JPH03219514A - Vacuum-type circuit-breaker - Google Patents

Vacuum-type circuit-breaker

Info

Publication number
JPH03219514A
JPH03219514A JP1362790A JP1362790A JPH03219514A JP H03219514 A JPH03219514 A JP H03219514A JP 1362790 A JP1362790 A JP 1362790A JP 1362790 A JP1362790 A JP 1362790A JP H03219514 A JPH03219514 A JP H03219514A
Authority
JP
Japan
Prior art keywords
vacuum
ring
voltage
time
current
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
JP1362790A
Other languages
Japanese (ja)
Inventor
Kiyobumi Otobe
乙部 清文
Kunio Yokokura
邦夫 横倉
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 JP1362790A priority Critical patent/JPH03219514A/en
Publication of JPH03219514A publication Critical patent/JPH03219514A/en
Pending legal-status Critical Current

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  • High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)

Abstract

PURPOSE:To suppress surge electric voltage generated by arcing at the shutting time of low current of delay power factor by installing a ferrite ring on an electrically conducting axle which is a part of a loop in which high frequency electric current flows at the time of arc regeneration. CONSTITUTION:A ferrite ring 10, which is ferromagnetic, is attached to electrically conducting axles 4, 5 of a vacuum 6, which is a part of a loop where high frequency electric current flows at the time of arc regeneration. Then, corresponding to the high frequency electric current flowing in a circuit, magnetic fluxes are generated in the inside of the ring 10 and the number of crossing magnetic fluxes increases. Inductance in the part thus becomes large so that time constant of a rising part becomes large. Since the same effect is achieved even if the ring 10 is installed in any point of the current loop, it is inserted in the electrically conducting axle 5 of the valve 6 and thus an insulation distance between a pair of electrodes 2, 3 of the ring 10 and the valve 6 is kept sufficiently. Since reactance increases, sharp surge electric voltage generated by arc generation between contacts at the shutting time of low current of delay power factor is suppressed.

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、とくに開閉時のサージ電圧を抑えた真空遮断
器に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Field of Industrial Application) The present invention particularly relates to a vacuum circuit breaker that suppresses surge voltage during switching.

(従来の技術) 真空遮断器で誘導性負荷の小電流を開閉するときに発生
する開閉サージ電圧は、電流さい断に伴なう数kHzの
サージ電圧と再発弧にともなう数MHzのサージ電圧が
あり、これらのサージ電圧を抑えるために、従来からC
Rサプレッサ、避雷器。
(Prior art) The switching surge voltage that occurs when switching a small current of an inductive load in a vacuum circuit breaker is composed of a surge voltage of several kHz associated with current interruption and a surge voltage of several MHz associated with re-ignition. In order to suppress these surge voltages, C
R suppressor, lightning arrester.

非直線抵抗体などが使われている。しかし、これらのサ
ージ抑制機器は、すべて対地電圧の抑制を対象とされ、
再発弧に伴なう数M)Izのサージ電圧を対象としてい
ない(ただし、対地電圧が抑制されることで、再発弧に
ともなう数MHzのサージ電圧の波高値の抑制効果が生
ずる。電気学会雑誌、Vo12.93. No8参照)
Nonlinear resistors are used. However, all of these surge suppression devices are aimed at suppressing ground voltage.
It does not target the surge voltage of several M) Iz that accompanies re-ignition (however, by suppressing the ground voltage, the effect of suppressing the peak value of the surge voltage of several MHz that accompanies re-ignition occurs. Journal of the Institute of Electrical Engineers of Japan) , Vo12.93.Refer to No.8)
.

ところで、高圧電動機などは系統の末端に接続されるこ
とから、従来インパルス耐電圧に対する規格がない。こ
のような高圧電動機の開閉に、もし、真空遮断器のよう
な高周波サージ電圧を発生する開閉器が接続されると、
高圧電動機との絶縁協調上問題が生ずることがある。す
なわち、高圧電動機に急峻な波頭長を有するサージ電圧
が侵入すると、高圧電動機の口出部のコイルで高い電圧
を分担してしまう。
By the way, since high-voltage motors and the like are connected to the end of the system, there is no standard for impulse withstand voltage. If a switch that generates high-frequency surge voltage, such as a vacuum circuit breaker, is connected to open and close such a high-voltage motor,
Problems may arise in insulation coordination with high-voltage motors. That is, when a surge voltage having a steep wavefront length enters the high-voltage motor, the high voltage is shared by the coil at the outlet of the high-voltage motor.

(発明が解決しようとする課題) すると、コイルの対地間の絶縁(主絶縁)だけではなく
、層間の絶縁が問題となる。商用周波数の交流電圧のと
きには、コイル間の電圧分担がほぼ均等になるため、コ
イル内部の層間には低い電圧しかかからず、したがって
層間絶縁耐圧は、低いレベルでもよい。しかし、短かい
波頭長のサージ電圧が侵入したときには、日出部のコイ
ルの分担電圧が増え、しかも、この分担電圧は、波頭長
が短かいほど大きくなり、例えば波頭長0.2μSのサ
ージが侵入したときには、日出部の分担電圧の比率は9
0%程度になることが知られている。
(Problem to be Solved by the Invention) Then, not only the insulation between the coil and the ground (main insulation) but also the insulation between the layers becomes a problem. When the alternating current voltage is at a commercial frequency, the voltage distribution between the coils is approximately equal, so only a low voltage is applied between the layers inside the coil, and therefore the interlayer dielectric strength voltage may be at a low level. However, when a surge voltage with a short wavefront length enters, the voltage shared by the coil at the sunrise part increases.Moreover, this shared voltage becomes larger as the wavefront length becomes shorter.For example, when a surge voltage with a wavefront length of 0.2μS When the invasion occurred, the ratio of the shared voltage in the sunrise section was 9.
It is known that it is about 0%.

このように、急峻なサージに対して各部の電圧分担のア
ンバランスが大きく、かつ、層間絶縁された機器との絶
縁協調を考慮するときには、急峻なサージ電圧が大きな
問題となる。
As described above, when considering the insulation coordination with interlayer-insulated equipment, where there is a large unbalance in voltage sharing among various parts in response to a sudden surge, the sudden surge voltage becomes a big problem.

そこで、本発明の目的は、遅れ力率の小電流遮断時に接
点間の発弧で発生する急峻なサージ電圧を抑えることの
できる真空遮断器を得ることである。
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide a vacuum circuit breaker that can suppress the steep surge voltage that occurs due to arcing between contacts when interrupting a small current with a lagging power factor.

〔発明の構成〕[Structure of the invention]

(課題を解決するための手段) 本発明は、10−” Pa以下の高真空度の真空容器内
に対向して一対の電極がそれぞれ通電軸を介して接離自
在に設けられた真空バルブが内蔵された真空遮断器にお
いて、真空容器内に、軸心に通電軸が貫通する環状の磁
性体を設けたことを特徴とする真空遮断器である。
(Means for Solving the Problems) The present invention provides a vacuum valve in which a pair of electrodes are provided facing each other in a vacuum container with a high degree of vacuum of 10-" Pa or less and are movable toward and away from each other via current-carrying shafts. This vacuum circuit breaker is a built-in vacuum circuit breaker, characterized in that an annular magnetic body is provided in the vacuum container, the axis of which is penetrated by a current-carrying shaft.

(作 用) 真空遮断器再発弧時の急峻なサージ電圧の波頭長は、真
空遮断器周りのインダクタンスと線路のサージインピー
ダンスで決まる。また、そのときの波頭長は、真空遮断
器周りのインダクタンスが大きくなると緩和されるから
、真空遮断器の高周波サージ電流が流れる通電部に設け
られた強磁性体の可飽和特性のよい磁性体で見かけ上の
真空遮断器周りのインダクタンスが大きくなり、再発弧
時の急峻なサージ電圧の立上りを緩和することができる
(Function) The wavefront length of the steep surge voltage when the vacuum circuit breaker re-ignites is determined by the inductance around the vacuum circuit breaker and the surge impedance of the line. In addition, the wavefront length at that time is relaxed as the inductance around the vacuum circuit breaker increases, so the ferromagnetic material with good saturability characteristics provided in the current-carrying part of the vacuum circuit breaker through which the high-frequency surge current flows. The apparent inductance around the vacuum circuit breaker increases, making it possible to alleviate the sudden rise in surge voltage at the time of re-ignition.

(実施例) 以下、本発明の真空遮断器の一実施例を図面を参照して
説明する。
(Example) Hereinafter, one example of the vacuum circuit breaker of the present invention will be described with reference to the drawings.

第1図において、真空容器1内に対向して一対3− 4− の電極2,3がそれぞれ通電軸4,5を介して接離自在
に配設された真空バルブ6は、真空遮断器7の主回路断
路部8,9に通電軸4,5を接続して取付けられている
。ここで、通電軸5には、フェライ1−リング10が外
挿されている。
In FIG. 1, a vacuum valve 6 in which a pair of electrodes 2, 3 facing each other in a vacuum vessel 1 are disposed so as to be freely accessible and separable via current-carrying shafts 4, 5, respectively, is connected to a vacuum circuit breaker 7. The current-carrying shafts 4 and 5 are connected to the main circuit disconnecting parts 8 and 9 of the main circuit. Here, the ferrite 1-ring 10 is extrapolated onto the current-carrying shaft 5.

このように構成された真空遮断器の作用を説明する。The operation of the vacuum circuit breaker configured in this way will be explained.

真空遮断器7で電動機負荷の小電流を遮断すると、第2
図に示すような繰返し再発弧(多重再発弧)が発生する
ことがある(注:折線は電極間電圧を示す)。この現象
は、真空バルブ内の接点が開離直後に電流が遮断され、
しかも充分接点が開いていないときに発生する。このた
め、電流遮断にともなう過渡回復電圧が接点間の耐圧を
超え、接点間で放電が発生し、このとき接点間を流れる
高周波電流がその電流零点で消弧される。これらの現象
が繰り返し発生し、次第に電圧が上っていくが、この現
象のある再発弧点近傍を拡大すると、一般に第3図のよ
うになる。すなわち、再発弧瞬時は急激に電圧が変化す
るため、線路を分布定数として考える必要がある。
When the vacuum circuit breaker 7 interrupts the small current of the motor load, the second
Repeated re-ignition (multiple re-ignition) as shown in the figure may occur (note: the broken line indicates the voltage between the electrodes). This phenomenon occurs because the current is cut off immediately after the contacts in the vacuum valve open.
Moreover, this occurs when the contacts are not sufficiently opened. For this reason, the transient recovery voltage accompanying the current interruption exceeds the withstand voltage between the contacts, and discharge occurs between the contacts, and at this time, the high frequency current flowing between the contacts is extinguished at its current zero point. These phenomena occur repeatedly and the voltage gradually rises, but if you zoom in on the vicinity of the re-ignition point where this phenomenon occurs, it will generally look like the one shown in Figure 3. That is, since the voltage changes rapidly at the moment of re-ignition, it is necessary to consider the line as a distributed constant.

一般の所内配電系統では、真空遮断器と電動機の間は一
般に電カケープルで接続される。ここである一つの真空
遮断器に着目した場合、真空遮断器の電源側には同様の
フィーダ遮断器が接続されることとなり、真空遮断器か
らみたサージインピーダンスは小さい。また、真空遮断
器とこれが収納される閉鎖配電盤の母線は、ストレーの
インダクタンス分を持っている。さらに、真空遮断器の
負荷側には、電カケープルが接続され、そのサージイン
ピーダンスは数10Ωである。また、電カケープルの他
端に接続される電動機のサージインピーダンスは、一般
に数にΩである。以上のことを考慮し、再発弧時の等節
回路を求めると第4図となる。同図において、電源側を
対地間のストレキャパシタンス11とし、接点間の放電
をスイッチ12が閉路することで模擬する。真空遮断器
周りのインダクタンスは、電源側ストレーインダクタン
ス13、負荷側ストレーインダクタンス14で表わし、
電カケープルはケーブル15で表わし、電動機はそのサ
ージインピーダンスが電カケープルのサージインピーダ
ンスと比較して大きいことから、急峻なサージ電圧に対
しては無視できるので、第4図の等何回路上は考慮せず
、ケーブル15の一方は開放端としている。
In a general in-house power distribution system, a vacuum circuit breaker and an electric motor are generally connected by an electric cable. When focusing on one vacuum breaker here, a similar feeder breaker is connected to the power supply side of the vacuum breaker, and the surge impedance seen from the vacuum breaker is small. Furthermore, the vacuum circuit breaker and the busbar of the closed switchboard in which it is housed have stray inductance. Further, a power cable is connected to the load side of the vacuum circuit breaker, and its surge impedance is several tens of ohms. Furthermore, the surge impedance of the motor connected to the other end of the power cable is generally approximately Ω. Taking the above into consideration, the equinodal circuit at the time of re-ignition is found as shown in Figure 4. In the figure, the power supply side is a strain capacitance 11 to ground, and the discharge between the contacts is simulated by closing the switch 12. The inductance around the vacuum circuit breaker is represented by the power supply side stray inductance 13 and the load side stray inductance 14,
The power cable is represented by a cable 15, and since the surge impedance of the motor is large compared to the surge impedance of the power cable, steep surge voltages can be ignored, so the circuit shown in Figure 4 does not need to be considered. First, one end of the cable 15 is open.

同図の等価回路で、スイッチ12が閉略したときにスト
レーインダクタンス14とケーブル15の接続点の対地
間に発生する電圧波形は、ケーブル15の線路長が充分
長いと仮定すると、第5図のようになる。この電圧波形
の立ち上り部の時定数Jは次式であられすことができる
In the equivalent circuit shown in the figure, when the switch 12 is closed, the voltage waveform generated between the stray inductance 14 and the connection point of the cable 15 to the ground is as shown in Fig. 5, assuming that the line length of the cable 15 is sufficiently long. It becomes like this. The time constant J of the rising portion of this voltage waveform can be expressed by the following equation.

J” (Lxa + Li4)/ Zにこで、Zcはケ
ーブル15のサージインピーダンス、L□3は電源側ス
トレートインダクタンス13のインダクタンス、Li4
は負荷側ストレートインダクタンスL□4のインダクタ
ンスである。
J” (Lxa + Li4)/Z is the surge impedance of the cable 15, L□3 is the inductance of the straight inductance 13 on the power supply side, Li4
is the inductance of the load side straight inductance L□4.

上式より明らかなように、再発弧時の急峻な立ち上りを
緩和するためには、L131L14を大きくするかZc
を小さくすることが考えられるが、Zcをサージ抑制だ
けのために小さ(することはむだが多い。また、L13
L14は母線形状、および配置から決まるので、これを
変えるのは困難である。このため、上記構成のように、
再発弧時に高周波電流の流れるループの一部である真空
バルブの通電軸5に強磁性体であるフェライトリング1
0を取り付けることにより、回路に流れる高周波電流に
対応した磁束がフェライトリング10内部に発生し、高
周波電流とフェライトリング10の磁路内の磁束とによ
る鎖交磁束数を増やし、この部分のインダクタンスを大
きくし、見かけ上第4図に示すL13+L14の値を大
きくすることで、立ち上り部の時定数Jを大きくするこ
とができる。
As is clear from the above formula, in order to alleviate the steep rise at the time of re-ignition, either increase L131L14 or change Zc
It is possible to reduce Zc, but it is often wasteful to reduce Zc just for surge suppression.
Since L14 is determined by the generatrix shape and arrangement, it is difficult to change this. Therefore, as in the above configuration,
A ferrite ring 1 made of ferromagnetic material is attached to the current-carrying shaft 5 of the vacuum valve, which is part of the loop through which high-frequency current flows during re-ignition.
By attaching 0, a magnetic flux corresponding to the high frequency current flowing in the circuit is generated inside the ferrite ring 10, increasing the number of flux linkages between the high frequency current and the magnetic flux in the magnetic path of the ferrite ring 10, and reducing the inductance of this part. By increasing the value of L13+L14 apparently shown in FIG. 4, the time constant J of the rising portion can be increased.

この方法によれば、フェライトリング10は高周波電流
の流れる電流ループのどの位置に設けても同様の効果が
期待できる。しかし、このようなフェライトリング10
を充電部に設置して絶縁距離を十分確保するのは場所に
よっては問題なので、本発明では真空遮断器に使われて
いる真空バルブ内部の通電軸5に挿入したもので、フェ
ライトリング10と真空バルブ6の一対の電極2,3を
取囲ん7− で設けられたシールド16との間の絶縁距離は十分確保
できる。
According to this method, the same effect can be expected no matter where the ferrite ring 10 is placed in the current loop through which the high-frequency current flows. However, such a ferrite ring 10
Since it is a problem to install the ferrite ring 10 in the live part and ensure sufficient insulation distance depending on the location, in the present invention, it is inserted into the current carrying shaft 5 inside the vacuum valve used in the vacuum circuit breaker. A sufficient insulation distance between the bulb 6 and the shield 16 provided at 7- surrounding the pair of electrodes 2 and 3 can be ensured.

この結果、本発明によれば、再発弧時の急峻な立ち上り
電圧を緩和することができ、電動機の層間絶縁破壊を防
ぎ再発弧サージの絶縁協調を図ることができる真空遮断
器となる。
As a result, according to the present invention, a vacuum circuit breaker is provided which can alleviate the steep rise voltage at the time of re-ignition, prevent interlayer dielectric breakdown of the motor, and achieve insulation coordination for re-ignition surge.

なお、上記実施例において、フェライトリング10の磁
路断面積は、小電流となる負荷のさい断電流値によって
決めればよく、更に、取付場所には絶縁物を介して取付
けてもよく、更に、第1図のシールド16をフェライト
で構成して兼用してもよい。
In the above embodiment, the magnetic path cross-sectional area of the ferrite ring 10 may be determined based on the severing current value of the load that generates a small current.Furthermore, the ferrite ring 10 may be installed through an insulator at the installation location. The shield 16 shown in FIG. 1 may also be made of ferrite.

〔発明の効果〕〔Effect of the invention〕

以上、本発明によれば、10−2Pa以下の高真空度の
真空容器内に対向して一対の電極がそれぞれ通電軸を介
して接離自在に設けられた真空バルブが内蔵された真空
遮断器において、真空容器内に、軸心に通電軸が貫通す
る環状の磁性体を設けたので、遅れ力率の小電流遮断時
に接点間の発弧で発生する急峻なサージ電圧を抑えるこ
とのできる真空遮断器を得ることができる。
As described above, according to the present invention, a vacuum circuit breaker has a built-in vacuum valve in which a pair of opposing electrodes are provided in a vacuum container with a high degree of vacuum of 10-2 Pa or less and can be freely connected to and separated from the other via the current-carrying shaft. In the vacuum chamber, an annular magnetic body is installed in the vacuum chamber, and the current-carrying shaft passes through the center of the vacuum chamber.The vacuum chamber is capable of suppressing the sudden surge voltage that occurs due to arcing between contacts when interrupting a small current with a lagging power factor. You can get a circuit breaker.

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

第1図は本発明の真空遮断器の一実施例を示す部分破断
側面図、第2図、第3図、第4図及び第5図は本発明の
真空遮断器の作用を示す図である。 1・・・真空容器      2,3・・・電極4、5
・・・通電軸       6・・・真空バルブ10・
・・フェライトリング (8733)  代理人 弁理士 猪 股 祥 晃(ほ
か1名)特開平3 219514 (4) 第2洒っAキP詳細回 第3図
FIG. 1 is a partially cutaway side view showing one embodiment of the vacuum circuit breaker of the present invention, and FIGS. 2, 3, 4, and 5 are diagrams showing the operation of the vacuum circuit breaker of the present invention. . 1... Vacuum container 2, 3... Electrodes 4, 5
...Electric shaft 6...Vacuum valve 10.
...Ferrite ring (8733) Agent Patent attorney Yoshiaki Inomata (and 1 other person) JP-A-3 219514 (4) 2nd AkiP details Figure 3

Claims (1)

【特許請求の範囲】[Claims] 10^−^2Pa以下の高真空度の真空容器内に対向し
て一対の電極がそれぞれ通電軸を介して接離自在に設け
られた真空バルブが内蔵された真空遮断器において、前
記真空容器内に、軸心に前記通電軸が貫通する環状の磁
性体を設けたことを特徴とする真空遮断器。
In a vacuum circuit breaker with a built-in vacuum valve in which a pair of electrodes are provided facing each other in a vacuum container with a high degree of vacuum of 10^-^2 Pa or less and can be freely connected and separated via current-carrying shafts, A vacuum circuit breaker, characterized in that an annular magnetic body is provided at the center of the axis through which the current-carrying shaft passes.
JP1362790A 1990-01-25 1990-01-25 Vacuum-type circuit-breaker Pending JPH03219514A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1362790A JPH03219514A (en) 1990-01-25 1990-01-25 Vacuum-type circuit-breaker

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1362790A JPH03219514A (en) 1990-01-25 1990-01-25 Vacuum-type circuit-breaker

Publications (1)

Publication Number Publication Date
JPH03219514A true JPH03219514A (en) 1991-09-26

Family

ID=11838478

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1362790A Pending JPH03219514A (en) 1990-01-25 1990-01-25 Vacuum-type circuit-breaker

Country Status (1)

Country Link
JP (1) JPH03219514A (en)

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