JPH011211A - Static magnetic field coil device for MRI - Google Patents

Static magnetic field coil device for MRI

Info

Publication number
JPH011211A
JPH011211A JP62-155378A JP15537887A JPH011211A JP H011211 A JPH011211 A JP H011211A JP 15537887 A JP15537887 A JP 15537887A JP H011211 A JPH011211 A JP H011211A
Authority
JP
Japan
Prior art keywords
magnetic field
static magnetic
field coil
mri
coil
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
JP62-155378A
Other languages
Japanese (ja)
Other versions
JPS641211A (en
Inventor
臼井 嘉行
Original Assignee
株式会社東芝
Filing date
Publication date
Application filed by 株式会社東芝 filed Critical 株式会社東芝
Priority to JP62-155378A priority Critical patent/JPH011211A/en
Publication of JPS641211A publication Critical patent/JPS641211A/en
Publication of JPH011211A publication Critical patent/JPH011211A/en
Pending legal-status Critical Current

Links

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) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 [発明の目的] (産業上の利用分野) 本発明は、電流供給によりMRI(磁気共鳴イメージン
グ)用静磁揚を形成する静磁場コイルを直えたMRI用
静磁場コイル装置に関する。
[Detailed Description of the Invention] [Object of the Invention] (Industrial Application Field) The present invention provides a static magnetic field coil for MRI (magnetic resonance imaging), which is a modified static magnetic field coil that forms a static magnetic lift for MRI (magnetic resonance imaging) by supplying current. Regarding equipment.

(従来の技術) 従来、常電39MRIにおいては、ひとたび、常電導静
磁場コイルへの電流の供給を断つと(電源をオフづ−る
と)、百度電源をオンしてから蹟影が可能となるまでに
長い時間(30分程度)を必要とした。この時間は通常
、余熱時開と称されているが、この時間の存在のために
、常電4MRIシステムの使用にあたっては、顕彰の必
要性の有無にかかわらず、静磁場コイルに常に定格電流
(敵影のために必要な静磁場を発生するための電流)が
流されていた。このため従来は電力料金についてのラン
ニングコストを上背ざぜていた。
(Prior art) Conventionally, in normal-current 39 MRI, once the current supply to the normal-conducting static magnetic field coil is cut off (when the power is turned off), it is possible to perform imaging after turning on the power supply. It took a long time (about 30 minutes). This time is usually referred to as the preheating period, but due to the existence of this time, when using a static 4MRI system, the static magnetic field coil is always supplied with the rated current ( A current (current) was flowing to generate the static magnetic field necessary for enemy shadows. For this reason, in the past, running costs related to electricity charges were high.

そこで本願発明者は先に、アイドリング方式によりラン
ニングコストの低下を図った磁気共鳴イメージング装置
を提案している(特願昭61−266561 )。
Therefore, the inventor of the present application has previously proposed a magnetic resonance imaging apparatus that uses an idling system to reduce running costs (Japanese Patent Application No. 61-266561).

この方式は、非岡影時には静磁場コイルへ流す電流を定
格電流の数分の−(たとえばL/4)に減少させるとと
もに、電源内部の電流検出用水冷シPン1〜抵抗及び静
磁場コイルを冷却する冷ム1水の流量を各々の温度か敵
影口)から変化しないように減少・制御しようというも
のでおる。
This method reduces the current flowing through the static magnetic field coil to a fraction of the rated current (for example, L/4) during non-operating conditions, and also reduces the current flowing through the static magnetic field coil from the water cooling system P1 for current detection inside the power supply to the resistor and the static magnetic field coil. The objective is to reduce and control the flow rate of cold water that cools the water so that it does not change from each temperature.

このディトリング方式によれば、■影が必要となったと
きに電流を定格電流に増ヤしてやれば、長い予熱時間を
必要とヒザに即座に蹟影が可能となる。また、非暗影時
には、消費電力は敵影時のそれの士数分の−(たとえば
1/16)となるので、それまでの方式(連続通電方式
)に比してランニングコストの大幅な低減を実現するこ
とができる。
According to this Detling method, if the current is increased to the rated current when shading is required, it becomes possible to immediately shading the knee even though a long preheating time is required. In addition, when there is no dark shadow, the power consumption is - (for example, 1/16) the power consumption when there is enemy shadow, so running costs are significantly reduced compared to the previous method (continuous energization method). It can be realized.

(発明か解決しようとする問題点) しかしながら、上記のアイドリング方式においては、非
岡影時にコイル供給電流が低減するものの、ある程度の
電流を流しておく必要があるため、静磁場コイルでの電
力消費を零とすることができない。
(Problem to be solved by the invention) However, in the above idling method, although the coil supply current is reduced during non-operation, it is necessary to keep a certain amount of current flowing, so the power consumption in the static magnetic field coil is reduced. cannot be made zero.

そこで本発明は、上記のアイドリング方式の場合よりも
更にランニングコストの低減を図ろうと16もので、非
暗影時に静磁場コイルでの電力消費を必要とぜず、しか
も敵影時には即座に必要な静ia場を形成し冑るMRI
用静磁場コイル装置の提供を目的としている。
Therefore, the present invention aims to further reduce the running cost compared to the above-mentioned idling method, and eliminates the need for power consumption in the static magnetic field coil when there is no dark shadow, and moreover, when there is enemy shadow, the static magnetic field coil that is required immediately MRI that creates and clears the ia field
The purpose of this project is to provide a static magnetic field coil device for use.

[発明の構成] (問題点を解決するための手段) 本発明は、電力供給によりMRI用静磁場を形成するコ
イルを備えたMRI用静磁揚]イコイ石において、前記
コイルと大気との間に該コイルよりの放熱を遮断する断
熱層を設けたものである。
[Structure of the Invention] (Means for Solving the Problems) The present invention provides a magnetostatic lift for MRI, which is equipped with a coil that forms a static magnetic field for MRI by supplying electric power. A heat insulating layer is provided to block heat radiation from the coil.

(作 用) 従来方式(連続通電方式)において、電源をオフした後
に、再度オンしてから囮影が可能となるまでに長い予熱
時間を必要とするのは人別して次の二つの特性による。
(Function) In the conventional method (continuous energization method), after the power is turned off and then turned on again, a long preheating time is required before decoy shadowing is possible due to the following two characteristics.

すなわち、 ■静磁場強度がドリフトづる。That is, ■Static magnetic field strength drifts.

MRIにおいては、暗影時間中において起こる磁場強度
のドリフ1へは数ppm以下であることが要求される。
In MRI, the magnetic field strength drift 1 that occurs during the dark shadow time is required to be several ppm or less.

■静磁場強度の分布が変化する。■The distribution of static magnetic field strength changes.

MRIにおいては、磁場強度の分布の均一性が高いこと
(10ppm程度)が要求される。
In MRI, it is required that the distribution of magnetic field strength be highly uniform (approximately 10 ppm).

上記2つの問題はいずれも、静磁場コイルの性能に起因
する。づなわち、静磁場コイルへ電流が供給されなくな
ると、冷却水の供給を停止しても静磁場コイルの熱は大
気中に放散され、静磁場コイル自体の温度が低下し、静
磁場コイルの寸法・正常に変化を生ずる。そして再び静
磁場コイルに電流を供給した場合、上記の寸法・形状変
化は直ちに元に戻るものではなく安定するまでには長い
時間を必要とする。
Both of the above two problems are caused by the performance of the static magnetic field coil. In other words, when current is no longer supplied to the static magnetic field coil, the heat of the static magnetic field coil is dissipated into the atmosphere even if the supply of cooling water is stopped, the temperature of the static magnetic field coil itself decreases, and the temperature of the static magnetic field coil decreases. Dimensions/normal changes occur. When a current is supplied to the static magnetic field coil again, the above-mentioned changes in size and shape do not immediately return to their original state, but require a long time to stabilize.

そこで、上記のように静磁場コイルと大気との間にr、
IJT熱層を設け、静磁場コイルよりの6文熱を遮断す
るようにすれば、静磁場コイルに電流が全く供給されな
くなっても、静磁場コイル自体の温度低下は)へめで小
さく、コイルの寸法・形状もほとんど変化しない。従っ
て、再び静磁場コイルに電流を供給した場合、該コイル
によって形成される静磁場は即座に安定する。
Therefore, as mentioned above, between the static magnetic field coil and the atmosphere,
If an IJT thermal layer is provided to block the heat from the static magnetic field coil, even if no current is supplied to the static magnetic field coil at all, the temperature drop in the static magnetic field coil itself will be small and small, and the coil's temperature will be small. The dimensions and shape also hardly change. Therefore, when a current is supplied to the static magnetic field coil again, the static magnetic field formed by the coil stabilizes immediately.

(実施例) 以下、本発明を実施例により具体的に説明する。(Example) Hereinafter, the present invention will be specifically explained with reference to Examples.

第1図は本発明の一実施例を示すものである。FIG. 1 shows an embodiment of the present invention.

2はMRI用静磁場コイル装置でおり、この装置2は、
静磁場コイル3を備え、この静磁場コイル3と人気との
間に断熱層4を設けて成る。この静磁場コイル3には電
源1より所定の電流が供給されるようになっており、こ
の電流供給により、静磁場コイル3はMRI用の所定の
静磁場を形成することになる。また、電源1内の主要部
(例えば出力電流検出用の水冷シャント抵抗等)及び静
v7:1揚]イル3と、冷却ユニット5との間で冷却水
が循環するようになっており、この冷却水により電源1
内の主要部及び静Ia場コイル3が適宜に冷却されるよ
うになっている。
2 is a static magnetic field coil device for MRI, and this device 2 is:
A static magnetic field coil 3 is provided, and a heat insulating layer 4 is provided between the static magnetic field coil 3 and the magnet. A predetermined current is supplied from the power supply 1 to the static magnetic field coil 3, and by supplying this current, the static magnetic field coil 3 forms a predetermined static magnetic field for MRI. In addition, cooling water is circulated between the main parts in the power supply 1 (for example, a water-cooled shunt resistor for output current detection, etc.) and the static pump 3, and the cooling unit 5. Power supply 1 by cooling water
The main parts inside and the static Ia field coil 3 are appropriately cooled.

ここで、前記MRI用静磁場コイル装置2における断熱
層4は、静磁場コイル3よりの放熱を遮断する機能、す
なわち静磁場コイル3を保温する機能を有する。
Here, the heat insulating layer 4 in the static magnetic field coil device 2 for MRI has a function of blocking heat radiation from the static magnetic field coil 3, that is, a function of keeping the static magnetic field coil 3 warm.

この断熱層4の具体的構成としては種々の方式が考えら
れる。例えば第2図に示すように、複数の静磁場コイル
3A角にコイル巻線の外側を断熱部vI4 Aによって
覆うようにしてもよいし、また第3図に示すように、複
数の静Ia場コイル3Aを収納するコイルケース体6の
内側に断熱部材4△を設けるようにしてもよい。要は、
静磁場コイルよりの放熱を遮断できる構成で必ればよく
、断熱部材の種類及びその取付箇所等については適宜に
決定することができる。
Various methods can be considered as the specific structure of this heat insulating layer 4. For example, as shown in FIG. 2, the outside of the coil winding may be covered with a heat insulating section vI4A at the 3A angle of a plurality of static magnetic field coils, or as shown in FIG. A heat insulating member 4Δ may be provided inside the coil case body 6 that houses the coil 3A. In short,
It is only necessary to have a configuration that can block heat radiation from the static magnetic field coil, and the type of heat insulating member and its mounting location can be determined as appropriate.

上記の構成において、撮影時には、従来装置と同様に電
源1より所定の電流が静磁場コイル3に供給され、これ
によりMRI用静磁静磁形成される。
In the above configuration, at the time of imaging, a predetermined current is supplied from the power source 1 to the static magnetic field coil 3 as in the conventional apparatus, thereby forming a magnetostatic field for MRI.

また、非岡影時においては、静磁場コイル3への電流供
給が完全に停止され、これと同時に冷却ユニツ1〜5に
よる冷却水循環が停止される。
Furthermore, during non-operation, the current supply to the static magnetic field coil 3 is completely stopped, and at the same time, the circulation of cooling water by the cooling units 1 to 5 is stopped.

第4図は本実施例のタイミングを示している。FIG. 4 shows the timing of this embodiment.

同図において、■は電源1より静磁場コイル3に供給さ
れる電流を示し、王は静磁場コイル3の温度を示し、1
−1は静磁場コイル3によって形成される静磁場の強度
を示している。また、特性曲線中、実線は本実施例を示
し、破線は従来例を示している。
In the same figure, ■ indicates the current supplied from the power source 1 to the static magnetic field coil 3, and the king indicates the temperature of the static magnetic field coil 3.
-1 indicates the strength of the static magnetic field formed by the static magnetic field coil 3. Furthermore, in the characteristic curves, the solid line indicates this embodiment, and the broken line indicates the conventional example.

同図より明らかなように、従来はミ電源1をオフして静
磁場コイル3への電流供給を停止すると(tl)、コイ
ル温度が急激に低下した。従って再度電源をオンすると
きには(丁2)、コイルの温度は大きくさがっており(
Δ丁)、静磁場コイルの寸法は小さくなっていた。従っ
てこのとぎに発生する静磁場は、コイル電流値■がオフ
以前と同一であるにもかかわらす大きくなっていたくΔ
1」)。ちなみに、コイルの温度変化へTと発生Jる磁
場の変動ΔHとの間には一般に次の式が成立する。
As is clear from the figure, in the past, when the power supply 1 was turned off and the current supply to the static magnetic field coil 3 was stopped (tl), the coil temperature dropped rapidly. Therefore, when the power is turned on again (Code 2), the temperature of the coil has dropped significantly (
ΔT), the dimensions of the static magnetic field coil were smaller. Therefore, the static magnetic field that is generated at this point will be larger than Δ even though the coil current value ■ is the same as before it was turned off.
1”). Incidentally, the following equation generally holds between the temperature change T of the coil and the fluctuation ΔH of the generated magnetic field.

Δ11’、2αΔ丁          ・・・(1)
ここで、 Δ11:磁場強度の変化量 α:コイル材料の線膨脹係数(ppm/’C)ΔT:コ
イルの温度変化(°C) 一方、本実施例によれば、断熱層4を設けたことにより
、電源1をオフしても大気中に放散される熱を極めて少
なくすることができるため、静磁場コイル3の温度の低
下は著しく小さくなる(Δ丁′ )。従って、静磁場コ
イル3の寸法の変化も小さくなり、再度電源1をオンし
たときの静磁場変化量も小さくなる(Δl」′)。
Δ11', 2αΔd...(1)
Here, Δ11: Amount of change in magnetic field strength α: Coefficient of linear expansion of coil material (ppm/'C) ΔT: Change in temperature of coil (°C) On the other hand, according to this embodiment, the heat insulating layer 4 is provided. Therefore, even if the power supply 1 is turned off, the heat dissipated into the atmosphere can be extremely reduced, so that the temperature drop of the static magnetic field coil 3 is significantly reduced (Δd'). Therefore, the change in the dimensions of the static magnetic field coil 3 becomes small, and the amount of change in the static magnetic field when the power supply 1 is turned on again becomes small (Δl''').

このように静磁場強度1−1の変化量を小さくすること
ができれば、撮影中の静磁場強度及び分布の変化が許容
値に入るまでに要する時間が大幅に短縮される。しかも
、本実施例では、非撮影時のコイル電流を零(消費電力
も零)とすることができるので、ランニングコストが大
幅に低減される。
If the amount of change in the static magnetic field strength 1-1 can be reduced in this manner, the time required for the change in the static magnetic field strength and distribution to fall within the allowable value during imaging can be significantly shortened. Furthermore, in this embodiment, since the coil current can be reduced to zero (power consumption is also zero) during non-imaging times, running costs are significantly reduced.

[発明の効果1 以上詳述したように本発明によれば、非撮影時に静磁場
コイルでの電力消費を必要とせず、しかも圀影時には即
座に必要な静磁場を形成し1qるMRI用静磁場コイル
装置を提供することができる。
[Effect of the invention 1] As detailed above, according to the present invention, the static magnetic field coil for MRI does not require power consumption during non-imaging periods, and the necessary static magnetic field is immediately generated during imaging. A magnetic field coil device can be provided.

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

第1図は本発明一実施例のブロック図、第2図及び第3
図は第1図の主要部の詳細な構成を示す断面図、第4図
は本実施例の作用を説明するためのタイミング図である
。 1・・・電源、 2・・・MRI用静磁場コイル装置、
3・・・静VIi場コイル、 4・・・断熱層。 代理人 弁理士 則  近  憲  告同     近
    藤     猛A /′ 3、A   / 弔3図・ 1    オフ    オン 第4図
Figure 1 is a block diagram of one embodiment of the present invention, Figures 2 and 3 are block diagrams of one embodiment of the present invention.
This figure is a sectional view showing the detailed structure of the main part of FIG. 1, and FIG. 4 is a timing chart for explaining the operation of this embodiment. 1... Power supply, 2... Static magnetic field coil device for MRI,
3... Static VIi field coil, 4... Heat insulation layer. Agent Patent Attorney Norihiro Kondo Takeshi Kondo A/' 3, A/Condolence 3 Figure 1 Off On Figure 4

Claims (1)

【特許請求の範囲】[Claims]  電流供給によりMRI用静磁場を形成する静磁場コイ
ルを備えたMRI用静磁場コイル装置において、前記静
磁場コイルと大気との間に該コイルよりの放熱を遮断す
る断熱層を設けたことを特徴とするMRI用静磁場コイ
ル装置。
A static magnetic field coil device for MRI comprising a static magnetic field coil that forms a static magnetic field for MRI by supplying current, characterized in that a heat insulating layer is provided between the static magnetic field coil and the atmosphere to block heat radiation from the coil. A static magnetic field coil device for MRI.
JP62-155378A 1987-06-24 Static magnetic field coil device for MRI Pending JPH011211A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62-155378A JPH011211A (en) 1987-06-24 Static magnetic field coil device for MRI

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62-155378A JPH011211A (en) 1987-06-24 Static magnetic field coil device for MRI

Publications (2)

Publication Number Publication Date
JPS641211A JPS641211A (en) 1989-01-05
JPH011211A true JPH011211A (en) 1989-01-05

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