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JPH073802B2 - Magnetic resonance device - Google Patents
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JPH073802B2 - Magnetic resonance device - Google Patents

Magnetic resonance device

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Publication number
JPH073802B2
JPH073802B2 JP61269150A JP26915086A JPH073802B2 JP H073802 B2 JPH073802 B2 JP H073802B2 JP 61269150 A JP61269150 A JP 61269150A JP 26915086 A JP26915086 A JP 26915086A JP H073802 B2 JPH073802 B2 JP H073802B2
Authority
JP
Japan
Prior art keywords
magnetic
permanent magnet
magnetic field
yoke
air gap
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
JP61269150A
Other languages
Japanese (ja)
Other versions
JPS63122204A (en
Inventor
武夫 金子
宏美 河本
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.)
Toshiba Corp
Original Assignee
Toshiba Corp
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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP61269150A priority Critical patent/JPH073802B2/en
Publication of JPS63122204A publication Critical patent/JPS63122204A/en
Publication of JPH073802B2 publication Critical patent/JPH073802B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は、永久磁石(permanent magnet)方式の磁気共
鳴装置に関する。
DETAILED DESCRIPTION OF THE INVENTION Object of the Invention (Field of Industrial Application) The present invention relates to a permanent magnet type magnetic resonance apparatus.

(従来の技術) 磁気共鳴装置は被検体の所望部位に一様な静磁場を印加
し、この静磁場と直角方向にRF磁場を形成する送信用RF
コイルによって断層像を得る特定のスライス部分のみに
磁気共鳴を生じさせ、さらにRF磁場の解除後に原紙核か
ら発生する磁場共鳴信号(以下MR信号と称する)を受信
用RFコイルによって検出するようにしたものである。さ
らに静磁場に体して直線的な傾斜を有する線形磁場勾配
を作用させて合成MR信号を得、この信号をフーリエ変換
することによりスライス部分のMR像を形成することが行
われる。
(Prior Art) A magnetic resonance apparatus applies a uniform static magnetic field to a desired site of a subject and forms an RF magnetic field in a direction perpendicular to the static magnetic field for transmission.
A magnetic resonance is generated only in a specific slice part where a tomographic image is obtained by the coil, and a magnetic field resonance signal (hereinafter referred to as MR signal) generated from the core of the original paper after the RF magnetic field is released is detected by the receiving RF coil. It is a thing. Further, a linear magnetic field gradient having a linear gradient is applied to the static magnetic field to obtain a composite MR signal, and the MR image of the slice portion is formed by Fourier transforming this signal.

上述した静磁場を形成する方式として、常伝導方式と超
伝導方式とが知られている。この両方式はいずれもコイ
ルに電流を流して静磁場を形成するものである。一方、
永久磁石を使用して静磁場を形成させるいわゆる永久磁
石方式も近年その経済性から脚光を浴びてきている。
As a method of forming the above-mentioned static magnetic field, a normal conduction method and a superconduction method are known. In both of these methods, a static magnetic field is formed by passing a current through the coil. on the other hand,
A so-called permanent magnet system that uses a permanent magnet to form a static magnetic field has recently been in the limelight due to its economical efficiency.

そして、磁界をかける方向として体軸(水平)磁場方式
と垂直磁場方式とがあることも知られている。
It is also known that there are a body axis (horizontal) magnetic field method and a vertical magnetic field method as a direction in which a magnetic field is applied.

ところで、上記永久磁石方式は第6図に示すようにほぼ
四角形状の純鉄からなるヨーク1と、このヨーク1の図
示上下方向のほぼ中央部分に取り付けられた永久磁石2
と、この永久磁石2の他面側には磁極3が取り付けられ
た構成となっている。
By the way, in the permanent magnet system, as shown in FIG. 6, a yoke 1 made of pure iron and having a substantially rectangular shape, and a permanent magnet 2 attached to a substantially central portion of the yoke 1 in the vertical direction in the drawing.
The magnetic pole 3 is attached to the other surface of the permanent magnet 2.

このような構成からなる従来装置では、ヨーク1に固定
されている永久磁石2の図示側面あるいは磁極3側面部
分から、永久磁石周囲に配置されたヨーク部材に漏れ磁
束Qが発生していた。
In the conventional device having such a configuration, the leakage magnetic flux Q is generated from the side surface of the permanent magnet 2 fixed to the yoke 1 in the drawing or the side surface of the magnetic pole 3 to the yoke member arranged around the permanent magnet.

(発明が解決しようとする問題点) 上述したように従来装置においては、ヨーク1に固定さ
れている永久磁石2図示側面あるいは磁極3図示側面部
分から、永久磁石の周囲に配置されたヨーク部材に漏れ
磁束が発生していた。即ち、発生される磁界は永久磁石
の強度により定まる。図中では上側の永久磁石から磁束
はエアギャップ4を通り下側の永久磁石に入り、ヨーク
1を通過して上側の永久磁石に戻る。しかしながら、漏
れ磁束のためにすべての磁束がこのような経路を経な
い。
(Problems to be Solved by the Invention) As described above, in the conventional device, the side surface of the permanent magnet 2 shown in the drawing or the side surface of the magnetic pole 3 shown in the figure is fixed to the yoke member arranged around the permanent magnet. Leakage magnetic flux was generated. That is, the magnetic field generated is determined by the strength of the permanent magnet. In the figure, the magnetic flux from the upper permanent magnet enters the lower permanent magnet through the air gap 4, passes through the yoke 1, and returns to the upper permanent magnet. However, due to leakage flux, all flux does not go through such a path.

磁界が磁性体内は通過し易く非磁性体は通過しにくいと
いう性質を有するために上記エアギャップ4より近距離
部分に多くの磁界が発生する結果となり、これが上記漏
れ磁束となる。この結果永久磁石の有する磁界強度のほ
ぼ30(%)乃至40(%)程度しか有効に作用しない。更
に、エアギャップ部分に必要磁界強度を得るためには永
久磁石の量を増加する必要を生じ、上記必要磁界強度を
得るには永久磁石の量をほぼ1.6乃至1.7倍の永久磁石に
しなければならいという問題がある。
Since the magnetic field has the property of easily passing through the magnetic body and hardly passing through the non-magnetic body, a large amount of magnetic field is generated in the portion closer to the air gap 4, and this becomes the leakage magnetic flux. As a result, only about 30 (%) to 40 (%) of the magnetic field strength of the permanent magnet works effectively. Furthermore, in order to obtain the required magnetic field strength in the air gap part, it is necessary to increase the amount of permanent magnets, and in order to obtain the above required magnetic field strength, the amount of permanent magnets must be approximately 1.6 to 1.7 times that of the permanent magnets. There is a problem.

[発明の構成] (問題点を解決するための手段) 上記問題点を解決するための本発明の構成は、閉磁路を
形成するヨークに取り付けられるとともにエアギャップ
を有して対向配置された1対の少なくとも永久磁石を具
備した静磁場発生手段を備え、該エアギャップ内に形成
される静磁場中に被検体を載置し磁気共鳴現象を利用し
て被検体断面の情報を得る磁気共鳴装置において、少な
くとも上記永久磁石の側面に非磁性体からなる磁気遮蔽
部材を設けたことを特徴としている。
[Structure of the Invention] (Means for Solving the Problems) According to the structure of the present invention for solving the above problems, the structure is attached to a yoke forming a closed magnetic circuit and is arranged to face each other with an air gap. A magnetic resonance apparatus including a static magnetic field generating means including at least a pair of permanent magnets, and placing the test object in a static magnetic field formed in the air gap to obtain information on the cross section of the test object by utilizing a magnetic resonance phenomenon. In the above, at least a side surface of the permanent magnet is provided with a magnetic shielding member made of a non-magnetic material.

(作用) 上記構成を有する本発明の作用は、ヨークに固定された
例えば永久磁石と磁極とからなる静磁場発生手段のヨー
ク部材の両側に凹部を形成するとともに、上記静磁場発
生手段のうち少なくとも永久磁石の側面に非磁性体から
なる磁気遮蔽部材を設けて該側面からの漏れ磁束の磁束
経路を大きくし、漏れ磁束の減少を図るとともに、対向
して配置された静磁場配置手段間のエアギャップでの磁
界強度を増加せしめている。
(Operation) The operation of the present invention having the above-described configuration is to form recesses on both sides of the yoke member of the static magnetic field generating means fixed to the yoke, which consists of, for example, permanent magnets and magnetic poles, and at least the static magnetic field generating means. A magnetic shielding member made of a non-magnetic material is provided on the side surface of the permanent magnet to increase the magnetic flux path of the leakage magnetic flux from the side surface to reduce the leakage magnetic flux, and the air between the static magnetic field arranging means arranged opposite to each other. The magnetic field strength in the gap is increased.

(実施例) 以下本発明の一実施例装置について図面を参照しながら
説明する。
(Embodiment) An embodiment of the present invention will be described below with reference to the drawings.

第1図は本発明装置の一実施例装置の正面図である。FIG. 1 is a front view of an embodiment of the device of the present invention.

同図に示す一実施例装置は、ほぼ四角形状からなる例え
ば純鉄から形成されたヨーク5と、このヨーク5の図示
上下のヨーク部材の中央部分にそれぞれ対向配置されて
固定される静磁場発生手段9とを有するとともに、この
磁界発生手段9が取り付けられたヨーク部材であって該
磁界発生手段9の取付支持面には凹部5a,5aを形成した
構成となっている。尚、本実施例ではヨーク部材と静磁
場発生手段9を構成する少なくとも永久磁石(後述す
る)との固定は非磁性体からなる磁気遮蔽部材15により
挾持することにより行っている。
The apparatus of the embodiment shown in FIG. 1 includes a yoke 5 formed of, for example, pure iron and having a substantially quadrangular shape, and a static magnetic field generation that is fixed by being opposed to central portions of upper and lower yoke members of the yoke 5 in the figure. And a concave member 5a, 5a is formed on the mounting support surface of the magnetic field generating means 9 in which the magnetic field generating means 9 is mounted. In this embodiment, the yoke member and at least the permanent magnet (described later) forming the static magnetic field generating means 9 are fixed by being held by the magnetic shielding member 15 made of a non-magnetic material.

即ち、第2図に示すように静磁場発生手段9を構成する
複数からなる永久磁石7を同図に示すように配列した後
に、15で示す非磁性体例えばニッケル鋼,マンガン鋼,1
8−8ステンレス鋼等の帯状部材をリング状とした磁気
遮蔽部材15により、上記のように一列に配列した永久磁
石7の側面方向から全体として挾持固定するようにす
る。この時、第1図に示す永久磁石7を固定するヨーク
部材先端部分(凹部5a,5aに挟まれた部分)を上記磁気
遮蔽部材15の側部15aにより同時に挾持固定している。
そして、以上のように固定された永久磁石7のエアーギ
ャップ8に面する側に磁極を例えば導電性の接着剤等の
他適宜方法によって固定する。
That is, as shown in FIG. 2, after arranging a plurality of permanent magnets 7 constituting the static magnetic field generating means 9 as shown in FIG. 2, a non-magnetic material such as nickel steel, manganese steel, 1
The band-shaped member made of 8-8 stainless steel or the like is clamped and fixed as a whole from the side surface direction of the permanent magnets 7 arranged in a line as described above by the ring-shaped magnetic shielding member 15. At this time, the tip portion of the yoke member (the portion sandwiched between the recesses 5a, 5a) for fixing the permanent magnet 7 shown in FIG. 1 is simultaneously held and fixed by the side portion 15a of the magnetic shield member 15.
Then, the magnetic pole is fixed to the side of the permanent magnet 7 fixed as described above facing the air gap 8 by an appropriate method such as a conductive adhesive.

そして、以上のように構成された本装置の外観は第3図
に示すようになっている。尚、第3図中Pで示すものは
エアーギャップ8部分に挿入載置される被検体である。
The appearance of the present apparatus configured as described above is as shown in FIG. In addition, what is shown by P in FIG. 3 is a subject to be inserted and placed in the air gap 8 portion.

上記静磁場発生手段9は、第1図に示すように例えばBa
フェライト等の永久磁石7と、この永久磁石7で発生す
る磁界を均一なものにする磁性体からなる磁極6から構
成されている。尚、磁極6は永久磁石7により発生する
磁界をエアーギャップ8において均一にするもので、こ
のために磁極6のエアーギャップ8に面する部分の形状
は図示緩かな凹部を設けた形状としている。尚、その形
状は同図に示すような緩かな凹部を形成させたものに限
定されず、例えば適当な曲率を有する曲面を該磁極に形
成するようにしてもよい(第4図参照)。
The static magnetic field generating means 9 is, for example, as shown in FIG.
It is composed of a permanent magnet 7 such as ferrite, and a magnetic pole 6 made of a magnetic material that makes the magnetic field generated by the permanent magnet 7 uniform. The magnetic pole 6 is to make the magnetic field generated by the permanent magnet 7 uniform in the air gap 8. For this reason, the shape of the portion of the magnetic pole 6 facing the air gap 8 is a shape provided with a gentle concave portion in the drawing. The shape of the magnetic pole is not limited to that having a gentle recess as shown in the figure, and a curved surface having an appropriate curvature may be formed on the magnetic pole (see FIG. 4).

次に前記ヨーク5には前述したように静磁場発生手段9
が取り付けられたヨーク部材の取付支持面に、凹部5a,5
aが形成されている。
Next, the yoke 5 has the static magnetic field generating means 9 as described above.
On the mounting support surface of the yoke member to which the
a is formed.

即ち、上記凹部5a,5aはその形状を半円形状としたもの
であり、永久磁石7の図示両側面と、この両側面と対向
するヨーク部材との距離をRとすると、本実施例では上
記半円の半径をR/2としている。このようにして永久磁
石7と近傍のヨーク部材との距離を大きくしている。
That is, the recesses 5a, 5a have a semicircular shape, and if the distance between the both side surfaces of the permanent magnet 7 in the figure and the yoke member facing the both side surfaces is R, then in the present embodiment, The radius of the semicircle is R / 2. In this way, the distance between the permanent magnet 7 and the adjacent yoke member is increased.

第4図は本発明装置の一変形例を示す正面図である。FIG. 4 is a front view showing a modification of the device of the present invention.

第1図に示す凹部は半円形状をしたものを例示したが、
例えば同図に示すように静磁場発生手段9を取付けたヨ
ーク部材の取付支持面にほぼU字状の凹部を設けてもよ
い。尚、同図中第1図と同様の部材には同一の符号を付
して説明を省略する。
The concave portion shown in FIG. 1 has a semicircular shape, but
For example, as shown in the figure, a substantially U-shaped recess may be provided on the mounting support surface of the yoke member to which the static magnetic field generating means 9 is mounted. The same members as those in FIG. 1 are designated by the same reference numerals in FIG.

以上のように構成された本発明装置の作用、効果につい
て第1図及び第5図を参照して説明する。
The operation and effect of the device of the present invention configured as described above will be described with reference to FIGS. 1 and 5.

第1図において図示上側の永久磁石7から出た磁界は磁
極6,エアーギャップ8を通過して、対向して配置された
磁極6、永久磁石7を通過してヨーク5に入り、再び永
久磁石5aに戻る。このとき、本実施例装置では該永久磁
石7の側面には非磁性体からなる磁気遮蔽部材15が、こ
の永久磁石7を包囲するように存在するので、該側面か
ら近傍のヨーク部材への漏れ磁束をいわば迂回させると
いう機能を有する。従って、永久磁石7側面からの漏れ
磁束の減少をさせることができるようにしている。尚、
同図には永久磁石の側面だけに磁気遮蔽部材を設けた例
を示すが、これを磁極側面まで延長して設けてもよい。
このようにした場合にはさらに漏れ磁束の減少を図るこ
とができるとともに、ヨーク部材,永久磁石,磁極の三
者を同一の磁気遮蔽部材により同時に挾持固定できるの
で製造工程の簡略化を図ることができる。
In FIG. 1, the magnetic field emitted from the permanent magnet 7 on the upper side of the drawing passes through the magnetic pole 6 and the air gap 8, passes through the magnetic pole 6 and the permanent magnet 7 which are arranged to face each other, and enters the yoke 5, and again the permanent magnet. Return to 5a. At this time, in the apparatus of this embodiment, since the magnetic shield member 15 made of a non-magnetic material is present on the side surface of the permanent magnet 7 so as to surround the permanent magnet 7, leakage from the side surface to the adjacent yoke member is prevented. It has the function of diverting the magnetic flux. Therefore, the leakage flux from the side surface of the permanent magnet 7 can be reduced. still,
Although the figure shows an example in which the magnetic shield member is provided only on the side surface of the permanent magnet, it may be provided by extending it to the side surface of the magnetic pole.
In such a case, the leakage flux can be further reduced, and the yoke member, the permanent magnet, and the magnetic pole can be simultaneously clamped and fixed by the same magnetic shield member, so that the manufacturing process can be simplified. it can.

さらに、ヨーク部材の静磁場発生手段の取付支持面に凹
部を形成しているので、該静磁場発生手段を構成する永
久磁石と周囲のヨーク部材との距離を増大させ、従来こ
の部分に発生していた漏れ磁束の減少を図っている。即
ち、第5図に示すように永久磁石7の例えば右側面から
の漏れ磁束は、従来図示点線で示す位置にヨーク部材が
ある場合には、A,B点で磁束が交わっていた。一方、本
発明ではこの部分には凹部を形成させているので、上記
A,B点に交わっていた磁束はそれぞれC,D点に移動するこ
とになる。即ち、磁束経路が大きくなるので磁気抵抗が
増大し、従来この部分を通過していた磁束はエアーギャ
ップ8を通過するようになる。従って、漏れ磁束つまり
磁界損失が減少するとともにエアーギャップ8を通過す
る有効磁界が増加するようになる。このことから、必要
とする有効磁界を得る際の永久磁石の量を低減させるこ
とができる。
Further, since the concave portion is formed on the mounting support surface of the static magnetic field generating means of the yoke member, the distance between the permanent magnets constituting the static magnetic field generating means and the surrounding yoke member is increased, and this is conventionally generated in this portion. We are trying to reduce the leakage flux. That is, as shown in FIG. 5, the leakage magnetic flux from, for example, the right side surface of the permanent magnet 7 intersects at the points A and B when the yoke member is located at the position indicated by the dotted line in the related art. On the other hand, in the present invention, since the concave portion is formed in this portion,
The magnetic flux intersecting at points A and B will move to points C and D, respectively. That is, since the magnetic flux path becomes large, the magnetic resistance increases, and the magnetic flux that has conventionally passed through this portion now passes through the air gap 8. Therefore, the leakage magnetic flux, that is, the magnetic field loss decreases, and the effective magnetic field passing through the air gap 8 increases. From this, it is possible to reduce the amount of permanent magnets when obtaining the required effective magnetic field.

さらに良好な結果を得るには磁極間のエアーギャップ8
の距離を短距離にするとよい。
Air gap 8 between magnetic poles for better results
It is good to shorten the distance of.

尚、本発明は上記図示された実施例に限定されず、本発
明の要旨の範囲内で様々に変形実施が可能であることを
付記する。
It should be noted that the present invention is not limited to the above-described embodiments, and various modifications can be made within the scope of the gist of the present invention.

[発明の効果] 以上詳述したように本発明装置によると、漏れ磁束の減
少を図ることができる磁気共鳴装置の提供ができる。
[Advantages of the Invention] As described in detail above, according to the device of the present invention, it is possible to provide a magnetic resonance device capable of reducing leakage flux.

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

第1図は本発明の一実施例装置の正面図、第2図は磁気
遮蔽部材により永久磁石を固定する状態を示す説明図、
第3図は第1図に示す装置の外観斜視図、第4図はヨー
ク部材に形成される凹部の一変形例の正面図、第5図は
永久磁石の側面から近傍のヨーク部材への漏れ磁束の説
明図、第6図は従来の磁気共鳴装置の正面図である。 5…ヨーク、6…磁極、7…永久磁石、8…エアーギャ
ップ、9(6,7)…静磁場発生手段、15…磁気遮蔽部
材。
FIG. 1 is a front view of an apparatus according to an embodiment of the present invention, and FIG. 2 is an explanatory view showing a state in which a permanent magnet is fixed by a magnetic shield member,
FIG. 3 is an external perspective view of the device shown in FIG. 1, FIG. 4 is a front view of a modified example of a recess formed in a yoke member, and FIG. 5 is a side view of a permanent magnet leaking to a nearby yoke member. FIG. 6 is an explanatory view of magnetic flux, and is a front view of a conventional magnetic resonance apparatus. 5 ... Yoke, 6 ... Magnetic pole, 7 ... Permanent magnet, 8 ... Air gap, 9 (6, 7) ... Static magnetic field generating means, 15 ... Magnetic shielding member.

Claims (2)

【特許請求の範囲】[Claims] 【請求項1】閉磁路を形成するヨークに取り付けられる
とともにエアギャップを有して対向配置された1対の少
なくとも永久磁石を具備した静磁場発生手段を備え、該
エアギャップ内に形成される静磁場中に被検体を載置し
磁気共鳴現象を利用して被検体断面の情報を得る磁気共
鳴装置において、少なくとも上記永久磁石の側面に非磁
性体からなる磁気遮蔽部材を設けたことを特徴とする磁
気共鳴装置。
1. A static magnetic field generating means, which is attached to a yoke forming a closed magnetic path and has a pair of at least permanent magnets facing each other with an air gap, and including a static magnetic field formed in the air gap. In a magnetic resonance apparatus for placing a subject in a magnetic field and obtaining information of a cross section of the subject by using a magnetic resonance phenomenon, at least a side surface of the permanent magnet is provided with a magnetic shield member made of a non-magnetic material. Magnetic resonance device.
【請求項2】前記ヨークは永久磁石の取付面側であって
該永久磁石の取付支持面に凹部を形成したものである特
許請求の範囲第1項記載の磁気共鳴装置。
2. The magnetic resonance apparatus according to claim 1, wherein the yoke is a mounting surface side of the permanent magnet and a recess is formed in a mounting support surface of the permanent magnet.
JP61269150A 1986-11-12 1986-11-12 Magnetic resonance device Expired - Lifetime JPH073802B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61269150A JPH073802B2 (en) 1986-11-12 1986-11-12 Magnetic resonance device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61269150A JPH073802B2 (en) 1986-11-12 1986-11-12 Magnetic resonance device

Publications (2)

Publication Number Publication Date
JPS63122204A JPS63122204A (en) 1988-05-26
JPH073802B2 true JPH073802B2 (en) 1995-01-18

Family

ID=17468372

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61269150A Expired - Lifetime JPH073802B2 (en) 1986-11-12 1986-11-12 Magnetic resonance device

Country Status (1)

Country Link
JP (1) JPH073802B2 (en)

Also Published As

Publication number Publication date
JPS63122204A (en) 1988-05-26

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