JPH0634022B2 - Parallel multi-line ground fault fault location method - Google Patents
Parallel multi-line ground fault fault location methodInfo
- Publication number
- JPH0634022B2 JPH0634022B2 JP23176784A JP23176784A JPH0634022B2 JP H0634022 B2 JPH0634022 B2 JP H0634022B2 JP 23176784 A JP23176784 A JP 23176784A JP 23176784 A JP23176784 A JP 23176784A JP H0634022 B2 JPH0634022 B2 JP H0634022B2
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Description
【発明の詳細な説明】 (産業上の利用分野) この発明は高抵抗接地系における平行多回線地絡故郷点
標定方式に関する。Description: TECHNICAL FIELD The present invention relates to a parallel multi-line ground fault home point locating system in a high resistance grounding system.
(従来の技術) 平行2回線送電線の地絡故障に対する故障点の標定には
一般的に零相電流分流比による故障点標定方式である。
この零相電流分流比による方式の原理について第3図乃
至第4図に基きまず説明する。(Prior Art) A fault point locating method based on a zero-phase current shunt ratio is generally used for locating a fault point for a ground fault in a parallel two-line transmission line.
The principle of the method based on the zero-phase current diversion ratio will be described first with reference to FIGS. 3 to 4.
第3図は平行2回線の系統図(単相表現)を示し、A,
Bは自端側(標定装置接地点側)、相手端側の各母線1
L,2Lは母線A,B間に設けられた平行する各回戦であ
る。いま図では回線1Lの個所Fで1線地絡故障が発生
したものとしている。そして上記故障に対する対称座標
法から得られる零相等価回路は第4図のように表わされ
る。ここでxは回線の全長をlとしたときの自端から故
障点Fまでの距離、0は各回線の単位長当りの零相イ
ンピーダンス、01,02は各回線の零相電流、0fは
故障点零相電流であり、これらは下記の関係式で表現で
きる。0 f=01+02 (1) x0 01=l0 02+(l−x)0 02 (2) (1),(2)式より が得られ、前記(3),(4)式はそれぞれ回線1L,2Lの
自端側から故障点までの距臨を与える。FIG. 3 shows a system diagram (single-phase representation) of two parallel lines, A,
B is the bus line 1 on the self-end side (grounding device ground point side) and the mating end side
L and 2L are parallel rounds between bus lines A and B. In the figure, it is assumed that a 1-line ground fault has occurred at the point F of the line 1L. The zero-phase equivalent circuit obtained from the symmetric coordinate method for the above failure is represented as shown in FIG. Where x is the distance from the self-end to the fault point F when the total length of the line is 1, 0 is the zero-phase impedance per unit length of each line, 01 and 02 are the zero-phase current of each line, and 0 f is It is the zero-phase current at the failure point, and these can be expressed by the following relational expressions. 0 f = 01 + 02 (1) x 0 01 = l 0 02 + (l-x) 0 02 (2) From equations (1) and (2) The above equations (3) and (4) give the distance from the self-end side of the lines 1L and 2L to the failure point, respectively.
ところで、第3図で示す系統において相手端側(B端)
に零相インピーダンスをもつ機器例えば消弧リアクトル
を設置することがあるが、その場合零相インピーダンス
の影響が顕著に現われて前記(3),(4)式を用いる標定誤
差が生ずることになる。以下これを解明する。第5図に
おいてReは相手端側(B端)に設けられる消弧リアク
トルであり、前記同様回線1LのF点で1線地絡故障が
発生したときの零相等価回路を第6図で示す。By the way, in the system shown in Fig. 3, the other end (end B)
A device having a zero-phase impedance, for example, an arc-extinguishing reactor may be installed in the device, but in this case, the influence of the zero-phase impedance will be prominently generated, and an orientation error using the equations (3) and (4) will occur. This will be elucidated below. In FIG. 5, R e is an arc-extinguishing reactor provided on the other end side (B end), and a zero-phase equivalent circuit when a one-line ground fault occurs at point F of the line 1L is the same as in FIG. Show.
ここで、0′1:B端よりF点への零相電流0 ′:B端の零相電圧 :B端の零相インピーダンス0 f:故障点の零相電圧0 f:故障点の零相電流 とすると、0 f=0−x0 01 (5)0 f=0−l0 02−(l−x)0 0′1 (6)0 ′1=02−0′/ (7) が成立する。(5),(6)式より x01=l02+(l−x)0′1 (8) (7),(8)式に 01+0′1=0f 即ち0 ′1=0f−01を用いると (9),(10)式より ここで前記零相電流分流比の原理を適用すると、 となり、(13)式の右辺第2項即ち が誤差の要因となる。高抵抗接地系では一般に零相電圧
は高く(完全地絡で健全時の相電圧程度となる)、
0′/の大きさは0fのそれと同程度になる場合も
ある。従つて前記のような相手端に中性点インピーダン
スつまり零相インピーダンセをもつ系統では零相電流分
流比による故障点標定は適用できない。Here, 0 '1: zero-phase current to the point F than B-end 0': B end of the zero-phase voltage: B end of the zero-phase impedance 0 f: zero-phase voltage 0 f point of failure: the zero-phase point of failure If it is a current, then 0 f = 0 −x 0 01 (5) 0 f = 0 −l 0 02 − (l−x) 0 0 ′ 1 (6) 0 ′ 1 = 02 −0 ′ / (7) To do. From equations (5) and (6), x 01 = l 02 + (l−x) 0 ′ 1 (8) In equations (7) and (8), 01 +1 0 ′ 1 = 0 f, that is, 0 ′ 1 = 0 f With -01 From equations (9) and (10) Applying the principle of the zero-phase current diversion ratio here, And the second term on the right side of equation (13), that is, Causes an error. Zero-phase voltage is generally high in a high resistance grounding system (because of a complete ground fault, the phase voltage is in a healthy state).
The magnitude of 0 '/ may be similar to that of 0 f. Therefore, the fault location based on the zero-phase current shunt ratio cannot be applied to the system having the neutral point impedance, that is, the zero-phase impedance, at the other end as described above.
(発明が解決しようとする問題点) この発明は前記のように相手端に零相インピーダンスを
もつ系統では(13)式の右辺第2項が誤差要因になる。本
発明は零相インピーダンスの影響を受けず、その故障点
までの距離を高精度で標定することを目的とする。(Problems to be Solved by the Invention) In the present invention, as described above, the second term on the right side of the equation (13) becomes an error factor in the system having the zero-phase impedance at the other end. It is an object of the present invention to locate the distance to the failure point with high accuracy without being affected by the zero-phase impedance.
(問題点を解決するための手段) この発明による方式の原理についてまず説明する。第7
図は平行n回線の系統図(単相表現)を示し、A,Bは
自端側(標定装置設置点側)、相手側の各母線、1L〜
nLは母線A,B間に設けられた平行する各回線であ
る。Reは前記同様相手端側(B端)に設けられる消弧リ
アクトルである。そして前記同様回線1LのF点で1線
地絡故障が発生したときの零相等価回路を第8図で示
す。(Means for Solving Problems) The principle of the system according to the present invention will be described first. 7th
The figure shows a system diagram (single-phase representation) of parallel n lines, where A and B are the self-end side (orientation device installation point side) and each partner's busbar, 1L-
nL is each parallel line provided between the buses A and B. Re is an arc-extinguishing reactor provided on the other end side (B end) as described above. FIG. 8 shows a zero-phase equivalent circuit when a one-line ground fault occurs at the point F of the line 1L as described above.
ここで、0′1:B端よりF点への零相電流0 ′:B端の零相電圧 :B端の零相インピーダンス0 f:故障点の零相電圧0 f:故障点の零相電流 とすると、前記同様に (14),(15)式より x01=l02+(l−x)0′1 (17) また(15)式より 02=03……=0n これを(16)式に用いて0 ′1=(n−1)02−0′/
(18) (17)式より x(01+0′1)=l(02+0′1) 故に この式に(18)式を用いると を得る。この(19)式が拡張された零相電流分流比による
標定演算式であり、ここで=∝(無限大)、n=2と
すれば前記した(4)式と一致することがわかる。Here, 0 '1: zero-phase current to the point F than B-end 0': B end of the zero-phase voltage: B end of the zero-phase impedance 0 f: zero-phase voltage 0 f point of failure: the zero-phase point of failure If the current is the same as above From equations (14) and (15), x 01 = l 02 + (l−x) 0 ′ 1 (17) Also, from equation (15) 02 = 03 …… = 0n Using this in equation (16), 0 ′ 1 = (n-1) 02 - 0 '/
(18) (17) from x (01 + 0 Thus '1) = l (02 + 0' 1) If equation (18) is used for this equation, To get It is understood that this equation (19) is the orientation calculation equation based on the extended zero-phase current shunt ratio, and if ∝ (infinity) and n = 2 are satisfied, it agrees with the above equation (4).
(19)式には自端即ちA電気所で直接得られる零相電流情
報以外に相手端即ちB電気所の零相電流情報が必要であ
る。自端電気所Aの電流電圧情報のみを用いて標定でき
ることが理想ではあるが、高抵抗接地系においては、変
圧器中性点インピーダンスの大きさが線路インピーダン
スに比べて非常に大きく、0′=0−l0 02にお
ける線路での電圧降下分l0 02は0に比べて無視す
ることができる。従って、0′0と考えて支障はな
い。Equation (19) requires zero-phase current information of the other end, that is, B electric station, in addition to the zero-phase current information directly obtained at its own end, that is, A electric station. Ideally, it can be located using only the current and voltage information of the local electric station A, but in the high resistance grounding system, the magnitude of the neutral point impedance of the transformer is much larger than the line impedance, and 0 '= The voltage drop l 0 02 on the line at 0 −l 0 02 is negligible compared to 0 . Therefore, there is no problem believe that 0 '0.
以上のことより相手端に中性点インピーダンスをもつ高
抵抗接地系平行n回線の1線地絡故障点標定式として を得る。From the above, as a one-wire ground fault fault localization formula for high resistance grounding parallel n line with neutral point impedance at the other end To get
ここで、01:故障回線零相電流02 :健全回線零相電流0 :自端零相電圧 :相手端中性点インピーダンス として、前(20)式を適用する場合、n回線中から故障回
線と健全回線を選択する必要があるが、この故障回線の
選択とその故障点までの標定を以下に詳述する。Where 01 : failure line zero-phase current 02 : sound line zero-phase current 0 : self-end zero-phase voltage: opposite end neutral point impedance When applying the formula (20), it is determined that there is a failure line from n lines. It is necessary to select a healthy line, and the selection of this faulty line and the orientation to the fault point will be described in detail below.
前(15)式より02=03=……=0n であるから前(20)式の分母は となる。Since 02 = 03 = ... = 0n from equation (15), the denominator of equation (20) is Becomes
ここでi回線について次の(20)式で計算されるxiを求め
ることにする。Here, x i calculated by the following equation (20) is determined for the i line.
(但しi=1,2,3,……,n) 前(17),(18)式及び01+0′1=0f,0′0の
関係を用いると または が得られるから(23)式を(21)式に用いると、 x1=nl−(n−1)x x2=x3=……xn=x となり、x≦nl−(n−1)xであるから、故障回線
の計算値xiが最大となることがわかり、更に故障点まで
の距離は故障回線以外の計算値xjにより与えられる事が
わかる。従つて故障回線の選択と、その故障点の標定を
次の要領で行うことができる。 (However, i = 1,2,3, ..., n) Using the previous equations (17) and (18) and the relationship of 01 + 0 ′ 1 = 0 f, 0 ′ 0 Or Therefore, by using the equation (23) in the equation (21), x 1 = nl− (n−1) x x 2 = x 3 = ... x n = x, and x ≦ nl− (n−1 ) X, it can be seen that the calculated value x i of the faulty line is the maximum, and that the distance to the fault point is given by the calculated value x j of other than the faulty line. Therefore, it is possible to select the faulty line and locate the faulty point in the following manner.
まず、前(21)式 但しi=1,2,3,……,nについて を計算する。上式にしたがえば が計算される。このx1,x2……,xnの中から最大値を呈
したiL回線を故障回線として選択する。更にxi以外のxj
を故障点までの標定値として選択する。First, the previous equation (21), where i = 1,2,3, ..., n To calculate. According to the above formula Is calculated. The iL line with the maximum value is selected from these x 1 , x 2, ..., x n as the faulty line. Furthermore, other than x i x j
Is selected as the reference value up to the failure point.
第2図は上記処理要領手順を細分化して示すフローチヤ
ートであり、ステツプ(1)で地絡故障が発生したか否か
を判定する。零層電圧0が予め設定された設定レベル
Lより大きいか等しいときステツプ(2)に進む。ステツ
プ(2)では相手端零相インピーダンスに流れ込む1回
線当りの電流の計算を行う。ステツプ(3)では零相イン
ピーダンスに流れる電流分を除去する。ステツプ(4)で
は電流分流比による距離の計算を行う。ステツプ(5)で
故障回線の選択を行なう。ステツプ(6)では故障点標定
値の平均化(演算誤差の平均化)を行う。ステツプ(7)
で上記の標定値を出力する。最後にステツプ(8)で地絡
故障が消滅したか否かを判定し、YESのとき終了する。FIG. 2 is a flow chart showing the procedure of the above process in detail, and it is judged in step (1) whether a ground fault has occurred. When the zero-layer voltage 0 is greater than or equal to the preset set level L, the process proceeds to step (2). In step (2), the current per line that flows into the zero-phase impedance of the other end is calculated. In step (3), the current component flowing in the zero phase impedance is removed. In step (4), the distance is calculated by the current diversion ratio. In step (5), select the faulty line. At step (6), the fault point orientation values are averaged (calculation errors are averaged). Step (7)
Outputs the above standard value. Finally, in step (8), it is determined whether or not the ground fault has disappeared, and if YES, the process ends.
このように本発明方式の原理にしたがえば高抵抗接地系
平行多回線送電線で相手端に中性点インピーダンス(零
相インピーダンス)をもつ場合にも適用できるほか、原
理的に殆んど誤差がなく高精度の標定が可能である特徴
を有するものである。As described above, according to the principle of the present invention, it can be applied to a parallel multi-line transmission line with high resistance grounding and has a neutral point impedance (zero phase impedance) at the other end, and in principle, there is almost no error. The feature is that there is no problem and highly accurate orientation is possible.
(実施例) 以下この発明の方式を用いた具体的実施例を第1図に示
す。回線1L〜nLの自端側に設けた変流器1CT〜nCTにより
回線単位の零相電流01〜0nを得る。1AXCT〜nAXCTは
前記零相電流01〜0nを適当な値の電圧に変換する補
助変流器、PTは計器用変圧器で系統の零相電圧0を
得る。AXPTは補助変圧器である。AFはそれぞれ前記系
統から得られる零相電圧0、零相電流01〜0n情報
に含まれる高調波成分をカツトし、折返し誤差を除去す
るために設けられるアナログフイルタである。S/Hはそ
れぞれサンプルホールド回路であり、前記系統から得ら
れた情報を制御回路CONからの指令に基き例えば1サイ
クル中に12回(30゜間隔)の同時刻サンプリングを行
いそのサンプル値を保持する。MPXは前記サンプル値を
順次切替えて出力するマルチプレクサ、A/Dは前記アナ
ログのサンプル値をデジタル量に変換するAD変換器であ
る。CPUは前記デジタル情報を記憶すると同時に所定の
演算を行うマイクロプロセツサ等の演算装置、OUTは出
力回路である。(Embodiment) A concrete embodiment using the method of the present invention is shown in FIG. Zero-phase currents 01 to 0n for each line are obtained by the current transformers 1CT to nCT provided at the ends of the lines 1L to nL. 1AXCT to nAXCT are auxiliary current transformers for converting the zero-phase currents 01 to 0n into voltages of appropriate values, and PT is an instrument transformer to obtain the zero-phase voltage 0 of the system. AXPT is an auxiliary transformer. AF is an analog filter provided for cutting the harmonic components contained in the zero-phase voltage 0 and zero-phase current 01 to 0n information obtained from the system, respectively, and removing the folding error. Each S / H is a sample and hold circuit, and based on a command from the control circuit CON, for example, performs 12 times (30 ° interval) simultaneous sampling based on the command from the control circuit CON and holds the sample value. To do. MPX is a multiplexer that sequentially switches and outputs the sample value, and A / D is an AD converter that converts the analog sample value into a digital amount. The CPU is an arithmetic unit such as a microprocessor that stores the digital information and at the same time performs a predetermined arithmetic operation, and OUT is an output circuit.
なお、MPX,A/D,CPUはS/H同様制御回路CONからの指令
に基き所定の動作を行う。The MPX, A / D, and CPU perform predetermined operations based on commands from the control circuit CON, like S / H.
而して、任意の回線で地絡故障が発生したとすると、零
相電圧0が生じ同時に各回線に零相電流01〜0nが
流れるのでこれらがサンプリングデータとしてCPUに記
憶される。そしてCPUでサンプリングデータより基本波
成分が抽出されるとともに、零相電圧0に対する設定
レベルL及び回線長lは既知であるから先の(21)式にし
たがつて演算する。この演算出力は故障回路とその故障
点までの距離xにほかならない。If a ground fault occurs in any line, zero-phase voltage 0 occurs and zero-phase currents 01 to 0n flow in each line at the same time, so these are stored in the CPU as sampling data. Then, the CPU extracts the fundamental wave component from the sampling data, and since the set level L and the line length 1 for the zero phase voltage 0 are known, the calculation is performed according to the equation (21). This calculation output is nothing but the distance x to the faulty circuit and its fault point.
(発明の効果) 以上詳述したようにこの発明によれば、高抵抗接地系平
行多回線送電線において相手端に中性点インピーダンス
をもつ系統に適用できるほか、原理的に殆んど誤差がな
く、高精度の故障点標定が実現できる効果を奏する。(Effects of the Invention) As described in detail above, according to the present invention, in addition to being applicable to a system having a neutral point impedance at the other end in a high resistance grounding parallel multi-line transmission line, in principle, almost no error occurs. In other words, it has the effect of realizing highly accurate fault location.
第1図は本発明の実施例を示すブロツク線図、第2図は
本発明による処理手順を示すフローチヤート図、第3図
は平行2回線送電線の単線系統図、第4図は故障時の零
相等価回路図、第5図は相手端に中性点インピーダンス
をもつ単線系統図、第6図は故障時の零相等価回路
図、第7図は本発明方式を説明するための平行n回線送
電線の単線系統図、第8図は故障時の零相等価回路図で
ある。 1L〜nL……回線 Re……中性点インピーダンスをもつ機器 AF……アナログフイルタ S/H……サンプルホールド回路 MPX……マルチプレクサ CON……制御回路 A/D……アナログデジタル変換器 CPU……演算装置FIG. 1 is a block diagram showing an embodiment of the present invention, FIG. 2 is a flow chart showing a processing procedure according to the present invention, FIG. 3 is a single line system diagram of a parallel two-line transmission line, and FIG. Fig. 5 is a single-line system diagram with a neutral point impedance at the other end, Fig. 6 is a zero-phase equivalent circuit diagram at the time of failure, and Fig. 7 is a parallel diagram for explaining the method of the present invention. FIG. 8 is a single-phase system diagram of the n-line transmission line, and FIG. 8 is a zero-phase equivalent circuit diagram at the time of failure. 1L to nL …… Line Re …… Device with neutral impedance AF …… Analog filter S / H …… Sample hold circuit MPX …… Multiplexer CON …… Control circuit A / D …… Analog digital converter CPU …… Arithmetic unit
Claims (1)
手母線端に設置される変圧器が中性点インピーダンスを
有する系統において、1線地絡時に生ずる自端電気所の
零相電圧と各回線に流れる零相電流を入力とし、xiを 但し i=1,2,3,…n n:回線数0i :回線零相電流0 :自端零相電圧 :相手母線端変圧器中性点インピーダンス l:回線長 にて演算し、この演算出力x1,x2,…,xnから最大値を
呈したxiよりi回線を故障回線と判断するとともに、xi
以外の演算出力xjを自端電気所から故障点までの距離に
標定してなる平行多回線地絡故障点標定方式。1. A zero-phase voltage of a self-terminal electric station that occurs at the time of a one-wire ground fault in a system of a high resistance grounding parallel multi-line transmission line in which a transformer installed at the other end of the bus has a neutral point impedance. And the zero-phase current flowing in each line as input, x i However, i = 1,2,3, ... n n: Number of lines 0i : Line zero-phase current 0 : Own zero-phase voltage: Opposite bus end transformer neutral point impedance l: Calculated by line length, and output this calculation It is determined that the i-line is a failed line from x i, which has the maximum value from x 1 , x 2 , ..., X n , and x i
A parallel multi-circuit ground fault fault location method in which the operation output x j other than is located at the distance from the local electric station to the fault point.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23176784A JPH0634022B2 (en) | 1984-11-02 | 1984-11-02 | Parallel multi-line ground fault fault location method |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP23176784A JPH0634022B2 (en) | 1984-11-02 | 1984-11-02 | Parallel multi-line ground fault fault location method |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS61110066A JPS61110066A (en) | 1986-05-28 |
| JPH0634022B2 true JPH0634022B2 (en) | 1994-05-02 |
Family
ID=16928707
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP23176784A Expired - Lifetime JPH0634022B2 (en) | 1984-11-02 | 1984-11-02 | Parallel multi-line ground fault fault location method |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0634022B2 (en) |
-
1984
- 1984-11-02 JP JP23176784A patent/JPH0634022B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS61110066A (en) | 1986-05-28 |
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