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JPH0713652B2 - Fault location method for parallel two-line transmission line - Google Patents
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JPH0713652B2 - Fault location method for parallel two-line transmission line - Google Patents

Fault location method for parallel two-line transmission line

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Publication number
JPH0713652B2
JPH0713652B2 JP62081395A JP8139587A JPH0713652B2 JP H0713652 B2 JPH0713652 B2 JP H0713652B2 JP 62081395 A JP62081395 A JP 62081395A JP 8139587 A JP8139587 A JP 8139587A JP H0713652 B2 JPH0713652 B2 JP H0713652B2
Authority
JP
Japan
Prior art keywords
zero
line
phase
parallel
phase 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.)
Expired - Lifetime
Application number
JP62081395A
Other languages
Japanese (ja)
Other versions
JPS63247673A (en
Inventor
茂 成田
勲 千原
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.)
Fuji Electric Co Ltd
Original Assignee
Fuji Electric Co Ltd
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 Fuji Electric Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP62081395A priority Critical patent/JPH0713652B2/en
Publication of JPS63247673A publication Critical patent/JPS63247673A/en
Publication of JPH0713652B2 publication Critical patent/JPH0713652B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Locating Faults (AREA)

Description

【発明の詳細な説明】Detailed Description of the Invention 【産業上の利用分野】[Industrial applications]

本発明は、送電線の少なくとも片端の中性点が直接に、
あるいは抵抗もしくはリアクトルを介して接地されてい
る場合でも、平行2回線送電線の1線地絡故障の故障点
を標定することのできる故障点標定方法に関する。
In the present invention, the neutral point of at least one end of the transmission line is directly
Alternatively, the present invention relates to a fault point locating method capable of locating a fault point of a one-line ground fault of a parallel two-line transmission line even when grounded via a resistor or a reactor.

【従来の技術】[Prior art]

平行2回線送電線における零相電流Ioを用いた故障点標
定方法(以下においてはIo方法と呼ぶ)として、特開昭
59-211869号公報に記載されているものが知られてい
る。このIo方法を簡単に説明すると、第4図に示すよう
に平行2回線1L,2Lの簡略化零相等価回路を考えた場
合、回線1L及び2Lに流れる零相電流1LIo,2LIoは故障点
Fから見た零相インピーダンスによって配分されるの
で、故障点標定装置FLを設置した片端より故障点Fまで
の距離αは次式で求めることができる。 α・1LIo=(2−α)・2LIo ……(1) なお、第4図においてNGRは中性点接地抵抗を示してい
る。(2)式は送電線の対地容量の影響、すなわち対地
キャパシタンスを無視したものであるので、送電線の全
長が長くなると対地キャパシタンスの影響が無視できな
くなり誤差が生じる。 そこで、(2)式に対して対地キャパシタンスによる誤
差の補正を行うために、対地キャパシタンスに流れる零
相電流が零相電圧に対して90°進み位相になることに着
目して、零相電圧に対する(2)式の各零相電流値の有
効分(COS分)をとることで対地キャパシタンスの影響
を補正することができる。この場合の演算式は次式のよ
うに表される。 なお、(3)式において1Lθ,2Lθは各零相電圧と各零
相電流との位相差である。この(3)式がIo方式の原理
式である。
As a fault location method (hereinafter referred to as Io method) using a zero-phase current Io in a parallel two-circuit power transmission line
The thing described in the 59-211869 gazette is known. This Io method will be briefly described. As shown in FIG. 4, when a simplified zero-phase equivalent circuit of parallel two lines 1L and 2L is considered, zero-phase currents 1L Io and 2L Io flowing in lines 1L and 2L fail. Since it is distributed by the zero-phase impedance viewed from the point F, the distance α from one end where the failure point locating device FL is installed to the failure point F can be obtained by the following equation. α ・1L Io = (2-α) ・2L Io …… (1) In addition, in FIG. 4, NGR represents a neutral point ground resistance. Since the equation (2) neglects the influence of the ground capacitance of the transmission line, that is, the capacitance to ground, the influence of the capacitance to ground cannot be ignored and an error occurs when the total length of the transmission line becomes long. Therefore, in order to correct the error due to the ground capacitance with respect to the equation (2), paying attention to the fact that the zero-phase current flowing through the ground capacitance is advanced by 90 ° with respect to the zero-phase voltage. By taking the effective component (COS component) of each zero-phase current value in equation (2), the effect of the ground capacitance can be corrected. The arithmetic expression in this case is represented as the following expression. In equation (3), 1L θ and 2L θ are the phase difference between each zero-phase voltage and each zero-phase current. This equation (3) is the principle equation of the Io method.

【発明が解決しようとする問題点】[Problems to be Solved by the Invention]

ところが、この(3)式は自端のみのデータで標定が行
えるが第4図の等価回路からも明らかなように相手端が
非電源・非接地という制約がついている。 本発明は平行2回線送電線において片端が非電源・非接
地でなくても故障点を標定できるようにした故障点標定
方法を提供することを目的とする。
However, although the expression (3) can be located only by the data of its own end, there is a restriction that the other end is non-power supply / non-grounding as is clear from the equivalent circuit of FIG. An object of the present invention is to provide a fault point locating method capable of locating a fault point in a parallel two-line transmission line even if one end is not a non-power source / non-ground.

【問題点を解決するための手段】[Means for solving problems]

両端に端末装置を設置し、両回線に流れる零相電流およ
び零相電圧をそれぞれ測定し、各零相電流、零相電圧を
1ケ所に集めて同期をとる。
Terminal devices are installed at both ends, zero-phase current and zero-phase voltage flowing in both lines are measured, and each zero-phase current and zero-phase voltage are collected in one place for synchronization.

【作用】[Action]

同期をとった各零相電流について、自端において測定さ
れた故障のない回線に流れる零相電流値の有効分の2倍
値と他端において測定された両回線に流れる零相電流値
の有効分との和を、両端において測定された両回線に流
れる各零相電流値の有効分の和で除算した値に基づいて
自端から故障点までの距離を求める。
For each synchronized zero-phase current, double the effective component of the zero-phase current value flowing through the line without failure measured at its own end and the effective zero-phase current value flowing through both lines measured at the other end. The distance from the self-end to the failure point is calculated based on the value obtained by dividing the sum of the minutes and the sum of the effective fractions of the zero-phase current values flowing in both lines measured at both ends.

【発明の実施例】Examples of the invention

第3図は本発明が適用される平行2回線送電線の構成図
を示している。図においてA1,B1はそれぞれA端,B端に
設置された端末を示しており、各端末A1,B1はそれぞれ
A端,B端において平行2回線1L,2Lに流れる零相電流1LI
oA,2LIoA,1LIoB,2LIoBおよび零相電圧を測定するように
構成されている。各端末A1,B1で測定された各零相電
流、零相電圧は処理装置Cに送られ、処理装置Cにおい
て各零相電流、零相電圧の同期がとられたのち故障点標
定の演算が行われる。なお、各零相電流、零相電圧の同
期のとり方については特願昭61-93069号に記載される方
法等を使用することができる。 次に処理装置Cにおける故障点標定の演算について説明
する。 第2図は両端接地系統の構成図を示しており、回線1Lの
中間の故障点Fにおいて1線地絡事故が発生した状態を
示している。平行2回線1L,2Lにはそれぞれ零相電流1LI
oA,2LIoA,1LIoB,2LIoBが流れ、またA端,B端にはそれぞ
れ中性点接地抵抗NGRA,NGRBを介して中性点電流IN A,IN B
が流れる。なお図においてRFは故障点抵抗を示してい
る。 ここで、第2図の回路をA端,B端を中心とした片端非接
地の2つの回路の重ね合わせと考えると、第2図の回路
は第1図(a),(b)のように分けることができる。
第1図(a)はB端を非接地とし、第1図(b)はA端
を非接地とした場合を示している、第1図(a),
(b)の回路は第4図と同一の構成となるので平行2回
線1L,2Lを流れる零相電流をそれぞれi1S,i2S,i1R,i2R
すると故障点Fの位置は(2)式と同様にして次のよう
に求めることできる。 (a)の回路の場合 (b)の回路の場合 ところで、第1図の回路と第2図の回路との間には次の
関係が成立する。1L IoA=i1S+i2R ……(6)2L IoA=i2S+i2R ……(7) IN A=i1S+i2S ……(8) IN B=i1R+i2R ……(9) (6),(7)式より次式が求まる。1L IoA+2LIoA=i1S+i2S ……(10) この(10)式を(4)式に代入することにより次式が求
まる。 (7)式よりi2S2LIoA+i2Rとなるので、i2Sを(11)
式に代入することにより次式が求まる。 また、(5)式に(9)式を代入することにより次式が
求まる。 (12),(13)式よりi2Rを消去することにより次式が
求まる。 α・(1LIoA+2LIoA)=2・2LIoA+(1−α)・IN B ……
(14) ここで、B端の各零相電流を1LIoB,2LIoBとすると、IN B
1LIoB+2LIOBという関係が成立するので、(15)式に
このIN Bを代入することにより次式が求まる。 この(16)式はA端,B端において各回線1L,2Lに流れる
各零相電流1LIoA,2LIoA,1LIoB,2LIoBのみで表現されて
いるので、A端,B端においてこれらの零相電流を測定
し、同期をとって(16)式に代入することにより故障点
位置を求めることができる。 なお、(16)式は回線1L側にて故障が発生した場合であ
るが、回線2L側にて故障が発生した場合には同様にして
次式により故障点位置を求めることができる。 また、対地キャパシタンスの影響を補正するために、
(3)式と同様にして零相電圧に対する有効分(COS
分)をとることができる。この場合、A端での零相電
圧,B端での零相電圧,故障点での零相電圧は近似的に同
位相と考えられるので、A端,B端のどちらの零相電圧を
基準にしても良い。したがって、対地キャパシタンスの
影響を補正した故障点標定演算式は(16)式より次式の
ように求められる。 (18)式において1LθA,2LθA,1LθB,2LθBはそれぞれ
A端,B端における各零相電圧と各零相電流との位相差を
表わしている。 回線2L側の故障の場合も、同様にして対地キャパシタン
スの影響を補正することができるのは勿論である。
FIG. 3 shows a configuration diagram of a parallel two-line transmission line to which the present invention is applied. In the figure, A1 and B1 indicate terminals installed at the A end and B end, respectively, and each terminal A1 and B1 has zero phase current 1L I flowing in parallel 2 lines 1L and 2L at the A end and B end, respectively.
o A, 2L Io A, 1L Io B, is configured to measure a 2L Io B and zero-phase voltage. The zero-phase currents and zero-phase voltages measured at the terminals A1 and B1 are sent to the processing device C, and the zero-phase currents and zero-phase voltages are synchronized in the processing device C, and then the calculation of the fault location is performed. Done. The method described in Japanese Patent Application No. 61-93069 can be used to synchronize the zero-phase current and the zero-phase voltage. Next, the calculation of the fault location in the processing device C will be described. FIG. 2 shows a configuration diagram of the both-ends grounding system and shows a state where a one-line ground fault accident occurs at a failure point F in the middle of the line 1L. Zero-phase current 1L I for parallel 2 lines 1L, 2L respectively
o A, 2L Io A, 1L Io B, 2L Io B flows, and A end, each neutral grounding resistor NGR A to B end, the neutral point current through the NGR B I N A, I N B
Flows. In the figure, R F shows the resistance at the fault point. Here, considering the circuit of FIG. 2 as a superposition of two circuits of which one end is not grounded centering on the A end and the B end, the circuit of FIG. 2 is as shown in FIG. 1 (a), (b). Can be divided into
FIG. 1 (a) shows the case where the end B is not grounded, and FIG. 1 (b) shows the case where the end A is not grounded.
Since the circuit of (b) has the same configuration as that of FIG. 4, assuming that the zero-phase currents flowing in the parallel two lines 1L, 2L are i 1S , i 2S , i 1R , i 2R , the position of the fault point F is (2 It can be calculated as follows in the same manner as the equation). In the case of circuit (a) For the circuit of (b) By the way, the following relationship is established between the circuit of FIG. 1 and the circuit of FIG. 1L Io A = i 1S + i 2R ...... (6) 2L Io A = i 2S + i 2R ...... (7) I N A = i 1S + i 2S ...... (8) I N B = i 1R + i 2R …… (9) The following formula is obtained from the formulas (6) and (7). 1L Io A + 2L Io A = i 1S + i 2S (10) By substituting this equation (10) into equation (4), the following equation is obtained. From equation (7), i 2S = 2L Io A + i 2R , so i 2S is given by (11)
By substituting into the formula, the following formula is obtained. Further, the following equation is obtained by substituting the equation (9) into the equation (5). By eliminating i 2R from Eqs. (12) and (13), the following equation is obtained. α ・ ( 1L Io A + 2L Io A ) = 2 ・2L Io A + (1-α) ・IN B ……
(14) Here, assuming that each zero-phase current at the B end is 1L Io B , 2L Io B , I N B
= 1L Io B + 2L IO B holds, so by substituting this I N B into Eq. (15), the following equation is obtained. This equation (16) is expressed only by the zero-phase currents 1L Io A , 2L Io A , 1L Io B , 2L Io B flowing in each line 1L, 2L at the A end and B end, so that A end, B By measuring these zero-phase currents at the ends and synchronizing them and substituting them into Eq. (16), the fault point position can be obtained. Equation (16) is for the case where a failure occurs on the line 1L side, but when a failure occurs on the line 2L side, the failure point position can be similarly calculated by the following equation. Also, in order to correct the effect of the ground capacitance,
Similar to equation (3), the effective component (COS
Minutes). In this case, since the zero-phase voltage at the A terminal, the zero-phase voltage at the B terminal, and the zero-phase voltage at the fault point are considered to be approximately in phase, whichever zero-phase voltage at the A terminal or the B terminal is used as a reference. You can Therefore, the formula for calculating the fault location, which corrects the influence of the capacitance to ground, can be obtained from Eq. (16) as follows. In the equation (18), 1L θ A , 2L θ A , 1L θ B , and 2L θ B represent the phase difference between each zero-phase voltage and each zero-phase current at the A and B ends, respectively. Of course, in the case of a failure on the line 2L side, the effect of the ground capacitance can be similarly corrected.

【発明の効果】【The invention's effect】

本発明によれば、平行2回線送電線系統の両端において
測定された零相電流、零相電圧を用いて標定を行うよう
に構成したので、系統の接地条件によらずに高精度な1
線地絡故障の標定を行うことができる。
According to the present invention, since the zero-phase current and zero-phase voltage measured at both ends of the parallel two-line transmission line system are used for the orientation, the high-precision 1
Line faults can be located.

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

第1図,第2図は本発明による故障点標定方法を説明す
るための系統回路図、第3図は本発明が適用される平行
2回線送電線の構成図、第4図は従来の故障点標定方法
を説明するための系統回路図を示している。 A1,B1……端末、C……処理装置、F……故障点、1L,2L
……回線、NGR,NGRA,NGRB……中性点接地抵抗、1LIoA,
1LIoB,2LIoA,2LIoB……零相電流、IN A,IN B……中性点電
流、RF……故障点抵抗。
1 and 2 are system circuit diagrams for explaining a fault location method according to the present invention, FIG. 3 is a configuration diagram of a parallel two-line transmission line to which the present invention is applied, and FIG. 4 is a conventional fault. The system circuit diagram for demonstrating a point orientation method is shown. A1, B1 ... Terminal, C ... Processor, F ... Failure point, 1L, 2L
…… Line, NGR, NGR A , NGR B …… Neutral ground resistance, 1L Io A ,
1L Io B , 2L Io A , 2L Io B …… Zero-phase current, I N A , I N B …… Neutral point current, R F …… Fault point resistance.

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】平行2回線送電線の1線地絡故障の故障点
を標定する故障点標定方法において、 両端で両回線に流れる零相電流および零相電圧をそれぞ
れ検出して一か所に集め、各零相電流、零相電圧の同期
をとったのち、自端において測定された故障のない回線
に流れる零相電流の有効分の2倍値と他端において測定
された両回線に流れる各零相電流値の有効分との和を、
両端において測定された両回線に流れる各零相電流の有
効分の和で除算した値に基づいて自端から故障点までの
距離を求めることを特徴とする平行2回線送電線の故障
点標定方法。
1. A fault point locating method for locating a fault point of a one-line ground fault of a parallel two-line power transmission line, wherein a zero-phase current and a zero-phase voltage flowing in both lines at both ends are detected and located in one place. After collecting and synchronizing each zero-phase current and zero-phase voltage, double the effective value of the zero-phase current flowing through the line without failure measured at its own end and flowing through both lines measured at the other end. The sum of each zero-phase current value and the effective component,
A fault point locating method for a parallel two-line transmission line, characterized in that the distance from the self end to the fault point is obtained based on a value divided by the sum of the effective components of the zero-phase currents flowing in both lines measured at both ends. .
JP62081395A 1987-04-02 1987-04-02 Fault location method for parallel two-line transmission line Expired - Lifetime JPH0713652B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62081395A JPH0713652B2 (en) 1987-04-02 1987-04-02 Fault location method for parallel two-line transmission line

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62081395A JPH0713652B2 (en) 1987-04-02 1987-04-02 Fault location method for parallel two-line transmission line

Publications (2)

Publication Number Publication Date
JPS63247673A JPS63247673A (en) 1988-10-14
JPH0713652B2 true JPH0713652B2 (en) 1995-02-15

Family

ID=13745114

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62081395A Expired - Lifetime JPH0713652B2 (en) 1987-04-02 1987-04-02 Fault location method for parallel two-line transmission line

Country Status (1)

Country Link
JP (1) JPH0713652B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103424669B (en) * 2013-08-05 2016-03-30 昆明理工大学 A kind of selection method utilizing fault feeder zero-sequence current matrix principal component analysis (PCA) first principal component

Family Cites Families (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0758305B2 (en) * 1986-04-22 1995-06-21 中部電力株式会社 Fault location method

Also Published As

Publication number Publication date
JPS63247673A (en) 1988-10-14

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