JPS6348368B2 - - Google Patents
Info
- Publication number
- JPS6348368B2 JPS6348368B2 JP3029580A JP3029580A JPS6348368B2 JP S6348368 B2 JPS6348368 B2 JP S6348368B2 JP 3029580 A JP3029580 A JP 3029580A JP 3029580 A JP3029580 A JP 3029580A JP S6348368 B2 JPS6348368 B2 JP S6348368B2
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- vacuum
- section
- shield
- gas
- 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.)
- Expired
Links
- 239000003990 capacitor Substances 0.000 claims description 17
- 238000000034 method Methods 0.000 description 6
- 238000010586 diagram Methods 0.000 description 4
- 230000005540 biological transmission Effects 0.000 description 2
- 238000009413 insulation Methods 0.000 description 2
- 238000010008 shearing Methods 0.000 description 2
- 230000015556 catabolic process Effects 0.000 description 1
- 239000012212 insulator Substances 0.000 description 1
- 238000005507 spraying Methods 0.000 description 1
Landscapes
- High-Tension Arc-Extinguishing Switches Without Spraying Means (AREA)
- Arc-Extinguishing Devices That Are Switches (AREA)
Description
【発明の詳細な説明】
本発明は、消弧方式の異なるしや断部即ち真空
しや断部とガスしや断部によりしや断器を構成す
ることにより、各々の消弧方式の長所を生かし、
欠点をカバーするようにしたしや断器に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION The present invention utilizes the merits of each arc extinguishing method by configuring a shredder breaker with a vacuum shield section and a gas shield section that employ different arc extinguishing methods. Taking advantage of
The present invention relates to a breaker designed to cover the drawbacks.
近年の系統における高電圧大容量化にともな
い、しや断器がしや断すべき短絡電流は急激に増
大し、かつ電圧もますます増大の傾向にある。こ
れら大容量の系統に接続されるしや断器は多数の
しや断部を直列に接続した構成とせざるを得ず、
この場合には部品点数が多く、系統の信頼性向上
の面からは、必らずしも望ましいものではなかつ
た。このためしや断器のしや断点数の低減化をは
かる努力がなされている。 In recent years, with the increase in high voltage and capacity in power systems, the short circuit current that must be cut by a short circuit breaker has rapidly increased, and the voltage has also tended to increase further. The cable breakers connected to these large-capacity systems have no choice but to have a configuration in which a large number of cable breakers are connected in series.
In this case, the number of parts was large, and this was not necessarily desirable from the standpoint of improving system reliability. Efforts are being made to reduce the number of test and break points.
ところで交流しや断器にとつてしや断すべき責
務のうち、最も過酷な条件として、端子短絡故障
と近距離線路故障がある。ここで端子短絡故障は
最大の短絡電流をしや断せねばならないものの、
再起電圧上昇率は近距離線路故障と比較して充分
低く、しや断に失敗する場合の現象は電圧の高さ
に帰因したいわゆる絶縁破壊的再点弧となる。こ
のような現象についてはガスの吹付をともなうい
わゆるガスしや断器が非常に適しており、1しや
断点あたり耐電圧特性の優れたものを提供でき
る。これに対して真空しや断器はガスしや断器と
比較して1しや断点あたりの電圧性能はほぼ1/3
にすぎない。 By the way, the most severe conditions among the responsibilities that an AC switch or disconnector must perform are terminal short-circuit failures and short-distance line failures. Here, the terminal short-circuit fault must suppress the maximum short-circuit current, but
The rate of rise in the re-electromotive voltage is sufficiently low compared to short-distance line faults, and the phenomenon in which shearing fails is so-called dielectric breakdown restriking due to the high voltage. For such a phenomenon, a so-called gas shield disconnector that involves spraying of gas is very suitable, and can provide excellent withstand voltage characteristics per disconnect point. On the other hand, the voltage performance of a vacuum disconnector is approximately 1/3 that of a gas disconnector.
It's nothing more than that.
一方近距離結線路故障の場合には、電流しや断
後の再起電圧上昇率が非常に高く、しや断に失敗
する場合の現象は、いわゆる熱的再発弧となる。
これは電流零点前の電流降下率とも深い関係をも
つており、電流零点後数μs以内にしや断の成否が
決まる。このような現象については、真空しや断
器の方がガスしや断器に比較して、ほぼ3倍程度
良い性能を有している。 On the other hand, in the case of a short-distance connection line failure, the rate of increase in the restart voltage after the current is interrupted is very high, and the phenomenon when the interruption fails is what is called thermal re-ignition.
This has a close relationship with the current drop rate before the current zero point, and the success or failure of shearing is determined within a few μs after the current zero point. With regard to such phenomena, vacuum insulation and disconnectors have approximately three times better performance than gas insulation and disconnection.
また最近、開発の必要性が強く言われている直
流しや断器においては、しや断時に他のコンデン
サ電源より強制的に電流を注入して、電流零点を
作るものが開発されているが、経済的な理由から
コンデンサの容量をできるだけ小さくすることが
望ましい。コンデンサ容量を小さくした場合電流
の降下率が大きくなるとともに再起電圧上昇率も
大きいものとなる。従つてしや断器としては前記
熱的再発弧現象に対して優れた性能を有するもの
が必要であり、その意味では前述の近距離線路故
障に対するのと同様に、真空しや断器が最も適し
ている。しかしながら、直流送電系統に使用され
る直流しや断器は交流の場合と同様に500KV程
度のものまで要求されており、真空しや断器で
は、耐電圧性能の面から多点切構造とせざるを得
ない。一方ガスしや断器では耐電圧性能は優れて
いるものの、前述のように熱的再発弧現象に関し
て真空しや断器ほどの性能がないため、1しや断
点あたりの再起電圧上昇率を下げるために、やは
り多点切構造とせざるを得ない。ガスしや断器
で、多点切構造をさけるためには、前記コンデン
サーの容量を増やして、電流降下率および再起電
圧上昇率を低くする方法がするがこれは経済的と
はいえない。 Recently, there has been a strong need for the development of direct current and circuit breakers, which have been developed to forcibly inject current from other capacitor power sources during power outages to create a current zero point. For economical reasons, it is desirable to make the capacitance of the capacitor as small as possible. When the capacitor capacity is made smaller, the rate of drop in current increases and the rate of increase in restart voltage also increases. Therefore, it is necessary to use a vacuum circuit breaker that has excellent performance against the thermal re-ignition phenomenon, and in this sense, a vacuum circuit breaker is the best option, as it is for short-distance line failures mentioned above. Are suitable. However, DC and disconnectors used in DC power transmission systems are required to be up to around 500KV, just like in the case of AC, and vacuum disconnectors must have a multi-point disconnection structure from the standpoint of withstand voltage performance. I don't get it. On the other hand, although gas shield disconnectors have excellent withstand voltage performance, as mentioned above, they do not have the same performance as vacuum disconnectors in terms of thermal re-ignition phenomena, so the rate of rise in the re-EMF voltage per circuit break is limited. In order to lower this, a multi-point cutting structure must be used. In order to avoid a multi-point disconnection structure with gas insulators and disconnectors, it is possible to increase the capacitance of the capacitor to lower the rate of current drop and the rate of increase in re-electromotive voltage, but this cannot be said to be economical.
以上のように交流しや断器においても直流しや
断器においてもガスしや断部ないし真空しや断部
のみで、超高圧以上のしや断器を構成した場合、
多点切構造とせざるを得ず、経済的でないばかり
か、部品点数も多くなるため信頼性向上の面から
も望ましいものではなかつた。 As mentioned above, in both AC and DC circuits, when a circuit breaker with ultra-high pressure or higher is configured with only a gas or vacuum section or a vacuum section or a section,
A multi-point cutting structure had to be used, which was not only uneconomical but also required a large number of parts, which was not desirable from the standpoint of improving reliability.
これらの問題を解決する手段として真空しや断
器とガスしや断器を直列に接続して、両者の欠点
を互いにカバーし、長所を生かす方法が考えられ
ているが、最適な性能を出すためにはしや断後に
印加される再起電圧を真空しや断部とガスしや断
部に各々の性能に適した値に分割して印加する必
要がある。 As a means to solve these problems, a method has been considered that connects a vacuum shield and gas disconnector in series to cover the shortcomings of both and take advantage of their strengths, but this method does not yield optimal performance. In order to do this, it is necessary to divide the re-electromotive voltage applied after the shield is broken into the vacuum shield section and the gas shield section into values suitable for the performance of each.
従来、複数のしや断部を電気的に直列に接続し
たいわゆる多点切しや断器では、これらしや断部
の電圧分担をできるだけ均等化するため、各しや
断部に並列に抵抗あるいはコンデンサのみを接続
し、再起電圧波形に対して各しや断部の電圧分担
が時間的にも常に一定となる抵抗分圧形あるいは
コンデンサ分圧形の電圧分担法を採用していた。 Conventionally, in so-called multi-point disconnectors or disconnectors in which multiple shields are electrically connected in series, a resistor is connected in parallel to each shield in order to equalize the voltage sharing among these shields as much as possible. Alternatively, only a capacitor is connected, and a resistor voltage division type or capacitor voltage division type voltage distribution method has been adopted, in which the voltage distribution of each shear and disconnection portion is always constant over time with respect to the re-EMF voltage waveform.
第1図に交流送電系統に発生する近距離線路故
障時の再起電圧波形例を示す。1の部分は線路側
に発生した再起電圧に帰因するもので、周波数が
高いため、再起電圧上昇率は非常に高いもののこ
の部分の電圧値は、全体の再起電圧と比較すると
充分低い。また2の部分は電源側に発生した再起
電圧に帰因するもので、電圧波高値が非常に高
い。このような再起電圧に対して、前記コンデン
サ分圧形あるいは抵抗分圧形の電圧分担方法を採
用したのでは、各しや断部に印加される波形は単
に1図のものと相似になるにすぎず、真空しや断
器とガスしや断部を直列に接続して構成しただけ
のしや断器では、意味がないことは前述の説明の
ように明らかである。 Figure 1 shows an example of the re-EMF voltage waveform when a short-distance line fault occurs in an AC power transmission system. The portion 1 is due to the re-electromotive voltage generated on the line side, and because the frequency is high, the rate of increase in the re-electromotive voltage is very high, but the voltage value in this portion is sufficiently low compared to the overall re-electromotive voltage. Part 2 is due to the re-electromotive voltage generated on the power supply side, and has a very high voltage peak value. If we adopt the above-mentioned capacitor voltage division type or resistor voltage division type voltage sharing method for this kind of re-electromotive voltage, the waveform applied to each cross section will simply be similar to that in Figure 1. As explained above, it is clear that a vacuum shield and disconnector simply constructed by connecting a vacuum shield and a gas shield in series is meaningless.
本発明は再起電圧を最適な値に調整することに
より優れたしや断性能を得ることができるしや断
器を提供することを目的とする。 SUMMARY OF THE INVENTION An object of the present invention is to provide a shear breaker that can obtain excellent shear breaker performance by adjusting the re-electromotive voltage to an optimal value.
第2図に本発明の回路図を示す。真空しや断器
よりなる真空しや断部7と、バツフア形ガスしや
断器よりなるガスしや断部8を直列に接続し、か
つ各しや断部7,8に並列に、抵抗3および4を
接続する。この抵抗3および4に並列にコンデン
サ5,6をさらに並列に接続する。また、抵抗3
の値は抵抗の4の値より小さくそしてコンデンサ
5の値も、コンデンサ6の値より小さくする。即
ち抵抗値3<抵抗値4、コンデンサ容量5<コン
デンサ容量6となつている。 FIG. 2 shows a circuit diagram of the present invention. A vacuum shield section 7 consisting of a vacuum shield disconnector and a gas shield section 8 consisting of a buffer type gas shield disconnector are connected in series, and a resistor is connected in parallel to each shield section 7 and 8. Connect 3 and 4. Capacitors 5 and 6 are further connected in parallel to the resistors 3 and 4. Also, resistance 3
The value of is smaller than the value of resistor 4, and the value of capacitor 5 is also smaller than the value of capacitor 6. That is, resistance value 3<resistance value 4, capacitor capacity 5<capacitor capacity 6.
このような構成としてしや断器を形成すること
により、急激な時間変化を伴なう電圧は、コンデ
ンサ分圧部を通して真空しや断部7に大部分が印
加され、ガスしや断部8には、ほとんど印加され
ないが、あるいは印加されたとしても、非常に低
い値とすることができる。また、時間変化の少な
い電圧あるいは直流電圧などは抵抗分圧部によ
り、大部分がガスしや断部8に印加され、真空し
や断部7には、ほとんど電圧が印加されないよう
にすることができる。 By forming the shield breaker with such a configuration, most of the voltage with rapid time changes is applied to the vacuum shield breaker 7 through the capacitor voltage dividing section, and the voltage that is accompanied by rapid time changes is applied to the vacuum shield breaker 7 through the capacitor voltage dividing section, and the voltage that is accompanied by rapid time changes is applied to the vacuum shield breaker 7 through the capacitor voltage dividing section. is hardly applied, or even if it is applied, it can be at a very low value. In addition, it is possible to apply most of the voltage with little time change or direct current voltage to the gas shield or disconnection section 8 using the resistive voltage divider, and to apply almost no voltage to the vacuum shield or disconnection section 7. can.
第1図に示した近距離線路故障の波形例では、
真空しや断部7には第3図に示したように、初期
の再起電圧上昇率の高い波形部1が印加される
が、その後の高い電圧値は、ほとんど印加されず
にすむ。また同じく第4図に示したように、ガス
しや断部8には初期部の上昇率の高い電圧はほと
んど印加されずその後の上昇率が低いものの電圧
値の高い部分2が印加されるようになる。すなわ
ち、前述のように真空しや断部7およびガスしや
断部8の各性能に最も適した電圧波形を印加する
ことができる。 In the waveform example of a short-distance line fault shown in Figure 1,
As shown in FIG. 3, the waveform portion 1 with a high initial rise rate of the re-electromotive voltage is applied to the vacuum shear break portion 7, but subsequent high voltage values are hardly applied. Also, as shown in FIG. 4, almost no voltage is applied to the gas shield section 8 in the initial part where the rate of increase is high, and thereafter the voltage is applied to the part 2 where the rate of increase is low but the voltage is high. become. That is, as described above, it is possible to apply a voltage waveform most suitable for each performance of the vacuum shield section 7 and the gas shield section 8.
またこれら電圧値の分担率は各素子の値を変化
させることにより比較的自由に得ることができ
る。 Moreover, the sharing ratio of these voltage values can be obtained relatively freely by changing the values of each element.
以上述べたように本発明のような構成とするこ
とによりしや断点数を最少に押え、しや断性能の
優れたしや断器を提供することができる。 As described above, by employing the structure of the present invention, it is possible to minimize the number of shear breakage points and provide a sheath breaker with excellent shear cutting performance.
また本例では、真空しや断部およびガスしや断
部各1点を用いた場合を説明したが、これらしや
断部を複数個用いてもよい。 Further, in this example, a case has been described in which one vacuum shield section and one gas shield section are used, but a plurality of these shield sections may be used.
第1図は近距離線路故障における再起電圧波形
例を示す説明図、第2図は本発明の一実施例を示
す回路図、第3図および第4図は本発明を適用し
た場合における真空しや断部の電圧波形とガスし
や断部の電圧波形を示す説明図である。
1,2……再起電圧、3,4……抵抗、5,6
……コンデンサ、7……真空しや断部、8……ガ
スしや断部。
Fig. 1 is an explanatory diagram showing an example of a re-electromotive voltage waveform in the case of a short-distance line fault, Fig. 2 is a circuit diagram showing an embodiment of the present invention, and Figs. FIG. 4 is an explanatory diagram showing a voltage waveform of a gas line break section and a voltage waveform of a gas line break section. 1, 2... Restart voltage, 3, 4... Resistance, 5, 6
...Capacitor, 7...Vacuum shield section, 8...Gas chamber section.
Claims (1)
に接続してしや断器を構成したものにおいて、各
しや断部に夫々抵抗とコンデンサを並列にした電
圧分担用素子を接続してなり、これら素子の抵抗
値および容量値は前記真空しや断部にとりつけた
ものが前記ガスしや断部にとりつけたものよりも
小さくなるように設定したことを特徴とするしや
断器。1 In a circuit breaker constructed by electrically connecting a vacuum shield section and a gas shield section in series, a voltage sharing element consisting of a resistor and a capacitor in parallel is installed in each shield section. The resistance and capacitance values of these elements are set so that the element attached to the vacuum shield section is smaller than the element attached to the gas shield section. Disconnector.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3029580A JPS56128527A (en) | 1980-03-12 | 1980-03-12 | Breaker |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP3029580A JPS56128527A (en) | 1980-03-12 | 1980-03-12 | Breaker |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS56128527A JPS56128527A (en) | 1981-10-08 |
| JPS6348368B2 true JPS6348368B2 (en) | 1988-09-28 |
Family
ID=12299736
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP3029580A Granted JPS56128527A (en) | 1980-03-12 | 1980-03-12 | Breaker |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS56128527A (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6155829A (en) * | 1984-08-28 | 1986-03-20 | 株式会社東芝 | Breaker |
| JP2535492B2 (en) * | 1993-04-21 | 1996-09-18 | 有限会社シン・タック | Piggy bank |
-
1980
- 1980-03-12 JP JP3029580A patent/JPS56128527A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS56128527A (en) | 1981-10-08 |
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