JPH0244484Y2 - - Google Patents
Info
- Publication number
- JPH0244484Y2 JPH0244484Y2 JP19483385U JP19483385U JPH0244484Y2 JP H0244484 Y2 JPH0244484 Y2 JP H0244484Y2 JP 19483385 U JP19483385 U JP 19483385U JP 19483385 U JP19483385 U JP 19483385U JP H0244484 Y2 JPH0244484 Y2 JP H0244484Y2
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- plate
- magnetic field
- yoke
- yokes
- 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
Links
- 230000004907 flux Effects 0.000 description 15
- 239000000463 material Substances 0.000 description 12
- 230000000694 effects Effects 0.000 description 4
- 230000007423 decrease Effects 0.000 description 3
- 238000009434 installation Methods 0.000 description 3
- 229910052777 Praseodymium Inorganic materials 0.000 description 2
- 229910052772 Samarium Inorganic materials 0.000 description 2
- 238000000034 method Methods 0.000 description 2
- 229910052761 rare earth metal Inorganic materials 0.000 description 2
- 150000002910 rare earth metals Chemical class 0.000 description 2
- 229910052684 Cerium Inorganic materials 0.000 description 1
- RYGMFSIKBFXOCR-UHFFFAOYSA-N Copper Chemical compound [Cu] RYGMFSIKBFXOCR-UHFFFAOYSA-N 0.000 description 1
- 229910052692 Dysprosium Inorganic materials 0.000 description 1
- 229910052691 Erbium Inorganic materials 0.000 description 1
- 229910052693 Europium Inorganic materials 0.000 description 1
- 229910052688 Gadolinium Inorganic materials 0.000 description 1
- 229910052765 Lutetium Inorganic materials 0.000 description 1
- 238000005481 NMR spectroscopy Methods 0.000 description 1
- -1 Nd and Pr Chemical class 0.000 description 1
- 229910052779 Neodymium Inorganic materials 0.000 description 1
- 229910052775 Thulium Inorganic materials 0.000 description 1
- 229910052769 Ytterbium Inorganic materials 0.000 description 1
- 229910000828 alnico Inorganic materials 0.000 description 1
- 229910052782 aluminium Inorganic materials 0.000 description 1
- XAGFODPZIPBFFR-UHFFFAOYSA-N aluminium Chemical compound [Al] XAGFODPZIPBFFR-UHFFFAOYSA-N 0.000 description 1
- 229910052796 boron Inorganic materials 0.000 description 1
- 229910017052 cobalt Inorganic materials 0.000 description 1
- 239000010941 cobalt Substances 0.000 description 1
- GUTLYIVDDKVIGB-UHFFFAOYSA-N cobalt atom Chemical compound [Co] GUTLYIVDDKVIGB-UHFFFAOYSA-N 0.000 description 1
- 230000000052 comparative effect Effects 0.000 description 1
- 239000002826 coolant Substances 0.000 description 1
- 238000001816 cooling Methods 0.000 description 1
- 239000000498 cooling water Substances 0.000 description 1
- 229910052802 copper Inorganic materials 0.000 description 1
- 239000010949 copper Substances 0.000 description 1
- RKTYLMNFRDHKIL-UHFFFAOYSA-N copper;5,10,15,20-tetraphenylporphyrin-22,24-diide Chemical compound [Cu+2].C1=CC(C(=C2C=CC([N-]2)=C(C=2C=CC=CC=2)C=2C=CC(N=2)=C(C=2C=CC=CC=2)C2=CC=C3[N-]2)C=2C=CC=CC=2)=NC1=C3C1=CC=CC=C1 RKTYLMNFRDHKIL-UHFFFAOYSA-N 0.000 description 1
- 230000008878 coupling Effects 0.000 description 1
- 238000010168 coupling process Methods 0.000 description 1
- 238000005859 coupling reaction Methods 0.000 description 1
- 238000003745 diagnosis Methods 0.000 description 1
- 230000005611 electricity Effects 0.000 description 1
- 229910052734 helium Inorganic materials 0.000 description 1
- 239000001307 helium Substances 0.000 description 1
- SWQJXJOGLNCZEY-UHFFFAOYSA-N helium atom Chemical compound [He] SWQJXJOGLNCZEY-UHFFFAOYSA-N 0.000 description 1
- 238000009413 insulation Methods 0.000 description 1
- 229910052742 iron Inorganic materials 0.000 description 1
- 229910052746 lanthanum Inorganic materials 0.000 description 1
- 239000007788 liquid Substances 0.000 description 1
- 230000003068 static effect Effects 0.000 description 1
- 238000003325 tomography Methods 0.000 description 1
- 229910052727 yttrium Inorganic materials 0.000 description 1
- 229910000859 α-Fe Inorganic materials 0.000 description 1
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. However, there is a problem in that not only the 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 piece. proposed a magnetic field generator (Japanese Unexamined Patent Publication No. 88407/1988).
また、高精度で均一かつ安定な磁界が得られる
磁気回路を目的に種々検討した結果、第4図に示
す如く、4本の円柱状継鉄1を間隔部材として空
隙5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2の対向面に永久磁石3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4を設けて、板状継鉄2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 result of various studies aimed at creating a magnetic circuit that can obtain a highly accurate, uniform, and stable magnetic field, we found that four cylindrical yokes 1 are used as spacing members to form gaps 5, as shown in Permanent magnets 3 are attached to opposing surfaces of a pair of square plate yokes 2 connected to and facing each other, and a magnetic pole piece 4 having an annular projection is provided on the opposing surface of each permanent magnet. proposed a magnetic field generating device (Japanese Patent Application No. 113,713/1983) that could finely adjust the distance between the gaps and generate a magnetic field in the gap.
上記磁界発生装置は、被診断対象物の空隙5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2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2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 has the advantage that the object to be diagnosed can enter the air gap 5 in any direction in any four directions, and because it uses the square plate-shaped yoke 2, the magnetic field uniformity on the horizontal plane is high. However, for example, when diagnosing the entire human body, the size of the plate-shaped yoke 2 is
At least one side is approximately 2,000 mm, and even if only the head is used for diagnosis, a side of approximately 1,500 mm is required. Therefore, excellent magnetic field uniformity is required due to requirements such as ease of transport into existing buildings and reduction of installation space. It was desired to further reduce the size and weight while maintaining the same characteristics.
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、前述の第4図の磁気回路において、板状継鉄
を長方形とし、少なくとも長辺側に磁性薄板を配
置することによつて、磁気回路の小型軽量化とと
もに、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 As a result of various studies aimed at creating a compact magnetic circuit that can obtain a highly accurate, uniform, and stable magnetic field, this invention was developed by making the plate yoke rectangular in the magnetic circuit shown in Fig. 4 above. It has been discovered that by arranging magnetic thin plates at least on the long sides, it is possible to reduce the size and weight of the magnetic circuit, significantly improve the magnetic field uniformity within the magnetic circuit gap, and expand the highly accurate and uniform magnetic field area. It is.
すなわち、この考案は、柱状継鉄を間隔部材と
して空隙を形成し磁気的に接続して対向する一対
の板状継鉄の対向面に永久磁石を着設し、各永久
磁石の対向面に磁極片を設けて、該空隙に磁界を
発生させる磁界発生装置において、一対の板状継
鉄を長方形となし、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D/Lを0.6
〜1.2となし、少なくとも板状継鉄の長辺側に、
板状継鉄に当接または近接する磁性薄板を配置し
たことを特徴とする磁界発生装置である。 That is, in this invention, permanent magnets are attached to the opposing surfaces of a pair of plate-shaped yokes that are magnetically connected by using columnar yokes as spacing members to form an air gap, and magnetic poles are attached to the opposing surfaces of each permanent magnet. In a magnetic field generating device that generates a magnetic field in the air gap by providing a pair of plate yokes, the short side (L) of the plate yoke and the dimension (D) of the magnetic pole piece in the direction of the short side are ) and the ratio D/L is 0.6
~1.2, at least on the long side of the plate yoke,
This is a magnetic field generating device characterized in that a magnetic thin plate is arranged in contact with or in close proximity to a plate-shaped yoke.
考案の好ましい構成
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、寸法等の応じて適宜
選定するが、通常1.5〜2.5程度が望ましい。Preferred configuration of the invention In the plate-shaped magnetic pole piece, the ratio L/W of the short side (L) and the long side (W) of the plate-shaped yoke is determined by the size of the object to be diagnosed;
It is appropriately selected depending on the dimension (D) of the magnetic pole piece in the direction of the short side, the shape and dimensions of the yoke to which the plate yoke is magnetically connected, and it is usually desirably about 1.5 to 2.5.
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
また、板状継鉄の短辺と永久磁石の当該方向の
寸法比は、永久磁石の形状等によるが磁極片と同
程度とするのが望ましい。 Furthermore, the dimensional ratio between the short side of the plate-shaped yoke and the permanent magnet in this direction is preferably about the same as that of the magnetic pole piece, although it depends on the shape of the permanent magnet.
この考案において、磁性薄板は、磁極片からの
磁束の一部を分路して、磁極片周囲の磁界分布
を、板状継鉄が正方形である場合と等価とし、か
つ磁気シールド効果を有するもので、少なくとも
板状継鉄の長辺側に配置し、幅は2/3W以上、あ
るいは磁極片の該長辺方向寸法相当以上の寸法が
望ましい、板状継鉄に着設したり、磁気回路外に
配置するなど、任意の設置方法が採用できる。 In this invention, the magnetic thin plate shunts part of the magnetic flux from the magnetic pole piece, making the magnetic field distribution around the magnetic pole piece equivalent to that of a square plate yoke, and has a magnetic shielding effect. The magnetic circuit is placed at least on the long side of the plate yoke, and preferably has a width of 2/3W or more, or a size equivalent to the length of the magnetic pole piece in the long side direction. Any installation method can be used, such as placing it outside.
また、磁性薄板の厚みtは、板状継鉄厚みTの
場合、t/T=0.005〜0.05が好ましく、厚すぎ
ると空隙内の磁界強度が低下し、また、薄すすぎ
ると前記のシヤント効果及び磁気シールド効果が
低下するため、永久磁石の磁気特性、磁極片形
状、寸法、空隙寸法などに応じて適宜選定する必
要がある。 In addition, the thickness t of the magnetic thin plate is preferably t/T = 0.005 to 0.05 in the case of the plate-like yoke thickness T. If it is too thick, the magnetic field strength in the gap will decrease, and if it is too thin, the above-mentioned shunt effect will occur. In addition, since the magnetic shielding effect decreases, it is necessary to select an appropriate amount according to the magnetic properties of the permanent magnet, the shape and size of the magnetic pole pieces, the gap size, etc.
また、磁極片は、種々形状が採用でき、磁極面
に環状の突起を設けるのもよく、磁極面平面の周
縁部や任意の箇所に断面三角形や台形の突起とす
るなど、種々の形状の突起が採用でき、また、環
状突起の中央に凸状突起を連続、非連続で設ける
のもよい。 In addition, the magnetic pole piece can have various shapes, and it is good to have an annular protrusion on the magnetic pole face, or a protrusion with a triangular or trapezoidal cross section on the periphery of the plane of the magnetic pole face or at any other location. It is also possible to provide convex projections in the center of the annular projection in a continuous or discontinuous manner.
また、板状継鉄を磁気的に接続する柱状継鉄
は、四方を開放できる4本の円柱状継鉄や開口部
を一方向とする一対の板状や角柱状継鉄を適宜選
定できる。 Further, as the columnar yokes that magnetically connect the plate yokes, four columnar yokes that can be opened on all sides, or a pair of plate or square columnar yokes that have an opening in one direction can be appropriately selected.
この考案において、磁性薄板と同様目的で、磁
極片からの磁束の一部を分路して、磁極片周囲の
磁界分布を、板状継鉄が正方形である場合と等価
とする磁束シヤント材を磁極片に近接または当接
させて配置するのもよく、その形状、寸法は、磁
極片に近接または当接する位置、永久磁石の磁気
特性などに応じて、適宜選定されるべきであり、
さらに、配置方法も磁極片への距離や位置関係を
可変となしたり、磁気回路外に設けたり、直接、
板状継鉄の着設するなど種々の手段が採用でき
る。 This idea uses a magnetic flux shunt material that has the same purpose as the magnetic thin plate and shunts part of the magnetic flux from the magnetic pole piece to make the magnetic field distribution around the magnetic pole piece equivalent to that when the plate-shaped yoke is square. It may also be placed close to or in contact with the magnetic pole piece, and its shape and dimensions should be selected appropriately depending on the position close to or in contact with the magnetic pole piece, the magnetic properties of the permanent magnet, etc.
Furthermore, the arrangement method is such that the distance and positional relationship to the magnetic pole piece can be varied, or it can be placed outside the magnetic circuit, or directly,
Various means can be adopted, such as installing a plate-like yoke.
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 important. 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図と第3図は
この考案による磁束シヤント材の配置を示す縦断
説明図である。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. FIGS. 2 and 3 are longitudinal cross-sectional views showing the arrangement of magnetic flux shunt materials according to this invention.
実施例の磁気回路は、4本の円柱状継鉄1を間
隔部材として、これを長方形主面を有する板状継
鉄2の4隅に配置して、一対の板状継鉄2間に空
隙5を形成し、かつ一対の板状継鉄2を磁気的に
接続し、さらに、各板状継鉄2の対向面に永久磁
石3を着設し、各永久磁石3の対向面に、環状突
起6を有する円板状の磁極片4を設けて、該空隙
5に磁界を発生させる構成からなる。 In the magnetic circuit of the embodiment, four cylindrical yokes 1 are used as spacing members, and these are arranged at the four corners of a plate-shaped yoke 2 having a rectangular main surface, thereby creating a gap between the pair of plate-shaped yokes 2. 5, and the pair of plate yokes 2 are magnetically connected, and furthermore, a permanent magnet 3 is attached to the opposing surface of each plate yoke 2, and an annular magnet is attached to the opposing surface of each permanent magnet 3. It has a configuration in which a disk-shaped magnetic pole piece 4 having a protrusion 6 is provided to generate a magnetic field in the gap 5.
磁極片4は、周縁部に断面台形の環状突起を6
を設けてあり、さらに環状突起6の中央にも平円
面状の突起部を設けてある。 The magnetic pole piece 4 has 6 annular protrusions with a trapezoidal cross section on its periphery.
Furthermore, a planar circular projection is provided at the center of the annular projection 6.
一対の板状継鉄2の長辺側に当接し、同部間を
全面的に覆うように、磁性薄板7が着設してあ
る。この磁性薄板7は中央部に空隙への開口8を
開設してあり、ここより被診断対象物を侵入させ
る構成である。 A magnetic thin plate 7 is attached so as to come into contact with the long sides of the pair of plate-shaped yokes 2 and completely cover the area between them. This magnetic thin plate 7 has an opening 8 to the air gap in the center thereof, through which the object to be diagnosed is allowed to enter.
また、一対の板状継鉄2の長辺中央部に、前記
の磁性薄板7を一部切欠して、長方形状の磁束シ
ヤント材9を装着し、磁極片4に近接配置させて
あり、磁束シヤント材9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、シヤント量を可変となしてある。 In addition, a rectangular magnetic flux shunt material 9 is attached to the center portion of the long side of the pair of plate-shaped yokes 2 by cutting out a portion of the magnetic thin plate 7, and is placed close to the magnetic pole piece 4. By bolting the shunt material 9 to the plate-like yoke through the elongated holes, it can be moved vertically and the amount of shunt can be varied.
この磁性薄板7と磁束シヤント材9とにより、
磁極片4からの磁束の一部を分路して、磁極片4
周囲の磁界分布を、板状継鉄2が正方形である場
合と等価とすることができる。 With this magnetic thin plate 7 and magnetic flux shunt material 9,
A portion of the magnetic flux from the pole piece 4 is shunted to the pole piece 4.
The surrounding magnetic field distribution can be made equivalent to the case where the plate-shaped yoke 2 is square.
この磁性薄板7と磁束シヤント材9は、各々単
独で配置することができ、磁性薄板7は、一対の
板状継鉄2の短辺側にも着設して、磁気回路に接
続するほか、第2図の如く、磁気回路を被包する
ように磁気回路外にも配置でき、均一磁界を得る
ため、その配置や形状が適宜選択される。 The magnetic thin plate 7 and the magnetic flux shunt material 9 can be arranged independently, and the magnetic thin plate 7 can also be attached to the short sides of the pair of plate yokes 2 to connect to the magnetic circuit. As shown in FIG. 2, it can be placed outside the magnetic circuit so as to enclose the magnetic circuit, and its placement and shape are appropriately selected in order to obtain a uniform magnetic field.
また同様に、磁束シヤント材9も種々形状と配
置が選定でき、通常、その先端部が磁極片4対向
面と板状継鉄2着設面間、第2図H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、
第3図の如く、磁性薄板7と伴に磁束シヤント材
9が磁気回路外に配置するなど、均一磁界を得る
ため、その配置や形状が適宜選択される。 Similarly, the magnetic flux shunt material 9 can be selected from various shapes and arrangements, and its tip is usually placed between the opposing surface of the magnetic pole piece 4 and the mounting surface of the plate-shaped yoke 2, between H in FIG. In addition to the L-shaped configuration with flat parts,
As shown in FIG. 3, the arrangement and shape of the magnetic flux shunting material 9 are appropriately selected in order to obtain a uniform magnetic field, such as by arranging the magnetic flux shunting material 9 together with the magnetic thin plate 7 outside the magnetic circuit.
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、板状継鉄寸法、1000mmL×1800mmW×120
mmT、磁極片外径Dを950mmとし、一対の板状継
鉄長辺側に厚さ2.5mmの磁性薄板を着設して組立
を行なつたところ、空隙中心における水平面上の
半径100mm内の磁界均一度は50ppm以下のすぐれ
た値が得られ、さらに、400mm長さ×250mm幅×15
mm厚さ寸法の磁束シヤント材を設置し、これを上
下動させて調整したところ、空隙中心における水
平面上の半径100mm内の磁界均一度は20ppm以下
の極めてすぐれた値が得られた。Example In the configuration shown in Fig. 1, an Fe-B-R permanent magnet having a maximum energy product of 35 MGOe is used, the facing distance of the magnetic pole pieces is set to 450 mm, and the plate yoke dimensions are 1000 mm L x 1800mmW×120
mmT, the outer diameter D of the magnetic pole piece is 950 mm, and a magnetic thin plate with a thickness of 2.5 mm is attached to the long side of a pair of plate yokes. Excellent magnetic field uniformity of less than 50 ppm was obtained, and in addition, 400 mm length x 250 mm width x 15
When a magnetic flux shunt material with a thickness of mm was installed and adjusted by moving it up and down, an extremely excellent magnetic field uniformity of less than 20 ppm was obtained within a radius of 100 mm on the horizontal plane at the center of the gap.
また、上記の構成からなる実施例の磁界発生装
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、第4図の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 embodiment with the above configuration, the installation space is 80% of that of the comparative magnetic field generator shown in Fig. 4 when compared with an equivalent uniform magnetic field.
It can be seen that the size and weight of the device are excellent.
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図と第3図は
この考案による磁束シヤント材の配置を示す縦断
説明図である。第4図は磁界発生装置を示す横断
上面図と正面説明図である。
1……円柱状継鉄、2……板状継鉄、3……
Fe−B−R系永久磁石、4……磁極片、5……
空隙、6……環状突起、7……磁性薄板、8……
開口、9……磁束シヤント材。
FIG. 1 is a cross-sectional top view and a front explanatory view showing a magnetic field generating device according to this invention. FIGS. 2 and 3 are longitudinal cross-sectional views showing the arrangement of magnetic flux shunt materials according to this invention. FIG. 4 is a cross-sectional top view and a front explanatory view showing the magnetic field generating device. 1...Cylindrical yoke, 2...Plate yoke, 3...
Fe-BR-based permanent magnet, 4... magnetic pole piece, 5...
Air gap, 6... Annular projection, 7... Magnetic thin plate, 8...
Opening, 9...Magnetic flux shunt material.
Claims (1)
に接続して対向する一対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磁極片を
設けて、該空隙に磁界を発生させる磁界発生装置
において、一対の板状継鉄を長方形となし、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D/Lを0.6〜1.2となし、少なくと
も板状継鉄の長辺側に、板状継鉄に当接または近
接する磁性薄板を配置したことを特徴とする磁界
発生装置。 Permanent magnets are attached to the opposing surfaces of a pair of plate-shaped yokes that are magnetically connected with the columnar yokes used as spacing members to form a gap, and magnetic pole pieces are provided on the opposing surfaces of each permanent magnet. In a magnetic field generating device that generates a magnetic field in an air gap, a pair of plate yokes are rectangular, and the ratio of the short side (L) of the plate yoke to the dimension (D) of the magnetic pole piece in the short side direction is D/ A magnetic field generating device characterized in that L is set to 0.6 to 1.2, and a magnetic thin plate is arranged at least on the long side of the plate-shaped yoke in contact with or close to the plate-shaped yoke.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19483385U JPH0244484Y2 (en) | 1985-12-17 | 1985-12-17 |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP19483385U JPH0244484Y2 (en) | 1985-12-17 | 1985-12-17 |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS62101206U JPS62101206U (en) | 1987-06-27 |
| JPH0244484Y2 true JPH0244484Y2 (en) | 1990-11-27 |
Family
ID=31152172
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP19483385U Expired JPH0244484Y2 (en) | 1985-12-17 | 1985-12-17 |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0244484Y2 (en) |
-
1985
- 1985-12-17 JP JP19483385U patent/JPH0244484Y2/ja not_active Expired
Also Published As
| Publication number | Publication date |
|---|---|
| JPS62101206U (en) | 1987-06-27 |
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