果が大きくなる。In the present invention, in the magnetic circuit, two yoke plates are arranged so as to face each other with four columnar yokes, and the pole pieces are attached to the facing surfaces of the yoke plates. In the case of a tubular yoke, various configurations can be adopted, such as arranging a pair of permanent magnet constituents inside each other and arranging a plurality of auxiliary permanent magnet constituents on the inner peripheral surface where the pair of permanent magnet constituents are not arranged. Although a soft magnetic material such as iron is used, the effect of reducing the eddy current is increased by using a yoke made of a laminated body of iron, a silicon steel plate or the like.
【0011】筒状継鉄の場合、上記一対の永久磁石構成
体は空隙内の磁界形成に寄与する主たる磁界発生源であ
り、通常空隙内の磁界方向に対して直交する方向に空隙
対向面を形成している。これら一対の永久磁石構成体の
内周面に沿って配置される傾斜磁界コイルの影響によっ
て、該永久磁石構成体の内部にその空隙対向面と平行方
向に渦電流が発生する。この渦電流の発生を低減させる
ためには、例えば、永久磁石構成体は各々の永久磁石ブ
ロックの磁化方向に直交方向に電気的に絶縁されること
が重要であり、かかる構成により見かけ上の比抵抗が大
きくなり、渦電流が抑制できる。永久磁石構成体の磁化
方向は、磁気回路の構成や継鉄上の配置箇所などに応じ
て種々選定されるが、所要空隙に均一な静磁界が得られ
るように配置されれば、いかなる方向でもよい。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30
MGOe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。In the case of a tubular yoke, the above-mentioned pair of permanent magnet constituents are the main magnetic field generating sources that contribute to the formation of the magnetic field in the air gap, and normally the air gap opposing surfaces are arranged in the direction orthogonal to the magnetic field direction in the air gap. Is forming. Due to the influence of the gradient magnetic field coils arranged along the inner peripheral surfaces of the pair of permanent magnet constituents, an eddy current is generated inside the permanent magnet constituents in the direction parallel to the air gap facing surface. In order to reduce the generation of this eddy current, for example, it is important that the permanent magnet structure is electrically insulated in the direction orthogonal to the magnetization direction of each permanent magnet block. The resistance increases and eddy current can be suppressed. The magnetizing direction of the permanent magnet structure is variously selected according to the structure of the magnetic circuit and the location on the yoke, but any direction can be used as long as it is arranged so that a uniform static magnetic field can be obtained in the required air gap. Good. Ferrite magnets, alnico magnets, and rare earth cobalt magnets can be used as the permanent magnets of the magnet structure used in such a magnetic circuit. Particularly, R is a light rare earth element rich in resources centered on Nd and Pr, 30 with B and Fe as main components
Fe-, which has an extremely high energy product over MGOe
By using the BR permanent magnet, the size can be significantly reduced.
【0012】この発明において、渦電流低減材の積層け
い素鋼板は、その積層方向が該磁極片の対向方向に積層
された場合、また、磁極片の対向方向と直交する方向に
積層された場合のいずれでもよく、さらに必要に応じて
積層方向を変えて複数層とした構成でもよく、あるいは
種々の形状からなる磁極片用部材となして、これを組み
合せて所要形状とすることができる。さらに、使用する
けい素鋼板の磁化容易軸方向の方向性は任意であるが、
無方向性けい素鋼板(JISC2552等)にて構成し
た場合、残磁現象低減に顕著な効果を示す。また、けい
素鋼板の厚みは任意の厚みでよいが、一般に入手し易い
けい素鋼板は0.35mm程度と薄いため、積層、組立
て作業性が極めて良好となる構成として、いったん所定
寸法からなる複数枚の矩形状無方向性けい素鋼板を磁極
片の対向方向と直交する方向に所定枚数積層したブロッ
ク状磁極片用部材を複数個作成し、これら複数個のブロ
ック状磁極片用部材を直接磁石構成体上に固着するか、
板状の磁性材ベースを介して磁石構成体上に固着する等
の構成を提案する。In the present invention, the laminated silicon steel sheet of the eddy current reducing material is laminated in the laminating direction in the facing direction of the magnetic pole pieces, or in the direction orthogonal to the facing direction of the magnetic pole pieces. Any of the above may be used, and if necessary, the stacking direction may be changed to form a plurality of layers. Alternatively, the pole piece member may have various shapes, and the members may be combined into a desired shape. Furthermore, the directionality of the easy axis of magnetization of the silicon steel sheet used is arbitrary,
When it is made of non-oriented silicon steel sheet (JISC2552 etc.), it shows a remarkable effect in reducing the residual magnetism phenomenon. The silicon steel sheet may have any thickness, but since a silicon steel sheet that is generally easily available is as thin as about 0.35 mm, it is possible to obtain a plurality of pieces having a predetermined size once as a configuration that has extremely good stacking and assembling workability. A plurality of rectangular non-oriented silicon steel sheets were laminated in a predetermined number in a direction orthogonal to the facing direction of the pole pieces to prepare a plurality of block pole piece members, and the plurality of block pole piece members were directly magnetized. Stick to the structure or
We propose a structure such as fixing onto a magnet structure via a plate-shaped magnetic material base.
【0013】この発明において、渦電流低減材のソフト
フェライトの材質は、Mn−Znフェライト粉、Ni−
Znフェライト粉等の種々のソフトフェライト材からな
り、ソフトフェライト製の大ブロックを所要形状に加工
したもの、あるいは小ブロックを所要形状に接着剤で組
立てたもの等が利用でき、さらに、磁界の均一度向上を
目的に、空隙側周辺部に種々断面形状の環状突起を設け
たり、中央部に円形凸状部や断面台形状の突起部を設け
たり、また、磁極片の所要位置に、磁界の均一度調整を
目的に、磁性材または磁石からなる磁界調整片を着設し
てもよい。上記ソフトフェライトの小ブロックを製造す
るには、例えば、Mn−Znフェライト粉等を所要形状
に圧縮成形した後、焼結し、さらに密度の向上のため、
HP、HIP(Hot Isostatic Pres
sing)法等の手段を併用するのもよく、得られた小
ブロックを、エポキシ樹脂などの接着剤等を用いて接着
して、所要形状に組み立てるとよい。ソフトフェライト
材のうち、例えば、Mn−Zn系ソフトフェライトは、
磁界の均等化手段として要求される高透磁率および高い
飽和磁束密度Bsを有し、また渦電流対策として十分に
高い比抵抗と、残磁現象を防止し得る低保磁力(数A/
m)の特性を持っている。この発明において、ソフトフ
ェライトは磁石構成体から発生する磁束を効率よく空隙
に作用させるためには、0.4T以上のBsを有するも
のが好ましい。すなわち、ソフトフェライト内を通過す
る磁束量は、そのBsにより決定され、その値が小さい
と必然的に飽和して磁界強度が低下してしまい、これを
防ぐには磁石を大きくする必要があり、装置の大型化を
招くこととなる。従って、Bsは0.4T以上が望まし
く、好ましくは0.5T以上、さらに好ましくは0.5
5T以上である。また、ソフトフェライトのHcが大き
すぎると、残磁現象が生じるため、Hcは50A/m以
下が望ましく、好ましくは20A/m以下、さらに好ま
しくは10A/m以下である。また、渦電流の低減に
は、比抵抗ρが10-5Ω・m以上、さらに好ましくは1
0-3Ω・m以上が望ましい。In the present invention, the material of the soft eddy current reducing material is Mn-Zn ferrite powder, Ni-
Made of various soft ferrite materials such as Zn ferrite powder, a large block made of soft ferrite processed into the required shape, or a small block assembled into the required shape with an adhesive can be used. For the purpose of improving once, an annular protrusion with various cross-sectional shapes is provided on the periphery of the air gap side, a circular convex part or a protrusion with a trapezoidal cross-section is provided in the center part, and the magnetic field is A magnetic field adjusting piece made of a magnetic material or a magnet may be attached for the purpose of adjusting the uniformity. In order to manufacture the above-mentioned small blocks of soft ferrite, for example, Mn-Zn ferrite powder or the like is compression-molded into a required shape, then sintered, and further for improving the density,
HP, HIP (Hot Isostatic Pres
Sing method and the like may be used together, and the obtained small blocks may be bonded with an adhesive such as an epoxy resin to assemble them into a desired shape. Among the soft ferrite materials, for example, Mn-Zn based soft ferrite is
It has a high magnetic permeability and a high saturation magnetic flux density Bs required as a magnetic field equalizing means, and has a sufficiently high specific resistance as a countermeasure for eddy currents and a low coercive force (several A / s).
It has the characteristics of m). In the present invention, it is preferable that the soft ferrite has Bs of 0.4 T or more in order to efficiently cause the magnetic flux generated from the magnet constituent to act on the air gap. That is, the amount of magnetic flux passing through the soft ferrite is determined by its Bs, and if its value is small, it will inevitably saturate and the magnetic field strength will decrease. To prevent this, it is necessary to enlarge the magnet, This leads to an increase in the size of the device. Therefore, Bs is preferably 0.4T or more, preferably 0.5T or more, and more preferably 0.5T.
It is 5T or more. Further, if Hc of the soft ferrite is too large, a residual magnetism phenomenon occurs. Therefore, Hc is preferably 50 A / m or less, preferably 20 A / m or less, and more preferably 10 A / m or less. To reduce the eddy current, the specific resistance ρ is 10 −5 Ω · m or more, and more preferably 1
0 -3 Ω · m or more.
【0014】[0014]
【作用】この発明によるMRI用磁界発生装置の構成並
びに作用を図面に基づいて詳述する。図1は板状及び柱
状継鉄を用いた磁気回路にこの発明を適用したMRI用
磁界発生装置の実施例を示す斜視説明図であり、Aは全
体、Bは磁極片を示す。図2は筒状継鉄を用いた磁気回
路にこの発明を適用したMRI用磁界発生装置の実施例
を示す斜視説明図であり、Aは全体、Bは磁極片を示
す。図1に示す磁界発生装置は、2枚の継鉄板1,1を
4本の柱状継鉄2にて対向配置し、各継鉄板1,1の対
向面中央に円盤状永久磁石構成体3,3を着設してあ
り、さらに永久磁石構成体3,3上に磁極片4,4を着
設してあり、磁極片4は図1のBに示す如く、鉄などの
円盤状ベース材料5の周縁上に突起6を配置してある。
突起6とその近傍の表層部7をけい素鋼板またはソフト
フェライトにて形成することにより、傾斜磁界コイルに
GCパルスが通電されても周縁突起部近傍に発生する渦
電流は低減される。また、磁極片4の中央部は大部分が
平坦突起からなるソフトフェライト製の中央突起部8を
設けることにより、空隙9の磁界が均一化され、傾斜磁
界コイルによる渦電流の低減の効果とともに、GCパル
スにより生じる残磁を低減させる作用効果がある。The structure and operation of the magnetic field generator for MRI according to the present invention will be described in detail with reference to the drawings. FIG. 1 is a perspective explanatory view showing an embodiment of a magnetic field generator for MRI in which the present invention is applied to a magnetic circuit using plate-like and columnar yokes, where A is the whole and B is the pole piece. 2 is a perspective explanatory view showing an embodiment of a magnetic field generator for MRI in which the present invention is applied to a magnetic circuit using a cylindrical yoke, where A is the whole and B is the pole piece. In the magnetic field generator shown in FIG. 1, two yoke plates 1 and 1 are arranged so as to face each other with four columnar yokes 2, and a disk-shaped permanent magnet structure 3, is provided at the center of the facing surface of each yoke plate 1, 1. 3 is provided, and magnetic pole pieces 4 and 4 are further provided on the permanent magnet constructing bodies 3 and 3. The magnetic pole piece 4 has a disc-shaped base material 5 such as iron as shown in FIG. 1B. The protrusions 6 are arranged on the peripheral edge of the.
By forming the projection 6 and the surface layer portion 7 in the vicinity thereof with a silicon steel plate or soft ferrite, the eddy current generated near the peripheral projection portion is reduced even when the gradient magnetic field coil is energized with a GC pulse. Further, the central portion of the pole piece 4 is provided with the central protrusion portion 8 made of soft ferrite, which is mostly a flat protrusion, so that the magnetic field of the air gap 9 is made uniform, and the effect of reducing the eddy current by the gradient magnetic field coil is It has an effect of reducing the residual magnetism generated by the GC pulse.
【0015】図2に示す磁界発生装置は、6角筒状の筒
状継鉄10の内周面に永久磁石構成体を配置する構成で
継鉄には鉄等の軟質磁性材料が用いられるが、特に鉄、
ケイ素鋼板等の積層体からなる継鉄を用いることにより
渦電流の低減効果が大きくなる。空隙内の磁界形成に寄
与する主たる磁界発生源である一対の永久磁石構成体1
1a,11dは、通常空隙12内の磁界方向Yに磁化方
向を有し、空隙対向面を形成している。その他の永久磁
石構成体11b,11c,11e,11fの磁化方向
は、磁気回路の構成や継鉄上の配置箇所などに応じて種
々選定されるが、所要空隙に均一な静磁界が得られるよ
うに配置されれば、いかなる方向でもよい。永久磁石構
成体はいかなる形状、構成でもよく、特に磁極片の設置
されていない図中の符号11b,11c,11e,11
fの永久磁石構成体を複数個の電気的に絶縁された永久
磁石ブロックで構成することにより、該永久磁石構成体
に発生する渦電流を低減することができる。なお、傾斜
磁界コイルは多角筒状に組合せ配置した永久磁石構成体
内周面に沿って設置される。The magnetic field generator shown in FIG. 2 has a structure in which a permanent magnet structure is arranged on the inner peripheral surface of a hexagonal tubular yoke 10, and a soft magnetic material such as iron is used for the yoke. , Especially iron,
By using a yoke made of a laminated body such as a silicon steel plate, the effect of reducing the eddy current is increased. A pair of permanent magnet constructions 1 which are main magnetic field generation sources contributing to the formation of a magnetic field in the air gap.
1a and 11d usually have a magnetization direction in the magnetic field direction Y in the void 12 and form void facing surfaces. The magnetization directions of the other permanent magnet components 11b, 11c, 11e, 11f are selected variously according to the configuration of the magnetic circuit and the location on the yoke, etc., so that a uniform static magnetic field can be obtained in the required air gap. Any orientation can be used as long as it is located at. The permanent magnet structure may have any shape and structure, and in particular, reference numerals 11b, 11c, 11e, 11 in the figure in which pole pieces are not installed.
By configuring the permanent magnet structure of f by a plurality of electrically insulated permanent magnet blocks, the eddy current generated in the permanent magnet structure can be reduced. The gradient magnetic field coil is installed along the inner circumferential surface of the permanent magnet constituting body which is arranged in combination in a polygonal cylindrical shape.
【0016】磁極片13は主要磁界を形成する一対の永
久磁石構成体11a,11dの空隙対向面に設置され、
ボルト等で磁石を貫通して継鉄10に固定される。磁極
片の形状は、磁気回路の構成や永久磁石構成体の配置箇
所などに応じて種々選定されるが、上記の磁極片形状の
範囲内で所要空隙に均一な静磁界が得られるように選定
すればよい。磁極片13のベース材料14の材質として
は、鉄などの軟質磁性材料が適宜選定でき、磁極片13
の開口部空隙対向面両端部に突起(シム)15を配置し
てある。突起15とその近傍の表層部16をけい素鋼板
またはソフトフェライトにて形成することにより、傾斜
磁界コイルにGCパルスが通電されても周縁突起部近傍
に発生する渦電流は低減される。また、磁極片13の中
央にも中央突起部17を設けてあり、中央突起部17を
ソフトフェライトにて形成することにより、空隙の磁界
が均一化され、傾斜磁界コイルによる渦電流の低減の効
果とともに、GCパルスにより生じる残磁を低減させる
作用効果がある。The pole piece 13 is installed on the surfaces of the pair of permanent magnet components 11a and 11d that form the main magnetic field, facing each other,
It is fixed to the yoke 10 by penetrating the magnet with a bolt or the like. The shape of the pole piece is selected variously according to the configuration of the magnetic circuit and the location of the permanent magnet structure, etc., but is selected so that a uniform static magnetic field can be obtained in the required air gap within the above-mentioned shape of the pole piece. do it. As the material of the base material 14 of the pole piece 13, a soft magnetic material such as iron can be appropriately selected.
Protrusions (shims) 15 are arranged at both ends of the opening facing the air gap. By forming the projection 15 and the surface layer portion 16 in the vicinity thereof with a silicon steel plate or soft ferrite, the eddy current generated near the peripheral projection portion is reduced even when the gradient magnetic field coil is energized with a GC pulse. Further, a central protrusion 17 is also provided in the center of the pole piece 13, and the magnetic field in the air gap is made uniform by forming the central protrusion 17 with soft ferrite, and the effect of reducing the eddy current by the gradient magnetic field coil is obtained. At the same time, there is an effect that the residual magnetism generated by the GC pulse is reduced.
【0017】この発明において、磁極片の突起部に用い
るけい素鋼板は飽和磁束密度Bsが高く、空隙の磁界均
一化が達成しやすく、また保磁力Hc及びヒステリシス
損の小さな電気的に絶縁されている薄板を複数枚積層し
た構成であることから、傾斜磁界コイルにGCパルスが
通電されても周縁突起部近傍に発生する渦電流は低減さ
れ、しかも残磁現象を低減させることも可能となる。ま
た、磁極片表層のソフトフェライト層により空隙の磁界
が均一化され、傾斜磁界コイルによる渦電流の低減の効
果とともに、GCパルスにより生じる残磁を低減させる
効果があり、鮮明な断層画像が得られる。In the present invention, the silicon steel sheet used for the protrusion of the pole piece has a high saturation magnetic flux density Bs, makes it easy to achieve a uniform magnetic field in the air gap, and is electrically insulated with a small coercive force Hc and hysteresis loss. Since a plurality of thin plates are laminated, the eddy current generated in the vicinity of the peripheral protrusion is reduced even when the gradient magnetic field coil is energized with the GC pulse, and the residual magnetism can be reduced. Further, the magnetic field of the air gap is made uniform by the soft ferrite layer on the surface of the pole piece, and the effect of reducing the eddy current by the gradient magnetic field coil and the effect of reducing the residual magnetism caused by the GC pulse are obtained, and a clear tomographic image can be obtained. .
【0018】[0018]
【実施例】図1の構成と同様の磁界発生装置に、BHm
ax35MGOeを有するNd−Fe−B系永久磁石を
用い、純鉄のベース材料の周縁上に突起を配置して突起
とその近傍の表層部をけい素鋼板で形成し、中央部は大
部分が平坦突起からなるソフトフェライト製の中央突起
部を設けた。この発明の構成において磁極片空隙対向面
間距離を500mmに設定し、傾斜磁界コイルにパルス
電流を与えて多数のパルス状傾斜磁界を加えて、傾斜磁
界の立ち上がり特性と画像特性を測定した。なお、無方
向性けい素鋼板は、Hc=40A/m、Bs=1.7
T、ρ=45×10-8Ω・mである。ソフトフェライト
はMn−Zn系フェライト、Hc=6.0A/m、Bs
=0.58T、ρ=0.2Ω・mである。純鉄は、Hc
=80A/m、Bs=2.0T、ρ=1×10-7Ω・m
である。EXAMPLE A magnetic field generator similar to that of FIG.
Using Nd-Fe-B based permanent magnet with ax35MGOe, the protrusions are arranged on the periphery of the base material of pure iron, the protrusions and the surface layer portion in the vicinity thereof are formed of silicon steel plate, and the central portion is mostly flat. A central protrusion made of soft ferrite was provided. In the structure of the present invention, the distance between the pole piece air gap facing surfaces was set to 500 mm, a pulse current was applied to the gradient magnetic field coil to apply a large number of pulsed gradient magnetic fields, and the rising characteristics and image characteristics of the gradient magnetic field were measured. The non-oriented silicon steel sheet has Hc = 40 A / m and Bs = 1.7.
T, ρ = 45 × 10 −8 Ω · m. Soft ferrite is Mn-Zn type ferrite, Hc = 6.0 A / m, Bs
= 0.58T and ρ = 0.2Ω · m. Pure iron is Hc
= 80 A / m, Bs = 2.0 T, ρ = 1 × 10 −7 Ω · m
Is.
【0019】比較のため、実施例1の磁界発生装置に全
てが上記性状純鉄からなる同一寸法、形状からなる磁極
片を配置して、同様に傾斜磁界の立ち上がり特性と画像
特性を測定した。この発明による磁界発生装置の傾斜磁
界の立ち上がり特性は、図3に実践で示す如く、一点鎖
線で示す比較例に対して大幅に向上して、すぐれた画像
が得られた。For comparison, magnetic pole pieces of the same size and shape, all of which were made of pure iron, were arranged in the magnetic field generator of Example 1, and the rising characteristics of the gradient magnetic field and the image characteristics were similarly measured. The rising characteristic of the gradient magnetic field of the magnetic field generator according to the present invention was significantly improved as compared with the comparative example indicated by the one-dot chain line, as shown in practice in FIG. 3, and an excellent image was obtained.
【0020】[0020]
【発明の効果】この発明によるMRI用磁界発生装置
は、磁極片の主体を軟鉄材などの磁性材ベースで構成
し、その上に磁極片の周縁突起部の表層を積層けい素鋼
板またはソフトフェライトで形成、あるいはさらに周縁
突起部近傍以外の表層部をソフトフェライトで形成した
ことを特徴とし、けい素鋼板は飽和磁束密度Bsが高
く、空隙の磁界均一化が達成しやすく、また保磁力Hc
及びヒステリシス損の小さな電気的に絶縁されている薄
板を複数枚積層した構成であることから、傾斜磁界コイ
ルにGCパルスが通電されても周縁突起部近傍に発生す
る渦電流は低減され、しかも残磁現象を低減させること
も可能となる。さらに、磁極片の加工、製造が容易で組
立て作業性にすぐれている。In the magnetic field generator for MRI according to the present invention, the main body of the magnetic pole piece is composed of a magnetic material base such as a soft iron material, and the surface layer of the peripheral projection of the magnetic pole piece is laminated on the laminated silicon steel plate or soft ferrite. Or the surface layer portion other than the vicinity of the peripheral protrusion is formed of soft ferrite. The silicon steel sheet has a high saturation magnetic flux density Bs, and it is easy to achieve a uniform magnetic field in the air gap and a coercive force Hc.
Also, since a plurality of electrically insulated thin plates having a small hysteresis loss are laminated, the eddy current generated in the vicinity of the peripheral protrusion is reduced even when a GC pulse is applied to the gradient magnetic field coil, and the remaining It is also possible to reduce the magnetic phenomenon. Further, the magnetic pole pieces can be easily processed and manufactured and the assembling workability is excellent.
【図1】板状及び柱状継鉄を用いた磁気回路にこの発明
を適用したMRI用磁界発生装置の実施例を示す斜視説
明図であり、Aは全体、Bは磁極片を示す。FIG. 1 is a perspective explanatory view showing an embodiment of a magnetic field generator for MRI in which the present invention is applied to a magnetic circuit using plate-like and columnar yokes, where A is the whole and B is a pole piece.
【図2】筒状継鉄を用いた磁気回路にこの発明を適用し
たMRI用磁界発生装置の実施例を示す斜視説明図であ
り、Aは全体、Bは磁極片を示す。FIG. 2 is a perspective explanatory view showing an embodiment of a magnetic field generator for MRI in which the present invention is applied to a magnetic circuit using a tubular yoke, where A is the whole and B is the pole piece.
【図3】傾斜磁界の立ち上がり率を示す時間とGC磁界
強度の関係を示すグラフである。FIG. 3 is a graph showing a relationship between a time showing a rising rate of a gradient magnetic field and a GC magnetic field strength.
1 継鉄板
2 柱状継鉄
3,11a,11b,11c,11d,11e,11f
永久磁石構成体
4,13 磁極片
9,12 空隙
10 筒状継鉄
5,14 ベース材料
6,15 突起
7,16 表層部
8,17 中央突起部1 Yoke Iron Plate 2 Column Yoke 3, 3, 11a, 11b, 11c, 11d, 11e, 11f
Permanent magnet structure 4,13 Pole piece 9,12 Void 10 Cylindrical yoke 5,14 Base material 6,15 Protrusion 7,16 Surface layer portion 8,17 Central protrusion portion
───────────────────────────────────────────────────── フロントページの続き (72)発明者 青木 雅昭 大阪府三島郡島本町江川2丁目15ー17 住友特殊金属株式会社 山崎製作所内 (72)発明者 竹内 博幸 東京都千代田区内神田一丁目1番14号 株式会社 日立メディコ内 (72)発明者 竹島 弘隆 東京都千代田区内神田一丁目1番14号 株式会社 日立メディコ内 (56)参考文献 特開 平4−138131(JP,A) 特開 平4−138132(JP,A) 特開 平4−23411(JP,A) ─────────────────────────────────────────────────── ─── Continued front page (72) Inventor Masaaki Aoki 2-15-17 Egawa, Shimamoto-cho, Mishima-gun, Osaka Prefecture Sumitomo Special Metals Co., Ltd. Yamazaki Works (72) Inventor Hiroyuki Takeuchi 1-1-14 Kanda, Uchida, Chiyoda-ku, Tokyo Hitachi Medical Co., Ltd. (72) Inventor Hirotaka Takeshima 1-1-14 Kanda, Uchida, Chiyoda-ku, Tokyo Hitachi Medical Co., Ltd. (56) References JP-A-4-138131 (JP, A) JP-A-4-138132 (JP, A) JP-A-4-23411 (JP, A)
Claims (2)
置され、各々が対向面の周縁部に環状突起を形成された
一対の磁極片とを有し、該空隙内に所定の均一磁界を発
生させ、傾斜磁界を高速で切りかえるパルスシーケンス
を利用するMRI用磁界発生装置において、前記各磁極
片は、前記環状突起部の内周面及び前記環状突起部同志
の対向面が渦電流低減材の層で覆われていることを特徴
とするMRI用磁界発生装置。1. A magnetic field generation source and a pair of magnetic pole pieces, which are arranged so as to face each other with a gap therebetween, and each of which has an annular projection formed on a peripheral edge portion of the facing surface. A pulse sequence that generates a magnetic field and switches the gradient magnetic field at high speed
In each of the magnetic pole pieces, the inner peripheral surface of the annular protrusion and the opposing surfaces of the annular protrusions are covered with a layer of an eddy current reducing material. Magnetic field generator for MRI.
凹部内の底面が渦電流低減材の層で覆われていることを
特徴とする請求項1記載のMRI用磁界発生装置。2. The magnetic field generator for MRI according to claim 1, wherein each of the magnetic pole pieces has a bottom surface inside the concave portion of the annular projection portion covered with a layer of an eddy current reducing material.
Priority Applications (5)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP06339793A JP3445303B2 (en) | 1993-02-25 | 1993-02-25 | Magnetic field generator for MRI |
| US08/146,191 US5621324A (en) | 1992-03-18 | 1993-03-17 | Magnetic field generator for MRI |
| PCT/JP1993/000320 WO1993018707A1 (en) | 1992-03-18 | 1993-03-17 | Magnetic field generator for mri |
| DE69332601T DE69332601D1 (en) | 1992-03-18 | 1993-03-17 | MAGNETIC FIELD GENERATOR FOR IMAGE DISPLAY BY MEANS OF A CORE RESONANCE |
| EP93906787A EP0591542B1 (en) | 1992-03-18 | 1993-03-17 | Magnetic field generator for mri |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP06339793A JP3445303B2 (en) | 1993-02-25 | 1993-02-25 | Magnetic field generator for MRI |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPH06251930A JPH06251930A (en) | 1994-09-09 |
| JP3445303B2 true JP3445303B2 (en) | 2003-09-08 |
Family
ID=13228137
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP06339793A Expired - Lifetime JP3445303B2 (en) | 1992-03-18 | 1993-02-25 | Magnetic field generator for MRI |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3445303B2 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2953659B1 (en) * | 1998-08-06 | 1999-09-27 | 住友特殊金属株式会社 | Magnetic field generator for MRI, method of assembling the same, and method of assembling magnet unit used therein |
| JP3788573B2 (en) * | 2000-11-16 | 2006-06-21 | 信越化学工業株式会社 | MRI magnetic circuit assembly method |
-
1993
- 1993-02-25 JP JP06339793A patent/JP3445303B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPH06251930A (en) | 1994-09-09 |
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