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JPH04207923A - Current limiting method and current limiting device - Google Patents

Current limiting method and current limiting device

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Publication number
JPH04207923A
JPH04207923A JP32904790A JP32904790A JPH04207923A JP H04207923 A JPH04207923 A JP H04207923A JP 32904790 A JP32904790 A JP 32904790A JP 32904790 A JP32904790 A JP 32904790A JP H04207923 A JPH04207923 A JP H04207923A
Authority
JP
Japan
Prior art keywords
current
superconducting
current limiting
limiting element
circuit
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
JP32904790A
Other languages
Japanese (ja)
Inventor
Takashi Sato
隆 佐藤
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP32904790A priority Critical patent/JPH04207923A/en
Publication of JPH04207923A publication Critical patent/JPH04207923A/en
Pending legal-status Critical Current

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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】 〔産業上の利用分野〕 本発明は、限流方法及び限流装置、すなわち、規定以上
の電流が回路に流れた時に電流を制限し。
DETAILED DESCRIPTION OF THE INVENTION [Industrial Application Field] The present invention relates to a current limiting method and a current limiting device, that is, a current limiting device that limits the current when a current exceeding a specified value flows through a circuit.

回路を保護するのに用いられる限流方法及び限流装置及
び限流遮断器に関する。
The present invention relates to a current limiting method, current limiting device, and current limiting circuit breaker used to protect a circuit.

〔従来の技術〕[Conventional technology]

超電導限流素子を用いた限流装置は超電導限流素子を超
電導状態から常電導状態に転移させることにより抵抗値
を上昇し、過電流を制限するもので、例えば、第7図に
特開昭63−307635号公報に示されている従来の
限流装置の構成を示す。
A current limiting device using a superconducting current limiting element increases the resistance value and limits overcurrent by transferring the superconducting current limiting element from a superconducting state to a normal conducting state. 63-307635, the configuration of a conventional current limiting device is shown.

図において、3は超電導物質、例えば、Y−Ba−Cu
−○系セラミックスで作られた超電導限流素子であって
、その両端には端子1,2を備えており、超電導限流素
子3の全長は常電導状態になったときには十分な限流が
できる抵抗値をもち、かつ、超電導状態にあっては定格
電流を流すのに十分な断面積をもつ大きさをしている。
In the figure, 3 is a superconducting material, such as Y-Ba-Cu.
- It is a superconducting current limiting element made of ○ series ceramics, and has terminals 1 and 2 at both ends, and the total length of the superconducting current limiting element 3 can provide sufficient current limiting when in a normal conduction state. It has a resistance value and is sized to have a cross-sectional area sufficient to flow the rated current when in a superconducting state.

端子1には電流検出用の計測用変圧器4が取り付けられ
、その信号によって磁場発生用コイル6a。
A measuring transformer 4 for detecting current is attached to the terminal 1, and its signal causes a magnetic field generating coil 6a to be activated.

6b、6cに時間遅れをもって電流を流す制御部5を備
えている。
A control section 5 is provided that causes current to flow through 6b and 6c with a time delay.

このように構成された従来の限流装置15に過電流を通
じると、計測用変圧器4の信号を受けた制御部5は時刻
をずらして、磁場発生用コイル6a、6b、6cに電流
を流す。この結果、コイル6a、6b、6cにそれぞれ
囲まれた超電導限流素子3の領域16a、16b、16
cに臨界磁場以上の磁場が印加され、超電導状態が崩れ
て常電導状態に転移し、各領域に対応して端子1,2及
び超電導限流素子3よりなる通電路にそれぞれ抵抗が生
じる。
When an overcurrent is passed through the conventional current limiting device 15 configured as described above, the control unit 5 receives the signal from the measuring transformer 4 and shifts the time to apply current to the magnetic field generating coils 6a, 6b, 6c. Flow. As a result, the regions 16a, 16b, 16 of the superconducting current limiting element 3 surrounded by the coils 6a, 6b, 6c, respectively
A magnetic field equal to or higher than the critical magnetic field is applied to c, the superconducting state collapses and transitions to a normal conducting state, and resistance is generated in the current-carrying path consisting of the terminals 1, 2 and the superconducting current-limiting element 3 corresponding to each region.

各コイルに流れる電流を時間をずらして与えることによ
り、電流は徐々に限流される。
By applying current to each coil at different times, the current is gradually limited.

このように、各コイルに流れる電流を与える時間を任意
に設定する事により、適用する回路条件にとって、最適
な限流特性を得ることができ、かつ、サージ電圧を発生
しない限流装置を得るものである。
In this way, by arbitrarily setting the time for applying the current to each coil, it is possible to obtain the optimum current-limiting characteristics for the applied circuit conditions, and to obtain a current-limiting device that does not generate surge voltage. It is.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

上記従来技術は超電導限流素子を数多くの領域に分けて
それぞれ転移させるために、電流検品用の計測用変圧器
、制御部、磁場発生用コイルが必要であり、装置の構成
が複雑になり、かつ、動作信頼性が低いという問題があ
った。
The conventional technology described above requires a measuring transformer for current inspection, a control unit, and a magnetic field generation coil in order to divide the superconducting current-limiting element into many areas and transfer them to each area, making the device configuration complicated. In addition, there was a problem of low operational reliability.

また、超電導限流素子のある一領域が常電導状態に転移
すると、その領域のジュール熱で、他の領域が臨界温度
に達してしまい、常電導状態への転移が波及してしまう
結果、段階的な限流を行うのが難しいという問題もあっ
た。
In addition, when one region of a superconducting current limiting element transitions to a normal conducting state, the Joule heat in that region causes other regions to reach a critical temperature, and as a result of the transition to a normal conducting state, the stage There was also the problem that it was difficult to perform effective current limiting.

本発明の目的は、動作信頼性が高く、限流特性を自在に
設定できる限流装置を提供することにある。
An object of the present invention is to provide a current limiting device that has high operational reliability and can freely set current limiting characteristics.

〔課題を解決するための手段〕[Means to solve the problem]

上記目的を達成するために、本発明は常時、電流を通じ
る超電導限流素子からなる主回路に過電流が流れたとき
に主回路中の超電導限流素子が常電導状態に転移し、主
回路を流れる過電流を限流した後、複数段の転流回路に
順次転流させることによって、上記過電流を段階的に限
流する限流方法により限流するものである。
In order to achieve the above object, the present invention provides that when an overcurrent flows through a main circuit consisting of a superconducting current limiting element through which current flows, the superconducting current limiting element in the main circuit is transferred to a normal conducting state, and the main circuit After limiting the overcurrent flowing through the motor, the current is limited by a current limiting method in which the overcurrent is limited in stages by sequentially commutating the current through a plurality of stages of commutation circuits.

また、このために、超電導限流素子からなる主回路と、
超電導限流素子とインピーダンスの直列にしてなる少な
くとも一段の転流回路と、インピーダンスのみからなる
転流回路より限流装置を構成したものである。
In addition, for this purpose, a main circuit consisting of a superconducting current limiting element,
A current limiting device is constructed from at least one stage of commutation circuit consisting of a superconducting current limiting element and an impedance in series, and a commutation circuit consisting only of impedance.

〔作用〕[Effect]

本発明において、主回路の超電導限流素子は通常、超電
導状態に保たれており、過電流が流れると常電導状態に
転移し、過電流を限流して転流回路に転流する。
In the present invention, the superconducting current limiting element of the main circuit is normally kept in a superconducting state, and when an overcurrent flows, it changes to a normal conducting state, limits the overcurrent, and commutates to the commutation circuit.

転流回路では転流されてきた電流をインピーダンスによ
って限流し、電流がさらに増加すると転流回路中の超電
導限流素子が常電導状態に転移して電流を限流すると共
に、次段の転流回路に転流する。
In the commutation circuit, the commutated current is limited by impedance, and when the current increases further, the superconducting current limiting element in the commutation circuit transitions to a normal conduction state, limiting the current, and starting the next stage of commutation. Commutates into the circuit.

このように、電流測定用の計測用変圧器、制御部、磁場
発生用コイルを用いずに簡単な構成で動作信頼性が高く
、また、各転流回路ごとにインピーダンスを設定するこ
とができるため、限流特性を自在に設定することができ
る。
In this way, it has a simple configuration and high operational reliability without using a measuring transformer for current measurement, a control unit, or a magnetic field generation coil, and the impedance can be set for each commutation circuit. , current-limiting characteristics can be set freely.

〔実施例〕〔Example〕

以下、本発明の一実施例を添付図面について説明する。 Hereinafter, one embodiment of the present invention will be described with reference to the accompanying drawings.

第1図は本発明の一実施例を示す回路図である。FIG. 1 is a circuit diagram showing an embodiment of the present invention.

図中、3aは超電導物質、例えば、Y−Ba−Cu−0
系セラミツクスで作られた超電導限流素子であって、そ
の両端には端子1.2を備えている。超電導限流素子3
aは超電導状態で定格電流を流すのに十分な断面積をも
ち、常電導状態で抵抗体7aよりも抵抗値が十分大きく
なる特性をもつ。超電導限流素子3aには抵抗体7aと
第2の超電導限流素子3bからなる転流回路が接続され
ている。超電導限流素子3bは超電導状態で求める制限
電流値の電流を流すのに十分な断面積をもち、常電導状
態で抵抗体7bよりも抵抗値が十分大きくなる特性をも
つ。超電導限流素子3bの両端には抵抗体7bからなる
転流回路が接続されている。
In the figure, 3a is a superconducting material, for example, Y-Ba-Cu-0
This is a superconducting current limiting element made of ceramics, and has terminals 1.2 at both ends. Superconducting current limiting element 3
A has a cross-sectional area sufficient to allow the rated current to flow in a superconducting state, and has a characteristic that its resistance value is sufficiently larger than that of the resistor 7a in a normal conducting state. A commutation circuit consisting of a resistor 7a and a second superconducting current limiting element 3b is connected to the superconducting current limiting element 3a. The superconducting current-limiting element 3b has a cross-sectional area sufficient to flow a current of the limiting current value determined in a superconducting state, and has a characteristic that its resistance value is sufficiently larger than that of the resistor 7b in a normal-conducting state. A commutation circuit consisting of a resistor 7b is connected to both ends of the superconducting current limiting element 3b.

次にこの回路の動作を説明する。通常、電流は超電導限
流素子3aを通じて流れている。このとき超電導限流素
子3aは超電導状態にあるため、端子1〜超電導限流素
子38〜端子2を通電路として流れる回路電流は何ら抵
抗を受けない。次に超電導限流素子3aの臨界電流に相
当する過電流がこの通電路を流れると、超電導限流素子
3aの超電導状態が崩れ常電導状態に転移する。その結
果、通電路を流れる過電流は制限され、合わせて超電導
限流素子3aの抵抗が抵抗体7aの抵抗より十分に大き
くなるため、電流は抵抗体7aと超電導限流素子3bか
らなる転流回路に転流され、抵抗体7aにより限流され
る。この時、電流は主に端子1〜抵抗体7a〜超電導限
流素子3b〜端子2なる第二の通電路を流れる。また、
この時点で超電導限流素子3bは超電導状態にあるため
、回路に何ら影響しない。次に、第二の通電路を流゛れ
る電流が徐々に大きくなり、超電導限流素子3bの臨界
電流に達すると超電導限流素子3bの超電導状態は崩れ
、常電導状態に転移し、抵抗値が上昇する。その結果、
第二の通電路を流れる電流は限流され、合わせて超電導
限流素子3bの抵抗値が抵抗体7bの抵抗値より十分に
大きくなるため、電流は抵抗体7bに転流され、この時
、電流は主に端子1〜抵抗体78〜抵抗体7b〜端子2
なる第三の通電路を流れる。
Next, the operation of this circuit will be explained. Normally, current flows through the superconducting current limiting element 3a. At this time, since the superconducting current-limiting element 3a is in a superconducting state, the circuit current flowing through the terminal 1 to the superconducting current-limiting element 38 to the terminal 2 as a conduction path is not subjected to any resistance. Next, when an overcurrent corresponding to the critical current of the superconducting current limiting element 3a flows through this current path, the superconducting state of the superconducting current limiting element 3a collapses and transitions to a normal conducting state. As a result, the overcurrent flowing through the current-carrying path is limited, and the resistance of the superconducting current-limiting element 3a becomes sufficiently larger than the resistance of the resistor 7a, so that the current is commutated between the resistor 7a and the superconducting current-limiting element 3b. The current is commutated to the circuit, and the current is limited by the resistor 7a. At this time, the current mainly flows through the second current path consisting of terminal 1 - resistor 7a - superconducting current limiting element 3b - terminal 2. Also,
At this point, the superconducting current limiting element 3b is in a superconducting state, so it does not affect the circuit at all. Next, the current flowing through the second current-carrying path gradually increases, and when it reaches the critical current of the superconducting current-limiting element 3b, the superconducting state of the superconducting current-limiting element 3b collapses, transitions to a normal conducting state, and the resistance value rises. the result,
The current flowing through the second current-carrying path is limited, and the resistance value of the superconducting current-limiting element 3b becomes sufficiently larger than the resistance value of the resistor 7b, so the current is commutated to the resistor 7b, and at this time, The current mainly flows from terminal 1 to resistor 78 to resistor 7b to terminal 2.
The current flows through the third current-carrying path.

このように通電路の抵抗値が増大するため、過電流は徐
々に限流され、図示しない回路遮断器の動作によって電
気回路は開路され、電流は遮断されて、超電導限流素子
3a、3bは超電導状態に転移し、回路は初期状態に戻
る。
As the resistance value of the current-carrying path increases in this way, the overcurrent is gradually limited, and the electric circuit is opened by the operation of a circuit breaker (not shown), the current is interrupted, and the superconducting current-limiting elements 3a and 3b It transitions to a superconducting state and the circuit returns to its initial state.

第7図にこのような変化を示す第1図の回路の通電電流
の変化の例を縦軸に通電電流、横軸に時間をとって示す
。第7図中−点鎖線10は限流装置が無い場合に流れる
過電流を示し、Icl。
FIG. 7 shows an example of a change in the conduction current of the circuit of FIG. 1 showing such a change, with the vertical axis representing the conduction current and the horizontal axis representing time. In FIG. 7, the dashed line 10 indicates the overcurrent flowing in the absence of a current limiting device, Icl.

■c2は超電導限流素子3a、3bの臨界電流を示す。(2) c2 indicates the critical current of the superconducting current limiting elements 3a and 3b.

また、横軸中tl、t2はそれぞれ超電導限流素子3a
、3bが転移する時間を示す。
In addition, tl and t2 on the horizontal axis are superconducting current limiting elements 3a, respectively.
, 3b shows the transition time.

第8図には、第7図に対応して、第1図に示した回路の
通電路抵抗の変化の例を縦軸に通電路抵抗、横軸に時間
をとって示す。図中曲線12は通電路抵抗特性、tl、
t2は第7図に対応して超電導限流素子3a、3bが転
移する時間を示す。
Corresponding to FIG. 7, FIG. 8 shows an example of a change in current-carrying path resistance of the circuit shown in FIG. 1, with the vertical axis representing the current-carrying path resistance and the horizontal axis representing time. Curve 12 in the figure is the current path resistance characteristic, tl,
t2 indicates the time during which the superconducting current limiting elements 3a and 3b transition, corresponding to FIG.

このように、超電導限流素子で一端、過電流を限流した
後に転流回路に電流を転流し、転流回路中の抵抗で主た
る限流を行わせるため、簡単な構成で、動作信頼性が高
く、また各抵抗の抵抗値を適切に選ぶことにより、適用
する回路条件にとって最適な限流特性を実現でき、サー
ジ電圧を発生しない限流装置が得られる。
In this way, the superconducting current limiting element first limits the overcurrent, and then the current is commutated to the commutation circuit, and the resistance in the commutation circuit performs the main current limiting, which improves operational reliability with a simple configuration. By appropriately selecting the resistance value of each resistor, it is possible to realize current-limiting characteristics that are optimal for the applied circuit conditions, and to obtain a current-limiting device that does not generate surge voltage.

なお、本実施例において、抵抗体7aに生じるジュール
熱を超電導限流素子3bに作用させることにより、超電
導限流素子3bを常電導状態へ転移させる機能を持たせ
ることもできる。
In this embodiment, the superconducting current-limiting element 3b can also be provided with a function of transitioning to a normal conductive state by causing Joule heat generated in the resistor 7a to act on the superconducting current-limiting element 3b.

第2図は、本発明のもう一つの実施例を示す回路図であ
る。これは、第1図に示す回路中の超電導限流素子と直
列にスイッチ17a、17bを接続したものである。こ
の回路の動作は次のとおりである。始め、スイッチ17
a、17bは投入されている。第一の通電路すなわち端
子1〜スイツチ17a〜超電導限流素子38〜端子2を
通して流れる電流は超電導限流素子3aが超電導状態に
あるため何ら抵抗を受けない。次に、超電導限流素子3
aの臨界電流に相当する過電流が第一の通電路を流れる
と超電導限流素子3aは常電導状態に転移し、抵抗が上
昇する。その結果、通電路を流れる過電流は制限され、
合わせて超電導限流素子3aの抵抗が抵抗体7aの抵抗
より十分に大きくなるため、電流は抵抗体7aとスイッ
チ17b、超電導限流素子3bからなる第二の通電路に
転流され、抵抗体7aにより限流される。これと同時に
スイッチ17aを開くと、常電導状態に転移した超電導
限流素子3aに流れる電流は遮断され、電流は第二の通
電路のみに流れることになり、超電導限流素子3aの損
傷を防ぐことができる。次に第二の通電路を流れる電流
が徐々に大きくなり超電導限流素子3bの臨界電流に達
すると、超電導限流素子3bは常電導状態に転移し、抵
抗値が上昇する。その結果、超電導限流素子3bを流れ
る電流は制限され、合わせて超電導限流素子3bの抵抗
が抵抗体7bの抵抗より十分に大きくなるため、電流は
抵抗体7bに転流される。これと同時に第二の通電路中
のスイッチ17bを開くと、常電導状態に転移した超電
導限流素子3bに流れる電流は遮断され、制限された電
流は抵抗体7bのみに流れることになり、常電導状態に
転移した超電導限流素子3bの損傷を防ぐことができる
FIG. 2 is a circuit diagram showing another embodiment of the present invention. This has switches 17a and 17b connected in series with the superconducting current limiting element in the circuit shown in FIG. The operation of this circuit is as follows. Start, switch 17
a and 17b are inserted. The current flowing through the first energizing path, that is, terminal 1 - switch 17a - superconducting current limiting element 38 - terminal 2 is not subjected to any resistance because superconducting current limiting element 3a is in a superconducting state. Next, superconducting current limiting element 3
When an overcurrent corresponding to the critical current a flows through the first current path, the superconducting current limiting element 3a transitions to a normal conductive state and its resistance increases. As a result, the overcurrent flowing through the current-carrying path is limited,
In addition, since the resistance of the superconducting current-limiting element 3a becomes sufficiently larger than the resistance of the resistor 7a, the current is diverted to the second current-carrying path consisting of the resistor 7a, the switch 17b, and the superconducting current-limiting element 3b, and the current is passed through the resistor. The current is limited by 7a. When the switch 17a is opened at the same time, the current flowing through the superconducting current-limiting element 3a that has transitioned to the normal conductive state is cut off, and the current flows only through the second current-carrying path, thereby preventing damage to the superconducting current-limiting element 3a. be able to. Next, when the current flowing through the second current-carrying path gradually increases and reaches the critical current of the superconducting current-limiting element 3b, the superconducting current-limiting element 3b transitions to a normal conductive state and its resistance value increases. As a result, the current flowing through the superconducting current-limiting element 3b is restricted, and the resistance of the superconducting current-limiting element 3b becomes sufficiently larger than the resistance of the resistor 7b, so that the current is commutated to the resistor 7b. At the same time, when the switch 17b in the second current-carrying path is opened, the current flowing through the superconducting current-limiting element 3b that has transitioned to the normal conductive state is cut off, and the limited current flows only through the resistor 7b. Damage to the superconducting current limiting element 3b that has transitioned to a conductive state can be prevented.

このように超電導限流素子と直列にスイッチを接続する
と、常電導状態に転移した超電導限流素子を流れる電流
を遮断することによって超電導限流素子の損傷を防ぎ、
合わせて確実に段階的な限流を可能とできる。
When a switch is connected in series with a superconducting current-limiting element in this way, it prevents damage to the superconducting current-limiting element by cutting off the current flowing through the superconducting current-limiting element that has transitioned to a normal conducting state.
In addition, it is possible to reliably limit the current in stages.

第3図は、本発明の第三の実施例を示す回路図である。FIG. 3 is a circuit diagram showing a third embodiment of the present invention.

これは第1図に示す回路中の抵抗体7a。This is the resistor 7a in the circuit shown in FIG.

7bをコイル6a、6bに置き換えたもので、コイルの
インダクタンスにより、第1図に示す回路と同様の作用
効果を示すものである。
7b is replaced with coils 6a and 6b, and due to the inductance of the coils, it exhibits the same effect as the circuit shown in FIG. 1.

改めて図示するまでもなく、コイル6aに抵抗体を直列
に接続し、コイルと抵抗体の両者で限流させる事も可能
であり、また、コイル6aのみを抵抗体に置き換えるよ
うなインピーダンスの選び方も考えられる。すなわち、
各限流インピーダンスは抵抗体とコイルのうち、少なく
とも、いずれか一方によって構成されていれば良い。
Needless to illustrate again, it is also possible to connect a resistor in series to the coil 6a and limit the current with both the coil and the resistor, and it is also possible to select the impedance by replacing only the coil 6a with a resistor. Conceivable. That is,
Each current-limiting impedance may be composed of at least one of a resistor and a coil.

第4図は、本発明の第四の実施例を示す回路図である。FIG. 4 is a circuit diagram showing a fourth embodiment of the present invention.

本実施例はコイル6a、6bに生ずる磁場を超電導限流
素子3b、3cに印加して臨界磁場を越えさせる事によ
っても常電導状態に転移させる事のできるものであり、
三段階に転流及び限流を行い、且つ、超電導限流素子の
損傷を防ぐために直列スイッチを備えた例である。本構
成によれば、臨界磁場、臨界電流の二通りの手段によっ
て超電導限流素子を転移させ得るため、限流特性の設定
の自由度が非常に高くなるものである。
In this embodiment, the magnetic field generated in the coils 6a, 6b is applied to the superconducting current limiting elements 3b, 3c to exceed the critical magnetic field, thereby making it possible to transition to the normal conductive state.
This is an example in which commutation and current limiting are performed in three stages, and a series switch is provided to prevent damage to the superconducting current limiting element. According to this configuration, the superconducting current limiting element can be transferred by two means, a critical magnetic field and a critical current, so the degree of freedom in setting the current limiting characteristics is greatly increased.

次に第5図に本発明の第五の他の実施例を示す。Next, FIG. 5 shows a fifth other embodiment of the present invention.

この場合、第1図に示した実施例が二段階に限流と転流
を行わせるのに対して、三段階の限流と転流を行わせる
もので、通電路の抵抗変化特性を第1図に示す回路に比
べてより細かく設定することができる。
In this case, whereas the embodiment shown in Fig. 1 performs current limiting and commutation in two stages, current limiting and commutation are performed in three stages, and the resistance change characteristics of the current carrying path are changed in the first stage. Compared to the circuit shown in FIG. 1, more detailed settings can be made.

次に第6図に本発明の第六の他の実施例を示す。Next, FIG. 6 shows a sixth other embodiment of the present invention.

この場合、四段階の限流と転流を行わせるもので、第6
図に示す回路の方が第5図に示す回路よりもより細かく
抵抗変化特性を設定することができる。
In this case, current limiting and commutation are performed in four stages, and the sixth
The circuit shown in the figure allows the resistance change characteristics to be set more finely than the circuit shown in FIG.

〔発明の効果〕〔Effect of the invention〕

本発明は、常時電流を通ずる超電導限流素子からなる主
回路と、超電導限流素子とインピーダンスの直列にして
なる少なくとも一段の転流回路と、インピーダンスのみ
からなる転流回路より構成される。そのため、過電流は
超電導限流素子で一端限流された後、転流回路に転流し
て、転流回路中のインピーダンスで限流されるが、転流
回路が数段接続されているため徐々に限流される。また
The present invention is comprised of a main circuit consisting of a superconducting current-limiting element that constantly conducts current, at least one stage of commutation circuit consisting of the superconducting current-limiting element and an impedance in series, and a commutation circuit consisting only of impedance. Therefore, after the overcurrent is limited at one end by the superconducting current limiting element, it is commutated to the commutation circuit and is limited by the impedance in the commutation circuit, but since the commutation circuit is connected in several stages, it gradually Current is limited. Also.

各転流回路のインピーダンスを適切に選択することで限
流特性を変更することができる。
Current-limiting characteristics can be changed by appropriately selecting the impedance of each commutation circuit.

これにより、電流測定用の計測用変圧器、制御部、磁場
発生用コイルを用いずに簡単な構成で動作信頼性が高く
、限流特性を自在に設定できる限流装置を実現できる。
As a result, it is possible to realize a current limiting device that has a simple configuration, has high operational reliability, and can freely set current limiting characteristics without using a measuring transformer for current measurement, a control unit, or a magnetic field generating coil.

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

第1図は本発明の一実施例を示す回路図、第2図は本発
明の第二の実施例を示す回路図、第3図は本発明の第三
の実施例を示す回路図、第4図は本発明の第四の実施例
を示す回路図、第5図は本発明の第五の実施例を示す回
路図、第6図は本発明の第六の他の実施例を示す回路図
、第7図は第1図に示す本発明の一実施例における通電
電流特性図、第8図は第1図に示す本発明の一実施例に
おける通電路抵抗特性図、第9図は超電導限流素子を用
いた従来の限流装置の構成図である。 1.2−=端子、3a、3b、3c、3d=超電導限流
素子、6a、6b−コイル、7a、7b。 7c、7d−抵抗体、17 a 、 17 b 、 1
7 c −第1図 第2図 @3図 Jα 第4図 @5図 第6図 ワd J出 第7図 第8図 第9図
FIG. 1 is a circuit diagram showing an embodiment of the present invention, FIG. 2 is a circuit diagram showing a second embodiment of the invention, FIG. 3 is a circuit diagram showing a third embodiment of the invention, and FIG. FIG. 4 is a circuit diagram showing a fourth embodiment of the invention, FIG. 5 is a circuit diagram showing a fifth embodiment of the invention, and FIG. 6 is a circuit diagram showing a sixth other embodiment of the invention. 7 is a current characteristic diagram of the embodiment of the present invention shown in FIG. 1, FIG. 8 is a current conduction path resistance characteristic diagram of the embodiment of the present invention shown in FIG. 1, and FIG. 9 is a superconducting current characteristic diagram. It is a block diagram of the conventional current limiting device using a current limiting element. 1.2-=terminal, 3a, 3b, 3c, 3d=superconducting current limiting element, 6a, 6b-coil, 7a, 7b. 7c, 7d - resistor, 17 a, 17 b, 1
7 c - Figure 1 Figure 2 @ Figure 3 Jα Figure 4 @ Figure 5 Figure 6 Wa d J Out Figure 7 Figure 8 Figure 9

Claims (1)

【特許請求の範囲】 1、超電導限流素子を超電導状態から常電導状態に転移
する事でその抵抗を上昇し、電流を制限する限流方法に
おいて、 常時電流を通じる主回路に過電流が流れたときに、前記
主回路中の超電導素子が常電導に転移し、前記主回路を
流れる過電流を限流した後、複数段の転流回路に順次転
流させる事によって過電流を段階的に限流することを特
徴とする限流方法。 2、超電導状態から常電導状態に転移することで抵抗値
が上昇し、電流を制限する超電導限流素子を含む通電路
を備えた限流装置において、前記超電導限流素子からな
る主回路と、前記超電導限流素子とインピーダンスの直
列にしてなる転流回路と、インピーダンスのみからなる
転流回路よりなることを特徴とする限流装置。
[Scope of Claims] 1. In a current limiting method that increases the resistance of a superconducting current limiting element by transferring it from a superconducting state to a normal conducting state to limit the current, an overcurrent flows in the main circuit through which the current always flows. When the superconducting element in the main circuit transitions to normal conductivity and limits the overcurrent flowing through the main circuit, the overcurrent is gradually reduced by commutating the current through multiple stages of commutation circuits. A current limiting method characterized by current limiting. 2. In a current limiting device comprising a current-carrying path including a superconducting current-limiting element whose resistance increases upon transition from a superconducting state to a normal-conducting state and limits current, a main circuit consisting of the superconducting current-limiting element; A current limiting device comprising: a commutation circuit made up of the superconducting current limiting element and an impedance in series; and a commutation circuit made up of only the impedance.
JP32904790A 1990-11-30 1990-11-30 Current limiting method and current limiting device Pending JPH04207923A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP32904790A JPH04207923A (en) 1990-11-30 1990-11-30 Current limiting method and current limiting device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP32904790A JPH04207923A (en) 1990-11-30 1990-11-30 Current limiting method and current limiting device

Publications (1)

Publication Number Publication Date
JPH04207923A true JPH04207923A (en) 1992-07-29

Family

ID=18217019

Family Applications (1)

Application Number Title Priority Date Filing Date
JP32904790A Pending JPH04207923A (en) 1990-11-30 1990-11-30 Current limiting method and current limiting device

Country Status (1)

Country Link
JP (1) JPH04207923A (en)

Cited By (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2007516690A (en) * 2003-12-23 2007-06-21 エー ビー ビー リサーチ リミテッド Power network
JP2007189228A (en) * 2006-01-13 2007-07-26 European High Temperature Superconductors Gmbh & Co Kg Current adjusting electric device
KR100706741B1 (en) * 1995-10-16 2008-11-21 벡톤 디킨슨 앤드 컴퍼니 Stopcock
CN105470911A (en) * 2015-12-22 2016-04-06 华中科技大学 Direct current limiter
JP2016521111A (en) * 2013-05-20 2016-07-14 スンシル ユニヴァーシティ リサーチ コンソーシアム テクノ−パーク Current limiting device

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100706741B1 (en) * 1995-10-16 2008-11-21 벡톤 디킨슨 앤드 컴퍼니 Stopcock
JP2007516690A (en) * 2003-12-23 2007-06-21 エー ビー ビー リサーチ リミテッド Power network
JP2007189228A (en) * 2006-01-13 2007-07-26 European High Temperature Superconductors Gmbh & Co Kg Current adjusting electric device
JP2016521111A (en) * 2013-05-20 2016-07-14 スンシル ユニヴァーシティ リサーチ コンソーシアム テクノ−パーク Current limiting device
EP3002845A4 (en) * 2013-05-20 2017-03-01 Soongsil University Research Consortium Techno-Park Current limiting device
US9866013B2 (en) 2013-05-20 2018-01-09 Soongsil University Research Consortium Techno-Park Current limiting device
CN105470911A (en) * 2015-12-22 2016-04-06 华中科技大学 Direct current limiter

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