JPH0452695B2 - - Google Patents

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Publication number
JPH0452695B2
JPH0452695B2 JP2034383A JP2034383A JPH0452695B2 JP H0452695 B2 JPH0452695 B2 JP H0452695B2 JP 2034383 A JP2034383 A JP 2034383A JP 2034383 A JP2034383 A JP 2034383A JP H0452695 B2 JPH0452695 B2 JP H0452695B2
Authority
JP
Japan
Prior art keywords
line
ground fault
phase
current
zero
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
JP2034383A
Other languages
Japanese (ja)
Other versions
JPS59149721A (en
Inventor
Junichi Inagaki
Fumio Ando
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.)
Toshiba Corp
Original Assignee
Tokyo Shibaura Electric Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Tokyo Shibaura Electric Co Ltd filed Critical Tokyo Shibaura Electric Co Ltd
Priority to JP2034383A priority Critical patent/JPS59149721A/en
Publication of JPS59149721A publication Critical patent/JPS59149721A/en
Publication of JPH0452695B2 publication Critical patent/JPH0452695B2/ja
Granted legal-status Critical Current

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Description

【発明の詳細な説明】 〔発明の技術分野〕 本発明は、地絡回線選択継電器、特に併架多回
線の1相地絡保護に用いられる地絡回線選択継電
器に関するものである。
DETAILED DESCRIPTION OF THE INVENTION [Technical Field of the Invention] The present invention relates to a ground fault line selection relay, and more particularly to a ground fault line selection relay used for one-phase ground fault protection of multiple parallel lines.

〔発明の技術的背景〕[Technical background of the invention]

高抵抗接地系の平行2回線送電線(以下被保護
送電線と云う)が他の送電線(以下起誘導送電線
と云う)と同一鉄塔に併架されている場合には、
起誘導送電線の電流による誘導のために被保護送
電線の2回線間を循環する零相電流が流れる。一
般の地絡回線選択継電器は被保護平行送電線の零
相差電流を演算電流として地絡事故回線を識別す
るものであるが、前記の循環零相電流が大きい場
合には、この影響のために正常な保護が不可能と
なる。
When a high-resistance grounded parallel two-circuit transmission line (hereinafter referred to as a protected transmission line) is installed on the same tower as another power transmission line (hereinafter referred to as an induced transmission line),
A zero-sequence current circulates between the two circuits of the protected power transmission line due to induction by the current in the power transmission line. A general ground fault line selection relay uses the zero-sequence difference current of the protected parallel transmission line as a calculation current to identify a ground-fault fault line, but when the above-mentioned circulating zero-sequence current is large, it Normal protection becomes impossible.

この対策として、1相地絡事故時における健
全相の循環電流から誘導による循環零相電流を求
め、この求められた循環零相電流により平行送電
線の零相差電流を補償した電流を演算電流とする
方法(方法1)及び、特開昭58−46832号で開
示されているように、事故相差電流(又は事故相
差電流を含む同一相差電流の合成電流)から得た
検出電流の事故変化分を同一相差電流(又は同一
相差電流の合成電流)から得た補償電流の事故変
化分によつて補償した電流を演算電流とする方法
(方法2)等を用いた補償形地絡回線選択継電器
が既に提案されている。これによつて循環零相電
流がある場合であつても1相地絡事故の保護が可
能となつた。
As a countermeasure to this, the circulating zero-sequence current due to induction is determined from the circulating current of the healthy phase at the time of a single-phase ground fault, and the current obtained by compensating the zero-sequence difference current of the parallel transmission line with this determined circulating zero-sequence current is used as the calculated current. As disclosed in JP-A No. 58-46832, the fault change in the detected current obtained from the fault phase difference current (or the composite current of the same phase difference current including the fault phase difference current) is Compensated ground fault line selection relays using a method (Method 2) in which the current compensated by the fault change in the compensation current obtained from the same phase difference current (or a composite current of the same phase difference current) are already available. Proposed. This makes it possible to protect against single-phase ground faults even when there is a circulating zero-sequence current.

第1図は従来技術及び本発明に共通して用いら
れる一般的なデイジタル保護継電装置の構成例を
示す図である。図において1は母線であつてa,
b,cは各相を示す。2及び3は平行送電線、4
及び5はしや断器、6及び7は変流器、8は計器
用変圧器、9は入力変換器、10はサンプルホー
ルド回路、11はマルチプレクサ、12はA/D
変換器である。13はデイジタル計算機であり内
部にCPU、メモリM、入力回路I、出力回路O
を有している。変流器6及び7により送電線2及
び3の電流に対応した電流を得、図示の接続によ
り両送電線のa,b,c各相の差電流ias,ibs
びicsと、3×(零相差電流)=3ipsが得られる。又、
計器用変圧器8により母線を通じて送電線2及び
3の端子のa,b,c各相電圧及び零相電圧に対
応した電圧va,vb,vc及びvpが得られる。これら
の電流、電圧は入力変換器9に加えられ、次のサ
ンプルホールド回路10に適した値の電圧に変換
される。入力変換器9にはフイルタが内蔵されて
おり、各電圧、電流の基本波分のみが出力として
得られる。サンプルホールド回路10では同一時
刻に一定周期(例えば電圧、電流の1周期の1/12
の周期)で入力値をサンプルしホールドする。こ
のホールド値はマルチプレクサ11により遂次
A/D変換器12に供給されてデイジタル値に変
換される。このデイジタル値によりデイジタル計
算機13が所要の演算を行ない、所定条件のとき
しや断器4又は5のしや断を指令する。
FIG. 1 is a diagram showing a configuration example of a general digital protective relay device commonly used in the prior art and the present invention. In the figure, 1 is the bus line a,
b and c indicate each phase. 2 and 3 are parallel transmission lines, 4
and 5 is a bridge and disconnector, 6 and 7 are current transformers, 8 is an instrument transformer, 9 is an input converter, 10 is a sample and hold circuit, 11 is a multiplexer, and 12 is an A/D
It is a converter. 13 is a digital computer, which includes a CPU, memory M, input circuit I, and output circuit O.
have. The current transformers 6 and 7 obtain currents corresponding to the currents in the transmission lines 2 and 3, and by the connections shown in the diagram, the difference currents i as , i bs and i cs of each phase of both transmission lines, i as , i bs and i cs , 3 × (zero-sequence difference current) = 3i ps is obtained. or,
Voltages v a , v b , v c and v p corresponding to the a, b , c phase voltages and zero-phase voltage of the terminals of the power transmission lines 2 and 3 are obtained by the instrument transformer 8 through the bus bar. These currents and voltages are applied to the input converter 9 and converted into voltages with values suitable for the next sample-and-hold circuit 10. The input converter 9 has a built-in filter, and only the fundamental waves of each voltage and current can be obtained as output. The sample and hold circuit 10 performs a constant cycle (for example, 1/12 of one cycle of voltage or current) at the same time.
The input value is sampled and held at the cycle of This hold value is sequentially supplied to the A/D converter 12 by the multiplexer 11 and converted into a digital value. Based on this digital value, the digital computer 13 performs necessary calculations and instructs the disconnector 4 or 5 to disconnect when a predetermined condition is met.

第2図はデイジタル計算機13が行なう演算フ
ローの一例を示し、前記した従来方法1を用いた
場合が示される。先ずステツプS1で開始指令を受
けると次のステツプS2において1相地絡事故検出
を行なう。前記ステツプS2において1相地絡事故
が検出されるとステツプS3に進み地絡相選別演算
を行なう。ステツプS3ではS3-1,S3-2,S3-3の順
に各々a,b及びc相地絡検出演算を行ない、
a,b又はc相地絡が各々検出されると、各々判
定3Ya,3Yb又は3Ycが得られ、又、ステツプS3
において地絡相が検出されなければ判定3Nが得
られて他の演算へ移る。
FIG. 2 shows an example of the calculation flow performed by the digital computer 13, and shows the case where the conventional method 1 described above is used. First, when a start command is received in step S1 , one-phase ground fault detection is performed in the next step S2 . If a one-phase ground fault is detected in step S2 , the process proceeds to step S3 , where a ground fault phase selection calculation is performed. In step S3 , a, b, and c phase ground fault detection calculations are performed in the order of S3-1 , S3-2 , and S3-3 , respectively.
When a, b, or c phase ground fault is detected, respectively, judgment 3Y a , 3Y b , or 3Y c is obtained, and step S 3
If no ground fault phase is detected in , the determination 3N is obtained and the process moves on to other calculations.

ステツプS3において判定3Ya,3Yb又は3Yc
いずれかが得られたときは、前記各判定のうちの
どの判定が得られたか、即ち、地絡相がいずれの
相であるかに応じ、ステツプS4において演算電流
iea,ieb又はiecと極性量epa,epb又はepcを求める。
これが求められるとステツプS5において回線選択
演算を行なう。ステツプS5ではステツプS5-1
S5-2の順に送電線2及び3の事故検出演算を行な
い、前記どちらかの事故が検出されれば各各判定
5Y1又は5Y2が得られて、事故送電線に対応した
しや断器4又は5をしや断する。いずれの送電線
の事故も検出されなければ判定5Nが得られて他
の演算に移る。
When any of the judgments 3Y a , 3Y b , or 3Y c is obtained in step S 3 , it depends on which judgment among the above judgments was obtained, that is, which phase is the ground fault phase. , the calculated current in step S4
Find i ea , i eb or i ec and the polarity e pa , e pb or e pc .
Once this is determined, a line selection calculation is performed in step S5 . In step S 5 , step S 5-1 ,
S Perform accident detection calculations for transmission lines 2 and 3 in the order of 5-2 , and if either of the above accidents is detected, each judgment will be made.
5Y 1 or 5Y 2 is obtained, and the disconnector 4 or 5 corresponding to the faulty power transmission line is disconnected. If no transmission line fault is detected, a determination of 5N is obtained and the process moves on to other calculations.

前記したステツプS2の1相地絡検出演算として
は、例えば零相電圧vpが一定値以上で且つ各相間
電圧va−vb,vb−vc及びvc−vaがいずれも一定値
以上のとき1相地絡事故と判断するものがあり、
ステツプS3の地絡相選別演算としては、例えば零
相電圧vpが各相間電圧vb−vc,vc−va及びva−vb
に対して一定位相範囲内にあるとき、夫々a,b
又はc相地絡と判断するもの、更にステツプS5
回線選択演算としては、例えば演算電流ieの極性
量epに対する有効成分が正の一定値以上のとき送
電線2の事故を検出し、負の一定値以下のとき送
電線3の事故を検出するもの等があり、これらは
いずれも公知である。なお、iea,ieb,iec,epa
epb及びepcのうち求められたものを各々ie,ipで示
す。
The above-mentioned one-phase ground fault detection calculation in step S2 is carried out when, for example, the zero-phase voltage v p is equal to or higher than a certain value, and the inter-phase voltages v a − v b , v b − v c , and v c − v a are all When the value exceeds a certain value, it is determined that a one-phase ground fault has occurred.
In the ground fault phase selection calculation in step S3 , for example, the zero-sequence voltage v p is changed to the inter-phase voltages v b −v c , v c −v a and v a −v b
a, b, respectively, within a certain phase range.
In addition, in the line selection calculation in step S5 , for example, a fault in the power transmission line 2 is detected when the active component of the calculated current i e with respect to the polarity e p is greater than a positive certain value. , which detects an accident on the power transmission line 3 when the value is below a certain negative value, and all of these are well known. In addition, i ea , i eb , i ec , e pa ,
The determined values of e pb and e pc are indicated by i e and i p, respectively.

ステツプS4の演算電流ie及び極性量epとしては
種々のものが提案されている。即ち、極性量ep
しては零相電圧の符号を変えた電圧−vpのほか、 epa=(vb−vc)∠90° epb=(vc−va)∠90° epc=(va−vb)∠90° 等種々のものが提案されている。又、演算電流ie
はいずれも検出電流idを補償電流ihで補償した電
流であつて次式で表わされる。
Various values have been proposed for the calculation current i e and the polarity e p in step S4 . That is, as the polarity e p , in addition to the voltage −v p with the sign of the zero-sequence voltage changed, e pa = (v b − v c )∠90° e pb = (v c − v a )∠90° e Various values have been proposed, such as pc = (v a − v b )∠90°. Also, the calculation current i e
Both are currents obtained by compensating the detection current i d with the compensation current i h , and are expressed by the following equation.

ie=id−ih ……(1) これらのうちで最も一般的なものは、検出電流id
を零相差電流ipsとし、補償電流ih健全相中の1相
の差電流とするもので、演算電流ieが次式で表わ
され、又、極性量はepa,epb及びepcとも零相電圧
−vpとするものである。
i e = i d − i h ...(1) The most common of these is the detection current i d
The zero-sequence difference current i ps is the zero-sequence difference current, and the compensation current i h is the difference current of one phase in the healthy phase.The calculated current i e is expressed by the following formula, and the polarity is e pa , e pb , and e Both pc and zero-sequence voltage are set to −v p .

iea=ips−K1bibs ……(2) ieb=ips−K1cics ……(3) iec=ips−K1aias ……(4) 但しK1a,K1b及びK1cは定数 上記した(2)〜(4)式より常時の循環零相電流を補
償した事故時の零相差電流を求めることができる
ことは特開昭58−46834号で開示した通りである。
即ち、多回線併架送電線において、被保護送電線
の各相及び零相の循環電流の関係比は被保護送電
線の運転状態によらずほぼ一定になる原理による
ものである。
i ea = i ps −K 1b i bs …(2) i eb = i ps −K 1c i cs …(3) i ec = i ps −K 1a i as …(4) However, K 1a , K 1b and K 1c are constants. As disclosed in JP-A No. 58-46834, the zero-sequence difference current at the time of a fault can be calculated by compensating for the normal circulating zero-sequence current from equations (2) to (4) above. be.
That is, in a multicircuit parallel power transmission line, the relative ratio of the circulating currents of each phase and zero phase of the protected power transmission line is based on the principle that it is almost constant regardless of the operating state of the protected power transmission line.

上記した原理にもとづき、(1)式にて示す方式に
て演算電流ieを求める他の例が提案されている。
これらの代表例を以下に示す。
Based on the above-mentioned principle, another example of calculating the calculation current i e using the method shown in equation (1) has been proposed.
Representative examples of these are shown below.

iea=ips−K1bibs ……(5)((2)式に同じ) ieb=ips−K1ca(ips+ias) ……(6) iec=ips−K1bibs ……(7) 但しK1caは定数 即ち、(5),(6),(7)式のものは補償電流として健
全相差電流のみを用いて演算するものである。更
に次式で示されるものもある。
i ea = i ps −K 1b i bs ...(5) (same as equation (2)) i eb = i ps −K 1ca (i ps + i as ) ...(6) i ec = i ps −K 1b i bs ... (7) However, K 1ca is a constant, that is, the equations (5), (6), and (7) are calculated using only the healthy phase difference current as the compensation current. Furthermore, there are also those expressed by the following formula.

iea=(ics+ias)−K2bibs ……(8) ieb=ibs−K2ca(ics+ias) ……(9) iec=(ics+ias)−K2bibs ……(10) ((7)式に同じ) (8),(9),(10)式のものは被保護送電線の配列にお
いて、a相を上相、b相を中相、c相を下相とす
るとき、上相(a相)と下相(c相)の地絡事故
の場合は検出電流idに上相(a相)と下相(c
相)の差電流の和を用い、補償電流ihに中相(b
相)差電流を用いている。又、中相(b相)の地
絡事故の場合は検出電流idに中相(b相)差電流
を用い、補償電流ihに上相(a相)と下相(c
相)の和を用いたものである。この例の場合、起
誘導回線が上下にあつても誤差を小さくすること
ができるものであり、これは交流回路に流れる事
故電流が事故相のみに流れることによる。
i ea = (i cs + i as ) − K 2b i bs ……(8) i eb = i bs −K 2ca (i cs + i as )……(9) i ec = (i cs + i as )−K 2b i bs ...(10) (same as equation (7)) In equations (8), (9), and (10), in the arrangement of protected transmission lines, phase a is the upper phase, phase b is the middle phase, When the c phase is the lower phase, in the case of a ground fault between the upper phase (a phase) and the lower phase (c phase), the detection current i d has the upper phase (a phase) and the lower phase (c
Using the sum of the difference currents of the middle phase (b
phase) difference current is used. In addition, in the case of a ground fault in the middle phase (phase b), the middle phase (phase b) difference current is used as the detection current i d , and the upper phase (phase a ) and lower phase (c
It uses the sum of the phases). In this example, the error can be reduced even if the induction lines are located above and below, and this is because the fault current flowing in the AC circuit flows only in the fault phase.

更に特開昭58−46832号では次の内容が開示さ
れている。
Further, JP-A-58-46832 discloses the following content.

iea=3ia2s−3K3ips ……(11) ieb=3ia2s−3aK3ips ……(12) iec=3ia2s−3a2K3ips ……(13) 但しia2sはa相差電流の逆相分 aはベクトルを120°進めるパラメータ K3常数 上記した(11)〜(13)式は事故相の対称分に関し
てa相の例を示し、 ia2s=ips=1/3iasの関係があることから、 iea=3(1−K3)ips ……(11)′ ieb=3(1−aK3)ips ……(12)′ iec=3(1−a2K3)ips ……(13)′ となり、零相事故分差電流を求めることができ
る。
i ea =3i a2s −3K 3 i ps ……(11) i eb =3i a2s −3aK 3 i ps ……(12) i ec =3i a2s −3a 2 K 3 i ps ……(13) However, i a2s is the negative phase component of the a phase difference current a is the parameter that advances the vector by 120° K 3 constant Equations (11) to (13) above show an example of the a phase regarding the symmetrical component of the fault phase, i a2s = i ps = 1 Since there is a relationship of /3i as , i ea = 3 (1-K 3 ) i ps ...(11)' i eb = 3 (1-aK 3 ) i ps ...(12)' i ec = 3 (1−a 2 K 3 ) i ps ……(13)′, and the zero-sequence fault difference current can be obtained.

以上に説明した(1)式で示される種々の例におい
て、補償電流ihの係数は固定(予め設定)のもの
を挙げているが、例えば特開昭55−106028号で開
示されているように、健全時の回線間循環電流の
間に一定の比率関係のあることを用いて常時演算
して求める方法もある。
In the various examples shown by equation (1) explained above, the coefficients of the compensation current i h are fixed (preset), but for example, as disclosed in Japanese Patent Application Laid-Open No. 106028/1982, Alternatively, there is a method of constantly calculating based on the fact that there is a certain ratio relationship between the circulating currents between lines when they are healthy.

上記従来技術の例としては第2図で示した処理
による方法1について説明してきたが、方法2の
場合は、演算電流が(1)式とは異なり、 i′e=(id−idM)−(ih−ihM) ……(14) とするものである。ここでid,idMは夫々事故相差
電流(又は事故相差電流を含む同一相差電流の合
成電流)の事故後及び事故前電流、ih,ihMは夫々
同一相差電流(又は同一相差電流の合成電流)の
事故後及び事故前の電流である。なおidとih,idM
とihMについて方法1で述べた種々の方法により、
検出電流と補償電流を夫々事故前及び事故後に求
めればよい。そして演算フローは第2図を変形
し、ステツプS2にて1相地絡検出でないとき(1)式
の値を記憶し、ステツプS4の処理の代りに、事故
後の(1)式の算出及び(14)式の値の算出を行なうよ
うにすればよい。(14)式は(1)式と比べたとき、補
償電流ihによる補償誤差を(idM−ihM)の演算に
よる補償誤差を差し引くこととなり、より誤差を
抑えることができる。
As an example of the above-mentioned conventional technology, method 1 using the processing shown in FIG . ) − (i h −i hM ) ...(14). Here, i d and i dM are the post-fault and pre-fault currents of the fault phase difference current (or the composite current of the same phase difference current including the fault phase difference current), respectively, and i h and i hM are the same phase difference current (or the composite current of the same phase difference current including the fault phase difference current), respectively. The composite current is the current after the accident and before the accident. Note that i d and i h , i dM
By using the various methods described in Method 1 for and i hM ,
The detection current and the compensation current may be obtained before and after the accident, respectively. Then, the calculation flow is modified from Fig. 2, and when a one-phase ground fault is not detected in step S2 , the value of equation (1) is memorized, and instead of the processing in step S4 , the value of equation (1) after the accident is What is necessary is to perform the calculation and the value of equation (14). When formula (14) is compared with formula (1), the compensation error due to the compensation current i h is subtracted from the compensation error due to the calculation of (i dM −i hM ), and the error can be further suppressed.

〔背景技術の問題点〕[Problems with background technology]

上記詳細に述べたことからわかるように、補償
形地絡回線選択継電器の動作判定においては、少
なくとも1相の各相差電流を入力し、この各相差
電流から(1)式における検出電流idと補償電流ih
うちの少なくとも一方を算出する必要がある。こ
のような従来技術の欠点を以下に説明する。
As can be seen from the above detailed description, in determining the operation of the compensated ground fault line selection relay, the phase difference current of at least one phase is input, and the detected current i d in equation (1) is calculated from this phase difference current. It is necessary to calculate at least one of the compensation currents i and h . The drawbacks of such prior art will be explained below.

第3図a,bは被保護送電線2,3における事
故前及び事故後の系統状態を示す図である。第3
図aにおいて、送電線2,3は母線1A,1Bに接
続されると共に抵抗R1によつて接地され、又、
負荷Lを有している。又、送電線2,3は充電容
量C1を有する。RY1はB端に設置されて送電線
2,3の地絡回線選択保護を行なう継電器であ
り、変流器6,7により送電線2,3の差電流に
対応した電流を入力し動作判定を行なう。この入
力電流として少なくとも各相差電流を用いる。こ
の系統構成のもとで、常時、送電線2,3には
夫々負荷電流IL1,IL2が各相に流れ、更に循環電
流Ithが図の向きにあるものとする。
FIGS. 3a and 3b are diagrams showing the system states of the protected power transmission lines 2 and 3 before and after the accident. Third
In figure a, power transmission lines 2 and 3 are connected to bus bars 1A and 1B and grounded by a resistor R1 , and
It has a load L. Moreover, the power transmission lines 2 and 3 have charging capacity C 1 . RY1 is a relay that is installed at the B end and performs ground fault line selection protection for the power transmission lines 2 and 3.It inputs a current corresponding to the difference current between the power transmission lines 2 and 3 using current transformers 6 and 7, and judges the operation. Let's do it. At least each phase difference current is used as this input current. Under this system configuration, it is assumed that load currents I L1 and I L2 always flow in each phase of the power transmission lines 2 and 3, respectively, and that a circulating current I th is in the direction shown in the figure.

第3図aにおいてはRY−1の各相差電流及び
零相差電流の入力の大きさは、ほぼ夫々の循環電
流の2倍である。この状態では、従来の補償形地
絡選択方式を採用しても、RY−1は正常な応動
を行なうことができる。
In FIG. 3a, the input magnitude of each phase difference current and zero-sequence difference current of RY-1 is approximately twice the respective circulating current. In this state, even if the conventional compensated ground fault selection method is employed, RY-1 can respond normally.

第3図bはA端近傍F点の100%1線地絡事故
により、A端設置の補償形地絡回線選択継電器
(図示せず)により、しや断器CB1が先行しや断
した状態を示す。このときCB1の「開」により循
環電流は消滅し、送電線2における各相電流は次
のようになる。
Figure 3b shows a state in which the 100% single-line ground fault at point F near end A caused the ground breaker CB1 to break in advance due to the compensated ground fault line selection relay (not shown) installed at end A. shows. At this time, the circulating current disappears due to the "opening" of CB1, and each phase current in the power transmission line 2 becomes as follows.

健全相2相の電流=IL1+IL2 ……(15) 事故相の電流=IL1+IL2+IF ……(16) 上記(16)式におけるIFは事故電流であり、抵抗
器電流INGRと充電々流ICの大きさによつて決まる
ものである。一般にはICはINGRより大きくなるこ
とがなく、90°の位相差があると考えればよいの
で、IFの大きさの最大値は下記となる。
Current in two healthy phases = I L1 + I L2 ……(15) Current in fault phase = I L1 + I L2 + I F ……(16) I F in equation (16) above is the fault current, and resistor current I It is determined by the size of NGR and charging current I C. In general, I C is never larger than I NGR , and it can be considered that there is a phase difference of 90°, so the maximum value of I F is as follows.

IF=√2×INGR ……(17) したがつて(16)式は下記となる。 I F =√2×I NGR ……(17) Therefore, equation (16) becomes as follows.

事故相の電流=IL1+IL2+√2INGR ……(18) しかし、一般に系統の運転状態を考えるとき、
負荷電流IL1とIL2の和の大きさは、CT定格×150
%まで考え、INGRの大きさは数百Aである。今、
C T定格を1200/5、INGRを400Aとするとき、(1
5),(17)式の値は下記となる。
Fault phase current = I L1 + I L2 + √2 I NGR ...(18) However, when considering the operating status of the system,
The sum of the load currents I L1 and I L2 is CT rating x 150
%, the size of I NGR is several hundred A. now,
When the CT rating is 1200/5 and the I NGR is 400A, (1
5), the values of equations (17) are as follows.

健全相2相の電流=1.2kA×1.5=1.8kA
……(19) IOF=√2×400A≒560A ……(20) したがつて第3図bのRY1の入力電気量の最
大値は差回路電流であることから、 健全相差電流=1.8kA ……(21) 事故相差電流=I1L+I2L+2IF =1.8kA+2×560A ≒3.0kA ……(22) 零相差電流=2×IF/3≒1.1/3kA ……(23) となる。したがつてRY1はこれらの入力の大き
さに対しても正しく応動しなければならない。
Healthy phase 2 phase current = 1.2kA x 1.5 = 1.8kA
...(19) I OF =√2×400A≒560A ...(20) Therefore, since the maximum value of the input electricity of RY1 in Figure 3b is the difference circuit current, healthy phase difference current = 1.8kA ...(21) Fault phase difference current = I 1L + I 2L + 2I F = 1.8kA + 2 × 560A ≒ 3.0kA ... (22) Zero-sequence difference current = 2 × I F /3 ≈ 1.1/3kA ... (23) Therefore, RY1 must also respond correctly to the magnitude of these inputs.

一方、デジタル計算機でRY1を構成するとき、
入力に対して正しく応動するためには、第1図の
AD変換器12におけるアナログ/デジタル変換
にて入力に正確に比例した大きさに変換する必要
がある。この入力変換において大きな入力まで変
換することを考えるとき、量子化があらくなるた
め小入力に対して誤差が大きくなる。したがつて
感度を良くしようと考えるときは、できるだけ小
さな入力をAD変換器12のフルスケール入力と
考えねばならない。しかし(21)〜(23)式の試算値
をみると、健全相差電流、事故相差電流の大きさ
は、3×零相差電流の大きさの夫々1.5倍、2.5倍
となり量子化のあらさもこれに比例することにな
る。
On the other hand, when configuring RY1 on a digital computer,
In order to respond correctly to input, it is necessary to follow the steps in Figure 1.
It is necessary to perform analog/digital conversion in the AD converter 12 to convert the input into a size that is accurately proportional to the input. When considering converting even large inputs in this input conversion, the error becomes large for small inputs because quantization becomes slow. Therefore, when considering improving the sensitivity, it is necessary to consider the smallest possible input as the full-scale input of the AD converter 12. However, looking at the estimated values of equations (21) to (23), the magnitudes of the healthy phase difference current and faulty phase difference current are 1.5 times and 2.5 times the magnitude of the 3 x zero phase difference current, respectively, and the roughness of quantization is also similar. It will be proportional to.

したがつて、いま、循環零相電流が無視できる
程小さな場合を考えると、各相差電流を入力する
必要のある補償形地絡回線選択継電器は、各相差
電流を入力する際の量子化誤差のため、零相差電
流のみを演算電流とする一般の地絡回線選択継電
器に比べ事故検出能力が劣ることとなる。
Therefore, if we consider the case where the circulating zero-sequence current is negligibly small, the compensated ground fault line selection relay that needs to input each phase difference current will be able to handle the quantization error when inputting each phase difference current. Therefore, the fault detection ability is inferior to that of a general ground fault line selection relay that uses only the zero-sequence difference current as the calculation current.

この性能劣化は第4図に示すT分岐付の完全2
端子送電線に適用する場合を考えると更にはげし
くなる。第4図は送電線3に負荷L2を有するT
分岐を有する系統であり、他は第3図bと同じで
ある。
This performance deterioration is due to the complete 2
This situation becomes even more serious when we consider the case where it is applied to terminal transmission lines. Figure 4 shows T with load L 2 on transmission line 3.
This is a branched lineage, and the rest is the same as in Fig. 3b.

第4図において、送電線2に流れる負荷電流
(IL1+IL2)のx%が負荷L2に流れ、(1−x)%
が負荷Lに流れるものとする。
In Fig. 4, x% of the load current (I L1 + I L2 ) flowing through the transmission line 2 flows to the load L 2 , and (1-x)%
Assume that the current flows to the load L.

このとき、RY1の入力電気量は、 健全相差電流=(IL1+IL2)(1+x) 事故相差電流=(IL1+IL2)(1+x)+2IF
……(24) となる。したがつてT分岐を有する系統に補償形
地絡回線選択継電器を適用しようとすると、各相
差電流をかなり大きな範囲まで考えなければなら
ないことになる。そのため事故検出能力を低下し
たまま使用するか、もしくは負荷電流を限定した
系統にのみ適用することを考えざるを得ない。
At this time, the input electricity amount of RY1 is as follows: Healthy phase difference current = (I L1 + I L2 ) (1+x) Fault phase difference current = (I L1 + I L2 ) (1+x) + 2I F
...(24) becomes. Therefore, if a compensated ground fault line selection relay is applied to a system having T-branches, each phase difference current must be considered over a fairly large range. Therefore, it is necessary to consider using the system with reduced fault detection capability, or applying it only to systems with limited load current.

〔発明の目的〕[Purpose of the invention]

本発明は上記問題点を解決することを目的とし
てなされたものであり、補償形地絡回線選択継電
器の性能を低下することなく、完全2端子送電線
の事故検出を行なうことのできる地絡回線選択継
電器を提供することを目的としている。
The present invention has been made with the aim of solving the above problems, and provides a ground fault line that can detect faults in complete two-terminal power transmission lines without degrading the performance of the compensated ground fault line selection relay. The purpose is to provide selective relays.

〔発明の概要〕[Summary of the invention]

本発明では循環零相電流の流れる2端子平行2
回線送電線の1相地絡事故に対して、循環零相電
流の存在する場合と存在しない場合との2通りに
事故区分を行なうと共に、先ず地絡相判別をした
後に健全相差電流又は相電流の大きさ判別を行な
い、これが所定値より大であれば相手端1回線し
や断と判定し、この場合は循環零相電流が消滅し
ているために循環零相電流による影響がないこと
にかんがみ、演算電流としては電流値の小さい零
相差電流と極正量とによる回線選択演算をし、一
方、健全相差電流又は相電流が所定値より小さい
場合は相手端1回線がしや断されていないため、
循環零相電流の影響を考慮して検出電流としての
零相差電流と補償電流としての健全相差電流又は
相電流とによつて得られた電流との差分からなる
演算電流及び極性量とによつて回線選択演算を
し、できるだけ小さい入力電流とすることにより
デジタル継電器のA/D変換回路のフルスケール
入力に合せるようにして地絡回線選択継電器の感
度向上をはかるようにしたものである。
In the present invention, two terminals parallel to each other through which a circulating zero-sequence current flows
For single-phase ground fault accidents in power transmission lines, the fault is classified into two types: when there is a circulating zero-sequence current and when there is not. If it is larger than a predetermined value, it is determined that one line at the other end has been disconnected, and in this case, it is determined that the circulating zero-sequence current has disappeared, so there is no influence from the circulating zero-sequence current. In consideration, the line selection calculation is performed using the zero-sequence difference current with a small current value and the extreme value as the calculation current.On the other hand, if the healthy phase difference current or the phase current is smaller than a predetermined value, it is assumed that one line at the other end is suddenly disconnected. Because there is no
Taking into account the influence of circulating zero-sequence current, the calculated current and polarity amount are calculated from the difference between the zero-sequence difference current as the detection current and the healthy phase difference current or phase current as the compensation current. By performing line selection calculations and setting the input current as small as possible, the sensitivity of the ground fault line selection relay is improved by matching the full scale input of the A/D conversion circuit of the digital relay.

〔発明の実施例〕[Embodiments of the invention]

以下図面を参照して実施例を説明する。第5図
は本発明による地絡回線選択継電器の演算フロー
図であり、本発明を実現するための具体的構成は
第1図と同様である。なお第2図と同一部分は同
一記号で示し、詳細部分は省略している。そして
第5図において第2図と異なる点はステツプS6
びステツプS7が追加されたことである。
Examples will be described below with reference to the drawings. FIG. 5 is a calculation flow diagram of the ground fault line selection relay according to the present invention, and the specific configuration for realizing the present invention is the same as that in FIG. 1. Note that the same parts as in FIG. 2 are indicated by the same symbols, and detailed parts are omitted. The difference between FIG. 5 and FIG. 2 is that step S6 and step S7 are added.

ステツプS6においては健全相差電流の大きさが
一定値以上であるか否かを判定する処理であり、
一定値以下(NO)のときステツプS4の処理に移
り、一定値以上(YES)のときステツプS7の処
理に移る。ステツプS6における処理は、事故相に
よつて差電流の大きさを判定する相が異なり、
a,b及びc相夫々の事故に対し、ステツプS6-1
ではb相差電流を、ステツプS6-2ではc相差電流
を、ステツプS6-3ではa相差電流の大きさ判定を
行なう。一方、ステツプS7では演算電流ieを零相
差電流ipsに設定すると共に極性量epを求める。極
性量epは零相電圧−vpを使用する。しかしステツ
プS6における事故相判定を記憶することにより従
来のものと同じものを使用できる。前記ステツプ
S7実行後はステツプS5の実行に移る。
Step S6 is a process of determining whether the magnitude of the healthy phase difference current is greater than or equal to a certain value.
If it is less than a certain value (NO), the process moves to step S4 , and if it is more than a certain value (YES), the process moves to step S7 . In the process in step S6 , the phase for which the magnitude of the difference current is determined differs depending on the fault phase.
Step S 6-1 for accidents a, b, and c.
In step S6-2 , the magnitude of the c-phase difference current is determined, and in step S6-3 , the magnitude of the a-phase difference current is determined. On the other hand, in step S7 , the calculation current i e is set to the zero-sequence difference current i ps , and the polarity amount e p is determined. The polarity e p uses the zero-sequence voltage −v p . However, by memorizing the accident phase determination in step S6 , the same method as the conventional one can be used. Said step
After executing S7 , the process moves to step S5 .

次に一連の応動について以下に説明する。先
ず、ステツプS1において開始指令を受けると、ス
テツプS2へ移つて1相地絡であるか否かを判定す
る。ここで1相地絡であることが検出されるとス
テツプS3へ移つて地絡相の演算を行ない、各相に
応じた各判定3Ya,3Yb,3Yc及び3Nが得られる。
前記各判定が得られると(3Nの場合は別)、ステ
ツプS6へ移つて健全相差電流の大小判別を行な
う。即ち、ステツプS6は1端がしや断か否かを判
定する処理であり、健全相差電流が一定値以上で
あるとき1端しや断と判定する。したがつて事故
発生後、1端しや断と判定するまでは従来と全く
同じ判定を行ない(ステツプ1からステツプ3ま
で)、1端しや断と判定した後はステツプS7によ
り零相差電流ipsと極性量epとによる動作原理に基
づく判定を行なう。即ち、1端しや断後は循環零
相電流が消滅するため、零相差電流を演算電流と
しても誤動作することがないためである。なお、
ステツプS6において健全相差電流が一定値以下の
ときはステツプS4へ移つて演算電流及び極性量を
求め、更にステツプS5において故障線路判定がな
される。そしてステツプS7の処理後もステツプS5
に移ることは前記同様である。
Next, a series of responses will be explained below. First, when a start command is received in step S1 , the process moves to step S2 to determine whether or not there is a one-phase ground fault. If a one-phase ground fault is detected here, the process moves to step S3 to calculate the ground fault phase, and each determination 3Y a , 3Y b , 3Y c and 3N corresponding to each phase is obtained.
When each of the above judgments is obtained (except in the case of 3N), the process moves to step S6 , and a judgment is made as to whether the healthy phase difference current is large or small. That is, step S6 is a process for determining whether or not one end is broken, and when the healthy phase difference current is equal to or higher than a certain value, it is determined that one end is broken. Therefore, after an accident occurs, the same judgment as before is performed until it is determined that one end is ruptured (from step 1 to step 3), and after it is determined that one end is sintered, the zero-sequence difference current is reduced in step S7 . Judgment is made based on the operating principle based on i ps and the polarity e p . That is, since the circulating zero-sequence current disappears after one end is disconnected, malfunction will not occur even if the zero-sequence difference current is used as the calculation current. In addition,
If the healthy phase difference current is below a certain value in step S6 , the process moves to step S4 to obtain the calculated current and polarity, and further, in step S5 , a faulty line is determined. Then, after the processing in step S 7 , the process continues in step S 5 .
The process of moving to is the same as above.

ここでステツプS6における健全相差電流の判定
レベルは以下のように判定することができる。
Here, the determination level of the healthy phase difference current in step S6 can be determined as follows.

即ち、1相地絡事故発生時において1端しや断
となる前の健全相の差電流は、第3図aから明ら
かなように、循環電流Ithによる電流値2Ithに等し
くなる(送電線2,3に関して負荷電流がバラン
スしているとみれば)。この差電流2Ithの大きさ
は、一般的には起誘導送電線が健全である場合
は、その負荷電流の約5%程度(計算の例では
2000Aの負荷電流として約100A程度)であり、
起誘導送電線に事故発生があつた場合はその事故
電流の約10%程度(計算の例では7000Aの1相地
絡電流として約500A程度)である。
In other words, when a single-phase ground fault occurs, the difference current between the healthy phases before one end becomes disconnected is equal to the current value 2I th due to the circulating current I th (as shown in Figure 3a). Assuming that the load currents are balanced for wires 2 and 3). Generally speaking, the magnitude of this difference current 2I th is about 5% of the load current (in the calculation example) when the induced power transmission line is healthy.
(approximately 100A as a load current of 2000A),
If an accident occurs in an induced power transmission line, the current will be approximately 10% of the fault current (in the calculation example, approximately 500A as a single-phase ground fault current of 7000A).

健全相の差電流は1端しや断となる前の最大値
は2Ithであり、この2Ith以上流れたときは少なく
とも1端しや断とみなすことができる。したがつ
てステツプS6における差電流の判定レベルとして
は、起誘導送電線の種々の運転条件下で想定され
る最大の循環電流(上記計算の場合500A)から
判定することができる。この値は(23)式で示した
零相差電流の一計算値と比較しても充分小さな値
である。
The maximum value of the differential current of a healthy phase before one end is interrupted is 2I th , and when it flows more than 2I th , it can be considered that at least one end is interrupted. Therefore, the determination level of the difference current in step S6 can be determined from the maximum circulating current (500 A in the above calculation) assumed under various operating conditions of the induction power transmission line. This value is sufficiently small compared to the calculated value of the zero-sequence difference current shown in equation (23).

したがつて第5図の演算処理方法によれば各相
差電流の入力の最大値を小さくすることができ
る。このことによりアナログ/デジタル変換にお
ける誤差を小さくすることができるので補償形地
絡回線選択継電器の演算電流の演算誤差を小さく
し、事故検出能力を高めることができる。
Therefore, according to the arithmetic processing method shown in FIG. 5, the maximum input value of each phase difference current can be reduced. This makes it possible to reduce the error in analog/digital conversion, thereby reducing the calculation error in the calculation current of the compensated ground fault line selection relay and improving the fault detection ability.

なお、ステツプS6における差電流の大きさ判定
において、a,b,c相地絡検出に対して夫々
b,c,a相を用いているが、これに限定される
ものではなく、例えばa,b相地絡に対してはc
相差電流を、c相地絡に対してはa相を用いるよ
うに、健全相2相のうちのいずれを用いてもよい
ことは明らかである。更に、健全相2相の絶対値
の和や、健全相2相の夫々の絶対値の平均値等を
用いてもよい。
In addition, in determining the magnitude of the difference current in step S6 , the b, c, and a phases are used for ground fault detection of the a, b, and c phases, respectively, but the present invention is not limited to this. , c for b-phase ground fault
It is clear that any of the two healthy phases may be used for the phase difference current, such as using the a phase for a c-phase ground fault. Furthermore, the sum of the absolute values of the two healthy phases, the average value of the respective absolute values of the two healthy phases, etc. may be used.

又、上記方式をT分岐付の2端子送電線に適用
する場合は各負荷電流IL1,IL2のアンバランス分
(IL1−IL2)を考慮して、ステツプS6における判定
値を決定すればよい。
Also, when applying the above method to a two-terminal power transmission line with a T-branch, the judgment value in step S6 is determined by considering the unbalanced portion (I L1 - I L2 ) of each load current I L1 and I L2 . do it.

第6図は本発明による他の実施例演算フロー図
である。
FIG. 6 is a calculation flow diagram of another embodiment according to the present invention.

本実施例においては地絡相判別をした後、相手
端1回線しや断を確認するのに、各健全相差電流
の正相分算出によつて行なおうとするものであ
る。即ち、ステツプ3の地絡相判別処理とステツ
プ4の演算電流及び極性量の算出処理の間に、ス
テツプ8として健全相差電流の正相分算出処理を
入れようとするものであり、その他は前記第5図
の場合と同様である。
In the present embodiment, after determining the ground fault phase, confirmation of disconnection of one line at the other end is performed by calculating the positive phase component of each healthy phase difference current. That is, between the ground fault phase discrimination process in step 3 and the calculation process for the calculated current and polarity amount in step 4, the process for calculating the positive phase component of the healthy phase difference current is inserted as step 8, and the rest is as described above. This is the same as the case in FIG.

ステツプ8による正相分の演算は以下のように
行なわれる。
The calculation of the positive phase component in step 8 is performed as follows.

ia1s=1/3(ias+aibs+a2ics) ……(25) ここでia1sはias基準の正相分である。 i a1s = 1/3 (i as + ai bs + a 2 i cs ) ...(25) Here, i a1s is the positive phase component of the i as standard.

そしてステツプS8-1,S8-2,S8-3では前記正相
分ia1sと所定値との大小関係を判断処理する。こ
の判断結果が所定値以下の場合(相手端1端しや
断でない)であるときはステツプS4へ移つて常時
の循環零相電流を補償した零相差電流と極性量と
を求め、又、所定値以上の場合(相手端1端しや
断である)はステツプS7へ移つて零相差電流と極
性量とを求めることは第5図に示したものと同じ
である。
Then, in steps S 8-1 , S 8-2 , and S 8-3, the magnitude relationship between the positive phase component i a1s and a predetermined value is determined. If the result of this judgment is less than a predetermined value (one end of the other end is not disconnected), the process moves to step S4 , where the zero-sequence difference current that compensates for the normal circulating zero-sequence current and the polarity amount are determined. If the value exceeds a predetermined value (one end of the other end is disconnected), the process moves to step S7 and the zero-sequence difference current and polarity are determined in the same manner as shown in FIG.

ここで平行回線の各相に流れる循環電流の一例
は下記の通りであり、これは既に提案されている
ものである。
Here, an example of the circulating current flowing through each phase of the parallel line is as follows, and this has already been proposed.

起誘導送電線が平常運転であり各負荷が
1000Aのとき、 2iath=94.4∠25° (A) 2ibth=42.8∠27° (A) 2icth=25.6∠27° (A) ……(26) 起誘導送電線が無負荷運転であり、1相地絡
が発生して事故電流が7000Aのとき 2iath=474∠142° (A) 2iath=474∠142° (A) 2ibth=232∠143° (A)2icth=150∠144° (A)……(2
7) 但し、iath,ibth,icthは夫々a,b,c相の循環
電流である。
The induction power transmission line is in normal operation and each load is
At 1000A, 2i ath = 94.4∠25° (A) 2i bth = 42.8∠27° (A) 2i cth = 25.6∠27° (A) ……(26) The electromotive transmission line is in no-load operation, When a 1-phase ground fault occurs and the fault current is 7000A, 2i ath = 474∠142° (A) 2i ath = 474∠142° (A) 2i bth = 232∠143° (A)2i cth = 150∠144 ° (A)……(2
7) However, i ath , i bth , and i cth are circulating currents of a, b, and c phases, respectively.

上記(26)式(27)式から明らかなように、各相に
流れる循環電流は起誘導送電線の運転状況によら
ず、ほぼ同相に流れ、大きさのみ多少異なる。一
方、各相差電流は、送電線2,3の負荷電流IL1
及びIL2がほぼバランスしていれば負荷電流の影
響はない。したがつて上記したの場合の条件下
において、(25)式の値を求めると下記となる。
As is clear from the above equations (26) and (27), the circulating currents flowing in each phase flow in almost the same phase regardless of the operating status of the induced power transmission line, and only the magnitude differs to some extent. On the other hand, each phase difference current is the load current I L1 of power transmission lines 2 and 3
If I L2 and I L2 are almost balanced, there is no influence of load current. Therefore, under the conditions described above, the value of equation (25) is determined as follows.

|ia1s|=|1/3(2iath+2aibth+2a2icth)| =|1/3(474+2×232∠120°+2×150∠ 240°)| =97 (A)……(28) 正相分の算出はどの相を基準にしても(28)式の
値となる。
|i a1s |=|1/3 (2i ath +2ai bth +2a 2 i cth )| =|1/3 (474+2×232∠120°+2×150∠240°)| =97 (A)……(28) Calculation of the positive phase component will be the value of equation (28) regardless of which phase is used as the reference.

上記(28)式の計算例からもわかるように、相手
端1端しや断の有無を判定するために正相分を算
出することにより、ステツプS8-1,S8-2,S8-3
おける判定レベルは、循環電流の最大値が474A
の場合でも97Aまで落すことができる。
As can be seen from the calculation example of equation (28) above, steps S 8-1 , S 8-2 , and S 8 The judgment level for -3 is that the maximum value of circulating current is 474A.
Even in the case of , it can be reduced to 97A.

以上(28)式の計算例では負荷電流IL1,IL2がバラ
ンスしている場合でも説明したが、T分岐を有す
る2端子送電線のように、負荷がアンバランスの
場合を以下に説明する。
In the calculation example of equation (28) above, we have explained the case where the load currents I L1 and I L2 are balanced, but below we will explain the case where the load is unbalanced, such as a two-terminal transmission line with a T-branch. .

即ち、負荷がアンバランスのときは、各相差電
流ias,ibs,icsにおいてアンバランスが発生する。
(25)式による正相分算出に際してアンバランス分
の大きさが導出されることになる。したがつて前
記(28)式による計算例を考えるとき、(28)式の値
に各相の負荷のアンバランス分を加味した値が、
各ステツプS8-1,S8-2,S8-3における判定レベル
となる。しかし、この場合にもステツプS8で示し
た相手端しや断の有無の判定が負荷電流の小さな
送電線でも正しく判定できることは明らかであ
る。
That is, when the load is unbalanced, unbalance occurs in each phase difference current i as , i bs , and i cs .
When calculating the positive phase component using equation (25), the magnitude of the unbalanced component is derived. Therefore, when considering the calculation example using equation (28) above, the value obtained by adding the unbalanced load of each phase to the value of equation (28) is
This is the judgment level at each step S 8-1 , S 8-2 , and S 8-3 . However, even in this case, it is clear that the determination of whether or not the other end is disconnected shown in step S8 can be correctly determined even in a transmission line with a small load current.

第7図は本発明が適用されるデイジタル保護継
電装置の他の構成図である。
FIG. 7 is another configuration diagram of a digital protective relay device to which the present invention is applied.

一般にデイジタル計算機では多要素の動作判定
が可能であり、地絡回線選択継電器と後備保護用
の継電器を1台に収納する場合がある。この場
合、電流入力は後備保護用にも各回線毎に入力す
る必要があり、差電流は内部で演算して求める方
法がとられる。第7図はこのような場合の適用例
を示すものである。
In general, digital computers are capable of determining the operation of multiple elements, and there are cases where a ground fault line selection relay and a back-up protection relay are housed in one computer. In this case, it is necessary to input the current for each line for back-up protection, and the difference current is calculated internally. FIG. 7 shows an example of application in such a case.

したがつて第7図においては各送電線2,3の
各相電流及び零相電流に対応した電流、ia1,ib1
ic1,ia2,ib2,ic2,ip1,ip2の夫々が入力変換器9
に入力される構成以外は第1図の構成と同じであ
る。そこで各回線毎に取込んだ各相電流と零相電
流をデイジタル計算機13による動作判定に先立
つて差を演算する方法を用いれば、第1図の構成
によつて説明した各演算フロー図がそのまま適用
できる。
Therefore, in FIG. 7, the currents corresponding to each phase current and zero-sequence current of each power transmission line 2 and 3, i a1 , i b1 ,
Each of i c1 , i a2 , i b2 , i c2 , i p1 , and i p2 is input to the input converter 9
The configuration is the same as that shown in FIG. 1 except for the configuration input in . Therefore, if a method is used that calculates the difference between each phase current and zero-sequence current taken in for each line prior to operation judgment by the digital computer 13, each calculation flowchart explained using the configuration of FIG. 1 can be used as is. Applicable.

第8図は本発明による演算フローの一実施例で
ある。第8図においてステツプS9は補償形地絡回
線選択継電器の演算に先立ち、各相電流及び零相
電流の差電流を算出し記憶する処理である。ステ
ツプS10は各回線の健全相の電流値の大きさを判
定する処理を行ない、両回線の同一相電流が共に
所定値以下のときステツプS4に実行を移し、いず
れか一方が所定値以上のときステツプS7へ実行を
移す。ステツプS10において、a相地絡が判定さ
れたときは送電線2におけるb相電流ib1の大き
さを判定する処理ステツプS101-1を実行する。こ
こでib1が所定値より小さいとき、次にステツプ
S102-1を実行する。このステツプS102-1において
は送電線3におけるb相電流ib2の大きさを判定
する。この大きさ判定レベルはステツプS101-1
同じである。そして前記各所定値より小さいと
き、次にステツプS4を実行する。又、ステツプ
S101-1,ステツプS102-1にて所定値より大きいと
判定されたときは、共にステツプS7へ実行を移
す。同様にしてステツプS101-2,S102-2,S101-3
S102-3においては夫々ic1,ic2,ia1,ia2の大きさ判
定を行なう。以上のステツプS10内における大き
さ判定レベルは等しくすることができ、以下のよ
うに決定することができる。
FIG. 8 shows an embodiment of the calculation flow according to the present invention. In FIG. 8, step S9 is a process of calculating and storing the difference current between each phase current and the zero-sequence current prior to calculation of the compensated ground fault line selection relay. Step S10 performs processing to determine the magnitude of the current value of the healthy phase of each line, and when the same phase currents of both lines are both below a predetermined value, the process moves to step S4 , and when either one is above a predetermined value. When , execution moves to step S7 . In step S10 , when an a-phase ground fault is determined, processing step S101-1 is executed to determine the magnitude of the b-phase current i b1 in the power transmission line 2. Here, when i b1 is smaller than the predetermined value, the next step is
Execute S 102-1 . In this step S102-1 , the magnitude of the b-phase current i b2 in the power transmission line 3 is determined. This size determination level is the same as step S101-1 . If it is smaller than each of the predetermined values, then step S4 is executed. Also, step
If it is determined in step S 101-1 and step S 102-1 that the value is larger than the predetermined value, the process moves to step S 7 . Similarly, steps S 101-2 , S 102-2 , S 101-3 ,
In S102-3 , the sizes of i c1 , i c2 , i a1 , and i a2 are determined, respectively. The size determination levels in step S10 above can be made equal and can be determined as follows.

即ち、1相地絡発生時、1端しや断までの各回
線健全相の電流の大きさの最大値は下記で表わせ
る。
That is, when a one-phase ground fault occurs, the maximum value of the current in each healthy phase of each line until one end is disconnected can be expressed as follows.

ip=iL+ith ……(29) 但し、iLは負荷電流、ithは循環電流である。 i p = i L + i th ... (29) where i L is the load current and i th is the circulating current.

ここで負荷電流iLは各相バランスしていると考
えることができる。一方、各相の循環電流は(2
6)、(27)式で示した如く、起誘導送電線の状況に
より多少異なるため、想定される最大の循環電流
を(29)式のith値をして選べばよい。
Here, it can be considered that the load current i L is balanced for each phase. On the other hand, the circulating current of each phase is (2
6), as shown in equation (27), it varies somewhat depending on the situation of the induced power transmission line, so the expected maximum circulating current can be selected by calculating the i th value of equation (29).

一方は、1端しや断後は健全回線側の健全相の
電流値は下記となる。
On the other hand, after one end is disconnected, the current value of the healthy phase on the healthy line side is as follows.

ip′=2iL ……(30) したがつて、負荷電流iLが循環電流ithより大きい
送電線に対しては、健全相2相が共に(29)式にて
決定される値以下か否かで1端しや断か否かを判
定することができる。よつて、各相入力の大きさ
は(29)式まで考えればよい。
i p ′=2i L ……(30) Therefore, for a transmission line where the load current i L is larger than the circulating current i th , both of the two healthy phases are below the value determined by equation (29). It is possible to determine whether or not there is an end or not. Therefore, the magnitude of each phase input can be determined by considering equation (29).

第9図は本発明による演算フローの他の実施例
である。
FIG. 9 shows another embodiment of the calculation flow according to the present invention.

本実施例では想定される循環電流が負荷電流よ
り大きな場合を説明するためのものである。第9
図においてステツプS11は各回線相電流ia1,ia2
準の正相分を算出する。その他の構成は第8図の
場合と同様である。ステツプS111-1は1回線a相
に関する正相分ia11の算出を行ない、その値が所
定値以下のとき、次のステツプS112-1に実行を移
す。ステツプS112-1では2回線a相ia2に関する正
相分ia21の算出を行ない、その値が所定値以下の
とき、次のステツプS4に実行を移す。そしてステ
ツプS111-1及びステツプS112-1において夫々所定
値以上のときはステツプS7に実行を移す。ステツ
プS111-2,ステツプS112-2,ステツプS111-3,ステ
ツプS112-3においても前記同様ia1,ia2に関する正
相分ia11,ia21の判定処理を行なう。このステツプ
S11における正相分の算出は(25)式において差電
流の代りに相電流を用いればよい。なお(25)式に
おいては差電流を用いていたため、(28)式に示し
たように循環電流分のみが僅かに算出されるもの
であつたが、ステツプS11における正相分の算出
では負荷電流分も含まれ、 iq=iL+Δith ……(31) となる。ここでΔithは相電流に含まれる循環電流
より算出するため、(28)式に示す値の1/2に相当
する。したがつて(29)式と比べたとき、相電流の
正相分の大きさには循環電流の影響は小さくな
る。故に第9図の演算フローを用いれば循環電流
が負荷電流より大きな送電線に対しても相手端し
や断か否かの判定が充分正確に行なえると云え
る。
This example is intended to explain a case where the assumed circulating current is larger than the load current. 9th
In the figure, step S11 calculates the positive phase component of each line phase current i a1 and i a2 reference. The other configurations are the same as in the case of FIG. 8. Step S111-1 calculates the positive phase component i a11 for the a phase of one line, and when the value is less than a predetermined value, the process moves to the next step S112-1 . In step S112-1 , the positive phase component i a21 of the second line a phase i a2 is calculated, and when the value is less than a predetermined value, the process moves to the next step S4 . In step S111-1 and step S112-1 , if the value is greater than the predetermined value, the process moves to step S7 . In step S 111-2 , step S 112-2 , step S 111-3 , and step S 112-3 , the determination process of positive phase components i a11 and i a21 regarding i a1 and i a2 is performed in the same manner as described above. This step
To calculate the positive phase component in S11 , phase current may be used instead of the difference current in equation (25). Note that since the differential current was used in equation (25), only the circulating current component was slightly calculated as shown in equation (28), but in the calculation of the positive phase component in step S11 , the load The current is also included, so i q = i L + Δi th ...(31). Since Δi th is calculated from the circulating current included in the phase current, it corresponds to 1/2 of the value shown in equation (28). Therefore, when compared with equation (29), the influence of the circulating current on the magnitude of the positive phase portion of the phase current is small. Therefore, it can be said that if the calculation flow shown in FIG. 9 is used, it is possible to determine with sufficient accuracy whether or not the other end is disconnected even for a power transmission line where the circulating current is larger than the load current.

第10図は本発明による他の一実施例演算フロ
ー図である。
FIG. 10 is a calculation flow diagram of another embodiment according to the present invention.

本実施例では検出電流と補償電流との差分の事
故前後の変化分を演算電流とするものである。即
ち、第5図との違いはステツプS2における1相地
絡検出処理において、1相地絡が検出されないと
き、ステツプS12、ステツプS13を実行すること、
及びステツプS4がステツプS14に代つたことであ
る。以下この変更部のみについて説明する。
In this embodiment, the amount of change in the difference between the detected current and the compensation current before and after the accident is used as the calculated current. That is, the difference from FIG. 5 is that in the one-phase ground fault detection process in step S2 , when a one-phase ground fault is not detected, steps S12 and S13 are executed;
and step S4 has replaced step S14 . Only this changed part will be explained below.

ステツプS12は、ステツプS2において1相地絡
検出判定がなされないとき、これに続いて短絡事
故の有無を判定する。しかしステツプS12におい
て短絡事故が検出されると、図示されない短絡処
理に移る。又、ステツプS12において短絡事故が
検出されない場合は次のステツプS13に移る。こ
こでステツプS13は後述する諸量の値を記憶する。
そしてこの記憶を行なつた後、ステツプS1の開始
に戻る。ステツプS14はどの相の地絡であるかに
応じ、各ステツプS14-1,S14-2及びS14-3におい
て、電圧、電流及び前記したステツプS13の記憶
量を用い、演算量eea,eeb又はeecを求める。
In step S12 , when a one-phase ground fault detection determination is not made in step S2 , it is subsequently determined whether or not there is a short circuit accident. However, if a short circuit accident is detected in step S12 , the process moves to short circuit processing (not shown). Further, if no short circuit fault is detected in step S12 , the process moves to the next step S13 . Here, in step S13 , values of various quantities described later are stored.
After performing this memorization, the process returns to the start of step S1 . Step S14 uses the voltage, current, and the amount of memory in step S13 described above to calculate the calculation amount in each step S14-1 , S14-2 , and S14-3 depending on which phase is the ground fault. Find e ea , e eb or e ec .

以下、ステツプS13,S14について説明する。 Steps S13 and S14 will be explained below.

ステツプS13においては次の演算を行ない、そ
の値を記憶する。
In step S13 , the following calculation is performed and its value is stored.

ipsM×vbeM,ipsM×vcaM,ipsM×vabM, K4bibsM×vbcM,K4ea(icsM+iasM)×vcaM, K4bibsM×vabM ……(31) 但し、ipsM,ibsM,icsM,iasMは夫々零相、b相、
c相及びa相の各差電流ips,ibs,ics及びiasの記憶
時の値、vbcM,vcaM,vabMは夫々bc相、ca相及び
ab相の各相間電圧vb−vc,vc−va及びva−vbの記
憶時の値、K4b,K4caは定数である。又、上式は
全ての外積であり、以下記号×でその関係を示
す。
i psM ×v beM , i psM ×v caM , i psM ×v abM , K 4b i bsM ×v bcM , K 4ea (i csM + i asM ) × v caM , K 4b i bsM ×v abM ……(31) However, i psM , i bsM , i csM , and i asM are zero phase, b phase, and i asM, respectively.
The stored values of the difference currents i ps , i bs , i cs and i as of the c-phase and a-phase, v bcM , v caM , v abM are the values of the bc-phase, ca-phase and ca-phase, respectively.
The values at the time of storage of the inter-phase voltages v b -v c , v c -v a and v a -v b of the ab phase, K 4b and K 4ca are constants. Further, the above equation is all cross products, and the relationship is shown below with the symbol x.

A×B=|AB|sim(θA−θB) ……(32) 但し、A及びBはベクトル量、|AB|はA,
Bの積の絶対値、θA及びθBは夫々ベクトル量A及
びBの角度である。
A×B=|AB|sim(θ A −θ B ) ...(32) However, A and B are vector quantities, |AB| is A,
The absolute values of the product of B, θ A and θ B , are the angles of the vector quantities A and B, respectively.

なお、ステツプS2又はS12において地絡事故及
び短絡事故が検出されるには、事故発生後若干時
間を必要とする。したがつてステツプS13の演算
は事故発生後、事故検出までの間は事故時の値で
行なわれる。しかし、この値が記憶値とされるこ
とは好ましくないので、記憶値の更新にあたつて
記憶値に変化が認められたときは、古い値を若干
時間保持し、一定時間内に事故が検出されないと
き記憶値を更新するようにする。
Note that it takes some time after the occurrence of the accident for the ground fault and short circuit fault to be detected in step S2 or S12 . Therefore, the calculation in step S13 is performed using the values at the time of the accident from the time the accident occurs until the accident is detected. However, it is not desirable for this value to be used as a memorized value, so if a change is observed in the memorized value when updating the memorized value, the old value is retained for a short period of time, and an accident is detected within a certain period of time. The stored value will be updated when the value is not stored.

第11図はステツプS13で行なわれる演算フロ
ー図である。先ず第10図のステツプS12におい
て短絡事故が検出されない場合に、ステツプ
S13-1にて前記した(31)式の値を演算する。次にス
テツプS13-2においてステツプS13-1の演算値とス
テツプS13-4に記憶値とを比較し有意差があるか
否かを判断する。もし差がなければステツプS1
戻る。差があればステツプS13-3に移り差が生じ
てから一定時間継続したことを検出する。一定時
間に達しないときはステツプS1に戻り、一定時間
継続と判断されるまでこの処理が繰り返される。
一定時間継続と判断されたときはステツプS13-4
に移り、ステツプS13-1の演算値を記憶する。な
お、上記した一定時間はステツプS12及びステツ
プS2の短絡及び地絡検出時間より若干長い時間と
する。これにより短絡又は地絡事故の検出に若干
の遅れがあつても、事故前の値が記憶される。第
10図のステツプS14においては、ステツプ
S14-1,S14-2又はS14-3で夫々次式で表わされる演
算量eea,eeb及びeecの値を算出する。
FIG. 11 is a flow diagram of the calculation performed in step S13 . First, if no short circuit fault is detected in step S12 of FIG.
In S 13-1 , the value of equation (31) described above is calculated. Next, in step S13-2 , the calculated value in step S13-1 and the stored value in step S13-4 are compared to determine whether there is a significant difference. If there is no difference, return to step S1 . If there is a difference, the process moves to step S13-3 , and it is detected that the difference has continued for a certain period of time since it occurred. If the predetermined time has not been reached, the process returns to step S1 , and this process is repeated until it is determined that the predetermined time has continued.
If it is determined that it will continue for a certain period of time, step S 13-4
The process moves to step S13-1 and stores the calculated value. Note that the above-mentioned fixed time is a slightly longer time than the short circuit and ground fault detection time in step S12 and step S2 . As a result, even if there is a slight delay in detecting a short circuit or ground fault, the value before the fault is stored. In step S14 of FIG.
In S 14-1 , S 14-2 , or S 14-3 , the values of the calculation amounts e ea , e eb , and e ec each expressed by the following equations are calculated.

eea=eda−eha eeb=edb−ehb eec=edc−ehc ……(33) 但し、eda,edb及びedcは検出量、eha,ehb及び
ehcは補償量であり、いずれも次式で表わされる。
e ea = e da −e ha e eb = e db −e hb e ec = e dc −e hc ...(33) However, e da , e db and e dc are the detected amounts, e ha , e hb and
e hc is the amount of compensation, both of which are expressed by the following equations.

eda=ips×vbc−ipsM×vbcM edb=ips×vcb−ipsM×vcaM edc=ips×vab−ipsM×vabM ……(34) eha=K4bibs×vbc−K4bibsM×vbcM eha=K4bibs×vbc−K4bibsM×vbcM ehb=K4ca(ics+ias)×vca−K4ca(icsM+iasM)×vc
aM
ehc=K4bibs×vab−K4bibsM×vabM ……(35) 但し、vbc,vca及びvabは相間電圧vb−vc,vc
va及びva−vbである。
e da = i ps ×v bc −i psM ×v bcM e db = i ps ×v cb −i psM ×v caM e dc = i ps ×v ab −i psM ×v abM ……(34) e ha = K 4b i bs ×v bc −K 4b i bsM ×v bcM e ha =K 4b i bs ×v bc −K 4b i bsM ×v bcM e hb =K 4ca (i cs +i as )×v ca −K 4ca (i csM + i asM )×v c
aM
e hc = K 4b i bs ×v ab −K 4b i bsM ×v abM ……(35) However, v bc , v ca and v ab are interphase voltages v b −v c , v c
v a and v a −v b .

上記した(34)式による検出量は、いずれも零相
差電流ipsと事故相に対する直角位相の電圧(以
後、単に直角電圧と云う)vbc,vca又はvabの外積
の値の事故検出前に記憶された記憶値に対する事
故検出後の値の変化分(以後、単に事故変化分と
云う)である。又、(35)式の補償量は健全相中の
1相の差電流ibs又は健全2相の差電流の合成値ics
+iasと直角電圧の外積の事故変化分である。
The detection amount according to equation (34) above is the fault detection of the cross product of the zero-sequence difference current i ps and the voltage in quadrature to the fault phase (hereinafter simply referred to as quadrature voltage) v bc , v ca or v ab . This is the amount of change in the value after the accident detection with respect to the previously stored stored value (hereinafter simply referred to as the amount of change in the accident). In addition, the compensation amount in equation (35) is the difference current i bs of one phase in the healthy phase or the composite value i cs of the difference current of two healthy phases.
This is the accidental change in the cross product of +i as and the orthogonal voltage.

以上説明したように検出電流idと補償電流ih
差分の事故前後の変化分に応動する補償形地絡回
線選択継電器において、1相地絡検出前は健全状
態の電気量を記憶し、1相地絡検出後はステツプ
S3による地絡相別の結果により健全相の差電流の
大きさを判定する。この健全相の差電流の大きさ
が所定値より小さいときはステツプS14により(3
3)式を算出して補償形の地絡回線選択を行なう
が、所定値より大きいときはステツプS13におけ
る記憶値に関係なく、零相差電流の大きさに応動
する普通の地絡回線選択を行なうものである。
As explained above, in the compensated ground fault line selection relay that responds to the change in the difference between the detection current i d and the compensation current i h before and after the fault, the amount of electricity in a healthy state is memorized before the detection of a 1-phase ground fault, Step after detecting 1-phase ground fault
Determine the magnitude of the difference current of the healthy phase based on the results for each ground fault phase in S3 . If the magnitude of the difference current of this healthy phase is smaller than the predetermined value, step S14 returns (3
3) Calculate the formula to select a compensated ground fault line, but if it is larger than a predetermined value, select a normal ground fault line that responds to the magnitude of the zero-sequence difference current, regardless of the value stored in step S13 . It is something to do.

なお、ステツプS13及びS14における演算量は(3
1),(34)及び(35)式に示したものに限る必要はな
く、(13)式にて示す演算量を使用することができ
る。
Note that the amount of calculations in steps S13 and S14 is (3
1), (34), and (35), and the calculation amount shown in equation (13) can be used.

第12図は本発明による他の演算フロー図であ
り、デイジタル保護継電器の構成は第1図によ
る。
FIG. 12 is another calculation flow diagram according to the present invention, and the configuration of the digital protective relay is based on FIG. 1.

本実施例では第5図における演算フローのステ
ツプS6をステツプS15に置き換えたものであり、
その他は第5図に同じであるため変更部のみ説明
する。
In this embodiment, step S6 of the calculation flow in FIG. 5 is replaced with step S15 ,
Since the other parts are the same as those in FIG. 5, only the changed parts will be explained.

ステツプS15は、ステツプS3において地絡相が
検出された後、各相電流の最大値が所定値以下で
あるか否かを判定し、所定値以下のときステツプ
S4の実行に移り、所定値以上のときステツプS7
実行に移る処理を行なう。そしてステツプS15
おいては、先ずステツプS15-1においてステツプ
S3における地絡相の判定結果を記憶する。ステツ
プS15-2では各相差電流ias,ibs及びicsの大きさを
算出し、そのうちの最大値を決定する。次にステ
ツプS15-3ではステツプS15-2において算出された
最大値の値と所定値との比較を行ない、所定値よ
り大きいときステツプS7の実行に移る。一方、所
定値より小さいときステツプS15-4に実行を移す。
ステツプS15-4においてはステツプS15-1で記憶し
た内容を読み出して地絡相を判定し、ステツプS4
における地絡相に応じた演算処理の実行を可能に
する。
In step S15 , after the ground fault phase is detected in step S3 , it is determined whether the maximum value of each phase current is less than or equal to a predetermined value, and if the maximum value is less than or equal to the predetermined value, step S15 is executed.
The process moves to step S4 , and when the value is equal to or greater than a predetermined value, the process moves to step S7 . In step S15 , first, step S15-1 is performed.
The determination result of the ground fault phase in S3 is stored. In step S15-2 , the magnitude of each phase difference current i as , i bs and i cs is calculated, and the maximum value thereof is determined. Next, in step S15-3 , the maximum value calculated in step S15-2 is compared with a predetermined value, and when it is larger than the predetermined value, the process moves to step S7 . On the other hand, if the value is smaller than the predetermined value, the process moves to step S15-4 .
In step S 15-4 , the contents stored in step S 15-1 are read out to determine the ground fault phase, and in step S 4
It is possible to perform calculation processing according to the ground fault phase in the ground fault phase.

なお、ステツプS15-3における比較対象の所定
値としては、入力の大きさがA/D変換のフルス
ケールを超過しているか否かが判定できるように
設定する。即ち、A/D変換のフルスケールは、
相手端しや断前の応動を正しく行なうため、当然
想定し得る循環電流値以上に設定される。したが
つて本実施例においては相手端しや断が生じて
も、各相差電流の入力がA/D変換のフルスケー
ル以内であるならば「補償形」による地絡回線選
択を継続して実行し、A/D変換のフルスケール
を超過する危険があるときのみ、通常の地絡回線
選択に切換えるものである。以上説明した本実施
例によつても入力のフルスケールを最小限に抑え
ることができるため地絡回線選択継電器の感度を
良くすることができる。
Note that the predetermined value to be compared in step S15-3 is set so that it can be determined whether or not the magnitude of the input exceeds the full scale of A/D conversion. That is, the full scale of A/D conversion is
In order to properly respond to the other end and before disconnection, the circulating current value is naturally set to be higher than the expected circulating current value. Therefore, in this embodiment, even if the other end is disconnected or disconnected, as long as the input of each phase difference current is within the full scale of A/D conversion, ground fault line selection using the "compensation type" is continued. However, only when there is a risk of exceeding the full scale of A/D conversion, the switch is made to the normal ground fault line selection. According to the present embodiment described above, the full scale of the input can be minimized, so that the sensitivity of the ground fault line selection relay can be improved.

本実施例におけるステツプS15の方法は第12
図に限られるものではなく、各相電流を用いる第
7図の構成においても適用可能である。この場合
には、両回線の各相電流ia1,ia2,ib1,ib2,ic1
ic2のうちから最大値を検出し、その大きさが所
定値より小さいことを判定する処理を第8図にお
けるステツプS10の代りに行なう演算フローとす
ればよい。
The method of step S15 in this example is the 12th
The present invention is not limited to the one shown in the figure, but can also be applied to the configuration shown in FIG. 7, which uses currents in each phase. In this case, each phase current of both lines i a1 , i a2 , i b1 , i b2 , i c1 ,
The calculation flow may be such that the process of detecting the maximum value among i c2 and determining that the magnitude thereof is smaller than a predetermined value is performed instead of step S10 in FIG.

更に本実施例におけるステツプS15を第10図
におけるステツプS6に置換えることにより、(13)
式の原理による補償形地絡回線選択継電器に適用
できることは明らかである。
Furthermore, by replacing step S15 in this embodiment with step S6 in FIG. 10, (13)
It is clear that the formula can be applied to a compensated ground fault line selection relay based on the principle of

第13図は本発明による他の演算フロー図であ
り、デイジタル保護継電器の構成は第7図によ
る。
FIG. 13 is another calculation flow diagram according to the present invention, and the configuration of the digital protective relay is as shown in FIG. 7.

本実施例では第8図における演算フローのステ
ツプS10をステツプS16に置換えたものであり、そ
の他は第8図に同じであるため変更部のみ説明す
る。
In this embodiment, step S10 of the calculation flow in FIG. 8 is replaced with step S16 , and since the rest is the same as in FIG. 8, only the changed part will be explained.

ステツプS16は、ステツプS3において地絡相が
検出された後、2回線の同一相電流の大きさの差
が所定値により大であるか否かを判定し、1相で
も所定値より大きいときステツプS7に実行を移
し、いずれも所定値より小であるときステツプS4
の実行に移る処理を行なうものである。そしてス
テツプS16では、先ずステツプS16-1において、ス
テツプS3における地絡相の判定結果を記憶する。
ステツプS16-2では送電線2,3のa相電流ia1
ia2の大きさを算出する。次にステツプS16-3では
前記a相電流ia1とia2の大きさの差が所定値より
も大きいか否かの判定をし、所定値より大きいと
きステツプS7の実行に移り、反対に所定値より小
さいときステツプS16-4の実行に移る。又、b,
c相電流についても全く同じであり、夫々ステツ
プS16-4,S16-6において大きさを算出し、ステツ
プS16-5,S16-7で所定値との判定を行なう。そし
てステツプS16-7において所定値より小さいこと
が判定されると、次のステツプS4の実行に移る。
In step S16 , after the ground fault phase is detected in step S3 , it is determined whether the difference in the magnitude of the same phase current of the two lines is larger than a predetermined value, and even one phase is larger than the predetermined value. If both values are smaller than the predetermined value, the process moves to step S 7 .
This is the process that moves on to execution. In step S16 , first, in step S16-1 , the ground fault phase determination result in step S3 is stored.
In step S16-2 , the a-phase current i a1 of transmission lines 2 and 3 is
i Calculate the size of a2 . Next, in step S16-3 , it is determined whether the difference in magnitude between the a-phase currents i a1 and i a2 is larger than a predetermined value, and when it is larger than the predetermined value, the process moves to step S7 , and When the value is smaller than the predetermined value, the process moves to step S16-4 . Also, b,
The same is true for the c-phase current, and its magnitude is calculated in steps S 16-4 and S 16-6 , respectively, and it is determined that it is a predetermined value in steps S 16-5 and S 16-7 . If it is determined in step S16-7 that the value is smaller than the predetermined value, the process moves to the next step S4 .

ところで通常は、負荷はバランスしていて負荷
電流の逆相分と零相分は無視可能な大きさである
が、負荷電流が大きくなつて、その逆相分が大き
くなると下記の問題がある。
Normally, the load is balanced and the negative phase and zero phase components of the load current are negligible, but as the load current increases and the negative phase component increases, the following problems occur.

即ち、(10)〜(12)で示したように逆相電流を演算
に使用する補償形地絡回線選択継電器の原理は、
逆相分は負荷電流に対して無視できることを前提
として循環電流を演算電流から消去しようとする
ものである。したがつて負荷電流に逆相成分が含
まれていた場合は、その分が演算誤差となつて性
能劣化を招くことになる。即ち、事故発生後も全
端子が「閉」の状態では差電流を用いて演算を行
なうために逆相成分による影響はないが、相手端
しや断後にあつては、差回路による逆相成分のキ
ヤンセルがなく、各相差電流に逆相分が含まれて
リレー入力となることである。
That is, as shown in (10) to (12), the principle of a compensated ground fault line selection relay that uses negative sequence current for calculation is as follows.
The purpose is to eliminate the circulating current from the calculation current on the premise that the negative phase component can be ignored with respect to the load current. Therefore, if the load current contains an anti-phase component, that amount becomes a calculation error and causes performance deterioration. In other words, even after an accident occurs, when all terminals are closed, calculations are performed using the difference current, so there is no effect of the negative phase component, but after the other end is disconnected or disconnected, the negative phase component due to the difference circuit There is no cancellation, and each phase difference current includes a negative phase component and becomes a relay input.

しかし、負荷電流が大きくその逆相分が問題に
なる系統条件においては、Ith≪IL1,IL2であるか
ら、第3図aの常時では、各相電流について、|
ia1|≒|ia2|,|ib1|≒|ib2|及び|ic1|≒|ic2
|が成り立ち、第3図bの一端しや断後は、|ia1
|=|ib1|=|ic1|=IL1+IL2となる。但し、事
故相はIL1+IL2+IFとなる。したがつて両回線の
各相電流の大きさの差を考えれば、常時は「0」
に等しく、一端しや断後は(IL1+IL2)となる。
そこでステツプS16-3,S16-5,S16-7における判定
レベルは負荷電流に比べて、ほとんど「0」に近
い値とすることができ、高感度に検出することが
できる。
However, under system conditions where the load current is large and its negative phase component becomes a problem, I th ≪ I L1 , I L2 , so at all times in Figure 3a, for each phase current, |
i a1 |≒|i a2 |, |i b1 |≒|i b2 | and |i c1 |≒|i c2
| holds true, and after one end of Fig. 3 b, |i a1
|=|i b1 |=|i c1 |=I L1 +I L2 . However, the accident phase is I L1 + I L2 + I F. Therefore, considering the difference in the magnitude of each phase current of both lines, it is always "0".
It is equal to (I L1 + I L2 ) after one end is cut off.
Therefore, the determination levels in steps S 16-3 , S 16-5 , and S 16-7 can be set to values almost close to "0" compared to the load current, and detection can be performed with high sensitivity.

故に本実施例を使用すれば、負荷電流が大き
く、その逆相分が問題となる系統においても、逆
相分電流を演算に使用する補償形地絡回線選択継
電器の性能向上が可能である。
Therefore, by using this embodiment, even in systems where the load current is large and its negative phase component is a problem, it is possible to improve the performance of the compensated ground fault line selection relay that uses the negative phase component current for calculation.

なお、ステツプS16における判定処理を(13)式
の原理にもとづく補償形回線選択継電器に適用で
きることは勿論である。
It goes without saying that the determination process in step S16 can be applied to a compensated line selection relay based on the principle of equation (13).

〔発明の効果〕〔Effect of the invention〕

以上説明した如く、本発明によれば循環零相電
流の流れる2端子平行2回線送電線の1相地絡事
故検出に対して、相手端1回線しや断か否かを検
出することによつて循環零相電流の影響を判別
し、1回線しや断前は補償形地絡回線選択継電器
により循環零相電流に影響されない事故検出を行
ない、相手端1回線しや断後は零相差電流にのみ
応動する従来の地絡回線選択継電器により事故検
出を行なうよう構成したので、補償形地絡回線選
択継電器の演算に用いる各相電流の大きさの範囲
を限定することができ、事故検出の性能を高める
ことができる。
As explained above, according to the present invention, when detecting a one-phase ground fault accident in a two-terminal parallel two-circuit transmission line through which a circulating zero-sequence current flows, it is possible to detect whether one line at the other end is disconnected or not. The effect of the circulating zero-sequence current is determined by using a compensation type ground fault line selection relay before one line is disconnected, and a fault that is not affected by the circulating zero-sequence current is detected. Since the configuration is configured so that fault detection is performed using a conventional ground fault line selection relay that responds only to Performance can be improved.

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

第1図は従来技術及び本発明に共通して用いら
れる一般的なデイジタル保護継電器装置の構成
図、第2図はデイジタル計算機が行なう演算フロ
ーの従来例図、第3図a,bは2回線からなる被
保護送電線の事故前、事故後の系統状態を示す
図、第4図はT分岐を有する2回線送電線におけ
る1相地絡事故発生の状態を示す図、第5図は本
発明による地絡回線選択継電器の演算フロー図、
第6図は他の実施例演算フロー図、第7図は本発
明が適用されるデイジタル保護継電装置の他の構
成図、第8図は他の実施例演算フロー図、第9図
は更に他の実施例演算フロー図、第10図は更に
他の実施例演算フロー図、第11図は第10図の
ステツプS13の詳細演算フロー図、第12図は更
に他の実施例演算フロー図、第13図は更に他の
実施例演算フロー図である。 1……母線、2,3……平行送電線、4,5…
…しや断器、6,7……変流器、8……計器用変
圧器、9……入力変換器、10……サンプルホー
ルド回路、11……マルチプレクサ、12……
A/D変換器、13……デイジタル計算機、1
A,1B……各端母線、IL1,IL2……負荷電流、
Ith……循環零相電流、IF……事故電流。
Fig. 1 is a configuration diagram of a general digital protective relay device commonly used in the prior art and the present invention, Fig. 2 is a conventional example diagram of the calculation flow performed by a digital computer, and Fig. 3 a and b are two-line circuit diagrams. Figure 4 is a diagram showing the state of a one-phase ground fault occurring in a two-circuit transmission line with a T-branch, and Figure 5 is a diagram showing the system status before and after an accident on a protected power transmission line consisting of a T-branch. Calculation flow diagram of ground fault line selection relay by
FIG. 6 is a calculation flow diagram of another embodiment, FIG. 7 is another configuration diagram of a digital protective relay device to which the present invention is applied, FIG. 8 is a calculation flow diagram of another embodiment, and FIG. 10 is a calculation flow diagram of yet another embodiment. FIG. 11 is a detailed calculation flow diagram of step S13 in FIG. 10. FIG. 12 is a calculation flow diagram of still another embodiment. , FIG. 13 is a calculation flow diagram of still another embodiment. 1... Bus bar, 2, 3... Parallel power transmission line, 4, 5...
...Shield disconnector, 6,7... Current transformer, 8... Instrument transformer, 9... Input converter, 10... Sample hold circuit, 11... Multiplexer, 12...
A/D converter, 13...Digital computer, 1
A, 1B...Each end bus bar, I L1 , I L2 ...Load current,
I th ... Circulating zero-sequence current, I F ... Fault current.

Claims (1)

【特許請求の範囲】 1 循環零相電流の流れる2端子平行2回線送電
線の1相地絡事故を保護する地絡回線選択継電器
において、各回線中の1相地絡事故を検出する手
段と、前記地絡事故の地絡相を選別する手段と健
全相の電流または正相電流を導出して所定値と比
較しその大小に応じて相手端1回線しや断を検出
する手段と、零相差電流と極性量とを算出して相
手端1回線しや断検出時に地絡回線を演算する第
1の地絡回線選択手段と、常時の循環零相電流を
補償した零相差電流と極性量とを算出して相手端
1回線しや断でない時に地絡回線を演算する第2
の補償形地絡回線選択手段とを夫々そなえ、相手
端1回線のしや断状態に応じて前記第1、第2の
各地絡回線選択手段を切換えることを特徴とする
地絡回線選択継電器。 2 相手端1回線しや断判定を、健全2相のうち
の少なくとも1相の回線電流値の大きさ、又は差
電流の大きさが所定値より大であることにより行
なうことを特徴とする特許請求の範囲第1項記載
の地絡回線選択継電器。 3 相手端1回線しや断判定を、差電流の正相分
が所定値より大であることにより行なうことを特
徴とする特許請求の範囲第1項記載の地絡回線選
択継電器。 4 循環零相電流の流れる2端子平行2回線送電
線の1相地絡事故を保護する地絡回線選択継電器
において、各回線各相電流及び零相電流の差電流
を導出し記憶する手段と、各回線中の1相地絡事
故を検出する手段と、前記地絡事故の地絡相を選
別する手段と、各回線同一健全相の電流値の大き
さを夫々導出して所定値と夫々個別に比較しその
大小に応じて相手端1回線しや断を検出する手段
と、零相差電流と極性量とを算出して相手端1回
線しや断検出時に地絡回線を演算する第1の地絡
回線選択手段と、常時の循環零相電流を補償した
零相差電流と極性量とを算出して相手端1回線し
や断でない時に地絡回線を演算する第2の補償形
地絡回線選択手段とを夫々そなえ、相手端1回線
のしや断状態に応じて前記第1、第2の各地絡回
線選択手段を切換えることを特徴とする地絡回線
選択継電器。 5 相手端1回線しや断判定を、各回線同一相基
準の正相分が所定値より大であることにより行な
うことを特徴とする特許請求の範囲第4項記載の
地絡回線選択継電器。 6 循環零相電流の流れる2端子平行2回線送電
線の1相地絡事故を保護する地絡回線選択継電器
において、各回線中の1相地絡事故を検出する手
段と、前記1相地絡事故でない場合に短絡事故の
有無を検出する手段と、各相電流及び零相電流の
各差電流と極性量とを夫々記憶すると共に前記記
憶値に変化が認められた場合であつて、かつ一定
時間内に事故が検出されない場合に記憶値を更新
する記憶手段と、前記地絡事故の地絡相を検出す
る手段と、健全相差電流を導出して所定値と比較
しその大小に応じて相手端1回線しや断を検出す
る手段と、零相差電流と極性量とを算出して相手
端1回線しや断検出時に地絡回線を演算する第1
の地絡回線選択手段と、常時の循環零相電流を補
償した零相差電流と極性量とを算出して前記記憶
手段の記憶内容を用いて相手端1回線しや断でな
い時に地絡回線を演算する第2の補償形地絡回線
選択手段とを夫々そなえ、相手端1回線のしや断
状態に応じて前記第1、第2の各地絡回線選択手
段を切換えることを特徴とする地絡回線選択継電
器。 7 循環零相電流の流れる2端子平行2回線送電
線の1相地絡事故を保護する地絡回線選択継電器
において、各回線中の1相地絡事故を検出する手
段と、各回線中の1相地絡相を選別する手段と、
前記地絡相を記憶する手段と、各回線同一相差電
流の大きさを夫々算出して最大値を決定する手段
と、前記最大値と所定値とを比較しその大小に応
じて相手端1回線しや断を検出する手段と、零相
差電流と極性量とを算出して相手端1回線しや断
時に地絡回線を演算する第1の地絡回線選択手段
と、常時の循環零相電流を補償した零相差電流と
極性量とを算出して相手端1回線しや断でない時
に地絡回線を演算する第2の補償形地絡回線選択
手段とを夫々そなえ、相手端1回線のしや断状態
に応じて前記第1、第2の各地絡回線選択手段を
切換えることを特徴とする地絡回線選択継電器。 8 循環零相電流の流れる2端子平行2回線送電
線の1相地絡事故を保護する地絡回線選択継電器
において、各回線各相電流及び零相電流の差電流
を算出し記憶する手段と、各回線中の1相地絡事
故を検出する手段と、前記地絡事故の地絡相を選
別する手段と、前記地絡相を記憶する手段と、各
回線同一相電流の大きさの差を算出して所定値と
比較し、前記比較結果としての差が少なくとも1
相以上大きい場合に相手端1回線しや断と判定す
る手段と、零相差電流と極性量とを算出して相手
端1回線しや断時に地絡回線を演算する第1の地
絡回線選択手段と、常時の循環零相電流を補償し
た零相差電流と極性量とを算出して相手端1回線
しや断でない時に地絡回線を演算する第2の補償
形地絡回線選択手段とを夫々そなえ、相手端1回
線のしや断状態に応じて前記第1、第2の各地絡
回線選択手段を切換えることを特徴とする地絡回
線選択継電器。
[Scope of Claims] 1. In a ground fault line selection relay that protects a 1-phase ground fault in a 2-terminal parallel 2-line power transmission line through which a circulating zero-sequence current flows, means for detecting a 1-phase ground fault in each line; , means for selecting the ground fault phase of the ground fault accident, means for deriving a healthy phase current or positive phase current and comparing it with a predetermined value and detecting a break in one line at the other end according to the magnitude thereof; a first ground fault line selection means that calculates a phase difference current and a polarity amount and calculates a ground fault line when one line at the other end is interrupted; The second method calculates the ground fault line when one line at the other end is not disconnected.
1. A ground fault line selection relay characterized in that said first and second fault line selection means are respectively provided with compensated ground fault line selection means, and are switched in response to a disconnection state of one line at the other end. 2. A patent characterized in that one line at the other end is determined to be disconnected based on the magnitude of the line current value of at least one of the two healthy phases or the magnitude of the difference current being larger than a predetermined value. A ground fault line selection relay according to claim 1. 3. The ground fault line selection relay according to claim 1, wherein the fault determination of one line at the other end is performed based on whether the positive-sequence portion of the differential current is larger than a predetermined value. 4. In a ground fault line selection relay that protects a 1-phase ground fault accident on a 2-terminal parallel 2-line transmission line through which circulating zero-sequence current flows, means for deriving and storing the difference current between each phase current and zero-sequence current of each line; Means for detecting a one-phase ground fault fault in each line; means for selecting the ground fault phase of the ground fault fault; and means for deriving the magnitude of the current value of the same healthy phase of each line and individually setting it to a predetermined value. A means for detecting a break in one line at the other end according to the magnitude thereof compared to A second compensation type ground fault line that calculates a ground fault line selection means and a zero sequence difference current that compensates for the constant circulating zero sequence current and a polarity amount and calculates a ground fault line when one line at the other end is not disconnected. 1. A ground fault line selection relay, characterized in that said first and second fault line selection means are respectively provided with selection means, and are switched between said first and second fault line selection means in response to a disconnected state of one line at the other end. 5. The ground fault line selection relay according to claim 4, wherein the fault determination of one line at the other end is performed based on whether the positive phase component of the same phase reference for each line is larger than a predetermined value. 6. In a ground fault line selection relay for protecting a 1-phase ground fault in a 2-terminal parallel 2-circuit transmission line through which a circulating zero-sequence current flows, a means for detecting a 1-phase ground fault in each line, and a means for detecting a 1-phase ground fault in each line; A means for detecting the presence or absence of a short-circuit accident when it is not an accident, and a means for storing each difference current and polarity of each phase current and zero-sequence current, respectively, and when a change is recognized in the memorized value, and when the value is constant. a storage means for updating a stored value when no fault is detected within the time; a means for detecting the ground fault phase of the ground fault fault; and a means for deriving a healthy phase difference current and comparing it with a predetermined value, A means for detecting a line breakage at one end, and a first means for calculating a ground fault line when a line breakage at the other end is detected by calculating the zero-sequence difference current and the polarity amount.
The ground fault line selection means calculates the zero sequence difference current and polarity amount that compensated for the constant circulating zero sequence current, and uses the stored contents of the storage means to select the ground fault line when one line at the other end is not disconnected. and a second compensating ground fault line selection means for calculating the ground fault, and the first and second ground fault line selection means are switched depending on the failure state of one line at the other end. Line selection relay. 7 In a ground fault line selection relay that protects a 1-phase ground fault in a 2-terminal parallel 2-circuit transmission line through which circulating zero-sequence current flows, a means for detecting a 1-phase ground fault in each line, and a means for detecting a 1-phase ground fault in each line, A means for selecting a phase-to-ground phase,
means for storing the ground fault phase; means for calculating the magnitude of the same phase difference current for each line and determining the maximum value; a first ground fault line selection means for calculating a zero-sequence difference current and a polarity amount to determine a ground fault line when one line at the other end is interrupted; and a constantly circulating zero-sequence current. and a second compensated ground fault line selection means for calculating a ground fault line when one line at the other end is disconnected by calculating the zero-sequence difference current and the polarity amount compensated for. A ground fault line selection relay, characterized in that the first and second fault line selection means are switched in accordance with a ground fault state. 8. In a ground fault line selection relay that protects a 1-phase ground fault accident on a 2-terminal parallel 2-line transmission line through which circulating zero-sequence current flows, means for calculating and storing the difference current between each phase current and zero-sequence current of each line; means for detecting a one-phase ground fault fault in each line; means for selecting the ground fault phase of the ground fault fault; means for storing the ground fault phase; calculated and compared with a predetermined value, and the difference as the comparison result is at least 1
Means for determining that one line at the other end is disconnected when it is larger than the phase, and a first ground fault line selection for calculating a ground fault line when one line at the other end is disconnected by calculating the zero-sequence difference current and polarity amount. and a second compensated ground fault line selection means that calculates the zero-sequence difference current that compensates for the constant circulating zero-sequence current and the polarity amount, and calculates the ground fault line when one line at the other end is not immediately disconnected. 1. A ground fault line selection relay, characterized in that said first and second fault line selection means are respectively provided and switch the respective first and second fault line selection means in response to a disconnection state of one line at the other end.
JP2034383A 1983-02-08 1983-02-08 Ground-fault channel selecting relay Granted JPS59149721A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP2034383A JPS59149721A (en) 1983-02-08 1983-02-08 Ground-fault channel selecting relay

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2034383A JPS59149721A (en) 1983-02-08 1983-02-08 Ground-fault channel selecting relay

Publications (2)

Publication Number Publication Date
JPS59149721A JPS59149721A (en) 1984-08-27
JPH0452695B2 true JPH0452695B2 (en) 1992-08-24

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Family Applications (1)

Application Number Title Priority Date Filing Date
JP2034383A Granted JPS59149721A (en) 1983-02-08 1983-02-08 Ground-fault channel selecting relay

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Country Link
JP (1) JPS59149721A (en)

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* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2558105B2 (en) * 1986-11-26 1996-11-27 日本精工株式会社 Tilt steering device with memory mechanism

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JPS59149721A (en) 1984-08-27

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