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JPS6011532B2 - 2-wire fault distance relay device - Google Patents
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JPS6011532B2 - 2-wire fault distance relay device - Google Patents

2-wire fault distance relay device

Info

Publication number
JPS6011532B2
JPS6011532B2 JP13200073A JP13200073A JPS6011532B2 JP S6011532 B2 JPS6011532 B2 JP S6011532B2 JP 13200073 A JP13200073 A JP 13200073A JP 13200073 A JP13200073 A JP 13200073A JP S6011532 B2 JPS6011532 B2 JP S6011532B2
Authority
JP
Japan
Prior art keywords
voltage
phase
circuit
negative
sequence
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
JP13200073A
Other languages
Japanese (ja)
Other versions
JPS5080452A (en
Inventor
高幸 松田
省介 中里
健治 鈴木
信一 東
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.)
Mitsubishi Electric Corp
Tokyo Electric Power Co Holdings Inc
Original Assignee
Tokyo Electric Power Co Inc
Mitsubishi Electric Corp
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 Tokyo Electric Power Co Inc, Mitsubishi Electric Corp filed Critical Tokyo Electric Power Co Inc
Priority to JP13200073A priority Critical patent/JPS6011532B2/en
Publication of JPS5080452A publication Critical patent/JPS5080452A/ja
Publication of JPS6011532B2 publication Critical patent/JPS6011532B2/en
Expired legal-status Critical Current

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Description

【発明の詳細な説明】 この発明は2線短絡故障を検出しこれを保護するに通し
た2線故障用距離継電装層の改良に関するものである。
DETAILED DESCRIPTION OF THE INVENTION This invention relates to an improvement in a two-wire fault distance relay system for detecting and protecting against two-wire short circuit faults.

この発明は分岐端のある系統にもない系統にも適用でき
るが,分岐端を有しない系統についてこの発明を説明す
る。途中に分岐端のない第1図に示す如き通常の送電線
の2線故障に応動する距離継電装魔としては、従来次の
ような動作式を満足する装置が提案された。
Although this invention can be applied to systems with and without branch ends, the invention will be described for systems without branch ends. Conventionally, as a distance relay device that responds to a two-wire failure in a normal power transmission line as shown in FIG. 1 without a branch end in the middle, a device that satisfies the following operating formula has been proposed.

IV2−ZS121>IV.−ZSI.1 ……
{11IV2一2212l>IV.1
……【21これは次のような考えにより提案されたもの
である。
IV2-ZS121>IV. -ZSI. 1...
{11IV2-2212l>IV. 1
...[21 This was proposed based on the following idea.

第2図aは第1図の系統に2線短絡故障が生じた場合の
等価回路図であり、継電器設置点RYにおける正相及び
逆相電圧をV,,V2、正相及び逆相電流を1,,12
、継電器設置点RYから故障点Fまでの正相及び逆相イ
ンピーダンスをZ,F,Z幻,故障点F‘こおける正相
及び逆相電圧をV,F,V奴とすればV,一Z,F1,
=V,F “”“【31V2−乞
披i2;マ2F ……【4}なる両式が
成立し、しかもVIFニV2F,.・ニ−12
”””【5Iなる関係を有する。
Figure 2a is an equivalent circuit diagram when a two-wire short circuit fault occurs in the system shown in Figure 1, where the positive-sequence and negative-sequence voltages at the relay installation point RY are V, , V2, and the positive-sequence and negative-sequence currents are 1,,12
, the positive-sequence and negative-sequence impedances from the relay installation point RY to the fault point F are Z, F, Z illusion, and the positive-sequence and negative-sequence voltages at the fault point F' are V, F, V, then V, - Z, F1,
=V,F """[31V2-I2; M2F .....[4] Both formulas hold true, and VIF2V2F,..Ni-12
"""[5I has the relationship.

なお上記{3},■式中において(以後も同機)、正相
及び逆相電流の極性は電源側から線路側に流れる方向を
正としている。したがって上識31,‘41式中のZ小
Z2F(一般にZ,F:Z2F=ZF)の代わりに保
護区間内のィンピーダンス則ち整定インピーダンスZs
を導入して(v,−乏S,.)及び(v2−Z3;2)
を導出すれ‘よ、整定点上の故障時即ちZs=Z,F=
Z2Fならば、(V,一Zsl,)=(V2−Zs12
) ……{6}V,=(V2一Zs12)
……のとなる。この場合の各ベクトルの関係を第2
図bに示す。ここで1.:ー12でありZ,F=Z2p
であるためZ,F1,とZ2F12は絶対値が等しく極
性が逆になる。したがって内部故樟即ちIZSー>ーZ
,FIならば(V,−ZS1,)<V化 (V2−乞Si2)>V岬 となって (VI−Zjl)<(V2−ZS12) 肌”■V
.<(V2一次s12) ……{9}となる。
Note that in the above {3}, (2) equations (hereinafter also referred to as the same device), the polarity of the positive-phase and negative-phase currents is positive in the direction of flowing from the power supply side to the line side. Therefore, instead of Z small Z2F (generally Z, F: Z2F = ZF) in the formula 31 and '41, the impedance within the protection area, ie, the settling impedance Zs
By introducing (v,-poorS,.) and (v2-Z3;2)
Derive the fault at the settling point, that is, Zs=Z, F=
If Z2F, (V, - Zsl,) = (V2 - Zs12
) ...{6}V, = (V2 - Zs12)
It becomes... The relationship between each vector in this case can be expressed as
Shown in Figure b. Here 1. :-12 and Z, F=Z2p
Therefore, Z, F1, and Z2F12 have equal absolute values and opposite polarities. Therefore, the internal fallen camphor, that is, IZS->-Z
, FI is (V, -ZS1,)<V conversion (V2-Shi2)>V cape (VI-Zjl)<(V2-ZS12) skin"■V
.. <(V2 primary s12) ...{9}.

また外部故障即ちIZslくIZ,FIならば(V,一
Zsl,)>V,F (V2−Zs12)<V2p となつて (Vュ−ZSII)>(V2−ZS12) ……
00VI>(V2−Z312) ……
血となる。
Also, if there is an external failure, that is, IZsl - IZ, FI, then (V, - Zsl,) > V, F (V2 - Zs12) < V2p, so (V - ZSII) > (V2 - ZS12) ...
00VI>(V2-Z312)...
Becomes blood.

したがって(V,一乞Si,)と(V2−ZS12)と
またはV,と(V2一Zs12)との大4・を比較すれ
ば2線故障が内部に生じたか外部に生じたかを検出でき
る。ところが周知のように故障相如何により正相成分と
逆相成分とがその位相関係を互いに120度異にする状
態となるので、結局両者の絶対値の大きさを比較する必
要が生ずる。この考えのもとに結局【1},■式に応動
する距離継電装直が提案されたわけである。しかしなが
ら上記‘1’,‘21式に応敷する継電装層は故障抵抗
則ちアーク抵抗Rfを考慮していない。アーク抵抗Rf
を考慮した場合にはその等価回路は第3図のようになる
。第3図においてアーク抵抗Rfによる電圧降下をVf
とすると故障点Fにおける正相電圧V,Fは逆相電圧V
的とVfとの和に等しいから、V2F+Vf=V,Fす
なわち、V冴ニVIF−VfニVI一ZIF11一Vf
ニV2一Z2F12..・.・・(12)という関係に
なる。
Therefore, by comparing (V, Si,) and (V2-ZS12) or V, and (V2-Zs12), it is possible to detect whether a two-wire fault has occurred internally or externally. However, as is well known, depending on the nature of the fault, the phase relationship between the normal phase component and the negative phase component may differ by 120 degrees from each other, so it becomes necessary to compare the magnitudes of their absolute values. Based on this idea, a distance relay system that responds to formulas [1] and (2) was eventually proposed. However, the relay equipment layer applied to the above formulas '1' and '21 does not take into account the fault resistance, that is, the arc resistance Rf. Arc resistance Rf
When considering this, the equivalent circuit becomes as shown in FIG. In Figure 3, the voltage drop due to arc resistance Rf is Vf
Then, the positive sequence voltage V at the fault point F, F is the negative sequence voltage V
Since it is equal to the sum of the target and Vf, V2F + Vf = V, F, that is, V - VIF - Vf - VI - ZIF11 - Vf
D V2-Z2F12. ..・.. ...The relationship is (12).

したがって上記{1},{2)式はアーク抵抗を考慮す
るとき正確な動作を期待できなくなる。このことを第4
図により説明する。第4図イはZs=Z,F=Z2Fす
なわち整定点上にアーク抵抗Rfを伴なつた故障が生じ
た場合の第3図の各ベクトルと−Zs12ベクトルを示
すベクトル図である。整定点上の故障の場合、アーク抵
抗Rfがなければ上記‘6}式からV2−孝処i2十Z
.F1.=V・v2一(Z的十字2F)12=V,…”
(13)(.:11ニ−12)となるはずである。
Therefore, the above equations {1} and {2) cannot be expected to operate accurately when arc resistance is taken into account. This is the fourth
This will be explained using figures. FIG. 4A is a vector diagram showing each vector in FIG. 3 and the -Zs12 vector when Zs=Z, F=Z2F, that is, a fault accompanied by arc resistance Rf occurs on the settling point. In the case of a failure on the settling point, if there is no arc resistance Rf, from the above equation '6}, V2 - Kosho i20Z
.. F1. =V・v21 (Z cross 2F) 12=V,…”
It should be (13) (.:11-12).

しかしアーク抵抗Rfによる電圧降下Vfがあると .
V2−(Z.F十字2F)12十Vf:V.……(14
)なる関係となり、Zs=Z,F=Z2Fを考えると、
(V2−2Si2)<(V.−ZSL)(V2−幻s1
2)<V,(.:1,=−12は不変である為)となっ
て、上記‘2},(11)式から明らかなように外部故
障と判定してしまうのである。
However, if there is a voltage drop Vf due to arc resistance Rf.
V2- (Z.F cross 2F) 120 Vf:V. ...(14)
), and considering Zs=Z, F=Z2F,
(V2-2Si2)<(V.-ZSL)(V2-phantom s1
2)<V, (because .:1,=-12 is unchanged), and as is clear from the above equation '2} and (11), it is determined that there is an external failure.

この誤差はいうまでもなくアーク抵抗Rfによる電圧降
下Vfが原因となっている。したがってこの誤差をなく
すにはアーク抵抗欠fによる電圧降下Vfの影響を避け
ればよいわけである。このアーク抵抗による電圧降下V
fは−12と同相であるのでVfの影響を避けるには上
記(14)式の電圧をすべて−ら‘こ直角な成分すなわ
ちリアクタンス分電圧のみとすればよい。即ち(14)
式においてV,と1,との相差角をQ,(V2−友s1
2)と(一12)との相差角を6とするときIV2−2
212lsin6>IV,lsinQ….・・(15)
なる動作式を得れば、もはやァ」ク抵抗Rfの影響を受
けない正確な距離継電装層が得られる。
Needless to say, this error is caused by the voltage drop Vf due to the arc resistance Rf. Therefore, in order to eliminate this error, it is sufficient to avoid the influence of the voltage drop Vf due to the lack of arc resistance f. Voltage drop V due to this arc resistance
Since f is in phase with -12, in order to avoid the influence of Vf, all the voltages in the above equation (14) should be made into only the component perpendicular to -ra', that is, the reactance component voltage. That is (14)
In the equation, the phase difference angle between V and 1 is defined as Q, (V2 - friend s1
When the phase difference angle between 2) and (-12) is 6, IV2-2
212lsin6>IV,lsinQ…. ...(15)
If the operating formula is obtained, an accurate distance relay layer that is no longer affected by the arc resistance Rf can be obtained.

第4図イではIV2−Zs12lsin6=IV,ls
inQとなって動作不動作の限界点となる。第4図口は
整定点よりもリレー設置則こ近い所で2線短絡故障が生
じた場合で動作となる場合のベクトル図である。
In Figure 4 A, IV2-Zs12lsin6=IV,ls
inQ, which becomes the limit point of inoperability. The opening in FIG. 4 is a vector diagram in the case where the relay is activated when a two-wire short circuit fault occurs at a location closer to the relay installation rule than the setting point.

IZsl>IZ,Fl,IZ2FIであるので−りこ直
角な成分を比較するとIV2−22121Sin8>I
V.ISinQとなって動作する。第4図ハは整定点よ
りも遠い所で2線短絡故障が生じた場合で不動作となる
場合のベクトル図である。
Since IZsl>IZ, Fl, IZ2FI, comparing the components perpendicular to Riko, IV2-22121Sin8>I
V. It operates as ISinQ. FIG. 4C is a vector diagram in the case where a two-wire short circuit fault occurs at a location far from the settling point and the device becomes inoperable.

このときは、ーZSI<IZ,Fl,IZ2plである
ので−12に直角な成分を比較するとIV2−2212
lsin6<IV,lsinQとなって不動作となる。
In this case, -ZSI<IZ, Fl, IZ2pl, so comparing the components perpendicular to -12, we get IV2-2212
lsin6<IV, lsinQ and becomes inoperable.

(15)式に代えて IV2−ZsらISin8>IV.一ZS121Sin
y.・・…(16)なる動作式を用いても同様である。
Instead of formula (15), IV2-Zs et al. ISin8>IV. 1ZS121Sin
y. The same effect can be obtained by using the operation formula (16).

ただし、8一‘まv2−2Si2と−12とのなす角度
、上記【1’,■,(15),(16)式なる動作式に
よる継電装層は、対称分電圧、電流を使用しているため
、系統のCT,PTより得た、各相電圧「電流より対称
分を得るための特別のフィルターが必要で、通常の距離
継電器に比して、その入力回路が煩雑となるのが欠点で
ある。
However, the angle formed by 81'ma v2-2Si2 and -12, the relay layer according to the operation formula of [1', Therefore, a special filter is required to obtain a symmetrical component from each phase voltage and current obtained from the CT and PT of the grid, and the disadvantage is that the input circuit is more complicated than a normal distance relay. It is.

第5図にその1例として式(16)を動作式とする継電
器回路をブロック図で示す。
As an example, FIG. 5 shows a block diagram of a relay circuit whose operation formula is expressed by equation (16).

すなわち、(16)式右辺を構成するものとして各相電
圧V^,VB,Vcより、正相電圧V,を導出する正相
電圧フィルタ{11と各相電流1^,IB,lcより正
相電流1,を導出する正相電流フィルタ‘21力ミ必要
で、これら出力を合成量である抑制力リアクタンス分電
圧ーv,一ZS;,ーsinyを演算する演算回路51
で合成して(v,一ZSi,)を得ると共に(v,一Z
Si,)の1,=−121こ対する正弦量、すなわちそ
のリアクタンス分電圧ーv,”ZSi,ーsinyを求
める。こ)でyは(v,−学si,)と−12の相差角
である。一方、(16)式の左辺については、各相電圧
V^,V8,Vcより逆相電圧V2を導出する逆相電圧
フィル夕3と各相電流1,,12,ヒより逆相電流を導
出する逆相電流フィル夕4が必要で、これら出力を合成
量である動作力リアクタンス分電圧IV2−Zs12l
sin8を演算する演算回路6で合成して、(V2一Z
s12)を得ると共に(V2一Zs12)の(一Z)に
対する正弦量、すなわちそのリアクタンス分電圧IV2
−Zs12lsin8を求める。こ)で3は(v2−Z
Si2)とく一12)の相差角である。更に7は判定回
路で前記演算回路5,6の出力の大小を比較し、演算回
路6の出力つまり動作力がまさる時のみ出力をとり出し
、継電器出力とするのである。しかして上記のように(
16)式ではV,,V2,1,,12の4つの対称分フ
ィル夕が必要であり、入力回路が煩雑となる。また、各
相の入力電圧に高調波成分が含まれ、例えばAB相間電
圧のみが、3角波となった場合上記フィル夕は大きく影
響を受ける。但しここで正相電圧及び逆相函圧フィルム
構成の見本式を式(17)及び(18)とする。対,=
マ岬十BCeJi肌“ (17). . ・ i
z3 (18)3V2=VBc十V^Be−
−…… y=群(Sino−きn38十夢in58・・・)・・
・・・・(19)ここでYは3角波の波高値。
In other words, the right side of equation (16) is composed of a positive-sequence voltage filter {11 that derives the positive-sequence voltage V, from each phase voltage V^, VB, and Vc, and a positive-sequence voltage filter {11} that derives the positive-sequence voltage V, from each phase current 1^, IB, and lc. A calculation circuit 51 that calculates the suppressing force reactance voltage -v, -ZS;, -siny, which is a composite quantity of these outputs, is necessary for the positive sequence current filter '21 which derives the current 1, -siny.
to obtain (v, -ZSi,) and (v, -ZSi,)
Find the sine quantity of 1,=-121 of Si,), that is, its reactance voltage -v,''ZSi,-siny.In this), y is the phase difference angle of (v,-Si,) and -12. On the other hand, regarding the left side of equation (16), the negative phase voltage filter 3 which derives the negative phase voltage V2 from each phase voltage V^, V8, Vc and the negative sequence current from each phase current 1, , 12, H A negative-sequence current filter 4 is required to derive the operating force reactance voltage IV2-Zs12l, which is a composite quantity of these outputs.
It is synthesized by the arithmetic circuit 6 that calculates sin8, and (V2-Z
s12) and the sine amount of (V2-Zs12) for (-Z), that is, its reactance voltage IV2
- Find Zs12lsin8. In this), 3 is (v2-Z
This is the phase difference angle of Si2) and Kuichi12). Furthermore, 7 is a determination circuit which compares the magnitude of the outputs of the arithmetic circuits 5 and 6, and takes out the output only when the output of the arithmetic circuit 6, that is, the operating force exceeds it, and uses it as a relay output. However, as mentioned above (
Equation 16) requires four symmetrical filters of V, , V2, 1, and 12, making the input circuit complicated. Further, if the input voltage of each phase contains a harmonic component, and for example, only the voltage between AB and phase becomes a triangular wave, the above-mentioned filter is greatly affected. However, here, sample equations for the positive-sequence voltage and the negative-sequence canal pressure film configuration are given by equations (17) and (18). pair, =
Ma Misaki 10 BCeJi skin” (17). . . ・i
z3 (18)3V2=VBc ten V^Be-
−... y=group (Sino-kin38 Tomu in58...)...
...(19) Here, Y is the peak value of the triangular wave.

第2項まで考えると、3角波=基本波一言X第3高調波
‐‐‐‐‐‐(20)例えば、比相2線短絡故障時、A
B相線間電圧^Bが3角波となると、式(17)より3
V,の誤差は(−きin38)となり、式(18)より
3 V2の誤差は(−きin38)ej型3=十きin
38(基本波の60度進みは、第3高調波の180度進
みに相当する)となるため、この誤差分を考慮すると正
相電圧V.はV,=基本波−第3高調波、逆相電圧V2
はV2=基本波十第3高調波となり、その概略の波形は
第6図C,Dに示すようになる。
Considering up to the second term, triangular wave = fundamental wave x 3rd harmonic --- (20) For example, in the case of a ratio-phase two-wire short circuit fault, A
When the B phase line voltage ^B becomes a triangular wave, 3 is obtained from equation (17).
The error of V, is (-ki in38), and from equation (18), the error of 3 V2 is (-ki in38) ej type 3 = tenki in
38 (a 60 degree lead of the fundamental wave corresponds to a 180 degree lead of the third harmonic), so if this error is taken into consideration, the positive sequence voltage V. is V, = fundamental wave - 3rd harmonic, negative phase voltage V2
V2=fundamental wave 10th harmonic, and its approximate waveform is shown in FIG. 6C and D.

尚第6図Aは基本波形、Bは第3高調波形である。この
ような場合、式(15)及び式(16)のようにリアク
タンス分電圧を求めても、正しい応動は期待できない。
第6図Aは基本波形、Bは第3高調波形、C,Dは正相
電圧V,逆相電圧V2の波形線図である。例えば(15
)式の右辺IV,lsinQを求めることは、交流電気
量V,が所定位相に達したときの瞬時値を求めることを
意味する。V,と−らの相差角がQであるときは、第7
図に示すようにしてサンプリングして求める。
Note that FIG. 6A shows the fundamental waveform, and B shows the third harmonic waveform. In such a case, correct response cannot be expected even if the reactance voltage is determined as in equations (15) and (16).
FIG. 6A is a fundamental waveform, B is a third harmonic waveform, and C and D are waveform diagrams of a positive phase voltage V and a negative phase voltage V2. For example (15
) Determining the right-hand side IV,lsinQ of the equation means determining the instantaneous value when the alternating current electrical quantity V, reaches a predetermined phase. When the phase difference angle between V, and - is Q, the seventh
Obtain it by sampling as shown in the figure.

VIニIVIISinのt −12ニI一12ISin(山t−Q) とすると、一Lコ0、すなわちのt一Q=0のときサン
プリングパルス凶が発生されるようにし、このPSのタ
イミングでV,をサンプリングすれば、このときのV,
の瞬時値は、■t=Qであるから、IV,lsinQと
なる。
If t-12I-12ISin (mountain t-Q) of VI-IVIISin, a sampling pulse is generated when 1L is 0, that is, t-Q=0, and V is set at the timing of this PS. , then V,
Since ■t=Q, the instantaneous value of is IV,lsinQ.

このようにしてサンプリングによつてIV,lsinは
を求めるときは、V,の波形が歪まないことが前提であ
って、V,の波形が第6図のように歪むと誤差が大きく
なる。
When determining IV,lsin by sampling in this manner, it is assumed that the waveform of V, is not distorted, and if the waveform of V, is distorted as shown in FIG. 6, the error becomes large.

例えば、相差角Q,8,y,6をすべて90度とすると
、第6図の波形からも明らかなように式(15)右辺I
V,lsinQは上記誤差分だけ値が増加し、また式(
16)右辺ーV,一ZSi,ーsinyも上記誤差分だ
け値を増す。
For example, if the phase difference angles Q, 8, y, and 6 are all 90 degrees, as is clear from the waveform in FIG.
The value of V,lsinQ increases by the above error, and the formula (
16) The values of -V, -ZSi, -siny on the right side are also increased by the above error.

一方式(15)左辺IV2−2ら12lsin6は上記
誤差分だけ値が減じ、また式(16)左辺,v2−2S
i21sinGも上記誤差分だけ値が減ずる。すなわち
左辺の値が減じ右辺の値が増すため、不動作方向に作用
し、アンダーリーチとなる。以上説明したように‘11
,■式の動作式による継電装層はアーク抵抗に弱く対称
分フィル夕が必要など回路も複雑であり、また(15)
,(16)式の動作式による継電装置はアーク抵抗に強
いがV,,V2,1,,12の4つの対称分フィル夕1
,2,3,4が必要なこと、および電圧歪の影響で正し
いリーチが得られないという欠点がある。
On the other hand, the value of the left side of equation (15) IV2-2 to 12l sin6 is reduced by the above error, and the left side of equation (16),
The value of i21sinG is also reduced by the above error. In other words, the value on the left side decreases and the value on the right side increases, which acts in the direction of non-operation, resulting in underreach. As explained above, '11
The relay layer based on the operating formula of the , ■ formula is weak in arc resistance and requires a symmetrical filter, and the circuit is complicated, and (15)
, (16) is strong against arc resistance, but the four symmetric filters V, , V2, 1, and 12
, 2, 3, and 4 are required, and correct reach cannot be obtained due to the influence of voltage distortion.

この発明はアーク抵抗には弱いが電圧入力の導入に前記
正相電圧フィル夕、逆相電圧フィル夕を不要として、入
力回路を煩雑とすることなく電圧歪の影響を回避できる
2線故障用距離継電装層を提供することを目的とする。
Although this invention is weak against arc resistance, it eliminates the need for the above-mentioned positive-sequence voltage filter and negative-sequence voltage filter when introducing voltage input, and the two-wire fault distance can avoid the effects of voltage distortion without complicating the input circuit. The purpose is to provide a relay system layer.

すなわち、各相電圧V^.VB,Vcの線間電圧を導入
して、それぞれlkVBcl,lkVc^l,lkV^
8l(但しkは定数)を得るようにした回路と、各相電
流i^,IB,ICより逆相電流12を導出する12フ
ィル夕をへて、l−滋12ー(但しZsは整定インピー
ダンス)をうるようにした回路とを備え、l−2212
lがlkVBcl,lkVc^l,lkV^BIのいず
れか1つよりも大なる時に判定出力が得られるように構
成する。今、式糊,‘4’,‘5}なる関係がある時V
,一V2=一ZF12 ……(21)整定
インピーダンスZsを考慮して、内部故障則ちIZsl
>IZ,plであるならば(V,−V2)く2212と
なるが、前記の理由により両辺の絶対値の大きさを比較
することによりIV,−V2lくIZs12l
……(22)とすることができる。
That is, each phase voltage V^. Introducing the line voltages of VB and Vc, lkVBcl, lkVc^l, lkV^, respectively
8l (where k is a constant) and 12 filters that derive the negative phase current 12 from each phase current i^, IB, IC, and then pass through a circuit designed to obtain 8l (k is a constant) and 12 filters that derive the negative phase current 12 from each phase current i^, IB, IC. ), the l-2212
The configuration is such that a determination output is obtained when l is larger than any one of lkVBcl, lkVc^l, and lkV^BI. Now, when there is a relationship like Shikinori, '4', '5} V
, - V2 = - ZF12 ... (21) Considering the setting impedance Zs, the internal fault, i.e., IZsl
> IZ, pl, then (V, -V2) × 2212, but for the reason mentioned above, by comparing the magnitudes of the absolute values on both sides, IV, -V2l × IZs12l
...(22) can be made.

ここで、第8図はこの発明の実施例ブロック図で、第9
図は下記の式を動作式とする本発明による総電器の位相
特性線図を示す。今BC相2線短絡故障時を考えると VBc=VB−Vc=(a2一a)(V,一V2)・・
・・・(23)v.−v2=a茸羊……(24)ぽい=
千ぷね 式(24)を式(22)に代入すると 1ま事1<1−ゑ3121……(25) 左辺は絶対値であるからk=1三三1=芸とするとlk
VBCI<1一22121 ……(26)とな
る。
Here, FIG. 8 is a block diagram of an embodiment of this invention, and FIG.
The figure shows a phase characteristic diagram of a general electric appliance according to the present invention whose operation formula is as shown below. Now considering the BC phase two wire short circuit failure, VBc = VB - Vc = (a2 - a) (V, - V2)...
...(23) v. -v2=a mushroom sheep...(24) Poi=
Substituting the Senpune equation (24) into the equation (22), 1 Makoto 1 < 1 - 3121... (25) Since the left side is the absolute value, if k = 1 3 1 = art, then lk
VBCI<1-22121 (26).

また、Cん相及びAB相2線短絡故障に対しては各々C
A相線間電圧V。
In addition, for C phase and AB phase two-wire short circuit failures,
A phase line voltage V.

^,AB相線間電圧V^8より、lkVC^1<1−2
ち121 …‐・‐(27)‘kV^8l<l一
2212l ……(28)なる動作式のものを適
用すればよい。
^, From AB phase line voltage V^8, lkVC^1 < 1-2
121...--(27)'kV^8l<l-2212l...(28) may be applied.

上記式(26),(27),(28)は線間電圧を使用
しているため正相電圧フィル夕、逆相電圧フィル夕並び
に正相電流フィル外ま不要で入力回路を簡素化できると
共に、前述の電圧歪による影響も、線間電圧の絶対値l
kV8Gl,lkVc^l,lkV^BI及びl一Zs
らlを使用するため、交流電気量を全波整流すればよい
ので波形の歪があっても誤差は少なくて済む。
Since the above equations (26), (27), and (28) use line voltage, the input circuit can be simplified by eliminating the need for positive-sequence voltage filters, negative-sequence voltage filters, and positive-sequence current filters. , the effect of the voltage distortion mentioned above also affects the absolute value l of the line voltage
kV8Gl, lkVc^l, lkV^BI and l-Zs
Since the AC voltage is used, it is sufficient to perform full-wave rectification of the alternating current electrical quantity, so even if there is waveform distortion, the error is small.

かくて第8図で式(26),(27),(28)の右辺
を構成するものとして、逆相電流12を導出する逆相電
流フィル夕9があり、左辺を構成するものとして各線間
電圧を導入してこれらに比例した入力をうる回路8があ
る。
Thus, in FIG. 8, the right-hand sides of equations (26), (27), and (28) include the negative-sequence current filter 9 that derives the negative-sequence current 12, and the left-hand sides of the There is a circuit 8 which introduces voltages and obtains an input proportional to these.

次に前述の回路8の出力は3つの抑制カーkVBc!,
lkVc^l,lkV^BI演算回路10a,10b,
10cに、逆相電流フィルタ回路9の出力は1つの動作
カー−Zsもl演算回路11にそれぞれ加えられ、更に
それぞれの出力l−2212lと出力lkVBCl,l
kVc^l,lkV^BIとをそれぞれの判定回路12
a,12b,12cで比較し、演算回路11の出力つま
り動作力がまさるときのみ出力をとり出しオア回路13
をへて逐電出力がえられるもので3つの判定回路12a
,12b,12.cの出力のうち1つでも出れば、継電
器出力がえられるのである。
Next, the output of the aforementioned circuit 8 is the three suppression cars kVBc! ,
lkVc^l, lkV^BI operation circuits 10a, 10b,
10c, the output of the negative phase current filter circuit 9 is applied to the operation circuit 11, respectively, and the output l-2212l and the output lkVBCl, l
kVc^l and lkV^BI are determined by respective judgment circuits 12.
A, 12b, and 12c are compared, and the output is taken out only when the output of the arithmetic circuit 11, that is, the operating force is superior, and the OR circuit 13
There are three judgment circuits 12a that can provide a reactive output through the
, 12b, 12. If even one of the outputs of c is output, the relay output can be obtained.

従って、第5図の従来例に比して、フィルタ回路は逆相
電流フィル夕9のみで良く、また、逆相電流12を使用
するため潮流の影響を受けにくいことは前記式【1},
{21,(15),(16)を動作式とする各継電器と
同様である。以上のようにこの発明の2縁故陣用距離継
電装層によれば、アーク抵抗による電圧降下分を回避で
きずアーク抵抗に対しては【1’,‘2}式による従釆
のものと同等性能となるが、フィルタ回路を逆相電流フ
ィル夕のみとして他は線間電圧を導入して使用するため
、回路構成が簡単で電圧歪の影響を回避できるのである
Therefore, compared to the conventional example shown in FIG. 5, the filter circuit requires only the negative-sequence current filter 9, and since the negative-sequence current 12 is used, it is less susceptible to the influence of power flow.
{21, (15), (16) are the same as each relay whose operation type is used. As described above, according to the distance relay system layer for two dependent relays of the present invention, the voltage drop due to arc resistance cannot be avoided, and the arc resistance is equivalent to that of the secondary relay based on formulas [1', '2}. In terms of performance, since the filter circuit is used only as a negative phase current filter and the line voltage is introduced for the rest, the circuit configuration is simple and the influence of voltage distortion can be avoided.

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

第1図は通常の2端子系統を示す系統図、第2図aは第
1図の系統に2線短絡故障が生じたときの等価回路図、
第2図bはこの場合のベクトル図、第3図は第1図の系
統にァーク抵抗を伴なつた2線短絡が生じたときの等価
回路図であり、第4図はこの場合のベクトル図、第5図
は従来の継電器回路のブロック図、第6図は従来の装置
で三角波の影響を受けた場合の正相電圧フィル夕、逆相
電圧フィル夕の出力波形線図、第7図はIJァクタンス
成分を求めるサンプリングの説明図、第8図はこの発明
の実施例継電回路のブロック図、第9図は本発明による
位相特性図である。 図で8は線間電圧に比例した入力を得る回路、9は逆相
電圧フィル夕、10a,10b,10cは夫々抑制力l
kV8cl,lkVc^l,lkV^BIを演算する演
算回路、1 1は動作力l−2も12lを演算する演算
回路、12a,12b,12cは判定回路、13はオア
回路である。第1図 第2図 第3図 第4図 第5図 第8図 第9図 第6図 第7図
Figure 1 is a system diagram showing a normal two-terminal system, Figure 2a is an equivalent circuit diagram when a two-wire short circuit fault occurs in the system in Figure 1,
Figure 2b is a vector diagram in this case, Figure 3 is an equivalent circuit diagram when a two-wire short circuit with arc resistance occurs in the system in Figure 1, and Figure 4 is a vector diagram in this case. , Fig. 5 is a block diagram of a conventional relay circuit, Fig. 6 is an output waveform diagram of a positive-sequence voltage filter and a negative-sequence voltage filter when affected by a triangular wave in a conventional device, and Fig. 7 is an output waveform diagram of a conventional device affected by a triangular wave. FIG. 8 is a block diagram of a relay circuit according to an embodiment of the present invention, and FIG. 9 is a phase characteristic diagram according to the present invention. In the figure, 8 is a circuit that obtains an input proportional to the line voltage, 9 is a negative phase voltage filter, and 10a, 10b, and 10c are suppressing forces l, respectively.
An arithmetic circuit that calculates kV8cl, lkVc^l, and lkV^BI; 11 is an arithmetic circuit that computes operating force l-2 and 12l; 12a, 12b, and 12c are determination circuits; and 13 is an OR circuit. Figure 1 Figure 2 Figure 3 Figure 4 Figure 5 Figure 8 Figure 9 Figure 6 Figure 7

Claims (1)

【特許請求の範囲】[Claims] 1 被保護系統の各相電圧■_A,■_B,■_Cの線
間電圧を導入して、それぞれ|k■_B_C|,|k■
_C_A|,|k■_A_B|(但しkは定数)を導出
する回路、各相電流■_A,■_B,■_Cを導入して
、被保護系統の逆相電流I_2を導出する逆相電流フイ
ルタ、この逆相電流フイルタの出力および整定インピー
ダンス■_Sから|−2■_S■_2|をうる演算回路
、ならびに|−2■_S■_2|が|k■_B_C|,
|k■_C_A|,|k■_A_B|のいずれかよりも
大なる時に判定出力を出力する判定回路を備えた2線故
障用距離継電装置。
1. Introducing the line voltages of each phase voltage ■_A, ■_B, ■_C of the protected system, respectively |k■_B_C|, |k■
A circuit that derives _C_A|, |k■_A_B| (where k is a constant), a negative-sequence current filter that introduces each phase current ■_A, ■_B, and ■_C and derives the negative-sequence current I_2 of the protected system. , an arithmetic circuit that obtains |-2■_S■_2| from the output of this negative-phase current filter and the setting impedance ■_S, and |-2■_S■_2| is |k■_B_C|,
A two-wire failure distance relay device comprising a determination circuit that outputs a determination output when it is larger than either |k■_C_A| or |k■_A_B|.
JP13200073A 1973-11-22 1973-11-22 2-wire fault distance relay device Expired JPS6011532B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP13200073A JPS6011532B2 (en) 1973-11-22 1973-11-22 2-wire fault distance relay device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP13200073A JPS6011532B2 (en) 1973-11-22 1973-11-22 2-wire fault distance relay device

Publications (2)

Publication Number Publication Date
JPS5080452A JPS5080452A (en) 1975-06-30
JPS6011532B2 true JPS6011532B2 (en) 1985-03-26

Family

ID=15071200

Family Applications (1)

Application Number Title Priority Date Filing Date
JP13200073A Expired JPS6011532B2 (en) 1973-11-22 1973-11-22 2-wire fault distance relay device

Country Status (1)

Country Link
JP (1) JPS6011532B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP3038144B2 (en) * 1995-12-25 2000-05-08 北陸電気工業株式会社 Circuit board

Also Published As

Publication number Publication date
JPS5080452A (en) 1975-06-30

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