JPH02210270A - Optical zero-sequence/positive-sequence current detection device - Google Patents

Optical zero-sequence/positive-sequence current detection device

Info

Publication number
JPH02210270A
JPH02210270A JP1031735A JP3173589A JPH02210270A JP H02210270 A JPH02210270 A JP H02210270A JP 1031735 A JP1031735 A JP 1031735A JP 3173589 A JP3173589 A JP 3173589A JP H02210270 A JPH02210270 A JP H02210270A
Authority
JP
Japan
Prior art keywords
optical
windings
sequence current
transformer
tertiary
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
JP1031735A
Other languages
Japanese (ja)
Other versions
JPH083503B2 (en
Inventor
Ryuzo Sugii
隆造 杉井
Masao Otsuka
正雄 大塚
Hideki Saito
秀樹 斉藤
Kozo Yukanami
床並 孝三
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 JP1031735A priority Critical patent/JPH083503B2/en
Publication of JPH02210270A publication Critical patent/JPH02210270A/en
Publication of JPH083503B2 publication Critical patent/JPH083503B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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  • Testing Of Short-Circuits, Discontinuities, Leakage, Or Incorrect Line Connections (AREA)
  • Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)
  • Measurement Of Current Or Voltage (AREA)

Abstract

PURPOSE:To measure a positive-phase current with high sensitivity by additionally providing a separate transformer. CONSTITUTION:Ring iron cores 8a-10a are arranged on each 3-phase transmission/distribution line and the 1st transformers 8-10 are provided with the secondary windings 8b-10b and tertiary windings 8c-10c wound up to these cores. These windings 8b-10b are connected to a common resistor 11 for load in parallel and also the windings 8c-10c are connected in series then a photoelectric voltage sensor 12 is provided between both terminals of this series circuit to detect a voltage proportional to a zero-phase current. At this time, the ring iron cores 13a, 14a are arranged in at least two phases of the circuits for the windings 8b-10b and the 2nd transformers 13, 14 are provided with the secondary windings 13b, 14b and the tertiary windings 13c, 14c wound up to these cores. Resistors 15, 16 are connected respectively to the circuits of each winding 13b, 14b of these transformers 13, 14, and photoelectric voltage sensors 17, 18 are connected to the circuits of the windings 13c, 14c. Thus, optical signals are conducted to a signal processing circuit for positive-phase current through an optical transmission passway and detected.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、送配電線路の零相電流及び正相電流を高感度
で信頼性高く検出するための光式零相・正相電流検出装
置に関する。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention provides an optical zero-sequence/positive-sequence current detection device for detecting zero-sequence current and positive-sequence current of power transmission and distribution lines with high sensitivity and high reliability. Regarding.

〔従来の技術〕[Conventional technology]

電力配電分野では、高圧回路の電流を測定する場合には
、一般に変流器が用いられているが、絶縁性や耐ノイズ
性を確保するために、従来から光学式電流検出器が提案
されている。
In the field of power distribution, current transformers are generally used to measure current in high-voltage circuits, but optical current detectors have traditionally been proposed to ensure insulation and noise resistance. There is.

例えば、第5図に示すように、−次導体26が貫通する
磁気コア24に設けたギャップに、ファラデー効果を有
する磁気光学結晶で構成された光磁界センサ25を挟み
、光送信路2から伝送された光の変調光を光送信路3か
ら取り出す方式のものがある。しかし、この方式では、
空隙があるにもかかられず磁気コア24の磁気飽和のた
めに大電流を正確に測定できず、また小電流を測定でき
るほど高精度ではないという問題がある。
For example, as shown in FIG. 5, an optical magnetic field sensor 25 made of a magneto-optic crystal having a Faraday effect is sandwiched between a gap provided in a magnetic core 24 through which a negative order conductor 26 passes, and transmission is transmitted from an optical transmission path 2. There is a system in which the modulated light of the transmitted light is taken out from the optical transmission path 3. However, with this method,
Despite the presence of air gaps, there is a problem in that large currents cannot be accurately measured due to the magnetic saturation of the magnetic core 24, and the accuracy is not high enough to measure small currents.

これに対して、第6図に示すように、−次導体26が貫
通する環状の磁気コア13aに二次巻線13b及び三次
巻線13cを巻回し、二次巻線13bの出力端子に抵抗
器15を接続し、電気光学効果素子を使用した光電圧セ
ンサ17を三次巻線13cの両端に接続して、光の変化
から一次導体26の電流を測定する方式のものがある。
On the other hand, as shown in FIG. 6, a secondary winding 13b and a tertiary winding 13c are wound around an annular magnetic core 13a through which a negative conductor 26 passes, and a resistor is connected to the output terminal of the secondary winding 13b. There is a method in which a photo voltage sensor 17 using an electro-optic effect element is connected to both ends of the tertiary winding 13c, and the current in the primary conductor 26 is measured from changes in light.

この方式のものは、巻数比を大きくすれば電圧を大きく
増幅できるので、小電流でも精度よく測定できる。また
、二次巻線に発生する電流によって該磁気コア13aの
磁気飽和が抑えられるので、大電流を測定できる。
With this method, the voltage can be greatly amplified by increasing the turns ratio, so even small currents can be measured with high accuracy. Further, since magnetic saturation of the magnetic core 13a is suppressed by the current generated in the secondary winding, a large current can be measured.

一方、非接地系の送配電線路に地絡事故が生じたときに
線路の浮遊容量に起因して流れる微弱な零相電流を検出
するために、第4図に示すように、3相の送配電線路の
各々に配置した鉄心3a、 9a。
On the other hand, in order to detect the weak zero-sequence current that flows due to the stray capacitance of the line when a ground fault occurs on an ungrounded power transmission/distribution line, a three-phase transmission line is used as shown in Figure 4. Iron cores 3a and 9a are placed on each of the distribution lines.

10a に二次巻線8b、 9b、 10b及び三次巻
線8c、 9c。
10a, secondary windings 8b, 9b, 10b and tertiary windings 8c, 9c.

10cを巻回した第1の変成器8,9.10を設け、3
相の二次巻線8b、 9b、 10bを共通の抵抗器1
1に並列に接続し、3相の三次巻線8c、 9c、 I
OCは直列に接続してその両端子間に光電圧センサ12
を設けて零相電流を検出する方式を先に提案したく特願
昭62−271299号) この方式によれば、送配電線に生じた零相電流に比例し
た電圧が三次巻線8c、 9c、 10c に発生し、
これを電磁的な影響を受けない前述の光電圧センサ12
に印加させれば、正確かつ精度良く零相電流を測定する
ことができる。なお、第4図において1は光送信器、2
は光送信路、3は光受信路、4は光受信機、5は信号処
理回路、6は表示装置、7は開閉器、7a、 7b、 
7cは3相の開閉器電極である。
A first transformer 8,9.10 wound with 10c is provided, 3
The phase secondary windings 8b, 9b, 10b are connected to a common resistor 1.
1, and three-phase tertiary windings 8c, 9c, I
The OCs are connected in series and a photovoltage sensor 12 is connected between both terminals.
According to this method, a voltage proportional to the zero-sequence current generated in the power transmission and distribution lines is applied to the tertiary windings 8c and 9c. , occurred at 10c,
This is the photo voltage sensor 12 that is not affected by electromagnetic effects.
If applied, the zero-sequence current can be measured accurately and precisely. In addition, in FIG. 4, 1 is an optical transmitter, 2
is an optical transmission path, 3 is an optical reception path, 4 is an optical receiver, 5 is a signal processing circuit, 6 is a display device, 7 is a switch, 7a, 7b,
7c is a three-phase switch electrode.

ここで、第4図に示した零相電流検出方式を用いて3相
の送配電線の零相電流を測定しながら、同時に各相の通
電電流(正相電流)をも測定することを考える。センサ
としては前記光電圧センサ12に何らかの方法で電圧を
印加した方が、前述のように有用である。例えば、当該
零相電流検出方式の二次巻線8b、 9b、 10bの
各相に各々抵抗器を直列に接続してその両端に発生する
電圧を各相の正相電流測定用光電圧センサ12に印加し
たとする。
Now, let's consider using the zero-sequence current detection method shown in Figure 4 to measure the zero-sequence current of a three-phase power transmission and distribution line, and at the same time measure the carrying current (positive-sequence current) of each phase. . As mentioned above, it is more useful as a sensor to apply a voltage to the optical voltage sensor 12 by some method. For example, a resistor is connected in series to each phase of the secondary windings 8b, 9b, and 10b of the zero-sequence current detection method, and the voltage generated across the resistors is measured using the optical voltage sensor 12 for measuring the positive-sequence current of each phase. Suppose that it is applied to

センサの感度を上げるためには、抵抗値を大きくして高
い電圧を発生させる必要があるが、そうすると変流器の
負担が大きくなり、コアの断面積を大きくすることにな
るなど、短所が多い。
In order to increase the sensitivity of the sensor, it is necessary to increase the resistance value and generate a high voltage, but this has many disadvantages, such as increasing the load on the current transformer and increasing the cross-sectional area of the core. .

そこで前述のように、磁気コアに巻回した二次巻線の抵
抗器に発生した電圧を三次巻線で増幅して光電圧センサ
で測定する単独CT(変流器)三次巻線方式を用いるこ
とが考えられる。しかし、この正相用単独CTの磁気コ
アと当該零相電流検出方式(3CT連結三次巻線方式)
の磁気コアを共通に使っては、原理的に意味がない。な
ぜなら、作動中の3CTのコアには結果として零相分の
磁界が通っているので、30Tのコアでは正相分を検出
できないからである。
Therefore, as mentioned above, we use a single CT (current transformer) tertiary winding method in which the voltage generated in the resistor of the secondary winding wound around the magnetic core is amplified by the tertiary winding and measured by a photovoltage sensor. It is possible that However, the magnetic core of this single CT for positive phase and the zero-sequence current detection method (3CT connected tertiary winding method)
There is no point in principle in using the same magnetic core. This is because, as a result, a zero-phase magnetic field passes through the operating 3CT core, so a 30T core cannot detect the positive phase.

〔発明が解決しようとする課題〕[Problem to be solved by the invention]

以上のように、当該3CT連結三次巻線方式のままでは
、正相電流まで同時に測定できず、正相電流測定用の付
属品を設置しても、信頼性や安全性が高く高性能なもの
を実現することが困難となる要因が多い。
As mentioned above, with the 3CT connected tertiary winding method, it is not possible to measure the positive sequence current at the same time, and even if accessories for measuring the positive sequence current are installed, it is not possible to measure the positive sequence current with high reliability, safety, and high performance. There are many factors that make it difficult to achieve this goal.

本発明は、この問題を解決し、零相電流検出器にわずか
な部品を加えることにより正相電流をも精度良く測定で
きる検出器を提供することを目的とする。
An object of the present invention is to solve this problem and provide a zero-sequence current detector that can also measure positive-sequence current with high accuracy by adding a few parts to the zero-sequence current detector.

〔課題を解決するための手段〕[Means to solve the problem]

この目的を達成するため、本発明の光式零相・正相電流
検出装置は、3相の送配電線路の各々に環状の鉄心を配
置し、各鉄心に二次巻線及び三次巻線を巻回した第1の
変成器を設け、これらの第1の変成器の二次巻線を共通
の抵抗器に並列に接続するとともに、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気光学結
晶を用いた光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光式零相電流検出装置におい
て、前記二次巻線回路の少なくとも2相に環状の鉄心を
配置し、該各鉄心に二次巻線及び三次巻線を巻回した第
2の変成器を設け、この第2の変成器の各々の二次回路
に各々抵抗器を接続するとともに、この第2の変成器の
各々の三次回路の両端子間に各々光電圧センサを設けて
正相電流を検出する手段を備えたことを特徴とする特〔
作用〕 本発明は、先に提案した第4図の零相電流検出装置の二
次巻線に第2の変成器を設けるものである。すなわち、
3相の送配電線路の各々に配置した鉄心に各々巻回され
た二次巻線の少なくとも2相に各々鉄心を配置し、各々
2次巻線と3次巻線を巻回して第2の変成器とする。そ
の第2の変成器の2次巻線には各相別々に抵抗器を接続
し、3次巻線には光学結晶を用いた光電圧センサを各相
別々に接続し、その光信号は発光・受光素子から送受信
され、信号処理回路へ送られる。
In order to achieve this objective, the optical zero-phase/positive-sequence current detection device of the present invention has a ring-shaped iron core placed on each of the three-phase power transmission and distribution lines, and a secondary winding and a tertiary winding on each iron core. The secondary windings of these first transformers are connected in parallel to a common resistor, and the tertiary windings of each phase are connected in series. In an optical zero-sequence current detection device comprising a means for detecting a voltage proportional to a zero-sequence current by providing an optical voltage sensor using an electro-optic crystal between both terminals of the circuit, at least two of the secondary winding circuits A second transformer is provided in which a ring-shaped iron core is arranged in the phase, a secondary winding and a tertiary winding are wound around each of the iron cores, and a resistor is provided in each secondary circuit of this second transformer. The second transformer is connected to the tertiary circuit of the second transformer, and includes a means for detecting the positive sequence current by providing a photovoltage sensor between both terminals of each tertiary circuit of the second transformer.
Effect] The present invention provides a second transformer in the secondary winding of the previously proposed zero-sequence current detection device shown in FIG. That is,
The iron cores are placed in at least two phases of the secondary windings, each of which is wound around the iron core placed in each of the three-phase power transmission and distribution lines, and the secondary winding and the tertiary winding are wound on each of the secondary windings. It is a transformer. A resistor is connected to the secondary winding of the second transformer for each phase separately, and a photovoltage sensor using an optical crystal is connected to the tertiary winding for each phase, and the optical signal is emitted. - Transmitted and received from the light receiving element and sent to the signal processing circuit.

3相に通電されている正相電流によって第1の変成器の
二次巻線回路に二次電流が流れる。この二次電流によっ
て、第2の変成器の二次巻線に電圧が誘起されて電流が
流れ、三次巻線に電圧が発生して光電圧センサに印加さ
れ、光信号の変化から三次電圧を測定して、第2の変成
器を設けた2相の正相電流が検出される。もし、第2の
変成器を2つの相だけに設けた場合には、残りの相の正
相電流は、検出された2相の正相電流のベクトル和を零
相電流からベクトル的に差し引くことによって得られる
。第2の変成器を3相とも設けると、各相のセンサの出
力で直接、各相の正相電流が得られる。
A secondary current flows through the secondary winding circuit of the first transformer due to the positive sequence current being applied to the three phases. This secondary current induces a voltage in the secondary winding of the second transformer, causing a current to flow, generating a voltage in the tertiary winding and applying it to the optical voltage sensor, which detects the tertiary voltage from the change in the optical signal. Measured to detect the positive sequence current of the two phases with the second transformer. If the second transformer is installed in only two phases, the positive sequence current of the remaining phases can be obtained by vectorially subtracting the vector sum of the detected positive sequence currents of the two phases from the zero sequence current. obtained by. If the second transformer is provided for all three phases, the positive sequence current of each phase can be directly obtained from the output of the sensor of each phase.

〔実施例〕〔Example〕

以下、本発明を実施例に基づいて具体的に説明する。 Hereinafter, the present invention will be specifically explained based on Examples.

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、1.31は光を送出する光送信器、
2.32及び3.33は光ファイバを用いた光送信路及
び光受信路、4,34は光受信器、5.35は信号処理
回路、6.36は表示装置である。
FIG. 1 is a block diagram showing the configuration of an embodiment of the present invention. In the figure, 1.31 is an optical transmitter that sends out light;
2.32 and 3.33 are optical transmission paths and optical reception paths using optical fibers, 4 and 34 are optical receivers, 5.35 is a signal processing circuit, and 6.36 is a display device.

7は消弧性ガスを封入した開閉器であり、この開閉器内
に、三相の送配電線路のそれぞれに接続する開閉器電極
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、 10a が設けられ、これらの鉄心3a、 9
a。
Reference numeral 7 denotes a switch filled with arc-extinguishing gas, and switch electrodes 7a, 7b, and 7c connected to each of the three-phase power transmission and distribution lines are housed in this switch. 8°9.10
is a transformer, and each of the switch electrodes 7a, 7b, and 7c has an annular iron core 8a disposed surrounding the electrodes.
9a, 10a are provided, and these iron cores 3a, 9
a.

10a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、 9c、 IOCが巻回されている。前
記二次巻線8b、 9b、 10b には、負担用抵抗
器11を並列に接続し、三次巻線8c、 9c、 10
c 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、
例えばし1Tao、、  LiNbO5,にOP(にH
−PO4)、  BGO(To+zGeOao)。
Secondary windings 8b, 9b, 10b and tertiary windings 3c, 9c, IOC are wound around 10a so that the transformation ratios of the respective transformers 8, 9, 10 are equal. A burden resistor 11 is connected in parallel to the secondary windings 8b, 9b, 10b, and the tertiary windings 8c, 9c, 10
c are connected to each other in series, and the terminals on both sides are connected to the electrodes of the photovoltage sensor 12, respectively. This optical voltage sensor 12 includes an electric field operated element such as a Pockels element,
For example, 1Tao, OP to LiNbO5 (to H
-PO4), BGO(To+zGeOao).

B50(Bi、2SiO,。)等の強誘電体系の材料が
主として用いられる。
Ferroelectric materials such as B50 (Bi, 2SiO, .) are mainly used.

13、14は正相電流検出のための第2の変成器であり
、第1の変成器の二次巻線を囲んで配置した環状の鉄心
13a、 14aが設けられ、これらの鉄心13a、 
14aには、各々の変成器13.14の変成比が等しく
なるように、二次巻線13b、 14b及び三次巻線1
3c、 14cが巻回されている。これらの二次巻線1
3b。
Reference numerals 13 and 14 designate a second transformer for detecting positive sequence current, and are provided with annular iron cores 13a and 14a arranged around the secondary winding of the first transformer.
14a has secondary windings 13b, 14b and tertiary winding 1 so that the transformation ratios of each transformer 13.14 are equal.
3c and 14c are wound. These secondary windings 1
3b.

14b には、負担用抵抗器15.16が各々接続され
、前記三次巻線13C,14Cには、光電圧センサ17
.18がそれぞれ接続され、正相電流用の信号処理回路
に光伝送路で光信号が導かれる。
Load resistors 15 and 16 are connected to the tertiary windings 14b and 14b, respectively, and a photovoltage sensor 17 is connected to the tertiary windings 13C and 14C.
.. 18 are connected to each other, and an optical signal is guided to a signal processing circuit for positive-sequence current through an optical transmission line.

この光電圧センサ12. 17.18を用いた電圧検出
システムを第2図に示す。1^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1
^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。光電圧センサ12は、端面に透明電極2
0.20を有する電界動作型素子19.偏光子21. 
 ’A波長板22及び検光子23より構成されている。
This optical voltage sensor 12. A voltage detection system using 17.18 is shown in FIG. 1^ is a pulse generator,
The output pulse is converted into an optical pulse by the electro-optical conversion element IB, and is applied to the optical voltage sensor 12 via the optical transmission path 2 using an optical fiber. These pulse generators 1
^ and the electro-optical conversion element IB are provided in the optical transmitter 1. The photovoltage sensor 12 has a transparent electrode 2 on the end surface.
19. Field-operated element with 0.20. Polarizer 21.
It is composed of an A wavelength plate 22 and an analyzer 23.

透明電極20.20は、第1図の三次巻線3c、 9c
、 IOCの直列回路の両端と、電気的に接続されてい
る。検光子23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。
The transparent electrodes 20.20 are the tertiary windings 3c and 9c in FIG.
, are electrically connected to both ends of the IOC series circuit. The optical output from the analyzer 23 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、第
1の変成器8,9,1.0の二次巻線Bb、 gb。
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 of the first transformers 8, 9, 1.0 Bb, gb.

10bにそれぞれ誘起された二次電流の和が零となるか
ら、負担用抵抗器11の両端には電圧は生じず、三次巻
線3c、 9c、 1.Oc 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は入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。
Since the sum of the secondary currents induced in each of the tertiary windings 3c, 9c, 1.10b becomes zero, no voltage is generated across the burden resistor 11. No voltage is generated at Oc. 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 is output from the optical reception path 3 to the optical receiver 4. 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 input electrical signal, performs signal processing, and outputs the signal to the display device 6.

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゜lOの三次巻線
3c、 9c、 IOC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 3c, 9c, IOC of the respective transformers 8, 9°lO. 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
。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は入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。
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. 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 input electrical signal, performs signal processing, and outputs it to the display device 6.

以上が零相電流検出の動作原理である。The above is the operating principle of zero-sequence current detection.

一方、正相電流については、零相電流の有無に拘わらず
、第1の変成器8,9の二次巻線3b、 gbには二次
電流が流れるため、第2の変成器13. 14の二次巻
線回路13b、 14bには抵抗器15. 16に応じ
てそれぞれ二次電流が流れ、三次巻線13c、 14c
に三次電圧が発生して、光電圧センサ17.18に印加
される。それからの動作は光電圧センサ12の場合と同
様である。これにより、送配電線2相の正相電流が測定
されることになるが、残りの1相については、第3図の
ように、測定された2相の正相電流1−、Ib のベク
トル和を、測定された零相電流1c から信号処理の段
階でベクトル的に差し弓けばよい。
On the other hand, regarding the positive-sequence current, regardless of the presence or absence of the zero-sequence current, the secondary current flows through the secondary windings 3b and gb of the first transformers 8 and 9, so that the second transformer 13. 14 secondary winding circuits 13b, 14b have resistors 15. 16, a secondary current flows respectively in the tertiary windings 13c and 14c.
A tertiary voltage is generated and applied to the optical voltage sensor 17,18. The operation thereafter is similar to that of the optical voltage sensor 12. As a result, the positive sequence currents of the two phases of the power transmission and distribution lines are measured, and for the remaining one phase, as shown in Fig. 3, the vector of the measured positive sequence currents 1- and Ib of the two phases is The sum can be vectorially calculated from the measured zero-sequence current 1c at the signal processing stage.

ここで消費電力については、第2の変成器の二次巻線と
三次巻線の巻数比を大きくすれば抵抗器15、16の抵
抗値は小さくできるので、電力消費を抑えることができ
る。
Regarding power consumption, if the turns ratio between the secondary winding and the tertiary winding of the second transformer is increased, the resistance values of the resistors 15 and 16 can be reduced, so that power consumption can be suppressed.

一方、本発明の手法とは別に、例えば各相の第1の変成
器の二次巻線の各々に抵抗器を直接接続してその両端に
発生した電圧をセンサに印加させる方法を採ったとする
と、センサの感度を本発明の手法と同程度に確保するた
めには大きな電力を消費することになり、その負担を補
うため、磁気コアの断面積を大きくとらなければならな
い。
On the other hand, apart from the method of the present invention, suppose that a method is adopted in which, for example, a resistor is directly connected to each of the secondary windings of the first transformer of each phase and the voltage generated across the resistor is applied to the sensor. In order to ensure the sensitivity of the sensor to the same level as the method of the present invention, a large amount of power will be consumed, and in order to compensate for this burden, the cross-sectional area of the magnetic core must be made large.

また、正相電流用の単独CTを第6図のように一次導体
に設置すると、本発明の第2の変成器と比べて一次電流
が大きいので、絶縁のためにコア径は大きくなり、二次
電流も二次電圧も大きくなるので、消費電力が大きくな
る。さらに、その消費電力を抑えるために抵抗を小さく
すると、三次電圧も小さくなるので、検出感度も悪くな
り、それを補うためには巻数比を大きくしなければなら
ないなど、実現困難になる要因が多く、本発明の方が有
用であることがわかる。
Furthermore, when a single CT for positive sequence current is installed on the primary conductor as shown in Figure 6, the primary current is larger than in the second transformer of the present invention, so the core diameter becomes larger for insulation, and the secondary Since both the secondary current and the secondary voltage increase, power consumption increases. Furthermore, if the resistance is made smaller in order to reduce power consumption, the tertiary voltage will also become smaller, which will reduce detection sensitivity, and in order to compensate for this, the turns ratio will have to be increased.There are many factors that make this difficult to implement. , it can be seen that the present invention is more useful.

なお、本実施例では開閉器の開閉器電極口りにlq状鉄
心を配置したが、送配電線路の回りでもよく、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、高人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 example, the lq-shaped iron core was placed at the opening of the switch electrode of the switch, but it may also be placed around power transmission and distribution lines, and the voltage sensor is not limited to an optical voltage sensor using an electro-optic crystal. Any type of voltage sensor may be used as long as it is a human impedance voltage sensor.

〔発明の効果〕〔Effect of the invention〕

以上に説明したように、本発明によれば、送配電線の零
相電流を高感度に検出する装置はそのままで、第2の変
成器を付加することにより、正相電流を感度よく測定で
きる。さらに、その第2の変成器の巻数比を大き(すれ
ば抵抗器で消費される電力を抑制でき、回路全体の負担
を軽減することができる。
As explained above, according to the present invention, positive sequence current can be measured with high sensitivity by adding a second transformer while leaving the device that detects zero-sequence current of power transmission and distribution lines with high sensitivity as is. . Furthermore, by increasing the turns ratio of the second transformer, the power consumed by the resistor can be suppressed, and the load on the entire circuit can be reduced.

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

第1図は本発明の実施例の構成を示すブロック図、第2
図は光電圧センサの構造説明図、第3図は正相電流の求
め方を示すベクトル図、第4図は従来の光式零相電流検
出装置の構成を示すブロック図、第5図は単独CT三次
巻線方式の構成を示すブロック図、第6図は光磁界セン
サを用いた従来の電流測定器の例を示す説明図である。 1.31:光送信器 2.32:光送信路 3.33:光受信路 4.34+光受信器 5.35+信号処理回路 6.36:表示装置 7;開閉器    7a、 7b、 7c8.9,10
:第1の変成器 8a、 9a、 10a: m状鉄心 8b、 9b、 iob:二次巻線 8c、 9c、 10c:三次巻線 11、15.16 :抵抗器 12、17.18 :光電圧センサ 13.14:第2の変成器 13a、 14a: 1m状鉄心 13b、 14b:二次巻線 13C,14C:三次巻線 :開閉器電極 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)第 図 第 図
FIG. 1 is a block diagram showing the configuration of an embodiment of the present invention, and FIG.
The figure is an explanatory diagram of the structure of an optical voltage sensor, Figure 3 is a vector diagram showing how to determine the positive sequence current, Figure 4 is a block diagram showing the configuration of a conventional optical zero-sequence current detection device, and Figure 5 is a stand-alone FIG. 6 is a block diagram showing the configuration of the CT tertiary winding system, and is an explanatory diagram showing an example of a conventional current measuring device using an optical magnetic field sensor. 1.31: Optical transmitter 2.32: Optical transmission path 3.33: Optical receiving path 4.34 + Optical receiver 5.35 + Signal processing circuit 6.36: Display device 7; Switches 7a, 7b, 7c 8.9 ,10
: First transformer 8a, 9a, 10a: M-shaped core 8b, 9b, iob: Secondary winding 8c, 9c, 10c: Tertiary winding 11, 15.16: Resistor 12, 17.18: Photovoltage Sensors 13, 14: Second transformers 13a, 14a: 1m-shaped iron cores 13b, 14b: Secondary windings 13C, 14C: Tertiary windings: Switch electrode Patent applicant Yasuyo Electric Manufacturing Co., Ltd. Manager Kobori Masu (and 2 others)

Claims (1)

【特許請求の範囲】 1、3相の送配電線路の各々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第1の変成器を
設け、これらの第1の変成器の二次巻線を共通の抵抗器
に並列に接続するとともに、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気光学結晶を用い
た光電圧センサを設けて零相電流に比例した電圧を検出
する手段を備えた光式零相電流検出装置において、 前記二次巻線回路の少なくとも2相に環状の鉄心を配置
し、該各鉄心に二次巻線及び三次巻線を巻回した第2の
変成器を設け、この第2の変成器の各々の二次回路に各
々抵抗器を接続するとともに、この第2の変成器の各々
の三次回路の両端子間に各々光電圧センサを設けて正相
電流を検出する手段を備えたことを特徴とする光式零相
・正相電流検出装置。
[Claims] A first transformer is provided in which an annular core is arranged on each of the first and third phase power transmission and distribution lines, a secondary winding and a tertiary winding are wound around each core, and The secondary winding of the transformer No. 1 is connected in parallel to a common resistor, and the tertiary windings of each phase are connected in series, and a photovoltaic voltage is generated using an electro-optic crystal between both terminals of the series circuit. In an optical zero-sequence current detection device equipped with a sensor and means for detecting a voltage proportional to the zero-sequence current, an annular iron core is disposed in at least two phases of the secondary winding circuit, and two A second transformer having a secondary winding and a tertiary winding is provided, a resistor is connected to each secondary circuit of this second transformer, and a resistor is connected to each tertiary circuit of this second transformer. 1. An optical zero-sequence/positive-sequence current detection device, comprising means for detecting a positive-sequence current by providing optical voltage sensors between both terminals of a circuit.
JP1031735A 1989-02-09 1989-02-09 Optical zero-phase / positive-phase current detector Expired - Lifetime JPH083503B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1031735A JPH083503B2 (en) 1989-02-09 1989-02-09 Optical zero-phase / positive-phase current detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1031735A JPH083503B2 (en) 1989-02-09 1989-02-09 Optical zero-phase / positive-phase current detector

Publications (2)

Publication Number Publication Date
JPH02210270A true JPH02210270A (en) 1990-08-21
JPH083503B2 JPH083503B2 (en) 1996-01-17

Family

ID=12339295

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1031735A Expired - Lifetime JPH083503B2 (en) 1989-02-09 1989-02-09 Optical zero-phase / positive-phase current detector

Country Status (1)

Country Link
JP (1) JPH083503B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103901252A (en) * 2014-04-08 2014-07-02 烟台市华能电器有限公司 10 KV electric transmission line zero-sequence current detection system

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN103901252A (en) * 2014-04-08 2014-07-02 烟台市华能电器有限公司 10 KV electric transmission line zero-sequence current detection system
CN103901252B (en) * 2014-04-08 2018-11-02 烟台市华能电器有限公司 10KV power transmission line zero-sequence current detecting systems

Also Published As

Publication number Publication date
JPH083503B2 (en) 1996-01-17

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