JPH0244485Y2 - - Google Patents

Info

Publication number
JPH0244485Y2
JPH0244485Y2 JP20354985U JP20354985U JPH0244485Y2 JP H0244485 Y2 JPH0244485 Y2 JP H0244485Y2 JP 20354985 U JP20354985 U JP 20354985U JP 20354985 U JP20354985 U JP 20354985U JP H0244485 Y2 JPH0244485 Y2 JP H0244485Y2
Authority
JP
Japan
Prior art keywords
magnetic field
magnetic
yoke
air gap
pole piece
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
Application number
JP20354985U
Other languages
Japanese (ja)
Other versions
JPS62112106U (en
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 filed Critical
Priority to JP20354985U priority Critical patent/JPH0244485Y2/ja
Priority to US06/909,327 priority patent/US4679022A/en
Priority to DE8686307272T priority patent/DE3676066D1/en
Priority to EP86307272A priority patent/EP0228154B1/en
Publication of JPS62112106U publication Critical patent/JPS62112106U/ja
Application granted granted Critical
Publication of JPH0244485Y2 publication Critical patent/JPH0244485Y2/ja
Expired legal-status Critical Current

Links

Landscapes

  • Magnetic Resonance Imaging Apparatus (AREA)

Description

【考案の詳細な説明】 産業分野 この考案は、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
鳴断層装置(以下、NMR−CTという)に用い
られる永久磁石を使用した磁界発生装置に係り、
大きな空隙内に強力かつ高精度で均一な静磁界を
発生する磁界発生装置に関する。
[Detailed description of the invention] Industrial field This invention is a permanent magnet used in medical nuclear magnetic resonance tomography (hereinafter referred to as NMR-CT), which can obtain cross-sectional images of objects and depict the properties of tissues. Regarding the magnetic field generator used,
This invention relates to a magnetic field generator that generates a strong, highly accurate, and uniform static magnetic field within a large air gap.

背景技術 NMR−CTは、人体の一部または全部を1〜
10KGの強力な磁界を形成する空隙内に挿入して
所要の断層イメージを得るため、この磁界が強力
かつ10-4以下の精度で一様で安定していることが
要求され、NMR−CT用の磁界発生装置として
は、銅またはアルミニウムからなる導線を円筒状
に巻着した常伝導磁石あるいは、特殊な導線を用
い、絶縁零度付近の温度に冷却して使用する超伝
導磁石が知られている。
BACKGROUND ART
In order to obtain the desired tomographic image by inserting the device into an air gap that generates a strong magnetic field of 10 KG, this magnetic field must be strong, uniform, and stable with an accuracy of 10 -4 or less. Known magnetic field generators include normal conducting magnets made of conductive wire made of copper or aluminum wrapped in a cylindrical shape, and superconducting magnets that use special conducting wire cooled to a temperature close to zero insulation. .

前者は構造上安価であるが、膨大な電力と冷却
水が必要であり、ランニングコストが高く、一
方、後者の超伝導磁石は、冷却用冷媒として高価
な液体ヘリウム等の使用が不可欠であり、いわゆ
るイニシヤルコストとともにランニングコストも
著しく高い問題がある。
The former is structurally inexpensive, but requires a huge amount of electricity and cooling water, and has high running costs.On the other hand, the latter superconducting magnet requires the use of expensive liquid helium as a cooling medium. There is a problem in that not only the so-called initial cost but also the running cost is extremely high.

本出願人は、先に、磁界強度が上記の常伝導磁
石と同等以上で電力の消費もなく、小型軽量で高
精度均一磁界が得られる永久磁石回路を有する磁
界発生装置として、空隙を形成して対向する磁極
片と、少なくとも1の永久磁石とを継鉄で磁気的
結合し該空隙に磁界を発生させる磁界発生装置に
おいて、上記磁極片の対向面の各々に環状突起を
設けたことを特徴とする磁界発生装置を提案(特
開昭60−88407号)した。
The applicant has previously developed an air gap-forming magnetic field generating device that has a permanent magnet circuit that has a magnetic field strength equal to or higher than that of the above-mentioned normal conduction magnet, consumes no power, is small and lightweight, and can obtain a highly accurate uniform magnetic field. A magnetic field generating device for magnetically coupling magnetic pole pieces facing each other and at least one permanent magnet with a yoke to generate a magnetic field in the gap, characterized in that an annular protrusion is provided on each opposing surface of the magnetic pole pieces. proposed a magnetic field generator (Japanese Unexamined Patent Publication No. 88407/1988).

この磁界発生装置によつて、空隙に発生する磁
界の均一精度を向上させることができた。しか
し、実用化に際しては、さらに高精度の均一磁界
が要求されるため、磁界の微調整が必要であつ
た。
With this magnetic field generator, it was possible to improve the uniformity and accuracy of the magnetic field generated in the air gap. However, for practical use, a uniform magnetic field with even higher precision is required, so fine adjustment of the magnetic field is required.

また、高精度で均一かつ安定な磁界が得られる
磁気回路として、4本の円柱状継鉄を間隔部材と
して空隙を形成して磁気的に接続されかつ対向す
る一対の正方形の板状継鉄の対向面に永久磁石を
着設し、各永久磁石の対向面に環状突起を有する
磁極片を設けて、板状継鉄間距離を微調整可能と
なし、該空隙に磁界を発生させる磁界発生装置を
提案(特願昭59−113713号)した。
In addition, as a magnetic circuit that can obtain a highly accurate, uniform, and stable magnetic field, a pair of square plate-shaped yokes that are magnetically connected by using four cylindrical yokes as spacing members to form an air gap, and facing each other, are used. A magnetic field generator in which a permanent magnet is attached to the opposing surface, a magnetic pole piece having an annular projection is provided on the opposing surface of each permanent magnet, the distance between the plate yokes can be finely adjusted, and a magnetic field is generated in the gap. was proposed (Special Application No. 113713-1981).

上記磁界発生装置は、被診断対象物の空隙内へ
の進入方向が四方の任意方向で至便であり、正方
形の板状継鉄を用いることから、水平面での磁界
均一度が高い利点があるが、例えば、人体全体を
診断する場合は、該板状継鉄の大きさは、少なく
とも一辺が2000mm程度となり、頭部のみ診断に用
いる場合でも、一辺が1500mm程度の寸法を要する
ため、既設建物内への搬入容易性や、設置スペー
スの削減などの要求から、すぐれた磁界均一度を
維持したまま、さらに、小型軽量化することが望
まれていた。
The magnetic field generating device described above can conveniently enter the air gap of the object to be diagnosed in any direction on all four sides, and because it uses a square plate-shaped yoke, it has the advantage of high magnetic field uniformity on the horizontal plane. For example, when diagnosing the entire human body, the size of the plate yoke is at least 2000 mm on one side, and even when only the head is used for diagnosis, the size of the plate yoke is approximately 1500 mm on each side, so it cannot be used inside an existing building. Due to demands such as ease of transport and reduction of installation space, it has been desired to further reduce size and weight while maintaining excellent magnetic field uniformity.

考案の目的 この考案は、かかる現状に鑑み、強力な磁界が
得られる永久磁石を使用した磁界発生装置におい
て、空隙内に高精度で均一かつ安定な磁界が得ら
れる小型軽量の磁気回路を有する磁界発生装置を
目的としている。
Purpose of the invention In view of the current situation, this invention has been developed in a magnetic field generator using permanent magnets that can generate a strong magnetic field. It is intended as a generator.

考案の構成と効果 この考案は、高精度で均一かつ安定な磁界が得
られる小型の磁気回路を目的に種々検討した結
果、かかる永久磁石を用いた磁気回路において、
磁極片に環状突起を設け、かつこの環状突起に磁
性材の小片を適宜着設することにより、空隙内の
磁界微調整が可能であり、この磁界調整により高
精度の均一磁界が得られるため、磁気回路の小型
軽量化が可能となり、また、磁気回路空隙内の磁
界均一度が著しく向上し、高精度で均一な磁界域
を拡大できることを知見したものである。
Structure and effect of the invention This invention was developed as a result of various studies aimed at creating a compact magnetic circuit that can obtain a highly accurate, uniform, and stable magnetic field.
By providing an annular protrusion on the magnetic pole piece and appropriately attaching small pieces of magnetic material to the annular protrusion, it is possible to finely adjust the magnetic field within the air gap, and by adjusting the magnetic field, a highly accurate uniform magnetic field can be obtained. It has been discovered that it is possible to make the magnetic circuit smaller and lighter, and that the uniformity of the magnetic field within the magnetic circuit air gap is significantly improved, making it possible to expand the highly accurate and uniform magnetic field area.

すなわち、この考案は、空隙を形成して対向す
る一対の磁極片と、少なくとも1の永久磁石とを
継鉄で磁気的結合し、該空隙に磁界を発生させる
磁界発生装置において、磁極片の各対向面に環状
突起を設け、かつ環状突起の所揚箇所に、1また
は複数の磁性材からなる磁界調整片を着設したこ
とを特徴とする磁界発生装置である。
That is, this invention provides a magnetic field generating device in which a pair of magnetic pole pieces facing each other with an air gap and at least one permanent magnet are magnetically coupled with a yoke to generate a magnetic field in the air gap. This magnetic field generating device is characterized in that an annular protrusion is provided on the opposing surface, and a magnetic field adjustment piece made of one or more magnetic materials is attached to the landing position of the annular protrusion.

考案の好ましい構成 磁気回路は、少なくとも1の永久磁石を用い
て、空隙を介して対向させかつ対向面に環状突起
を設けた磁極片を継鉄で磁気的に結合すればいか
なる構成も利用でき、被診断対象物の大きさや装
置の設置スペース等に応じて、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、磁極片、環状突起の形状等を適宜選定する
ことが望ましい。
Preferred configuration of the invention The magnetic circuit can use any configuration as long as at least one permanent magnet is used and magnetic pole pieces facing each other with an air gap and provided with annular protrusions on the opposing surfaces are magnetically coupled with a yoke. Depending on the size of the object to be diagnosed, the installation space of the device, etc., the magnetic properties and shape of the permanent magnet, the shape and size of the yoke, the required air gap size, the shape of the magnetic pole piece, the annular protrusion, etc. should be selected as appropriate. is desirable.

また、継鉄形状は、磁界発生装置の全体形状並
びに設置スペースを決定するため、例えば、第1
図に示す長方形の板状継鉄と円柱状継鉄を用いる
構成や、第3図の円筒体継鉄等の省スペース性に
すぐれた形状が好ましく、特に、この考案による
磁界調整片を用いることにより、高精度な均一磁
界を得ることができるため、設置スペースに応じ
た継鉄形状等の設定、変更、修正が容易になる利
点がある。
In addition, the shape of the yoke determines the overall shape and installation space of the magnetic field generator, so for example,
A structure that uses a rectangular plate-shaped yoke and a cylindrical yoke as shown in the figure, or a configuration that is excellent in space-saving properties such as the cylindrical yoke shown in Fig. 3 is preferable, and in particular, it is preferable to use the magnetic field adjustment piece according to this invention. As a result, a highly accurate uniform magnetic field can be obtained, which has the advantage of making it easy to set, change, and modify the yoke shape etc. according to the installation space.

また、環状突起は、磁極面平面の周縁部や任意
の個所に、断面三角形や台形の突起とする等種々
形状の突起が採用でき、環状突起の内周面形状
は、上方へ拡大する傾斜面が好ましい。
In addition, the annular protrusion can have various shapes such as a triangular or trapezoidal cross-sectional protrusion on the periphery of the magnetic pole surface plane or any other location, and the inner peripheral surface shape of the annular protrusion is an inclined surface that expands upward. is preferred.

環状突起の所要箇所に着設する1または複数の
磁性材からなる磁界調整片は、いかなる形状、寸
法、数でもよく、また、その着設位置も、第2図
に示す如く、磁極片13に突設された環状突起1
5の上面a、内側傾斜面b、外周面cのいずれの
位置でもよく、寸法、形状、着設位置は、磁気回
路、永久磁石の磁気特性、磁極片の形状寸法、環
状突起の形状寸法などに応じて、所要の均一磁界
を得るべく適宜選定する必要がある。また、磁界
調整片は、磁気回路の組立後に適宜着設するほ
か、環状突起に一体化して設けるのもよい。
The magnetic field adjustment pieces made of one or more magnetic materials that are attached to desired locations on the annular protrusion may be of any shape, size, and number, and their attachment positions may be placed on the magnetic pole piece 13 as shown in FIG. Protruding annular projection 1
5 may be on the upper surface a, the inner inclined surface b, or the outer circumferential surface c, and the dimensions, shape, and mounting position may be determined by the magnetic circuit, the magnetic properties of the permanent magnet, the shape and size of the magnetic pole piece, the shape and size of the annular protrusion, etc. It is necessary to select it appropriately in order to obtain the required uniform magnetic field. Further, the magnetic field adjustment piece may be provided as appropriate after assembling the magnetic circuit, or may be provided integrally with the annular protrusion.

また、磁極片の対向方向の磁界の均一度を向上
させる目的で、前記磁界調整片とは別個に、磁極
片における該環状突起の中央に凸状突起を環状突
起と連続、非連続で設けるのもよい。
In addition, in order to improve the uniformity of the magnetic field in the direction in which the magnetic pole piece faces, a convex protrusion may be provided at the center of the annular protrusion on the magnetic pole piece, which may be continuous or discontinuous with the annular protrusion, separately from the magnetic field adjusting piece. Good too.

この考案の磁界発生装置に用いる永久磁石は、
フエライト磁石、アルニコ系磁石、希土類コバル
ト系磁石が使用できるが、先に出願人が提案し
た、高価なSmやCoを含有しない新しい高性能永
久磁石としてFe−B−R系永久磁石は、その最
大エネルギー積が大きいだけでなく、残留磁束密
度(Br)の温度係数が、0.07%/℃〜0.15%/℃
なる温度特性を有するため、この永久磁石を上記
のNMR−CTに適用することにより、装置の小
形化が達成でき、すぐれた性能が得られ、さら
に、この永久磁石の磁気特性は、特に0℃以下に
冷却して使用することにより、著しく高い最大エ
ネルギー積を得ることができ、磁石の有効利用が
できる。
The permanent magnet used in the magnetic field generator of this invention is
Ferrite magnets, alnico magnets, and rare earth cobalt magnets can be used, but Fe-B-R permanent magnets, which the applicant previously proposed as new high-performance permanent magnets that do not contain expensive Sm or Co, are the most effective. Not only is the energy product large, but the temperature coefficient of residual magnetic flux density (Br) is 0.07%/°C to 0.15%/°C.
By applying this permanent magnet to the above-mentioned NMR-CT, it is possible to downsize the device and obtain excellent performance. By cooling and using the magnet, a significantly higher maximum energy product can be obtained and the magnet can be used more effectively.

上記のFe−B−R系永久磁石は、R(RはNd,
Pr,Dy,Ho,Tbのうち少なくとも1種あるい
はさらにLa,Ce,Sm,Gd,Er,Eu,Tm,
Yb,Lu,Yのうち少なくとも1種)8原子%〜
30原子%、B2原子%〜28原子%、Fe42原子%〜
90原子%を主成分とし、主相が正方晶相からなる
永久磁石であり、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25MGOe以上の極めて高いエネルギー
積を示す、すぐれた永久磁石である。
The above Fe-BR-based permanent magnet has R (R is Nd,
At least one of Pr, Dy, Ho, Tb or further La, Ce, Sm, Gd, Er, Eu, Tm,
At least one of Yb, Lu, Y) 8 atomic % ~
30 atomic%, B2 atomic% ~ 28 atomic%, Fe42 atomic% ~
It is a permanent magnet whose main component is 90 atomic% and whose main phase is a tetragonal phase.R is a resource-rich light rare earth mainly Nd and Pr, and B and Fe are the main components. It is an excellent permanent magnet that exhibits an extremely high energy product.

図面に基づく考案の開示 第1図はこの考案による磁界発生装置を示す横
断上面図と正面説明図である。第2図は磁極片の
環状突起の詳細を示す説明図である。第3図はこ
の考案による他の磁界発生装置の縦断斜視図であ
る。
Disclosure of the invention based on the drawings FIG. 1 is a cross-sectional top view and a front explanatory view showing a magnetic field generating device according to the invention. FIG. 2 is an explanatory diagram showing details of the annular protrusion of the magnetic pole piece. FIG. 3 is a longitudinal sectional perspective view of another magnetic field generating device according to this invention.

第1図の磁気回路は、4本の円柱状継鉄10を
間隔部材として、これを長方形主面を有する板状
継鉄11の4隅に配置して、一対の板状継鉄11
間に空隙14を形成し、かつ一対の板状継鉄11
を磁気的に接続し、さらに、各板状継鉄11の対
向面に永久磁石12を着設し、各永久磁石12の
対向面に、環状突起15を有する円板状の磁極片
13を設けて、該空隙14に磁界を発生させる構
成からなる。
In the magnetic circuit shown in FIG. 1, four cylindrical yokes 10 are used as spacing members, and these are arranged at the four corners of a plate-shaped yoke 11 having a rectangular main surface, and a pair of plate-shaped yokes 11
A pair of plate-shaped yokes 11 with a gap 14 formed therebetween.
Further, a permanent magnet 12 is attached to the opposing surface of each plate-shaped yoke 11, and a disk-shaped magnetic pole piece 13 having an annular projection 15 is provided to the opposing surface of each permanent magnet 12. This configuration generates a magnetic field in the air gap 14.

磁極片13は、周縁部に断面台形の環状突起1
5を設けてあり、さらに環状突起15の中央にも
平円面状の突起部を設けてある。
The magnetic pole piece 13 has an annular protrusion 1 having a trapezoidal cross section on its periphery.
5 is provided, and a planar circular projection is also provided at the center of the annular projection 15.

上記の環状突起15には、板状継鉄11の短辺
に対抗する位置にある環状突起15の内側傾斜面
に、それぞれ磁界調整片16が着設してある。
Magnetic field adjustment pieces 16 are respectively attached to the inner inclined surfaces of the annular projections 15 at positions opposite to the short sides of the plate-shaped yoke 11.

また、一対の板状継鉄11の長辺中央部に、長
方形状の磁束シヤント材17を装着し、磁極片1
3に近接配置させてあり、磁束シヤント材17の
長孔に板状継鉄へのボルト止めをする構成によ
り、上下方向に移動可能となし、磁極片13から
の磁束のシヤント量を可変となしてある。
In addition, a rectangular magnetic flux shunt material 17 is attached to the center of the long side of the pair of plate yokes 11, and the magnetic pole piece 1
3, and is configured to bolt to the plate-shaped yoke through the elongated hole of the magnetic flux shunt material 17, making it movable in the vertical direction and making it possible to vary the shunt amount of magnetic flux from the magnetic pole piece 13. There is.

上記の構成において、環状突起15の付設によ
る磁界均一度の向上効果を、さらに高めることが
できる磁界調整片16による空隙14の所要空間
における磁界の均一度調整、並びに磁束シヤント
材17による磁極片13からの磁束の一部を分路
する効果、これらの相乗効果によつて、磁極片1
3周囲の磁界分布を、板状継鉄11が正方形であ
る場合と等価とし、極めて磁界均一度を得ること
ができる。
In the above configuration, the effect of improving the magnetic field uniformity by attaching the annular protrusion 15 can be further enhanced by adjusting the uniformity of the magnetic field in the required space of the air gap 14 by the magnetic field adjustment piece 16, and by adjusting the magnetic field uniformity in the magnetic pole piece 13 by the magnetic flux shunting material 17. The effect of shunting a part of the magnetic flux from the pole piece 1, due to the synergistic effect of these
The magnetic field distribution around 3 is made equivalent to the case where the plate-shaped yoke 11 is square, and extremely uniform magnetic field can be obtained.

この磁束シヤント材17は、その先端部が磁極
片13対向面と板状継鉄11の永久磁石12着設
面間に配置され、該先端部が平面となつたL字型
構成のほか、磁束シヤント材17が磁気回路外に
配置されたり、また、永久磁石12の側端面側の
板状継鉄11上に直接配置するなど、磁界調整片
16と伴に均一磁界を得るため、その配置や形状
が適宜選択される。
This magnetic flux shunt material 17 has an L-shaped configuration in which its tip is arranged between the facing surface of the magnetic pole piece 13 and the permanent magnet 12 mounting surface of the plate-shaped yoke 11, and the tip is flat. In order to obtain a uniform magnetic field together with the magnetic field adjusting piece 16, the shunt material 17 may be placed outside the magnetic circuit or placed directly on the plate-shaped yoke 11 on the side end surface of the permanent magnet 12. The shape is selected appropriately.

前記の磁気回路において、板状磁極片は、板状
継鉄の短辺(L)と長辺(W)との比率L/W
は、被診断対象物の大きさ、磁極片の該短辺方向
の寸法(D)、板状継鉄を磁気的に接続する継鉄
の形状、寸法等に応じて適宜選定するが、通常
1.5〜2.5程度が望ましい。
In the above magnetic circuit, the plate-shaped magnetic pole piece has a ratio L/W of the short side (L) and the long side (W) of the plate-shaped yoke.
is selected as appropriate depending on the size of the object to be diagnosed, the dimension (D) of the magnetic pole piece in the short side direction, the shape and dimensions of the yoke that magnetically connects the plate yoke, but usually
Approximately 1.5 to 2.5 is desirable.

また、板状継鉄の短辺(L)と磁極片の該短辺
方向の寸法(D)との比が0.6未満では、空隙に
おける水平面での磁界均一度の低下は僅かである
が、磁気回路の小型化が実現できず、また、1.2
を越えると、板状継鉄からの突出部が増えて、該
磁極片よりの漏洩磁束が増加し、空隙内の磁界均
一度と伴に磁界強度も低下させるため、該比D/
Lを0.6〜1.2となすが、該、永久磁石の磁気特
性、板状継鉄及びこの板状継鉄を磁気的に接続す
る継鉄の形状寸法、及び所要空隙の大きさ等に応
じて適宜選定することが望ましい。
Furthermore, if the ratio of the short side (L) of the plate-shaped yoke to the dimension (D) of the magnetic pole piece in the short side direction is less than 0.6, the magnetic field uniformity on the horizontal plane in the air gap will decrease slightly, but the magnetic It is not possible to miniaturize the circuit, and 1.2
If the ratio D/
L is set to 0.6 to 1.2, but it can be adjusted as appropriate depending on the magnetic properties of the permanent magnet, the shape and dimensions of the plate yoke and the yoke that magnetically connects the plate yoke, and the size of the required air gap. It is desirable to select

第3図に示す磁気回路は、一対のFe−B−R
系永久磁石20の各々の一方端に磁極片21固着
して対向させ、永久磁石20の他方端を、円筒体
からなりその円周部の一部を開口した形状の継鉄
22を結合し、磁極片21間の空隙23内に、静
磁界を発生させる構成であり、一対の磁極片21
には、その対向面の周縁に、所定の内径、高さか
らなる断面三角形の環状突起24を突設し、Fe
−B−R系永久磁石20は同一方向に磁化してあ
る。
The magnetic circuit shown in Fig. 3 consists of a pair of Fe-B-R
A magnetic pole piece 21 is fixed to one end of each of the system permanent magnets 20 to face each other, and the other end of the permanent magnet 20 is connected to a yoke 22 which is made of a cylindrical body and has a part of its circumference open. It is configured to generate a static magnetic field in the air gap 23 between the magnetic pole pieces 21, and the pair of magnetic pole pieces 21
An annular protrusion 24 with a triangular cross section having a predetermined inner diameter and height is protruded from the periphery of the opposing surface of the Fe.
-BR permanent magnets 20 are magnetized in the same direction.

この環状突起24の内側傾斜面の対向位置、す
なわち、継鉄22の開口よりの被診断対象物の進
退方向に直交方向の対向位置に、それぞれ3個の
磁界調整片25を着設してある。これにより、空
隙23の所要空間内における磁界の均一度を調
整、向上させることができる。
Three magnetic field adjusting pieces 25 are installed at opposing positions on the inner inclined surface of this annular protrusion 24, that is, at opposing positions perpendicular to the advancing and retreating direction of the object to be diagnosed from the opening of the yoke 22. . Thereby, the uniformity of the magnetic field within the required space of the air gap 23 can be adjusted and improved.

実施例 第1図に示した構成において、最大エネルギー
積35MGOeの特性を有するFe−B−R系板状永
久磁石を用い、磁極片の対向距離として、450mm
に設定し、板状磁極片寸法、1000mmL×1800mmW
×120mmT、磁極片外径Dを950mmとし、組立を行
なつたのち、環状突起の内側傾斜面に磁界調整片
を着設した。
Example In the configuration shown in Figure 1, Fe-B-R plate permanent magnets having a maximum energy product of 35 MGOe are used, and the opposing distance of the magnetic pole pieces is 450 mm.
Plate magnetic pole piece dimensions: 1000mmL x 1800mmW
x 120 mm T and a magnetic pole piece outer diameter D of 950 mm. After assembly, a magnetic field adjustment piece was attached to the inner inclined surface of the annular projection.

磁界調整片は磁極片中心からみて、板状長辺方
向中心軸を中心に45゜の範囲内に、13mmφ×8mm
φ×5mmの鉄製の磁界調整片を7個づつ着設する
ことにより、空隙中心より半径100mmの水平面に
おける板状継鉄の短辺方向と長辺方向の磁界均一
度が170ppmから70ppmとなつた。
The magnetic field adjustment piece is 13mmφ x 8mm within a 45° range around the central axis in the long side direction of the plate when viewed from the center of the magnetic pole piece.
By installing seven φ x 5 mm iron magnetic field adjustment pieces, the magnetic field uniformity in the short and long sides of the plate yoke on a horizontal plane with a radius of 100 mm from the center of the gap was changed from 170 ppm to 70 ppm. .

また、さらに、400mm長さ×250mm幅×15mm厚み
寸法の磁束シヤント材を付設し、これを上下動さ
せて調整したところ、前記水平面での磁界均一度
は、10ppm以下のすぐれた値が得られた。
Furthermore, when we attached a magnetic flux shunt material with dimensions of 400 mm length x 250 mm width x 15 mm thickness and adjusted it by moving it up and down, an excellent value of less than 10 ppm was obtained for the magnetic field uniformity on the horizontal plane. Ta.

また、上記の構成からなる本考案の磁界発生装
置の場合、その設置スペースは、同等の均一磁界
で比較すると、板状継鉄を正方形とした比較磁界
発生装置の80%程度でよく、装置の小型軽量化に
すぐれていることが分る。
In addition, in the case of the magnetic field generator of the present invention having the above configuration, the installation space is about 80% of that of a comparative magnetic field generator with a square plate yoke when compared with an equivalent uniform magnetic field. It can be seen that it is excellent in size and weight reduction.

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

第1図はこの考案による磁界発生装置を示す横
断上面図と正面説明図である。第2図は磁極片の
環状突起の詳細を示す説明図である。第3図はこ
の考案による他の磁界発生装置の縦断斜視図であ
る。 10……円柱状継鉄、11……板状継鉄、1
2,20……Fe−B−R系永久磁石、13,2
1……磁極片、14,23……空隙、15,24
……環状突起、16,25……磁界調整片、17
……磁束シヤント材、22……継鉄。
FIG. 1 is a cross-sectional top view and a front explanatory view showing a magnetic field generating device according to this invention. FIG. 2 is an explanatory diagram showing details of the annular protrusion of the magnetic pole piece. FIG. 3 is a longitudinal sectional perspective view of another magnetic field generating device according to this invention. 10...Cylindrical yoke, 11...Plate yoke, 1
2,20...Fe-BR-based permanent magnet, 13,2
1...Magnetic pole piece, 14, 23...Air gap, 15, 24
...Annular projection, 16, 25...Magnetic field adjustment piece, 17
...Magnetic flux shunt material, 22...Yoke.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 空隙を形成して対向する一対の磁極片と、少な
くとも1の永久磁石とを継鉄で磁気的結合し、該
空隙に磁界を発生させる磁界発生装置において、
磁極片の各対向面に環状突起を設け、かつ環状突
起の所要箇所に、1または複数の磁性材からなる
磁界調整片を着設したことを特徴とする磁界発生
装置。
A magnetic field generating device that magnetically couples a pair of magnetic pole pieces facing each other with an air gap and at least one permanent magnet using a yoke to generate a magnetic field in the air gap,
1. A magnetic field generating device characterized in that an annular projection is provided on each opposing surface of a magnetic pole piece, and magnetic field adjusting pieces made of one or more magnetic materials are attached at required locations on the annular projection.
JP20354985U 1985-12-27 1985-12-27 Expired JPH0244485Y2 (en)

Priority Applications (4)

Application Number Priority Date Filing Date Title
JP20354985U JPH0244485Y2 (en) 1985-12-27 1985-12-27
US06/909,327 US4679022A (en) 1985-12-27 1986-09-19 Magnetic field generating device for NMR-CT
DE8686307272T DE3676066D1 (en) 1985-12-27 1986-09-22 DEVICE FOR GENERATING MAGNETIC FIELDS FOR MAGNETIC NUCLEAR RESONANCE TOMOGRAPHY.
EP86307272A EP0228154B1 (en) 1985-12-27 1986-09-22 Magnetic field generating device for nmr-ct

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP20354985U JPH0244485Y2 (en) 1985-12-27 1985-12-27

Publications (2)

Publication Number Publication Date
JPS62112106U JPS62112106U (en) 1987-07-17
JPH0244485Y2 true JPH0244485Y2 (en) 1990-11-27

Family

ID=31168983

Family Applications (1)

Application Number Title Priority Date Filing Date
JP20354985U Expired JPH0244485Y2 (en) 1985-12-27 1985-12-27

Country Status (1)

Country Link
JP (1) JPH0244485Y2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
WO2003075757A1 (en) * 2002-03-14 2003-09-18 Hitachi, Ltd. Magnet device and magnetic resonance imaging using the same

Also Published As

Publication number Publication date
JPS62112106U (en) 1987-07-17

Similar Documents

Publication Publication Date Title
US4672346A (en) Magnetic field generating device for NMR-CT
JPH0244485Y2 (en)
JP2764458B2 (en) Magnetic field generator for MRI
JPH0244483Y2 (en)
JPH0345886B2 (en)
JPH0244486Y2 (en)
JPH0244484Y2 (en)
JPH037124B2 (en)
JPH10146326A (en) Magnetic field generator for mri
JPH0249683Y2 (en)
JP2557905B2 (en) Magnetic field generator
JPH0246003Y2 (en)
JPH0537446Y2 (en)
JP3056883B2 (en) Magnetic field generator for MRI
JPH0246002Y2 (en)
JPH0421107Y2 (en)
JPH0246004Y2 (en)
JPH0246001Y2 (en)
JPH0241842Y2 (en)
JPH0320053B2 (en)
JPS6088407A (en) Magnetic field generating device
JPH0241841Y2 (en)
JPH0314012Y2 (en)
JP3059596B2 (en) Magnetic field generator for MRI
JPH0314207B2 (en)