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JPH0223010B2 - - Google Patents
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JPH0223010B2 - - Google Patents

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Publication number
JPH0223010B2
JPH0223010B2 JP58196785A JP19678583A JPH0223010B2 JP H0223010 B2 JPH0223010 B2 JP H0223010B2 JP 58196785 A JP58196785 A JP 58196785A JP 19678583 A JP19678583 A JP 19678583A JP H0223010 B2 JPH0223010 B2 JP H0223010B2
Authority
JP
Japan
Prior art keywords
magnetic field
magnetic
magnetic pole
permanent magnet
annular protrusion
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
Application number
JP58196785A
Other languages
Japanese (ja)
Other versions
JPS6088407A (en
Inventor
Takanobu Myamoto
Hideya Sakurai
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Proterial Ltd
Original Assignee
Sumitomo Special Metals Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Sumitomo Special Metals Co Ltd filed Critical Sumitomo Special Metals Co Ltd
Priority to JP58196785A priority Critical patent/JPS6088407A/en
Publication of JPS6088407A publication Critical patent/JPS6088407A/en
Publication of JPH0223010B2 publication Critical patent/JPH0223010B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01FMAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
    • H01F7/00Magnets
    • H01F7/02Permanent magnets [PM]
    • H01F7/0273Magnetic circuits with PM for magnetic field generation
    • H01F7/0278Magnetic circuits with PM for magnetic field generation for generating uniform fields, focusing, deflecting electrically charged particles
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R33/00Arrangements or instruments for measuring magnetic variables
    • G01R33/20Arrangements or instruments for measuring magnetic variables involving magnetic resonance
    • G01R33/28Details of apparatus provided for in groups G01R33/44 - G01R33/64
    • G01R33/38Systems for generation, homogenisation or stabilisation of the main or gradient magnetic field
    • G01R33/383Systems for generation, homogenisation or stabilisation of the main or gradient magnetic field using permanent magnets

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Magnetic Resonance Imaging Apparatus (AREA)

Description

【発明の詳細な説明】 利用産業分野 この発明は、医療用核磁気共鳴断層撮影装置に
用いられる永久磁石を使用した磁界発生装置に係
り、被検者の一部または全部が挿入可能な大きな
空間部に、強力かつ高精度で均一な磁界を長時間
安定して発生する永久磁石式磁界発生装置に関す
る。
[Detailed Description of the Invention] Field of Application The present invention relates to a magnetic field generating device using a permanent magnet used in a medical nuclear magnetic resonance tomography device, and the present invention relates to a magnetic field generating device using a permanent magnet used in a medical nuclear magnetic resonance tomography device. Partly, the present invention relates to a permanent magnet type magnetic field generator that stably generates a strong, highly accurate, and uniform magnetic field over a long period of time.

背景技術 医療用核磁気共鳴断層撮影装置{NMR−CT
あるいは医療用MRI(Magnetic Resonance
Lmaging)等、以下医療用MRIと称する)}は、
強力な磁界を形成する磁界発生装置の空〓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。
Background technology Medical nuclear magnetic resonance tomography device {NMR-CT
Or medical MRI (Magnetic Resonance)
(hereinafter referred to as medical MRI)},
Inside the sky of a magnetic field generator that creates a strong magnetic field,
This device is capable of inserting part or all of a subject into the test subject, obtaining a tomographic image of the object, and depicting the nature of its tissue.

上記医療用MRIの磁界発生装置において、空
〓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〓内の例えば、所要半径の球
体空間の撮像視野内には、0.05〜2.0T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。
In the medical MRI magnetic field generator described above, the space must be wide enough to allow part or all of the subject to be inserted, and in order to obtain a clear tomographic image, usually, for example, Within the imaging field of view of a spherical space with the required radius, there is a
It is required to create a stable and strong uniform magnetic field with an accuracy of 10 -4 or less.

医療用MRI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、絶対零
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。
As magnetic field generators for medical MRI, there are two types of magnets: normal conductive magnets made of copper or aluminum conductive wire wrapped around a cylinder, and superconducting magnets that use special conductive wire cooled to a temperature close to absolute zero. It is being

前者は構造上安価であるが十分な強力磁界を発
生させるためには、膨大な電力とこれに伴う発熱
を冷却するための膨大な冷却水が必要であり、ラ
ンニングコストが高く、コイルが作る大きな漏洩
磁界は使用用途によつては悪影響の要因となる等
の問題があり、一方、後者の超伝導磁石は、電力
の消費が少なく小型で強力な磁界を発生し得る利
点があるが、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という問
題がある。
The former is structurally inexpensive, but in order to generate a sufficiently strong magnetic field, it requires a huge amount of electric power and a huge amount of cooling water to cool down the heat generated by this, resulting in high running costs and the large size generated by the coil. Leakage magnetic fields may cause problems depending on the intended use, while the latter type of superconducting magnets have the advantage of consuming less power and being able to generate strong magnetic fields in a small size. The use of expensive liquid helium or the like is essential, and there is a problem that the so-called initial cost and running cost are extremely high.

永久磁石を用いた磁気回路の場合、例えば、人
の頭部あるいは全身が入る程度の大きな空間に発
生させた磁界の強度が、前述した常伝導、超伝導
電磁石と同等に得られるのであるならば、電力の
消費もなく、漏洩磁界は弱く、上記用途の実用化
に理想的であるといえるが、現在知られている構
成の磁気回路では、実用化に際して種々の問題を
生じ、その用途が極めて限定されてしまう。
In the case of a magnetic circuit using permanent magnets, for example, if the strength of the magnetic field generated in a space large enough to fit a person's head or whole body can be obtained equal to that of the normal conducting or superconducting electromagnets mentioned above. , there is no power consumption, the leakage magnetic field is weak, and it can be said that it is ideal for the practical application of the above-mentioned applications. However, the magnetic circuit of the currently known configuration causes various problems when it is put into practical use, and its application is extremely difficult. It will be limited.

また、電磁石を用いて磁極間距離が4cm程度の
ごく小さな空〓に高均一磁界を発生させるMRI
用磁気回路が提案されている。詳述すると、対向
した平坦面からなる磁極間の中心を通る横断平面
を想定すると、中心から所要距離位置では距離に
比例して僅かずつ磁界が減衰していることに鑑
み、磁極面に磁界の減衰に見合うだけの厚みを有
する磁性材を順次配置、すなわち、磁極面外周側
へ順次厚みを増した環状の補助磁極を配置する構
成の磁気回路が提案(特公昭35−7545号公報)さ
れている。
In addition, MRI uses electromagnets to generate a highly uniform magnetic field in a very small space with a distance between magnetic poles of about 4 cm.
magnetic circuits have been proposed. To be more specific, assuming a transverse plane passing through the center between magnetic poles consisting of opposing flat surfaces, the magnetic field attenuates slightly at a required distance from the center in proportion to the distance. A magnetic circuit has been proposed (Japanese Patent Publication No. 7545/1983) in which magnetic materials having a thickness sufficient for attenuation are sequentially arranged, that is, an annular auxiliary magnetic pole whose thickness is gradually increased toward the outer periphery of the magnetic pole surface. There is.

さらに、対向した平坦面からなる磁極における
磁極材料の透磁率の影響を考慮すると、磁極面上
で得られる磁界の等高線たる等磁面は所要曲率の
凸球面であることを知見し、これを補償するため
磁極面を、予め該影響に基づいて算出して所要曲
率の凹球面にラツピングした構成のMRI用磁気
回路が提案(特公昭36−4664号公報)されてい
る。
Furthermore, considering the influence of the magnetic permeability of the magnetic pole material on the magnetic poles consisting of opposing flat surfaces, we found that the isomagnetic surfaces, which are the contour lines of the magnetic field obtained on the magnetic pole surfaces, are convex spherical surfaces with the required curvature, and we compensated for this. Therefore, an MRI magnetic circuit has been proposed (Japanese Patent Publication No. 36-4664) in which the magnetic pole surface is calculated in advance based on this influence and wrapped into a concave spherical surface with a required curvature.

かかる提案は、磁極径が非常に大きく磁極間距
離が磁極径に比較して非常に小さい場合は、磁極
間の磁界強さが均一であるとの考えに立脚し、磁
極間距離に対する磁極径の比、磁極径D、磁極間
距離Lgとすると、D/Lgの大きな(D/Lg=5
〜10)電磁石式磁気回路、すなわち、磁極間距離
が4cm程度のごく小さな空〓に高均一磁界を発生
させるものであり、特に、小さな試料などが入る
中心空間では極めて高い均一磁界が得られてい
る。
This proposal is based on the idea that when the magnetic pole diameter is very large and the distance between the magnetic poles is very small compared to the magnetic pole diameter, the magnetic field strength between the magnetic poles is uniform. ratio, magnetic pole diameter D, and distance between magnetic poles Lg, if D/Lg is large (D/Lg=5
~10) An electromagnetic magnetic circuit, which generates a highly uniform magnetic field in a very small space with a distance between magnetic poles of about 4 cm.In particular, an extremely high uniform magnetic field can be obtained in the central space where a small sample is placed. There is.

ところが、逆に磁極径Dに対する磁極間距離
Lgの比の大きな永久磁石磁気回路、すなわち、
人の頭部あるいは全身が入る程度の磁極間方向の
距離の大きな空間でかつ永久磁石を用いた磁界発
生装置に、上記の磁極片の磁性材料を増減させて
凹球面状に形成し磁極片間の中心横断面(x−y
平面)上の磁界を補正する技術を適用しても、前
記磁気回路の空〓とは比較にならないほど磁極片
間方向(Lg、z軸方向)に著しく拡大された広
大な三次元空間であるため、医療用MRIとして
要求される所要の高均一磁界を得ることは全くで
きない。
However, conversely, the distance between the magnetic poles with respect to the magnetic pole diameter D
A permanent magnet magnetic circuit with a large ratio of Lg, i.e.
In a magnetic field generator using permanent magnets, the distance between the magnetic poles is large enough to fit a person's head or whole body, and the magnetic material of the magnetic pole pieces is increased or decreased to form a concave spherical shape. Center cross section (x-y
Even if we apply technology to correct the magnetic field on the magnetic circuit (plane), it is a vast three-dimensional space that is significantly expanded in the direction between the magnetic pole pieces (Lg, z-axis direction), which is incomparable to the sky in the magnetic circuit. Therefore, it is completely impossible to obtain the required highly uniform magnetic field required for medical MRI.

また、上記提案は電磁石式磁気回路であり、所
要の高均一磁界を長時間安定して得ることができ
ず、膨大な電力とこれに伴う発熱を冷却するため
の膨大な冷却水が必要であり、ランニングコスト
が高いという問題がある。
In addition, the above proposal is an electromagnetic magnetic circuit, which cannot stably obtain the required high uniform magnetic field for a long time, and requires a huge amount of power and a huge amount of cooling water to cool down the heat generated. , there is a problem of high running costs.

発明の目的 この発明は、強力な磁界が得られる永久磁石を
用いたMRI用の磁界発生装置が提案されていな
い現状に鑑み、永久磁石を使用し強力な磁界が得
られ、かつ空〓において、人の頭部あるいは全身
が入る程度の大きな空間で高精度で均一かつ安定
な磁界が得られる磁気回路を有する磁界発生装置
の提供を目的としている。
Purpose of the Invention In view of the current situation where no magnetic field generating device for MRI using permanent magnets that can generate a strong magnetic field has been proposed, the present invention has been developed to generate The object of the present invention is to provide a magnetic field generating device having a magnetic circuit that can obtain a highly accurate, uniform, and stable magnetic field in a space large enough to accommodate a person's head or whole body.

発明の概要 この発明は、 空〓を形成して対向する永久磁石を継鉄で磁気
的結合し、各永久磁石の空〓対向面に磁極片を着
設して、該空〓中央部の所要空間内に高均一磁界
を発生させる医療用核磁気共鳴断層装置用の永久
磁石式磁界発生装置において、 上記磁極片の対向面周縁部の各々に下記式を満
足する環状突起を設けたことを特徴とする永久磁
石式磁界発生装置である。
Summary of the Invention This invention forms a space and magnetically couples opposing permanent magnets with a yoke, attaches a magnetic pole piece to the surface of each permanent magnet facing the space, and connects the space as required in the center of the space. A permanent magnet type magnetic field generator for a medical nuclear magnetic resonance tomography apparatus that generates a highly uniform magnetic field in a space, characterized in that an annular projection satisfying the following formula is provided on each peripheral edge of the opposing surface of the magnetic pole piece. This is a permanent magnet type magnetic field generator.

D2≧1/2・D1 H≦1/4・Lg 但し、D1;磁極片外径、 D2;環状突起内径、 Lg;磁極片間距離、 H;環状突起の高さ。 D 2 ≧1/2・D 1 H≦1/4・Lg However, D 1 : External diameter of the magnetic pole piece, D 2 : Inner diameter of the annular protrusion, Lg : Distance between the magnetic pole pieces, H : Height of the annular protrusion.

発明の構成 この発明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を必ずしも含有しない新しい
高性能永久磁石であるFe−B−R系(RはYを
含む希土類元素のうち少なくとも1種)永久磁石
(特願昭57−145072号は、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MRIに
適用することにより、装置の小形化が達成でき、
すぐれた性能を得られ、さらに、この永久磁石を
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る性質を
有効に利用できる。
Structure of the invention The permanent magnet used in the magnetic field generating device of this invention is
Ferrite magnets, alnico magnets, and rare earth cobalt magnets can be used, but Fe-B-R magnets (R is Y (at least one kind of rare earth element containing %/℃, so by applying this permanent magnet to the above MRI, it is possible to downsize the device.
Excellent performance can be obtained, and furthermore, by cooling this permanent magnet to 0° C. or below, it is possible to effectively utilize the property that a significantly high maximum energy product can be obtained.

上記Fe−B−R系永久磁石は、R(但しRはY
を含む希土類元素のうち少なくとも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 is R (where R is Y
(at least one of rare earth elements containing It is an excellent permanent magnet that uses resource-rich light rare earths such as Nd and Pr as R, and has B and Fe as its main components and exhibits an extremely high energy product of 25 MGOe or more.

この発明による永久磁石式磁界発生装置の磁気
回路は、後述の実施例に限定されるものでなく、
空〓を介して対向した一対の永久磁石のそれぞれ
に、環状突起を対向面に設けた磁極片を配置でき
る構成であればいかなる磁気回路にも適用でき
る。
The magnetic circuit of the permanent magnet type magnetic field generator according to the present invention is not limited to the embodiments described below.
The present invention can be applied to any magnetic circuit as long as it has a configuration in which a pair of permanent magnets facing each other with a space in between is provided with a magnetic pole piece having annular projections on opposing surfaces.

環状突起の形状寸法も、永久磁石の寸法、磁気
特性、空〓の大きさにより適宜選定すればよい
が、特に、下記範囲内が有効である。
The shape and dimensions of the annular protrusion may be appropriately selected depending on the dimensions of the permanent magnet, the magnetic properties, and the size of the cavity, but the following range is particularly effective.

D2≧1/2・D1 H≦1/4・Lg 但し、D1;磁極片外径、 D2;環状突起内径、 Lg;磁極片間距離、 H;環状突起の高さ。 D 2 ≧1/2・D 1 H≦1/4・Lg However, D 1 : External diameter of the magnetic pole piece, D 2 : Inner diameter of the annular protrusion, Lg : Distance between the magnetic pole pieces, H : Height of the annular protrusion.

さらに、環状突起の内周側の内径面は、上方へ
拡がる傾斜面とすることにより、より良好な均一
磁界が安定して得られる。
Furthermore, by forming the inner diameter surface on the inner peripheral side of the annular protrusion into an inclined surface that expands upward, a more uniform magnetic field can be stably obtained.

なお、磁極片間距離Lgは、例えば、第1図の
場合は、各磁極片の環状突起内径D2の測定点、
すなわち内径面の傾斜始点である平坦面部間の距
離である。
In addition, the distance Lg between the magnetic pole pieces is, for example, in the case of FIG. 1, the measurement point of the annular protrusion inner diameter D 2 of each magnetic pole piece,
In other words, it is the distance between the flat surface portions that are the starting points of the inclination of the inner diameter surface.

図面に基づく発明の開示 第1図はこの発明による永久磁石式磁界発生装
置を示す縦断説明図である。第2図a〜dは第1
図における磁極片の環状突起の種々の形状を示す
縦断説明図である。
DISCLOSURE OF THE INVENTION BASED ON THE DRAWINGS FIG. 1 is a longitudinal sectional view showing a permanent magnet type magnetic field generating device according to the present invention. Figures 2 a to d are the first
FIG. 6 is a vertical cross-sectional view showing various shapes of the annular protrusions of the magnetic pole pieces in the figures.

第1図に示す永久磁石式磁界発生装置は、一対
のFe−B−R系永久磁石1の各々の一方端に磁
極片2を固着して対向させ、他方端を継鉄3で結
合した構成からなり、磁極片2間の空〓4は人体
の一部または全部を入れて診断できる程度の大き
な空間であり、該空〓4内に0.05〜2.0Tの強い磁
界を発生させる。
The permanent magnet type magnetic field generator shown in FIG. 1 has a structure in which a pair of Fe-B-R permanent magnets 1 are each fixed with a magnetic pole piece 2 at one end facing each other, and the other end is connected with a yoke 3. The space 4 between the magnetic pole pieces 2 is large enough to accommodate part or all of a human body for diagnosis, and a strong magnetic field of 0.05 to 2.0 T is generated within the space 4.

また、一対の磁極片2はそれぞれ外径がD1
あり、空〓4側の対向面の周縁部には、内径D2
高さH寸法で断面形状が台形状でかつ内周面が上
方に拡大する如き傾斜面を形成した環状突起5が
突設してあり、この一対の磁極片2が対向する空
〓4中心部の所要空間に高精度で均一かつ安定し
た磁界が得られる。
Each of the pair of magnetic pole pieces 2 has an outer diameter of D 1 , and the outer diameter of the opposing surface on the air 4 side has an inner diameter of D 2 ,
An annular protrusion 5 having a height H dimension, a trapezoidal cross-sectional shape, and an inclined surface whose inner peripheral surface expands upward is protruded, and the pair of magnetic pole pieces 2 face each other at the center of the hollow 4. A highly accurate, uniform, and stable magnetic field can be obtained in the required space.

第2図には磁極片2の縦断面図を示すが、同図
aは環状突起5断面が三角形の場合、同図bは環
状突起5断面が台形の場合、同図cは環状突起5
断面が三角形で内径側斜面が湾曲している場合、
同図dは環状突起5断面が台形でそのの角部の面
取りを行ない曲面構成として場合を示している。
FIG. 2 shows longitudinal cross-sectional views of the magnetic pole piece 2. FIG. 2a shows a case where the annular projection 5 has a triangular cross section, FIG.
If the cross section is triangular and the inner slope is curved,
Figure d shows a case where the annular protrusion 5 has a trapezoidal cross section and its corners are chamfered to form a curved surface.

いずれの環状突起5も、内径面が上方に拡大す
る如き傾斜面を形成し、磁極片2間距離をLgと
すると、D2≧1/2・D1、H≦1/4・Lgを満足して
いる。
Each of the annular protrusions 5 forms an inclined surface such that the inner diameter surface expands upward, and if the distance between the magnetic pole pieces 2 is Lg, then D 2 ≧1/2・D 1 and H≦1/4・Lg are satisfied. are doing.

ちなみに、第1図に示した構成の磁界発生装置
に、常温時の(BH)maxが30MGOeを示すFe−
B−R系永久磁石を用い、Lgを350mmに設定し、
D1=500mm、D2=400mm、H=30mmの環状突起を
有する磁極片を配置した場合と、環状突起を有し
ない外径500mmの磁極片を配置した場合の空〓内
の磁界分布を測定したところ、環状突起を有する
この発明の場合は比較例に比べて、均一磁界の
10-3領域の体積が3倍に拡大した。
By the way, the magnetic field generator with the configuration shown in Figure 1 has an Fe-
Using a B-R permanent magnet, set Lg to 350mm,
Measure the magnetic field distribution in the air when a magnetic pole piece with an annular protrusion of D 1 = 500 mm, D 2 = 400 mm, and H = 30 mm is placed, and when a magnetic pole piece with an outer diameter of 500 mm without an annular protrusion is placed. As a result, in the case of this invention having an annular protrusion, compared to the comparative example, the uniform magnetic field was
The volume of the 10 -3 region expanded three times.

また、この発明の構成による磁極片の場合、同
一の磁界強度で比較すると、上記の比較例よりも
ずつと小径の磁極片並びに磁石でよく、小型軽量
化に有利であつた。
Further, in the case of the magnetic pole piece according to the structure of the present invention, when compared at the same magnetic field strength, the magnetic pole piece and magnet were required to have a smaller diameter than those of the above-mentioned comparative example, which was advantageous in reducing the size and weight.

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

第1図はこの発明による永久磁石式磁界発生装
置を示す縦断説明図である。第2図a〜dは第1
図における磁極片の環状突起の種々の形状を示す
縦断説明図である。 1……Fe−B−R系永久磁石、2……磁極片、
3……継鉄、4……空〓、5……環状突起。
FIG. 1 is a longitudinal sectional view showing a permanent magnet type magnetic field generator according to the present invention. Figures 2 a to d are the first
FIG. 6 is a vertical cross-sectional view showing various shapes of the annular protrusions of the magnetic pole pieces in the figures. 1... Fe-BR-based permanent magnet, 2... Magnetic pole piece,
3... Yoke, 4... Sky, 5... Annular protrusion.

Claims (1)

【特許請求の範囲】 1 空〓を形成して対向する永久磁石を継鉄で磁
気的結合し、各永久磁石の空〓対向面に磁極片を
着設して、該空〓中央部の所要空間内に高均一磁
界を発生させる医療用核磁気共鳴断層撮影装置用
の永久磁石式磁界発生装置において、 上記磁極片の対向面周縁部の各々に下記式を満
足する環状突起を設けたことを特徴とする永久磁
石式磁界発生装置。 D2≧1/2・D1 H≦1/4・Lg 但し、D1;磁極片外径、 D2;環状突起内径、 Lg;磁極片間距離、 H;環状突起の高さ。
[Scope of Claims] 1. Permanent magnets facing each other are magnetically coupled by a yoke to form a void, and a magnetic pole piece is attached to the surface of each permanent magnet facing the void, and a required amount of space is provided in the center of the void. In a permanent magnet type magnetic field generator for a medical nuclear magnetic resonance tomography apparatus that generates a highly uniform magnetic field in a space, an annular protrusion satisfying the following formula is provided on each peripheral edge of the opposing surface of the magnetic pole piece. Characteristic permanent magnet type magnetic field generator. D 2 ≧1/2・D 1 H≦1/4・Lg However, D 1 : External diameter of the magnetic pole piece, D 2 : Inner diameter of the annular protrusion, Lg : Distance between the magnetic pole pieces, H : Height of the annular protrusion.
JP58196785A 1983-10-19 1983-10-19 Magnetic field generating device Granted JPS6088407A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58196785A JPS6088407A (en) 1983-10-19 1983-10-19 Magnetic field generating device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58196785A JPS6088407A (en) 1983-10-19 1983-10-19 Magnetic field generating device

Publications (2)

Publication Number Publication Date
JPS6088407A JPS6088407A (en) 1985-05-18
JPH0223010B2 true JPH0223010B2 (en) 1990-05-22

Family

ID=16363593

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58196785A Granted JPS6088407A (en) 1983-10-19 1983-10-19 Magnetic field generating device

Country Status (1)

Country Link
JP (1) JPS6088407A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0691548A1 (en) 1994-07-08 1996-01-10 Sumitomo Special Metals Company Limited Magnetic field generating device for use in MRI

Families Citing this family (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US4827235A (en) * 1986-07-18 1989-05-02 Kabushiki Kaisha Toshiba Magnetic field generator useful for a magnetic resonance imaging instrument
US4931760A (en) * 1986-10-08 1990-06-05 Asahi Kasei Kogyo Kabushiki Kaisha Uniform magnetic field generator
DE69129687T2 (en) 1990-09-29 1999-03-11 Sumitomo Special Metals Co., Ltd., Osaka Device for generating a magnetic field for imaging by means of magnetic resonance
US10446307B2 (en) * 2017-05-23 2019-10-15 AOSense, Inc. Magnetic field generators based on high magnetic permeability materials

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP0691548A1 (en) 1994-07-08 1996-01-10 Sumitomo Special Metals Company Limited Magnetic field generating device for use in MRI

Also Published As

Publication number Publication date
JPS6088407A (en) 1985-05-18

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