JPS60183706A - Equipment for generating magnetic field - Google Patents

Equipment for generating magnetic field

Info

Publication number
JPS60183706A
JPS60183706A JP59039962A JP3996284A JPS60183706A JP S60183706 A JPS60183706 A JP S60183706A JP 59039962 A JP59039962 A JP 59039962A JP 3996284 A JP3996284 A JP 3996284A JP S60183706 A JPS60183706 A JP S60183706A
Authority
JP
Japan
Prior art keywords
permanent magnet
magnetic field
magnetic
max
center
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.)
Pending
Application number
JP59039962A
Other languages
Japanese (ja)
Inventor
Shinichi Hayashi
真一 林
Hirobumi Takabayashi
博文 高林
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 JP59039962A priority Critical patent/JPS60183706A/en
Publication of JPS60183706A publication Critical patent/JPS60183706A/en
Pending 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

Abstract

PURPOSE:To obtain an equipment which has a magnetic circuit of enabling high accuracy, uniform and stable magnetic field by making each face of a magnetic pole piece a recessed and curved surface and making adjacent to the center of a permanent magnet having specific (BH) max. CONSTITUTION:Magnetic pole pieces 2 facing each other are each made a recessed and curved surface 5 and adjacent to the center of a permanent magnet 1 is made a permanent magnet 1b having 10MGOe or more less (BH) max. than the (BH) max. of the surrounding permanent magnet 1a. For example, in the case of a magnetic circuit used in an NMR-CT equipment, in the bore of a ring Fe-B-R permanent magnet 1a of external diameter D and internal diameter (d), a disk type Sr ferrite magnet 1b of external diameter (d) is inserted and fixed. At one end of the permanent magnet 1 integrated with 1a and 1b, magnetic pole pieces 2 is fixed facing each other and the other ends are connected with a yoke 3. In a void 4 between the pole pieces 2, strong magnetic field of 1-10kg is generated to diagnose part or the whole of a human body placed in the void.

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冑で組織の性質よ
P 1?rさ出りことのできる医療用核磁気j4鳴断層
装置(以下、N M R−CI−という)等に用いられ
る人ぎ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 is a method to obtain a cross-sectional image of an object based on the properties of the tissue. This invention relates to a magnetic field generating device that generates a strong, highly accurate, and uniform magnetic field in a narrow air gap, which is used in medical nuclear magnetic j4 sound tomography devices (hereinafter referred to as NMR-CI-) that can be exposed to the outside. .

N M R−CTは、人体の一部または全部を1〜1.
5K 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、この磁界が強ツノかつ10
−4以下の精度で一様で安定していることが要求され、
NMI”10丁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心線を円筒状に巻ねした常伝導磁石
あるい[よ、特殊な導線を用い、絶対零度イ」近の温度
に冷却して使用づる超伝導磁石が知られている。
NMR-CT examines part or all of the human body in 1 to 1.
In order to obtain the required tomographic image by inserting it into the air gap that forms a strong magnetic field of 5 KG, this magnetic field has a strong horn and a
It is required to be uniform and stable with an accuracy of -4 or less,
The magnetic field generator for 10 NMI's uses a normal conducting magnet with a core wire made of copper or aluminum wound into a cylindrical shape, or a special conducting wire cooled to a temperature close to absolute zero. Superconducting magnets are known for use in

前者は構造上安価であるが十分な強ツノ磁界を発生ざぜ
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」ストが高く、」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 horn magnetic field, it requires a huge amount of electricity and cooling water, and the running stress is high, and the leakage magnetic field created by the horn may be harmful depending on the application. On the other hand, the latter type of superconducting magnet has the advantage of consuming less power and being able to generate a strong magnetic field in a small size, but it requires the use of expensive liquid helium etc. as a coolant. However, there is a problem that the initial cost and running cost are extremely high, so it has not been widely used.

本出願人は、先に、磁界強麿が上記の常電711石と同
等以上で電力の消費もなく、漏洩磁界の少ない永久磁石
回路として、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6ど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J3いて、上記磁4’k 
)’+−の対向面の各々を凹状湾曲面とした磁界発生装
置を提案した(特駈1昭58−196787> )。し
かし、空隙に発生りる磁界は中心部イ・」近では最高値
が行られるが、中心部より遠ざかるにつれて、周辺部空
隙では磁界の強さが低下し、極め−C高精度で均一かつ
安定な磁界を賀ることができなかった。
The present applicant has previously developed a permanent magnet circuit with a magnetic field intensity equal to or higher than the above-mentioned regular electric current 711 magnets, no power consumption, and a small leakage magnetic field, with magnetic pole pieces facing each other with an air gap formed therein, and at least one The magnetic field generator J3 magnetically couples the permanent magnets 6 and the like with a yoke to generate a magnetic field in the air gap.
) proposed a magnetic field generating device in which each of the opposing surfaces of + and - was a concave curved surface. However, the magnetic field generated in the air gap has its highest value near the center, but as it moves away from the center, the strength of the magnetic field decreases in the peripheral air gap, making it uniform and stable with extremely high precision. It was not possible to withstand strong magnetic fields.

この発明は、かかる現状に鑑み、強ツノな磁界が得られ
る永久磁石を使用した磁界発生装置の空隙にiJ′3い
て、高精度で均一かつ安定な磁界が1′ノられる磁気回
路を右づる磁界発生装置を目的としている。
In view of the current situation, the present invention proposes a magnetic circuit that can generate a highly accurate, uniform, and stable magnetic field by placing it in the air gap of a magnetic field generator using permanent magnets that can generate a strong horned magnetic field. It is intended as a magnetic field generator.

すなわら、この発明は、空隙を形成して対向りる磁極片
と、少なくとも1の永久磁石とを粗鉱で磁気的結合し該
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を凹状湾曲面どし、かつ永久磁石の
中心部付近をその周辺部の永久磁石が右する( B )
−1) maxよりIOMGOQ以上小さな(BHンm
axを右ケる永久+41石としたことを14徴とりる磁
界発生装置である。
In other words, the present invention provides 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 coarse ore to avoid generating a magnetic field in the air gap. Each of the opposing surfaces is a concave curved surface, and the permanent magnet in the peripheral part is right in the vicinity of the center of the permanent magnet (B)
-1) IOMGOQ smaller than max (BH n m
It is a magnetic field generating device that has 14 characteristics, with the ax being a permanent +41 stone.

この発明の磁界発生装置においC,極めて高れ゛」度−
(均一かつ安定な空隙磁界をr!るため、永久磁石の中
心部トJ近の(B H) maxを、イの周辺部の永久
磁イ」の([3H> maxより小さくりるが、la 
(4j片中心部の(B l−1) maxが10M G
 Oeを越え、周辺部イ」近の(1311)maxが2
0MGOe末)91で、両者の差が10MGOθ未満で
は、広範囲で均一な空隙磁界が1.7られないため、少
なくとも中心部角近どその周辺部どの(B l−1) 
max差を10MGOe以上とするのが好ましく、該中
心部イー」近の永久磁石の([3+−1)maxが10
〜+GOθ以下、中心部の外周囲の永久磁石の(F31
1)maxが20MGOe以上であることが望ましい。
In the magnetic field generator of this invention, the degree of C is extremely high.
(In order to create a uniform and stable air-gap magnetic field, (B H) max near the center of the permanent magnet J is smaller than ([3H> la
((B l-1) max at the center of 4j piece is 10M G
Beyond Oe, the peripheral part A' (1311) max is 2
If the difference between the two is less than 10 MGO θ, a uniform air gap magnetic field cannot be obtained over a wide range.
It is preferable that the max difference is 10MGOe or more, and the ([3+-1)max of the permanent magnet near the center E' is 10
~+GOθ or less, the permanent magnet around the center (F31
1) It is desirable that max is 20 MGOe or more.

この発明の磁界発生装置に用いる永久磁石は、フエライ
1〜磁Tjsノフルニコ系磁石、希土類コバル1〜系磁
石/J<使用c′きるが、先に出願人か提案した、高1
IIIなSmやGを含有しない新しい高性能永久磁石と
してFe−B−R系(RはYを含む希土類元素のうら少
なくとも1種)永久磁石(特願昭57−1450728
)は、イの最大エネルギー積が大きいた()でなく、残
留磁束密磨(Br)の温度係数が、0.07%/”C〜
0.15%/℃なる温度特性を右づるため、この永久磁
石を」上記のNMR−C1−に適用することにより、装
置の小形化が達惑でき、づぐれた性能が4Jられ、さら
に、この永久磁石の磁気特性が特に0℃以下に冷2J]
 L/て使用りることにより、ab<高い最大エネルギ
ー積をが1′、Iられる性質を有効に利用できる。
The permanent magnets used in the magnetic field generating device of the present invention include Ferrai 1 ~ magnetic Tjs nofurnico type magnets, rare earth Kobal 1~ type magnets
Fe-B-R system (R is at least one rare earth element including Y) permanent magnet as a new high-performance permanent magnet that does not contain Sm or G (Japanese Patent Application No. 57-1450728)
) has a large maximum energy product, but the temperature coefficient of residual magnetic flux density (Br) is 0.07%/"C~
In order to obtain a temperature characteristic of 0.15%/℃, by applying this permanent magnet to the above-mentioned NMR-C1-, the device can be made smaller, the performance improved by 4J, and furthermore, The magnetic properties of this permanent magnet are particularly low at 2J below 0℃]
By using L/, the property that ab<high maximum energy product 1', I can be effectively utilized.

上記のFe−B−R系永久磁石は、1で(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%〜3
0原子%、B 21にi子%・〜・28+几)了%、F
e42原子%へ・90原子%を主成分とし、主相が正方
晶相からなる永久磁6′c゛あり、RとしてMやPrを
中心とする資源的に豊富な軽希土類を用(X、B、Fe
を主成分として25MGOθ以上の極め−C高いエネル
ギー積を承り、すぐれた永久磁石である。
The above Fe-B-R permanent magnet contains 1 (where R is at least one kind of rare earth elements including Y) 8 atomic % to 3
0 atomic %, B 21 i child%...28+几)了%, F
e42 atomic% - 90 atomic% is the main component, and there is a permanent magnetic 6'c゛ whose main phase is a tetragonal phase, and resource-rich light rare earths, mainly M and Pr, are used as R (X, B, Fe
It is an excellent permanent magnet that has an extremely high energy product of -C of 25MGOθ or more with its main component.

以下、この発明を図面に基づいて詳述づ−る。Hereinafter, this invention will be explained in detail based on the drawings.

第1図は、この発明によるNMR−CT装置に使用づる
磁気回路の説明図であり、外径り、内径dのリング状の
Fe −B −tり系永久磁(i(1a)の内径部に外
径dの円?Ii(型Srフェライト磁石(11))を挿
入固るし、外径りの一体となした永久磁で】(1)の各
々の一方9M;に磁極片(2)を固るして対向ざU、他
方端を継鉄(3)で結合し、磁極)’i−(2)間の空
隙(4)内に1〜10KGの強い磁界を発生ざぜ、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。一対の磁極片(2)は外径がDでその対向面の全
面が凹状湾曲面(5)を(育成しUJ5す、換言づれば
1面が平面の凹レンズ状の形状からなる磁極j1℃・′
あり、一対の凹状湾曲面(5)を空隙(4)で対向させ
ることにJ、す、高粘度で均一かつ安定した磁界が1“
lられる。
FIG. 1 is an explanatory diagram of a magnetic circuit used in the NMR-CT apparatus according to the present invention. Insert a circle Ii (type Sr ferrite magnet (11)) with an outer diameter of d into and harden it, and with a permanent magnet made of an integral piece of outer diameter, insert a magnetic pole piece (2) into one 9M of each of The opposite ends are connected by a yoke (3), and a strong magnetic field of 1 to 10 KG is generated in the gap (4) between the magnetic poles)'i and (2). It is configured to insert part or all of the human body into the body for diagnosis. A pair of magnetic pole pieces (2) have an outer diameter of D, and the entire surface of their opposing surfaces has a concave curved surface (5) (UJ5), in other words, one surface is a flat concave lens shape.
By making a pair of concave curved surfaces (5) face each other with a gap (4), a highly viscous, uniform and stable magnetic field is created.
I will be beaten.

なJ3、凹状湾曲面(5)は、曲率半径R”(−形成し
てあり、第1図中の0点は空隙(/l) (1−g)の
中心点を示し、曲率半径Rの中心点−Cある01は0点
の鉛直線上にある。
J3, the concave curved surface (5) is formed with a radius of curvature R" The center point -C, 01, is on the vertical line of the 0 point.

また、他の実施例として第2図に示りNMR−C]−用
磁気回路は、一端に磁極片(2)を固るした継’IJ、
(31(1)−%J ヲ対向配[I′へ゛して空隙(/
l)を形成し、臀ai(3)の他端を、永久磁石(1)
、すなわら、一対の継鉄(3)聞の中心部をSrフエラ
イ−1〜磁石(ill> 、外周部をFe−El−R系
永久磁石(li)で構成しIこ一体の永久磁石(1)で
結合した回路であり、磁極片(2)の対向面の全面に一
定曲率で湾曲した凹状湾曲面(5))を八わノ ノζ4
+/7 I戊 (゛ある。。
In addition, as another example, the magnetic circuit for NMR-C shown in FIG.
(31(1)-%J)
l) and the other end of the buttock ai (3) with a permanent magnet (1)
In other words, the center part of the pair of yokes (3) is composed of Sr ferrite magnets (ill>), and the outer periphery is composed of Fe-El-R permanent magnets (li), making it an integrated permanent magnet. (1), a concave curved surface (5) curved at a constant curvature is formed on the entire opposing surface of the magnetic pole piece (2).
+/7 I 戊 (゛There is..

この発明にa3い゛C,磁気回路は1−記の例(3限定
されるしの(゛なく、単一曲率半径や複数の曲率半径を
有したなだらかな曲面の凹状湾曲面を対向101に設(
ノた磁極片を配置でさる()へ成で゛あれぽいか4jる
(6気回路にも適用−C−さる、2 磁気回路の永久磁石は、中心部fJ 3Jiの永久VG
L」(D (I3 N ) maxがIOM(20e以
ト、周辺部ト1近の永久磁石)((311) max 
r、+t20M GOe以」二であることが望ましく、
口の([3t−1) may、のiテがtOM G O
e以上である2種の永久)41石の組み合わせ材質とし
ては、中心部イ1近にはj/ルニ′J磁イj、バートノ
1シイ1〜磁石、くの周辺部には希土類コバル1〜系磁
石。
In this invention, a3-C, the magnetic circuit includes the following examples (3), including but not limited to, a gently curved concave curved surface having a single radius of curvature or multiple radii of curvature, Setting (
The permanent magnet of the magnetic circuit is the permanent VG of the central part fJ 3Ji.
L'' (D (I3 N) max is IOM (20e or more, permanent magnet near the peripheral part) ((311) max
It is preferable that r, +t20M GOe 2,
Mouth ([3t-1) may,'s ite is tOM G O
As for the combination materials of 2 types of permanent) 41 stones that are more than e, there is J/Luni' J magnet near the center A1, a rare earth Kobal 1 near the center, and a rare earth Kobal 1-41 stone around the center. system magnet.

FQ −B−R系磁石が最ム好ましく、磁石\」法も、
0.6D≦d ≦ 0.9D の場合がI4シイj効て′ある、7 また、凹状湾曲面の曲率や形状用?人も、永久磁石のN
法、磁気′ls性、空隙の人ささにj、り退官選定りれ
ばJ、いが、特に);記範囲内が有効である5゜1/2
・l−’) 、”F= R:”4.4/ b・D、t1
≦3/1G・1つ !こたし、[〕:罎極J)外径、「<;曲率rF径、支
:空隙1−9の中心yj、ζ0から)での中心点○lま
での鉛直 一方向の圧端、。
FQ-BR-based magnets are most preferable, and the magnet\” method also uses
I4 is effective when 0.6D≦d≦0.9D.7 Also, for the curvature and shape of concave curved surfaces? People and permanent magnets
If you choose law, magnetism, and the size of the gap, it is important to note that the above range is valid.
・l-'), "F= R:" 4.4/ b・D, t1
≦3/1G・1! Here, []: 罎极J) Outer diameter, <; Curvature rF diameter, Support: Center yj of void 1-9, pressure end in one vertical direction from ζ0 to center point ○l.

以下に実施例を説明覆る。Examples are described below.

2′)1図[こ小した41.S成の磁気回路に、常Wl
a I!;’iの(1,3l 1 > IIIaXが3
0MGOeを承り、外径1000 m:n 、内径80
01i、lllのリング状のFe−5−R系永久磁石(
1a)の内径81Xに外径800mm T’ (131
! ) 1llaX = /IM GOeの円9aろl
’! Srフ」−ライ1ル磁石(1b)を挿入した一体
の永久(磁石(コ)を用い、l) = 1000nun
、R= 720mm、’l = 1!1onunの凹状
湾曲面を右りる磁極)1を配tζ1゛シた本発明の場合
と、永久磁石(1)に(1311) max =4MG
OeのSrフ」−ライト磁石を用いて同一構成の磁4%
 J’iを配置した比較例の場合について、いfれも、
Lgを700 mmに保持ざゼた空隙内の磁界分布を測
定したところ、第3図の磁界分布結果を49だ。
2') Figure 1 [Small 41. In the magnetic circuit of S configuration, Wl is always
a I! ;'i's (1,3l 1 > IIIaX is 3
0MGOe available, outer diameter 1000 m:n, inner diameter 80
01i, lll ring-shaped Fe-5-R permanent magnet (
1a) inner diameter 81X and outer diameter 800mm T' (131
! ) 1llaX = /IM GOe's circle 9a
'! An integrated permanent magnet (using a magnet (ko), l) with a Sr metal magnet (1b) inserted = 1000nun
, R = 720 mm, 'l = 1! The case of the present invention in which the magnetic pole) 1 is placed on the right side of the concave curved surface of
4% magnet of the same composition using Oe's Sr magnet
Regarding the case of the comparative example in which J'i is placed,
When we measured the magnetic field distribution in the gap while keeping Lg at 700 mm, the magnetic field distribution result shown in Figure 3 was 49.

なお、第3図中のイ線は本弁明の場合、口線は比較例の
場合を示J。
In addition, the A line in FIG. 3 indicates the case of the present defense, and the open line indicates the case of the comparative example.

第3図の結果から明らかなように、空隙中心点Oから半
径(r) 180mmの球状空間内において、(B I
−1) maxの責なる2種の永久磁石を配置した本発
明の場合は、比較例の均一度か0.2%であるのに対し
て、0.03%と極めて高い均一度がiilられ、磁界
が極めて高精1哀で均一かつ安定していることが分る。
As is clear from the results shown in Figure 3, in a spherical space with a radius (r) of 180 mm from the gap center point O, (B I
-1) In the case of the present invention in which two types of permanent magnets responsible for max are arranged, the uniformity is extremely high at 0.03%, compared to 0.2% in the comparative example. It can be seen that the magnetic field is extremely precise, uniform, and stable.

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

第1図と第2図は、この発明による磁界発生装置の縦断
説明Nである。第3図は実施例の磁気回路空隙にお()
る磁界分布図て゛ある。 1・・・永久磁石、1a・・・Fe−El−It系永久
磁石、111・・・Srフェライト磁石、2・・・磁極
片、3・・・継鉄、4・・・空隙、5・・・凹状湾曲。 第1図 第2図 第3図 1 (イ) 6、’j+”:I(’+n−,3、QQ’#I G特許
庁長官 名杉(1」大 殿 1、事件の表示 IIu和59イ■ 特6′F Ifl+’i 第399
625”i2、発明の名称 磁界発生装置 3、補正をJる省 jJiイ′1どの関係 出19iI人 住所 大阪市東区北浜5 ’J−[−] 22番地スミ
F〜し1−クシュ1ンンク 名称 住友特殊金属株式会社 4、代理人 ) 5、ネ11j正のλ・j象 1、明III占第1頁19行から20行の1−1−4.
!1KGJを11〜15K G Jと補正づる。 2、明細実弟7頁11行から12行の1いかなる臣へ一
回路にt)適用(゛きる。」を[いかなるilD気回路
にも適用て〜さ、51:た、さらに、i11人工ネルA
゛−積の異なる2+++の永久磁石の組み合UにJ3い
て、永久磁石に(イ日仏片をf号設しない場合し、空隙
内の磁yI強1哀の均一化に有効−C゛ある1、」ど補
止りる。
FIGS. 1 and 2 are longitudinal sectional views N of the magnetic field generating device according to the present invention. Figure 3 shows the magnetic circuit gap () of the example.
There is a magnetic field distribution map. DESCRIPTION OF SYMBOLS 1... Permanent magnet, 1a... Fe-El-It system permanent magnet, 111... Sr ferrite magnet, 2... Magnetic pole piece, 3... Yoke, 4... Air gap, 5... ...Concave curvature. Figure 1 Figure 2 Figure 3 Figure 1 (a) 6, 'j+': I ('+n-, 3, QQ'#I G Patent Office Commissioner Nasugi (1' Odono 1, Incident Display IIu W59 I ■Special 6'F Ifl+'i No. 399
625''i2, Name of the invention Magnetic field generator 3, Correction of JJI'1 Which relation: Address 22, Kitahama, Higashi-ku, Osaka-shi, J-[-] 22, SumiF~shi1-Kush1unk Name Sumitomo Special Metals Co., Ltd. 4, Agent) 5, Ne11j Positive λ・j Elephant 1, Mei III Zhan, page 1, lines 19 to 20, 1-1-4.
! Correct 1KGJ to 11-15KGJ. 2. Apply (t) apply to any subject in a circuit from line 11 to line 12 on page 7 of the specification.
If there is a combination U of 2+++ permanent magnets with different products, and the permanent magnets are not equipped with a Japanese-French piece, there is a 1,” is correct.

Claims (1)

【特許請求の範囲】[Claims] 1 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
ける磁界発生装置において、上記磁極片の対向面の各々
を凹状湾曲面とし、かつ永久磁石の中心部(=J近をそ
の周辺部の永久磁石が有づる(8H)maxJ:す10
MGOeJ、u上小さな(B1−1 ) maxを右づ
る永久46石としたことを特徴どゾる磁界発生装hjl
 a
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, each of the opposing surfaces of the magnetic pole pieces is formed into a concave curved surface. And the center of the permanent magnet (= near J is the permanent magnet at its periphery (8H) maxJ: 10
MGOeJ, small on u (B1-1) An amazing magnetic field generator hjl characterized by a permanent 46 stones with the max on the right.
a
JP59039962A 1984-03-01 1984-03-01 Equipment for generating magnetic field Pending JPS60183706A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP59039962A JPS60183706A (en) 1984-03-01 1984-03-01 Equipment for generating magnetic field

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP59039962A JPS60183706A (en) 1984-03-01 1984-03-01 Equipment for generating magnetic field

Publications (1)

Publication Number Publication Date
JPS60183706A true JPS60183706A (en) 1985-09-19

Family

ID=12567580

Family Applications (1)

Application Number Title Priority Date Filing Date
JP59039962A Pending JPS60183706A (en) 1984-03-01 1984-03-01 Equipment for generating magnetic field

Country Status (1)

Country Link
JP (1) JPS60183706A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100423775B1 (en) * 2002-02-27 2004-03-30 (주)에스시엠아이 Magnetic pole of electro magnet for forming equalized magnetic field
ITGE20090059A1 (en) * 2009-07-28 2011-01-29 Esaote Spa MRI DETECTION MACHINE

Cited By (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100423775B1 (en) * 2002-02-27 2004-03-30 (주)에스시엠아이 Magnetic pole of electro magnet for forming equalized magnetic field
ITGE20090059A1 (en) * 2009-07-28 2011-01-29 Esaote Spa MRI DETECTION MACHINE
EP2284558A1 (en) * 2009-07-28 2011-02-16 Esaote S.p.A. Magnetic resonance imaging apparatus with offset imaging volume
US8598875B2 (en) 2009-07-28 2013-12-03 Esaote S.P.A. MRI apparatus with offset imaging volume

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