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JPS6217452B2 - - Google Patents
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JPS6217452B2 - - Google Patents

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Publication number
JPS6217452B2
JPS6217452B2 JP54005742A JP574279A JPS6217452B2 JP S6217452 B2 JPS6217452 B2 JP S6217452B2 JP 54005742 A JP54005742 A JP 54005742A JP 574279 A JP574279 A JP 574279A JP S6217452 B2 JPS6217452 B2 JP S6217452B2
Authority
JP
Japan
Prior art keywords
distance
time
circuit
voltage
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
Application number
JP54005742A
Other languages
Japanese (ja)
Other versions
JPS5597127A (en
Inventor
Norio Suda
Yoshihiro Kawasaki
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.)
Meidensha Electric Manufacturing Co Ltd
Original Assignee
Meidensha Electric Manufacturing 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 Meidensha Electric Manufacturing Co Ltd filed Critical Meidensha Electric Manufacturing Co Ltd
Priority to JP574279A priority Critical patent/JPS5597127A/en
Publication of JPS5597127A publication Critical patent/JPS5597127A/en
Publication of JPS6217452B2 publication Critical patent/JPS6217452B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 本発明は電力系統の送電線を保護するデイジタ
ル式保護継電方式に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a digital protective relay system for protecting power transmission lines of a power system.

電力系統を保護する保護継電装置(以下リレー
と略称)は、系統の拡大、電源容量および短絡容
量の増大、送電線の超高圧化、長距離化、ケーブ
ル化等に伴いリレー性能、即ち事故判定速度と判
定精度の向上が要求され、初期の電磁形リレーか
らトランジスタ形リレーへと技術進歩に伴い発展
してきた。現在はマイクロコンピユータの出現に
より従来のアナログ方式とは異なつたデイジタル
方式によるコンピユータリレーの開発が各方面で
なされ、様々なデイジタル保護方式が提案されて
いる。
Protective relay devices (hereinafter referred to as relays) that protect power systems are becoming more and more important due to the expansion of power systems, increases in power supply capacity and short-circuit capacity, ultra-high voltage of power transmission lines, longer distances, cables, etc. Improvements in judgment speed and accuracy were required, and as technology progressed, relays evolved from early electromagnetic relays to transistor relays. Currently, with the advent of microcomputers, computer relays are being developed in various fields using a digital method, which is different from the conventional analog method, and various digital protection methods are being proposed.

しかしながら従来のアナログリレーを含めこれ
まで提案されているデイジタル保護方式の大部分
はその保護原理が単一の基本周波数成分に着目し
た交流理論に基づくものであつた。このため入力
に他周波成分が重畳した場合は大きな誤差となり
誤動作、誤不動作を招く事になる。これを避ける
ため入力段にフイルタを設置して基本周波数以外
の成分を除去しなければならず、論理的には基本
周波数の1周期(50Hzで20ms)のフイルタ過度
遅れ分が生じ、これがリレーの動作時間遅れの主
要因となつていた。またフイルタはリレーの精度
を決定する主要因でもあるため、フイルタの設計
は動作速度と動作精度というリレーの性能を決定
するものであつた。
However, most of the digital protection systems that have been proposed so far, including conventional analog relays, have a protection principle based on AC theory that focuses on a single fundamental frequency component. Therefore, if other frequency components are superimposed on the input, a large error will result, leading to malfunction or malfunction. To avoid this, it is necessary to install a filter at the input stage to remove components other than the fundamental frequency, and logically, an excessive filter delay of one period of the fundamental frequency (20 ms at 50 Hz) is generated, which is caused by the delay of the relay. This was the main cause of delay in operation time. Furthermore, since the filter is the main factor that determines the accuracy of the relay, the design of the filter determines the performance of the relay in terms of operating speed and operating accuracy.

一方、電力系統では送電線の超高圧化およびケ
ーブル系統の増設に伴う静電容量の増大のため事
故が発生すると非常に激しい過渡現象が生じてい
る。しかもこの過渡現象は線路抵抗の減少によつ
て系統時定数が長くなつているため、相当長く続
く傾向にある。このため、事故時にリレーに入力
される電圧、電流も時定数の長い歪率の大きい歪
波形となり、高精度に事故を判別しようとすると
忠実に基本波のみを通過させるフイルタの設置は
不可避である。
On the other hand, in electric power systems, due to the ultra-high voltage of power transmission lines and the increase in capacitance due to the expansion of cable systems, extremely severe transient phenomena occur when an accident occurs. Moreover, this transient phenomenon tends to last for quite a long time because the system time constant has become longer due to the decrease in line resistance. For this reason, the voltage and current input to the relay at the time of an accident will have a distorted waveform with a long time constant and a large distortion factor, and in order to accurately identify an accident, it is unavoidable to install a filter that faithfully passes only the fundamental wave. .

しかしながら、短絡容量の増大と送電線の長距
離化によつて過渡安定度の維持および向上のため
にますます高速度な事故除去が必要であり、リレ
ーの動作速度も速いものが要求されている。従つ
て、これまでのような交流理論によるリレー原理
では、基本波の1周期分というフイルタの過渡遅
れ分を持つため、このような要求を満たすために
は本質的な欠陥があつた。
However, as short-circuit capacity increases and power transmission lines become longer distances, faster fault removal is required to maintain and improve transient stability, and relays are also required to operate at higher speeds. . Therefore, the conventional relay principle based on AC theory has an essential defect in satisfying such requirements because it has a transient delay of the filter corresponding to one period of the fundamental wave.

また従来の距離継電器は分布定数回路において
抵抗をR、インダクタンスをLとしてインピーダ
ンスをZ=R+jωLとして表わしてきた。しか
しながら、キヤパシタンスCを無視することは、
特に長距離架空線やケーブル系統においては距離
継電器が大きな誤差を持ち好ましくない。
Further, in a conventional distance relay, impedance has been expressed as Z=R+jωL, where resistance is R and inductance is L in a distributed constant circuit. However, ignoring the capacitance C,
Especially in long-distance overhead lines and cable systems, distance relays have large errors and are undesirable.

本発明は以上のような点に鑑みてなされたもの
で、従来の単一周波数に基づいた交流理論による
従来形の距離リレーでは動作時間に限界を有して
いたのを、時間に基づく新しい原理を導くことに
より、これを応用した高速度で、しかもキヤパシ
タンスを無視せずに高精度な距離継電方式を提供
しようとするもので、以下本発明を従来例と比較
しながら詳細に説明する。
The present invention has been made in view of the above points, and is based on a new principle based on time, which has a limited operating time in conventional distance relays based on AC theory based on a single frequency. By deriving this, the present invention is applied to provide a high-speed, high-precision distance relaying method without neglecting capacitance.The present invention will be explained in detail below in comparison with a conventional example.

まず、分布定数を持つ送電線の偏微分方程式に
ついて述べる。
First, we will discuss partial differential equations for power transmission lines with distributed constants.

第1図は送電線一条に対する等価回路図で、単
位長当りの分布定数であるインダクタンスL
〔H/Km〕、抵抗R〔Ω/Km〕、キヤパシタンスC
〔H/Km〕、コンダクタンスG〔/Km〕が線路に
そつて分布する様を表わしている。図中e(o,
t),i(o,t)は位置x=0、時刻tにおけ
る電圧、電流で、時間tに関して既知量あるいは
計測量である。e(x,t),i(x,t)は送
電線の位置x=x、時刻tにおける電圧、電流で
あり、これらは次の偏微分方程式を満足する事は
周知である。
Figure 1 is an equivalent circuit diagram for a single power transmission line, and shows the inductance L, which is a distributed constant per unit length.
[H/Km], resistance R [Ω/Km], capacitance C
It shows how [H/Km] and conductance G [/Km] are distributed along the track. In the figure e(o,
t), i(o, t) are voltage and current at position x=0 and time t, and are known or measured quantities with respect to time t. e(x, t) and i(x, t) are the voltage and current at the power transmission line position x=x and time t, and it is well known that these satisfy the following partial differential equation.

この偏微分方程式をxについて積分しxの境界
条件を考慮すれば解を得る。境界条件としてx=
o点の電圧、電流を用い、位置x=o点をリレー
の設置点とすれば、この解は位置x=x点の電圧
e(x,t)、電流i(x,t)のふるまいをリ
レー設置点の電圧e(o,t)、電流i(o,
t)で表わすものとなる。
A solution is obtained by integrating this partial differential equation with respect to x and taking into account the boundary conditions of x. As a boundary condition x=
Using the voltage and current at point o, and assuming position x = point o as the relay installation point, this solution describes the behavior of voltage e (x, t) and current i (x, t) at position x = x. Voltage e (o, t) and current i (o, t) at the relay installation point
t).

(1)式において、時間偏微分演算子∂/∂をPとお
い て行列表現すれば次のようになる。
In equation (1), if the time partial differential operator ∂/∂ t is expressed as a matrix by P, the following is obtained.

ここで とおくと、uについて、次のようなxの1階常微
分方程式となる。
here Then, for u, the first-order ordinary differential equation of x is as follows.

−d/du(x、t)=(A+BP)u(x、t)… …(3) (3)式を境界条件を考慮して解くと次式となる。 −d/d x u(x, t)=(A+BP)u(x, t)... (3) When equation (3) is solved taking into account the boundary conditions, the following equation is obtained.

u(x、t)=ε-(A+BP)u(O、t) ……(4) ここでε-(A+BP)をテーラ展開し、(4)式に代入
すると次式になる。
u (x, t) = ε - (A + BP) u (O, t) ... (4) Here, when ε - (A + BP) is expanded by Taylor and substituted into equation (4), the following equation is obtained. .

u(x、t)=u(o、t)−(A+BP)u(o、t)x+(A+BP)2u(o、t)x/2〓−(A+BP)3u
(o、t)x/3〓+…… また (A+BP)2=A2+(AB+BA)P+B2P2 (A+BP)3=A3+(A2B+ABA+BA2)P+(AB2+BAB+B2A)P2+B3P3 であるから、これを前式に代入すれば、 u(x、t)=u(O、t)−{Au(O、t)+B∂/∂u(O、t)}x +{A2u(O、t)+(AB+BA)∂/∂u(O、t)+B2/∂t2u(O、t)}x/2〓 −{A3u(O、t)+(A2B+ABA+BA2)∂/∂u(O、t) +(AB2+BAB+B2A)∂/∂u(O、t)+B3/∂t3u(O、t)}x/3〓+…… ……(5) となる。
u (x, t) = u (o, t) - (A + BP) u (o, t) x + (A + BP) 2 u (o, t) x 2 /2〓 - (A + BP) 3 u
( o , t ) _ _ _ _ _ _ )P 2 +B 3 P 3 , so by substituting this into the previous equation, u(x, t) = u(O, t) - {Au(O, t) + B∂/∂ t u(O, t)}x + {A 2 u(O, t)+(AB+BA)∂/∂ t u(O, t)+B 22 /∂ t2 u(O, t)}x 2 /2〓 −{A 3 u(O, t) + (A 2 B+ABA+BA 2 ) ∂/∂ t u(O, t) + (AB 2 +BAB+B 2 A) ∂ 2 /∂ t u(O, t)+B 33 /∂ t3 u(O, t)}x 3 /3〓+......(5).

以上により偏微分方程式の解(5)式を得た。また
(5)式よりxの3次項以上は無視でき、通常コンダ
クタンスも無視できるので次式となる。
From the above, we obtained the solution to the partial differential equation (5). Also
From equation (5), the third-order term or higher of x can be ignored, and the normal conductance can also be ignored, so the following equation is obtained.

e(x、t)=e(o、t)−{Ri((o、t)+L(∂/∂i(o、t))}x +1/2{RC(∂/∂e(t))+LC(∂/∂t2e(t))}x2 ……(6) 本発明は距離継電方式に関するものであり、故
障地点では電圧は0であり、電圧の時間偏微分も
0であるという故障条件に基づいているので、(6)
式より、本発明の原理式である次式を得る。
e(x, t)=e(o, t)−{Ri((o, t)+L(∂/∂ t i(o, t))}x +1/2{RC(∂/∂ t e(t ))+LC(∂ 2 /∂ t2 e(t))}x 2 ...(6) The present invention relates to a distance relay method, where the voltage is 0 at the fault point and the time partial differential of the voltage is also 0. Since it is based on the failure condition that (6)
From the equation, the following equation, which is the principle equation of the present invention, is obtained.

以上、本発明の原理式である(7)式を得る過程を
示してきた。
The process of obtaining equation (7), which is the principle equation of the present invention, has been described above.

一方、従来の交流理論では、(1)式を積分する際
に時間tを周波数ωに置き換える積分の一手法を
用いている。
On the other hand, the conventional AC theory uses an integration method in which time t is replaced by frequency ω when integrating equation (1).

このような従来の交流理論における従来の距離
リレーのブロツク図を第2図に示す。この従来の
距離リレーは時間に関して得られるリレー設置点
の電圧e(t)、電流i(t)を入力し、これを
周波数変換回路21で単一周波数の量E〓(ω)、
I〓(ω)にフーリエ変換し、次の判定回路22で
様々なリレー原理によつて事故の有無を判定する
ものである。
A block diagram of a conventional distance relay based on such conventional AC theory is shown in FIG. This conventional distance relay inputs the voltage e(t) and current i(t) at the relay installation point obtained with respect to time, and converts these into the single frequency quantity E〓(ω) by the frequency conversion circuit 21.
The signal is Fourier-transformed into I〓(ω), and the next determination circuit 22 determines whether or not there is an accident using various relay principles.

このような交流理論に基づく従来の距離リレー
は周波数変換回路21と判定回路22から構成さ
れ、周波数変換回路21は必要不可欠のものであ
る。このため、電磁形リレーあるいはトランジス
タ形リレーなどのアナログリレーはLCRフイル
タによつて、またデイジタル形コンピユータリレ
ーはデイジタルフイルタによつて、この周波数変
換回路を備えているのである。しかしながら着目
する周波数が基本周波数(例えば50Hz、60Hz)で
あるため、このフイルタの過渡応答時間が1周期
程度あり、判定回路22の処理時間がいくら速く
ても総合的なリレーの動作時間には限界があつた
のである。
A conventional distance relay based on such AC theory is composed of a frequency conversion circuit 21 and a determination circuit 22, and the frequency conversion circuit 21 is indispensable. For this reason, analog relays such as electromagnetic relays or transistor relays are equipped with frequency conversion circuits using LCR filters, and digital computer relays are equipped with digital filters. However, since the frequency of interest is the fundamental frequency (for example, 50 Hz, 60 Hz), the transient response time of this filter is about one cycle, and no matter how fast the processing time of the judgment circuit 22 is, there is a limit to the overall operating time of the relay. It was hot.

本発明は以上述べた交流理論による従来形の距
離リレーの動作時間の限界という欠点を改良する
ために、前述したように時間に基づく新しい原理
を導くことにより、これを応用した高速度で、か
つキヤパシタンスを無視せずに、高精度な、しか
も本質的にデイジタルコンピユータ形リレーに適
した距離継電方式を提供するものである。
In order to improve the drawback of the limited operating time of conventional distance relays based on AC theory, the present invention introduces a new principle based on time as described above, and applies this to high speed and The object of the present invention is to provide a distance relay method that is highly accurate without neglecting capacitance, and is essentially suitable for digital computer type relays.

第3図は本発明による距離継電方式の基本ブロ
ツク図であつて、本発明による距離継電方式は、
電気所に設置された変成器、変流器により計測さ
れた電圧e(t)、電流i(t)を入力し、微分
回路31においてe(t)とその時間偏微分値∂/∂ e(t)、∂/∂t2e(t)、∂/∂t3e(t
);i(t)と その時間偏微分値∂/∂i(t)、∂/∂t2i(
t)を出力 し、判定回路32において様々なリレー原理によ
つて事故の有無を判定し、演算回路33において
故障点までの距離xを算出するものであり、この
演算回路33は必要に応じて省かれる。
FIG. 3 is a basic block diagram of the distance relay method according to the present invention.
The voltage e(t) and current i(t) measured by a transformer and current transformer installed at an electric station are input, and a differentiation circuit 31 calculates e(t) and its time partial differential value ∂/∂ t e (t), ∂ 2 /∂ t2 e(t), ∂ 3 /∂ t3 e(t
); i(t) and its time partial differential value ∂/∂ t i(t), ∂ 2 /∂ t2 i(
t), a determination circuit 32 determines the presence or absence of an accident using various relay principles, and an arithmetic circuit 33 calculates the distance x to the failure point. omitted.

次に距離xを算出する演算回路33について説
明する。
Next, the arithmetic circuit 33 that calculates the distance x will be explained.

(7)式の二つの式を組み合わせることによつて以
下に示す距離xを算出する手法が与えられる。
By combining the two equations (7), the following method of calculating the distance x is given.

(e0i1−e1i0)−L(i −i0i2)x+1/2{RC(e1i1−e2i0)+LC(e2i1−e3i0)}x2=0 ……(8) (e1i1−e0i2)−R(i1 2−i0i2)X+1/2{RC(e2i1−e1i2)+LC(e3i1−e2i2)}X2=0 ……(9) ただし、 e0=e(o、t)=e(t) i0=i(o、t)=
i(t) eo=∂n/∂ne(o、t)=∂n/∂
te(t) io=∂n/∂ni(o、t)=∂n/∂ni(t
) n=1、 2、3 ここで次のような置換をする。
(e 0 i 1 - e 1 i 0 ) - L (i 2 1 - i 0 i 2 ) x + 1/2 {RC (e 1 i 1 - e 2 i 0 ) + LC (e 2 i 1 - e 3 i 0 )}x 2 = 0 ...(8) (e 1 i 1 −e 0 i 2 )−R(i 1 2 −i 0 i 2 )X+1/2 {RC(e 2 i 1 −e 1 i 2 ) +LC(e 3 i 1 −e 2 i 2 )}X 2 = 0 ...(9) However, e 0 = e (o, t) = e (t) i 0 = i (o, t) =
i(t) e o = ∂n/∂ t ne(o, t) = ∂n/∂
t
te(t) i o =∂n/∂ t ni(o, t)=∂n/∂ t ni(t
) n=1, 2, 3 Here, perform the following replacement.

上述の置換により、(8)、(9)式は簡略化され、そ
れぞれ(11)、(12)式となる。
By the above substitution, equations (8) and (9) are simplified to become equations (11) and (12), respectively.

a0−a1x+a2x2=0 ……(11) b0−b1x+b2x2=0 ……(12) さて、現在の距離継電器はインピーダンス平面
上において、横軸を抵抗成分(Rx)、縦軸をリア
クタンス成分(ωLx)としていることは周知で
ある。ここで、〓、(12)式のxの2次項を無視すれ
ば、それぞれ(13)、(14)式が得られる。
a 0 −a 1 x+a 2 x 2 =0 ……(11) b 0 −b 1 x+b 2 x 2 =0 ……(12) Now, in the current distance relay, on the impedance plane, the horizontal axis is the resistance component ( It is well known that the vertical axis represents the reactance component (ωLx). Here, if we ignore the quadratic term of x in equations (12) and (12), equations (13) and (14) are obtained, respectively.

Lx=a/aL ……(13) Rx=b/bR ……(14) さらにi0=Isinωt、e0=Esin(ωt+θ)と
すれば、 ωLx=IEsinθ/I ……(15) Rx=IEcosθ/I ……(16) となる。
Lx= a0 / a1L ...(13) Rx= b0 / b1R ...(14) Furthermore, if i0 =Isinωt and e0 =Esin(ωt+θ), ωLx=IEsinθ/ I2 ... ...(15) Rx=IEcosθ/I 2 ...(16)

以上のように現在の距離継電器は(11)、(12)式にお
いてxの2次項を無視していることがわかる。
As mentioned above, it can be seen that the current distance relay ignores the quadratic term of x in equations (11) and (12).

本発明はxの2次項、つまりキヤパシタンスを
考慮することにより高精度の距離継電方式を提供
するものであり、その原理式である(11)、(12)式を適
用する。また、現在の距離継電器に対応させるた
めに、(10)式の解(xL)をキヤパシタンスを考慮
したリアクタンス成分の距離、(11)式の解(xR
をキヤパシタンスを考慮した抵抗成分の距離とす
る。
The present invention provides a highly accurate distance relay method by considering the quadratic term of x, that is, capacitance, and applies the principle equations (11) and (12). In addition, in order to correspond to the current distance relay, the solution (x L ) of equation (10) is changed to the distance of the reactance component considering capacitance, and the solution (x R ) of equation (11) is
Let be the distance of the resistance component considering capacitance.

(11)、(12)式の解はニユートン法などを使い、安定
した次の近似解を得る。
To solve equations (11) and (12), use Newton's method or the like to obtain the following stable approximate solution.

L=a/a+a /a(a −2a
)……(17) xR=b/b+b /b(b −2b
)……(18) (17)、(18)式の右辺第2項がキヤパシタンス
を考慮することによる補正項である。
x L =a 0 /a 1 +a 0 2 a 2 /a 1 (a 1 2 -2a
2
a 0 )...(17) x R =b 0 /b 1 +b 0 2 b 2 /b 1 (b 1 2 -2b
2
b 0 )...(18) The second term on the right side of equations (17) and (18) is a correction term based on consideration of capacitance.

(17)、(18)式を本発明の演算回路33内の演
算式とし、これにより故障点までの距離xを算出
する。
Equations (17) and (18) are used as arithmetic expressions in the arithmetic circuit 33 of the present invention, and the distance x to the failure point is calculated from these.

次に、事故の有無を判定する判定回路32につ
いて説明する。
Next, the determination circuit 32 that determines the presence or absence of an accident will be explained.

(11)、(12)式のa2,b2はそれれぞれa1,b1
比べ小さく、xの2次項は補正項の役割をする。
In equations (11) and (12), a 2 and b 2 are smaller than a 1 and b 1 , respectively, and the quadratic term of x serves as a correction term.

第4図に示す特性を有するリアクタンスリレー
の判定式は(10)式を用いて次の判定式(19)で示さ
れる。
The determination formula for a reactance relay having the characteristics shown in FIG. 4 is expressed by the following determination formula (19) using formula (10).

a0−a1x1+a2x1 2≦0 ……(19) 第5図に示す特性を有する抵抗リレーの判定式
は(11)式を用いて次の判定式(20)で示される。
a 0 −a 1 x 1 + a 2 x 1 2 ≦0 ...(19) The determination formula for a resistance relay having the characteristics shown in Figure 5 is expressed by the following determination formula (20) using formula (11). .

b0−b1x1+b2x1 2≦0 ……(20) ただし、x1は整定値である。 b 0 −b 1 x 1 +b 2 x 1 2 ≦0 (20) However, x 1 is a setting value.

(19)、(20)式を本発明の判定回路32内の判
定式とし、これにより事故の有無を判定する。
Equations (19) and (20) are used as the determination formulas in the determination circuit 32 of the present invention, and the presence or absence of an accident is determined based on these.

最後に微分回路31について説明する。 Finally, the differentiation circuit 31 will be explained.

微分回路31は入力データe(t),i(t)
よりその時間偏微分値i1=∂/∂i(t)、i2=∂
/∂t2i (t)、e1=∂/∂e(t)、e2=∂/∂t2e(
t)、e3=∂/∂t3 e(t)を算出し、これらの時間偏微分値をi0
i(t)、e0=e(t)とともに送出するもので
あり、この微分回路31において、この微分演算
に要する時間幅は系統の基本周波数に依存せず、
比較的短く取ることできるので、この微分回路3
1における過渡応答時間も短くなり、総合リレー
動作時間が大巾に短縮できる。以下に微分回路3
1において、電圧e(t)、電流i(t)の時間
偏微分値を導出する微分演算手法をe(t)、i
(t)の代りに一般にf(t)に関してデイジタ
ル方式で示す。
The differentiating circuit 31 receives input data e(t), i(t)
Therefore, its time partial differential value i 1 = ∂/∂ t i (t), i 2 = ∂ 2
/∂ t2 i (t), e 1 =∂/∂ t e(t), e 2 =∂ 2 /∂ t2 e(
t), e 3 = ∂ 3 /∂ t3 e(t), and calculate these time partial differential values as i 0 =
i(t), e 0 =e(t), and in this differentiation circuit 31, the time width required for this differentiation operation does not depend on the fundamental frequency of the system,
Since it can be relatively short, this differentiator circuit 3
The transient response time in No. 1 is also shortened, and the total relay operation time can be greatly shortened. Below is the differential circuit 3
1, the differential calculation method for deriving the time partial differential values of voltage e(t) and current i(t) is described as e(t), i
Instead of (t), we generally denote f(t) in digital form.

第6図aはサンプリング間隔時間がτsで、サ
ンプリングされた奇数個n(=2m−1;mは自
然数)のデータから(n−1)次曲線で近似する
様を表わしている。
FIG. 6a shows that the sampling interval time is τ s and that an odd number n (=2m−1; m is a natural number) of sampled data is approximated by an (n−1)th order curve.

今、(n−1)次曲線 f(t)=ao-1n-1+ao-2n-2+……+a1t+a0 ……(21) が図中の一点鎖線に示すように時刻−(m−1)
τs,……,−τs,0,τs,……,(m−1)τs
でA-(n-1),……,A-1,A0,A1,……,A(n-1
の値を取るとすると、 A-(n-1)=f(−(m−1)τs : A-1=f(−τs) A0=f(o) A1=f(τs) 〓 A(n-1)=f((m−1)τs) となり、未知数n(=2m−1)個(a0,a1,…
…,ao-1)であり、方程式も(2m−1)個あ
り、a0,a1,……,ao-1を決定することができ
る。
Now, the (n-1)th order curve f(t)=a o-1 t n-1 + a o-2 t n-2 +...+a 1 t+a 0 ...(21) is shown by the dashed line in the figure. So time - (m-1)
τ s , ..., −τ s , 0, τ s , ..., (m-1) τ s
So A -(n-1) , ..., A -1 , A 0 , A 1 , ..., A (n-1
) , then A -(n-1) = f(-(m-1)τ s : A -1 = f(-τ s ) A 0 = f(o) A 1 = f(τ s ) 〓 A (n-1) = f((m-1)τ s ), and there are n (=2m-1) unknowns (a 0 , a 1 ,...
..., ao-1 ), and there are (2m-1) equations, and a0 , a1 , ..., ao-1 can be determined.

時刻t=0におけるf(t)の微分値はd/df (t)|t=0=a1、……、d/dkf(t)|t=0
k 〓ak、……、dn−1/dn−1f(t)|t=0=(
n−1) 〓ao-1である。
The differential value of f(t) at time t=0 is d/d t f (t) | t=0 = a 1 , ..., d k /d t kf(t) | t=0 =
k 〓a k ,..., dn-1/d t n-1f(t) | t=0 =(
n-1) 〓a o-1 .

第6図bは偶数個n(=2m)のサンプリング
データから(n−1)次曲線で近似する様を表わ
しているが、同図aと異なる点は(21)式で表わ
される(n−1)次曲線が図中の一点鎖線に示す
ように時刻−(m−1/2)τs、……、−τ/2、
τ/2、… …、(m−1/2)τsでA-n、……、A-1、A1、… …、Anの値を取ることである。この場合もt=
0における微分値は前述と同様に求まる。
Figure 6b shows the approximation by an (n-1)th order curve from an even number n (= 2m) sampling data, but the difference from Figure 6a is that (n- 1) As shown in the dashed line in the figure, the following curve shows time - (m-1/2)τ s , ..., -τ s /2,
It is to take the values of A -n , ..., A -1 , A 1 , ..., A n at τ s /2, . . . , (m-1/2) τ s . In this case too, t=
The differential value at 0 is found in the same manner as described above.

次に一例として3次曲線近似と4次曲線近似を
示す。
Next, cubic curve approximation and quartic curve approximation will be shown as examples.

3次曲線近似 4示曲線近似 このような演算を、各入力量e(t)、i
(t)に対して施こせばよい。
Cubic curve approximation 4 Indicative curve approximation Such calculations are performed for each input quantity e(t), i
It should be applied to (t).

本発明に必要な微分値はe0=e(o)、i0=i
(o)、e1=∂/∂e(t)|t=0 i1=∂/∂
(t)|t =0 、e2=∂/∂t2e(t)|t=0 i2=∂/∂
i(t)|t =0 、e3=∂/∂t3e(t)|t=0であるから(21)
式 が3次曲線でも良いことになる。
The differential values necessary for the present invention are e 0 = e(o), i 0 = i
(o), e 1 = ∂/∂ t e(t) | t=0 i 1 = ∂/∂ t i
(t) | t =0 , e 2 = ∂ 2 /∂ t2 e(t) | t=0 i 2 =∂ 2 /∂ t
2
i(t) | t =0 , e 3 = ∂ 3 /∂ t3 e(t) | Since t=0 (21)
This means that the equation may be a cubic curve.

このように、微分回路31の過渡時間は微分演
算に要するサンプル数で決まり、4点近似(3次
曲線近似)による手法は4τs、5点近似(4次
曲線近似)による手法は、5τsとなる。τsはサ
ンプリング周波数によつて決まるが、デイジタル
サンプリングに伴う折り返し誤差の軽減と標本化
定理によつてfsは決まる。今、600Hz以上を減衰
させるローパスフイルタを前置して、1200Hzサン
プリングを行つてデイジタル保護を行なう場合、
τs=1/f≒0.833msとなる。よつて本発明方式で は過渡応答時間は高々5τs=4.165msである。
但し、ローパスフイルタの過渡応答時間約1.66m
sが加算される。これに対し、従来の距離リレー
はデイジタルフイルタなどによつて約20ms(但
し、基本周波数が50Hzの場合)の過渡応答時間を
持つ。この設計例から分かるように本発明の距離
リレーは非常に高速度な判定ができる事が判る。
In this way, the transition time of the differentiating circuit 31 is determined by the number of samples required for differential operation, and the method using four points approximation (cubic curve approximation) is 4τ s , and the method using five points approximation (quartic curve approximation) is 5τ s becomes. Although τ s is determined by the sampling frequency, f s is determined by the reduction of aliasing errors associated with digital sampling and the sampling theorem. Now, when performing digital protection by pre-installing a low-pass filter that attenuates frequencies above 600Hz and performing 1200Hz sampling,
τ s =1/f s ≒0.833ms. Therefore, in the method of the present invention, the transient response time is at most 5τ s =4.165 ms.
However, the transient response time of the low-pass filter is approximately 1.66 m.
s is added. In contrast, conventional distance relays have a transient response time of approximately 20 ms (provided the fundamental frequency is 50 Hz) due to digital filters and the like. As can be seen from this design example, the distance relay of the present invention is capable of very high-speed determination.

第7図は本発明を適用した一具体例を示し、特
に前述した3次曲線近似を使用した場合を例にと
り説明する。
FIG. 7 shows a specific example to which the present invention is applied, and in particular, a case will be described using the above-mentioned cubic curve approximation as an example.

アナログ入力量e(t)をローパスフイルタ7
1、サンプルホールド回路72を通してマルチプ
レクサ73に入力し、またアナログ入力量i
(t)をローパスフイルタ74、サンプルホール
ド回路75を通してマルチプレクサ73に入力
し、このマルチプレクサ73の出力をアナログ−
デイジタル変換部76でデイジタル化する。そし
て記憶回路77ではアナログ−デイジタル変換部
76の出力により3τs前の電圧、電流の夫々の
デイジタル値E-2、I-2、2τs前のデイジタル値
E-1、I-1、τs前のデイジタル値E1、I1、現在の
デイジタル値E2、I2を記憶し、微分回路78では
記憶回路77で記憶されたデイジタル値を前記
(22)式に適用してe0、i0、e1、i1、e2、i2、e3
計算により決定し、これらを変換回路79に入力
し、この変換回路79では微分回路78で計算さ
れた微分値などを(10)式に適用して、a0,b0,a1
b1、a1、b1、a2、b2を決定し、演算回路80では
(17)あるいは(18)式で事故点までの距離xを
演算し、判定回路81では(19)あるいは(20)
式の判定式で事故の有無を判定する。
The analog input amount e(t) is passed through the low-pass filter 7.
1. Input to multiplexer 73 through sample hold circuit 72, and analog input amount i
(t) is input to the multiplexer 73 through the low-pass filter 74 and sample hold circuit 75, and the output of this multiplexer 73 is input to the analog
A digital conversion section 76 digitizes the data. Then, in the storage circuit 77, the digital values of the voltage and current from 3τ s ago are stored as E -2 , I -2 , and the digital value from 2τ s ago by the output of the analog-to-digital converter 76 .
E -1 , I -1 , τ s The previous digital values E 1 , I 1 and the current digital values E 2 , I 2 are stored, and the differentiating circuit 78 converts the digital values stored in the storage circuit 77 into the (22 ) equation to determine e 0 , i 0 , e 1 , i 1 , e 2 , i 2 , e 3 by calculation, and input these to the conversion circuit 79 , where the differentiation circuit 78 calculates Applying the calculated differential values to equation (10), a 0 , b 0 , a 1 ,
b 1 , a 1 , b 1 , a 2 , b 2 are determined, the arithmetic circuit 80 calculates the distance x to the accident point using equation (17) or (18), and the determination circuit 81 calculates the distance x from (19) or ( 20)
The presence or absence of an accident is determined using the following formula.

上述した本発明による距離継電方式を用いれ
ば、次のような飛躍的な性能の向上をはかること
ができる。
By using the distance relay method according to the present invention described above, the following dramatic improvements in performance can be achieved.

(1) 従来の如く周波数変換回路(フイルタ)を必
要とせず、このため高速度な事故判定が可能で
ある。
(1) Unlike conventional methods, a frequency conversion circuit (filter) is not required, and therefore high-speed accident determination is possible.

(2) 送電線の分布定数であるキヤパシタンスCを
無視せず考慮したことにより高精度な事故判定
が可能である。
(2) Highly accurate accident determination is possible by considering the capacitance C, which is a distribution constant of the power transmission line, without ignoring it.

(3) 入力波形が歪波でも正確に応動する。(3) Accurate response even if the input waveform is a distorted wave.

(4) 減衰する直流分を含む場合も正確に応動す
る。
(4) Accurate response even when there is an attenuated DC component.

(5) 直流送電系統にも設置でき、この場合事故時
に発生する過渡現象にも正確に応動する。
(5) It can also be installed in DC power transmission systems, in which case it can accurately respond to transient phenomena that occur during accidents.

(6) 複雑な演算を用いるデイジタルフイルタが不
要で、アルゴリズムが簡略となる。
(6) There is no need for a digital filter that requires complex calculations, and the algorithm is simplified.

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

第1図は分布定数線路の等価回路図、第2図は
従来の距離リレーの基本ブロツク図、第3図は本
発明による距離継電方式の基本ブロツク図、第4
図はリアクタンスリレーの特性図、第5図は抵抗
リレーの特性図、第6図aおよびbは夫々サンプ
リング数が奇数の場合および偶数の場合における
微分演算を説明するための図、第7図は本発明を
適用した一具体例を示すブロツク図であつて、図
中31は微分回路、32は判定回路、33は演算
回路、71,74はローパスフイルタ、72,7
5はサンプルホールド回路、73はマルチプレク
サ、76はアナログ−デイジタル変換部、77は
記憶回路、78は微分回路、79は変換回路、8
0は演算回路、81は判定回路、Lはインダクタ
ンス、Rは抵抗、Cはキヤパシタンス、xは故障
点までの距離、e(t)は電圧、i(t)は電流
を示す。
Figure 1 is an equivalent circuit diagram of a distributed constant line, Figure 2 is a basic block diagram of a conventional distance relay, Figure 3 is a basic block diagram of a distance relay system according to the present invention, and Figure 4 is a basic block diagram of a distance relay system according to the present invention.
Figure 5 is a characteristic diagram of a reactance relay, Figure 5 is a characteristic diagram of a resistance relay, Figures 6a and b are diagrams for explaining differential operations when the number of samples is odd and even, respectively. This is a block diagram showing a specific example to which the present invention is applied, in which 31 is a differentiation circuit, 32 is a determination circuit, 33 is an arithmetic circuit, 71 and 74 are low-pass filters, and 72, 7
5 is a sample hold circuit, 73 is a multiplexer, 76 is an analog-digital converter, 77 is a storage circuit, 78 is a differentiation circuit, 79 is a conversion circuit, 8
0 is an arithmetic circuit, 81 is a determination circuit, L is an inductance, R is a resistance, C is a capacitance, x is a distance to a failure point, e(t) is a voltage, and i(t) is a current.

Claims (1)

【特許請求の範囲】 1 電力系統の被保護送電線より得られたアナロ
グ量をアナログ−デイジタル変換部にてデイジタ
ル量に変換し、時間tに関して得られる電圧e
(t)、電流i(t)のデイジタル値を微分するた
めの微分回路を備え、この微分回路にて前記電圧
e(t)、電流i(t)よりその時間偏微分値を
導出し、演算回路にて電圧e(t)と電流i
(t)とその導出された時間偏微分値と送電線の
単位長当りの分布定数であるインダクタンスL、
抵抗R、キヤパシタンスCから次の(1)、(2)式、即
ち e(t)−{Ri(t)+L(∂/∂i(t))}x+1/2{RC(∂/∂e(t)) +LC(∂/∂t2e(t))}x2=0 ……(1) ∂/∂e(t)−{R(∂/∂i(t))+L(∂/∂t2i(t))}x+1/2{RC(∂/∂t2e(
t)) +LC(∂/∂t3e(t))}x2=0 ……(2) を用いて、故障点までの距離xの算出若しくは距
離xの存在する範囲を規定するようにしたことを
特徴とする距離継電方式。 2 (1)式と(2)式を組み合せて得られる次の(3)式、
(4)式、即ち {e(t)(∂/∂i(t))−(∂/∂e(t))i(t)}−L{(∂/∂i(t))−i(t) (∂/∂t2i(t))}x+1/2〔RC{(∂/∂e(t))(∂/∂i(t))−(∂/∂t2e(
t))i(t)} +LC{(∂/∂t2e(t))(∂/∂i(t))−(∂/∂t3e(t))i(t)}〕x2=0 ……(3) {(∂/∂e(t))(∂/∂i(t))−e(t)(∂/∂t2i(t))}−R{(∂/∂i(t))
−i(t) (∂/∂t2i(t)}x+1/2〔RC{(∂/∂t2e(t))(∂/∂i(t)) −(∂/∂e(t))(∂/∂t2i(t))}+LC{(∂/∂t3e(t))(∂/∂i(t)) −(∂/∂t2e(t))(∂/∂t2i(t))}〕x2=0 ……(4) を用いて、故障点までの距離xを算出することお
よび距離xの存在する範囲を規定するようにした
ことを特徴とする特許請求の範囲第1項記載の距
離継電方式。 3 電圧e(t)、電流i(t)の時間偏微分値
を導出する際、等間隔でサンプリングされたn個
のデイジタル信号f1,f2,……,foより次の(5)
式、即ち ここで、 d/dtf(t)|t=0:時刻t=0における第k
次時 間偏微分値 bk,CkJ:定数 k=0,1,……,n−1 によつて、f(t)の時間偏微分値を求めること
を利用したことを特徴とする特許請求の範囲第1
項又は第2項記載の距離継電方式。
[Claims] 1. An analog quantity obtained from a protected power transmission line of a power system is converted into a digital quantity by an analog-digital converter, and the voltage e obtained with respect to time t is
(t), and a differentiation circuit for differentiating the digital values of current i(t), and this differentiation circuit derives the time partial differential value from the voltage e(t) and current i(t), and calculates In the circuit, voltage e(t) and current i
(t), its derived time partial differential value, and the inductance L, which is the distribution constant per unit length of the power transmission line,
From the resistance R and capacitance C, the following equations (1) and (2) are obtained: e(t)−{Ri(t)+L(∂/∂ t i(t))}x+1/2{RC(∂/∂ t e(t)) +LC(∂ 2 /∂ t2 e(t))}x 2 =0 ...(1) ∂/∂ t e(t)−{R(∂/∂ t i(t))+L( ∂ 2 /∂ t2 i(t))}x+1/2{RC(∂ 2 /∂ t2 e(
t)) +LC(∂ 3 /∂ t3 e(t))}x 2 =0 ...(2) is used to calculate the distance x to the failure point or define the range in which the distance x exists. Distance relay method characterized by: 2 The following equation (3) obtained by combining equations (1) and (2),
Equation (4), that is, {e(t)(∂/∂ t i(t))−(∂/∂ t e(t))i(t)}−L{(∂/∂ t i(t)) 2 −i(t) (∂ 2 /∂ t2 i(t))}x+1/2[RC{(∂/∂ te (t))(∂/∂ t i(t))−(∂ 2 /∂ t2 e(
t))i(t)} +LC{(∂ 2 /∂ t2 e(t))(∂/∂ t i(t))−(∂ 3 /∂ t3 e(t))i(t)}]x 2 = 0 ...(3) {(∂/∂ t e(t))(∂/∂ t i(t))-e(t)(∂ 2 /∂ t2 i(t))}-R{( ∂/∂ t i(t))
2 −i(t) (∂ 2 /∂ t2 i(t)}x+1/2[RC{(∂ 2 /∂ t2 e(t))(∂/∂ t i(t)) −(∂/∂ t e(t))(∂ 2 /∂ t2 i(t))}+LC{(∂ 3 /∂ t3 e(t))(∂/∂ t i(t)) −(∂ 2 /∂ t2 e(t )) (∂ 2 /∂ t2 i(t))}] x 2 = 0...Using (4), calculate the distance x to the failure point and define the range in which the distance x exists. 3. When deriving the time partial differential values of voltage e(t) and current i(t), n values sampled at equal intervals are used. From the digital signals f 1 , f 2 , ..., f o , the following (5)
formula, i.e. Here, d k /dt k f(t) | t=0 : k-th at time t=0
A patent claim characterized in that the time partial differential value of f(t) is determined using the following time partial differential values b k , C kJ : constant k=0, 1, ..., n-1. range 1
Distance relay method described in Section 2 or Section 2.
JP574279A 1979-01-20 1979-01-20 Distance relay system Granted JPS5597127A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP574279A JPS5597127A (en) 1979-01-20 1979-01-20 Distance relay system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP574279A JPS5597127A (en) 1979-01-20 1979-01-20 Distance relay system

Publications (2)

Publication Number Publication Date
JPS5597127A JPS5597127A (en) 1980-07-24
JPS6217452B2 true JPS6217452B2 (en) 1987-04-17

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ID=11619545

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Application Number Title Priority Date Filing Date
JP574279A Granted JPS5597127A (en) 1979-01-20 1979-01-20 Distance relay system

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JP (1) JPS5597127A (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
DE2264064A1 (en) * 1972-12-29 1974-07-04 Siemens Ag DISTANCE PROTECTION DEVICE

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JPS5597127A (en) 1980-07-24

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