JPH053206B2 - - Google Patents
Info
- Publication number
- JPH053206B2 JPH053206B2 JP58189658A JP18965883A JPH053206B2 JP H053206 B2 JPH053206 B2 JP H053206B2 JP 58189658 A JP58189658 A JP 58189658A JP 18965883 A JP18965883 A JP 18965883A JP H053206 B2 JPH053206 B2 JP H053206B2
- Authority
- JP
- Japan
- Prior art keywords
- phase
- current
- zero
- zero point
- short
- 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 - Lifetime
Links
Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01H—ELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
- H01H9/00—Details of switching devices, not covered by groups H01H1/00 - H01H7/00
- H01H9/54—Circuit arrangements not adapted to a particular application of the switching device and for which no provision exists elsewhere
- H01H9/56—Circuit arrangements not adapted to a particular application of the switching device and for which no provision exists elsewhere for ensuring operation of the switch at a predetermined point in the AC cycle
- H01H9/563—Circuit arrangements not adapted to a particular application of the switching device and for which no provision exists elsewhere for ensuring operation of the switch at a predetermined point in the AC cycle for multipolar switches, e.g. different timing for different phases, selecting phase with first zero-crossing
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01H—ELECTRIC SWITCHES; RELAYS; SELECTORS; EMERGENCY PROTECTIVE DEVICES
- H01H33/00—High-tension or heavy-current switches with arc-extinguishing or arc-preventing means
- H01H33/006—High-tension or heavy-current switches with arc-extinguishing or arc-preventing means adapted for interrupting fault currents with delayed zero crossings
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Emergency Protection Circuit Devices (AREA)
- Driving Mechanisms And Operating Circuits Of Arc-Extinguishing High-Tension Switches (AREA)
- Keying Circuit Devices (AREA)
- Measurement Of Current Or Voltage (AREA)
Abstract
Description
【発明の詳細な説明】
〔発明の属する技術分野〕
この発明は三相のうちのいずれか1相の短絡電
流がしや断されるべき所定の時間内において零点
を通過しない波形を有する三相短絡電流を通常の
交流遮断器ないし交流回路用半導体遮断器によつ
て遮断する際の遮断方法に関する。[Detailed Description of the Invention] [Technical Field to Which the Invention Pertains] This invention relates to a three-phase circuit having a waveform in which the short-circuit current of any one of the three phases does not pass through a zero point within a predetermined time period in which the short-circuit current of any one of the three phases is to be cut off. The present invention relates to a method for interrupting short-circuit current using an ordinary AC circuit breaker or a semiconductor circuit breaker for AC circuits.
従来、零点を通過しない短絡電流を交流遮断器
により遮断する方法として、高周波の振動電流を
この短絡電流に重畳し、強制的に零点をつくつて
遮断する方法と、遮断器中のアークの抵抗によつ
てこの短絡電流中の直流分を急速に減衰させて零
点を通過する波形とし、その零点において遮断す
る方法とが知られている。これらの方法のうち、
振動電流を重畳する前者の方法においては、振動
電流の発生源として大量のコンデンサと、このコ
ンデンサをあらかじめ充電する高圧の昇圧変圧器
と高耐圧の整流器と、リアクトルと、放電装置と
その制御装置などとを必要とし、経済的負担が極
めて重い。また遮断器中のアーク抵抗によつて電
流の零点をつくる方法は、半導体遮断器のように
順方向電圧降下の小さいものには適用できないと
いう欠点があつた。
Conventionally, as a method for interrupting short-circuit current that does not pass through the zero point using an AC circuit breaker, there are two methods: superimposing a high-frequency oscillating current on this short-circuit current to forcibly create a zero point and interrupting the current, and another method that uses an AC circuit breaker to interrupt the short-circuit current that does not pass through the zero point. Therefore, a method is known in which the direct current component of this short circuit current is rapidly attenuated to form a waveform that passes through a zero point, and the waveform is cut off at that zero point. Of these methods,
In the former method of superimposing oscillating current, a large number of capacitors are used as sources of oscillating current, a high-voltage step-up transformer for pre-charging the capacitors, a high-voltage rectifier, a reactor, a discharge device, its control device, etc. The economic burden is extremely heavy. Furthermore, the method of creating a current zero point using arc resistance in the circuit breaker has the drawback that it cannot be applied to devices such as semiconductor circuit breakers, which have a small forward voltage drop.
そこで経済的負担が小さくかつ順方向電圧降下
の小さい半導体遮断器にも適用しうる遮断方法と
して、零点を通過しない電流と交差しない電流を
最初に遮断することにより、前記零点を通過しな
い電流が零点を通過するようになりまた零点を通
過していた残りの1相の電流も零点を通過しなく
なることがない点に着目し、零点を通過しない電
流と交差しない電流を最初に遮断するという方法
が提案されている(特願昭58−20503)。しかしな
がらこの方法においては最初に遮断される相を検
出するのに、各相の電流が零点を通過するか否か
の検出のほか、2つの相の電流が互に交差するか
否かの検出をも必要とし、このためにたとえばそ
の検出装置に入力すべき電流波形を得るための変
流器3相分を必要とすることから、経済性の面で
なお改善されるべき点を残していた。 Therefore, as a breaking method that can be applied to semiconductor circuit breakers with a small economic burden and a small forward voltage drop, by first cutting off the current that does not pass through the zero point and the current that does not intersect, the current that does not pass through the zero point becomes the zero point. Focusing on the fact that the current in the remaining one phase, which was passing through the zero point, does not stop passing through the zero point, there is a method of first cutting off the current that does not pass through the zero point and the current that does not intersect. It has been proposed (Japanese Patent Application No. 58-20503). However, in this method, in order to detect the first phase to be cut off, in addition to detecting whether the current of each phase passes through the zero point, it is also necessary to detect whether the currents of two phases cross each other. For this reason, for example, a three-phase current transformer is required to obtain a current waveform to be input to the detection device, so there remains a point to be improved in terms of economy.
この発明は上記従来の欠点を除去し、経済性が
さらに高く、遮断器のアーク抵抗の大小にかかわ
らず普遍的に適用できる遮断方法を提供すること
を目的とする。
It is an object of the present invention to provide a breaking method that eliminates the above-mentioned conventional drawbacks, is more economical, and is universally applicable regardless of the magnitude of the arc resistance of the circuit breaker.
この発明は零点を通過する2つの相の電流のう
ち、隣り合つた零点間間隔の差の絶対値が大きい
方の相の電流を最初に遮断することにより、残り
の2相の電流が零点を通過するようになることに
着目してなされたものである。これにより遮断さ
れるべき所定の時間内において、零点を通過しな
い1相の短絡電流が零点を通るようになるととも
に、零点を通過していた相が零点を通らなくなる
ということもないことから、遮断器のアーク抵抗
の大小にかかわらず普遍的に交流遮断器の適用を
可能にするとともに、最初に遮断すべき相の検出
を、各相電流の零点間間隔の計測とその大小比較
とのみから行ない、2相電流の交差の有無の検出
のような2相に跨がる検出を不要のものとして、
遮断方法の経済性をさらに高めようとするもので
ある。
In this invention, among the two phase currents passing through the zero point, the current of the phase with the larger absolute value of the difference in the interval between adjacent zero points is cut off first, so that the current of the remaining two phases passes the zero point. This was done with a focus on the ability to pass through. As a result, during the predetermined period of time to be cut off, the short circuit current of one phase that does not pass through the zero point will pass through the zero point, and the phase that was passing through the zero point will not stop passing through the zero point, so the cutoff will occur. This makes it possible to universally apply AC circuit breakers regardless of the magnitude of the arc resistance of the device, and the phase to be shut off is first detected only by measuring the interval between the zero points of each phase current and comparing their magnitudes. , eliminating the need for detection across two phases, such as detecting the presence or absence of two-phase current crossings.
This is an attempt to further improve the economic efficiency of the shutoff method.
第1図に零点を通過しない短絡電流がT相に流
通する場合の三相短絡電流の波形の例を示す。同
図において、R相の電流は時刻A,B,E,F等
において零点を通過し、S相の電流は時刻C,
D,G,H等において零点を通過している。ここ
で時刻A,B間の間隔とB,E間の間隔との差異
は時刻C,D間の間隔とD,Gの間隔との差異よ
りも小さい。このように三相短絡電流の遮断に際
し隣り合つた零点間間隔の差の絶対値が小さい方
の相すなわちR相の電流をその第1の零点Aにお
いて遮断すると、第2図に示すように当初零点を
有していたS相の電流が零点のない電流となり、
S、T相の電流はともに零点を通過しなくなる。
第3図は第2図と同様にR相の電流をその第2の
零点Bにおいて最初に遮断した場合を示す。この
場合にも第2図と同様、S、T相の電流には零点
を生じない。
FIG. 1 shows an example of the waveform of a three-phase short-circuit current when a short-circuit current that does not pass through the zero point flows through the T phase. In the figure, the R-phase current passes through zero points at times A, B, E, F, etc., and the S-phase current passes at times C, F, etc.
It passes through the zero point at D, G, H, etc. Here, the difference between the interval between times A and B and the interval between times B and E is smaller than the difference between the interval between times C and D and the interval between D and G. In this way, when interrupting a three-phase short-circuit current, if the current of the phase with the smaller absolute value of the difference in the spacing between adjacent zero points, that is, the R phase, is interrupted at its first zero point A, the initial The S-phase current that had a zero point becomes a current without a zero point,
Both the S and T phase currents no longer pass through the zero point.
FIG. 3 shows the case where the R-phase current is first cut off at its second zero point B, similar to FIG. 2. In this case, as in FIG. 2, no zero point occurs in the S and T phase currents.
そこで第4図に示すように隣り合つた零点間間
隔の差の絶対値が大きい方の相すなわちS相の電
流をその第1の零点Cにおいて最初に遮断する
と、残る2相すなわちR、T相の電流はともに零
点を通過する波形となる。第5図は第4図と同様
にS相の電流をその第2の零点Dにおいて最初に
遮断した場合を示す。この場合にも第4図と同
様、R、T相の電流は零点を通過する。このよう
に隣り合つた零点間間隔の差の絶対値が大きい方
の相の短絡電流を最初に遮断することにより、零
点のない短絡電流をいずれかの相に有する三相短
絡電流を通常の交流遮断器または交流回路用半導
体遮断器によつて遮断できることが判明した。従
つてこのような遮断方法を適用することによつ
て、近年、大容量の発変電所において問題となつ
ている零点のない短絡電流の遮断を極めて経済的
に遂行することができる。 Therefore, as shown in Fig. 4, if the current in the phase with the larger absolute value of the difference in the spacing between adjacent zero points, that is, the S phase, is first interrupted at its first zero point C, the current in the remaining two phases, that is, the R and T phases, is cut off at its first zero point C. Both currents have waveforms that pass through the zero point. FIG. 5 shows the case where the S-phase current is first interrupted at its second zero point D, similar to FIG. 4. In this case, as in FIG. 4, the R and T phase currents pass through the zero point. In this way, by first interrupting the short-circuit current of the phase with the larger absolute value of the difference in the spacing between adjacent zero points, the three-phase short-circuit current that has a short-circuit current without a zero point in one of the phases can be converted into a normal alternating current. It was found that the circuit breaker or the semiconductor circuit breaker for AC circuits can be used to interrupt the operation. Therefore, by applying such a breaking method, it is possible to very economically cut off short-circuit currents without zero points, which have recently become a problem in large-capacity power generation and substations.
以上に述べた、最初に遮断すべき相の検出はた
とえば次のような方法によつて行なうことができ
る。 The above-mentioned detection of the phase to be cut off first can be performed, for example, by the following method.
第6図は各相電流における隣り合つた零点間間
隔の差の絶対値が最大となる相を検出する方法を
説明するためのブロツク図であり、第7図にその
検出手段回路の一例を示す。 FIG. 6 is a block diagram for explaining a method for detecting the phase in which the absolute value of the difference between the intervals between adjacent zero points in each phase current is maximum, and FIG. 7 shows an example of the detection means circuit. .
第6図の主回路1の各相に設けられた変流器2
の2次側電流における零点検出手段3は以下のと
おりである。第7図に示した零点検出回路3の逆
並列されたダイオード31にて前記2次側電流を
整流し、抵抗32にて電圧に変換しコンデンサ3
3に充電させ充電電圧VCを発生させる、また抵
抗34により変換した電圧VRの零点近傍での値
と前記VCの値が一致する時点でパルストランス
35が導通しサイリスタ36のゲートに電圧が発
生し前記2次電流の第1零点に対応するパルス信
号をVPに発生させることにより零点を検出する。 Current transformer 2 installed in each phase of main circuit 1 in Fig. 6
The zero point detection means 3 for the secondary current is as follows. The secondary current is rectified by the anti-parallel diode 31 of the zero point detection circuit 3 shown in FIG.
3 to generate a charging voltage V C , and when the value near the zero point of the voltage V R converted by the resistor 34 and the value of V C match, the pulse transformer 35 becomes conductive and generates a voltage at the gate of the thyristor 36. occurs, and the zero point is detected by generating a pulse signal at V P corresponding to the first zero point of the secondary current.
このような動作を繰り返し、順次2次側電流の
各零点を検出し以下の零点間間隔検出手段によ
り、検出する相の零点間間隔の差を求める。 By repeating such an operation, each zero point of the secondary current is sequentially detected, and the difference in the spacing between zero points of the detected phases is determined using the following zero point spacing detection means.
前記の第1の零点に対応するパルス信号t1によ
つて、第7図の零点間間隔検出回路の抵抗とコン
デンサからなる第1積分器4のコンデンサに、ス
イツチング素子42が導通することにより定電圧
直流電源41より充電する。この場合前記スイツ
チング素子42が導通すると抵抗コンデンサから
決まる時定数をもつてスイツチング素子43が導
通する。次に同様に零点検出手段3から得られた
第2零点のパルス信号t2によつてスイツチング素
子44が導通することによつて第1積分器4の充
電電圧を放電させることにより第1積分器4の作
動を停止する。この場合の前記した第1積分器4
の作動中のコンデンサの充電電圧は第8図に示す
ように最大値V1をもつた電圧波形を示す。 The pulse signal t1 corresponding to the first zero point causes the switching element 42 to conduct to the capacitor of the first integrator 4, which is composed of a resistor and a capacitor, of the zero-point interval detection circuit shown in FIG. It is charged from a voltage DC power source 41. In this case, when the switching element 42 becomes conductive, the switching element 43 becomes conductive with a time constant determined by the resistance capacitor. Next, the switching element 44 is made conductive by the pulse signal t2 of the second zero point obtained from the zero point detection means 3 in the same manner, and the charging voltage of the first integrator 4 is discharged. Stop the operation of 4. In this case, the first integrator 4
The charging voltage of the capacitor during operation shows a voltage waveform with a maximum value V 1 as shown in FIG.
更に上記第2零点パルス信号t2によつてスイツ
チング素子45も同時に導通するので第2積分器
5を構成するコンデンサが定電圧直流電源41に
より充電される。またスイツチング素子45が導
通するとスイツチング素子46が導通する。次に
第3零点のパルス信号t3によつてスイツチング素
子47が導通し第2積分器5の作動を停止させ
る。この場合も第8図のように第2積分器5の作
動中の充電電圧は最大値V2をもつた電圧波形を
示す。 Further, since the switching element 45 is also made conductive at the same time by the second zero point pulse signal t2 , the capacitor constituting the second integrator 5 is charged by the constant voltage DC power supply 41. Further, when switching element 45 becomes conductive, switching element 46 becomes conductive. Next, the switching element 47 is brought into conduction by the pulse signal t3 at the third zero point, and the operation of the second integrator 5 is stopped. In this case as well, as shown in FIG. 8, the charging voltage during operation of the second integrator 5 shows a voltage waveform having a maximum value V2 .
第1積分器4および第2積分器5のそれぞれの
コンデンサに充電された充電電圧V1およびV2は、
第8図に示したように零点間間隔が長いほど高い
ので、これらの充電電圧V1,V2を演算増幅器を
用いた減算器6に入力し、その差でもつてその相
における隣り合つた零点間間隔(t2−t1)と(t3
−t2)の差を求めることができる。以下各相にお
いての零点間間隔の差を求め、それらの値の絶対
値を求める演算増幅器を用いた絶対値回路7を経
由して比較器8に入力して比較することにより、
零点間間隔が最大の相すなわち最初に遮断すべき
相を検出することができる。この場合零点を有し
ない電流は零点検出手段3からの出力がないから
比較器8への入力も0であり、零点間間隔の差も
零として他の相と比較される。従つてこの相が遮
断第1相として検出されることはない。 The charging voltages V 1 and V 2 charged to the respective capacitors of the first integrator 4 and the second integrator 5 are:
As shown in Fig. 8, the longer the interval between zero points, the higher the value, so these charging voltages V 1 and V 2 are input to a subtracter 6 using an operational amplifier, and the difference is used to calculate the difference between adjacent zero points in that phase. interval (t 2 −t 1 ) and (t 3
−t 2 ) can be calculated. By calculating the difference in the interval between zero points in each phase and inputting it to the comparator 8 via an absolute value circuit 7 using an operational amplifier to calculate the absolute value of these values,
It is possible to detect the phase with the largest interval between zeros, that is, the phase that should be shut off first. In this case, since there is no output from the zero point detecting means 3 for a current having no zero point, the input to the comparator 8 is also 0, and the difference in interval between zero points is also assumed to be zero and is compared with other phases. Therefore, this phase will not be detected as the first phase of interruption.
このようにして最初に遮断すべき相が検出され
た後、この相が遮断第1相として最初に電流を遮
断するように遮断動作を制御する方法の一例を以
下に説明する。 After the phase to be cut off first is detected in this way, an example of a method for controlling the cutoff operation so that current is cut off first in this phase as the first cutoff phase will be described below.
第9図はこの制御方法をブロツク図で示したも
のであつて、主回路1の各相には前述のように遮
断第1相を検出するための入力装置として変流器
2が設けられ、その2次側電流を入力として遮断
第1相を検出する初相判別手段9に接続される。
この初相判別手段9は前述の第6図における3な
いし8からなる。一方、主回路1の短絡電流によ
つて遮断指令を出力する保護継電器10からの出
力は以下に説明する論理積の回路11に入る。 FIG. 9 is a block diagram showing this control method, in which each phase of the main circuit 1 is provided with a current transformer 2 as an input device for detecting the first phase being cut off as described above. The secondary current is input to the first phase determining means 9 which detects the first phase being cut off.
This initial phase discriminating means 9 consists of 3 to 8 in FIG. 6 mentioned above. On the other hand, the output from the protective relay 10, which outputs a cut-off command based on the short-circuit current of the main circuit 1, enters an AND circuit 11, which will be described below.
周知のように、通常の交流遮断器においては、
短絡電流を遮断できるために必要な最小限のアー
ク時間が存在し、このアーク時間以上の時間が経
過すれば、どの時点で短絡電流の零点がきてもそ
の零点において遮断することができる。従つて最
初に遮断されるべき相すなわちS相が第10図
(第1図の時間軸を延長したもの)の時刻Gにお
いて検出された後、このつぎの小ループすなわち
時刻MとNとの間の波高値上に最小アーク時間の
位置がくるように遮断器の遮断指令を与えること
により、S相の短絡電流が確実に時刻Nにおいて
最初に遮断される。この遮断指令の位置は、最小
アーク時間の位置がS相短絡電流中の交流分の波
高値上にあるので、直流分の大小に関係なく交流
分の波形のみを利用して決定することができる。
すなわち第10図においてS相の電流が検出され
た後の最初の波高値の位置Pをたとえば抵抗とコ
ンデンサからなる微分回路を使用して検出し、こ
の位置からある時間経過した位置で遮断指令を与
えた場合に、最小アーク時間の位置が前記の時刻
MとNとの間の波高値上にくるようにすればよ
い。 As is well known, in a normal AC breaker,
There is a minimum arcing time necessary to interrupt the short-circuit current, and if a time longer than this arcing time has elapsed, the short-circuit current can be interrupted at any point where the zero point occurs. Therefore, after the first phase to be shut off, that is, the S phase, is detected at time G in FIG. 10 (an extension of the time axis in FIG. 1), this next small loop, that is, between times M and N By giving the interrupting command to the circuit breaker so that the position of the minimum arc time is on the peak value of , the S-phase short-circuit current is reliably interrupted first at time N. The position of this cutoff command can be determined using only the waveform of the AC component, regardless of the magnitude of the DC component, since the position of the minimum arc time is on the peak value of the AC component in the S-phase short circuit current. .
That is, in Fig. 10, the position P of the first peak value after the S-phase current is detected is detected using, for example, a differential circuit consisting of a resistor and a capacitor, and a cutoff command is issued after a certain period of time has elapsed from this position. In this case, the position of the minimum arc time may be placed on the peak value between the above-mentioned times M and N.
第9図の12は主回路1の各相に設けられた変
流器17のうち最初に遮断すべき相の変流器の2
次側電流のみを通過させる相選択手段であつて、
どの相を選択すべきかの指示は初相判別手段9か
ら与えられる。また13は選択された相の電流の
波高値の位置すなわち波高点を検出する手段であ
る。最初に遮断される相のこの波高点の信号と、
保護継電器10からの三相遮断の指令との論理積
の結果が11から出力され、この出力信号が14
によつて所定の時間遅延して遮断器の引外しコイ
ルに到達すると、最初に遮断すべき相の電流がま
ず遮断される。ここで遮断器が1個の共通操作器
によつて三相一括操作される場合には、つづく2
相の電流が零値を通過する際にその零値において
遮断される。もし遮断器が各相個別に設けられた
操作器によつて各相が独立に開閉駆動される構成
の場合は、時間遅れを付与する遅延手段14から
の出力を、約0.5サイクルの時間遅れを付与する
遅延手段15に導き、最初に遮断される相からこ
の時間だけ遅れて他の2相を遮断することにより
三相短絡電流の遮断が可能となる。なお最初に遮
断された相の補助接触子のa接点は遮断器本体の
遮断動作とともに開放され、このa接点と直列に
接続されている引外しコイルの電流も遮断されて
おり、15から時間遅れをもつて遮断器に伝達さ
れる遮断指令が三相分であつても、最初に遮断し
た相の引外しコイルに再び遮断指令が伝達される
ことはない。 12 in FIG. 9 is the current transformer 2 of the phase to be cut off first among the current transformers 17 provided in each phase of the main circuit 1.
A phase selection means for passing only the next-side current,
An instruction as to which phase should be selected is given from the initial phase determining means 9. Further, 13 is means for detecting the position of the peak value of the current of the selected phase, that is, the peak point. The signal at this peak point of the phase that is first blocked,
The result of the AND with the three-phase cutoff command from the protective relay 10 is output from 11, and this output signal is output from 14.
When the tripping coil of the circuit breaker is reached after a predetermined time delay, the current of the phase to be interrupted first is interrupted first. If the circuit breaker is operated in three phases by one common operating device, please refer to the following 2.
When the phase current passes through the zero value, it is cut off at that zero value. If the circuit breaker is constructed such that each phase is driven to open and close independently by an operating device provided for each phase, the output from the delay means 14 that provides a time delay is delayed by about 0.5 cycles. The three-phase short-circuit current can be interrupted by leading to the delay means 15 to interrupt the other two phases after a delay of this time from the first phase to be interrupted. Note that the A contact of the auxiliary contact of the phase that was cut off first is opened with the breaking operation of the circuit breaker body, and the current in the tripping coil connected in series with this A contact is also cut off. Even if the shutdown command transmitted to the circuit breaker is for three phases, the shutdown command will not be transmitted again to the tripping coil of the phase that was shut off first.
この発明はいずれか1相の短絡電流が零点を通
過しない三相短絡電流の遮断に際し、零点を通過
する2つの相の電流のうち、隣り合つた零点間間
隔の差の絶対値が大きい方の相の電流を最初に遮
断することにより、残りの2相の電流に自然に零
点を生ぜしめるものであるから、アーク電圧また
は遮断器中の電圧降下の大小にかかわらず普遍的
に適用できるのみならず、最初に遮断すべき相の
検出を、各相電流の零点間間隔の計測とその大小
比較とのみから行ない、2相電流の交差の有無の
検出のような2相に跨がる検出を不要のものとし
たので、たとえばこれに必要な変流器を節約する
ことができ、遮断方法の経済性がさらに高められ
るという効果が得られる。
When interrupting a three-phase short-circuit current in which the short-circuit current of any one phase does not pass through the zero point, the current of the two phases passing through the zero point, whichever has the larger absolute value of the difference in interval between adjacent zero points, By first interrupting the phase current, a zero point is naturally created in the remaining two phase currents, so it is universally applicable regardless of the magnitude of the arc voltage or the voltage drop in the circuit breaker. First, the phase to be shut off is first detected only by measuring the interval between the zero points of each phase current and comparing their magnitudes. Since it is unnecessary, for example, the current transformer required for this can be saved, and the economical efficiency of the interrupting method can be further improved.
第1図はT相の短絡電流が零点を通過しない場
合の三相短絡電流の波形の例を示す図、第2図は
零点を通過する2つの相の電流のうち、隣り合つ
た零点間間隔の差の絶対値が小さい方の相すなわ
ちR相の電流をその第1零点Aにおいて遮断した
とき、遮断後の残り2相の電流波形の変化を示す
図、第3図は同じくR相の電流をその第2零点B
において最初に遮断したとき、遮断後の残り2相
の電流波形の変化を示す図、第4図は前記零点間
間隔の差の絶対値が大きい方の相すなわちS相の
電流をその第1零点Cにおいて最初に遮断したと
き、遮断後の残り2相の電流波形の変化を示す
図、第5図は同じくS相の電流をその第2零点D
において最初に遮断したとき、遮断後の残り2相
の電流波形の変化を示す図、第6図は各相電流に
おける隣り合つた零点間間隔の差の絶対値が最大
となる相を検出する方法の例を示す図、第7図は
第6図の具体的な実施例検出を示す構成図、第8
図は第7図における要部における波形図、第9図
は最初に遮断される相が検出された後、その相が
遮断第1相として電流を最初に遮断するように遮
断動作を制御する方法の一例を示す図、第10図
は第1図の時間軸を延長した図である。
Figure 1 is a diagram showing an example of the waveform of a three-phase short-circuit current when the T-phase short-circuit current does not pass through the zero point, and Figure 2 shows the interval between adjacent zero points of the two phase currents that pass through the zero point. When the current of the phase with the smaller absolute value of the difference, that is, the R phase, is interrupted at its first zero point A, the current waveforms of the remaining two phases change after the interruption. Figure 3 shows the current of the R phase as well. its second zero point B
Figure 4 shows the changes in the current waveforms of the remaining two phases after the interruption when the current is interrupted for the first time. Figure 5 shows the changes in the current waveforms of the remaining two phases after the interruption when the current is first interrupted at C.
Figure 6 shows the changes in the current waveforms of the remaining two phases after the first shutdown in , and the method for detecting the phase where the absolute value of the difference in the interval between adjacent zero points in each phase current is maximum. FIG. 7 is a block diagram showing a specific example of detection in FIG. 6, and FIG.
The figure is a waveform diagram of the main part in Figure 7, and Figure 9 is a method of controlling the interrupting operation so that after the first phase to be interrupted is detected, that phase is the first phase to be interrupted and the current is interrupted first. FIG. 10 is an extension of the time axis of FIG. 1.
Claims (1)
ない三相短絡電流を遮断する方法であつて、前記
各相の短絡電流の零点を検出する零点検出手段
と、該零点検出手段により検出した各相の短絡電
流の零点と、それぞれに続く各相での隣り合つた
零点との零点間間隔の差の絶対値を求める零点間
間隔検出手段と、零点間間隔検出手段により求め
られた零点を通過する2つの相での隣り合つたそ
れぞれの零点間間隔の差の絶対値の大・小を比較
する比較手段とからなり、この比較手段より得ら
れた零点間間隔の差の最大の相を最初に遮断する
相とすることを特徴とする三相短絡電流の遮断方
法。1. A method for interrupting a three-phase short-circuit current in which the short-circuit current of any one of the three phases does not pass through the zero point, comprising a zero-point detection means for detecting the zero point of the short-circuit current of each phase, and a zero-point detection means for detecting the zero point of the short-circuit current of each phase. Inter-zero interval detection means for determining the absolute value of the difference in inter-zero interval between the zero point of the short-circuit current of each phase and the adjacent zero points of each subsequent phase; It consists of a comparison means for comparing the magnitude of the absolute value of the difference in the interval between two adjacent zero points in two passing phases, and the phase with the maximum difference in the interval between zero points obtained by this comparison means is A method for interrupting a three-phase short-circuit current, characterized in that the phase is the first phase to be interrupted.
Priority Applications (4)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58189658A JPS6082016A (en) | 1983-10-11 | 1983-10-11 | 3-phase shortcircuit current interrupting method |
| EP84112088A EP0142022B1 (en) | 1983-10-11 | 1984-10-09 | Device for the interruption of currents |
| DE8484112088T DE3463321D1 (en) | 1983-10-11 | 1984-10-09 | Device for the interruption of currents |
| AT84112088T ATE26773T1 (en) | 1983-10-11 | 1984-10-09 | ARRANGEMENT FOR SHUTTING OFF CURRENT. |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP58189658A JPS6082016A (en) | 1983-10-11 | 1983-10-11 | 3-phase shortcircuit current interrupting method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS6082016A JPS6082016A (en) | 1985-05-10 |
| JPH053206B2 true JPH053206B2 (en) | 1993-01-14 |
Family
ID=16244999
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP58189658A Granted JPS6082016A (en) | 1983-10-11 | 1983-10-11 | 3-phase shortcircuit current interrupting method |
Country Status (4)
| Country | Link |
|---|---|
| EP (1) | EP0142022B1 (en) |
| JP (1) | JPS6082016A (en) |
| AT (1) | ATE26773T1 (en) |
| DE (1) | DE3463321D1 (en) |
Families Citing this family (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JP2660842B2 (en) * | 1988-02-23 | 1997-10-08 | 株式会社明電舎 | Overvoltage protection device for vacuum switchgear |
| JP5159075B2 (en) * | 2006-09-25 | 2013-03-06 | 株式会社東芝 | Circuit breaker switching control device |
Family Cites Families (3)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| DE1563656A1 (en) * | 1966-01-26 | 1970-02-19 | Siemens Ag | Circuit breaker protection |
| SE338092B (en) * | 1968-03-15 | 1971-08-30 | Asea Ab | |
| JPS57101514A (en) * | 1980-12-15 | 1982-06-24 | Tokyo Shibaura Electric Co | Defect current breaking system |
-
1983
- 1983-10-11 JP JP58189658A patent/JPS6082016A/en active Granted
-
1984
- 1984-10-09 EP EP84112088A patent/EP0142022B1/en not_active Expired
- 1984-10-09 DE DE8484112088T patent/DE3463321D1/en not_active Expired
- 1984-10-09 AT AT84112088T patent/ATE26773T1/en not_active IP Right Cessation
Also Published As
| Publication number | Publication date |
|---|---|
| EP0142022B1 (en) | 1987-04-22 |
| ATE26773T1 (en) | 1987-05-15 |
| EP0142022A1 (en) | 1985-05-22 |
| DE3463321D1 (en) | 1987-05-27 |
| JPS6082016A (en) | 1985-05-10 |
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