JPH0136594B2 - - Google Patents

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Publication number
JPH0136594B2
JPH0136594B2 JP56152484A JP15248481A JPH0136594B2 JP H0136594 B2 JPH0136594 B2 JP H0136594B2 JP 56152484 A JP56152484 A JP 56152484A JP 15248481 A JP15248481 A JP 15248481A JP H0136594 B2 JPH0136594 B2 JP H0136594B2
Authority
JP
Japan
Prior art keywords
phase
load
δic
δia
δib
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
JP56152484A
Other languages
Japanese (ja)
Other versions
JPS5853770A (en
Inventor
Motohiko Shimada
Toshihiko Tanioka
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.)
Kansai Electric Power Co Inc
Daihen Corp
Original Assignee
Daihen Corp
Kansai Denryoku KK
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 Daihen Corp, Kansai Denryoku KK filed Critical Daihen Corp
Priority to JP56152484A priority Critical patent/JPS5853770A/en
Publication of JPS5853770A publication Critical patent/JPS5853770A/en
Publication of JPH0136594B2 publication Critical patent/JPH0136594B2/ja
Granted legal-status Critical Current

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Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R31/00Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
    • G01R31/50Testing of electric apparatus, lines, cables or components for short-circuits, continuity, leakage current or incorrect line connections
    • G01R31/54Testing for continuity
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R31/00Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
    • G01R31/50Testing of electric apparatus, lines, cables or components for short-circuits, continuity, leakage current or incorrect line connections
    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R31/00Arrangements for testing electric properties; Arrangements for locating electric faults; Arrangements for electrical testing characterised by what is being tested not provided for elsewhere
    • G01R31/50Testing of electric apparatus, lines, cables or components for short-circuits, continuity, leakage current or incorrect line connections
    • G01R31/52Testing for short-circuits, leakage current or ground faults

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Testing Of Short-Circuits, Discontinuities, Leakage, Or Incorrect Line Connections (AREA)

Description

【発明の詳細な説明】[Detailed description of the invention]

本発明は、3相負荷に電力を供給する電線路の
断線と負荷の開放との区別を変電所において確実
にかつ簡単に検出することができる電線路の断線
検出方法に関するものである。 配電線は一般に中性点非接地方式であり、系統
は樹枝状である。このような配電線の地絡および
過電流等の事故に対しては地絡継電器、過電流継
電器等で検出されているが、配電線への信頼度の
向上、安全性の確保等の理由から線路の絶縁電線
化が進んでいる。しかし、絶縁電線が断線して大
地に落下しても、絶縁電線の被覆があるために、
その内部の導体と大地とが接触しないので零相電
流が流れず、地絡事故として変電所で検出できな
い場合があり、保安上および電力供給上の障害と
なつていた。 本発明は上記の問題を解決するために、3相負
荷に電力を供給する配電線の1線断線および負荷
開放によつて各相の線電流が変化したとき、例え
ばA相については、A相の線電流のベクトル変化
分とB相およびC相の線電流のベクトル変化分の
ベクトル差との比の絶対値を求め、さらに残る2
つの相すなわちB相およびC相についても上記と
同様にして絶対値を求める。このようにして求め
られる3つの絶対値の和またはその各々の絶対値
が、1線断線時と負荷開放時とは異なる関係にあ
ることを利用して、断線を検出する電線路の断線
検出方法を提供したものである。 以下、本発明の断線検出方法について図面を参
照して説明する。 第1図は、変電所T1に負荷L1および負荷L2
接続された線路を示す図であつて、変電所におけ
る線路電流I0は、負荷状態又はその負荷にのみ接
続された線路状態が変化しない負荷L1の線路電
流I1と、負荷状態または線路状態が変化する負荷
L2の線路電流I2とのベクトル和となるが、変電所
と各負荷との間の線路インピーダンスは各負荷の
インピーダンスにくらべて小さいものとして線路
インピーダンスを無視する。さらに各線間電圧は
それぞれ120゜の位相差を有するとともに負荷L2
線路状態が変化しても第1図に示すP点における
各線間電圧と各線電流とのそれぞれの位相差はい
ずれも変化しないものとする。したがつて変電所
における線路電流の変化分ΔI0は、負荷L2の線路
の状態の変化による変化分ΔI2にのみ左右され、
負荷L1の変化分ΔI0=0となるので、以下の説明
においては、負荷L1については考慮しないもの
とする。したがつて、負荷L2の線路の状態変化
は第2図A乃至Dの等価回路で示すことができ
る。ただし、第2図AはA相1線断線時の等価回
路であり、同図BはBC相単相負荷開放時の等価
回路であり、同図CはAB・CA相V負荷開放時
の等価回路であり、また同図Dは3相負荷開放時
の等価回路である。 第2図A乃至Dにおいて、定常状態におけるA
相、B相およびC相の各線電流をIa,IbおよびIc
各線間電圧をVab,VbcおよびVca、各線間に接
続された負荷の電流をIab,IbcおよびIcaとし、
それらの絶対値をiab,ibcおよびicaとし、各負
荷の力率角をα,βおよびτとすると各線電流
は、 Ia=Iab−Ica=iabej〓−icaej〓・a ……(1) Ib=Ibc−Iab=ibcej〓・a2−iabej〓 ……(2) Ic=Ica−Ibc=icaej〓・a−ibcej〓・a2 ……(3) となる。ただし、a=ej2/3π、a2=aj4/3πであ る。 ここで、第2図Aに示すようにA相の線路が断
線したとき、断線後の各線電流をIa′,Ib′および
Ic′とし、負荷電流をIab′,Ibc′およびIca′とすれ
ば、 Ia′=0 Ib′=Ibcej〓・a2
1/1/iabej〓+1/icaej〓・a2 Ic′=−Ib′ となり、各線電流の変化分ΔIa,ΔIbおよびΔIc
は次式のようになる。 ΔIa=I′a−Ia=−(iabej〓−icaej〓・a)……(4
) ΔIb=ΔI′b−Ib=iabej〓/iabej〓+icaej〓(iabej
〓−icaej〓.a)=−iabej〓/iabej〓+icaej〓・Δ
Ia……(5) ΔIc=I′c−Ic=iabej〓/iabej〓+icaej〓(iabej
〓−icaej〓・a)=−icaej〓/iabej〓+icaej〓・Δ
Ia……(6) (5)式と(6)式とから ΔIb/ΔIc=iab/icaej(α−τ) ……(7) (4)式と(7)式とから ΔIa=(iabej〓−icaej〓・a) =−ica(iab/icaej〓・a) =−ica(ΔIb/ΔIcej〓−ej〓・a) =−ica/ΔIc(ΔIbej〓−ΔIcej〓・a) ……(8) (8)式を変形すると ΔIc/ica=−(ΔIb−ΔIc・a)/ΔIa・ej〓……(
9) になり、右辺の絶対値をとると、次式がA相の断
線指数STaを求める式になる。 STa=|ΔIb−ΔIc・a/ΔIa| ……(10) 同様にして、B相およびC相断線時の断線指数を
求める式はそれぞれ次式のようになる。 STb=|ΔIc・a2−ΔIa/ΔIb| =|ΔIc−ΔIa・a/ΔIb| ……(11) STc=|ΔIa・a−ΔIb・a2/ΔIc| =|ΔIa−ΔIb・a/ΔIc| ……(12) つぎに上記(10)式乃至(12)式を用いて、1線断線時
および種々の負荷開閉時の断線指数STa,STbお
よびSTcの値を第3図乃至第7図を参照しながら
求める。 第3図A乃至Dは、それぞれ3相平衡負荷にお
けるA相1線断線時、BC相単相負荷開放時
AB・CA相V負荷開放時および3相負荷開放時
の変電所における線電流のベクトル図であつて、
A相、B相およびC相の各線電流Ia,IbおよびIc
が変動して、それぞれIa′,Ib′およびIc′になつた
ときのこれらの各ベクトル値の変化分ΔIa,ΔIb
およびΔIcを示している。第4図A、第5図A、
第6図Aおよび第7図Aは、それぞれ第3図A乃
至Dにおけるベクトル値の変化分ΔIa,ΔIbおよ
びΔIcを示すベクトル図である。なお、各相の線
電流の変化分ΔIa,ΔIbおよびΔIcを示すベクト
ルは、それぞれ絶対値の比すなわち|ΔIa|:|
ΔIb|:|ΔIc|を便宜上、第4図Aについては
2:1:1とし、以下第5図A、第6図Aおよび
第7図Aについてはそれぞれ0:1:1、√3:
1:1および1:1:1にしたときのものであ
る。 (1) A相1線断線 (i) (10)式においてはΔIcにaを乗じることは、
ΔIcを反時計方向に120゜ベクトル回転させるこ
とであるから、第4図Aに示すベクトルΔIa,
ΔIbおよびΔIcの関係は第4図Bのようになる。
この図から明らかなように、(10)式の|ΔIb−
ΔIc・a|は√3であり、|ΔIa|は2であるの
でSTaは√3/2となる。 (ii) このときのSTbをつぎのとおり求める。(11)式
のΔIaを(i)と同様に120゜回転させれば、第4図
Aに示すベクトルΔIa,ΔIbおよびΔIcの関係
は第4図Cのようになり、|ΔIc−ΔIa・a|は
√3であり、|ΔIb|は1であるのでSTbは√
3となる。 (ii) さらにこのときのSTcをつぎのとおり求め
る。(12)式のΔIbを(i)と同様に120゜回転させれば、
第4図AのΔIa,ΔIbおよびΔIcの関係は第4
図Dのようになり、|ΔIa−ΔIb・a|は√3で
あり、|ΔIc|は1であるのでSTcは√3とな
る。 (2) BC相単相負荷開放 前述したのと同様にすれば、第5図Aはそれぞ
れ第5図B、第5図Cおよび第5図Dのようにな
り、ΔIaは0であるのでSTaは1/0=∞となる。 また、STbおよびSTcはともに1/1=1となる。 (3) AB・CA相V負荷開放 前述したのと同様にすれば、第6図Aはそれぞ
れ第6図B、第6図Cおよび第6図Dのようにな
り、STaは1/√3、STbおよびSTcはともに1/1= 1となる。 (4) 3相負荷開放 前述したのと同様にすれば、第7図Aはそれぞ
れ第7図B、第7図Cおよび第7図Dのようにな
り、|ΔIb−ΔIc・a|、|ΔIc−ΔIa・a|および
|ΔIa−ΔIb・a|がともに0であるのでSTa=
STb=STc=0となる。 ここに、A相1線断線時および種々の負荷開放
時のSTa,STbおよびSTcの値を第1表に示す。
The present invention relates to a method for detecting disconnection of an electric line that can reliably and easily distinguish between a disconnection of an electric line supplying power to a three-phase load and an open load at a substation. Distribution lines are generally ungrounded at the neutral point, and the system is dendritic. Accidents such as ground faults and overcurrents on distribution lines are detected using ground fault relays, overcurrent relays, etc., but in order to improve the reliability of distribution lines and ensure safety, The use of insulated wires for railway lines is progressing. However, even if the insulated wire breaks and falls to the ground, the insulated wire has a covering, so
Since the internal conductor does not contact the ground, zero-sequence current does not flow, and there are cases where a ground fault cannot be detected at the substation, posing a problem in terms of safety and power supply. In order to solve the above-mentioned problems, the present invention has been developed to solve the above problem. Find the absolute value of the ratio of the vector change in the line current and the vector difference in the vector change in the line current of the B phase and C phase, and then calculate the remaining 2
The absolute values of the two phases, ie, the B phase and the C phase, are determined in the same manner as above. A wire breakage detection method for detecting a wire breakage by utilizing the fact that the sum of the three absolute values obtained in this way or the absolute value of each of them has a different relationship between when one line is broken and when the load is released. was provided. Hereinafter, the disconnection detection method of the present invention will be explained with reference to the drawings. FIG. 1 is a diagram showing a line in which a load L 1 and a load L 2 are connected to a substation T 1 , and the line current I 0 in the substation is in a loaded state or in a line connected only to that load. The line current I 1 for a load L 1 which does not change and the load whose load condition or line condition changes
This is the vector sum of L 2 and the line current I 2 , but the line impedance between the substation and each load is ignored as it is smaller than the impedance of each load. Furthermore, each line voltage has a phase difference of 120°, and even if the line condition of load L 2 changes, the phase difference between each line voltage and each line current at point P shown in Figure 1 does not change. shall be taken as a thing. Therefore, the change ΔI 0 in the line current at the substation depends only on the change ΔI 2 due to the change in the line condition of the load L 2 ,
Since the change in load L 1 is ΔI 0 =0, the load L 1 will not be considered in the following explanation. Therefore, the change in the line state of the load L2 can be shown by the equivalent circuits shown in FIGS. 2A to 2D. However, Figure 2A is the equivalent circuit when one wire of A phase is disconnected, Figure B is the equivalent circuit when the BC phase single-phase load is opened, and Figure C is the equivalent circuit when the AB/CA phase V load is opened. Figure D is an equivalent circuit when the three-phase load is released. In FIGS. 2A to 2D, A in the steady state
The line currents of phase, B phase and C phase are Ia, Ib and Ic
Let the voltage between each line be Vab, Vbc and Vca, and the current of the load connected between each line Iab, Ibc and Ica,
If their absolute values are iab, ibc, and ica, and the power factor angles of each load are α, β, and τ, then each line current is Ia=Iab−Ica=iabe j 〓−icae j 〓・a ……(1) Ib=Ibc−Iab=ibce j 〓・a 2 −iabe j 〓 ...(2) Ic=Ica−Ibc=icae j 〓・a−ibce j 〓・a 2 ...(3). However, a=ej2/3π and a 2 =aj4/3π. Here, when the A-phase line is disconnected as shown in Figure 2A, each line current after the disconnection is Ia', Ib' and
Ic′ and the load currents Iab′, Ibc′ and Ica′, Ia′=0 Ib′=Ibce j 〓・a 2 +
1/1/iabe j 〓+1/icae j 〓・a 2 Ic′=−Ib′, and the changes in each line current ΔIa, ΔIb, and ΔIc
is as follows. ΔIa=I′a−Ia=−(iabe j 〓−icae j 〓・a)……(4
) ΔIb=ΔI′b−Ib=iabe j 〓/iabe j 〓+icae j 〓(iabe j
〓−icae j 〓. a)=−iabe j 〓/iabe j 〓+icae j 〓・Δ
Ia……(5) ΔIc=I′c−Ic=iabe j 〓/iabe j 〓+icae j 〓(iabe j
〓−icae j 〓・a)=−icae j 〓/iabe j 〓+icae j 〓・Δ
Ia...(6) From equations (5) and (6), ΔIb/ΔIc=iab/icaej(α−τ)...(7) From equations (4) and (7), ΔIa=(iabe j 〓−icae j 〓・a) =−ica(iab/icae j 〓・a) =−ica(ΔIb/ΔIce j 〓−e j 〓・a) =−ica/ΔIc(ΔIbe j 〓−ΔIce j 〓・a) ……(8) Transforming equation (8), ΔIc/ica=−(ΔIb−ΔIc・a)/ΔIa・e j 〓……(
9), and taking the absolute value of the right-hand side, the following formula becomes the formula for determining the A-phase disconnection index STa. STa=|ΔIb−ΔIc·a/ΔIa| (10) Similarly, the formulas for determining the disconnection index at the time of B-phase and C-phase disconnection are as follows. STb=|ΔIc・a 2 −ΔIa/ΔIb| =|ΔIc−ΔIa・a/ΔIb| ...(11) STc=|ΔIa・a−ΔIb・a 2 /ΔIc| =|ΔIa−ΔIb・a/ΔIc | ...(12) Next, using equations (10) to (12) above, the values of the breakage indices STa, STb, and STc at the time of one wire breakage and when switching various loads are shown in Figures 3 to 7. Find it while referring to. Figures A to D show the case when one wire of the A phase is disconnected and the single phase load of the BC phase is opened under a three-phase balanced load, respectively.
A vector diagram of the line current in the substation when the AB/CA phase V load is opened and the 3-phase load is opened,
Line currents Ia, Ib and Ic of A phase, B phase and C phase
The changes in these vector values ΔIa, ΔIb when the vector values change and become Ia′, Ib′, and Ic′, respectively.
and ΔIc are shown. Figure 4A, Figure 5A,
6A and 7A are vector diagrams showing vector value changes ΔIa, ΔIb, and ΔIc in FIGS. 3A to 3D, respectively. Note that the vectors indicating the changes in the line current of each phase ΔIa, ΔIb, and ΔIc are the ratio of their absolute values, that is, |ΔIa|:|
For convenience, ΔIb|:|ΔIc| is set to 2:1:1 for Figure 4A, and 0:1:1 and √3: for Figures 5A, 6A, and 7A, respectively.
This is when the ratio is 1:1 and 1:1:1. (1) A phase 1 wire disconnection (i) In equation (10), multiplying ΔIc by a is
Since the purpose is to rotate ΔIc counterclockwise by 120 degrees, the vectors ΔIa and ΔIa shown in Figure 4A are
The relationship between ΔIb and ΔIc is as shown in FIG. 4B.
As is clear from this figure, |ΔIb− of equation (10)
Since ΔIc·a| is √3 and |ΔIa| is 2, STa is √3/2. (ii) Calculate STb at this time as follows. If ΔIa in equation (11) is rotated by 120° as in (i), the relationship between vectors ΔIa, ΔIb, and ΔIc shown in Figure 4A becomes as shown in Figure 4C, |ΔIc−ΔIa・a | is √3 and |ΔIb| is 1, so STb is √
It becomes 3. (ii) Furthermore, calculate STc at this time as follows. If ΔIb in equation (12) is rotated by 120° as in (i), we get
The relationship between ΔIa, ΔIb and ΔIc in Figure 4A is
As shown in Figure D, |ΔIa−ΔIb·a| is √3, and |ΔIc| is 1, so STc is √3. (2) BC phase single-phase load release If you do the same thing as described above, Fig. 5A will become as shown in Fig. 5B, Fig. 5C, and Fig. 5D, respectively, and since ΔIa is 0, STa becomes 1/0=∞. Further, both STb and STc are 1/1=1. (3) AB/CA phase V load release If you do the same thing as described above, Figure 6A will become like Figure 6B, Figure 6C, and Figure 6D, respectively, and STa will be 1/√3 , STb and STc are both 1/1=1. (4) 3-phase load release If you do the same thing as described above, Fig. 7A will become as shown in Fig. 7B, Fig. 7C, and Fig. 7D, respectively, |ΔIb−ΔIc・a|, | Since ΔIc−ΔIa・a| and |ΔIa−ΔIb・a| are both 0, STa=
STb=STc=0. Here, Table 1 shows the values of STa, STb, and STc when one wire of the A phase is disconnected and when various loads are released.

【表】 この表は、3相平衡負荷におけるA相1線断線
時および負荷開放時のSTa,STbおよびSTcの値
を算出したものであつて、この2つの状態の間で
はこれらの値が異なつていることを示している。
したがつて、断線であると判定する値例えば1.5
を設定し、断熱条件としてSTa,STbおよびSTc
のうちといずれか2つが1.5(ただし、∞の値はと
らないものとする。)より大きいとき断線である
とすれば、第1表から判るように3相平衡負荷に
おける1線断線を検出することができる。さら
に、断線検出を高めるためにSTa,STbおよび
STcの3つの値を加算した直例えば4.0(ただし、
∞の値はとらないものとする。)を断線であると
判定する値としてもよい。 ところが、不平衡負荷においてはその不平衡度
によつて第1表に示す値が変化することになり、
特にA相1線断線時とAB・CA相V負荷開放時
では重なることがある。したがつて、1線断線と
V負荷開放とを区別しようとすれば、ある不平衡
度の範囲を設定して、その条件の下でのA相1線
断線時およびAB・CA相V負荷開放時のSTa,
STbおよびSTcを算出することによつて断線であ
ると判定する値を決定しなければならない。以下
にその値の算出について説明する。 (a) A相1線断線 Y=ica/iab(>0)とおき、これを(4)式乃至(6) 式に代入し、さらにこれらの式を(10)式乃至(12)式
に代入して求めた式はそれぞれ次式のようにな
る。 STb=√1+2−2(−−120゜
……(14) STc=1/Y√1+2−2(−−120゜) ……(15) また、 (b) AB・CA相V負荷開放 第2図Cに示すようにV負荷開放後の各線電
流Ia′,Ib′およびIc′は Ia′=0 Ib′=ibcej〓・a2 Ic′=−ibcej〓・a2 となり、各電流の変化分ΔIa,ΔIbおよびΔIc
は次式のようになる。 ΔIa=−iabej〓+icaej〓・a ……(17) ΔIb=iabej〓 ……(18) ΔIc=−icaej〓・a ……(19) ここで、Y=ica/iab(>0)とおき、これを (17)式乃至(19)式に代入し、さらにこれら
の式を(10)式乃至(12)式に代入して求めた式はそれ
ぞれ次式のようになる。 このようにして求めたSTa,STbおよびSTcに
ついて、(α−τ)をパラメータとして|α−τ
|≦30゜の範囲でのYとA相1線断線時およびV
負荷開放時のそれぞれのSTa,STbおよびSTcと
の関係をグラフに描く(図示しない)。このグラ
フでY=1のときのSTa,STbおよびSTcの値か
ら断線であると判定する値Aを予め設定し、その
値Aを基にして次の3つの断線条件を考える。 P;STa,STbおよびSTcのうちいずれか2つが
Aより大きいときに断線とする。 Q;STa,STbおよびSTcのうち少なくとも1つ
がAより大きいときに断線とする。ただし、∞
の値はとらないものとする。 R;STがAより大きいときに断線とする。ただ
し、∞の値はとらないものとする。 したがつて、このAの値を求めるためには、A
を種々に変化させて、|α−τ|≦30゜、0.1≦Y
≦2の範囲で断線条件P,QおよびRをそれぞれ
満足するように、上述した図示しないグラフから
それぞれの断線を検出できる範囲とV負荷開放を
検出できる範囲とを表にする(図示しない)。例
えば、断線および負荷開放が検出できるときに
は、○印を付け、検出できないときには×印を付
ける。 この表から断線検出範囲をできるだけ広く、か
つV負荷開放時の誤動作をできるだけ少なくする
ようなAを断線条件P,QおよびRについてそれ
ぞれ知ることができる。つぎに、それぞれのAを
基にして、断線を検出できる範囲とV負荷開放を
検出できる範囲とを上述した図示しない表から、
Yを横軸に、(α−τ)を縦軸にした表を作成す
ることによつて、あるYと(α−τ)との範囲で
のA相1線断線の検出を確認することができる。 このようにして、断線条件Pについては、A=
1.15となり、このときのYと(α−τ)の条件は
0.4≦Y≦2.0、−30゜≦α−τ≦+10゜となる。ま
た、断線条件Qについては、A=1.63となり、こ
のときのYと(α−τ)の条件は、0.1≦Y≦
2.0、−30゜≦α−τ≦+10゜となる。さらに、断線
条件Rについては、A=3.56となり、このときの
Yと(α−τ)の条件は0.5≦Y≦2.0、−10゜≦α
−τ≦+30゜となる。 したがつて、断線条件P,QおよびRのいずれ
か1つを満足すれば、1線断線と負荷開放とを判
別することができる。このことは、第1表に示し
た値から3相平衡負荷におけるA相1線断線が検
出できることからして明らかである。 なお、以上の説明は、A相の断線を検出する場
合についてであつたが、B相またはC相の断線検
出についても、前述したのと同様の手法によつて
検出することができることは明らかである。 以上のように、本発明の電線路の断線検出方法
によれば、それぞれの断線条件に応じた値を予め
設定することによつて、そのいずれかの条件でも
3相平衡負荷はもちろん不平衡負荷であつても、
3相負荷開放、V負荷開放または単相負荷開放な
どの負荷変化と1線の断線とを変電所において検
出することができる利点があり有益である。
[Table] This table shows the calculated values of STa, STb, and STc when one wire of A phase is disconnected and when the load is opened under a three-phase balanced load.These values differ between these two states. It shows that it is on.
Therefore, the value for determining a disconnection is, for example, 1.5.
and set STa, STb and STc as the adiabatic conditions.
If any two of these are greater than 1.5 (however, the value of ∞ is not taken), it is considered a wire breakage, then as can be seen from Table 1, a single wire breakage in a three-phase balanced load is detected. be able to. Additionally, STa, STb and
For example, the sum of the three values of STc is 4.0 (however,
Assume that the value of ∞ is not taken. ) may be used as a value to determine that the wire is disconnected. However, in the case of an unbalanced load, the values shown in Table 1 will change depending on the degree of unbalance.
In particular, the situation may overlap when one wire of the A phase is disconnected and when the AB/CA phase V load is released. Therefore, in order to distinguish between a single wire break and a V load release, it is necessary to set a certain range of unbalance, and under that condition, to distinguish between a single wire break in the A phase and a V load release in the AB and CA phases. Time STa,
By calculating STb and STc, the value at which it is determined that the wire is disconnected must be determined. The calculation of this value will be explained below. (a) A phase 1 wire disconnection Set Y = ica/iab (>0), substitute this into equations (4) to (6), and then convert these equations into equations (10) to (12). The equations obtained by substituting are as follows. STb=√1+ 2 −2(−−120°
……(14) STc=1/Y√1+ 2 −2(−−120°) ……(15) Also, (b) AB/CA phase V load released As shown in Figure 2C, each line current Ia', Ib' and Ic' after V load is released is Ia'=0 Ib'=ibce j 〓・a 2 Ic'= −ibce j 〓・a 2 , and the changes in each current ΔIa, ΔIb and ΔIc
is as follows. ΔIa=−iabe j 〓+icae j 〓・a ...(17) ΔIb=iabe j 〓 ...(18) ΔIc=−icae j 〓・a ...(19) Here, Y=ica/iab(>0 ), then substitute these into equations (17) to (19), and then substitute these equations into equations (10) to (12) to obtain the following equations. For STa, STb, and STc obtained in this way, |α−τ
|When Y and A phase 1 wire is disconnected in the range of ≦30° and V
Draw a graph of the relationship between STa, STb, and STc when the load is released (not shown). In this graph, a value A for determining a wire breakage is set in advance from the values of STa, STb, and STc when Y=1, and the following three wire breakage conditions are considered based on the value A. P: When any two of STa, STb, and STc are greater than A, the wire is broken. Q: When at least one of STa, STb, and STc is greater than A, the wire is broken. However, ∞
Assume that the value of is not taken. R: When ST is greater than A, the wire is broken. However, the value of ∞ shall not be taken. Therefore, in order to find the value of A,
By variously changing |α−τ|≦30°, 0.1≦Y
In order to satisfy each of the disconnection conditions P, Q, and R in the range of ≦2, the range in which each disconnection can be detected and the range in which V load release can be detected are tabulated from the above-mentioned graph (not shown) (not shown). For example, if a disconnection or load release can be detected, mark it with a circle, and if it cannot be detected, mark it with an x. From this table, it is possible to know, for each of the disconnection conditions P, Q, and R, A that makes the disconnection detection range as wide as possible and minimizes the malfunction when the V load is released. Next, based on each A, the range in which disconnection can be detected and the range in which V load release can be detected are determined from the table (not shown) mentioned above.
By creating a table with Y on the horizontal axis and (α-τ) on the vertical axis, it is possible to confirm the detection of A phase 1 wire disconnection in a certain Y and (α-τ) range. can. In this way, for the disconnection condition P, A=
1.15, and the conditions for Y and (α−τ) at this time are
0.4≦Y≦2.0, −30°≦α−τ≦+10°. Also, regarding the disconnection condition Q, A=1.63, and the condition of Y and (α-τ) at this time is 0.1≦Y≦
2.0, −30°≦α−τ≦+10°. Furthermore, regarding the disconnection condition R, A=3.56, and the conditions for Y and (α-τ) are 0.5≦Y≦2.0, -10°≦α
−τ≦+30°. Therefore, if any one of the wire breakage conditions P, Q, and R is satisfied, it is possible to distinguish between a single wire break and a load release. This is clear from the fact that a single wire break in the A phase can be detected in a three-phase balanced load from the values shown in Table 1. Although the above explanation has been about detecting a disconnection in the A phase, it is clear that the same method as described above can also be used to detect a disconnection in the B phase or C phase. be. As described above, according to the wire breakage detection method of the present invention, by setting values in advance according to each breakage condition, it is possible to detect not only a three-phase balanced load but also an unbalanced load under any of the conditions. Even if it is,
It is advantageous that load changes such as three-phase load opening, V load opening, or single-phase load opening, and one-wire breakage can be detected at a substation.

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

第1図は変電所T1に負荷L1および負荷L2が接
続された線路を示す図、第2図A乃至Dはそれぞ
れA相1線断線時の等価回路、BC相単相負荷開
放時の等価回路、AB・CA相V負荷開放時の等
価回路、3相負荷開放時の等価回路を示す図、第
3図A乃至Dはそれぞれ3相平衡負荷におけるA
相1線断線時、BC相単相負荷開放時、AB・CA
相V負荷開放時および3相負荷開放時の変電所に
おける線電流のベクトル図、第4図A、第5図
A、第6図Aおよび第7図Aはそれぞれ第3図A
乃至Dにおけるベクトル値の変化分ΔIa,ΔIbお
よびΔIcを示すベクトル図、第4図B乃至D、第
5図B乃至D、第6図B乃至Dおよび第7図B乃
至Dはそれぞれ第4図A、第5図A、第6図Aお
よび第7図Aに示すベクトルを反時計方向に120゜
ベクトル回転させた後のベクトル図である。
Figure 1 is a diagram showing the lines where load L 1 and load L 2 are connected to substation T 1. Figure 2 A to D are equivalent circuits when one wire of A phase is disconnected, and when a single phase load of BC phase is opened. Figures 3A to 3D show the equivalent circuit when the AB/CA phase V load is opened, and the equivalent circuit when the 3-phase load is opened.
When one phase wire is disconnected, when the BC phase single phase load is opened, AB/CA
Vector diagrams of line currents in the substation when phase V load is released and phase 3 load is released, Figures 4A, 5A, 6A, and 7A are respectively Figure 3A
Vector diagrams showing changes in vector values ΔIa, ΔIb, and ΔIc in D to D, FIG. 4 B to D, FIG. 5 B to D, FIG. 6 B to D, and FIG. 7 B to D are respectively shown in FIG. A is a vector diagram after the vectors shown in FIG. 5A, FIG. 6A, and FIG. 7A are rotated counterclockwise by 120 degrees.

Claims (1)

【特許請求の範囲】 1 3相電線路の各線電流Ia,IbおよびIcがそれ
ぞれIa′,Ib′およびIcに変化したときの各ベクト
ル値の変化分ΔIa=Ia′−Ia,ΔIb=Ib′−Ibおよび
ΔIc=Ic′−Icから、A相、B相およびC相断線時
の断線指数STa,STbおよびSTc STa=|ΔIb−ΔIc・a/ΔIa| STb=|ΔIc−ΔIa・a/ΔIb| STc=|ΔIa−ΔIb・a/ΔIc| を求め、これらのSTa,STbおよびSTcの値が予
め定めた関係になつたことを検出して断線である
と判定する電線路の断線検出方法。 2 前記予め定めた関係は、STa,STbおよび
STcの値のうちいずれか2つが1.15より大きいと
きである特許請求の範囲第1項に記載の電線路の
断線検出方法。 3 前記予め定めた関係は、STa,STbおよび
STcの値のうち少なくとも1つが1.63(ただし、
∞の値はとらないものとする。)より大きいとき
である特許請求の範囲第1項に記載の電線路の断
線検出方法。 4 前記予め定めた関係は、STa+STb+STcの
値が3.56(ただし、∞の値はとらないものとす
る。)より大きいときである特許請求の範囲第1
項に記載の電線路の断線検出方法。
[Claims] 1. Changes in each vector value when the line currents Ia, Ib and Ic of the three-phase electric line change to Ia', Ib' and Ic, respectively ΔIa = Ia' - Ia, ΔIb = Ib' From −Ib and ΔIc=Ic′−Ic, the disconnection index STa, STb, and STc at the time of A-phase, B-phase, and C-phase disconnection STa=|ΔIb−ΔIc・a/ΔIa| STb=|ΔIc−ΔIa・a/ΔIb A method for detecting a break in an electric line by determining |STc=|ΔIa−ΔIb・a/ΔIc| and determining that the wire is broken by detecting that the values of STa, STb, and STc have a predetermined relationship. 2 The predetermined relationship is STa, STb and
The method for detecting disconnection in an electric line according to claim 1, wherein any two of the values of STc are larger than 1.15. 3 The predetermined relationship is STa, STb and
At least one of the STc values is 1.63 (but
Assume that the value of ∞ is not taken. ) The method for detecting disconnection of an electric line according to claim 1, wherein the wire breakage detection method is larger than . 4. Claim 1, wherein the predetermined relationship is when the value of STa + STb + STc is larger than 3.56 (however, the value of ∞ is not taken).
Disconnection detection method of electric line as described in section.
JP56152484A 1981-09-25 1981-09-25 Detection of disconnection for line Granted JPS5853770A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56152484A JPS5853770A (en) 1981-09-25 1981-09-25 Detection of disconnection for line

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56152484A JPS5853770A (en) 1981-09-25 1981-09-25 Detection of disconnection for line

Publications (2)

Publication Number Publication Date
JPS5853770A JPS5853770A (en) 1983-03-30
JPH0136594B2 true JPH0136594B2 (en) 1989-08-01

Family

ID=15541492

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56152484A Granted JPS5853770A (en) 1981-09-25 1981-09-25 Detection of disconnection for line

Country Status (1)

Country Link
JP (1) JPS5853770A (en)

Also Published As

Publication number Publication date
JPS5853770A (en) 1983-03-30

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