JPS6365849A - Nuclear magnetic resonance imaging apparatus - Google Patents

Nuclear magnetic resonance imaging apparatus

Info

Publication number
JPS6365849A
JPS6365849A JP61207932A JP20793286A JPS6365849A JP S6365849 A JPS6365849 A JP S6365849A JP 61207932 A JP61207932 A JP 61207932A JP 20793286 A JP20793286 A JP 20793286A JP S6365849 A JPS6365849 A JP S6365849A
Authority
JP
Japan
Prior art keywords
coil
magnetic field
resonance imaging
magnetic resonance
nuclear magnetic
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
JP61207932A
Other languages
Japanese (ja)
Inventor
典子 前田
博 西村
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.)
Hitachi Healthcare Manufacturing Ltd
Original Assignee
Hitachi Medical 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 Hitachi Medical Corp filed Critical Hitachi Medical Corp
Priority to JP61207932A priority Critical patent/JPS6365849A/en
Publication of JPS6365849A publication Critical patent/JPS6365849A/en
Pending legal-status Critical Current

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  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Abstract] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔発明の利用分野〕 本発明は核磁気共鳴イメージング装置に係り。[Detailed description of the invention] [Field of application of the invention] The present invention relates to a nuclear magnetic resonance imaging apparatus.

特に被検者への圧迫感を少なくし、高画質の画像を得る
のに好適な傾斜磁場コイルを有する核磁気共鳴イメージ
ング装置に関するものである。
In particular, the present invention relates to a nuclear magnetic resonance imaging apparatus having a gradient magnetic field coil suitable for reducing pressure on a subject and obtaining high-quality images.

〔発明の背景〕[Background of the invention]

傾斜磁場コイルとして第6図に示すような矩形状のコイ
/I/10a、10’a、10b、10’bがある。核
磁気共鳴イメージング装置において質の良い画像を得る
為の傾斜磁場コイルの条件として。
As gradient magnetic field coils, rectangular coils/I/10a, 10'a, 10b, and 10'b as shown in FIG. 6 are available. As a condition for gradient magnetic field coils to obtain high quality images in nuclear magnetic resonance imaging equipment.

コイルが作る磁場の傾斜の均一度が高いことと、磁場の
傾斜が大きいという2つが上げられるが。
Two things that can be mentioned are that the gradient of the magnetic field created by the coil is highly uniform, and the gradient of the magnetic field is large.

矩形状のコイル10a、  10’a、  10b、 
 10’bの場合、上記条件を満たす為には、コイルの
大きさが大きくなる(核磁気共鳴医学研究会11iNM
R医学(基礎と臨床)、P82 )。
Rectangular coils 10a, 10'a, 10b,
In the case of 10'b, the size of the coil must be large to satisfy the above conditions (Nuclear Magnetic Resonance Medical Research Society 11iNM
R Medicine (Basic and Clinical), P82).

一方質の良い画像を得る為の静磁場の条件としては、磁
場の均一度が高いことと1強度が高いことの2つが上げ
られ、前者を満たすためにポールピースが用いられ、特
に中心部の均一度を上げるには凹状の構造をしたポール
ピースが用いられる。
On the other hand, two conditions for the static magnetic field to obtain high-quality images are high uniformity of the magnetic field and high magnetic field strength. To satisfy the former, pole pieces are used, especially in the center. To improve uniformity, a pole piece with a concave structure is used.

後者を満たす為にポールピース間の距離は短くとられる
To satisfy the latter requirement, the distance between the pole pieces is kept short.

上記により、ポールピースと矩形状のコイルを組み合わ
せると、コイルがポールピースよリチラに内側に位置す
ることになり、ポールピース間のギャップが狭くなり、
質の良い画像を得る為には。
Due to the above, when a pole piece and a rectangular coil are combined, the coil will be located further inside the pole piece, and the gap between the pole pieces will become narrower.
In order to obtain high quality images.

被検者に圧迫感を与える。あるいは圧迫感ととり除く為
にポールピース間隔を長くとると静磁場の強度が弱まり
信号対雑音比が悪くなるという問題点があったが、ポー
ルピースの凹部内に傾斜磁場コイルを配置し、被検者へ
の圧迫感を少なくするためのコイルの形状に対する考察
は従来なされていなかった。
Gives a feeling of pressure to the subject. Alternatively, if the distance between the pole pieces is increased to eliminate the feeling of pressure, the strength of the static magnetic field will weaken and the signal-to-noise ratio will deteriorate. Conventionally, no consideration has been given to the shape of the coil to reduce the feeling of pressure on the person.

〔発明の目的〕[Purpose of the invention]

本発明の目的は、核磁気共鳴イメージング装置において
、被検者への圧迫感を少なくし、画質の優れた画像が得
られる傾斜a4コイルを提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a gradient A4 coil that reduces pressure on a subject and provides images with excellent image quality in a nuclear magnetic resonance imaging apparatus.

〔発明の概要〕[Summary of the invention]

核磁気共鳴イメージフグ装置では画像作成上スライシン
グあるいは保の位江決めの為に傾斜磁場を利用している
。#i斜m場のつくり方は基本的に静磁場に鉛直(Z軸
)方向と水平(X、Y軸)方向の2つに分かれるので、
各々につき簡単々原理を以下に記す。前者の場合、第4
図(a)に示すように円形コイルを2つ対向させ、逆向
きの電流を流すことにより、第4図(′b)に示すよう
なZ軸方向の傾斜磁場を発生させている。又後者の場合
、2つのへルムホルツコイル8a、8bを第3図に示す
ように配置し、コイルに流す電流の向きをa、  b互
いに逆向きにすると、第3図に示すように、Xあるいは
Y軸方向の傾斜磁場が生じる。今はへルムホルツコイル
をとり上げたが、一般的に円環でなくても閉ループであ
れば傾斜磁場が生じる。
Nuclear magnetic resonance image puffer fish equipment uses gradient magnetic fields for slicing and positioning of images. #i The way to create an oblique m field is basically that the static magnetic field is divided into two directions: vertical (Z axis) direction and horizontal (X, Y axis) direction.
The principles for each are briefly described below. In the former case, the fourth
As shown in FIG. 4(a), by arranging two circular coils facing each other and passing currents in opposite directions, a gradient magnetic field in the Z-axis direction as shown in FIG. 4('b) is generated. In the latter case, if the two Helmholtz coils 8a and 8b are arranged as shown in Fig. 3, and the directions of the currents a and b are opposite to each other, as shown in Fig. 3, Alternatively, a gradient magnetic field in the Y-axis direction is generated. We have just discussed the Helmholtz coil, but in general, even if it is not a circular ring, if it is a closed loop, a gradient magnetic field will be generated.

上記水平方向傾斜磁場コイルの閉ループの形状を矩形に
したものが、第6図に示すコイル10であり、直線と円
弧を組み合わせた扇形のコイルが第5図に示す本発明に
よるコイル6である。第5図、第6図において、2D=
450mmとした時のそれぞれのコイルの傾斜磁場コイ
ルとしての性能(傾斜の均一度、大きさ)が同等な場合
の形状を具体的に表1に示した。この表によるとコイル
6の場合はポールピース凹状の内面に入れられる。
A rectangular closed loop of the horizontal gradient magnetic field coil is the coil 10 shown in FIG. 6, and a fan-shaped coil that is a combination of straight lines and circular arcs is the coil 6 according to the present invention shown in FIG. In Figures 5 and 6, 2D=
Table 1 specifically shows the shapes when the performance (uniformity of gradient, size) of each coil as a gradient magnetic field coil is the same when the diameter is 450 mm. According to this table, coil 6 is inserted into the concave inner surface of the pole piece.

表1 従来コイルと本発明コイルとの大きさの違い(性
能が同等の場合) 骨図、参照 肴畳コイル全体が入る円の直径の最小値〔発明の実施例
〕 以下1本発明の一実施例を第1図、第2図により説明す
る。継鉄1,1′を上下対称に配置し、各々の継鉄1,
1′の4角に継鉄2を取り付ける。
Table 1 Difference in size between the conventional coil and the coil of the present invention (if the performance is the same) Minimum diameter of the circle in which the entire reference tatami coil can fit (bone diagram) [Example of the invention] The following is an implementation of the present invention An example will be explained with reference to FIGS. 1 and 2. The yokes 1 and 1' are arranged vertically symmetrically, and each yoke 1,
Attach yoke 2 to the four corners of 1'.

継鉄1,1′各々の内側に、上下対称になるように、内
に向かい永久磁石3.3’、ポールピース4.4′の順
に配置し、支持枠5,5′により。
Inside each of the yokes 1 and 1', a permanent magnet 3.3' and a pole piece 4.4' are arranged in this order in a vertically symmetrical manner, and supported by support frames 5 and 5'.

設置する。ポールピース4,4′は静磁場の均一度を上
げるために凹面状に形成する。ボールピー  4ス4,
4′の内側にそれぞれ、傾斜磁場コイル6゜6′をとり
つけた支持板7,7′を、コイルがポールピース側にく
るように支持枠に取り付ける。
Install. The pole pieces 4, 4' are formed in a concave shape to increase the uniformity of the static magnetic field. Ball Piece 4s 4,
Support plates 7 and 7' each having a gradient magnetic field coil 6°6' attached to the inside of the pole piece 4' are attached to the support frame so that the coils are on the pole piece side.

コイル6.6′の支持板7,7′への取り付けは。Attaching the coils 6, 6' to the support plates 7, 7'.

支持板にコイルの形状と同じ溝を作り、そこに銅線をは
め、接着剤などで固定すればよい。コイル6.6′の形
状パラメータとポールピース4,4′の凹面の縁の直径
D2との関係はDs<Ihである。支持板7.7′間の
距離はり、となる。
All you have to do is make a groove in the support plate that has the same shape as the coil, fit the copper wire into it, and fix it with adhesive. The relationship between the shape parameter of the coil 6,6' and the diameter D2 of the concave edge of the pole pieces 4,4' is Ds<Ih. The distance between the support plates 7 and 7' is .

核磁気共鳴イメージング装置では、永久磁石3゜3′と
傾斜磁場コイル6.6′が作るg&場空間内に被検者を
設置し、第1図では省略しであるが他に支持板7,7′
間にラジオ波ノくルスを発生させるコイルを設け、被検
者にパルス的に電磁波を照射し、その後被検者より計測
される核磁気共鳴信号により断層像を形成している。
In a nuclear magnetic resonance imaging system, a subject is placed in a G& field space created by a permanent magnet 3°3' and a gradient magnetic field coil 6.6'. 7′
A coil that generates radio waves is installed in between, and the subject is irradiated with electromagnetic waves in pulses, and a tomographic image is then formed using nuclear magnetic resonance signals measured from the subject.

〔発明の効果〕〔Effect of the invention〕

本発明によれば、被検者への圧迫感を除去し、画像の質
を高めることができる。
According to the present invention, it is possible to eliminate the feeling of pressure on the subject and improve the quality of the image.

【図面の簡単な説明】 第1図は本発明の一実施例を示す核磁気共鳴イメージン
グ装置の永久磁石方式磁場発生装置の斜視図でおる。第
2図(a)は上記装置を上から見た平面図である。42
図(b)は第2図aのA−人′線断面図である。第3図
は水平方向の傾斜磁場コイルの斜視図である。第4図(
a)は鉛直方向の傾斜磁場コイルの斜視図である。第4
図(b)は第4図(a)に示したコイルにより発生した
磁場の2成分(Bz )とZとの関係図である。45図
は本発明による傾斜磁場コイルの斜視図である。第6図
は従来の傾斜磁場コイルの斜視図である。 1.1′・・・継鉄、 2. 2’・・・継鉄、3,3
’・・・永久磁石、4,4′・・・ポールピース、5.
5’・・・支持枠、6・・・6′・・・本発明の傾斜磁
場コイル(6a。 6 / a・・・X方向傾斜磁場コイル、 6b、  
6’b・・・X方向傾斜磁場コイル)、7.7’・・・
支持板、8a。 8b・・・ヘルムホルツコイル、9・・・鉛直力M斜磁
場コイル+  10 a *  10’ b・・・従来
のX方向傾斜磁場コイル、10b、10’b・・・従来
のy方向傾斜磁第j図 第2の (a) 第3 回
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a perspective view of a permanent magnet type magnetic field generator of a nuclear magnetic resonance imaging apparatus showing an embodiment of the present invention. FIG. 2(a) is a top plan view of the above device. 42
Figure (b) is a sectional view taken along the line A--person' in Figure 2a. FIG. 3 is a perspective view of a horizontal gradient coil. Figure 4 (
a) is a perspective view of a vertical gradient coil; Fourth
FIG. 4(b) is a diagram showing the relationship between the two components (Bz) of the magnetic field generated by the coil shown in FIG. 4(a) and Z. FIG. 45 is a perspective view of a gradient coil according to the present invention. FIG. 6 is a perspective view of a conventional gradient magnetic field coil. 1.1'...Yoke, 2. 2'...Yoke, 3,3
'...Permanent magnet, 4,4'...Pole piece, 5.
5'...Support frame, 6...6'...Gradient magnetic field coil of the present invention (6a. 6/a...X direction gradient magnetic field coil, 6b,
6'b...X-direction gradient magnetic field coil), 7.7'...
Support plate, 8a. 8b... Helmholtz coil, 9... Vertical force M gradient magnetic field coil + 10 a * 10' b... Conventional X-direction gradient magnetic field coil, 10b, 10'b... Conventional y-direction gradient magnetic field coil Figure j 2nd (a) 3rd

Claims (1)

【特許請求の範囲】[Claims] 1、磁石、ポールピース、継鉄により磁気回路を構成す
る静磁場発生手段と傾斜磁場コイルとを有する核磁気共
鳴イメージング装置において、前記ポールピースが凹状
の形状を有し、更に前記傾斜磁場コイルがポールピース
の凹面によつて作られる空間内に配置されたことを特徴
とする核磁気共鳴イメージング装置。
1. In a nuclear magnetic resonance imaging apparatus having a static magnetic field generating means and a gradient magnetic field coil that constitute a magnetic circuit by a magnet, a pole piece, and a yoke, the pole piece has a concave shape, and further the gradient magnetic field coil has a concave shape. A nuclear magnetic resonance imaging device characterized in that it is disposed within a space created by a concave surface of a pole piece.
JP61207932A 1986-09-05 1986-09-05 Nuclear magnetic resonance imaging apparatus Pending JPS6365849A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP61207932A JPS6365849A (en) 1986-09-05 1986-09-05 Nuclear magnetic resonance imaging apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP61207932A JPS6365849A (en) 1986-09-05 1986-09-05 Nuclear magnetic resonance imaging apparatus

Publications (1)

Publication Number Publication Date
JPS6365849A true JPS6365849A (en) 1988-03-24

Family

ID=16547928

Family Applications (1)

Application Number Title Priority Date Filing Date
JP61207932A Pending JPS6365849A (en) 1986-09-05 1986-09-05 Nuclear magnetic resonance imaging apparatus

Country Status (1)

Country Link
JP (1) JPS6365849A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000126152A (en) * 1998-10-26 2000-05-09 Ge Yokogawa Medical Systems Ltd Mri apparatus

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2000126152A (en) * 1998-10-26 2000-05-09 Ge Yokogawa Medical Systems Ltd Mri apparatus

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