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JPS644411B2 - - Google Patents
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JPS644411B2 - - Google Patents

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Publication number
JPS644411B2
JPS644411B2 JP11140180A JP11140180A JPS644411B2 JP S644411 B2 JPS644411 B2 JP S644411B2 JP 11140180 A JP11140180 A JP 11140180A JP 11140180 A JP11140180 A JP 11140180A JP S644411 B2 JPS644411 B2 JP S644411B2
Authority
JP
Japan
Prior art keywords
zero
waveform
surge
distribution line
lightning
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
Application number
JP11140180A
Other languages
Japanese (ja)
Other versions
JPS5736536A (en
Inventor
Yutaka Urano
Hideo Kobayashi
Atsushi Tegawa
Yoshihiro Kawasaki
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.)
Meidensha Corp
Chubu Electric Power Co Inc
Original Assignee
Meidensha Corp
Chubu Electric Power Co Inc
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 Meidensha Corp, Chubu Electric Power Co Inc filed Critical Meidensha Corp
Priority to JP11140180A priority Critical patent/JPS5736536A/en
Publication of JPS5736536A publication Critical patent/JPS5736536A/en
Publication of JPS644411B2 publication Critical patent/JPS644411B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は配電用変電所一括の襲雷を検出し、配
電線を避災停電させる装置に関するもので、配電
線の各相に誘導する雷サージと母線に接続された
零相変圧器より得られる零相電圧波形が類似であ
り雷撃の誘導を受けた配電線の零相変流器より得
られる零相電流と前記零相電圧の間に一定の関係
があることを利用したもので、その目的とすると
ころは、特別な検出用センサを必要とせずに従来
の零相変圧器(GPT)と零相変流器(ZCT)の
出力を利用して雷サージの検出を可能ならしめる
ところにある。
[Detailed Description of the Invention] The present invention relates to a device that detects lightning strikes in distribution substations and causes disaster-prevention power outage of distribution lines. The zero-sequence voltage waveforms obtained from the zero-sequence transformers are similar and there is a certain relationship between the zero-sequence current obtained from the zero-sequence current transformer of the distribution line that has been induced by a lightning strike and the zero-sequence voltage. The purpose is to detect lightning surges using the output of conventional zero-phase transformers (GPTs) and zero-phase current transformers (ZCTs) without the need for special detection sensors. It lies in making it possible.

従来の雷警報装置には、雷放電に伴つて発生す
る空電パルスを受信したり、地上電界強度を測定
したりする方式があるが、いずれの場合もアンテ
ナ装置を必要としていたために、装置自体、特別
なものとなつていた。また、雷撃点を測定する装
置として、電界と磁界の比で求めたり、雷空電サ
ージを各電気所で受信し、雷空電サージの到着す
る時間差により求める方式などがあるが、この場
合も装置自体特別なものとなり、しかも雷撃点付
近の配電線を避災停電できる可能性はない。
Conventional lightning warning devices include systems that receive aerial pulses generated by lightning discharges and measure ground electric field strength, but in both cases, antenna devices are required, so the device It was something special in itself. In addition, there are devices to measure the point of lightning strike, such as by calculating the ratio of the electric field and magnetic field, or by receiving lightning and air surges at each electrical station and calculating them based on the time difference between the arrival of the lightning and air surges. The device itself would be special, and there is no possibility that it would be possible to perform an emergency power outage on distribution lines near the lightning strike point.

本発明はこの点を鑑みてなされたものであり、
配電用変電所の既設設備である零相変圧器、零相
変流器により得られる情態により、変電所一括の
襲雷を検出する機能と、落雷した近傍の配電線を
検出しその配電線が故障に至ると推測した場合に
避災停電させる機能を備えた装置を提案するもの
である。また、零相電圧、零相電流を入力として
いることで配電線の地絡故障を同一入力より検出
する方向地絡検出機能を容易に付加できるように
した誘導雷サージ検出装置を提案するものであ
る。
The present invention has been made in view of this point,
Based on the conditions obtained from the existing equipment of the distribution substation, such as zero-phase transformers and zero-phase current transformers, it is possible to detect lightning strikes in the entire substation, and to detect nearby distribution lines that have been struck by lightning. We propose a device that has the ability to shut off power outage in case a failure is predicted. We also propose an induced lightning surge detection device that uses zero-sequence voltage and zero-sequence current as inputs, making it easy to add a directional ground fault detection function that detects ground faults in distribution lines from the same input. be.

以下図面を参照して本発明を詳細に説明する。 The present invention will be described in detail below with reference to the drawings.

第1図は雷雲が負極性で近傍落雷時の場合の多
重雷で高さhの線路導体上の任意の点(図中P)
に発生する誘導雷サージの時間変化を示したもの
である。第1図B中のaは主放電によるサージ、
bは雷雲による拘束電荷で生じるサージ、Lは先
行放電によるサージ、Rはaとb重畳したサー
ジ、Dは投搶状先行放電によるサージを示す。図
示のように近傍落雷時には誘導雷サージは双極性
サージとなり、その大きさは点Pの位置により異
なる。
Figure 1 shows multiple lightning in the case of negative polarity thunderclouds and nearby lightning strikes at an arbitrary point on the line conductor at height h (P in the figure).
This figure shows the temporal changes in induced lightning surges that occur during the period. a in Figure 1B is the surge due to the main discharge,
b indicates a surge caused by a restrained charge caused by a thundercloud, L indicates a surge caused by a preceding discharge, R indicates a surge caused by superimposing a and b, and D indicates a surge caused by a cascading preceding discharge. As shown in the figure, when lightning strikes nearby, the induced lightning surge becomes a bipolar surge, and its magnitude differs depending on the position of point P.

第2図は本発明を概念的に示す配電用変電所の
構成例であり、図中1は主変圧器、21〜2o+1
しや断器、3は母線、41〜4oは配電線、51
oは零相変流器、6は零相変圧器、7は本発明
の誘導雷サージ検出装置である。配電線41〜4o
は変電所を中心に放射状に走つており、任意の配
電線近傍に落雷した場合には各相の電圧は母線も
含めて双極性サージの重畳した波形となり、零相
電圧は各相に重畳した双極性サージと相似にな
る。従つて、変電所一括の襲雷を検知するには零
相電圧が双極性サージ(双極性サージの閃絡した
波形を含む)であることを検出すればよい。以
下、上記の正当性を実測結果をもとに示す。
FIG. 2 is a configuration example of a distribution substation conceptually illustrating the present invention, in which 1 is the main transformer, 2 1 to 2 o+1 beams and disconnectors, 3 is the bus bar, and 4 1 to 4 o is distribution line, 5 1 ~
5 o is a zero-phase current transformer, 6 is a zero-phase transformer, and 7 is an induced lightning surge detection device of the present invention. Distribution line 4 1 ~ 4 o
The waves run radially around the substation, and if a lightning strike occurs near any distribution line, the voltage of each phase will become a waveform in which bipolar surges are superimposed, including on the busbar, and the zero-sequence voltage will become a waveform in which bipolar surges are superimposed on each phase. Similar to bipolar surge. Therefore, in order to detect a lightning strike in a substation all at once, it is sufficient to detect that the zero-sequence voltage is a bipolar surge (including the waveform of a bipolar surge). The validity of the above will be shown below based on actual measurement results.

第3図Aは第2図の配電線4iの引出口におい
て、a相、b相、c相の各相の対地電圧を測定し
た結果である。この図より、誘導雷サージは配電
線各相に同時に進入し、波高値、および波形もほ
ぼ等しいことがわかる。この場合のa相に重畳し
た誘導雷サージは第3図Bに示す通りであり、双
極性サージとなつている。これは、配電線に隣接
した地点での近傍落雷時である。また、測定回線
が停電中の誘導雷サージを観測した結果から測定
回線の近傍落雷時にも双極性サージとなり、落雷
地点が測定回線より遠方になるに従つて双極性サ
ージの負極性部分は低い値となり完全に遠方にな
ると負極性部分の存在しない正極性部分のみの単
極性サージとなることが確かめられている。
FIG. 3A shows the results of measuring the ground voltage of each phase, a phase, b phase, and c phase, at the outlet of the distribution line 4 i in FIG. 2. This figure shows that induced lightning surges enter each phase of the distribution line at the same time, and the peak values and waveforms are almost the same. The induced lightning surge superimposed on the a-phase in this case is as shown in FIG. 3B, and is a bipolar surge. This occurs when a nearby lightning strike occurs at a point adjacent to a power distribution line. In addition, the results of observing induced lightning surges when the measurement line is out of power show that bipolar surges occur even when lightning strikes near the measurement line, and the negative polarity portion of the bipolar surge decreases as the lightning strike point becomes further away from the measurement line. It has been confirmed that when the surge is completely far away, it becomes a unipolar surge with only the positive polarity part and no negative polarity part.

また誘導雷サージの波高値が線路に施設されて
いる工作物の衝撃絶縁耐電圧に比べて低い傾向に
あるが、この理由としては配電線に生じる誘導雷
サージの電位分布は線路上一様に分布するのでは
なく、落雷点近傍を中心に急峻な分布状態を示
し、線路工作物が閃絡しない場合でも配電線引出
口に進入する誘導雷サージは低くなると考えられ
る。
In addition, the peak value of induced lightning surges tends to be lower than the shock insulation withstand voltage of the structures installed on the lines, but the reason for this is that the potential distribution of induced lightning surges that occur on distribution lines is Rather than being distributed, it shows a steep distribution centered around the lightning strike point, and it is thought that the induced lightning surge that enters the distribution line outlet will be low even if there is no flash fault on the line structure.

第3図Cは誘導雷サージの閃絡波形、Dは閃絡
により瞬間故障に至つた波形であり、双極性サー
ジの負極性部分で閃絡を生じている。この閃絡は
各配電線の各柱上に施設されている工作物特有の
BIL(Basic Insulation Level)に依存している
ものと考えられる。
FIG. 3C shows a flashflash waveform of an induced lightning surge, and D shows a waveform that leads to an instantaneous failure due to a flashflash, and the flashflash occurs in the negative polarity portion of a bipolar surge. This flash fault is caused by structures installed on each pole of each distribution line.
It is thought that it depends on BIL (Basic Insulation Level).

第4図A,Bは第3図B,Dに示した誘導雷サ
ージ波形と第2図に示す零相変圧器6より得られ
る零相電圧(V0サージ)の比較を示したもので、
同図Aには閃絡のない場合をBには閃絡の場合を
示し両方共に良く一致している。従つて、誘導雷
サージは零相変圧器より得ることができる。
Figures 4A and 4B show a comparison between the induced lightning surge waveforms shown in Figures 3B and D and the zero-sequence voltage (V 0 surge) obtained from the zero-phase transformer 6 shown in Figure 2.
Figure A shows the case without flash faults, and B shows the case with flash faults, both of which are in good agreement. Therefore, induced lightning surge can be obtained from a zero-phase transformer.

第5図は配電線41の近傍落雷時の多重雷にお
ける零相変圧器6より得られた零相電圧と各配電
線(41〜45、n=5)の零相変流器51〜55
り得られた零相電流I01〜I05の関係を示したもの
である。この関係から、雷撃点近傍の配電線の零
相電流の値は大きく、極性は他の配電線と逆にな
つている。これは通常の地絡故障と同様に考えら
れる。従つて、零相電圧が誘導雷サージであるこ
とを条件として、各配電線の零相電流の絶対値比
較、あるいは極性比較を行うことにより、落雷近
傍の配電線を検出できる。
Figure 5 shows the zero-sequence voltage obtained from the zero-phase transformer 6 during multiple lightning strikes in the vicinity of the distribution line 4 1 and the zero-phase current transformer 5 of each distribution line (4 1 to 4 5 , n=5). 1 to 55 shows the relationship between zero-sequence currents I 01 to I 05 . Because of this relationship, the value of the zero-sequence current in the distribution line near the lightning strike point is large, and the polarity is opposite to that of other distribution lines. This can be considered similar to a normal ground fault. Therefore, on the condition that the zero-sequence voltage is an induced lightning surge, by comparing the absolute value or polarity of the zero-sequence current of each distribution line, it is possible to detect a distribution line near a lightning strike.

第6図は上述のことを考慮して第2図における
誘導雷サージ検出装置7をデイジタル処理装置で
構成した一実施例を示す。
FIG. 6 shows an embodiment in which the induced lightning surge detection device 7 in FIG. 2 is constructed with a digital processing device in consideration of the above.

入力V0,I01〜I0oは第2図の零相変圧器6、零
相変流器51〜5oで得られた情報であり、所定の
周期でサンプルホールド(S/H)80〜8o、マ
ルチプレクサ(MPX)9、A/D変換器10に
より順次A/D変換されてデイジタルデータとな
り、メモリ11にDMAする。CPu12はメモリ
11に格納されたデータにより、所定の演算処理
を行い、結果をI/O13により出力する。整定
I/F14は処理に必要な整定を行うものであ
る。
The inputs V 0 , I 01 to I 0o are information obtained from the zero-phase transformer 6 and zero-phase current transformers 5 1 to 5 o in FIG. 0 to 8 o , are sequentially A/D converted by a multiplexer (MPX) 9 and an A/D converter 10 to become digital data, and are DMAed to a memory 11 . The CPU 12 performs predetermined arithmetic processing using the data stored in the memory 11 and outputs the result through the I/O 13. The setting I/F 14 performs setting necessary for processing.

第7図は、A/D変換された入力V0又はI01
I0oをNサンプルまとめてDMAする様を表わして
おり、CPuの処理はN△t以内に完了する。な
お、△tはサンプリング間隔を表わす。
FIG. 7 shows the A/D converted input V 0 or I 01 ~
This shows how N samples of I 0o are DMAed at once, and the CPU processing is completed within NΔt. Note that Δt represents the sampling interval.

第8図はCPu12の処理をブロツク図で表わし
たものである。
FIG. 8 is a block diagram showing the processing of the CPU 12.

ステツプS1はDMAされた入力情報V0の瞬時デ
ータをメモリ11より取り込む。ステツプS2は
ステツプS1の入力情報をレベル検出し、ステツ
プS3は或る区間TのV0が双極性サージ(閃絡波
形を含む)であるかを処理し、ステツプS4はS3
の結果より、V0が双極性サージかを判断し、ス
テツプS5は時間T1内にN回V0が双極性サージを
検出したかの判断、ステツプS6は襲雷警報を発
生させるもので、各配電線の近傍の落雷を知らせ
る。ステツプS7は最後に双極性サージを認識し
てから、時間T2内に一度も双極性サージを検出
しなかつたかの判断をし、ステツプS8は襲雷警
報を解除して、雷雲が変電所より遠ざかつたこと
を知らせる。
In step S1, the instantaneous data of the DMA input information V0 is fetched from the memory 11. Step S2 detects the level of the input information of step S1, step S3 processes whether V 0 in a certain section T is a bipolar surge (including a flash waveform), and step S4 detects the level of the input information of step S1.
Based on the result, it is determined whether V 0 is a bipolar surge, step S5 is to determine whether V 0 has detected a bipolar surge N times within time T 1 , and step S6 is to generate a lightning warning. Notify of lightning strikes near each power distribution line. Step S7 determines whether no bipolar surge has been detected within the time period T2 since the last bipolar surge was recognized, and step S8 cancels the lightning warning and indicates that the thundercloud has moved away from the substation. Let them know what happened.

ステツプS9はDMAされた入力情報I0iの瞬時デ
ータをメモリより取り込む。ステツプS10はS9の
入力情報をレベル検出し、ステツプS11は区間T
のT0iの極性判別を行い、ステツプS12はS11の結
果により、配電線4i(第2図)の近傍落雷かど
うかを判断し、ステツプS13は配電線4iが故障
に至るかどうかを判断する所で、一例として連続
判定を行い、M回連続かどうかを判断し、ステツ
プS14は配電線4iのトリツプ指令を出す。ステ
ツプS15はi=nの判断をする。結局ステツプS9
〜S15の処理Aはi=1、〜nまで行うことにな
る。
In step S9, the instantaneous data of the DMA input information I0i is fetched from the memory. Step S10 detects the level of the input information of S9, and step S11 detects the level of the input information of S9.
The polarity of T 0i is determined, and step S12 determines whether there is a lightning strike near the distribution line 4i (Fig. 2) based on the result of S11, and step S13 determines whether or not the distribution line 4i will fail. Then, as an example, a continuity determination is made to determine whether or not it has been repeated M times, and a step S14 issues a trip command to the power distribution line 4i. In step S15, it is determined that i=n. Eventually step S9
Process A of ~S15 will be performed from i=1 to ~n.

処理Bにおいて、ステツプS16はステツプS9と
同じステツプS9Aの入力情報を絶対値加算し、ス
テツプS17は区間TのI0iの絶対値加算をし、ステ
ツプS18はS17の絶対値Kiがあるレベルより大き
いことを判断し、ステツプS19は配電線4iの近
傍落雷の可能性があると判断する。ステツプS20
はS15と同じS15Aを経たステツプS19の近傍落雷
の可能性ありと判断された絶対値の比較をし、最
も大きい絶対値の配電線を判断する。ステツプ
S20のnoはS19の処理が行われない場合である。
ステツプS20の処理以後はS13、S14と同様のステ
ツプS13A、S14Aを経てトリツプ指令を得る。
In process B, step S16 adds the absolute value of the input information of step S9A, which is the same as step S9, step S17 adds the absolute value of I0i in interval T, and step S18 adds the absolute value of the input information of step S9A, which is the same as step S9, and step S18 adds the absolute value of the input information of step S9A, which is the same as step S9. Based on this, it is determined in step S19 that there is a possibility of a lightning strike near the distribution line 4i. Step S20
compares the absolute values determined to be likely to be struck by nearby lightning in step S19, which went through the same S15A as S15, and determines the distribution line with the largest absolute value. step
No in S20 means that the process in S19 is not performed.
After the processing in step S20, a trip command is obtained through steps S13A and S14A similar to S13 and S14.

第9図は第8図のフローにおける入力波形図と
入力との関係である。N=2、M=3とした場合
であり、雷撃により配電線3iが故障に至つたケ
ースである。図中V0、I0i、I0jは入力情報であり、
双極性サージ出力は第8図のステツプS4の判断
より得られ、フイーダー出力はステツプS12又は
S20の判断より得られる。襲雷警報出力はステツ
プS6の処理により、トリツプ指令はステツプ
S14、S14Aの処理による。
FIG. 9 shows the relationship between the input waveform diagram and the input in the flow of FIG. 8. This is a case where N=2 and M=3, and the distribution line 3i has broken down due to a lightning strike. In the figure, V 0 , I 0i , and I 0j are input information,
The bipolar surge output is obtained from the judgment in step S4 in Figure 8, and the feeder output is obtained from step S12 or
Obtained from S20's judgment. The lightning warning output is processed in step S6, and the trip command is processed in step S6.
Due to processing of S14 and S14A.

第10図は第8図のステツプS2、S10の処理
(レベル検出処理))を説明するための図であり、
一例としてV0について述べる。DMAされた時点
を現時点とし、その前T区間の入力情報をあるス
ライスレベルV+、V-によりレベル検出する様を
表わしている。入力データv0がv0≧V+の時に
(正)、v0≦−V-の時に(負)、−V-<v0<V+の時
に(零)とする。nOFはT区間の初めの(零)円
間のサンプリング個数、n-は初めの(負)区間
のサンプリング個数、npnは第2番目の(零)区
間のサンプリング個数、n+は最初の(正)区間
のサンプリング個数、nOBは最後の(零)区間の
サンプリング個数を示している。なお、現時点は
時間間隔N△tごとに変わる。
FIG. 10 is a diagram for explaining the processing of steps S2 and S10 (level detection processing) in FIG.
As an example, V 0 will be described. The time point at which DMA is performed is defined as the current time, and the level of the input information of the previous T interval is detected using certain slice levels V + and V - . When the input data v 0 is v 0 ≧V + , it is positive, when v 0 ≦−V , it is negative, and when −V < v 0 < V + , it is zero. n OF is the number of samplings between the first (zero) circles in the T interval, n - is the number of samplings in the first (negative) interval, n pn is the number of samplings in the second (zero) interval, and n + is the number of samplings in the first (negative) interval. The number of samples in the (correct) interval, n OB indicates the number of samples in the last (zero) interval. Note that the current time changes every time interval NΔt.

第11図は第8図のステツプS3、S11の処理
(極性判別処理)を説明するための図であり、一
例として第10図のv0が双極性サージ(閃絡波形
を含まず)であるかどうかの判定フローを示す。
ステツプSS1は、nOF≧NOF(整定値)の判定を行
い、区間Tの初めは(零)が連続することを確認
し、ステツプSS2によりnOB≧NOBの判定を行い区
間Tの終りも(零)が連続することを確認する。
SS3により初めの(零)区間の次は(負)区間で
あることを判定し、SS4によりn-≧N-の判定で
(負)が連続していることを確かめ、SS5ではこ
の(負)区間の次に(零)区間、あるいは(正)
区間が続くことを確かめ、SS6によりNpn≦NOM
の判定により、第2番目の(零)区間はないか、
あるいは短いことを確認し、次にSS7により、n+
≧N+の判定を行い(正)が連続していることを
確かめる。SS1〜SS7の判定がすべてyeSであれ
ばSS8によりこのT区間の波形は双極性サージで
あると判断し、SS1〜SS7の判定の一つでもnp
あればSS9によりこのT区間の波形は双極性サー
ジでないと判断する。なお、閃絡波形についても
同様の方法で検出できる。
FIG. 11 is a diagram for explaining the processing (polarity determination processing) in steps S3 and S11 in FIG. 8. As an example, v 0 in FIG. 10 is a bipolar surge (not including a flash waveform). The flow of determining whether or not
In step SS1, it is determined that n OF ≧N OF (setting value), and it is confirmed that (zero) is continuous at the beginning of section T. In step SS2, it is determined that n OB ≧N OB and at the end of section T. Also check that (zero) is continuous.
SS3 determines that the first (zero) interval is followed by a (negative) interval, SS4 determines that n - ≧ N - and confirms that (negative) is continuous, and SS5 determines that this (negative) Interval followed by (zero) interval or (positive)
Confirm that the interval continues and use SS6 to find N pn ≦N OM
By determining whether there is a second (zero) interval,
Or make sure it's short, then by SS7, n +
Make a judgment of ≧N + and confirm that (correct) results are continuous. If all the judgments from SS1 to SS7 are yeS, the waveform of this T interval is determined to be a bipolar surge by SS8, and if any of the judgments from SS1 to SS7 is n p , the waveform of this T interval is determined by SS9. It is determined that it is not a bipolar surge. Incidentally, the flash waveform can also be detected in a similar manner.

最後に、方向地絡検出機能を付加した場合を述
べる。第12図Aは方向地絡検出装置71と誘導
雷サージ検出装置72を別ハードとした場合であ
り、71のトリツプ指令出力と72のトリツプ指令
出力の論理和により、最終出力を得る誘導雷サー
ジ検出装置73の場合である。
Finally, we will discuss the case where a directional ground fault detection function is added. Figure 12A shows the case where the directional ground fault detection device 7 1 and the induced lightning surge detection device 7 2 are separate hardware, and the final output is determined by the logical sum of the trip command output of 7 1 and the trip command output of 7 2 . This is the case of the induced lightning surge detection device 73 obtained.

第12図Bは方向地絡検出機能を第6図のハー
ド構成をそのままにして付加した場合であり、ス
テツプS21は方向地絡検出処理、S22はその出力、
S23は誘導雷サージ検出処理、S24はその出力、
S25はS22とS24の論理和演算により最終出力を決
定する誘導雷サージ検出装置の場合である。
FIG. 12B shows a case where a directional ground fault detection function is added while leaving the hardware configuration of FIG.
S23 is induced lightning surge detection processing, S24 is its output,
S25 is the case of an induced lightning surge detection device in which the final output is determined by the OR operation of S22 and S24.

以上の説明は雷雲が負極性の場合についての説
明であるが、雷雲が正極性の場合はV0、I0iの極
性が逆になるだけで、本発明を適用できる。
The above explanation is for the case where the thundercloud has negative polarity, but when the thundercloud has positive polarity, the present invention can be applied by simply reversing the polarity of V 0 and I 0i .

以上のとおり、本発明によれば、母線から分岐
する配電線の零相電圧波形と零相電流波形から該
配電線が故障に至るか否か推測することができ、
配電線の機器の損焼や断線等を未然に防止できる
し、襲雷検出に特別な装置を必要としない効果が
ある。
As described above, according to the present invention, it is possible to estimate from the zero-sequence voltage waveform and zero-sequence current waveform of the distribution line branching from the bus bar whether or not the distribution line will malfunction.
It is possible to prevent damage to distribution line equipment, disconnection, etc., and there is no need for special equipment to detect lightning strikes.

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

第1図は雷雲が負極性の場合の多重雷の誘導雷
サージ波形図、第2図は配電用変電所の単線結線
図、第3図は誘導雷サージ波形の実測例を示す
図、第4図は誘導雷サージ波形とV0サージ波形
の比較図、第5図はV0サージ波形とI0サージ波形
の実測例を示す図、第6図は本発明の一実施例の
ハード構成図、第7図はDMAする手法を示す
図、第8図はCPuの処理内容を示すフローチヤー
ト、第9図は本発明における入力波形と出力関係
を示す図、第10図はレベル検出を説明するため
の図、第11図は双極性サージを検出するための
フローチヤート、第12図は地絡検出機能を付加
した本発明の他の実施例を示す図である。 21〜2o+1……しや断器、3……母線、41
o……配電線、51〜5o……零相変流器、6…
…零相変圧器、7……誘導雷サージ検出装置、8
〜8o……サンプルホールド、9……マルチプレ
クサ、10……A/D変換器、11……メモリ、
12……CPU、13……I/O、14……整定
I/F、71……方向地絡検出装置、72……誘導
雷サージ検出装置。
Figure 1 is an induced lightning surge waveform diagram of multiple lightning when a thundercloud has negative polarity, Figure 2 is a single line diagram of a distribution substation, Figure 3 is a diagram showing an actual measurement example of an induced lightning surge waveform, and Figure 4 is a diagram showing an example of the induced lightning surge waveform. The figure is a comparison diagram of the induced lightning surge waveform and the V 0 surge waveform, Figure 5 is a diagram showing an actual measurement example of the V 0 surge waveform and the I 0 surge waveform, and Figure 6 is a hardware configuration diagram of an embodiment of the present invention. Fig. 7 is a diagram showing the DMA method, Fig. 8 is a flowchart showing the processing contents of CPU, Fig. 9 is a diagram showing the input waveform and output relationship in the present invention, and Fig. 10 is for explaining level detection. 11 is a flowchart for detecting a bipolar surge, and FIG. 12 is a diagram showing another embodiment of the present invention in which a ground fault detection function is added. 2 1 ~ 2 o+1 ...Shin breaker, 3...Bus bar, 4 1 ~
4 o ... Distribution line, 5 1 ~ 5 o ... Zero phase current transformer, 6 ...
…Zero-phase transformer, 7…Induced lightning surge detection device, 8
0 to 8 o ... Sample hold, 9... Multiplexer, 10... A/D converter, 11... Memory,
12... CPU, 13... I/O, 14... Setting I/F, 7 1 ... Directional ground fault detection device, 7 2 ... Induced lightning surge detection device.

Claims (1)

【特許請求の範囲】 1 電力系統における配電用変電所において、複
数の配電線が分岐する母線に接続されて該母線の
零相電圧を検出する零相変圧器と、前記各配電線
の零相電流を夫々検出する複数の零相変流器と、
前記零相電圧波形のサンプリングデータ及び各零
相電流波形のサンプリングデータを記憶するメモ
リと、このメモリから読込んだ前記零相電圧波形
のサンプリングデータのレベル変化が雷撃によつ
て架空の線状導体に生じる双極性サージ波形又は
双極性サージの閃絡した波形と類似するときに前
記各配電線の近傍の襲雷を検出し、この襲雷を検
出したときに前記メモリから読出した各零相電流
波形のサンプリングデータの極性が双極性サージ
に一致して所定レベル以上又は絶縁値加算が所定
値を越えることにより当該配電線の近傍に落雷し
たことを各配電線毎に検出し、この検出で当該配
電線が故障に至ると推測したときに当該配電線を
避災停電させるデータ処理装置とを備えたことを
特徴とする誘導雷サージ検出装置。 2 前記データ処理装置は、前記メモリから読込
んだ前記零相電圧波形及び各零相電流波形のサン
プリングデータから方向地絡検出を行う処理手段
を含む特許請求の範囲第1項記載の誘導雷サージ
検出装置。
[Scope of Claims] 1. In a distribution substation in an electric power system, a zero-phase transformer connected to a bus bar from which a plurality of distribution lines branch and detects the zero-sequence voltage of the bus, and a zero-phase transformer for detecting the zero-phase voltage of each distribution line. a plurality of zero-phase current transformers each detecting current;
A memory that stores sampling data of the zero-sequence voltage waveform and sampling data of each zero-sequence current waveform, and a level change of the sampling data of the zero-sequence voltage waveform read from this memory is caused by a lightning strike to cause an imaginary linear conductor. Detecting a lightning strike near each distribution line when the waveform is similar to a bipolar surge waveform or a flashing waveform of a bipolar surge occurring in When the polarity of the waveform sampling data matches a bipolar surge and exceeds a predetermined level, or when the insulation value addition exceeds a predetermined value, it is detected for each distribution line that a lightning strike has occurred in the vicinity of the distribution line. An induced lightning surge detection device comprising: a data processing device that causes an emergency power outage of the distribution line when it is estimated that the distribution line will fail. 2. The induced lightning surge according to claim 1, wherein the data processing device includes processing means for detecting a directional ground fault from sampling data of the zero-sequence voltage waveform and each zero-sequence current waveform read from the memory. Detection device.
JP11140180A 1980-08-13 1980-08-13 JUDORAISAAJIKENSHUTSUSOCHI Granted JPS5736536A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11140180A JPS5736536A (en) 1980-08-13 1980-08-13 JUDORAISAAJIKENSHUTSUSOCHI

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11140180A JPS5736536A (en) 1980-08-13 1980-08-13 JUDORAISAAJIKENSHUTSUSOCHI

Publications (2)

Publication Number Publication Date
JPS5736536A JPS5736536A (en) 1982-02-27
JPS644411B2 true JPS644411B2 (en) 1989-01-25

Family

ID=14560210

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11140180A Granted JPS5736536A (en) 1980-08-13 1980-08-13 JUDORAISAAJIKENSHUTSUSOCHI

Country Status (1)

Country Link
JP (1) JPS5736536A (en)

Also Published As

Publication number Publication date
JPS5736536A (en) 1982-02-27

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