JPH07174803A - Superconductive coil quenching detection device - Google Patents

Superconductive coil quenching detection device

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Publication number
JPH07174803A
JPH07174803A JP5317884A JP31788493A JPH07174803A JP H07174803 A JPH07174803 A JP H07174803A JP 5317884 A JP5317884 A JP 5317884A JP 31788493 A JP31788493 A JP 31788493A JP H07174803 A JPH07174803 A JP H07174803A
Authority
JP
Japan
Prior art keywords
superconducting coil
coil
bridge
quench
resistor
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
JP5317884A
Other languages
Japanese (ja)
Inventor
Ichiro Takano
野 一 郎 高
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 JP5317884A priority Critical patent/JPH07174803A/en
Publication of JPH07174803A publication Critical patent/JPH07174803A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To easily detect any quenching occurring at the distant arbitrary coil section of a superconducting coil by leading out two intermediate taps from the superconducting coil and connecting it to fixed terminals of a 3-terminal variable resistor. CONSTITUTION:Intermediate taps 17 and 18 in addition to coil ends 5 and 6 are led out from a superconducting coil 1, led in a quench circuit 4, respectively, and connected to fixed terminals 19 and 20 of a 3-terminal variable resistor 21. A rough bridge balance is achieved by adjusting the resistance value of a bridge resistor 12, and a bridge circuit is balanced by adjusting the partial potential point of the resistor 21. For example, if any quenching occurs between the coil end 5 and the tap 17, a normal conducting resistance component occurs at that coil section, a normal conducting voltage is generated, and the balance condition of the bridge circuit is broken. When the voltage generated due to unbalance continuously exceeds the limit for the required period of time or longer, a protective method connected to detection output ends 11 and 12 determines the occurrence of a quenching and outputs a quenching detection signal.

Description

【発明の詳細な説明】Detailed Description of the Invention

【0001】[0001]

【産業上の利用分野】本発明は、超電導コイルのクエン
チ検出装置に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a quench detecting device for a superconducting coil.

【0002】[0002]

【従来の技術】従来技術による超電導コイルのクエンチ
検出装置の回路図を図3に示す。検出対象となる超電導
コイル1は、直流遮断器3を介して直流電源2に接続さ
れ、保護投入用スイッチ15を介して保護抵抗16と並
列に接続される。超電導コイル1のコイル端5,6及び
中間タップ7がクエンチ検出回路4に導かれる。
2. Description of the Related Art A circuit diagram of a quench detecting device for a superconducting coil according to the prior art is shown in FIG. The superconducting coil 1 to be detected is connected to the DC power source 2 via the DC circuit breaker 3 and is connected in parallel with the protection resistor 16 via the protection switching switch 15. The coil ends 5 and 6 of the superconducting coil 1 and the intermediate tap 7 are guided to the quench detection circuit 4.

【0003】クエンチ検出回路4には電圧入力端8,1
0及び検出出力端9,11が設けられている。電圧入力
端8,10にはそれぞれ一方では超電導コイル1のコイ
ル端5,6から導出されたリード線が接続されると共
に、他方では直列接続の2つのブリッジ抵抗12,13
の両端が接続される。ブリッジ抵抗12は可変抵抗器か
らなっており、ブリッジ抵抗13は固定抵抗からなって
いる。超電導コイル1の中間タップ7から導出されたリ
ード線が第1の検出出力端9に接続され、2つのブリッ
ジ抵抗12,13の共通接続点が第2の検出出力端11
を構成する。中間タップ7によって区分された超電導コ
イル1の2つの部分(以下、「コイル部分」という)と
2つのブリッジ抵抗12,13とでクエンチ検出のため
のブリッジ回路が構成されている。
The quench detection circuit 4 has voltage input terminals 8, 1
0 and detection output terminals 9 and 11 are provided. Lead wires derived from the coil ends 5 and 6 of the superconducting coil 1 are connected to the voltage input ends 8 and 10, respectively, and the two bridge resistors 12 and 13 connected in series are connected to each other on the other hand.
Both ends of are connected. The bridge resistor 12 is a variable resistor, and the bridge resistor 13 is a fixed resistor. The lead wire derived from the intermediate tap 7 of the superconducting coil 1 is connected to the first detection output end 9, and the common connection point of the two bridge resistors 12 and 13 is the second detection output end 11.
Make up. A bridge circuit for quench detection is configured by two portions of the superconducting coil 1 (hereinafter, referred to as “coil portion”) divided by the intermediate tap 7 and two bridge resistors 12 and 13.

【0004】次に、図3の検出回路の動作について説明
する。まず、図3の検出回路において、正常時の場合、
つまり超電導コイル1にクエンチが発生していない場合
を考える。保護投入用スイッチ15を開いた状態で、直
流遮断器3を閉じ、直流電源2から超電導コイル1に調
整用の電圧を印加し、電流を流す。超電導コイル1に流
れる電流の大きさをi、超電導コイル1のインダクタン
スをLとすると、コイル端5,6の間に、L×(di/
dt)の大きさの誘導性電圧が発生する。そこで検出出
力端9,11間に電流計Mを接続し、前記の条件下でブ
リッジ回路が平衡するように、すなわち検出出力端9,
11間に接続された電流計Mの振れ(電流値)が零(ゼ
ロ)になるように可変のブリッジ抵抗12の値を調整す
る。
Next, the operation of the detection circuit shown in FIG. 3 will be described. First, in the detection circuit of FIG.
That is, consider the case where the quench does not occur in the superconducting coil 1. With the protection switch 15 open, the DC breaker 3 is closed, a voltage for adjustment is applied from the DC power supply 2 to the superconducting coil 1, and a current is passed. If the magnitude of the current flowing through the superconducting coil 1 is i and the inductance of the superconducting coil 1 is L, then L × (di /
An inductive voltage of magnitude dt) is generated. Therefore, an ammeter M is connected between the detection output terminals 9 and 11 so that the bridge circuit is balanced under the above conditions, that is, the detection output terminals 9 and 11.
The value of the variable bridge resistor 12 is adjusted so that the swing (current value) of the ammeter M connected between 11 becomes zero.

【0005】次に、超電導コイル1に超電導状態で電流
が流れているときに、何らかの原因で超電導コイル1の
一部にクエンチが発生した場合を考える。超電導コイル
1の少なくとも一部にクエンチが発生すると、超電導コ
イル1は少なくとも部分的に常電導抵抗成分が挿入され
たのと等価の状態になり、図4に示すように、あたかも
常電導抵抗成分に対応する抵抗25が超電導コイル1内
に接続されたかのような状態になる。この時、抵抗25
に流れる電流によって、常電導電圧が抵抗25の両端に
発生する。この常電導電圧が発生することにより、ブリ
ッジ回路の平衡条件が崩れ、検出出力端9,11間に電
圧を生ずる。この電圧が所定値を超えた状態が所定時間
以上継続することによりクエンチ発生と判断し、クエン
チ検出信号を出力する。
Next, consider a case where a quench occurs in a part of the superconducting coil 1 for some reason while a current is flowing in the superconducting coil 1 in a superconducting state. When the quench occurs in at least a part of the superconducting coil 1, the superconducting coil 1 becomes at least partially equivalent to the state in which the normal conducting resistance component is inserted, and as shown in FIG. It becomes as if the corresponding resistor 25 is connected in the superconducting coil 1. At this time, the resistance 25
A current flowing in the resistor 25 causes a normal conduction voltage across the resistor 25. The generation of this normal conducting pressure breaks the equilibrium condition of the bridge circuit and generates a voltage between the detection output terminals 9 and 11. When the voltage exceeds the predetermined value for a predetermined time or more, it is determined that the quench has occurred, and the quench detection signal is output.

【0006】この検出出力により、図示していない保護
回路を介して、保護投入用スイッチ15を閉じ、直流遮
断器3を開く。これによって、超電導コイル1の保有磁
気エネルギーは、超電導コイル1から保護抵抗16を介
して、時定数=L/(保護抵抗16の抵抗値)の値で減
衰しながら循環する電流として消費される。このよう
に、クエンチ発生時の電流が保護抵抗16を介して流れ
ることによって、超電導コイル1の保有磁気エネルギー
は保護抵抗16によって消費され、その分だけ超電導コ
イル1自体でのエネルギー消費すなわち温度上昇も抑制
され、ここに超電導コイル1を熱破壊から保護すること
ができる。
With this detection output, the protection switch 15 is closed and the DC circuit breaker 3 is opened via a protection circuit (not shown). As a result, the magnetic energy possessed by the superconducting coil 1 is consumed as a circulating current from the superconducting coil 1 via the protective resistor 16 while being attenuated with a value of time constant = L / (resistance value of the protective resistor 16). As described above, since the current at the time of occurrence of quench flows through the protective resistance 16, the magnetic energy possessed by the superconducting coil 1 is consumed by the protective resistance 16, and the energy consumption, that is, the temperature rise in the superconducting coil 1 itself is correspondingly consumed. It is suppressed and here the superconducting coil 1 can be protected from thermal destruction.

【0007】[0007]

【発明が解決しようとする課題】しかし、従来の超電導
コイルのクエンチ検出装置では、1つの超電導コイルの
中間タップ7の両側に直接連なる2つのコイル部分のい
ずれかに発生したクエンチ現象しか検出することができ
ず、コイル中間タップから離れている任意の範囲での超
電導コイルのクエンチを検出するものではない。この種
の検出装置は、原理的には直列接続の2つの超電導コイ
ルを対象としてそのいずれかのクエンチを検出するのに
は適していない。
However, in the conventional quench detecting device for a superconducting coil, only the quench phenomenon occurring in either of the two coil portions directly connected to both sides of the intermediate tap 7 of one superconducting coil is detected. However, it does not detect the quench of the superconducting coil in an arbitrary range away from the coil center tap. This type of detection device is in principle not suitable for detecting quench of either of two superconducting coils connected in series.

【0008】そこで、本発明は、離れている任意のコイ
る部分に発生する超電導コイルのクエンチを検出しうる
超電導コイルのクエンチ検出装置を提供することを目的
とするものである。
Therefore, an object of the present invention is to provide a quenching apparatus for a superconducting coil capable of detecting a quench of the superconducting coil generated in an arbitrary coiled portion that is separated.

【0009】[0009]

【課題を解決するための手段】本発明の超電導コイルの
クエンチ検出装置は、検出対象の超電導コイルから2つ
の中間タップを導出し、その2つの中間タップ間に3端
子可変抵抗器の固定端子を接続すると共に、超電導コイ
ルの両コイル端間に直列接続の2つのブリッジ抵抗を接
続して、超電導コイル及びブリッジ抵抗によりブリッジ
回路を形成し、3端子可変抵抗器の可動端子及び両ブリ
ッジ抵抗の共通接続点を検出出力端としたものである。
A quench detecting device for a superconducting coil according to the present invention derives two intermediate taps from a superconducting coil to be detected and inserts a fixed terminal of a three-terminal variable resistor between the two intermediate taps. In addition to connecting, connect two bridge resistors in series between both coil ends of the superconducting coil to form a bridge circuit with the superconducting coil and the bridge resistor, and the movable terminal of the three-terminal variable resistor and both bridge resistors are common The connection point is the detection output end.

【0010】[0010]

【作用】本発明の超電導コイルのクエンチ検出装置にお
けるブリッジ回路の平衡は、可変のブリッジ抵抗及び3
端子可変抵抗器の少なくとも一方の抵抗値を調整するこ
とによって行われる。ブリッジ回路の一部を構成する超
電導コイルの一部に、クエンチが発生すると、平衡状態
のブリッジ回路の検出出力端間に電圧が発生し、それに
基いてクエンチを検出することができる。このように、
本発明によれば、超電導コイルの離れている任意のコイ
ル部分に発生するクエンチを検出することができる。
The balance of the bridge circuit in the quench detecting device for a superconducting coil according to the present invention is controlled by a variable bridge resistance and 3
This is performed by adjusting the resistance value of at least one of the terminal variable resistors. When a quench occurs in a part of the superconducting coil forming a part of the bridge circuit, a voltage is generated between the detection output terminals of the bridge circuit in the balanced state, and the quench can be detected based on the voltage. in this way,
According to the present invention, it is possible to detect a quench occurring in an arbitrary coil portion that is apart from the superconducting coil.

【0011】[0011]

【実施例】図1は本発明による超電導コイルのクエンチ
検出装置の一実施例を示すものである。検出対象の超電
導コイル1は、直流遮断器3を介して直流電源2に接続
され、保護投入用スイッチ15を介して保護抵抗16に
並列に接続される。超電導コイル1から、コイル端5,
6のほかに、中間タップ17,18が導出され、それぞ
れクエンチ検出回路4に導入されている。クエンチ検出
回路4には電圧入力端8,10および検出出力端11,
22が備えられている。電圧入力端8にはコイル端5か
ら導出されたリード線が接続され、電圧入力端10には
コイル端6から導出されたリード線が接続される。電圧
入力端8及び検出出力端11の間に可変のブリッジ抵抗
12が接続され、電圧入力端10及び検出出力端11の
間に固定のブリッジ抵抗13が接続されている。超電導
コイル1から導出された2つの中間タップ17,18は
それぞれ3端子可変抵抗器21の固定端子19,20に
接続されている。3端子可変抵抗器21の可動端子23
は検出出力端22に接続されている。
DESCRIPTION OF THE PREFERRED EMBODIMENTS FIG. 1 shows an embodiment of a quench detecting device for a superconducting coil according to the present invention. The superconducting coil 1 to be detected is connected to the DC power supply 2 via the DC circuit breaker 3 and is connected in parallel to the protection resistor 16 via the protection switching switch 15. From the superconducting coil 1 to the coil end 5,
In addition to 6, intermediate taps 17 and 18 are derived and introduced into the quench detection circuit 4, respectively. The quench detection circuit 4 includes voltage input terminals 8 and 10 and a detection output terminal 11,
22 is provided. A lead wire derived from the coil end 5 is connected to the voltage input end 8, and a lead wire derived from the coil end 6 is connected to the voltage input end 10. A variable bridge resistor 12 is connected between the voltage input terminal 8 and the detection output terminal 11, and a fixed bridge resistor 13 is connected between the voltage input terminal 10 and the detection output terminal 11. The two intermediate taps 17 and 18 derived from the superconducting coil 1 are connected to fixed terminals 19 and 20 of a 3-terminal variable resistor 21, respectively. Movable terminal 23 of 3-terminal variable resistor 21
Is connected to the detection output terminal 22.

【0012】図1において、正常時の場合、つまり超電
導コイル1にクエンチが発生していない場合を考える。
保護投入用スイッチ15を開いた状態で、直流遮断器3
を閉じ、直流電源2から超電導コイル1に電流を流し、
その電流値を変化させる。一方、ブリッジ回路の平衡を
取る場合、すでに述べた電流調整の過程を通して可変の
ブリッジ抵抗12の調整によって行うほかに、3端子可
変抵抗器21の可動端子23の抵抗値調整すなわち分圧
比調整によって行うことができる。この調整のために、
例えば検出出力端11,22間に電流計Mを接続し、そ
の電流計Mの振れ(電流値)が零(ゼロ)になるように
ブリッジ抵抗12及び3端子可変抵抗器21の少なくと
も一方の抵抗値を調整する。
In FIG. 1, consider the case of normal operation, that is, the case where the superconducting coil 1 is not quenched.
With the protection switch 15 open, the DC circuit breaker 3
Closed, and a current is passed from the DC power supply 2 to the superconducting coil 1,
The current value is changed. On the other hand, in order to balance the bridge circuit, in addition to the adjustment of the variable bridge resistor 12 through the above-described current adjustment process, the resistance value of the movable terminal 23 of the three-terminal variable resistor 21, that is, the division ratio adjustment is performed. be able to. For this adjustment,
For example, an ammeter M is connected between the detection output terminals 11 and 22, and the resistance of at least one of the bridge resistor 12 and the three-terminal variable resistor 21 is set so that the deflection (current value) of the ammeter M becomes zero. Adjust the value.

【0013】図1の回路構成によれば、ブリッジ抵抗1
2の抵抗値調整によって概略のブリッジ平衡をとり、3
端子可変抵抗器21の分圧点調整によって、電流計Mの
正負の振れを確認しながらブリッジ回路を平衡させるこ
とができる。
According to the circuit configuration of FIG. 1, the bridge resistor 1
By adjusting the resistance value of 2, a rough bridge balance is obtained, and 3
By adjusting the voltage dividing point of the terminal variable resistor 21, the bridge circuit can be balanced while confirming positive and negative swings of the ammeter M.

【0014】次に、超電導コイルに電流を流している状
態で、何らかの原因で超電導コイル1の一部にクエンチ
が発生した場合を考える。例えば、超電導コイル1のコ
イル端5と電圧タップ17との間にクエンチが発生する
と、そのコイル部分に常電導抵抗成分が発生し、常電導
電圧が生じる。この常電導電圧の発生はブリッジ回路の
平衡条件を崩す。この不平衡によって生じた電圧が所定
値以上になった状態が比較的短い所定時間以上継続した
とき、検出出力端11,22間に接続された図示してい
ない保護手段によってクエンチ発生と判断され、クエン
チ検出信号が出力される。
Next, consider a case in which a quench occurs in a part of the superconducting coil 1 for some reason while a current is being applied to the superconducting coil. For example, when a quench occurs between the coil end 5 of the superconducting coil 1 and the voltage tap 17, a normal conducting resistance component is generated in the coil portion, and a normal conducting pressure is generated. The generation of this normal conducting pressure destroys the equilibrium condition of the bridge circuit. When the voltage generated by this imbalance exceeds a predetermined value and continues for a relatively short predetermined time, it is determined that a quench has occurred by a protection means (not shown) connected between the detection output terminals 11 and 22. A quench detection signal is output.

【0015】この検出出力により、保護手段を介して保
護投入用スイッチ15が閉じられ、直流遮断器3が開か
れる。これによって、超電導コイル1に保護抵抗16が
並列に接続され、超電導コイル1の保有磁気エネルギー
は、保護抵抗16を介して時定数=L/(保護抵抗16
の抵抗値) (ただし、Lは超電導コイル1のインダク
タンス)の値で減衰しながら流れる電流のジュール損失
として消費される。このように、クエンチ発生時の電流
が保護抵抗16を介して流れることによって、超電導コ
イル1の保有磁気エネルギーは保護抵抗16によって消
費され、その分だけ超電導コイル1自体でのエネルギー
消費すなわち温度上昇も抑制され、ここに超電導コイル
1を熱破壊から良好に保護することができる。
With this detection output, the protection switch 15 is closed and the DC breaker 3 is opened via the protection means. As a result, the protection resistance 16 is connected in parallel to the superconducting coil 1, and the magnetic energy possessed by the superconducting coil 1 is time constant = L / (protection resistance 16
Resistance value (where L is the inductance of the superconducting coil 1) and is consumed as Joule loss of the flowing current while being attenuated. As described above, since the current at the time of occurrence of quench flows through the protective resistance 16, the magnetic energy possessed by the superconducting coil 1 is consumed by the protective resistance 16, and the energy consumption, that is, the temperature rise in the superconducting coil 1 itself is correspondingly consumed. Suppressed, where the superconducting coil 1 can be well protected from thermal destruction.

【0016】図2に本発明の他の実施例の回路図を示
す。図示のように、この実施例は2つの超電導コイル2
7,28に対して1つのクエンチ検出回路4を設けたも
のである。2つの超電導コイル27,28は接続部26
によって互いに直列接続されている。超電導コイル27
のコイル端30は電圧入力端8に接続され、電圧タップ
31は3端子可変抵抗器21の固定端19に接続されて
いる。同様に超電導コイル28のコイル端33は電圧入
力端10に接続され、電圧タップ32は3端子可変抵抗
器21の固定端20に接続されている。他の構成部分は
図1の実施例と変わりが無い。
FIG. 2 shows a circuit diagram of another embodiment of the present invention. As shown, this embodiment has two superconducting coils 2
One quench detection circuit 4 is provided for 7, 28. The two superconducting coils 27 and 28 have a connecting portion 26
Are connected to each other in series. Superconducting coil 27
The coil end 30 of is connected to the voltage input end 8 and the voltage tap 31 is connected to the fixed end 19 of the three-terminal variable resistor 21. Similarly, the coil end 33 of the superconducting coil 28 is connected to the voltage input end 10, and the voltage tap 32 is connected to the fixed end 20 of the three-terminal variable resistor 21. The other components are the same as in the embodiment of FIG.

【0017】図2のクエンチ検出回路4自体は図1のも
のと何ら変わりが無く、ブリッジ回路平衡のための調整
及びクエンチ検出の原理はすでに述べた図1のものと同
一である。図2のコイル構成の場合であっても、図1の
場合と全く同様にクエンチ検出を行うことができる。
The quench detection circuit 4 itself of FIG. 2 is no different from that of FIG. 1, and the principles of adjustment for bridge circuit balancing and quench detection are the same as those of FIG. 1 already described. Even in the case of the coil configuration of FIG. 2, quench detection can be performed in exactly the same manner as in the case of FIG.

【0018】このように、ブリッジ部に接続する超電導
コイルの部分を任意に変更することができるため、2つ
の超電導コイルのそれぞれの任意のコイル部分に発生す
るクエンチを容易に検出することができる。
As described above, since the portion of the superconducting coil connected to the bridge portion can be arbitrarily changed, the quench generated in the arbitrary coil portion of each of the two superconducting coils can be easily detected.

【0019】[0019]

【発明の効果】本発明によれば、超電導コイルの離れて
いる任意のコイル部分に発生するクエンチを容易に検出
しうるクエンチ検出装置を提供することができる。
According to the present invention, it is possible to provide a quenching detection device capable of easily detecting a quenching which occurs in an arbitrary coil portion of a superconducting coil which is separated.

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

【図1】本発明による超電導コイルのクエンチ検出装置
の一実施例を示す回路図。
FIG. 1 is a circuit diagram showing an embodiment of a quench detecting device for a superconducting coil according to the present invention.

【図2】本発明によるクエンチ検出装置の別の実施例を
示す回路図。
FIG. 2 is a circuit diagram showing another embodiment of the quench detection device according to the present invention.

【図3】従来の超電導コイルのクエンチ検出装置を示す
回路図。
FIG. 3 is a circuit diagram showing a conventional quench detection device for a superconducting coil.

【図4】クエンチ検出の原理を説明するための図。FIG. 4 is a diagram for explaining the principle of quench detection.

【符号の説明】[Explanation of symbols]

1,27,28 超電導コイル 2 直流電源 3 直流遮断器 4 クエンチ検出回路 5,6,30,33 コイル端 8,10 電圧入力端子 11,22 検出出力端子 12,13 ブリッジ抵抗 15 保護投入用スイッチ 16 保護抵抗 17,18,31,32 電圧タップ 19,20 3端子可変抵抗器の固定端子 21 3端子可変抵抗器 23 3端子可変抵抗器の可動端子 1, 27, 28 Superconducting coil 2 DC power supply 3 DC breaker 4 Quench detection circuit 5, 6, 30, 33 Coil end 8, 10 Voltage input terminal 11, 22 Detection output terminal 12, 13 Bridge resistance 15 Protection switch 16 Protection resistor 17,18,31,32 Voltage tap 19,20 Fixed terminal of 3 terminal variable resistor 21 3 terminal variable resistor 23 3 Movable terminal of variable resistor

Claims (3)

【特許請求の範囲】[Claims] 【請求項1】検出対象の超電導コイルから2つの中間タ
ップを導出し、その2つの中間タップ間に3端子可変抵
抗器の固定端子を接続すると共に、前記超電導コイルの
両コイル端間に直列接続の2つのブリッジ抵抗を接続し
て、前記超電導コイル及びブリッジ抵抗によりブリッジ
回路を形成し、前記3端子可変抵抗器の可動端子及び前
記両ブリッジ抵抗の共通接続点を検出出力端とした超電
導コイルのクエンチ検出装置。
1. A two-way tap is derived from a superconducting coil to be detected, a fixed terminal of a three-terminal variable resistor is connected between the two taps, and a series connection is made between both coil ends of the superconducting coil. Of the superconducting coil, in which a bridge circuit is formed by connecting the two bridge resistors of (1) and (2) to the movable terminal of the three-terminal variable resistor and the common connection point of the two bridge resistors. Quench detector.
【請求項2】前記2つのブリッジ抵抗の少なくとも一方
が可変抵抗器である請求項1に記載の超電導コイルのク
エンチ検出装置。
2. The quench detection device for a superconducting coil according to claim 1, wherein at least one of the two bridge resistors is a variable resistor.
【請求項3】前記超電導コイルは構造的に別個の2つの
コイルからなっており、前記中間タップは各コイルの中
間から導出されている請求項1または2に記載の超電導
コイルのクエンチ検出装置。
3. The quench detection device for a superconducting coil according to claim 1, wherein the superconducting coil is composed of two structurally separate coils, and the intermediate tap is led out from the middle of each coil.
JP5317884A 1993-12-17 1993-12-17 Superconductive coil quenching detection device Pending JPH07174803A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5317884A JPH07174803A (en) 1993-12-17 1993-12-17 Superconductive coil quenching detection device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5317884A JPH07174803A (en) 1993-12-17 1993-12-17 Superconductive coil quenching detection device

Publications (1)

Publication Number Publication Date
JPH07174803A true JPH07174803A (en) 1995-07-14

Family

ID=18093133

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5317884A Pending JPH07174803A (en) 1993-12-17 1993-12-17 Superconductive coil quenching detection device

Country Status (1)

Country Link
JP (1) JPH07174803A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2315042A1 (en) * 2009-10-20 2011-04-27 Karlsruher Institut für Technologie Method and device for indirect monitoring of an electric conductance
JP2014229753A (en) * 2013-05-22 2014-12-08 中部電力株式会社 Quench detector and quench detection method of superconducting coil

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
EP2315042A1 (en) * 2009-10-20 2011-04-27 Karlsruher Institut für Technologie Method and device for indirect monitoring of an electric conductance
JP2014229753A (en) * 2013-05-22 2014-12-08 中部電力株式会社 Quench detector and quench detection method of superconducting coil

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