JPS6088407A - Magnetic field generating device - Google Patents
Magnetic field generating deviceInfo
- Publication number
- JPS6088407A JPS6088407A JP58196785A JP19678583A JPS6088407A JP S6088407 A JPS6088407 A JP S6088407A JP 58196785 A JP58196785 A JP 58196785A JP 19678583 A JP19678583 A JP 19678583A JP S6088407 A JPS6088407 A JP S6088407A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic field
- pole pieces
- air gap
- magnetic
- annular projections
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F7/00—Magnets
- H01F7/02—Permanent magnets [PM]
- H01F7/0273—Magnetic circuits with PM for magnetic field generation
- H01F7/0278—Magnetic circuits with PM for magnetic field generation for generating uniform fields, focusing, deflecting electrically charged particles
-
- G—PHYSICS
- G01—MEASURING; TESTING
- G01R—MEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
- G01R33/00—Arrangements or instruments for measuring magnetic variables
- G01R33/20—Arrangements or instruments for measuring magnetic variables involving magnetic resonance
- G01R33/28—Details of apparatus provided for in groups G01R33/44 - G01R33/64
- G01R33/38—Systems for generation, homogenisation or stabilisation of the main or gradient magnetic field
- G01R33/383—Systems 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)
Abstract
Description
【発明の詳細な説明】
この発明は、対象物の断面イメージを得て組織の性質ま
で描き出すことのできる医療用核磁気共鳴断層装置(以
下、NMR−CTという)等に用いられる大きな空隙内
に強力かつ高精度で均一な磁界を発生する磁界発生装置
に関す−る。DETAILED DESCRIPTION OF THE INVENTION The present invention provides a method for detecting a cross-sectional image of a target object in a large cavity used in a medical nuclear magnetic resonance tomography system (hereinafter referred to as NMR-CT), which can depict the properties of tissues. This invention relates to a magnetic field generator that generates a strong, highly accurate, and uniform magnetic field.
N M R−CTは、人体の一部または全部を1〜10
K G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、NM
R−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。NMR-CT tests part or all of the human body at 1 to 10
In order to obtain the required tomographic image by inserting it into the air gap that forms the strong magnetic field of KG, this magnetic field is strong and 10-4
It is required to be uniform and stable with the following accuracy, NM
Magnetic field generators for R-CT include normal conducting magnets made of conductive wire made of copper or aluminum wrapped around them in a cylindrical shape, and superconducting magnets that use special conducting wire and are cooled to a temperature close to absolute zero. Are known.
前者は構造上安価であるが十分な強力磁界を発生ざμる
ためには、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、コイルが作る漏洩磁界は使用用途によ
っ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Φ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、いわゆるイニシャルコス
トとともにランニングコストも著しく高い問題があり、
汎用されるには至っていない。The former is structurally inexpensive, but in order to generate a sufficiently strong magnetic field, it requires a huge amount of electricity and cooling water, resulting in high running costs, and the leakage magnetic field created by the coil can be a negative factor depending on the application. On the other hand, the latter type of superconducting magnet has the advantage of consuming less power and being small and generating a strong magnetic field, but it requires the use of expensive liquid helium or the like as a coolant. , there is a problem that the running cost is extremely high as well as the so-called initial cost.
It has not yet become widely used.
また、永久磁石回路は、もし磁界の強度が上記のソレノ
イド、電磁石と同等に1りられるのならば、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、現在用・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 addition, if the magnetic field strength of a permanent magnet circuit can be equal to that of the above-mentioned solenoids and electromagnets, it can be said that it consumes no power and has a weak leakage magnetic field, making it ideal for practical use in the above applications. However, the currently used magnetic circuits have various problems when put into practical use, and their applications are extremely limited.
この発明は、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の空隙におい“C1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
る磁界発生装置を目的としている。In view of the current situation, the present invention aims to provide a magnetic field generator having a magnetic circuit that can obtain a uniform and stable magnetic field with high precision in the air gap of a magnetic field generator using permanent magnets that can obtain a strong magnetic field. There is.
すなわち、この発明は、空隙を形成して対向づる磁極片
と、すくなくとも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ぼる磁界発生装置において、上記
!!磁極片対向面の各々に環状突起を設りたことを特徴
とJ−る磁界発生装置である。That is, the present invention provides a magnetic field generating device in which magnetic pole pieces facing each other with an air gap are magnetically coupled to at least one permanent magnet using a yoke to generate a magnetic field in the air gap. ! This magnetic field generating device is characterized in that an annular projection is provided on each of the opposing surfaces of the magnetic pole pieces.
この発明の磁界発生装置に用いる永久磁石は、フェライ
ト磁石、アルニコ系磁石、希土類コバル1−系磁石が使
用できるが、先に出願人が従業した、高価なSmやGを
含有しない新しい^性能永久磁石としてFe−8’−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57−145012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11(Br
>の温度係数が、0.07%/℃〜0.15%/℃なる
温度特性を有づるため、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、
すぐれた性能を得られ、さらに、この永久磁石の磁気特
性が特に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る性質を有
効に利」できる。The permanent magnet used in the magnetic field generator of the present invention can be a ferrite magnet, an alnico magnet, or a rare earth Kobal 1-based magnet. Fe-8'-R as a magnet
The system (R is at least one rare earth element including Y) permanent magnet (Japanese Patent Application No. 57-145012) not only has a large maximum energy product, but also has a residual magnetic flux density of 11 (Br
> has a temperature coefficient of 0.07%/℃ to 0.15%/℃, so this permanent magnet can be
By applying it to CT, the device can be made smaller.
Excellent performance can be obtained, and furthermore, the magnetic properties of this permanent magnet, especially when used after being cooled to 0° C. or below, can be effectively utilized to obtain a significantly high maximum energy product.
上記のFe−B−R系永久磁石は、[<り但しRはYを
含む希土類元素のうち少なくとも1種)8原イ%〜30
原子%、B 2原子%〜28原子%、Fe42原子%〜
90原子%を主成分とし、主相が正方晶相かうなる永久
磁石であり、Rとして陶やPrを中心とする資源的に豊
富な軽希土類を用い、El、Feを主成分として25M
GOe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-mentioned Fe-B-R permanent magnet has a composition of 8% to 30% (where R is at least one rare earth element including Y)
atomic%, B 2 atomic% to 28 atomic%, Fe42 atomic% to
It is a permanent magnet whose main component is 90 atomic % and whose main phase is a tetragonal phase.R is a light rare earth that is abundant in resources, mainly ceramics and Pr, and 25M is made with El and Fe as the main components.
It is an excellent permanent magnet that exhibits an extremely high energy product exceeding GOe.
以下、この発明を図面に基づいて詳述する。Hereinafter, this invention will be explained in detail based on the drawings.
第1図は、N M R−CT装置に使用する磁気回路の
説明図であり、一対のFe’E3R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、磁極片(2)間の空隙(4)
内に1〜10K Gの強い磁界を発生させ、この空隙内
に人体の一部または全部を入れて診断する構成である。FIG. 1 is an explanatory diagram of a magnetic circuit used in the NMR-CT device, in which a pair of Fe'E3R permanent magnets (1) are each fixed with a magnetic pole piece (2) at one end and faced to each other. , the other end is connected with a yoke (3), and the air gap (4) between the pole pieces (2) is
A strong magnetic field of 1 to 10 KG is generated within the cavity, and a part or all of the human body is inserted into this cavity for diagnosis.
一対の磁極片(2)は外形がDlでその対向面の周縁に
、内径Dz+高ざ1」なる環状突起(5)が突設してあ
り、空隙(4)で対向さ眩ることにより、高精度で均一
かつ安定した磁界が得られる。この環状突起(5)は内
径面が上方へ拡がる傾斜面であれば、良好な均一磁界が
安定して得られる。The pair of magnetic pole pieces (2) have an outer diameter of Dl, and an annular protrusion (5) with an inner diameter of Dz + height of 1'' is protruded from the periphery of the opposing surface, and the two magnetic pole pieces (2) face each other in the gap (4). A highly accurate, uniform and stable magnetic field can be obtained. If the annular protrusion (5) has an inclined inner surface that expands upward, a good uniform magnetic field can be stably obtained.
第2図には磁極片(2)の縦断面図を承りが、同a図は
断面が三角形の場合、同す図は断面が台形の場合、同C
図は断面三角形の内径側斜面が湾曲している場合、同d
図は例えば断面台形のものの角部の面取りを行ない曲面
構成とした場合を示す。Figure 2 shows a vertical cross-sectional view of the magnetic pole piece (2); Figure A shows a case where the cross section is triangular, Figure 2 shows a case where the cross section is trapezoidal, and Figure C
The figure shows the same d when the inner slope of the triangular cross section is curved.
The figure shows, for example, a case where the corners of a trapezoidal cross section are chamfered to create a curved surface structure.
第3図に示すNMR−CT用磁気回路は、一端に磁極片
(2)を固着した継鉄(3)の一対を対向配置して空隙
(4)を形成し、他端をFe−B−R系永久磁石(1)
で結合した回路であり、磁極片(2)の対向面周縁に断
面三角形の環状突起(5)を設番ノだ構成である。In the magnetic circuit for NMR-CT shown in FIG. 3, a pair of yokes (3) with a magnetic pole piece (2) fixed to one end are arranged facing each other to form a gap (4), and the other end is made of Fe-B- R-based permanent magnet (1)
It is a circuit in which an annular protrusion (5) with a triangular cross section is provided on the periphery of the opposing surface of the magnetic pole piece (2).
また、磁気回路も上記の例に限定されるものでなく、環
状突起を対向面に段Gノだ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、環状突起の形状寸
法も、永久磁石の寸法、磁気特性、空隙の大きさにより
適宜選定すればよいが、特に下記範囲内が有効である。Furthermore, the magnetic circuit is not limited to the above example, and can be applied to any magnetic circuit as long as the annular protrusion is configured to have a stepped G-node magnetic pole piece on the opposing surface, and the shape and dimensions of the annular protrusion are It may be appropriately selected depending on the dimensions of the permanent magnet, magnetic properties, and size of the air gap, but it is particularly effective within the following range.
D2≧1/2・Dl、 H≦1/4・LQただし、DI
;磁極片外径、D2:環状突起内径、LQ;空隙、H
;環状突起の高さ。D2≧1/2・Dl, H≦1/4・LQ However, DI
; External diameter of magnetic pole piece, D2: Inner diameter of annular protrusion, LQ: Air gap, H
; Height of the annular process.
ちなみに、第1図に示した構成の磁気回路に、常温間の
(Bl−1)maxが30MGOeを示すFe B−1
<系永久磁石を用い、DI= 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50
0mmの磁極片を配置した場合のいずれも、LGを35
0mmに保持させた空隙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, in the magnetic circuit having the configuration shown in FIG.
<Using permanent magnet, DI=500mm, D2=
400 mm, H = 30 mm with a magnetic pole piece with an annular protrusion and an outer diameter of 50 mm without an annular protrusion.
In both cases when 0mm pole piece is placed, LG is 35
When we measured the magnetic field distribution in the air gap maintained at 0 mm, we found that in the case of this invention having an annular protrusion, compared to the comparative example,
The volume of the 10-3 region of uniform magnetic field was 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っと小径の磁
極片並びに磁石でよく、小型軽量化に有利であった。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 may have a much smaller diameter than those of the above-mentioned comparative example, which is advantageous in reducing the size and weight.
第1図と第3図は、この発明による磁界発生装置の縦1
17i説明図であり、第2図は磁極片の縦Vji説明図
である。
1・・・Fe−B I<系永久磁石、2・・・磁極片、
3・・・継鉄、4・・・空隙、5・・・環状突起。
出願人 住友特殊金属株式会召
代理人 押 目コ 良 久け一]II
第1図
第2図
(Q) (b)
(c) (d)
第3図FIG. 1 and FIG. 3 show the longitudinal direction of the magnetic field generating device according to the present invention.
17i is an explanatory diagram, and FIG. 2 is an explanatory diagram of the vertical Vji of the magnetic pole piece. 1...Fe-B I< system permanent magnet, 2... Magnetic pole piece,
3...Yoke, 4...Gap, 5...Annular protrusion. Applicant Sumitomo Special Metals Co., Ltd. Representative Ryo Hisakeichi] II Figure 1 Figure 2 (Q) (b) (c) (d) Figure 3
Claims (1)
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
け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。1. In a magnetic field generating device that magnetically couples magnetic pole pieces facing each other with an air gap and at least one permanent magnet using a yoke to avoid generating a magnetic field in the air gap, an annular projection is provided on each of the opposing surfaces of the magnetic pole pieces. A magnetic field generating device characterized in that:
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 true JPS6088407A (en) | 1985-05-18 |
JPH0223010B2 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 (4)
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 |
EP0479514A1 (en) | 1990-09-29 | 1992-04-08 | Sumitomo Special Metals Co., Ltd. | Magnetic field generating device used for MRI |
US20180342339A1 (en) * | 2017-05-23 | 2018-11-29 | AOSense, Inc. | Magnetic field generators based on high magnetic permeability materials |
Families Citing this family (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPH0831635A (en) | 1994-07-08 | 1996-02-02 | Sumitomo Special Metals Co Ltd | Mri magnetic field generating device |
-
1983
- 1983-10-19 JP JP58196785A patent/JPS6088407A/en active Granted
Cited By (5)
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 |
EP0479514A1 (en) | 1990-09-29 | 1992-04-08 | Sumitomo Special Metals Co., Ltd. | Magnetic field generating device used for MRI |
US20180342339A1 (en) * | 2017-05-23 | 2018-11-29 | AOSense, Inc. | Magnetic field generators based on high magnetic permeability materials |
US10446307B2 (en) * | 2017-05-23 | 2019-10-15 | AOSense, Inc. | Magnetic field generators based on high magnetic permeability materials |
Also Published As
Publication number | Publication date |
---|---|
JPH0223010B2 (en) | 1990-05-22 |
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