JPS61107704A - Method of stabilizing superconductive coil - Google Patents
Method of stabilizing superconductive coilInfo
- Publication number
- JPS61107704A JPS61107704A JP23060284A JP23060284A JPS61107704A JP S61107704 A JPS61107704 A JP S61107704A JP 23060284 A JP23060284 A JP 23060284A JP 23060284 A JP23060284 A JP 23060284A JP S61107704 A JPS61107704 A JP S61107704A
- Authority
- JP
- Japan
- Prior art keywords
- coil
- superconductive
- partial
- cooled
- stabilizing
- 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
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01F—MAGNETS; INDUCTANCES; TRANSFORMERS; SELECTION OF MATERIALS FOR THEIR MAGNETIC PROPERTIES
- H01F6/00—Superconducting magnets; Superconducting coils
- H01F6/06—Coils, e.g. winding, insulating, terminating or casing arrangements therefor
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Superconductors And Manufacturing Methods Therefor (AREA)
Abstract
Description
【発明の詳細な説明】
〔産業上の利用分野〕
この発明は超電導コイルの安定化方法に関する〔従来技
術〕
超電導マグネットのコイルに常電導転移(クエンチ)が
生ずると、コイルの焼損、液体Heの突出等の事故を招
く恐れがあり、また電流・磁場の急変等電気的特性の乱
れが発生する。[Detailed Description of the Invention] [Industrial Application Field] This invention relates to a method for stabilizing a superconducting coil [Prior Art] When a normal conduction transition (quench) occurs in the coil of a superconducting magnet, the coil burns out and liquid He There is a risk of accidents such as ejection, and disturbances in electrical characteristics such as sudden changes in current and magnetic fields may occur.
この為、従来、コイル、の冷却能を高めたり、コイル線
材の固定構造を工夫したりているが、信頼性が十分でな
く、コイル自体の臨界電流値をコイル線材である超電導
線に固有の臨界電流値より低く設定せざるを得ないと云
う問題があった。For this reason, conventional efforts have been made to improve the cooling capacity of the coil and to improve the fixing structure of the coil wire, but the reliability is insufficient and the critical current value of the coil itself is There was a problem in that the current value had to be set lower than the critical current value.
この発明は上記した問題点を解決するためになされたも
ので、臨界電流値が高く、信頼性の高い超電導コイルを
得ることを目的とする。This invention was made to solve the above-mentioned problems, and aims to obtain a highly reliable superconducting coil with a high critical current value.
この発明は超電導コイル体の小部分づつに強制的にクエ
ンチを起こさせてトレーニングする構成としたものであ
る。This invention has a configuration in which training is performed by forcibly quenching each small portion of a superconducting coil body.
この発明においては、超電導コイル体の小部分づつにク
エンチを発生させるので温度上昇を防ぎ、トレ−ニグ効
果を得ることができる。In this invention, since quenching is generated in small portions of the superconducting coil body, temperature rise can be prevented and a training effect can be obtained.
第1図はこの発明の一実施例を示したものであり、1は
超電導マクネットの超電導コイル体であって、タップI
A、IA、中間タップIB、IBを有している。3はコ
イル冷却部(クライオスタット装置)、4はコイル励磁
用直流電源、5は保護抵抗である。FIG. 1 shows an embodiment of the present invention, in which 1 is a superconducting coil body of a superconducting maknet, and tap I
A, IA, and intermediate taps IB and IB. 3 is a coil cooling unit (cryostat device), 4 is a DC power source for coil excitation, and 5 is a protective resistor.
本実施例においては、超電導コイル体1の製作・冷却終
了後に、中間タップIB、18間に直流電源4から励磁
電圧を印加する。中間タップIB、18間のコイル小部
分Bは流れる電流がある値に達するとクエンチを起こす
ので、これを検出すると同時に、直流電源4をコイル小
部分Bから切離して励磁を停止する。この励磁停止によ
り、保護抵抗5を通る閉回路が閉成され、コイル小部分
Bの蓄積エネルギーは保護抵抗5によりその大半が消費
される。In this embodiment, after the superconducting coil body 1 has been manufactured and cooled, an excitation voltage is applied between the intermediate taps IB and 18 from the DC power supply 4. When the current flowing through the coil small portion B between the intermediate taps IB and 18 reaches a certain value, it quenches, and at the same time this is detected, the DC power source 4 is disconnected from the coil small portion B to stop excitation. By stopping the excitation, a closed circuit passing through the protective resistor 5 is closed, and most of the energy stored in the small coil portion B is consumed by the protective resistor 5.
茸
この時のクエンチ発生部分Bはコイル体1の小部分であ
るのでコイル体1の蓄積エネルギーは小さく、しかも該
蓄積エネルギーの大半は保護抵抗5により消費されるの
で、コイル冷却部3により冷却されているコイル小部分
は殆ど温度上昇しない。Since the quench generation part B at this time is a small part of the coil body 1, the energy stored in the coil body 1 is small, and most of the stored energy is consumed by the protective resistor 5, so it is cooled by the coil cooling part 3. The temperature of the small part of the coil that is inside the coil hardly rises.
超電導コイル体では、クエンチが発生してもコイルの温
度がこれを冷却している液体He温度から余り上昇しな
ければ、クエンチ耐力が増大し、臨界電流密度が上昇す
る現象(トレーニング)を呈するので、上記コイル小部
分Bは上記励磁もしくはその繰返しによりトレーニング
されることになる。このコイル小部分Bのトレーニング
が終ねると、同様の操作を繰返して他のコイル小部分A
のトレニンーングを行い、次いで、コイル小部分Cのト
レーニングを行えば、コイル体1全体がトレニーングさ
れることになり、コイル体1の臨界電流値は超電導線自
体がもつ臨界電流に近づく。In a superconducting coil body, even if a quench occurs, if the temperature of the coil does not rise much from the temperature of the liquid He that cools it, the quench resistance increases and a phenomenon (training) occurs in which the critical current density increases. , the coil small portion B is trained by the excitation or its repetition. After training this coil small section B, repeat the same operation to train other coil small sections A.
, and then the small coil portion C, the entire coil body 1 will be trained, and the critical current value of the coil body 1 will approach the critical current of the superconducting wire itself.
なお、タップIB、IB等は超電導マグネット″′!″
″”°°゛“75−@EE+*ll[−FhL、−“1
1.1することができる。In addition, taps IB, IB, etc. are superconducting magnets ''!''
″”°°゛“75-@EE+*ll[-FhL,-“1
1.1 can be done.
第2図は永久電流モードで動作する超電導コイルの永久
電流スイッチ回路をトレーニングする場合の実施例を示
したものである。FIG. 2 shows an example of training a persistent current switch circuit of a superconducting coil operating in persistent current mode.
同図において、6は永久電流スイッチ回路の永久電流ス
イッチコイル、7は永久電流スイッチ回路用ヒータ、8
はヒータ回路用電源、9はスイッチである。In the figure, 6 is the persistent current switch coil of the persistent current switch circuit, 7 is the heater for the persistent current switch circuit, and 8 is the persistent current switch coil of the persistent current switch circuit.
9 is a power supply for the heater circuit, and 9 is a switch.
この構成において、永久電流スイッチコイル6のトレニ
ーングは、スイッチ9をオフにしておいて直流電源4か
らタラップIA、IAを通して励磁電流Ioを供給する
。これにより、コイル体1とスイッチコイル6にそれぞ
れ電流■1と■2が流れるが、永久電流スイッチコイル
6のインダクタンスがコイル体1のインダクタンスより
十分小さければ、コイル体1には殆ど電流が流れずI。In this configuration, for training the persistent current switch coil 6, the switch 9 is turned off and the excitation current Io is supplied from the DC power supply 4 through the ramps IA and IA. As a result, currents ■1 and ■2 flow through the coil body 1 and the switch coil 6, respectively, but if the inductance of the persistent current switch coil 6 is sufficiently smaller than the inductance of the coil body 1, almost no current flows through the coil body 1. I.
=2となるので、このスイッチイコル6だけにクエンチ
を発生させることができ、上記したトレーニングを行う
ことができる。=2, the quench can be generated only in this switch equal to 6, and the above-described training can be performed.
この発明は以上説明した通り、超電導コイル体の小部分
づつにクエンチを発生させてコイル体自体のクエンチ耐
力を増大させるようにしたので、簡単な方法でコイル体
の臨界電流値をコイル線材の臨界電流値に近づけること
ができ、この効果はコイル体自体のクエンチ耐力を高め
て得られるので、信頼性の高い超電導コイルを得ること
ができる。As explained above, this invention increases the quench resistance of the superconducting coil body by generating quench in small parts of the superconducting coil body, so that the critical current value of the coil body can be easily adjusted to the critical current value of the coil wire material. This effect can be obtained by increasing the quench resistance of the coil body itself, making it possible to obtain a highly reliable superconducting coil.
第1図はこの発明の詳細な説明するための回路図、第2
図はこの発明の他の実施例を説明するための回路図であ
る。
図において、1−・超電導コイル体、2−・−コイル小
部分、3−冷却部、4−・コイル励磁用直流電源 1
.5−保護抵抗、6−永久電流スイッチコイルなお、図
中同一符号は同一または相当部分を示す。Figure 1 is a circuit diagram for explaining the invention in detail, Figure 2 is a circuit diagram for explaining the invention in detail.
The figure is a circuit diagram for explaining another embodiment of the invention. In the figure, 1--superconducting coil body, 2--small coil section, 3-cooling section, 4--DC power supply for coil excitation 1
.. 5-protective resistor, 6-persistent current switch coil Note that the same reference numerals in the figures indicate the same or corresponding parts.
Claims (3)
部分づつを励磁して強制的に常電導転移させて常電導転
移耐力を増大させることを特徴とする超電導コイルの安
定化方法。(1) A method for stabilizing a superconducting coil, which comprises, after fabricating and cooling a superconducting coil body, energizing small portions of the coil body to force the normal conduction transition to increase the normal conductivity transition proof strength.
該タップが電圧検出用タップとして利用されることを特
徴とする特許請求の範囲第1項記載の超電導コイルの安
定化方法。(2) The superconducting coil body has a tap for small part excitation,
The method for stabilizing a superconducting coil according to claim 1, wherein the tap is used as a voltage detection tap.
、これを小部分として励磁することを特徴とする特許請
求の範囲第1項記載の超電導コイルの安定化方法。(3) In the case where a persistent current switch coil is provided, the method for stabilizing a superconducting coil according to claim 1, characterized in that this is excited as a small portion.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP23060284A JPS61107704A (en) | 1984-10-30 | 1984-10-30 | Method of stabilizing superconductive coil |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP23060284A JPS61107704A (en) | 1984-10-30 | 1984-10-30 | Method of stabilizing superconductive coil |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS61107704A true JPS61107704A (en) | 1986-05-26 |
Family
ID=16910314
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP23060284A Pending JPS61107704A (en) | 1984-10-30 | 1984-10-30 | Method of stabilizing superconductive coil |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS61107704A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP5686733B2 (en) * | 2009-06-11 | 2015-03-18 | 株式会社日立メディコ | Method for adjusting superconducting magnet used in magnetic resonance imaging apparatus and dock for exciting superconducting magnet |
-
1984
- 1984-10-30 JP JP23060284A patent/JPS61107704A/en active Pending
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP5686733B2 (en) * | 2009-06-11 | 2015-03-18 | 株式会社日立メディコ | Method for adjusting superconducting magnet used in magnetic resonance imaging apparatus and dock for exciting superconducting magnet |
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