JPH0223025A - Distance relay - Google Patents

Distance relay

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Publication number
JPH0223025A
JPH0223025A JP16781188A JP16781188A JPH0223025A JP H0223025 A JPH0223025 A JP H0223025A JP 16781188 A JP16781188 A JP 16781188A JP 16781188 A JP16781188 A JP 16781188A JP H0223025 A JPH0223025 A JP H0223025A
Authority
JP
Japan
Prior art keywords
amount
output
circuit
polarity
relay
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.)
Pending
Application number
JP16781188A
Other languages
Japanese (ja)
Inventor
Masuo Nakajima
益雄 中島
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
Toshiba Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Toshiba Corp filed Critical Toshiba Corp
Priority to JP16781188A priority Critical patent/JPH0223025A/en
Publication of JPH0223025A publication Critical patent/JPH0223025A/en
Pending legal-status Critical Current

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Abstract

PURPOSE:To discriminate between inner fault and outer fault reliably by limiting the period of polarity amount corresponding to the system voltage below a predetermined value and judging the overlap angle between the polarity amount and an electrical amount obtained through combination of voltage and current. CONSTITUTION:Output K2V from an auxiliary transformer 1 is connected with a polarity amount circuit 3 in order to obtain a polarity amount VP, while output K1I from an auxiliary current transformer 2 is combined with the output K2V to produce an operational amount K1I-K2V. The polarity amount VP and the operational amount K1I-K2V are converted through conversion circuits 4, 5 into square waves. The VP converted into square wave and a signal limited 8 within 180 deg. are employed for inhibition 9. The operational amount K1I-K2V converted into a square wave and the output from the inhibit circuit 9 are fed to an AND gate 6 in order to detect overlap of the polarity amount VP and the operational amount K1I-K2V thus judging whether they are overlapped more than 90 deg. through a time measuring circuit 7. By such arrangement, duration of DC transient component produced from the auxiliary transformer 1 is limited resulting in prevention of erroneous function.

Description

【発明の詳細な説明】 〔発明の目的〕 (産業上の利用分野) 本発明は保護継電器、特に誤動作防止対策を施した保護
継電器に関する。
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention] (Industrial Application Field) The present invention relates to a protective relay, and particularly to a protective relay with measures to prevent malfunction.

(従来の技術) 第5図は従来の電力系統保護用距離継電器の一種である
モー形継電器の概要図であり、第6図は第5図の動作説
明のための各部波形図である。このモー形継電器の動作
原理の概要を説明する。
(Prior Art) FIG. 5 is a schematic diagram of a Moh type relay, which is a type of conventional power system protection distance relay, and FIG. 6 is a waveform diagram of each part for explaining the operation of FIG. An overview of the operating principle of this Moh type relay will be explained.

送電線の電圧、電流に比例した交流電圧V、及び交流電
流■が大々モー形継電器の補助変圧器1及び補助変流器
2に導入され、■に比例した電気tK v、及び■に比
例した電気量に1 Iが得られる、補助変圧器1の出力
は極性量回路3に導入され、KVと同位相でK 2 V
に比例したV、なる極性量を出力する。ス、KIとに2
vの合成電気量に11−に2Vが動作量として用いられ
、継電器の動作判定が行なわれる。この様にして得相差
が90゛以内であるか否かが判定される。
An alternating current voltage V proportional to the voltage and current of the power transmission line, and an alternating current The output of the auxiliary transformer 1 is introduced into the polarity circuit 3, and the output of the auxiliary transformer 1 is introduced into the polarity circuit 3, and the output of the auxiliary transformer 1 is in the same phase as KV
Outputs a polarity amount of V, which is proportional to . Su, KI and 2
2V is used as the operation amount in the combined electricity amount of v, and the operation of the relay is determined. In this way, it is determined whether the gain phase difference is within 90°.

即ち、■ 及びK  I−に2Vが夫々方形波変換回路
4.5に導入されて方形波(V、)’及び(K  I−
に2V) ′となり、次段のアンド回路6に導入される
。アンド回路6では(V、)’と(K  T−に2V)
’とが共に「1」である時に−に2V)’が時間測定回
路7によって時間測定が行なわれ、90゛以上であれば
モー形継電器は勤生状態となる。
That is, 2V is introduced into the square wave converting circuit 4.5 to ■ and K I-, respectively, and the square waves (V, )' and (K I-
2V)' and is introduced into the AND circuit 6 at the next stage. In AND circuit 6, (V,)' and (K T- 2V)
The time measurement circuit 7 measures the time of -2V) when both 1 and 1 are 1, and if it is 90 degrees or more, the Moo-type relay is in a working state.

第7図は以上の動作を説明するベクトル図で、電流■に
対する電圧Vの動作限界を示す。即ち、■、とに11 
 K2 Vなる電気量の位相差は第7図のθで表わされ
、この位相差θが90°以内であれば動作し、従って第
7図の円内が動作域となる。
FIG. 7 is a vector diagram illustrating the above operation, and shows the operating limit of voltage V with respect to current {circle around (2)}. That is, ■, Toni 11
The phase difference between the electric quantities K2 V is represented by θ in FIG. 7, and if this phase difference θ is within 90°, the device will operate, and therefore the operating range will be within the circle in FIG.

第8図は一般的に両端に電源P s 、P Rがある送
電源りの電源P8端に第5図と同様なモー形継電器8を
適用したものである。潮流はP、端側からPR端へ流れ
ているものとする。送電線■5のA点での故障、即ち、
内部故障ではモー形継電器8は前述の様な動作を行ない
動作状態となる。ス、B点での故障、即ち、外部至近点
故障では第9図の各部波形に示す様に電圧Vが零となり
、これに伴ない極性量V、も零となることから、モー形
継電器は不動作となる。
In FIG. 8, a Moo type relay 8 similar to that shown in FIG. 5 is applied to the power source P8 end of a transmission power source, which generally has power sources P s and P R at both ends. Assume that the current is P, flowing from the end side to the PR end. Failure at point A of power transmission line ■5, i.e.
In the event of an internal failure, the Moh type relay 8 operates as described above and becomes operational. In the case of a failure at point B or point B, that is, an external close point failure, the voltage V becomes zero as shown in the waveforms of each part in Figure 9, and the polarity V also becomes zero, so the Moh type relay It becomes inactive.

即ち、内部故障では動作、外部故障では不動作となるの
が正常な応動である。
In other words, the normal response is to operate in case of an internal failure, but not to operate in case of an external failure.

(発明が解決しようとする課題) しかし、周知の様に第5図に示した1a電器の補助変圧
81は入力電圧■が無となっても、2次側の出力V′は
完全に零とはならず、過渡直流分を発生する。これにつ
いて第10図の補助変圧器の等価回路を用いて説明する
。先ず、故障前には入力電圧■により励磁インピーダン
スZ、に励磁電流が流れて励磁エネルギーが蓄えられて
いる。ところが、入力電圧Vが瞬時に零になると、この
vjJ磁インピーダンスZ1−に蓄えられていた励磁エ
ネルギーが矢印のように2次側に放出されるために2次
側出力v′は瞬時には零にならず、第11図に示す様に
過渡直流分■1が発生する。
(Problem to be Solved by the Invention) However, as is well known, in the auxiliary transformer 81 of the 1A electric appliance shown in FIG. This will generate a transient DC component. This will be explained using the equivalent circuit of the auxiliary transformer shown in FIG. First, before a failure occurs, an excitation current flows through the excitation impedance Z due to the input voltage ■, and excitation energy is stored. However, when the input voltage V instantaneously becomes zero, the excitation energy stored in this vjJ magnetic impedance Z1- is released to the secondary side as shown by the arrow, so the secondary side output v' instantaneously becomes zero. Instead, a transient DC component (1) occurs as shown in FIG.

この補助変圧器1が発生する過渡直流分V□が従来のモ
ー形継電器の応動に悪影響を及ぼし外部故障で誤動作と
ならしめる。
The transient DC component V□ generated by the auxiliary transformer 1 adversely affects the response of the conventional MoW type relay, causing it to malfunction due to an external failure.

即ち、第8図の送電線のB点で事故が発生すると前述の
様に電圧Vが零になるが、補助変圧器1の出力V′は直
ちに零とはならず、前述の過渡直流分■1が残る。この
状態でのモー形継電器旦の応動は第12図のようになる
。即ち、極性量V−よ補助変圧器1の出力に2Vに所定
の係数を乗じたものだからに2vに比例した波形となる
。補助変圧器1の出力に2vは事故発生後しばらく過渡
直流分が残っているため極性NVpは第12図のように
なる。
That is, when an accident occurs at point B of the power transmission line in Fig. 8, the voltage V becomes zero as described above, but the output V' of the auxiliary transformer 1 does not immediately become zero, and the transient DC component 1 remains. The response of the motor type relay in this state is as shown in FIG. That is, since the polarity amount V- is the output of the auxiliary transformer 1 multiplied by 2V by a predetermined coefficient, the waveform becomes proportional to 2V. Since the 2V transient DC component remains in the output of the auxiliary transformer 1 for a while after the accident occurs, the polarity NVp becomes as shown in FIG.

ス、事故電流■は潮流とは逆向きだから第12図のよう
に事故時に反転する。この事故電流■が前述したKVに
比べ充分大きく、K2Vの影響を無視できるとK  I
−に2Vは第12図のようになす る。
The fault current ■ is in the opposite direction to the current, so it reverses at the time of an accident as shown in Figure 12. If this fault current ■ is sufficiently large compared to the KV mentioned above and the influence of K2V can be ignored, then K I
- and 2V are set as shown in Fig. 12.

これらを方形波に変換すると(V、)’は過渡直流分が
残っている間連続゛1”となっており、(K  I−に
2V> ハ180°の期間だけ“1”となっている。し
たがって、アンド回路6の出力vANDは1サイクルご
とに180°の方形波出力となって、時間測定回路7の
出力、即ち、モー形継電器の出力V。、tは、1サイク
ルに1回の誤出力を生ずることになる。
When these are converted into square waves, (V, )' remains ``1'' continuously while the transient DC component remains, and remains ``1'' only during the period of 180° (2V in K I-). Therefore, the output vAND of the AND circuit 6 becomes a 180° square wave output for each cycle, and the output of the time measuring circuit 7, that is, the output V. This will result in erroneous output.

以上のように、従来のモー形継電器はその補助変圧器が
発生ずる過渡直流分によって、外部故障では本来は不動
作であるべきところが誤動作するという欠点があった。
As described above, the conventional Moh type relay has the drawback that the transient DC component generated by the auxiliary transformer causes the malfunction of a part that should not normally operate in the event of an external failure.

以上においては継電器の補助変圧器で不具合現象を説明
したが、コンデンサ形計器用変圧器回路でも類似の現象
が生じ得る。
Although the malfunction phenomenon has been explained above with respect to the auxiliary transformer of the relay, a similar phenomenon may also occur in the capacitor-type voltage transformer circuit.

これは、モー形継電器の基本的な応動である方向判別機
能が失われるという、根本的な欠点でもあった。
This was also a fundamental drawback in that the direction discrimination function, which is the basic response of the Moh-type relay, was lost.

本発明は上記欠点を解決するためになされたものであり
、継電器の補助変圧器の発生する過渡直流分によって誤
動作することのない距M@j、電器を提供することを目
的としている。
The present invention has been made to solve the above-mentioned drawbacks, and an object of the present invention is to provide an electric appliance with a distance M@j that does not malfunction due to the transient DC component generated by the auxiliary transformer of the relay.

〔発明の構成〕[Structure of the invention]

(課題を解決するための手段) 上記目的を達成するため、本発明では電力系統からの電
圧に対応した極性UV、と、電力系統からの電圧と電流
とを合成した電気量<K、T−に2■)の重なり角が所
定の値以内か否かを判定する距Mi!1!電器において
、極性量Vpの周期を所定の値以下に制限する回路を設
けるよう構成した。
(Means for Solving the Problems) In order to achieve the above object, the present invention uses polarity UV corresponding to the voltage from the power system, and the amount of electricity <K, T- Distance Mi! to determine whether the overlapping angle of (2) is within a predetermined value. 1! The electric appliance is configured to include a circuit that limits the period of the polarity amount Vp to a predetermined value or less.

(作 用) 極性量の周期を制限することにより、継電器の補助変圧
器から発生する過渡直流分のIl!続時開時間気角で1
80°相当に制限でき、継電器の誤動作を防止できる。
(Function) By limiting the period of the polarity amount, the transient DC component Il! generated from the auxiliary transformer of the relay is reduced. Continuation opening time 1
It can be limited to the equivalent of 80 degrees, preventing relay malfunctions.

(実施例) 以下図面を参照して実施例を説明する。(Example) Examples will be described below with reference to the drawings.

第1図は本発明によるモー形継電器の一実施例を示すブ
ロック図である。第1図において、補助変圧器1の出力
が極性量回路3に接続されて極性K 2 Vが得られ、
方形波変換回路5に導入されることは第5図の場合と同
様である。方形波変換回路4の出力は次段のインしビッ
ト回路9の入力端子、及び時間測定回路8に導入され、
更に時間測定回路8の出力は前記インしビット回路9の
インしビット端子に導入される。
FIG. 1 is a block diagram showing an embodiment of a Moh type relay according to the present invention. In FIG. 1, the output of the auxiliary transformer 1 is connected to the polarity circuit 3 to obtain the polarity K 2 V,
The introduction into the square wave conversion circuit 5 is the same as in the case of FIG. The output of the square wave conversion circuit 4 is introduced into the input terminal of the next-stage input bit circuit 9 and the time measurement circuit 8,
Furthermore, the output of the time measuring circuit 8 is introduced into the in/out bit terminal of the in/out bit circuit 9.

ス、前記動作量K  I−に2Vも方形波変換回路5に
導入される。そして方形波変換回路5とインしビット回
路9の各出力はアンド回路6、及び時間測定回路7にて
動作判定が行なわれ継電器出力を得る。なお、第5図と
第1図で同一符号のものは同様の■きをするものである
2V is also introduced into the square wave conversion circuit 5 to the operating amount K I-. Then, each output of the bit circuit 9 inputted to the square wave conversion circuit 5 is subjected to an operation judgment in an AND circuit 6 and a time measuring circuit 7 to obtain a relay output. Components with the same reference numerals in FIG. 5 and FIG. 1 have the same symbol.

次に本発明による(−形継電器の作用を説明する。Next, the operation of the negative type relay according to the present invention will be explained.

第2図は第1図に示した本発明のモー形@電器の動作を
説明する各部波形であり、第12図で示した従来のモー
形継電器と同様な事故状態、即ち、第8図の送電線りの
B点はおける外部事故が発生した場合の動作を示す。前
述の様に、モー形継電器設置点の背後至近点外部で事故
が発生すると送電線のリレー設置点の電圧は零となる。
FIG. 2 shows waveforms of various parts to explain the operation of the Moh type electric appliance of the present invention shown in FIG. Point B on the power transmission line shows the behavior when an external accident occurs. As mentioned above, if an accident occurs outside the closest point behind the Moh type relay installation point, the voltage at the relay installation point on the power transmission line becomes zero.

しかし継電器の補助変圧器1の出力は完全に零にならず
、過渡直流分が発生するため仁第2図のに2vのように
なる。又、故障後電流■は潮流とは反転しているので、
動作量K  I−に2Vは第2図のような波形となる。
However, the output of the auxiliary transformer 1 of the relay does not become completely zero, and because a transient DC component is generated, the output becomes 2V as shown in Figure 2. Also, since the post-failure current ■ is the opposite of the power flow,
When the operating amount K I- is 2V, a waveform as shown in FIG. 2 is obtained.

したがって、第2図のように動作量(K  I−に2V
)は方形波変換回路5によつて方形波に変換され、1サ
イクル毎に180°の方形波出力となる。
Therefore, as shown in Fig. 2, the operating amount (K I- is 2V
) is converted into a square wave by the square wave conversion circuit 5, and a 180° square wave is output for each cycle.

ところが極性量vpの過渡直流分による方形波変換回路
4の出力は直流分が発生している間遠続「1」出力であ
る。
However, the output of the square wave conversion circuit 4 due to the transient DC component of the polarity vp is a long-duration "1" output while the DC component is generated.

は時間測定回路8へ導入される。時間測定回路8では入
力が“0”から“1”へなった時点から所定の時間経過
後出力が“1”となる、いわゆる限時動作回路であり、
ここでは限時時間を入力の半周期に相当する電気角表現
で180°相当にしている。そのため第2図に示すよう
に定常時の時間測定回路8の出力■ は“O”であり入
力<v、)’が連続“1”となってから180゛相当の
時間経過後に連続“1″となるう時間測定回路8の出力
v2は後段のインヒビット回路9の禁止入力となってい
るので、■2が“0″のときインしビット回路のもう一
つの入力である(V、)’が“1″ならば、インしビッ
ト回路出力は“1”、禁止人力v2が“IHならばイン
ヒビット回路9の出力■1は常に“0″であるため、イ
ンヒビット回路9の出力V、は第2図に示すようになる
is introduced into the time measuring circuit 8. The time measurement circuit 8 is a so-called time-limited operation circuit in which the output becomes "1" after a predetermined time has elapsed since the input changed from "0" to "1".
Here, the time limit is expressed as an electrical angle equivalent to 180°, which corresponds to a half cycle of the input. Therefore, as shown in Fig. 2, the output of the time measuring circuit 8 in steady state is "O", and after the input <v, )' becomes continuous "1", it becomes continuous "1" after a time equivalent to 180゛ has elapsed. The output v2 of the time measuring circuit 8 is an inhibit input to the inhibit circuit 9 in the subsequent stage, so when ■2 is "0", it is input and the other input of the bit circuit (V, )' is If it is “1”, the input bit circuit output is “1”, and if the inhibit power v2 is “IH”, the output of the inhibit circuit 9 is always “0”, so the output V of the inhibit circuit 9 is the second The result will be as shown in the figure.

このインヒビット回路9の出力V[と、動作量がAND
回路6でANDをとられるので、その出力は第2回に示
すVAN、となり、これの時間幅が電気角相当で90°
以上あるか否かを時間測定回路7で測定するが、(V、
)’の連続“1”出力の影響は時間測定回路8の出力V
、にて消されているので誤動作することはない。即ち、
外部故障時に補助変圧器1で発生する過渡直流分による
誤動作は防止できることになる。
The output V[ of this inhibit circuit 9 and the operating amount are AND
Since the AND is performed in circuit 6, the output is VAN shown in the second part, and the time width of this is equivalent to 90 degrees in electrical angle.
The time measurement circuit 7 measures whether or not the voltage is higher than or equal to (V,
)' continuous "1" output influences the output V of the time measurement circuit 8.
, so there will be no malfunction. That is,
Malfunctions due to transient DC components generated in the auxiliary transformer 1 at the time of external failure can be prevented.

なお、距離継電器では一般に送電線のインピーダンス角
を考慮してその角度分だけ継電器内部で電流Iの位相を
進めており、動作を速めるために交流電気量の正半波、
及び負半波に大々別々の方形波変換回路、アンド回路等
を使用しているが、これまでの説明においては説明を簡
単にするためにこれらを省略して述べたが、負波に対し
ても同様に考え得ることは勿論である。
In addition, in distance relays, the phase of current I is generally advanced within the relay by that angle in consideration of the impedance angle of the transmission line, and in order to speed up the operation, the positive half wave of the AC quantity of electricity,
Separate square wave conversion circuits, AND circuits, etc. are used for the negative half wave and negative half wave, but these have been omitted in the explanation so far to simplify the explanation, but for the negative wave Of course, it can be considered in the same way.

このように極性量が入力される方形波変換回路4の出力
を180°以内に抑えることにより、外部故障時におけ
る誤動作を防止できる利点がある。
By suppressing the output of the square wave conversion circuit 4 to which the polarity is input within 180 degrees in this way, there is an advantage that malfunctions can be prevented in the event of an external failure.

なお、本案の実施例においては、iJ電器内の補助変圧
器の過渡直流分及びP、)ランジェントによる作用効果
を記述したが、これとは別に入力回路にフィルタを用い
た継電器においてフィルタにより発生する過渡トランジ
ェントに対しても、本発明一実施例を適用することがで
きる。他の実棒例としては以下は示すものが考えられる
In addition, in the embodiment of this proposal, we have described the effects caused by the transient DC component and P, ) transient of the auxiliary transformer in the iJ electric appliance, but separately from this, we have described the effect caused by the transient DC component of the auxiliary transformer in the iJ electric appliance. An embodiment of the present invention can also be applied to transients that occur. Other examples of actual rods include those shown below.

(a)上記実施例では補助変圧器1の過渡直流分の幅を
制限する回路として時間測定回路8とインヒビット回路
9で説明したが、本発明はこれに限定されるものではな
い。例えば第3図に示すようにワンショットパルス回路
10とAND回路6−1組合せでも同様の効果が期待で
きる。
(a) In the above embodiment, the time measurement circuit 8 and the inhibit circuit 9 have been described as circuits that limit the width of the transient DC component of the auxiliary transformer 1, but the present invention is not limited thereto. For example, as shown in FIG. 3, a similar effect can be expected by combining the one-shot pulse circuit 10 and the AND circuit 6-1.

(b)更に、上記実施例では継電器に入力する電圧。(b) Furthermore, in the above embodiment, the voltage input to the relay.

電流は同じ相(例えばR相)を基本に説明した。The explanation has been made based on the assumption that the current is in the same phase (for example, R phase).

しかし、本発明はこれに限定されるものではない。例え
ば三相回路の特徴を生かしR相の保護@1電器としてS
T相の電圧を入力し、90°移相した電気量を極性量と
して用いても同様の効果が期待できる。
However, the present invention is not limited thereto. For example, taking advantage of the characteristics of a three-phase circuit, protection of the R phase @1 S as an electric appliance
A similar effect can be expected by inputting the T-phase voltage and using the amount of electricity phase-shifted by 90° as the polarity amount.

この実施例を第4図に示す。第4図において11は90
°移相回路を示す。
This embodiment is shown in FIG. In Figure 4, 11 is 90
° Phase shift circuit is shown.

〔発明の効果〕〔Effect of the invention〕

以上説明した如く、本発明によればa電器の補助変圧器
などに過渡直流分が発生した場合でも、。
As explained above, according to the present invention, even when a transient DC component occurs in an auxiliary transformer of an electric appliance,

外部故障時に誤動作することなく簡単な装置を付加する
だけで、確実に内部事故、外部事故の判別が行なえる距
離継電器を提供できる。
It is possible to provide a distance relay that can reliably distinguish between internal and external accidents by simply adding a simple device without malfunctioning when an external failure occurs.

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

第1図は本発明による距離継電器の一実施例の構成図、
第2図は第1図に示す距離a電器の外部至近f4事故に
対する応動を示す図、第3図は過渡直流分の幅を制限す
るための他の実施例の構成図、第4図は本発明による更
に他の実施例の構成図、第5図は従来の距離継電器の梢
或例図、第6図は第5図に示す距離継電器の内部事故に
対する応動を示す図、第7図は動作特性図、第8図は電
力系統に距離継電器を適用した図、第9図は外部至近点
事故に対する応動を示す波形図、第10図は補助変圧器
の等価回路、第11図は過渡直流分の発生を示す図、第
12図は第5図に示した従来の距離継電器の外部至近点
事故等の応動を示す波形図である。 1・・・補助変圧器 3・・・極性量回路 6・・・アンド回路 9・・・インヒビット回路 2・・・補助変流器 4.5・・・方形波変換回路 7.8・・・時間測定回路
FIG. 1 is a configuration diagram of an embodiment of a distance relay according to the present invention;
Fig. 2 is a diagram showing the response to an external close f4 accident of the distance a electric appliance shown in Fig. 1, Fig. 3 is a configuration diagram of another embodiment for limiting the width of the transient DC component, and Fig. 4 is a diagram of the present invention. A block diagram of still another embodiment according to the invention, FIG. 5 is a top view of a conventional distance relay, FIG. 6 is a diagram showing the response to an internal accident of the distance relay shown in FIG. 5, and FIG. 7 is an operation diagram. Characteristics diagram, Figure 8 is a diagram of applying a distance relay to a power system, Figure 9 is a waveform diagram showing the response to an external close point fault, Figure 10 is an equivalent circuit of an auxiliary transformer, and Figure 11 is a transient DC component. FIG. 12 is a waveform diagram showing the response of the conventional distance relay shown in FIG. 5 to an external close point accident. 1... Auxiliary transformer 3... Polarity circuit 6... AND circuit 9... Inhibit circuit 2... Auxiliary current transformer 4.5... Square wave conversion circuit 7.8... time measurement circuit

Claims (1)

【特許請求の範囲】[Claims] 電力系統からの電圧に対応した極性量V_pと、電力系
統からの電圧と電流とを合成した電気量(K_1I−K
_2V)の重なり角が所定の値以内か否かを判定する距
離継電器において、前記極性量V_pの周期を所定の値
以下に制限する回路を備えたことを特徴とする距離継電
器。
The polarity amount V_p corresponding to the voltage from the power system and the amount of electricity (K_1I-K
What is claimed is: 1. A distance relay that determines whether an overlapping angle of _2V) is within a predetermined value, comprising a circuit that limits the period of the polarity amount V_p to a predetermined value or less.
JP16781188A 1988-07-07 1988-07-07 Distance relay Pending JPH0223025A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP16781188A JPH0223025A (en) 1988-07-07 1988-07-07 Distance relay

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP16781188A JPH0223025A (en) 1988-07-07 1988-07-07 Distance relay

Publications (1)

Publication Number Publication Date
JPH0223025A true JPH0223025A (en) 1990-01-25

Family

ID=15856545

Family Applications (1)

Application Number Title Priority Date Filing Date
JP16781188A Pending JPH0223025A (en) 1988-07-07 1988-07-07 Distance relay

Country Status (1)

Country Link
JP (1) JPH0223025A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100322386B1 (en) * 1998-08-19 2002-06-20 최 균 용 Anchor plate for improvement of soft ground.

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100322386B1 (en) * 1998-08-19 2002-06-20 최 균 용 Anchor plate for improvement of soft ground.

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