JPH019242Y2 - - Google Patents

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Publication number
JPH019242Y2
JPH019242Y2 JP11445881U JP11445881U JPH019242Y2 JP H019242 Y2 JPH019242 Y2 JP H019242Y2 JP 11445881 U JP11445881 U JP 11445881U JP 11445881 U JP11445881 U JP 11445881U JP H019242 Y2 JPH019242 Y2 JP H019242Y2
Authority
JP
Japan
Prior art keywords
zero
phase
zct
phase current
current transformer
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
JP11445881U
Other languages
Japanese (ja)
Other versions
JPS5821873U (en
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 filed Critical
Priority to JP11445881U priority Critical patent/JPS5821873U/en
Publication of JPS5821873U publication Critical patent/JPS5821873U/en
Application granted granted Critical
Publication of JPH019242Y2 publication Critical patent/JPH019242Y2/ja
Granted legal-status Critical Current

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  • Testing Of Short-Circuits, Discontinuities, Leakage, Or Incorrect Line Connections (AREA)
  • Emergency Protection Circuit Devices (AREA)

Description

【考案の詳細な説明】 一般に配電盤より制御盤までの配線で電路の電
流容量が1000Aというように大きいとき工事の容
易性からダブルまたはトリプル配線が行われる。
[Detailed explanation of the invention] Generally, double or triple wiring is used for wiring from the switchboard to the control panel for ease of construction when the current capacity of the electric line is large, such as 1000A.

例えば、第1図示のように配電盤側のバー端子
1と制御盤側のバー端子2の間でダブル配線され
ている場合、一方の分流電路に設置した零相変流
器ZCTのみで漏れ電流を測定しようとすると、
並列配線の抵抗値の違いから負荷電流がバランス
良く分流しないため、そのアンバランス分を測定
することになる。
For example, in the case of double wiring between bar terminal 1 on the switchboard side and bar terminal 2 on the control panel side as shown in the first diagram, leakage current can be controlled only by the zero-phase current transformer ZCT installed in one branch circuit. When trying to measure,
Because the load current is not shunted in a well-balanced manner due to differences in the resistance values of the parallel wiring, the unbalanced portion is measured.

実験において、良荷電流が約800Aのとき、零
相変流器ZCTに10〜15A程度の零相分が検出され
るのはそのためである。
This is why, in experiments, when the good load current is about 800 A, a zero-sequence component of about 10 to 15 A is detected in the zero-sequence current transformer ZCT.

本考案は、電路の途中において負荷電流が分流
するように並列配線されている各分流電路に零相
変流器をそれぞれ設置し、これらの零相変流器間
に零相電流負担用抵抗と、一方の零相変流器の出
力電圧の位相を他方の零相変流器の出力電圧の位
相と同相になるように調整する可変抵抗と、高調
波フイルターとを接続して、各零相変流器のばら
つきによる出力電圧の位相差を調整するととに高
調波分を減衰させることにより各分流電路からの
アンバランス電流分を相殺し、電路の漏れ電流の
みを検出することのできる漏れ電流測定装置を提
供しようとするものである。
In this invention, a zero-phase current transformer is installed in each branch circuit that is wired in parallel so that the load current is divided in the middle of the circuit, and a zero-phase current burden resistor is installed between these zero-phase current transformers. , a variable resistor that adjusts the phase of the output voltage of one zero-phase current transformer to be in phase with the phase of the output voltage of the other zero-phase current transformer, and a harmonic filter are connected, and each zero-phase By adjusting the phase difference in the output voltage due to variations in the current transformer and attenuating the harmonics, the unbalanced current from each branch circuit can be canceled out, making it possible to detect only the leakage current in the circuit. The purpose is to provide a measuring device.

以下図面第2図ないし第7図にもとずいて本考
案の実施例を説明すると、第2図において1,2
は三相電路3の途中でダブル配線された分流電
路、ZCT1,ZCT2は各分流電路1,2にそれぞれ
設置した零相変流器、R0は零相変流器ZCT1
ZCT2の二次側端子間に共通接続した零相電流負
担用抵抗、RXは一方の零相変流器ZCT1の二次側
端子間において抵抗R0と直列になるように接続
した位相調整用抵抗、Rは他方の零相変流器
ZCT2の二次側端子間において抵抗R0と直列にな
るように接続した位相用抵抗、Cは抵抗R0と並
列になるように接続した高調波フイルター、Iaは
負荷電流のアンバランス分、V0は漏れ電流出力
を示す。
Embodiments of the present invention will be described below based on FIGS. 2 to 7 of the drawings.
is a double-wired branch line in the middle of the three-phase line 3, ZCT 1 and ZCT 2 are zero-phase current transformers installed in each branch line 1 and 2, respectively, and R 0 is a zero-phase current transformer ZCT 1 ,
The zero-sequence current-bearing resistor is commonly connected between the secondary terminals of ZCT 2 , and R Adjustment resistor, R is the other zero-phase current transformer
The phase resistor is connected in series with the resistor R 0 between the secondary terminals of ZCT 2 , C is the harmonic filter connected in parallel with the resistor R 0 , Ia is the unbalanced load current, V 0 indicates leakage current output.

上記零相変流器ZCT1,ZCT2の各々の簡易等価
回路を示すと第3図のようになる。
FIG. 3 shows a simplified equivalent circuit of each of the zero-phase current transformers ZCT 1 and ZCT 2 .

ここで、上記2個の零相変流器ZCT1,ZCT2
全く同一、即ちXL1=XL2になるように製造でき
れば問題がないが、実際の製造においては無理で
あることからXL1≠XL2となる。
Here, there would be no problem if the above two zero-phase current transformers ZCT 1 and ZCT 2 could be manufactured to be exactly the same, that is, XL 1 = XL 2 , but since this is not possible in actual manufacturing, XL 1 ≠XL 2 .

零相変流器ZCT2の出力電圧V2は V2=R0Ia/n/1+R0+Rx/j×L2 となる。 The output voltage V 2 of the zero-phase current transformer ZCT 2 is V 2 =R 0 Ia/n/1+R 0 +Rx/j×L 2 .

位相調整用抵抗RXを可変させた時のV2のベク
トル軌跡は分母1+R0+Rx/JXL2の軌跡(第4図参 照)の逆図形のR0・Ia/n倍となる。
The vector locus of V 2 when the phase adjustment resistor R

また零相変流器ZCT1の出力電圧V1は軌跡は第
5図のようになる。
The trajectory of the output voltage V 1 of the zero-phase current transformer ZCT 1 is as shown in FIG.

第5図において漏れ電流出力V0はV0=V2−V1
である。
In Fig. 5, the leakage current output V 0 is V 0 = V 2V 1
It is.

位相調整用抵抗Rxを増加するように調整する
ことによりV2のベクトルはOPを直径とする半円
上を矢印方向に移動し、ある場所でV0=0とな
る。
By increasing the phase adjustment resistor Rx, the vector of V 2 moves in the direction of the arrow on a semicircle with a diameter of OP, and V 0 =0 at a certain location.

電路3に漏れ電流が発生すると、漏れ電流によ
る出力V0はベクトル的に各零相変流器ZCT1
ZCT2の出力の和となり検出することができる。
When a leakage current occurs in the electrical circuit 3, the output V 0 due to the leakage current is vectored to each zero-phase current transformer ZCT 1 ,
It becomes the sum of the outputs of ZCT 2 and can be detected.

しかし実際上は、各零相変流器ZCT1,ZCT2
鉄芯が磁性材料でできているためにそれらの二次
出力に高調波分が残りΔV0が発生する。
However, in reality, since the iron cores of each zero-phase current transformer ZCT 1 and ZCT 2 are made of magnetic material, harmonic components remain in their secondary outputs and ΔV 0 is generated.

そのため本考案は、高調波フイルターCを接続
して、高調波分を減衰させ、基本波の零相電流の
選択性を良くしてある。
Therefore, in the present invention, a harmonic filter C is connected to attenuate the harmonic component and improve the selectivity of the zero-sequence current of the fundamental wave.

以上の構成により各分流電路1,2からアンバ
ランス電流分が相殺され、電路3の漏れ電流のみ
が検出できる。
With the above configuration, the unbalanced currents from the respective branch circuits 1 and 2 are canceled out, and only the leakage current of the circuit 3 can be detected.

第6図には、本考案の別の実施例が示してあ
り、その説明すると、各分流電路1,2に設置し
た零相変流器ZCT1,ZCT2の二次側端子間に零相
電流負担用抵抗R1,R2をそれぞれ接続するとと
もに、これらの抵抗が直列になるように接続し、
一方の零相変流器ZCT1の二次側端子間において
位相調整用抵抗Rxを抵抗R1と直列に接続し、他
方の零相変流器ZCT2の出力電圧V2が一方の零相
変流器ZCT1の出力電圧V1に一致するように、即
ち第7図のベクトル図で説明すれば、OPの延長
とOCDの円との交点P′に一致するように抵抗Rx
を調整し、その後で抵抗R2に設けた中間タツプ
4により出力電圧V2が出力電圧V1と等しい出力
電圧V′2に減少するように調整し、かつ抵抗R1
R2と高調波フイルターCとを並列に設けて、漏
れ電流による出力V0を検出するように構成する。
FIG . 6 shows another embodiment of the present invention. To explain it, a zero-phase Connect the current burden resistors R 1 and R 2 respectively, and connect these resistors in series.
The phase adjustment resistor Rx is connected in series with the resistor R 1 between the secondary terminals of one zero-phase current transformer ZCT 1 , and the output voltage V 2 of the other zero-phase current transformer ZCT 2 is The resistor Rx is adjusted so as to correspond to the output voltage V 1 of the current transformer ZCT 1 , that is, to correspond to the intersection point P' of the extension of OP and the circle of OCD, as explained in the vector diagram of Fig. 7.
is adjusted so that the output voltage V 2 is reduced to an output voltage V' 2 equal to the output voltage V 1 by the intermediate tap 4 provided on the resistor R 2 , and the resistors R 1 ,
R 2 and a harmonic filter C are provided in parallel to detect the output V 0 due to leakage current.

本考案は、叙上のように構成したから電路の途
中においてダブルまたはトリプル配線された分流
電路からアンバランス電流分を相殺して電路の漏
れ電流のみを簡単に検出することができる利点を
有する。
Since the present invention is constructed as described above, it has the advantage of being able to easily detect only the leakage current in the circuit by canceling out the unbalanced current from the double or triple-wired branch circuit in the middle of the circuit.

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

第1図は三相電路の途中でダブル配線された例
を示す図、第2図は本考案に係る漏れ電流測定装
置の回路図、第3図は同装置にける各零相変流器
の等価回路図、第4図は零相変流器ZCT2の出力
電圧の位相調整用抵抗可変時におけるベクトル軌
跡を示す図、第5図は零相変流器ZCT1,ZCT2
各出力電圧のペクトル軌跡と漏れ電流出力のベク
トルの関係を示す図、第6図は本考案の変更実施
例の回路図、第7図は同実施例における各出力ベ
クトルの関係を示す図である。 1,2……分流電路、3……三相電路、ZCT1
ZCT2……零相変流器、R0……零相電流負担用抵
抗、Rx……位相調整用抵抗、R……位相用抵抗、
R1,R2……零相電流負担用抵抗、4……中間タ
ツプ、C……高調波フイルター。
Figure 1 is a diagram showing an example of double wiring in the middle of a three-phase circuit, Figure 2 is a circuit diagram of the leakage current measuring device according to the present invention, and Figure 3 is a diagram of each zero-phase current transformer in the device. Equivalent circuit diagram, Figure 4 is a diagram showing the vector trajectory when the phase adjustment resistance of the output voltage of zero-phase current transformer ZCT 2 is variable, and Figure 5 is a diagram showing each output voltage of zero-phase current transformer ZCT 1 and ZCT 2 . FIG. 6 is a circuit diagram of a modified embodiment of the present invention, and FIG. 7 is a diagram showing the relationship between each output vector in the same embodiment. 1, 2...Diversion line, 3...Three-phase line, ZCT 1 ,
ZCT 2 ... Zero-phase current transformer, R 0 ... Resistor for zero-phase current burden, Rx... Resistor for phase adjustment, R... Resistor for phase,
R 1 , R 2 ... Resistor for zero-phase current burden, 4 ... Intermediate tap, C ... Harmonic filter.

Claims (1)

【実用新案登録請求の範囲】[Scope of utility model registration request] 電路の途中において負荷電流が分流するように
並列配線されている各分流電路にそれぞれ設置す
る零相変流器の二次側端子間に、零相電流負担用
抵抗と、一方の零相変流器の出力電圧の位相を他
方の零相変流器の出力電圧の位相と同相になるよ
うに調整する可変抵抗と、高調波フイルターとを
接続して成る並列配線における漏れ電流測定装
置。
Between the secondary terminals of the zero-phase current transformers installed in each branch circuit that is wired in parallel so that the load current is divided in the middle of the circuit, a zero-phase current burden resistor and one zero-phase current transformer are installed. A device for measuring leakage current in parallel wiring, which consists of a harmonic filter and a variable resistor that adjusts the phase of the output voltage of one zero-phase current transformer to be in phase with the phase of the output voltage of the other zero-phase current transformer.
JP11445881U 1981-08-03 1981-08-03 Leakage current measuring device in parallel wiring Granted JPS5821873U (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP11445881U JPS5821873U (en) 1981-08-03 1981-08-03 Leakage current measuring device in parallel wiring

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP11445881U JPS5821873U (en) 1981-08-03 1981-08-03 Leakage current measuring device in parallel wiring

Publications (2)

Publication Number Publication Date
JPS5821873U JPS5821873U (en) 1983-02-10
JPH019242Y2 true JPH019242Y2 (en) 1989-03-14

Family

ID=29908734

Family Applications (1)

Application Number Title Priority Date Filing Date
JP11445881U Granted JPS5821873U (en) 1981-08-03 1981-08-03 Leakage current measuring device in parallel wiring

Country Status (1)

Country Link
JP (1) JPS5821873U (en)

Also Published As

Publication number Publication date
JPS5821873U (en) 1983-02-10

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