JPH0428349A - Static magnetic field magnet for mri device - Google Patents

Static magnetic field magnet for mri device

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Publication number
JPH0428349A
JPH0428349A JP2134009A JP13400990A JPH0428349A JP H0428349 A JPH0428349 A JP H0428349A JP 2134009 A JP2134009 A JP 2134009A JP 13400990 A JP13400990 A JP 13400990A JP H0428349 A JPH0428349 A JP H0428349A
Authority
JP
Japan
Prior art keywords
magnetic field
coil
coils
static magnetic
mri apparatus
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
JP2134009A
Other languages
Japanese (ja)
Inventor
Tadatoshi Ota
太田 忠利
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 JP2134009A priority Critical patent/JPH0428349A/en
Publication of JPH0428349A publication Critical patent/JPH0428349A/en
Pending legal-status Critical Current

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  • Magnetic Resonance Imaging Apparatus (AREA)

Abstract

PURPOSE:To reduce the axial length in order to prevent a patient from being given with uneasy feeling and generate the highly uniform magnetic field by using a superconductive coil and normal conductive coils for generating a main magnetic field and arranging the superconductive coil at the center part and the normal conductive coils at both the sides. CONSTITUTION:A vacuum container 6 is constituted by using only a superconductive coil 1b having a short axis, and the normal conductive coils 1a' and 1c' are installed outside the vacuum container 6, and a vacuum heat- shielding space 3 including the heat shielding plates 2a and 2b is formed. Accordingly, for the normal electric conductive coils 1a' and 1c', the need of the container having a heat shielding space is obviated, and it is enough only to take account of the space for an electric insulating member 7, etc., and the length of the axis can be shortened in compassion with the constituted case only of the superconductive coil. Further, since each of the coils, 1a', 1b, and 1c' for generating a main magnetic field B is at the same position to the conventional device and has the equal magnetomotive force, the magnetic field uniformity in a diagnosis space 5 is equal to that in the conventional device.

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、医療用磁気共鳴イメージング装置(MRI装
置)に用いられる静磁場マグネッ1−に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a static magnetic field magnet 1- used in a medical magnetic resonance imaging apparatus (MRI apparatus).

(従来の技vfI) MRI装置に用いる静磁場マグネッ1−1特に超電導コ
イルを使ったマグネットは、その構成上、軸長が長くな
る。すなわち、患者を診断するのに必要な空間において
高均一磁場を発生させるためのコイル配置、超電導コイ
ルを極低温に保つための断熱空間等が必要になり、軸長
が長くなる。MRI装置用超電導マグネットの従来の一
例を第6図に示す。このように従来のものは高均一磁場
を出すための3つの超電導コイル1.a、 lb、 l
c、及び熱シールド板2a、2bを含む真空断熱空間3
を有する。これに、磁気シールド4 (鉄などの磁性体
)が取り付けられ、全長として2m前後の装置となる。
(Prior art vfI) Static magnetic field magnet 1-1 used in an MRI apparatus In particular, a magnet using a superconducting coil has a long axial length due to its configuration. That is, a coil arrangement for generating a highly uniform magnetic field in a space necessary for diagnosing a patient, an insulating space for keeping the superconducting coil at an extremely low temperature, etc. are required, and the axial length becomes long. An example of a conventional superconducting magnet for an MRI apparatus is shown in FIG. In this way, the conventional system uses three superconducting coils to generate a highly uniform magnetic field.1. a, lb, l
c, and a vacuum insulation space 3 including heat shield plates 2a and 2b.
has. A magnetic shield 4 (made of a magnetic material such as iron) is attached to this, resulting in a device with a total length of approximately 2 m.

(磁気シールドは周辺機器へ磁場の影響がないようにす
るために用いられる。) (発明が解決しようとする課題) このように、超電導マグネットを用いたMRI装置は、
高磁場を発生させられる、時間的に磁場が安定している
等の利点がある反面、マグネット軸長が長く、大型化し
、患者に不安感を与える問題がある。軸長を短かくする
と、診断空間5内の磁場均一性が悪くなり、均一性を保
とうとすると、誤差磁場を打消すための逆向き電流を流
すコイルが必要となり、コスト高になるという問題があ
る。
(Magnetic shielding is used to prevent the influence of magnetic fields on peripheral equipment.) (Problem to be solved by the invention) In this way, an MRI apparatus using a superconducting magnet can:
Although it has advantages such as being able to generate a high magnetic field and having a stable magnetic field over time, it has the problem that the magnet axis is long and large, giving the patient a sense of anxiety. If the axial length is shortened, the uniformity of the magnetic field within the diagnostic space 5 deteriorates, and in order to maintain the uniformity, a coil is required to flow a current in the opposite direction to cancel the error magnetic field, resulting in an increase in cost. be.

本発明は、軸長が短かく患者に不安感を与えることの少
い高均一磁場のMRI装置用静磁場マグネットを提供す
ることを目的とする。
SUMMARY OF THE INVENTION An object of the present invention is to provide a static magnetic field magnet for an MRI apparatus that has a short axial length and has a highly uniform magnetic field that does not give a patient a feeling of anxiety.

〔発明の構成〕[Structure of the invention]

(課題を解決するための手段) 本発明においては主磁場発生のために超電導コイルと常
電導コイルを用いる。そして好ましくは中央部に超電導
コイルを配置し端側に常電導コイルを配置して、両コイ
ルで高均一な主磁場を発生させる。
(Means for Solving the Problems) In the present invention, a superconducting coil and a normal conducting coil are used to generate the main magnetic field. Preferably, a superconducting coil is disposed at the center and a normal conductive coil is disposed at the ends, so that both coils generate a highly uniform main magnetic field.

(作用) 常電導コイルは、断熱空間をもった容器等は不用であり
、電気絶縁材等のスペースを考慮するだけで良いので、
結果的に超電導コイルのみで構成した場合よりも軸長が
短かくなる。
(Function) Normally conductive coils do not require a container with an insulating space, and only need to consider the space for electrical insulating material, etc.
As a result, the axial length is shorter than when constructed with only superconducting coils.

(実施例) 第1図に本発明の実施例を示す。(Example) FIG. 1 shows an embodiment of the present invention.

短軸の超電導コイル1bだけを用いて真空容器を構成す
る。この超電導コイルIbだけでは診断空間5内に高均
一磁場を形成できないので、真空容器の外に常電導コイ
ルIa’と1c′を設け、コイル配置としては、第6図
のLa、 Ib、 lcと同じようにする。
A vacuum vessel is constructed using only the short-axis superconducting coil 1b. Since this superconducting coil Ib alone cannot form a highly uniform magnetic field in the diagnostic space 5, normal conducting coils Ia' and 1c' are provided outside the vacuum container, and the coil arrangement is as shown in Fig. 6, La, Ib, lc. Do the same.

また、真空断熱空間は、コイルla’、lb間及びlb
In addition, the vacuum insulation space is between the coils la' and lb and between the coils la' and lb.
.

Ic’間のスペースを利用して構成できる。常電導コイ
ルには、断熱空間をもった容器等は不用であり、電気絶
縁材7等のスペースを考慮すれば良いので、結果的に超
電導コイルのみで構成した場合よりも軸長が短かくなる
。つまり、第6図のコイル]、a、lcの外側の断熱空
間に相当する分だけ短軸となり、磁気シールド4もそれ
に合わせて小型化できる。
It can be configured using the space between Ic'. A normal conducting coil does not require a container with an insulating space, and the space for the electrical insulating material 7, etc. can be taken into account, so the axial length will be shorter than when it is composed only of superconducting coils. . In other words, the short axis corresponds to the adiabatic space outside the coils], a, and lc shown in FIG. 6, and the magnetic shield 4 can be miniaturized accordingly.

第2図に常電導コイル用心体9を示す。この導体には、
冷却水を通すための穴10があり、この穴に水を流して
、導体を冷却する。
FIG. 2 shows the normal conducting coil core body 9. This conductor has
There is a hole 10 for passing cooling water, and water is allowed to flow through this hole to cool the conductor.

(実施例の作用) 第1図の主磁場Bを発生させるコイル1a’ 、 lb
 。
(Operation of the embodiment) Coils 1a' and lb that generate the main magnetic field B shown in FIG.
.

1c′は従来(第6図)と同じ位置で同じ起磁力をもつ
ので、診断空間5内の磁場均一性は、従来と同じである
。真空断熱空間3は、コイル1a′〜1b間及び1b〜
lc’間に構成し、熱シールド板2a、2bを配置して
、超電導コイルの冷却媒体である液体ヘリウムの蒸発量
を最小限にする。また、その外側に磁気シールド4を配
置して、漏洩磁場を減少させる。このような構成とした
ことにより、超電導コイルの外側の真空断熱空間の分だ
け軸長が短かくなる。従来、断熱空間は約100〜15
0mm必要であったので、全体として200〜300m
m軸長が短縮できることになる。
1c' has the same magnetomotive force at the same position as in the conventional case (FIG. 6), so the magnetic field uniformity within the diagnostic space 5 is the same as in the conventional case. The vacuum insulation space 3 is between the coils 1a' and 1b and between the coils 1b and 1b.
lc', and heat shield plates 2a and 2b are arranged to minimize the amount of evaporation of liquid helium, which is a cooling medium for the superconducting coil. Furthermore, a magnetic shield 4 is placed outside of the magnetic shield 4 to reduce leakage magnetic fields. With such a configuration, the axial length is shortened by the vacuum insulation space outside the superconducting coil. Conventionally, the insulation space is approximately 100 to 15
0mm was required, so the total length was 200-300m.
This means that the m-axis length can be shortened.

(実施例の効果) このように、主磁場を発生させる超電導コイルのうち、
マグネット中央付近のコイルを超電導コイルで構成し、
端に位置するコイルを常電導コイルで構成する。こうす
ることで両端の真空断熱空間が不要となり、マグネッ1
〜軸長が短かくなる効果がある。
(Effects of Example) In this way, among the superconducting coils that generate the main magnetic field,
The coil near the center of the magnet is composed of a superconducting coil,
The coil located at the end is composed of a normal conducting coil. This eliminates the need for a vacuum insulation space at both ends, and the magnet 1
- Has the effect of shortening the axial length.

(他の実施例) 第3図に本発明の他の実施例を示す。この例は、常電導
コイルを漏洩磁界を低減させるキャンセルコイルとする
ものである。
(Other Embodiments) FIG. 3 shows another embodiment of the present invention. In this example, the normally conducting coil is used as a canceling coil that reduces leakage magnetic field.

超電導コイル1bの軸方向に常電導コイル1a″1c″
を配置する。常電導コイル1a“、 lc“は漏洩磁場
を低減させるキャンセルコイルとするので、シールド効
果を良くするためにその径を大きくしである。すなわち
、常電導コイルla’ 、 1.c”の発生する磁場に
より、超電導コイル1bの発生する漏洩磁場を打ち消す
のであるが、常電導コイル1a“10″の径を超電導コ
イル1bの径よりも大きくすれば、軸方向、及び径方向
の漏洩磁場を効率良く低減できることになる。
In the axial direction of the superconducting coil 1b, there is a normal conducting coil 1a″1c″.
Place. Since the normal conducting coils 1a", lc" are used as canceling coils to reduce leakage magnetic fields, their diameters are made large to improve the shielding effect. That is, normally conducting coil la', 1. The leakage magnetic field generated by the superconducting coil 1b is canceled by the magnetic field generated by the superconducting coil 1b, but if the diameter of the normal conducting coil 1a is made larger than the diameter of the superconducting coil 1b, the axial and radial This means that the leakage magnetic field can be efficiently reduced.

このような構成とすることにより、マグネット両端の真
空断熱空間が省略できるので、第1図の例と同様にマグ
ネットの軸長が短かくできる。また、常電導コイルを磁
気シールドの役目をするキャンセルコイルとしたので、
磁性体の磁気シール1くは不要となり、その分マグネッ
トの軸長をさらに短かくできるという効果がある。
With such a configuration, the vacuum insulation space at both ends of the magnet can be omitted, so the axial length of the magnet can be shortened similarly to the example shown in FIG. In addition, since the normal conduction coil is used as a canceling coil that acts as a magnetic shield,
The magnetic seal 1 made of magnetic material is no longer necessary, and the axial length of the magnet can be further shortened accordingly.

第4図に本発明を用いた他の実施例を示す。これは、超
電導コイル1bを収容する真空容器を磁性体で構成し、
磁性体真空容器6′としたものである。
FIG. 4 shows another embodiment using the present invention. This consists of a vacuum container containing a superconducting coil 1b made of a magnetic material,
This is a magnetic vacuum container 6'.

こうすることで、真空容器6′も磁気シールドの一部と
なるので、マグネットの外に配置する磁気シールド4は
第1図の実施例よりも薄くてすむ。よって、マグネット
の軸長がさらに短かくなるとともに、磁気シールド4は
軽量となるので、組立、据付が容易となる効果がある。
In this way, the vacuum container 6' also becomes a part of the magnetic shield, so that the magnetic shield 4 disposed outside the magnet can be thinner than in the embodiment shown in FIG. Therefore, the axial length of the magnet is further shortened, and the magnetic shield 4 is also lightweight, which has the effect of facilitating assembly and installation.

第5図は本発明において、超電導コイルと永久磁石を用
いた例で、超電導コイル1bを収納する真空容器6の外
側に、超電導コイル1bと合わせて所定の主磁場Bを発
生させるような強度の永久磁石8を配置したものである
。このような構成としても、従来技術(第6図)よりも
マグネットの軸長が短かくなる。
Figure 5 shows an example in which a superconducting coil and a permanent magnet are used in the present invention. Permanent magnets 8 are arranged. Even with this configuration, the axial length of the magnet is shorter than that of the prior art (FIG. 6).

=8− 上記実施例はいずれも常電導コイルまたは永久磁石を超
電導コイルの軸方向両端側に配置したものを示したが、
これらは片端側に配置してもよい。
=8- All of the above embodiments have shown normal conducting coils or permanent magnets arranged at both ends of the superconducting coil in the axial direction.
These may be placed at one end.

このようにすると主磁場が非対称となりMRI装置を設
置する部屋の空間利用率が向上することがある。
If this is done, the main magnetic field will be asymmetrical, which may improve the space utilization of the room in which the MRI apparatus is installed.

〔発明の効果〕〔Effect of the invention〕

以上のように、本発明においては、主磁場を発生させる
コイル群のうち、マグネット中央付近に位置するコイル
を超電導コイルで構成し、端側のコイルを常電導コイル
又は永久磁石で構成するので、マグネット全長が短縮で
き、患者の不安感を緩和する効果がある。
As described above, in the present invention, of the coil group that generates the main magnetic field, the coil located near the center of the magnet is composed of a superconducting coil, and the coils on the end side are composed of normal conducting coils or permanent magnets. The total length of the magnet can be shortened, which has the effect of alleviating patients' anxiety.

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

第1図は本発明の第1の実施例を示す図、超電導コイル
の両側に常電導コイルを配置した断面図、第2図は上記
実施例に用いる常電導コイル用導体を示す図、第3図は
本発明において常電導コイルをキャンセルコイルとして
使用した実施例の図、第4図は本発明において真空容器
を磁性体で構成した実施例の図、第5図は本発明におい
て永久磁石と超電導コイルとを用いた実施例の図、第6
図は従来の超電導マグネッ1〜を示す図である。 la、 lb、 lc・・・超電導コイル18′、1c
′・・・常電導コイル 1a” ]cH・・・常電導キャンセルコイル2a、2
b・・・熱シールド板  3・・・真空断熱空間4・・
・磁気シールド    5・・・診断空間6・・真空容
器      6′・・・磁性体真空容器7・・・電気
絶縁材     8・・永久磁石9・・常電導コイル用
導体 10・・・冷却水用の六B・・主磁場     
  Z・・・Z軸(中心軸)代理人 弁理士 則 近 
憲 佑 Qト
FIG. 1 is a diagram showing a first embodiment of the present invention, a cross-sectional view showing a normal conducting coil arranged on both sides of a superconducting coil, FIG. 2 is a diagram showing a conductor for a normal conducting coil used in the above embodiment, and FIG. The figure shows an example in which a normal conducting coil is used as a canceling coil in the present invention, Figure 4 shows an example in which the vacuum container is made of a magnetic material in the present invention, and Figure 5 shows a permanent magnet and a superconducting coil in the present invention. 6th diagram of an embodiment using a coil
The figure shows conventional superconducting magnets 1 to 1. la, lb, lc...superconducting coils 18', 1c
'...Normal conduction coil 1a'' ]cH...Normal conduction canceling coil 2a, 2
b...Heat shield plate 3...Vacuum insulation space 4...
・Magnetic shield 5...Diagnostic space 6...Vacuum container 6'...Magnetic vacuum container 7...Electrical insulating material 8...Permanent magnet 9...Conductor for normal conducting coil 10...For cooling water 6B...Main magnetic field
Z...Z axis (center axis) agent Patent attorney Nori Chika
Kensuke Qt

Claims (9)

【特許請求の範囲】[Claims] (1)主磁場発生用コイルとして超電導コイルと常電導
コイルを具え、両コイルで所定の主磁場を発生すること
を特徴とするMRI装置用静磁場マグネット。
(1) A static magnetic field magnet for an MRI apparatus, comprising a superconducting coil and a normal conducting coil as main magnetic field generating coils, both coils generating a predetermined main magnetic field.
(2)常電導コイルのかわりに永久磁石が用いられてい
ることを特徴とする請求項(1)記載のMRI装置用静
磁場マグネット。
(2) The static magnetic field magnet for an MRI apparatus according to claim (1), characterized in that a permanent magnet is used in place of the normally conducting coil.
(3)常電導コイルが超電導コイルの発生する漏洩磁界
を低減させるために、超電導コイルとは逆向きの電流を
流すキャンセルコイルとなっていることを特徴とする請
求項(1)記載のMRI装置用静磁場マグネット。
(3) The MRI apparatus according to claim (1), wherein the normal conductive coil is a canceling coil that flows a current in the opposite direction to that of the superconducting coil in order to reduce the leakage magnetic field generated by the superconducting coil. Static magnetic field magnet.
(4)常電導コイルの径は超電導コイルの径よりも大き
いことを特徴とする請求項(1)記載のMRI装置用静
磁場マグネット。
(4) The static magnetic field magnet for an MRI apparatus according to claim (1), wherein the diameter of the normal conducting coil is larger than the diameter of the superconducting coil.
(5)常電導コイルは超電導コイルの軸方向両側に配置
していることを特徴とする請求項(1)記載のMRI装
置用静磁場マグネット。
(5) The static magnetic field magnet for an MRI apparatus according to claim (1), wherein the normal conducting coils are arranged on both sides of the superconducting coil in the axial direction.
(6)超電導コイルの軸方向両側に配置した常電導コイ
ルはそれぞれ別々に励磁できることを特徴とする請求項
(5)記載のMRI装置用静磁場マグネット。
(6) The static magnetic field magnet for an MRI apparatus according to claim (5), wherein the normal conductive coils arranged on both sides of the superconducting coil in the axial direction can be individually excited.
(7)常電導コイルは超電導コイルよりも径が大きく、
超電導コイルとは逆向きの電流を流して超電導コイルの
漏洩磁場を低減させるキャンセルコイルとなっているこ
とを特徴とする請求項(5)記載のMRI装置用静磁場
マグネット。
(7) Normal conducting coils have a larger diameter than superconducting coils,
The static magnetic field magnet for an MRI apparatus according to claim 5, characterized in that the magnet is a canceling coil that reduces leakage magnetic field of the superconducting coil by passing a current in the opposite direction to that of the superconducting coil.
(8)漏洩磁界が軸方向非対称になっていることを特徴
とする請求項(7)記載のMRI装置用静磁場マグネッ
ト。
(8) The static magnetic field magnet for an MRI apparatus according to claim (7), wherein the leakage magnetic field is axially asymmetric.
(9)超電導コイルを収納する真空容器が磁性体となっ
ていることを特徴とする請求項(1)記載のMRI装置
用静磁場マグネット。
(9) The static magnetic field magnet for an MRI apparatus according to claim (1), wherein the vacuum container housing the superconducting coil is made of a magnetic material.
JP2134009A 1990-05-25 1990-05-25 Static magnetic field magnet for mri device Pending JPH0428349A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2134009A JPH0428349A (en) 1990-05-25 1990-05-25 Static magnetic field magnet for mri device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2134009A JPH0428349A (en) 1990-05-25 1990-05-25 Static magnetic field magnet for mri device

Publications (1)

Publication Number Publication Date
JPH0428349A true JPH0428349A (en) 1992-01-30

Family

ID=15118249

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2134009A Pending JPH0428349A (en) 1990-05-25 1990-05-25 Static magnetic field magnet for mri device

Country Status (1)

Country Link
JP (1) JPH0428349A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2022521391A (en) * 2019-02-22 2022-04-07 プロマクソ インコーポレイテッド Systems and methods for performing magnetic resonance imaging

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2022521391A (en) * 2019-02-22 2022-04-07 プロマクソ インコーポレイテッド Systems and methods for performing magnetic resonance imaging
JP2024109788A (en) * 2019-02-22 2024-08-14 プロマクソ インコーポレイテッド Systems and methods for performing magnetic resonance imaging - Patents.com

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