JPH0222605B2 - - Google Patents
Info
- Publication number
- JPH0222605B2 JPH0222605B2 JP7968883A JP7968883A JPH0222605B2 JP H0222605 B2 JPH0222605 B2 JP H0222605B2 JP 7968883 A JP7968883 A JP 7968883A JP 7968883 A JP7968883 A JP 7968883A JP H0222605 B2 JPH0222605 B2 JP H0222605B2
- Authority
- JP
- Japan
- Prior art keywords
- signal
- signals
- relay device
- protective relay
- angle
- 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
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- Emergency Protection Circuit Devices (AREA)
Description
【発明の詳細な説明】
この発明は、電力系統を保護する保護継電装置
に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a protective relay device for protecting a power system.
従来、この種の装置として第1図に示すものが
あつた。1,2は電源、3,4は遮断器、5は遮
断器3,4を介して電源1,2の接続する送電
線、6a,6bは電源1,2の母線、7a,7b
は遮断器3,4の近傍の送電線5に設けられた変
流器、8は母線6aに接続された変圧器、9は保
護継電装置である。 Conventionally, there has been a device of this type as shown in FIG. 1 and 2 are power supplies, 3 and 4 are circuit breakers, 5 is a power transmission line to which power supplies 1 and 2 are connected via circuit breakers 3 and 4, 6a and 6b are busbars of power supplies 1 and 2, 7a and 7b
8 is a current transformer provided on the power transmission line 5 near the circuit breakers 3 and 4, 8 is a transformer connected to the bus bar 6a, and 9 is a protective relay device.
第2図は保護継電装置の構成を示すブロツク図
である。10は変流器7より送電線5の電流の信
号I1(t)を入力し、変圧器8より母線6aの電
圧の信号V1(t)を入力し、インピーダンスZ
(t)(=V1(t)/I1(t)を計算し、出力する演算
回路、
11は演算回路10からインピーダンスZ(t)
を表わす信号(以下、信号Z(t)という)を入
力し、その軌跡からゾーン通過時間とゾーン通過
の有無とを判定して信号11a,11bで出力す
る判定回路、12は信号11aのレベルを検出す
る検出器、13は検出器12の信号12aと判定
回路11の信号11bとのアンドをとるアンド・
ゲートで、遮断器3へ遮断信号9aを供給する。 FIG. 2 is a block diagram showing the configuration of the protective relay device. 10 inputs the current signal I 1 (t) of the transmission line 5 from the current transformer 7, inputs the voltage signal V 1 (t) of the bus 6a from the transformer 8, and inputs the impedance Z
(t)(=V 1 (t)/I 1 (t)) and an arithmetic circuit that calculates and outputs it.
A determination circuit 12 inputs a signal representing Z(t) (hereinafter referred to as signal Z(t)), determines the zone passage time and the presence or absence of zone passage based on its locus, and outputs the results as signals 11a and 11b. A detector 13 performs an AND operation of the signal 12a of the detector 12 and the signal 11b of the determination circuit 11.
A cutoff signal 9a is supplied to the circuit breaker 3 at the gate.
次に、動作について説明する。第3図は信号
V1をY軸方向に固定し、母線7の電圧の信号V2
が相対的に信号V1に対する角度Θを開いて行く
ときのベクトル関係を示す。母線6bの電圧の信
号V2が信号V1と同相のときは、両者間に電圧差
がなく、信号I1(0)は零である。しかし、この
角度Θが90゜のときは、両者間に電圧差が生じ、
信号I1(90)は零でなくなる。以下、同様に各角
度Θについて関係を示すと、信号I1(t)は円軌
跡14上を移動する。系統が正常な状態では、信
号V1,V2はほぼ同相又はわずかな開きをもつて
いる。このため、信号Z(t)のR,jX座標上の
位置は、R成分大、jX成分≒0の点にある。こ
のような関係を角度Θとの対応で示すと、第4図
のようになる。 Next, the operation will be explained. Figure 3 is a signal
V 1 is fixed in the Y-axis direction, and the voltage signal of bus 7 is V 2
shows the vector relationship when increasing the angle Θ relative to the signal V 1 . When the voltage signal V 2 of the bus 6b is in phase with the signal V 1 , there is no voltage difference between them, and the signal I 1 (0) is zero. However, when this angle Θ is 90°, a voltage difference occurs between the two,
The signal I 1 (90) is no longer zero. Below, similarly showing the relationship for each angle Θ, the signal I 1 (t) moves on the circular locus 14. When the system is normal, the signals V 1 and V 2 are almost in phase or have a slight difference. Therefore, the position of the signal Z(t) on the R, jX coordinates is at a point where the R component is large and the jX component is approximately 0. FIG. 4 shows such a relationship in relation to the angle Θ.
系統の事故等の擾乱により、脱調に進む過程の
例として、信号V1とV2との間の角度が開いて行
くとき、インピーダンス軌跡はR−jX座標の中
心部分を通過して第2又は第3象現へ移動するこ
とが分る。従つて、判定回路11はこのようなイ
ンピーダンスZ(t)の性質に基づき、これが第
5図のZに示すような検出ゾーンを通過する時間
とゾーンを通過するか否かを判定することによつ
て脱調現象の発生を検知し、それらの結果を信号
11a,11bで出力する。信号11aは検出器
12でレベルが判定され、信号12aとなる。ア
ンド・ゲート13は信号11a,12aのアンド
により信号9aを出力して遮断器8の遮断を実行
させる。 As an example of a process in which synchronization progresses due to a disturbance such as a system accident, when the angle between signals V 1 and V 2 increases, the impedance locus passes through the center of the R-jX coordinate and becomes the second Or it can be seen that it moves to the third quadrant. Therefore, the determination circuit 11 determines the time it takes for impedance Z(t) to pass through the detection zone as shown by Z in FIG. The occurrence of the synchronization phenomenon is detected, and the results are output as signals 11a and 11b. The level of the signal 11a is determined by the detector 12 and becomes a signal 12a. AND gate 13 outputs signal 9a by ANDing signals 11a and 12a to cause circuit breaker 8 to shut off.
従来の保護継電装置は、以上のように構成され
ており、系統脱調に対する対応が系統網計算や動
揺試験との照合によつていたために、系統の変貌
への対応が難しい欠点があり、また脱調の判別を
インピーダンス軌跡の座標に換算して系統をとら
えているので、特異な現象点又は状態量の変極点
でとらえることができず、検出整定値の決定が困
難であるなどの欠点があつた。 Conventional protective relay devices are configured as described above, and have the disadvantage that it is difficult to respond to changes in the power grid because the response to power outages is based on grid network calculations and verification with oscillation tests. In addition, since the system is detected by converting the step-out determination into the coordinates of the impedance locus, it is not possible to detect it at a singular phenomenon point or an inflection point of the state quantity, and it is difficult to determine the detection setting value. There were flaws.
この発明は、上記のような従来のものの欠点を
除去するためになされたもので、脱調現象を信号
I,V及びその間の角度Θから算出した電気量を
示す信号P,Qの変化から検出するべく、信号P
の値が極大となり、かつ信号Qの値が増加を続け
ることを判定することにより、系統構成に影響さ
れることなく、かつ整定項目が少なく、明確に脱
調の判定して保護動作を実行できる保護継電装置
を提供することを目的とする。 This invention was made in order to eliminate the drawbacks of the conventional ones as described above, and detects the step-out phenomenon from changes in the signals P and Q indicating the amount of electricity calculated from the signals I and V and the angle Θ between them. In order to do so, the signal P
By determining that the value of is maximum and the value of signal Q continues to increase, it is possible to clearly determine step-out and execute protective action without being affected by the system configuration and with fewer setting items. The purpose is to provide a protective relay device.
以下、この発明による一実施例を図について説
明する。保護継電装置9と系統との間の接続は第
1図に示すものと同様である。この発明による保
護継電装置9の構成は第6図に示すようになつて
いる。第6図において、14は信号V(t)、I
(t)から信号P,Qを算出する算出部、15信
号P,QからP−Q座標を設定する設定部、16
は設定部15の出力から以下で説明する論理判定
をする論理部である。 An embodiment according to the present invention will be described below with reference to the drawings. The connection between the protective relay device 9 and the grid is similar to that shown in FIG. The structure of the protective relay device 9 according to the present invention is shown in FIG. In FIG. 6, 14 is the signal V(t), I
(t) a calculation unit that calculates signals P and Q; 15 a setting unit that sets P-Q coordinates from signals P and Q; 16
is a logic unit that makes a logical decision based on the output of the setting unit 15, which will be explained below.
次に動作について説明する。算出部14は、信
号V(t)、I(t)を入力し、P=VIcosΘ、Q=
VIsinΘの演算をして信号P,Qを出力する。信
号P,Qは、グラフで示すと角度Θに対して第7
図に示すような変化をし、信号Pは角度Θ=90゜
で極大値を示し、信号Qは角度Θ=180゜で極大値
を示し、両者はA点で等しくなる。設定部15は
このA点を検出し、それを示す信号P2,Q2を出
力する。 Next, the operation will be explained. The calculation unit 14 inputs the signals V(t) and I(t), and calculates that P=VIcosΘ, Q=
It calculates VIsinΘ and outputs signals P and Q. The signals P and Q are shown as 7th with respect to the angle
The changes occur as shown in the figure, with signal P showing a maximum value at an angle Θ=90°, signal Q showing a maximum value at an angle Θ=180°, and both become equal at point A. The setting unit 15 detects this point A and outputs signals P 2 and Q 2 indicating it.
一般に電力系統では、その同期化力の大小も関
係するが、角度Θが90゜以上開くと、脱調したと
判断してよい。ただし、このときの信号Qは増加
を継続している場合である。このため、この発明
において、論理部16は、脱調を示す点である信
号Pが増加から減少に転ずる点、即ち系統動揺に
よる信号Pの振動のピークを示し、かつ両端の角
度Θが90゜に開いたことにより信号Pが極大値と
なり、かつそのときに信号Qが増加していことを
脱調発生の判定条件とする。なお、信号Pが極大
となり、かつ信号Qの値も極大となる点Aは、角
度Θが90゜以内で信号P及びQが振動している状
態である。即ち、論理部16は、信号Pが極大と
なり、かつ信号Qの値が一定値k以上で増加中の
とき、即ちdQ/dt>kのときは、信号Θが90゜を超
えて大きくなつたと判定し、かつ脱調と判定す
る。この状態を第8図のP−Q座標上に示す。信
号P,Qが共に極大となる振動の場合は、軌跡
P,QがBのように一定の楕円上を往復する。こ
のとき、信号Pは最大値P1となり、信号Qは最
大値Q1となり、信号P及びQはこれより大きい
値の組み合せをもたない。角度Θが90゜を超える
場合、軌跡P,Qは、Cで示すように図中のA点
を通過するときに信号Pが最大値P2となつた後
減少に転じ、信号QがQ1→Q2→Q3と増加する傾
向にある。このようなA点を通過することによつ
て脱調を判定し、判定部16は信号9aを出力す
る。 In general, in power systems, the magnitude of the synchronization force is also relevant, but if the angle Θ opens by 90 degrees or more, it can be determined that synchronization has occurred. However, the signal Q at this time continues to increase. Therefore, in the present invention, the logic unit 16 indicates the point at which the signal P, which indicates step-out, changes from increasing to decreasing, that is, the peak of vibration of the signal P due to system fluctuation, and the angle Θ at both ends is 90°. The condition for determining the occurrence of step-out is that the signal P reaches its maximum value due to the opening, and that the signal Q increases at that time. Note that at point A, where the signal P is at its maximum and the value of the signal Q is also at its maximum, the signals P and Q are oscillating within an angle Θ of 90°. That is, when the signal P reaches a maximum and the value of the signal Q is increasing beyond a certain value k, that is, when dQ/dt>k, the logic unit 16 determines that the signal Θ has increased beyond 90°. and is determined to be out of synch. This state is shown on the P-Q coordinates in FIG. In the case of vibration where both the signals P and Q are maximum, the trajectories P and Q reciprocate on a fixed ellipse like B. At this time, the signal P has a maximum value P1 , the signal Q has a maximum value Q1 , and the signals P and Q have no combination of values larger than these. When the angle Θ exceeds 90°, the trajectories P and Q reach the maximum value P2 when passing through point A in the figure, as shown by C, and then begin to decrease, and the signal Q becomes Q1. There is a tendency to increase from →Q 2 →Q 3 . Step-out is determined by passing through such a point A, and the determining section 16 outputs a signal 9a.
なお、上記実施例では、脱調の場合について説
明したが、アナログ演算回路を備え、ピーク検出
(P)+時間微分量レベル検出(Q)を実行させて
もよく、また電気量のデイジタルサンプリング値
によりプログラム制御をするマイクロコンピユー
タを用いてもよい。更に、第8図のA点における
Qの時間微分が一定値以上であるとしたが、Q2
±ΔQの両値の間を通過する時間が一定値以内で
あると判定する論理部を備えてもよい。ただし、
ΔQは信号Qの微小値である。 Although the above embodiment describes the case of step-out, an analog calculation circuit may be provided to perform peak detection (P) + time differential amount level detection (Q), or digital sampling value of electrical quantity may be used. A microcomputer that performs program control may also be used. Furthermore, it is assumed that the time derivative of Q at point A in Figure 8 is greater than a certain value, but Q 2
The device may include a logic unit that determines that the time passing between both values of ±ΔQ is within a certain value. however,
ΔQ is a minute value of signal Q.
以上のように、この発明によれば、信号Pが最
大となり、かつ信号Qが増加中であることを脱調
の判定条件として保護動作をするので、角度が
90゜に開くような状況を正しく応動することがで
き、また判定条件を定める整定値の設定が簡単と
なり、系統の変更に対しても対応が簡単になる効
果がある。 As described above, according to the present invention, since the protection operation is performed using the signal P being at its maximum and the signal Q being increasing as the condition for determining step-out, the angle
It is possible to respond correctly to situations such as opening to 90 degrees, and it is also easier to set the setting values that determine the judgment conditions, making it easier to respond to changes in the system.
第1図は保護継電装置と系統の接続図、第2図
は従来の保護継電装置のブロツク図、第3図は第
1図に示す系統の電圧及び電流のベクトル図、第
4図は第1図に示す系統の電圧及び電流のベクト
ル図そのインピーダンスのグラフ、第5図は従来
の保護継電装置で脱調現象を検出する時のインピ
ーダンス平面上での検出ゾーンを説明するための
図、第6図はこの発明の一実施例による保護継電
装置のブロツク図、第7図及び第8図は第6図に
示す保護継電装置の信号のグラフである。
1,2……電源、3,4……遮断器、5……送
電線、7a,7b……変流器、8……変圧器、9
……保護継電装置、14……算出部、15……設
定部、16……論理部、なお、図中、同一符号は
同一又は相当部分を示す。
Fig. 1 is a connection diagram of the protective relay device and the system, Fig. 2 is a block diagram of a conventional protective relay device, Fig. 3 is a vector diagram of the voltage and current of the system shown in Fig. 1, and Fig. 4 is Figure 1 is a vector diagram of the voltage and current of the system and its impedance graph. Figure 5 is a diagram for explaining the detection zone on the impedance plane when detecting a step-out phenomenon with a conventional protective relay device. , FIG. 6 is a block diagram of a protective relay device according to an embodiment of the present invention, and FIGS. 7 and 8 are graphs of signals of the protective relay device shown in FIG. 6. 1, 2... Power source, 3, 4... Circuit breaker, 5... Power transmission line, 7a, 7b... Current transformer, 8... Transformer, 9
...Protective relay device, 14... Calculation section, 15... Setting section, 16... Logic section. In the drawings, the same reference numerals indicate the same or equivalent parts.
Claims (1)
圧信号V及び上記自端と相手端の電源とを接続す
る送電線における上記自端の電流を示す電流信号
Iから第1及び第2の電力量P,Q(ただし、P
=I(t)・V(t)cosΘ、Q=I(t)V(t)
sinΘ、ΘはI及びVがなす角度)を算出する算
出部と、上記第1の電力量Pの極大値を検出し、
かつ上記第2の電力量Qが所定値以上の増大量と
なるのを検出したときに脱調を示す信号を出力す
る論理部とを備え、脱調を示す上記信号に従つて
上記送電線を保護するようにした保護継電装置。1. The first and second signals are obtained from the voltage signal V indicating the voltage of the bus connected to the power supply at the own end and the current signal I indicating the current at the own end in the transmission line connecting the power supply at the own end and the power supply at the opposite end. Electric energy P, Q (however, P
=I(t)・V(t) cosΘ, Q=I(t)V(t)
sinΘ, Θ is the angle formed by I and V); and a calculation unit that detects the maximum value of the first power amount P;
and a logic unit that outputs a signal indicating step-out when it is detected that the second power amount Q increases by a predetermined value or more, and the power transmission line is controlled in accordance with the signal indicating step-out. A protective relay device designed to protect the user.
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7968883A JPS59204419A (en) | 1983-05-07 | 1983-05-07 | Protecting relaying device |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP7968883A JPS59204419A (en) | 1983-05-07 | 1983-05-07 | Protecting relaying device |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59204419A JPS59204419A (en) | 1984-11-19 |
| JPH0222605B2 true JPH0222605B2 (en) | 1990-05-21 |
Family
ID=13697139
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP7968883A Granted JPS59204419A (en) | 1983-05-07 | 1983-05-07 | Protecting relaying device |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPS59204419A (en) |
-
1983
- 1983-05-07 JP JP7968883A patent/JPS59204419A/en active Granted
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59204419A (en) | 1984-11-19 |
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