JPH04145603A - Quench detection method of superconductive coil - Google Patents

Quench detection method of superconductive coil

Info

Publication number
JPH04145603A
JPH04145603A JP26833990A JP26833990A JPH04145603A JP H04145603 A JPH04145603 A JP H04145603A JP 26833990 A JP26833990 A JP 26833990A JP 26833990 A JP26833990 A JP 26833990A JP H04145603 A JPH04145603 A JP H04145603A
Authority
JP
Japan
Prior art keywords
quench
coil
superconducting coil
critical current
terminals
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
JP26833990A
Other languages
Japanese (ja)
Inventor
Masanori Yamamoto
山本 雅教
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.)
Takaoka Toko Co Ltd
Original Assignee
Takaoka Electric Mfg Co Ltd
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 Takaoka Electric Mfg Co Ltd filed Critical Takaoka Electric Mfg Co Ltd
Priority to JP26833990A priority Critical patent/JPH04145603A/en
Publication of JPH04145603A publication Critical patent/JPH04145603A/en
Pending legal-status Critical Current

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  • Superconductive Dynamoelectric Machines (AREA)

Abstract

PURPOSE:To prevent burning of a superconductive coil through early detection of quench by providing a part whose critical current is lower than a critical current value to a superconductive coil and by detecting quench generation for the part. CONSTITUTION:When a d.c. current between terminals (a), (b) of a superconductive coil 1 is increased gradually and quenched, a change in resistance is determined from voltages between terminals c and d and between terminals e and f. A resistant element is produced in a part of a superconductive coil 2 when quench is generated and a resistance element of a coil 1 increases gradually. That is, it shows that quench generation is started from a part of the superconductive coil 2; therefore, it is possible to detect quench generation early and to avoid burning and impossibility of operation. The part 2 whose critical current value is set a little low is provided with a small bending radius once using the same superconductive line material as the coil 1 and is provided with distortion hysteresis. A temperature sensor 3 is used for a quench detection sensor.

Description

【発明の詳細な説明】 「産業上の利用分野」 本発明はクエンチの発生を早期に検出できるようにした
超電導コイルに関するものである。
DETAILED DESCRIPTION OF THE INVENTION "Field of Industrial Application" The present invention relates to a superconducting coil that enables early detection of the occurrence of quench.

「従来の技術」 超電導コイルのクエンチ検出については一般的に検討さ
れているが、実際に具体的な方法はまだ確立されておら
ず、本発明のクエンチの早期検出の手段は具体的に実施
した全く新しい技術である。
"Prior art" Although quench detection in superconducting coils has been generally studied, no concrete method has yet been established, and the means for early quench detection of the present invention has not been specifically implemented. This is a completely new technology.

「発明が解決しようとする課題」 超電導コイルは磁界、温度、電流のいずれかでも臨界値
を超過すると常電導状態に転移し、焼損あるいは継続運
転不能の状態になる。
``Problems to be Solved by the Invention'' When a superconducting coil exceeds a critical value in the magnetic field, temperature, or current, it transitions to a normal conductive state, resulting in burnout or a state in which continued operation is impossible.

そのため超電導コイルの使用にあたっては、これらの臨
界値を越えないような条件にしなけらばならないが、こ
のうち磁界、温度については、設定条件に対して比較的
安定に維持できる。しかし電流に対しては、超電導コイ
ルの運用上、外部事故その他の要因によって臨界値を超
過するような過電流が流れる場合がある。
Therefore, when using a superconducting coil, conditions must be set so that these critical values are not exceeded, but the magnetic field and temperature can be maintained relatively stably within the set conditions. However, in the operation of superconducting coils, an overcurrent that exceeds a critical value may flow due to external accidents or other factors.

したがって、この過電流が臨界電流を越えないようにす
るための保護対策を必要とする一方、万一超電導コイル
がクエンチを起こした場合には、超電導コイル側で早期
にこれを検出して、電流遮断その他の処置を施す必要が
ある。
Therefore, while protective measures are required to prevent this overcurrent from exceeding the critical current, in the event that the superconducting coil quenches, this can be detected early on the superconducting coil side and the current It is necessary to shut off or take other measures.

超電導コイルのクエンチ現象はコイル全体に亘って一瞬
に常電導転移するのではなく、ある局部的な部分から発
生して、その局部的な常電導化による抵抗成分の発生に
よって熱損失が生じ、その熱が超電導コイル線材に伝播
し、クエンチを助長進行させる過程を経る。
The quenching phenomenon of superconducting coils does not occur in an instantaneous transition to normal conductivity over the entire coil, but occurs in a certain local part, and heat loss occurs due to the generation of a resistance component due to localized normal conductivity. Heat propagates to the superconducting coil wire and undergoes a process that promotes quenching.

クエンチ発生の検出が遅れ、電流遮断などの保護対策が
遅れた場合には、最初のクエンチ発生点が特に大きな損
傷を受け、場合によってはその部分から焼損に至る。
If the detection of quench occurrence is delayed and protective measures such as cutting off the current are delayed, the point where the first quench occurs will be particularly severely damaged, and in some cases, that area will be burnt out.

そのため、クエンチ発生の検出を早期にして、かつ早期
の保護対策を講するゼ・要がある。しかしながら超電導
コイルのクエンチ発生点は不明であり、そのクエンチ検
出センサの取り付は位置も明解でないために、任意の位
置に取り付けたセンサの応答では遅い場合がある。
Therefore, it is necessary to detect the occurrence of quenching early and to take early protective measures. However, the quench generation point of the superconducting coil is unknown, and the mounting position of the quench detection sensor is also not clear, so the response of a sensor mounted at an arbitrary position may be slow.

本発明は、このようなセンサの応答の遅れを解決するた
めに新しい手段を提供するものである。
The present invention provides a new means for solving this delay in sensor response.

「課題を解決するための手段」 本発明を第1図に基づいて説明する。第1図において、
1は超電導コイル、2は超電導コイル1のクエンチ発生
点の起点とするために超電導コイル1の臨界電流値より
やや低い臨界電流値となるようにした超電導コイル1の
一部分、3はクエンチの発生を検出するためのセンサで
、上述の2の近傍に取り付けである。
"Means for Solving the Problems" The present invention will be explained based on FIG. 1. In Figure 1,
1 is a superconducting coil, 2 is a part of the superconducting coil 1 whose critical current value is slightly lower than the critical current value of the superconducting coil 1 in order to use it as the starting point of the quench generation point of the superconducting coil 1, and 3 is a part of the superconducting coil 1 that is set to have a critical current value slightly lower than the critical current value of the superconducting coil 1. This is a sensor for detection and is installed near the above-mentioned 2.

以上の構成において、超電導コイル1にその臨界電流を
越えるような過電流が発生した場合には、最初に超電導
コイルの2の部分からクエンチが発生するので、検出セ
ンサの応答遅れが少なく、クエンチの検出が早期にでき
る。
In the above configuration, when an overcurrent that exceeds its critical current occurs in superconducting coil 1, quenching occurs first in section 2 of superconducting coil, so there is less delay in the response of the detection sensor, and the quenching Detection can be done early.

この超電導コイルの2の部分の構成として、超電導コイ
ル1を形成させるときに、線材に局所的に他より強い曲
げストレスを与えておく、異なる線材を接続する、冷却
効果を悪くしておく、磁界を与えておく、などの方法に
よって可能である。
The structure of the second part of this superconducting coil is that when forming the superconducting coil 1, the wire rods are locally subjected to stronger bending stress than others, different wire rods are connected, the cooling effect is deteriorated, and the magnetic field is This can be done by giving the following information.

「作用」 本発明の作用を第1図および第2図に基づいて説明する
"Operation" The operation of the present invention will be explained based on FIGS. 1 and 2.

第1図においてaおよびbは超電導コイル1の端子、c
、d、e、fは超電導コイルに流れる電流によって、超
電導コイル線材に発生する電圧を計測するために設けた
端子であり、C,d間は超電導コイル1のクエンチ発生
の起点となるように構成した部分2に発生する電圧を計
測するための端子、e、fは上記2以外の超電導コイル
1の全体に発生する電圧を計測するための端子である。
In FIG. 1, a and b are terminals of superconducting coil 1, and c
, d, e, and f are terminals provided to measure the voltage generated in the superconducting coil wire by the current flowing through the superconducting coil, and the terminal between C and d is configured to be the starting point of quenching of the superconducting coil 1. Terminals e and f are terminals for measuring the voltage generated in the superconducting coil 1 other than the portion 2 mentioned above.

なお、これらのc、d、e、fの端子は上記2の部分が
クエンチ発生の起点となるかどうかの作用を確認するた
めに設けたものであり、通常は必要としない。
Note that these terminals c, d, e, and f are provided to confirm whether or not the above-mentioned portion 2 serves as a starting point for quench generation, and are normally not required.

第2図は第1図に示す端子a、bより直流電流を徐々に
増加させながらクエンチを発生させたときの端子c、d
及びe、fそれぞれに発生する電圧より抵抗値変化に換
算して表した曲線である。
Figure 2 shows terminals c and d when a quench is generated while gradually increasing the DC current from terminals a and b shown in Figure 1.
, and is a curve expressed by converting the voltage generated at each of e and f into a change in resistance value.

第2図において、1および2はそれぞれ第1図の端子c
、dおよびe、f間に発生する抵抗変化を示す。なお、
ここで電流を徐々に増加させているので超電導コイルの
もつインタフタンスと電流変化に基ずく逆起電力はほと
んど計測されない。
In FIG. 2, 1 and 2 are terminals c in FIG. 1, respectively.
, d and shows the resistance change occurring between e and f. In addition,
Since the current is gradually increased here, the interface of the superconducting coil and the back electromotive force based on current changes are hardly measured.

第2図に示す通り、超電導コイルがクエンチを起した時
点において、最初に超電導コイルの2の部分に抵抗成分
が発生し、次に超電導コイルの1の部分の抵抗成分が暫
時増大して行くのが分かる。
As shown in Figure 2, at the point when the superconducting coil quenches, a resistance component is first generated in part 2 of the superconducting coil, and then a resistance component in part 1 of the superconducting coil increases for a while. I understand.

この曲線1.2の抵抗発生の立ち上がり部分の時間差は
、第1図の端子dとeの取り付は位置によって変わるが
、dおよびeが同一点であっても、おおむね第2図に示
す曲線となる。すなわち、これは明らかにクエンチ発生
が超電導コイルの2の部分を起点として生じていること
を示し、これによりクエンチ発生の検出を早期に行える
ことを可能としている。
The time difference between the rising parts of the resistance generation in curve 1.2 will vary depending on the position of the terminals d and e in Figure 1, but even if d and e are at the same point, the time difference between the rising parts of the resistance generation will generally be the same as the curve shown in Figure 2. becomes. That is, this clearly shows that the quench occurs starting from the second part of the superconducting coil, and this makes it possible to detect the quench at an early stage.

「実施例」 本発明の実施例を第1図に基づいて説明する。"Example" An embodiment of the present invention will be described based on FIG.

超電導コイル1の臨界電流値をやや低めに設定する部分
2として、超電導コイル1と同じ超電導線材を用いてコ
イル巻線作業時に一旦より小さな曲げ半径としたストレ
スを与えた履歴を持たせた部分として形成している。こ
の構成によって、超電導コイルはストレスを与えない場
合に比べて、やや性能が低くなると考えられる。しかし
、クエンチによる焼損防止のために非常に効果的な方法
となっている。また、クエンチ検出センサとして温度セ
ンサを用いた例である。
Part 2 sets the critical current value of superconducting coil 1 to be slightly lower, and is part 2 that has a history of applying stress to a smaller bending radius during coil winding work using the same superconducting wire as superconducting coil 1. is forming. Due to this configuration, the performance of the superconducting coil is considered to be slightly lower than when stress is not applied. However, this is a very effective method for preventing burnout due to quenching. This is also an example in which a temperature sensor is used as the quench detection sensor.

「発明の効果」 以上説明したように、超電導コイルは臨界電流値以上の
過電流てクエンチし、高抵抗コイルに急変し、焼損また
は継続運転不能の状態になる危険性がある。そのため、
超電導コイルは早期にクエンチを検出して保護対策を講
する必要がある。しかし、超電導コイルの局部的に発生
した段階のクエンチを早期に検出して、保護対策を講す
ることは困難であった。
"Effects of the Invention" As explained above, a superconducting coil quenches when an overcurrent exceeds a critical current value, suddenly changes to a high-resistance coil, and there is a risk of burning out or becoming unable to continue operation. Therefore,
It is necessary to detect quenching of superconducting coils early and take protective measures. However, it has been difficult to early detect locally generated quench in superconducting coils and take protective measures.

直流用超電導コイルで電流変化の少ない場合は、コイル
全体の抵抗成分を検出して行うことができる場合がある
が、特に交流用超電導コイルの場合はその手段を用いる
ことができないので、特にクエンチ発生の検出が遅れる
ことが多い。
If the current changes are small in a DC superconducting coil, it may be possible to detect the resistance component of the entire coil, but this method cannot be used especially in the case of an AC superconducting coil, so it is especially difficult to detect quench occurrence. Detection is often delayed.

本発明の方法は、直流用にも交流用にも応用でき、早期
にクエンチの発生を検出できるようにしたもので超電導
コイルの保護対策上非常に効果がある方法である。
The method of the present invention can be applied to both direct current and alternating current applications, and enables early detection of the occurrence of quench, making it a very effective method for protecting superconducting coils.

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

第1図は本発明の詳細な説明するための説明図、第2図
は第1図の超電導コイルがクエンチを生じた場合の抵抗
成分発生の変化を示した図である。 第1図において、1は超電導コイル、2は超電導コイル
1の臨界電流値よりやや低い臨界電流値をもたせるよう
にした超電導コイル1の一部分、3はクエンチ検出用セ
ンサ、a、bは超電導コイルの端子、C,dおよびe、
fはそれぞれ超電導コイルの2の部分および超電導コイ
ル1の部分の電圧を計測するための端子である。 第2図において、1および2はそれぞれ第1図のc、d
およびe、f間に発生した抵抗成分の変化を示す曲線で
ある。 特許出願人 株式会社 高岳製作所 第1図 → 時間 第2図
FIG. 1 is an explanatory diagram for explaining the present invention in detail, and FIG. 2 is a diagram showing changes in resistance component generation when the superconducting coil of FIG. 1 quenches. In Fig. 1, 1 is a superconducting coil, 2 is a part of the superconducting coil 1 which has a critical current value slightly lower than the critical current value of the superconducting coil 1, 3 is a quench detection sensor, and a and b are superconducting coils. terminals, C, d and e;
f is a terminal for measuring the voltage of the superconducting coil 2 part and the superconducting coil 1 part, respectively. In Figure 2, 1 and 2 are c and d in Figure 1, respectively.
and a curve showing a change in the resistance component occurring between e and f. Patent applicant: Takatake Seisakusho Co., Ltd. Figure 1 → Time diagram 2

Claims (1)

【特許請求の範囲】[Claims]  超電導コイルに当該超電導コイルの臨界電流値より低
い臨界電流を有する部分を形成させ、この臨界電流値の
低い部分についてクエンチ発生検出を行うことによつて
、コイル全体がクエンチに至らない前に早期にクエンチ
検出を可能とした超電導コイルのクエンチ検出方式。
By forming a part in the superconducting coil that has a critical current lower than the critical current value of the superconducting coil, and detecting the occurrence of quenching in this part with a low critical current value, it is possible to quickly detect the occurrence of quench before the entire coil reaches quench. A quench detection method for superconducting coils that enables quench detection.
JP26833990A 1990-10-08 1990-10-08 Quench detection method of superconductive coil Pending JPH04145603A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP26833990A JPH04145603A (en) 1990-10-08 1990-10-08 Quench detection method of superconductive coil

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP26833990A JPH04145603A (en) 1990-10-08 1990-10-08 Quench detection method of superconductive coil

Publications (1)

Publication Number Publication Date
JPH04145603A true JPH04145603A (en) 1992-05-19

Family

ID=17457171

Family Applications (1)

Application Number Title Priority Date Filing Date
JP26833990A Pending JPH04145603A (en) 1990-10-08 1990-10-08 Quench detection method of superconductive coil

Country Status (1)

Country Link
JP (1) JPH04145603A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010010632A (en) * 2008-06-30 2010-01-14 Toshiba Corp Superconducting coil
JP2017028154A (en) * 2015-07-24 2017-02-02 古河電気工業株式会社 High temperature superconducting coil

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6344710A (en) * 1986-08-12 1988-02-25 Toshiba Corp Quenching detection device for superconductive coil

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS6344710A (en) * 1986-08-12 1988-02-25 Toshiba Corp Quenching detection device for superconductive coil

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010010632A (en) * 2008-06-30 2010-01-14 Toshiba Corp Superconducting coil
JP2017028154A (en) * 2015-07-24 2017-02-02 古河電気工業株式会社 High temperature superconducting coil

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