JPH0235539B2 - ITSUSENCHIRAKUKENSHUTSUKEIDENKI - Google Patents
ITSUSENCHIRAKUKENSHUTSUKEIDENKIInfo
- Publication number
- JPH0235539B2 JPH0235539B2 JP6251683A JP6251683A JPH0235539B2 JP H0235539 B2 JPH0235539 B2 JP H0235539B2 JP 6251683 A JP6251683 A JP 6251683A JP 6251683 A JP6251683 A JP 6251683A JP H0235539 B2 JPH0235539 B2 JP H0235539B2
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- Prior art keywords
- phase
- voltage
- zero
- ground fault
- line
- Prior art date
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Description
【発明の詳細な説明】
この発明は高抵抗接地系の電力系統の1線地絡
事故を検出する一線地絡検出継電器に関するもの
である。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a single line ground fault detection relay for detecting a single line ground fault in a high resistance grounding power system.
従来、この種の一線地絡検出継電器としては第
1図に示すものがある。図において1は相電圧検
出用の計器用変成器(以下PTと称する)、2−1
ないし2−3はPT2次線間電圧導入トランス、3
はPT3次零相電圧導入トランスである。4−1な
いし4−6及び5−1ないし5−4はベクトル合
成用抵抗、6は零相過電圧検出要素で入力信号を
PT3次零相電圧導入トランス3の2次側より得
る。7−1,7−2,7−3,8は矩形波変換回
路、9−1ないし9−3はNAND回路、10−
1ないし10−3は位相弁別回路、11−1ない
し11−3は夫々AND回路である。 Conventionally, there is one shown in FIG. 1 as this type of single line ground fault detection relay. In the figure, 1 is a voltage transformer for phase voltage detection (hereinafter referred to as PT), 2-1
or 2-3 is the PT secondary line voltage introduction transformer, 3
is a PT 3rd order zero-phase voltage introduction transformer. 4-1 to 4-6 and 5-1 to 5-4 are resistors for vector synthesis, and 6 is a zero-phase overvoltage detection element that receives the input signal.
Obtained from the secondary side of the PT tertiary zero-phase voltage introduction transformer 3. 7-1, 7-2, 7-3, 8 are rectangular wave conversion circuits, 9-1 to 9-3 are NAND circuits, 10-
1 to 10-3 are phase discrimination circuits, and 11-1 to 11-3 are AND circuits, respectively.
次に第1図に示した従来回路の動作について説
明する。第2図は第1図に示す従来継電器の一線
地絡検出特性図で12−1ないし12−3は夫々
第1図に示したAND回路11−1ないし11−
3の出力特性で、特性12−4は第1図の零相過
電検出要素6の出力特性を示している。また、電
圧−VAないし−VCは基準電圧で第3図にその基
準電圧−VAないし−VCの導出原理を示している。
すなわち、電圧EAB,EBC,ECAは各々線間電圧で
あつて第1図のPT12次側相電圧をPT2次線間
電圧導入トランス2−1ないし2−3で線間電圧
に変換したもので、この線間電圧に比例した合成
電流を得るためベクトル合成用抵抗4−1ないし
4−6を介して前記合成電流をベクトル合成する
ことにより第3図に示す−VAないし−VCに比例
した電気量を得るように回路構成している。つま
り、基準電圧−VAに比例した電気量はベクトル
合成用抵抗4−1,4−6により各々線間電圧
EAB,ECAをベクトル合成したもので前記基準電圧
−VB,−VCも同様にして得ることができる。次に
第2図に示した第1図のAND回路11−1ない
し11−3の出力特性12−1ないし12−3の
導出原理を第1相分について第4図に示す。この
特性12−1ないし12−3は第3図で導出した
基準電圧−VAに比例した電気量−K1VAと第1図
に示すPT1の3次回路より得た零相電圧3V0と
をPT3次零相電圧導入トランス3で受け、零相電
圧3V0に比例した出力電圧をベクトル合成用抵抗
5−1を介すことによつて導出したもので、その
ベクトル合成用抵抗5−1によつて得た−K2V0
の電気量を更にベクトル合成して−K2V0−K2V0
を得ている。そして、PT3次零相電圧導入トラン
ス3の出力よりベクトル合成用抵抗5−4を介し
て得た−K2V0の電気量との位相差θが一定値と
なるようにして軌跡を示したのが第4図に表す左
右対象の円弧である。尚、この−K2V0と−K1VA
の2つのベクトルの位相角θが規定値以上180°>
θ>90°であるときに一線地絡検出継電器から第
1図の動作出力を得る例を第5図に示した。波形
−K2V0は第1図のベクトル合成用抵抗5−4の
出力波形で波形−K2V0−K1VAは第1図の矩形波
変換回路7−1の入力波形である。この入力波形
−K2V0−K1VAを各々矩形波変換回路7−1ない
し7−3及び8を介すことによつて第5図に示し
た矩形波変換回路8及び7−1の出力信号を得
る。そしてこの2つの矩形波変換回路8及び7−
1の出力信号を第1図のNAND回路9−1に印
加することにより矩形波変換回路7−1の出力及
び矩形波変換回路8出力が両者共存在しないロー
レベル状態時のみハイレベルの出力信号を得るこ
とができる。これが第5図のNAND回路9−1
の出力波形であり、そのNAND回路9−1の出
力パルス幅は波形−K2V0及び−K2V0−K1VAの
位相が同位相の場合180°となり逆位相の場合は零
となる。したがつて、このパルス幅すなわち
NAND回路9−1の出力信号を何らかの方法に
よつて検出することにより前記−K2V0−K1VAの
2つの入力の位相角が規定値以上か否かを判定す
ることができる。第5図の波形は位相角θが規定
値以下で継電器が不動作の場合を示し、このパル
ス幅が規定値より大きくNAND回路9−1の出
力信号(H信号)をロツク信号としているため位
相弁別回路10−1の出力が送出していない。
尚、零相過電圧検出要素6はPT3次零相電圧導入
トランス3の出力信号を受け、零相電圧が規定値
以上あつた場合に動作するものであり、ストツパ
ー用として位相弁別回路10−1ないし10−3
の出力とAND回路11−1ないし11−3で使
用する。 Next, the operation of the conventional circuit shown in FIG. 1 will be explained. FIG. 2 is a single line ground fault detection characteristic diagram of the conventional relay shown in FIG. 1, and 12-1 to 12-3 are AND circuits 11-1 to 11- shown in FIG.
3, the characteristic 12-4 shows the output characteristic of the zero-sequence overcurrent detection element 6 in FIG. Further, the voltages -V A to -V C are reference voltages, and FIG. 3 shows the principle of deriving the reference voltages -V A to -V C.
That is, the voltages E AB , E BC , and E CA are each line voltages, and the PT 1 secondary phase voltage in Fig. 1 is converted into a line voltage by the PT secondary line voltage introduction transformers 2-1 to 2-3. In order to obtain a composite current proportional to this line voltage, the composite currents are vector-combined via vector combination resistors 4-1 to 4-6 to obtain -V A to -V C as shown in FIG. The circuit is configured to obtain an amount of electricity proportional to . In other words, the amount of electricity proportional to the reference voltage -V
The reference voltages -V B and -V C can be obtained in the same manner by vector synthesis of E AB and E CA. Next, the principle for deriving the output characteristics 12-1 to 12-3 of the AND circuits 11-1 to 11-3 of FIG. 1 shown in FIG. 2 is shown in FIG. 4 for the first phase. These characteristics 12-1 to 12-3 are the electrical quantity -K 1 V A proportional to the reference voltage -V A derived in Fig. 3 and the zero-sequence voltage 3 V 0 obtained from the tertiary circuit of PT1 shown in Fig. 1. is received by the PT tertiary zero-phase voltage introduction transformer 3, and an output voltage proportional to the zero-sequence voltage 3V0 is derived through the vector synthesis resistor 5-1. −K 2 V 0 obtained by 1
Further vector synthesis of the electric quantities of −K 2 V 0 −K 2 V 0
I am getting . Then, the trajectory was shown so that the phase difference θ with the electrical quantity of −K 2 V 0 obtained from the output of the PT third-order zero-phase voltage introduction transformer 3 via the vector synthesis resistor 5-4 was a constant value. This is the left-right symmetrical arc shown in FIG. Furthermore, this −K 2 V 0 and −K 1 V A
The phase angle θ of the two vectors is greater than the specified value 180°>
FIG. 5 shows an example in which the operating output shown in FIG. 1 is obtained from the single line ground fault detection relay when θ>90°. The waveform -K 2 V 0 is the output waveform of the vector synthesis resistor 5-4 in Fig. 1, and the waveform -K 2 V 0 -K 1 V A is the input waveform of the rectangular wave conversion circuit 7-1 in Fig. 1. . By passing this input waveform -K 2 V 0 -K 1 V A through the rectangular wave converting circuits 7-1 to 7-3 and 8, respectively, the rectangular wave converting circuits 8 and 7-1 shown in FIG. Obtain the output signal of And these two square wave conversion circuits 8 and 7-
By applying the output signal of 1 to the NAND circuit 9-1 in FIG. 1, the output signal becomes high level only when the output of the rectangular wave conversion circuit 7-1 and the output of the rectangular wave conversion circuit 8 are in a low level state where both are not present. can be obtained. This is the NAND circuit 9-1 in Figure 5.
The output pulse width of the NAND circuit 9-1 is 180° if the phases of the waveforms -K 2 V 0 and -K 2 V 0 -K 1 V A are in the same phase, and 0 if they are in opposite phases. becomes. Therefore, this pulse width, i.e.
By detecting the output signal of the NAND circuit 9-1 by some method, it is possible to determine whether the phase angle of the two inputs -K 2 V 0 -K 1 V A is greater than or equal to a specified value. The waveform in Figure 5 shows the case where the phase angle θ is less than the specified value and the relay is inoperable.The pulse width is larger than the specified value and the output signal (H signal) of the NAND circuit 9-1 is used as the lock signal, so the phase The output of the discrimination circuit 10-1 is not being sent.
The zero-sequence overvoltage detection element 6 receives the output signal of the PT tertiary zero-sequence voltage introducing transformer 3 and operates when the zero-sequence voltage exceeds a specified value, and is used as a stopper for the phase discrimination circuit 10-1 or 10-3
It is used with the output of AND circuits 11-1 to 11-3.
また、第6−1図の回路図は高抵抗接地系の例
における1線地絡事故時の等価回路で、13は中
性点接地抵抗(以下NGRと称す)、14は中性点
接地リアクトル(以下NGLと称す)、15はケー
ブル系送電線の対地静電容量(以下対地容量と称
す)、16は故障点抵抗、EAは発電機誘起電圧、
Zgは背後インピーダンスである。前記第6−1
図は対象座標法における等価回路で置き換えると
第6−2図の如くとなる。更に背後インピーダン
スZgは無視可能なためこれを省略すると第6−
3図となる。 In addition, the circuit diagram in Figure 6-1 is an equivalent circuit in the event of a single-line ground fault in an example of a high-resistance grounding system, where 13 is a neutral point grounding resistor (hereinafter referred to as NGR), and 14 is a neutral point grounding reactor. (hereinafter referred to as NGL), 15 is the ground capacitance of the cable system transmission line (hereinafter referred to as ground capacity), 16 is the fault point resistance, E A is the generator induced voltage,
Zg is the back impedance. Said No. 6-1
If the diagram is replaced with an equivalent circuit in the object coordinate method, it will become as shown in Figure 6-2. Furthermore, since the rear impedance Zg can be ignored, if this is omitted, the 6th -
Figure 3 is shown.
又、同地点における2線地絡事故を表わすと第
7−1図となる。これを第6図と同様にして対象
座標法における等価回路で置き変えると第7−2
図の如くなり、更に簡略化すれば第7−3図のよ
うに表わすことができる。ここで前述の第6−3
図と第7−3図の零相電圧V0を比較すると明ら
かにそのV0の大きさ及び位相に差異があり前記、
零相電圧V0のベクトルは故障点抵抗16の大き
さRFによつて左右されることがわかる。前記の
様子を第8図及び第9図に示す。まず、第8図は
A相1線地絡事故時の零相電圧−V0のベクトル
軌跡であり第6−3図の故障点抵抗3RFを零か
ら無限大の大きさまで変化させた場合であり、第
9図はBC相の同地点2線地絡事故時の零相電圧
−V0のベクトル軌跡で、第7−3図の故障点抵
抗RFを零から無限大まで変化させた場合を表わ
している。したがつて継電器の動作範囲としては
第10図に示す様に1線地絡事故時の零相電圧−
V0の軌跡17−1、又は17−2を検出できる
ように特性12−1のようにすることが必要であ
る。一方、同地点2線地絡事故時の零相電圧−
V0ベクトル軌跡は第9図の如くであるためこれ
を誤検出しないようにしなければならない。しか
し、継電器の特性は第2図に示すように各相の基
準電圧VA,VB,VCに対して円弧となるようにな
つているため、例えば、BC相の2線地絡事故で
あれば継電器のB相又はC相の特性範囲内に零相
電圧−V0のベクトルが入つてくる可能性がある
ことであり、この性能限界が1線地絡検出継電器
としての性能の良否を決定してしまうことにな
る。この様子を第11図に示す。第11図はBC
相の2線地絡事故の場合であり電圧三角形はEA,
EB,ECとなりBC相の線間電圧が低下する。基準
電圧VA,VB,VCは線間電圧よりベクトル合成し
て得たものであるから電圧三角形の重心点零より
三角形の頂点に向いた位相となり大きさもそれに
比例したものとなる。したがつて継電器の特性1
2−1,12−2,12−3も第11図の如く基
準電圧VA,VB,VCに対する円弧となりB相の特
性12−2とC相の特性12−3は線間電圧EBC
の大きさに応じ互いに接近してくることになる。
したがつて上記線間電圧EBCが一定以下となれば
特性12−2と12−3は重なつてしまい2線地
絡事故でも動作することになるので、従来はこの
対策として第1図では図示してないが、線間電圧
が一定値以下でロツクする方法あるいは2相が動
作した場合は出力信号を出さないように回路に工
夫をこらしている。 Figure 7-1 shows a two-wire ground fault accident at the same location. If we replace this with the equivalent circuit in the object coordinate method in the same way as in Figure 6, we will see 7-2.
If it is further simplified, it can be expressed as shown in Fig. 7-3. Here, the above-mentioned 6-3
Comparing the zero-sequence voltage V 0 in Figure 7-3 and Figure 7-3, there is clearly a difference in the magnitude and phase of V 0 as described above.
It can be seen that the vector of the zero-sequence voltage V 0 is influenced by the magnitude RF of the fault point resistance 16. The above situation is shown in FIGS. 8 and 9. First, Figure 8 shows the vector locus of the zero-sequence voltage -V 0 at the time of an A-phase 1-wire ground fault, and shows the vector locus of the zero-sequence voltage -V 0 when the fault point resistance 3RF in Figure 6-3 is varied from zero to infinity. , Figure 9 shows the vector locus of the zero-sequence voltage -V 0 at the same point two-wire ground fault of the BC phase, and represents the case where the fault point resistance RF in Figure 7-3 is varied from zero to infinity. ing. Therefore, as shown in Figure 10, the operating range of the relay is zero-sequence voltage -
It is necessary to have the characteristic 12-1 so that the trajectory 17-1 or 17-2 of V 0 can be detected. On the other hand, the zero-sequence voltage at the time of a two-wire ground fault accident at the same point -
Since the V 0 vector locus is as shown in FIG. 9, it is necessary to avoid erroneously detecting this. However, as shown in Figure 2, the characteristics of the relay are arcuate with respect to the reference voltages V A , V B , and V C of each phase. If so, there is a possibility that the zero-sequence voltage -V 0 vector will enter the characteristic range of the B-phase or C-phase of the relay, and this performance limit determines the quality of the performance as a one-wire ground fault detection relay. It will be decided. This situation is shown in FIG. Figure 11 is BC
In the case of a phase two-wire ground fault, the voltage triangle is E A ,
E B and E C , and the line voltage of the BC phase decreases. Since the reference voltages V A , V B , and V C are obtained by vector synthesis from the line voltages, the phases are directed from the center of gravity zero of the voltage triangle to the apex of the triangle, and the magnitude is proportional thereto. Therefore, characteristics of relay 1
2-1, 12-2, and 12-3 are also circular arcs with respect to the reference voltages V A , V B , and V C as shown in FIG. B.C.
They will move closer to each other depending on the size of the .
Therefore, if the line voltage E BC falls below a certain level, characteristics 12-2 and 12-3 will overlap and it will operate even in the event of a two-wire ground fault. Although not shown, the circuit is devised so that it locks when the line voltage is below a certain value, or so that no output signal is output when two phases are activated.
このように従来の一線地絡検出継電器の第1の
欠点は第10図で既述のように1線地絡事故時の
電力変換部−V0ベクトルを確実に検出できるよ
うにするためには円弧を相当大きくとらなければ
ならず、第11図の特性12−2と12−3が重
畳する限界の線間電圧EBCを相当大きくすること
であり、換言すれば線間電圧低下検出ロツク値を
高くすることで、前記ロツク要素に頼らない範囲
が狭くなることである。次に従来の一線地絡検出
継電器の第2の欠点は例えばB相至近端C相遠方
端のような異地点2線地絡事故の場合でこの時に
は零相電圧−V0の位相が大きく変化することに
なり、この様子を第11図のベクトルOFで示し
ている。つまり、前記の線間電圧低下検出ロツク
要素が応動しない程度に線間電圧が残つたケース
であれば全面的に本来の位相特性12−2及び、
12−3で判別しなればならないが、この場合に
は継電器の特性12−2及び12−3の動作範囲
が広いので異支点2線地絡事故に対しては大変具
合が悪い。 In this way, the first drawback of the conventional one-line ground fault detection relay is that, as already mentioned in Fig. 10, in order to be able to reliably detect the power converter -V 0 vector in the event of a one-line ground fault, The arc must be made considerably large, and the limit line voltage E BC at which characteristics 12-2 and 12-3 in Fig. 11 overlap must be made considerably large.In other words, the line voltage drop detection lock value By increasing the value, the range in which the locking element is not relied on becomes narrower. Next, the second drawback of the conventional one-line ground fault detection relay is in the case of a two-wire ground fault at different points, such as at the close end of phase B and the far end of phase C. In this case, the phase of the zero-sequence voltage -V 0 is large. This is shown by the vector OF in FIG. 11. In other words, in the case where the line voltage remains to such an extent that the line voltage drop detection lock element does not respond, the original phase characteristic 12-2 and
12-3, but in this case, the operating range of the relay characteristics 12-2 and 12-3 is wide, so it is very difficult to handle a two-wire ground fault at different supports.
従来の1線地絡検出継電器はその動作範囲は第
2図に示す中心点Oを通る円弧となり、その円弧
の大きさは1線地絡事故時のV0ベクトル軌跡よ
りは充分大きくなる必要があり、そのため至近端
2線地絡事故で誤動作を起すという欠点があつ
た。 The operating range of a conventional one-wire ground fault detection relay is an arc passing through the center point O shown in Figure 2, and the size of the arc needs to be sufficiently larger than the V 0 vector locus at the time of a one-wire ground fault. As a result, there was a drawback that malfunctions could occur due to a two-wire ground fault at the close end.
本発明は上記の欠点を除去するためになされた
もので、従来の継電器が至近端2線地絡事故時に
誤動作する改善策として線間電圧低下検出要素を
特別に設けず、かつ、電圧ロツク要素との感度
的、時間的な協調が不要な一線地絡検出継電器を
提供することを目的とする。 The present invention was made in order to eliminate the above-mentioned drawbacks, and as a measure to improve the malfunction of conventional relays in the event of a close-end two-wire ground fault, the present invention does not require a special line-to-line voltage drop detection element, and has a voltage lock function. The purpose of the present invention is to provide a single line ground fault detection relay that does not require sensitivity or time coordination with elements.
以下本発明の一実施例を図について説明する。
図中第1図と同一の部分は同一の符号をもつて図
示した第12図において、19−1ないし19−
3は移相回路用抵抗、20−1ないし20−3は
移相回路用コンデンサである。 An embodiment of the present invention will be described below with reference to the drawings.
In FIG. 12, the same parts as in FIG. 1 are designated by the same reference numerals.
3 is a resistor for the phase shift circuit, and 20-1 to 20-3 are capacitors for the phase shift circuit.
次に本発明の動作について以下に説明する。第
13図は本発明の継電器の特性図を示したもの
で、図中特性12−1は本発明は継電器の特性で
あり従来の特性図は第10図で既述のように1線
地絡事故時の零相電圧−V0の軌跡を包む大きさ
の円弧となつている。一方第13図の特性12−
4は従来と同じで第12図の零相過電圧検出要素
6の特性を表わし地絡事故に対する検出感度を決
定するために設けている。また従来の特性を示す
第4図と異なる点は基準電圧のとり方で、従来の
基準電圧が第3図で示すように線間電圧より合成
した相電圧と同位相の電気量を取り出していたの
に比し本発明では線間電圧EBCを90°移相したもの
をK1EBC<90°として利用している。その具体的な
例を示したのが第12図のトランス2−1ないし
2−3でPT1の2次線間電圧に比例した電圧を
導出している。そして前記の導出された電圧を移
相回路用抵抗19−1ないし19−3、及び移相
回路用コンデコサ20−2ないし20−3にて適
当な進み電流に変換し、前記移相回路用コンデン
サ20−1ないし20−3と前記PT2次線間電圧
導入トランス2−1ないし2−3の中間タツプの
間に発生する電圧を取り出すことで各々90°遅れ
の電圧移相としている。このようにして導出した
基準電圧K1EBC<90°及び零相電圧−K2V0をベク
トル合成した電気量と零相電圧−K2V0の相互位
相角θとを一定となるように作図したのが第13
図の円弧である。すなわち、第12図のベクトル
合成用抵抗4−2の出力はA相(第1相)の基準
電圧として利用するものでPT1の2次線間電圧
EBCに比例し、これを90°遅らせたK1EBC<90°であ
り、このA相の相電圧とは逆位相関係にある。同
様にしてベクトル合成用抵抗4−3,4−1の出
力信号は各々B相(第2相)、C相(第3相)の
基準電圧となり、B相用はK1ECA<90°、C相用は
K1EAB<90°となる。上記夫々の基準電圧とPT3次
零相電圧導入トランス3を介してベクトル合成用
抵抗5−1ないし5−3より導出した零相電圧−
K2V0を各相毎にベクトル合成すればA相は−
K2V0+K1EBC<90°、B相は−K2V0+K1ECA<
90°、C相は−K2V0+K1EAB<90°となり、これを
各々パルス波形変換回路7−1ないし7−3に導
入しパルス波形に変換する。さらにベクトル合成
用抵抗5−4の出力−K2V0を矩形波変換回路8
でパルス変換したものと前記のパルスの立下りま
での時間を測定すれば第13図のような円弧特性
が得られることは従来例と同一である。 Next, the operation of the present invention will be explained below. Fig. 13 shows a characteristic diagram of the relay of the present invention. In the figure, characteristic 12-1 is the characteristic of the relay of the present invention, and the conventional characteristic diagram is shown in Fig. It is an arc with a size that encompasses the locus of the zero-sequence voltage -V 0 at the time of the accident. On the other hand, characteristic 12- in Fig. 13
4, which is the same as the conventional one, represents the characteristics of the zero-sequence overvoltage detection element 6 shown in FIG. 12, and is provided to determine the detection sensitivity for ground faults. What is different from Figure 4, which shows the conventional characteristics, is the way the reference voltage is taken.The conventional reference voltage extracts the amount of electricity in the same phase as the phase voltage synthesized from the line voltage, as shown in Figure 3. In contrast, in the present invention, the line voltage E BC is phase-shifted by 90° and used as K 1 E BC <90°. A specific example of this is shown in FIG. 12, where transformers 2-1 to 2-3 derive a voltage proportional to the secondary line voltage of PT1. Then, the derived voltage is converted into an appropriate leading current by the phase shift circuit resistors 19-1 to 19-3 and the phase shift circuit capacitors 20-2 to 20-3, and the phase shift circuit capacitor By extracting the voltage generated between the intermediate taps of the PT secondary line voltage introduction transformers 20-1 to 20-3 and the PT secondary line voltage introducing transformers 2-1 to 2-3, the voltage phase is shifted by 90 degrees. The mutual phase angle θ of the electric quantity obtained by vector synthesis of the reference voltage K 1 E BC <90° and the zero-sequence voltage −K 2 V 0 derived in this way and the zero-sequence voltage −K 2 V 0 is kept constant. The 13th drawing was drawn in
This is the arc in the figure. In other words, the output of the vector synthesis resistor 4-2 in Fig. 12 is used as the reference voltage of phase A (first phase), and is the secondary line voltage of PT1.
K 1 E BC is proportional to E BC and delayed by 90 degrees, so that K 1 E BC <90 degrees, and has an antiphase relationship with the phase voltage of the A phase. Similarly, the output signals of the vector synthesis resistors 4-3 and 4-1 become reference voltages for phase B (second phase) and phase C (third phase), respectively, and for phase B, K 1 E CA <90° , for C phase
K 1 E AB <90°. The zero-sequence voltage derived from the vector synthesis resistors 5-1 to 5-3 via the respective reference voltages and the PT tertiary zero-sequence voltage introduction transformer 3.
If K 2 V 0 is vector-combined for each phase, the A phase is -
K 2 V 0 +K 1 E BC <90°, B phase is −K 2 V 0 +K 1 E CA <
90°, and the C phase is −K 2 V 0 +K 1 E AB <90°, which are respectively introduced into pulse waveform conversion circuits 7-1 to 7-3 and converted into pulse waveforms. Furthermore, the output of the vector synthesis resistor 5-4 -K 2 V 0 is converted into a rectangular wave conversion circuit 8.
As in the conventional example, if the time from the pulse conversion to the fall of the pulse is measured, an arc characteristic as shown in FIG. 13 can be obtained.
次に従来の継電器の欠点とされていた至近端2
線地絡事故での誤動作対策として本発明の実施例
を下記に説明する。すなわち、高抵抗接地系の1
線地絡事故では事故相の電圧は通常低下するが線
間電圧は健全時と同じ3相平衡三角形である事は
周知の通りである。したがつて、1線地絡事故時
における本発明継電器の基準電圧は前述の通りA
相はEBC<90°に比例し、B相はECA<90°、C相は
EAB<90°に各々比例するようにしているため第1
3図に示す特性となる。しかし2線地絡の場合に
は事故相の相電圧と共に線間電圧も低下するので
零相電圧−3V0は第9図で既述のように1線地絡
事故時とは逆位相方向となる。この時の本発明継
電器の特性変化をBC相2線地絡事故の例で、第
14図に示した。まず、A相の基準電圧K1EBC<
90°の位相は1線地絡事故時と同じくA相の相電
圧と逆位相方向で大きさは事故点によつて変わり
至近端事故であれば零となる。次にB相の基準電
圧K1ECA<90°及びC相の基準電圧K1EAB<90°は
各々BC相の線間電圧が低下するにつれて相互の
位相角が広がり、BC相の線間電圧が零になれば
180°となり、大きさも、√3/2まて小さくな
る。これは継電器の円弧特性の基準となる基準電
圧が2線地絡事故時の線間電圧低下に伴ないその
時発生する零相電圧−3V0のベクトルより離れて
いくことを意味し、継電器としては従来のものと
丁度反対に線間電圧が低下すればするほど動作範
囲が狭くなる。そして動作範囲自体が2線地絡事
故時の零相電圧ベクトル存在から遠くなるので、
至近端2線地絡事故時に誤動作することがなくな
る。 Next, the closest end 2, which was considered a drawback of conventional relays.
Embodiments of the present invention will be described below as a countermeasure against malfunctions caused by line-to-ground faults. In other words, 1 of the high resistance grounding system
In a line-to-ground fault, the voltage of the faulty phase usually decreases, but it is well known that the line voltage is the same three-phase balanced triangle as in normal conditions. Therefore, the reference voltage of the relay of the present invention at the time of a one-wire ground fault is A as described above.
The phase is proportional to E BC <90°, the B phase is proportional to E CA <90°, and the C phase is proportional to E BC <90°.
Since E AB < 90°, the first
The characteristics are shown in Figure 3. However, in the case of a two-wire ground fault, the line voltage decreases as well as the phase voltage of the faulted phase, so the zero-sequence voltage -3V 0 is in the opposite phase direction from that in the case of a one-wire ground fault, as described in Figure 9. Become. The characteristic changes of the relay of the present invention at this time are shown in Fig. 14 as an example of a BC phase two-wire ground fault accident. First, the A-phase reference voltage K 1 E BC <
The 90° phase is in the opposite phase direction to the A-phase voltage as in the case of a single-wire ground fault, and its magnitude varies depending on the fault point and will be zero if it is a near-end fault. Next, for the B-phase reference voltage K 1 E CA <90° and the C-phase reference voltage K 1 E AB <90°, the mutual phase angle widens as the BC-phase line voltage decreases, and the BC-phase line If the voltage between
It becomes 180°, and the size becomes smaller by √3/2. This means that the reference voltage, which is the basis for the arc characteristic of the relay, moves away from the zero-sequence voltage -3V 0 vector that occurs at that time due to the drop in line voltage at the time of a two-wire ground fault, and as a relay, Just the opposite of the conventional system, the lower the line voltage, the narrower the operating range becomes. And since the operating range itself becomes far from the existence of the zero-sequence voltage vector at the time of a two-wire ground fault,
This eliminates malfunctions in the event of a ground fault in two wires at the close end.
なお、上記実施例では基準電圧に線間電圧を
90°移相した値を使用しているが前記の基準電圧
に微小の零相電圧成分を加味し基準電圧の原点を
移動させる事により円弧特性の中心点を適当に移
動させたオフセツト付円弧特性としてもよい。 Note that in the above embodiment, the line voltage is used as the reference voltage.
Although a value shifted by 90° is used, a minute zero-sequence voltage component is added to the reference voltage mentioned above, and the center point of the arc characteristic is appropriately moved by moving the origin of the reference voltage.Circular characteristic with offset You can also use it as
以上のように本発明によれば1線地絡事故では
継電器の特性は従来と変わらず、また2線地絡事
故では事故相の線間電圧が低下するのでそれにつ
れて動作範囲が狭くなる様に回路構成したので、
至近端2線地絡事故対策としての特別な回路を改
めて設ける必要もなく安価かつ確実に動作する高
性能な一線地絡検出継電器を提供できる効果があ
る。 As described above, according to the present invention, the characteristics of the relay remain unchanged in a one-wire ground fault accident, and the operating range becomes narrower as the line voltage of the faulty phase decreases in a two-wire ground fault fault. After configuring the circuit,
This has the effect of providing a high-performance one-line ground fault detection relay that operates reliably at low cost without the need to newly provide a special circuit as a countermeasure against two-wire ground faults at the close end.
第1図は従来の一線地絡検出継電器のブロツク
回路図、第2図は第1図の検出特性図、第3図な
いし第11図は従来及び本発明を説明するための
補足説明図、第12図は本発明の一実施例を示す
一線地絡検出継電器の原理回路図、第13図及び
第14図は本発明による零相位相特性図の例であ
る。
1……計器用変成器、2−1ないし2−3……
PT2次線間電圧導入トランス、3……PT3次零相
電圧導入トランス、4−1ないし4−6,5−1
ないし5−4……ベクトル合成用抵抗、6……零
相過電圧検出要素、7−1ないし7−3,8……
矩形波変換回路、9−1ないし9−3……
NAND回路、10−1ないし10−3……位相
弁別回路、11−1ないし11−3……AND回
路、19−1ないし19−3……移相回路用抵
抗、20−1なし20−3……移相回路用コンデ
ンサ。なお、図中同一符号は同一又は相当部分を
示す。
Fig. 1 is a block circuit diagram of a conventional single line ground fault detection relay, Fig. 2 is a detection characteristic diagram of Fig. 1, Figs. 3 to 11 are supplementary explanatory diagrams for explaining the conventional one and the present invention, FIG. 12 is a principle circuit diagram of a single line ground fault detection relay showing an embodiment of the present invention, and FIGS. 13 and 14 are examples of zero-phase phase characteristic diagrams according to the present invention. 1...Instrument transformer, 2-1 to 2-3...
PT secondary line voltage introduction transformer, 3...PT tertiary zero-phase voltage introduction transformer, 4-1 to 4-6, 5-1
or 5-4... Resistor for vector synthesis, 6... Zero-phase overvoltage detection element, 7-1 or 7-3, 8...
Square wave conversion circuit, 9-1 to 9-3...
NAND circuit, 10-1 to 10-3...Phase discrimination circuit, 11-1 to 11-3...AND circuit, 19-1 to 19-3...Resistance for phase shift circuit, 20-1 without 20-3 ...Capacitor for phase shift circuit. Note that the same reference numerals in the figures indicate the same or equivalent parts.
Claims (1)
器の2次線間電圧に比例した電気量を90°移相し
て得る各相毎の基準電圧と、前記計器用変成器の
3次巻線より導出した該計器用変成器の3次零相
電圧と、前記基準電圧及び計器用変成器の3次零
相電圧とを各相毎にベクトル合成した電気量とし
て得る各相毎の第1の電気量と、前記計器用変成
器の3次零相電圧に比例した第2の電気量と、前
記第1の電気量と前記第2の電気量との位相差を
検出する位相弁別回路とを備えた一線地絡検出継
電電器。1 A reference voltage for each phase obtained by phase-shifting the quantity of electricity proportional to the secondary line voltage of the instrument transformer that detects the phase voltage of the AC power transmission system, and the tertiary winding of the instrument transformer. The first electrical quantity for each phase is obtained by vector-synthesizing the tertiary zero-sequence voltage of the instrument transformer derived from the line, the reference voltage, and the tertiary zero-sequence voltage of the instrument transformer for each phase. a second quantity of electricity proportional to the tertiary zero-sequence voltage of the instrument transformer; and a phase discrimination circuit that detects a phase difference between the first quantity of electricity and the second quantity of electricity. A single line ground fault detection relay equipped with
Priority Applications (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6251683A JPH0235539B2 (en) | 1983-04-08 | 1983-04-08 | ITSUSENCHIRAKUKENSHUTSUKEIDENKI |
Applications Claiming Priority (1)
| Application Number | Priority Date | Filing Date | Title |
|---|---|---|---|
| JP6251683A JPH0235539B2 (en) | 1983-04-08 | 1983-04-08 | ITSUSENCHIRAKUKENSHUTSUKEIDENKI |
Publications (2)
| Publication Number | Publication Date |
|---|---|
| JPS59188329A JPS59188329A (en) | 1984-10-25 |
| JPH0235539B2 true JPH0235539B2 (en) | 1990-08-10 |
Family
ID=13202419
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP6251683A Expired - Lifetime JPH0235539B2 (en) | 1983-04-08 | 1983-04-08 | ITSUSENCHIRAKUKENSHUTSUKEIDENKI |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JPH0235539B2 (en) |
Families Citing this family (1)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| JPS6074922A (en) * | 1983-09-29 | 1985-04-27 | 三菱電機株式会社 | One-line ground-fault voltage detecting relay |
-
1983
- 1983-04-08 JP JP6251683A patent/JPH0235539B2/en not_active Expired - Lifetime
Also Published As
| Publication number | Publication date |
|---|---|
| JPS59188329A (en) | 1984-10-25 |
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