JPH01112169A - Optical zero-phase current detector - Google Patents

Optical zero-phase current detector

Info

Publication number
JPH01112169A
JPH01112169A JP62271299A JP27129987A JPH01112169A JP H01112169 A JPH01112169 A JP H01112169A JP 62271299 A JP62271299 A JP 62271299A JP 27129987 A JP27129987 A JP 27129987A JP H01112169 A JPH01112169 A JP H01112169A
Authority
JP
Japan
Prior art keywords
zero
optical
tertiary
sequence current
current
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP62271299A
Other languages
Japanese (ja)
Other versions
JPH07104380B2 (en
Inventor
Masao Otsuka
正雄 大塚
Kozo Yukanami
床並 孝三
Hideki Saito
秀樹 斉藤
Koichi Hori
浩一 堀
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.)
Yaskawa Electric Corp
Original Assignee
Yaskawa Electric Manufacturing Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Yaskawa Electric Manufacturing Co Ltd filed Critical Yaskawa Electric Manufacturing Co Ltd
Priority to JP62271299A priority Critical patent/JPH07104380B2/en
Publication of JPH01112169A publication Critical patent/JPH01112169A/en
Publication of JPH07104380B2 publication Critical patent/JPH07104380B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Landscapes

  • Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)

Abstract

(57)【要約】本公報は電子出願前の出願データであるた
め要約のデータは記録されません。
(57) [Summary] This bulletin contains application data before electronic filing, so abstract data is not recorded.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、零相電流を高感度で信頼性高く検出するため
の、光式零相電流検出器に関する。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to an optical zero-sequence current detector for detecting zero-sequence current with high sensitivity and reliability.

〔従来の技術〕[Conventional technology]

非接地系の送配電線路に地絡事故が生じたときには、線
路の浮遊静電容量に起因して微弱な零相電流が流れる。
When a ground fault occurs in an ungrounded power transmission/distribution line, a weak zero-sequence current flows due to the stray capacitance of the line.

この微弱な零相電流を検出するために、零相電流検出装
置が必要となる。
In order to detect this weak zero-sequence current, a zero-sequence current detection device is required.

従来の高圧非接地系の送配電線路に用いる零相電流検出
装置としては、零相変流器(ZCT)が:千とんどであ
った。
Zero-phase current transformers (ZCTs) have been used as zero-phase current detection devices for conventional high-voltage ungrounded power transmission and distribution lines.

しかし、高圧架空配電線路のように三相電線の線間距離
が離れているため、ZCTが使用しにくい場合や、大容
量になって、大面積の貫通導体と相間絶縁のためZCT
が大型になる場合がある。
However, in some cases, such as in high-voltage overhead distribution lines, where the three-phase wires are far apart, it is difficult to use ZCT, or when the capacity is large, ZCT is used due to the large area of through conductors and interphase insulation.
may become large.

このような場合においては、精度はZCTiご比・へ1
若干劣るものの、そのコンノ々クト性、相間絶縁の容易
さから、3個0CT(変流器)を用いた3 CT方式が
用いられることがある。
In such cases, the accuracy is 1 to 1 compared to ZCTi.
Although slightly inferior, a 3CT system using three 0CTs (current transformers) is sometimes used because of its connectivity and ease of interphase insulation.

3CTで三相回路の零相電流を測る方法としては、第5
図に示す二次残留回路方式と、第6図(こ示す三次零相
分路方式とがある。
The fifth method for measuring the zero-sequence current of a three-phase circuit with a 3CT is
There is a secondary residual circuit system shown in FIG. 6, and a tertiary zero-phase shunt system shown in FIG.

二次残留回路方式は、一般に400A以下に用(1られ
、第5図に示すように、三相の電線21a、 21b。
The secondary residual circuit system is generally used for applications below 400A, and as shown in FIG. 5, three-phase electric wires 21a and 21b are used.

21Cのそれぞれに、各々単一のコアを一次回路として
これに二次巻線を施した変成器22a、 22b、 2
2cを装着し、負担23によってこれらの並列回路を短
絡した構成である。この方式においては、二次零相電流
成分は負担23を通る電流(。2として現れ、その電流
も。2の大きさは、各変成器22a、 22b、 22
cの二次巻線数をNターンとすると、−吹雪相電流の1
/Nになる。ただし、各変成器22a、 22b、 2
2cは貫通型CTとして、それらの−次側巻線は1ター
ンとする。この二次巻線数Nは二次正相分電流で決まる
が、この電流は通常5Aであるので、−次定格電流が4
00Aの場合はN−80ターンとなる。
21C, each transformer 22a, 22b, 2 each has a single core as a primary circuit and a secondary winding thereon.
2c is attached, and these parallel circuits are short-circuited by a load 23. In this scheme, the secondary zero-sequence current component appears as a current (.2) passing through the burden 23, and the magnitude of the current also
If the number of secondary windings of c is N turns, -1 of the snowstorm phase current
/N becomes. However, each transformer 22a, 22b, 2
2c is a through-type CT, and the negative side winding thereof has one turn. The number of secondary windings N is determined by the secondary positive sequence current, and since this current is normally 5A, the -order rated current is 4
In the case of 00A, it becomes N-80 turns.

たとえばZCTの特性を規定する一次零相電流が200
+++ Aの場合、二次零相電流to2は200/80
 =2.5mAしか流れない。−次定格電流がさらに大
きくなると、二次正相分電流が5A一定であるから、二
次巻数はさらに大きくなり、したがって二次零相電流t
02はますます小さくなる。
For example, if the primary zero-sequence current that defines the characteristics of ZCT is 200
+++ In the case of A, the secondary zero-sequence current to2 is 200/80
= Only 2.5mA flows. - When the secondary rated current becomes larger, the secondary positive sequence current is constant at 5A, so the number of secondary turns becomes larger, and therefore the secondary zero-sequence current t
02 becomes smaller and smaller.

このため、一般に400A以上の大電流を検出する場合
には、第6図に示す三次零相分路方式が用いられる。こ
の方式は、三相の電線31a、 31b、 31cのそ
れぞれに、各々単一のコアを一次回路としてこれに二次
巻線33a、 33b、 33c及び三次巻線34a、
34b。
Therefore, when detecting a large current of 400 A or more, a three-order zero-phase shunt system shown in FIG. 6 is generally used. In this method, three-phase electric wires 31a, 31b, and 31c each have a single core as a primary circuit, and are connected to secondary windings 33a, 33b, and 33c, and tertiary windings 34a,
34b.

34Cを施した変成器32a、 32b、 32cを装
着したものである。そして、二次巻線33a、 33b
、 33c は正相分の各相電流をキャンセルするため
に両端が短絡され、三次巻線34a、 34b、 34
c の直列回路には負担35が接続されている。
34C transformers 32a, 32b, and 32c are installed. And secondary windings 33a, 33b
, 33c are short-circuited at both ends to cancel the positive phase currents, and the tertiary windings 34a, 34b, 34
A load 35 is connected to the series circuit of c.

この第6図の方式においては、正相分のキャンセル用の
二次巻数回路とは無関係に三次巻線34a。
In the method shown in FIG. 6, the tertiary winding 34a is independent of the secondary winding circuit for canceling the positive phase component.

34b、 34c に零相成分を流すことができるため
、三次巻線34a、 34b、 34c の巻数は自由
に選定できる。
Since the zero-phase component can flow through 34b and 34c, the number of turns of the tertiary windings 34a, 34b, and 34c can be freely selected.

そのため、三次巻線34a、 34b、 34c の巻
数を少なくすれば、三次零相電流t。3としては、さほ
ど小さくならず、比較的大きな零相電流出力を得ること
ができる。しかし、巻数をどんどん小さくしても、1タ
ーン以下にはできないため、原理的に、−吹雪相電流以
上には増幅することはできない。
Therefore, if the number of turns of the tertiary windings 34a, 34b, and 34c is reduced, the tertiary zero-sequence current t. 3, it is not so small and a relatively large zero-sequence current output can be obtained. However, even if the number of turns is gradually reduced, it cannot be reduced to less than one turn, and therefore, in principle, the current cannot be amplified to more than the -blizzard phase current.

たとえば、ZCTの特性を規定している一次零相電流が
200m Aの場合、三次零相出力としては、200m
 A以上にはなり得ないことになる。この対策として、
三次巻線34a、 34b、 34c の負担用抵抗3
5の両端に発生ずる零相電流に比例した電圧を、出力信
号として見る方法も考えられるが、この出力電圧を大き
くするには負担用抵抗を大きくし、且つ三次巻線回路の
電流を大きくしなければならない。
For example, if the primary zero-sequence current that defines the characteristics of ZCT is 200mA, the tertiary zero-sequence output is 200mA.
This means that it cannot be higher than A. As a countermeasure for this,
Resistor 3 for burden of tertiary windings 34a, 34b, 34c
One possible method is to view the voltage proportional to the zero-sequence current generated across the terminals of 5 as an output signal, but in order to increase this output voltage, the burden resistor must be increased and the current in the tertiary winding circuit must be increased. There must be.

このため、三次巻線34a、 34b、 34c の巻
数を増し、コアサイズも太き(することが必要となるが
、これには、実用上、限度があった。
For this reason, it is necessary to increase the number of turns of the tertiary windings 34a, 34b, and 34c and to increase the core size, but there is a practical limit to this.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

このように、−法王相電流が大きくなってくると、零相
電流を測定する方法としては、三次零相分路方式が非常
に有効になってくるが、この方式の欠点としては、三次
巻線に電流が流れるため、二次分路電流が生じ、変流比
が変動し、正確な零相電流を測定できないという問題が
ある。
In this way, as the −Positive phase current increases, the tertiary zero-sequence shunt method becomes very effective as a method for measuring the zero-sequence current, but the disadvantage of this method is that the tertiary winding Since current flows through the line, a secondary shunt current occurs, the current transformation ratio fluctuates, and there is a problem that accurate zero-sequence current cannot be measured.

また、異相地絡時のように、極めて大きな一次零相電流
が流れる場合、三次巻線にもそれに比例した大きな電流
が流れるため、巻線寸法も大きくなる。さらに、電磁力
も加わるため、巻線の機械的支持も堅固にする必要があ
るという欠点があった。
Furthermore, when an extremely large primary zero-sequence current flows, such as in the case of a different-phase ground fault, a proportionately large current also flows in the tertiary winding, resulting in a large winding size. Furthermore, since electromagnetic force is also applied, there is a drawback that the mechanical support of the windings must also be strong.

本発明は、このような従来の問題点に鑑みてなされたも
のであり、零相電流を高感度で信頼性高く検出すること
を目的とする。
The present invention has been made in view of such conventional problems, and an object of the present invention is to detect zero-sequence current with high sensitivity and high reliability.

〔問題点を解決するための手段〕[Means for solving problems]

この目的を達成するため、本発明の光式零相電流検出器
は、三相の送配電線路のそれぞれに環状の鉄心を配置し
、各鉄心に二次巻線及び三次巻線を巻回した変成器を設
け、これらの変成器の二次残留回路の負担として抵抗を
接続するとともに、前記各相の三次巻線を直列に接続し
、該直列回路の両端子間に電圧センサを設けて零相電流
に比例した電圧を検出する手段を備えたことを特徴とす
る。
In order to achieve this objective, the optical zero-phase current detector of the present invention has an annular iron core placed on each of the three-phase power transmission and distribution lines, and a secondary winding and a tertiary winding wound around each iron core. A transformer is provided, a resistor is connected as a load for the secondary residual circuit of these transformers, the tertiary windings of each phase are connected in series, and a voltage sensor is provided between both terminals of the series circuit to obtain a zero voltage. It is characterized by comprising means for detecting a voltage proportional to the phase current.

この電圧センサとしては、ポッケルス素子のように、電
界によって媒質の屈折率が異なる電気光学結晶素子を用
いることにより、外界のノイズに影響されない信号抽出
が可能となる。
As this voltage sensor, by using an electro-optic crystal element, such as a Pockels element, in which the refractive index of the medium changes depending on the electric field, signal extraction that is not affected by external noise becomes possible.

〔作用〕[Effect]

本発明は、前記の構成であるから、三相−次導体である
一次巻線に零相分が含まれず、かつ3個の変成器の変成
比が等しい場合は、二次電流の和は零となる。したがっ
て、この場合には、二次残留回路に接続された負担用抵
抗の両端に電圧を生じず、三次巻線にも電圧は誘起され
ず、電圧センサは動作しない。
Since the present invention has the above-described configuration, if the primary winding, which is a three-phase-order conductor, does not include a zero-phase component and the transformation ratios of the three transformers are equal, the sum of the secondary currents is zero. becomes. Therefore, in this case, no voltage is generated across the burden resistor connected to the secondary residual circuit, no voltage is induced in the tertiary winding, and the voltage sensor does not operate.

一方、変成器の一次巻線に零相電流が流れると、この変
成器の二次残留回路に、零相電流に比例した電流が流れ
、この二次残留回路の両端に接続された負担用抵抗には
、発生した零相電流に比例した電圧が発生ずる。この電
圧は三次巻線で電圧増幅され、電圧センサの両端に電圧
出力として取り出される。電圧センサを電気光学結晶素
子のような誘電体で構成すると、三次回路に三次零相電
流を流さずに電圧出力が取り出される。このため、三次
巻線を増やせば容易に大きな電圧出力として取り出せ、
しかも三次巻線には電流が流れないため、前述の三次零
相分路方式の欠点が全て除かれる。すなわち、三次巻線
は単位長さ当たりの抵抗の大きな極細線が巻けるため、
多数回巻回しても大きな寸法にならず、また負担も小さ
くできる。
On the other hand, when a zero-sequence current flows through the primary winding of a transformer, a current proportional to the zero-sequence current flows through the secondary residual circuit of this transformer, and the burden resistor connected to both ends of this secondary residual circuit flows. , a voltage proportional to the generated zero-sequence current is generated. This voltage is amplified by the tertiary winding and output as a voltage across the voltage sensor. When the voltage sensor is constructed of a dielectric material such as an electro-optic crystal element, a voltage output can be obtained without passing a tertiary zero-sequence current to the tertiary circuit. Therefore, if you increase the number of tertiary windings, you can easily obtain a large voltage output.
Moreover, since no current flows through the tertiary winding, all the drawbacks of the tertiary zero-phase shunt method described above are eliminated. In other words, the tertiary winding can be wound with extremely thin wire that has a high resistance per unit length.
Even if it is wound many times, the size does not become large and the load can be reduced.

このため、コアサイズも小さくなり、コンパクトな高感
度aCT方式が実現できる。
Therefore, the core size becomes smaller, and a compact high-sensitivity aCT method can be realized.

〔実施例〕〔Example〕

以下、本発明を図面に示す実施例に基づいて具体的に説
明する。
Hereinafter, the present invention will be specifically described based on embodiments shown in the drawings.

第1図は、本発明の実施例の構成を示すブロック図であ
る。同図において、1は光を送出する光送信器、2及び
3は光ファイバを用いた光送信路及び光受信路、5は信
号処理回路、6は表示装置である。7は消弧性ガスを封
入した開閉器であり、器内に三相の送配電線路のそれぞ
れに接続する開閉電極7a、 7b、 7cが収納され
ている。8,9.10は変成器であり、開閉器電極7a
、 7b、 7cのそれぞれに前記電極を囲んで配置し
た環状の鉄心8a、 9a。
FIG. 1 is a block diagram showing the configuration of an embodiment of the present invention. In the figure, 1 is an optical transmitter that sends out light, 2 and 3 are optical transmission paths and optical reception paths using optical fibers, 5 is a signal processing circuit, and 6 is a display device. 7 is a switch filled with arc-extinguishing gas, and switching electrodes 7a, 7b, and 7c connected to three-phase power transmission and distribution lines are housed inside the switch. 8, 9.10 is a transformer, switch electrode 7a
, 7b, 7c, annular iron cores 8a, 9a are disposed surrounding the electrodes, respectively.

10aが設けられ、これらの鉄心8a、 9a、 10
a に、それぞれの変成器8,9.10の変成比が等し
くなるように、二次巻線8b、 9b、 10b及び三
次巻線3c。
10a are provided, and these iron cores 8a, 9a, 10
a, the secondary windings 8b, 9b, 10b and the tertiary winding 3c such that the transformation ratios of the respective transformers 8, 9, 10 are equal.

9c、 IOCが巻回されている。前記二次巻線8b、
 9b。
9c, IOC is wound. the secondary winding 8b;
9b.

10b には、負担用抵抗11を並列に接続し、二次巻
線3c、 9c、 IOCは互いに直列に接続して、両
側の端子を光電圧センサ12の電極にそれぞれ接続して
いる。この光電圧センサ12には、ポッケルス素子のよ
うな電界動作型素子、例えばLiTa0.、、 LiN
bO3゜KDP(KN、PO,)、 BGO(Bi、2
Ge12o)、 B50(Bi、2Si02o)等の強
誘電体系の材料が主として用いられる。
A load resistor 11 is connected in parallel to 10b, and the secondary windings 3c, 9c, and IOC are connected in series, and the terminals on both sides are connected to the electrodes of the optical voltage sensor 12, respectively. This optical voltage sensor 12 includes an electric field operated element such as a Pockels element, for example LiTa0. ,, LiN
bO3゜KDP (KN, PO,), BGO (Bi, 2
Ferroelectric materials such as Ge12o) and B50 (Bi, 2Si02o) are mainly used.

この光電圧センサ12を用いた電圧検出システムを第2
図に示す。IAはパルス発生器であり、その出力パルス
は電気−光変換素子IBにより光パルスに変換され、光
ファイバを用いた光送信路2を介して光電圧センサ12
に与えられる。これらのパルス発生器IA及び電気−光
変換素子IBは、前記光送信器1内に設けられている。
The voltage detection system using this optical voltage sensor 12 is
As shown in the figure. IA is a pulse generator, and its output pulses are converted into optical pulses by an electro-optical conversion element IB, and sent to an optical voltage sensor 12 via an optical transmission path 2 using an optical fiber.
given to. These pulse generator IA and electro-optical conversion element IB are provided within the optical transmitter 1.

光電圧センサ12は、端面に透明電極14.14を有す
る電界動作型素子13゜偏光子15.  !/1波長板
16及び検光子17より構成されている。透明電極14
.14は、第1図の三次巻線3c。
The optical voltage sensor 12 includes an electric field-operated element 13 having a transparent electrode 14.14 on its end face, and a polarizer 15. ! It is composed of a /1 wavelength plate 16 and an analyzer 17. Transparent electrode 14
.. 14 is the tertiary winding 3c in FIG.

9c、 10c の直列回路の両端と、電気的に接続さ
れている。検光子17からの光出力は、光ファイバを用
いた光受信路3を介して、光−電気変換素子を備えた光
受信器4に伝達され、電気信号に変換されて信号処理回
路5に送られる。
It is electrically connected to both ends of the series circuit of 9c and 10c. The optical output from the analyzer 17 is transmitted via an optical receiving path 3 using an optical fiber to an optical receiver 4 equipped with an optical-to-electrical conversion element, where it is converted into an electrical signal and sent to a signal processing circuit 5. It will be done.

次に、第1図のブロック図の動作について説明する。開
閉器7の開閉電極7a、 7b、 7cに接続された送
配電線路(図示せず)に正常に通電しているときは、変
成器8.9.10の二次巻線8b、 9b、 101]
にそれぞれ誘起された二次電流の和が零となるから、負
担用抵抗11の両端には電圧は生じず、三次巻線3c、
 9c、 IOCに電圧は生じない。したがって、光送
信器1から光送信路2に送信された連続光は、電圧が印
加されていない光電圧センサ12を透過して光受信路3
から光受信器4に出力される。光受信器4は光信号を電
気信号に変換して信号処理回路5に出力する。信号処理
回路5は人力した電気信号を増幅して信号処理を行って
表示装置6に出力する。
Next, the operation of the block diagram in FIG. 1 will be explained. When the power transmission and distribution lines (not shown) connected to the switching electrodes 7a, 7b, 7c of the switch 7 are normally energized, the secondary windings 8b, 9b, 101 of the transformer 8.9.10 ]
Since the sum of the secondary currents induced in each becomes zero, no voltage is generated across the burden resistor 11, and the tertiary windings 3c,
9c, no voltage is generated at IOC. Therefore, the continuous light transmitted from the optical transmitter 1 to the optical transmission path 2 passes through the optical voltage sensor 12 to which no voltage is applied, and passes through the optical receiving path 2.
The signal is output from the optical receiver 4 to the optical receiver 4. The optical receiver 4 converts the optical signal into an electrical signal and outputs it to the signal processing circuit 5. The signal processing circuit 5 amplifies the manually generated electrical signal, performs signal processing, and outputs the signal to the display device 6.

第3図は送配電線路が正常に通電されているときの検出
信号の特性図を示すもので、縦軸に出力を、横軸に時間
をとると、検出信号は水平な信号特性となる。
FIG. 3 shows a characteristic diagram of the detection signal when the power transmission and distribution line is normally energized, and when the vertical axis is the output and the horizontal axis is the time, the detection signal has a horizontal signal characteristic.

次に、送配電線路の1相が地絡し、開閉器7の開閉電極
7aに零相電流が流れると、この開閉電極7aに設けた
変成器8の二次巻線8bに二次電流及び二次電圧が発生
し、他の開閉電極7b、 7cに設けた変成器9.10
の二次巻線9b、 10bのそれぞれに同一の二次電圧
が印加され、それぞれの変成器8,9゜10の三次巻線
8c、 9c、 10c に検出電圧が誘起される。こ
れらの変成器8,9.10の三次巻線8c、 9c。
Next, when one phase of the power transmission and distribution line has a ground fault and a zero-sequence current flows through the switching electrode 7a of the switch 7, a secondary current and A transformer 9.10 in which a secondary voltage is generated and provided on the other switching electrodes 7b, 7c
The same secondary voltage is applied to each of the secondary windings 9b, 10b, and a detection voltage is induced in the tertiary windings 8c, 9c, 10c of the respective transformers 8, 9.10. Tertiary windings 8c, 9c of these transformers 8, 9.10.

10Cは直列に接続されているので、検出電圧が加算さ
れて光電圧センサ12の電極に印加される。これにより
、光電圧センサ12を透過する光が偏光されて、光受信
路3から光受信器4に偏光された光信号が伝送される。
10C are connected in series, the detected voltages are added and applied to the electrodes of the optical voltage sensor 12. As a result, the light transmitted through the optical voltage sensor 12 is polarized, and a polarized optical signal is transmitted from the optical receiving path 3 to the optical receiver 4.

光受信器4は光信号を電気信号に変換して信号処理回路
5に出力し、信号処理回路5は人力した電気信号を増幅
して信号処理を行って表示装置6に出力する。
The optical receiver 4 converts the optical signal into an electrical signal and outputs it to the signal processing circuit 5. The signal processing circuit 5 amplifies the manually generated electrical signal, performs signal processing, and outputs it to the display device 6.

第4図は地絡事故発生時に零相電流が流れたときの検出
信号の特性図を示すもので、縦軸に出力を、横軸に時間
をとると、検出信号は図に示すように、正弦波の波形と
して表示される。
Figure 4 shows the characteristics of the detection signal when a zero-sequence current flows when a ground fault occurs.If the vertical axis is the output and the horizontal axis is the time, the detection signal will be as shown in the figure. Displayed as a sine wave waveform.

なお、本実施例においては、開閉器の開閉電極の回りに
環状鉄心を配置したが、送配電線路の回りに変流器を配
置するようにしてもよく、また、電圧センサとしては、
電気光学結晶を用いた光電圧センサに限らず、高入力イ
ンピーダンスの電圧センサであれば、いかなる方式でも
よい。
In this embodiment, a ring-shaped iron core is arranged around the switching electrode of the switch, but a current transformer may be arranged around the power transmission and distribution line, and as a voltage sensor,
It is not limited to an optical voltage sensor using an electro-optic crystal, but any type of voltage sensor with high input impedance may be used.

〔発明の効果〕〔Effect of the invention〕

以上に説明したように、本発明においては、三相の送配
電線路である一次導体を囲んで配置した環状鉄心を設け
、この環状鉄心に二次巻線及び三次巻線を巻回した変成
器を備え、これら変成器の二次残留回路に負担用抵抗を
接続し、三次巻線を直列に接続し、両側の端子を電圧セ
ンサの電極に接続して非接地系の送配電線路の微弱な零
相電流を測定するようにしている。これにより、従来の
三次零相分路方式での欠点であった三次巻線に電流を流
すことからくる大型化、変流比の狂い、さらには三次出
力電流もしくは出力電圧が低い等の問題点が容易に解決
され、コアサイズ、巻線径の小さなコンパクトな変流器
が可能となり、正確な零相電流の測定ができる。さらに
、電圧センサとして電気光学結晶素子を用いることによ
り、非接地で計測できるので、多点アースによる回り回
路を流れる迷走電流による誤動作がなく、外界のノイズ
にも影響されに<<、信頼性の高いシステムを構築する
ことが可能となる。
As explained above, in the present invention, a transformer is provided with an annular core arranged around a primary conductor that is a three-phase power transmission and distribution line, and a secondary winding and a tertiary winding are wound around this annular core. A burden resistor is connected to the secondary residual circuit of these transformers, the tertiary winding is connected in series, and the terminals on both sides are connected to the electrodes of a voltage sensor to detect weak voltages on ungrounded power transmission and distribution lines. I am trying to measure the zero-sequence current. This eliminates the drawbacks of the conventional tertiary zero-phase shunt system, such as increased size due to passing current through the tertiary winding, irregularities in the current transformation ratio, and low tertiary output current or output voltage. This problem can be easily resolved, making it possible to create a compact current transformer with a small core size and winding diameter, allowing accurate zero-sequence current measurement. Furthermore, by using an electro-optic crystal element as a voltage sensor, measurements can be made without being grounded, so there is no malfunction due to stray current flowing through a multi-point grounded circuit, and it is not affected by external noise, improving reliability. It becomes possible to build a sophisticated system.

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

第1図は本発明の実施例を示すブロック図、第2図は光
電圧センサの構造を示す図、第3図は送配電線路が正常
に通電されているときの検出信号の特性図、第4図は地
絡事故発生時に零相電流が流れたときの検出信号の特性
図、第5図は従来の二次残留回路方式の接続図、第6図
は三吹雪を目分路方式の接続図である。 1:光送信器 、   1八ツパルス発生器IB:電気
−光変換素子 2:光送信路3:光受信路     4
:光受信器 5:信号処理回路   6:表示装置 7:開閉器      7a、 7b、 7c :開閉
電極8.9,1.0:変成器  8a、 9a、 lQ
a+鉄心8b、 9b、 lQb:二次巻線  8c、
 9c、 10c:三次巻線11:負担用抵抗    
12:光電圧センサ13;電界動作型素子  14:透
明電極15゛偏光子      16;z波長板17;
検光子 特許出願人  株式会社 安用電機製作所代  理  
人   小  堀   益 (ほか2名)刊g 刊g −5/
Fig. 1 is a block diagram showing an embodiment of the present invention, Fig. 2 is a diagram showing the structure of the optical voltage sensor, Fig. 3 is a characteristic diagram of the detection signal when the power transmission and distribution line is normally energized, and Fig. Figure 4 is a characteristic diagram of the detection signal when a zero-sequence current flows when a ground fault occurs, Figure 5 is a connection diagram of the conventional secondary residual circuit method, and Figure 6 is a connection diagram of the three-flight shunt method. It is a diagram. 1: Optical transmitter, 1-eight pulse generator IB: Electrical-optical conversion element 2: Optical transmission path 3: Optical reception path 4
: Optical receiver 5: Signal processing circuit 6: Display device 7: Switch 7a, 7b, 7c: Switching electrode 8.9, 1.0: Transformer 8a, 9a, lQ
a+ iron core 8b, 9b, lQb: secondary winding 8c,
9c, 10c: Tertiary winding 11: Load resistance
12: Photovoltage sensor 13; Electric field operated element 14: Transparent electrode 15' polarizer 16; Z wavelength plate 17;
Analyzer patent applicant Anyo Electric Manufacturing Co., Ltd. Agent
Masu Kobori (and 2 others) Publication g Publication g -5/

Claims (1)

【特許請求の範囲】 1、三相の送配電線路のそれぞれに環状の鉄心を配置し
、各鉄心に二次巻線及び三次巻線を巻回した変成器を設
け、これらの変成器の二次残留回路の負担として抵抗を
接続するとともに、前記各相の三次巻線を直列に接続し
、該直列回路の両端子間に電圧センサを設けて零相電流
に比例した電圧を検出する手段を備えたことを特徴とす
る光式零相電流検出器。 2、電圧センサとして電気光学結晶素子を用いたことを
特徴とする特許請求の範囲第1項記載の光式零相電流検
出器。
[Claims] 1. A ring-shaped iron core is arranged on each of the three-phase power transmission and distribution lines, and a transformer with a secondary winding and a tertiary winding wound around each iron core is provided, and the secondary winding of these transformers is Next, a resistor is connected as a burden on the residual circuit, and the tertiary windings of each phase are connected in series, and a voltage sensor is provided between both terminals of the series circuit to detect a voltage proportional to the zero-sequence current. An optical zero-sequence current detector characterized by: 2. The optical zero-sequence current detector according to claim 1, characterized in that an electro-optic crystal element is used as the voltage sensor.
JP62271299A 1987-10-26 1987-10-26 Optical zero-phase current detector Expired - Lifetime JPH07104380B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP62271299A JPH07104380B2 (en) 1987-10-26 1987-10-26 Optical zero-phase current detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP62271299A JPH07104380B2 (en) 1987-10-26 1987-10-26 Optical zero-phase current detector

Publications (2)

Publication Number Publication Date
JPH01112169A true JPH01112169A (en) 1989-04-28
JPH07104380B2 JPH07104380B2 (en) 1995-11-13

Family

ID=17498106

Family Applications (1)

Application Number Title Priority Date Filing Date
JP62271299A Expired - Lifetime JPH07104380B2 (en) 1987-10-26 1987-10-26 Optical zero-phase current detector

Country Status (1)

Country Link
JP (1) JPH07104380B2 (en)

Also Published As

Publication number Publication date
JPH07104380B2 (en) 1995-11-13

Similar Documents

Publication Publication Date Title
US4578639A (en) Metering system for measuring parameters of high AC electric energy flowing in an electric conductor
AU701621B2 (en) A device for sensing of electric discharges in a test object
US4749940A (en) Folded bar current sensor
US5923514A (en) Electronic trip circuit breaker with CMR current sensor
US5063472A (en) Device for detecting superconductor quenching and application to a superconducting current limiter
Song et al. A prototype clamp-on magneto-optical current transducer for power system metering and relaying
JPH10185961A (en) Optical current transformer
Bull et al. A new hybrid current sensor for high-voltage applications
CA2021712C (en) Optical current transformer
US4280093A (en) Zero-current detector for high voltage DC transmission line
JPH01112169A (en) Optical zero-phase current detector
US4814930A (en) Optical zero-phase current and zero phase voltage sensing arrangement
JPH02210270A (en) Optical zero-sequence/positive-sequence current detection device
CN115932364B (en) Dual-ring electromagnetic magneto-optical hybrid current transformer
JPH0792481B2 (en) Gas-insulated sealed electric appliance voltage and partial discharge detection device
JPS6234065A (en) Zero-phase voltage detection device for three-phase power lines
HINO et al. Optical fiber current transformer applications on railway electric power supply systems
JP2722749B2 (en) Zero-phase voltage detector
Kesri et al. Latest Trends in Non-Conventional Instrument Transformers
JPH10300796A (en) Photocurrent sensor
JP2959228B2 (en) Optical transformer
JPH0679049B2 (en) Optical zero-phase current detector
CA1157095A (en) Zero-current detector for high voltage dc transmission line
JP2673010B2 (en) Supporting insulator with optical CT
JPH055755A (en) Optical transformer