JPS5897664A - Voltage measuring device - Google Patents

Voltage measuring device

Info

Publication number
JPS5897664A
JPS5897664A JP56198282A JP19828281A JPS5897664A JP S5897664 A JPS5897664 A JP S5897664A JP 56198282 A JP56198282 A JP 56198282A JP 19828281 A JP19828281 A JP 19828281A JP S5897664 A JPS5897664 A JP S5897664A
Authority
JP
Japan
Prior art keywords
light
voltage
measuring device
light emitting
conductor
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Pending
Application number
JP56198282A
Other languages
Japanese (ja)
Inventor
Yoshiaki Ida
井田 芳明
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.)
Mitsubishi Electric Corp
Original Assignee
Mitsubishi Electric Corp
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Mitsubishi Electric Corp filed Critical Mitsubishi Electric Corp
Priority to JP56198282A priority Critical patent/JPS5897664A/en
Publication of JPS5897664A publication Critical patent/JPS5897664A/en
Pending legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G01MEASURING; TESTING
    • G01RMEASURING ELECTRIC VARIABLES; MEASURING MAGNETIC VARIABLES
    • G01R15/00Details of measuring arrangements of the types provided for in groups G01R17/00 - G01R29/00, G01R33/00 - G01R33/26 or G01R35/00
    • G01R15/14Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks
    • G01R15/22Adaptations providing voltage or current isolation, e.g. for high-voltage or high-current networks using light-emitting devices, e.g. LED, optocouplers

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Measuring Instrument Details And Bridges, And Automatic Balancing Devices (AREA)

Abstract

PURPOSE:To obtain a voltage measuring device having high reliability and superior surge resistance and noise resistance and is not influenced by the loss of an optical transmission system, by frequency modulating the voltage signal of a high potential part and transmitting the result in the form of a light output. CONSTITUTION:When an AC high voltage is applied between a conductor 1 and a reference potential, voltages are induced at electrodes 2 and 3 at specified distance apart from the conductor 1 and when the polarity is positive or negative, an electroluminescence element 4 or 5 performs respectively electric field light emission. This light emission turns phototransistors TRs 8 and 9 conductive to hold the potentials of the electrodes 2 and 3 nearly at zero. The, the electroluminescence element turns off and the TRs 8 and 9 are cut off to induce voltages at electrodes 2 and 3 again, repeating said operation thereafter. The frequency-modulated light signal is transmitted to a remote point through optical fiber cables 12 and 13 and converted by photodetectors 14 and 15 into electric signals, which are inputted to a polarity inverting circuit 20 through waveform shaping circuits 16 and 17, AND circuit 18, and frequency-voltage converting circuit 19.

Description

【発明の詳細な説明】 この発明は、変電所等高電圧が印加されている電気機器
において、その高電位部の電圧を測定する電圧測定装置
に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a voltage measuring device for measuring the voltage of a high potential section of an electrical device such as a substation to which a high voltage is applied.

従来、この種の電圧測定装置としては、計器用変圧器、
コンデンサ分圧等のように印加源に直接接続さn、出力
信号も電気的な伝送でなされるもの、あるいは電気光学
素子(ポッケルス効果を利用したもの)による純光学的
な測定装置があるが、前者はサージ等のため、ノイズが
侵入するという悪影蕃があった。また、これを避けるた
めに、検山部(計器用変圧器等)近傍で電気信号を光信
号に変換して伝送する方式も使われているが、この場合
、変換に必要な電源が必要であった。また、後者の場合
は前者のような欠点はないが、電圧情報として振幅変調
されたものとなるため、伝送系のわずかな損失変化が、
誤差となるという欠点があった。
Conventionally, this type of voltage measuring device includes a voltage transformer,
There are measurement devices that are directly connected to the applied source, such as a capacitor partial voltage, and the output signal is also transmitted electrically, or purely optical measurement devices that use electro-optical elements (using the Pockels effect). The former had the negative effect of noise intrusion due to surges, etc. In order to avoid this, a method is also used in which electrical signals are converted into optical signals and transmitted near the measuring part (instrument transformer, etc.), but in this case, a power source is required for the conversion. there were. In the latter case, although there is no drawback like the former, the voltage information is amplitude-modulated, so slight changes in loss in the transmission system
This had the disadvantage of causing errors.

この発明は、上記の欠点を解消□するためになさ口たも
ので、耐ノイズ性を向上させるために光信号で伝送する
こと、検出部で電源を必要としないこと、光信号は振幅
変調ではなく周波数変調した地圧測定装置を提供する。
This invention was made in order to eliminate the above-mentioned drawbacks, and includes transmitting optical signals in order to improve noise resistance, requiring no power supply in the detection section, and using optical signals that are not amplitude modulated. To provide a ground pressure measurement device that is frequency modulated without any frequency modulation.

以下、図に示すこの発明の一実施例について説明する。An embodiment of the present invention shown in the drawings will be described below.

図において、(1)は高電位に充電された導体、(2)
(3)は導体(1)と所定の距離隔てた一対の電極、(
4) (5)はエレクトロルミネセンス素子、(6)(
7)はそれぞれフォトトランジスタ(8J (9)の導
通時の制限抵抗、QQqυはダイオードで、導体(1)
の交流電圧によシ交互に動作するようにフォトトランジ
スタ(3)(9)、ダイオードの極性を変えている。(
6)α違は光フアイバケーブル、α◆(至)は光フアイ
バケーブル@α4で伝送された光を電気信号に変換する
受光素子、αQαηは受光素子α4)Qf9の出力を一
定の振幅にする波形整形(ロ)路、(ト)は波形整形回
路αΦαηの出力を加算するAND回路、011!AN
D回路の出力の周波数を電圧に変換する変換回路、翰は
波形整形回路αηの出力にパルスがある期間のみ変換回
路Qlの出力を極性反転する極性反転回路、Qυは波形
整形回路aηの出力にパルスがぎる期間の間、極性反転
回路(ホ)に信号を出す極性識別回路でおる。
In the figure, (1) is a conductor charged to a high potential, (2)
(3) is a pair of electrodes separated from the conductor (1) by a predetermined distance, (
4) (5) is an electroluminescent element, (6) (
7) are the limiting resistances when the phototransistor (8J (9) is turned on, QQqυ is the diode, and the conductor (1)
The polarities of the phototransistors (3) and (9) and diodes are changed so that they operate alternately depending on the alternating current voltage. (
6) α difference is the optical fiber cable, α◆ (to) is the light receiving element that converts the light transmitted by the optical fiber cable @α4 into an electrical signal, αQαη is the waveform that makes the output of the light receiving element α4)Qf9 a constant amplitude Shaping circuit (B), (G) is an AND circuit that adds the outputs of the waveform shaping circuit αΦαη, 011! AN
A conversion circuit that converts the frequency of the output of circuit D into a voltage, a polarity inversion circuit that inverts the polarity of the output of the conversion circuit Ql only during the period when there is a pulse in the output of the waveform shaping circuit αη, and Qυ the output of the waveform shaping circuit aη. During the pulse period, there is a polarity identification circuit which sends a signal to the polarity inversion circuit (e).

次に動作について説明する。図において、導体(1)と
基準電位(ここでは大地電位)との間に交流の高地圧が
印加されると、導体(1)とある一定距離を隔てた電極
(2) (3)に電圧が誘起される。ところでglL極
(2) (3)を同一形状にすれは同一の電圧が誘起さ
れる。そこ−e、vet極(2)側について説明すると
、電極(2)の極性が正の場合、電極(2)に誘起され
た地圧がエレクトロルミネセンス素子(4)の両端にか
かシ、エレクトロルミネセンス素子(4)が電界発光す
る。
Next, the operation will be explained. In the figure, when high AC ground pressure is applied between a conductor (1) and a reference potential (earth potential here), a voltage is applied to electrodes (2) and (3) that are separated by a certain distance from the conductor (1). is induced. By the way, if the glL poles (2) and (3) have the same shape, the same voltage will be induced. To explain about the -e,vet pole (2) side, when the polarity of the electrode (2) is positive, the ground pressure induced in the electrode (2) is applied to both ends of the electroluminescent element (4), The electroluminescent element (4) emits electroluminescence.

この発光は、光フアイバケーブル(2)によって伝送さ
口るとともに、フォトトランジスタ(8)に受光さ口る
。フォトトランジスタ(3)に受光さnるとフォトトラ
ンジスタ(8)が導通状態となシ、電極(2)の電位を
ほぼ零にする。抵抗(6)はフォトトランジスタ(8)
が導通状態になった時、フォトトランジスタ(3)を過
電流から保護するための制限抵抗である。次に、電極(
2)の電位が零になると、エレクトロルミネセンス素子
(4)が発光しなくなシ、フォトトランジスタ(8)が
カットオフとなり、再び電極(2)に電圧が誘起される
こととなシ、後は同じ動作を繰り返す。ここに、導体(
1)の交流の周期に対して、前述の繰シ返し点滅動作の
回数が、十分多くなるように一極(2)及びエレクトロ
ルミネセンス51(4)を適当に選べば導体(1)の電
圧(正極性)が周波数変調されることとなる。なお、こ
れは、エレクトロルミ不セ:/スi子(4)自身のキャ
パシタンス分と抵抗分による充電時定数により、エレク
トロルミネセンス素子(4)の両端電圧が導体<1)の
印加電圧に対応して上昇し、即ち、導体(1)の印加電
圧が高い程、早く充電され、ある一定地圧になると、エ
レクトロルミネセンス素子(4)が発光することとなシ
、エレクトロルミネセンス素子(4)の点滅が導体(1
)の地圧により周波数変調される。なお、導体(1)の
電圧の極性が負の場合は、ダイオードαOが導通となり
、エレクトロルミネセンス素子(4)は発光しない。亀
fllI(3) @ ハ* 極(2)側と動作が同様で
あるが、導体(1)の電圧の極性が負の場合、エレクト
ロルミネセンス素子(5)が点滅する。
This light emission is transmitted by an optical fiber cable (2) and is received by a phototransistor (8). When the phototransistor (3) receives light, the phototransistor (8) becomes conductive and the potential of the electrode (2) is reduced to approximately zero. Resistor (6) is phototransistor (8)
This is a limiting resistor for protecting the phototransistor (3) from overcurrent when it becomes conductive. Next, the electrode (
When the potential of 2) becomes zero, the electroluminescent element (4) stops emitting light, the phototransistor (8) is cut off, and a voltage is induced in the electrode (2) again. repeats the same action. Here, the conductor (
If the single pole (2) and electroluminescence 51 (4) are appropriately selected so that the number of the above-mentioned repeated blinking operations is sufficiently large with respect to the alternating current cycle of (1), the voltage of the conductor (1) can be increased. (positive polarity) will be frequency modulated. Note that this means that the voltage across the electroluminescent element (4) corresponds to the applied voltage of the conductor (<1) due to the charging time constant due to the capacitance and resistance of the electroluminescent element (4) itself. In other words, the higher the voltage applied to the conductor (1), the faster it is charged, and when a certain ground pressure is reached, the electroluminescent element (4) will emit light. ) blinks when the conductor (1
) is frequency modulated by the ground pressure. Note that when the polarity of the voltage on the conductor (1) is negative, the diode αO becomes conductive and the electroluminescent element (4) does not emit light. Tortoise fllI (3) @ Ha* The operation is similar to the pole (2) side, but when the polarity of the voltage on the conductor (1) is negative, the electroluminescent element (5) blinks.

このように周波数変調された光信号は光フアイバケーブ
ル(2)Q3で遠隔地に伝送さ口、受光素子α4(15
で電気信号に変換される。変換された信号は、それぞ0
波形整形回路a00ηで一定振幅のシャープなパルスに
される。この両者の信号をAND回路で。
The frequency-modulated optical signal is transmitted to a remote location via optical fiber cable (2) Q3, and is then sent to photodetector α4 (15).
is converted into an electrical signal. The converted signals are each 0
The waveform shaping circuit a00η converts the signal into a sharp pulse with a constant amplitude. Use an AND circuit for these two signals.

加算すると、導体(1)の地圧が全波整流された形で周
波数変調さnた信号となる。この信号を変換(ロ)路Q
lによ多導体(1)と相似の電圧信号に変換する。
When added, a signal is obtained in which the ground pressure of the conductor (1) is frequency modulated in a full-wave rectified form. Convert this signal (b) path Q
1 to convert it into a voltage signal similar to that of the multi-conductor (1).

ただし、導体(1)の電圧が全波整流された形であるの
で、波形整形回w4aηの出力にパルスmがある期間の
間、変換回路Qlの出力を極性反転回路(1)で極性を
反転する。極性識別回路なりは、例えば、波形整形回路
αηの出力のパルス群の周波数と導体(1)の電圧の周
波数の中間にカットオフ周波数のあるローパスフィルタ
と波形整形回路から成り、極性反転回路−に極性を反転
する信号を与えるものである。なお、本実施例は基本構
成を示すもので、例えは、エレクトロルミネセンス素子
(4)の点滅をシャープにするためにフォトトランジス
タにシュミット回路を付加する等のことは省いている。
However, since the voltage of the conductor (1) is in a full-wave rectified form, the polarity of the output of the conversion circuit Ql is inverted by the polarity inverting circuit (1) during the period when the output of the waveform shaping circuit w4aη has a pulse m. do. The polarity identification circuit is, for example, composed of a low-pass filter and a waveform shaping circuit with a cutoff frequency between the frequency of the pulse group output from the waveform shaping circuit αη and the frequency of the voltage of the conductor (1), and a polarity inversion circuit. It provides a signal that inverts the polarity. Note that this embodiment shows the basic configuration, and does not include, for example, adding a Schmitt circuit to the phototransistor in order to sharpen the blinking of the electroluminescent element (4).

上記実施例では、電極に誘起された電圧を光信号に変換
する発光素子としてエレクトロルミネセンス素子を用い
た例であるが、発光ダイオードを用いても良い。この場
合、発光時定数を決めるため、外部にコンデンサ、抵抗
を付加する。
In the above embodiment, an electroluminescent element is used as a light emitting element that converts the voltage induced in the electrode into an optical signal, but a light emitting diode may also be used. In this case, an external capacitor and resistor are added to determine the light emission time constant.

また、エレクトロルミネセンス素子の発光を受光して電
極電位を零にする受光素子として、上記実施例ではフォ
トトランジスタを用いた例であるが、フォトダイオード
、カドニウムセルのような光により抵抗値が小さくなる
素子を用いても艮い。
In addition, in the above embodiment, a phototransistor is used as a light-receiving element that receives light emitted from an electroluminescent element and reduces the electrode potential to zero, but a phototransistor such as a photodiode or cadmium cell, which has a small resistance value due to light, may also be used. It is also possible to use a different element.

上記のようにこの発明は非接触で高電位部の電圧を検出
でき、しかも検出部で電源を使うことなく、高電位部の
電圧信号を周波数変調し、光出力で伝送されるので、信
頼性が高< 、fig サー ’) 、 耐ノイズ性に
優れ、光伝送系の損失にもルーされない、高精度の電圧
測定ができる。
As mentioned above, this invention can detect the voltage of the high potential part without contact, and the voltage signal of the high potential part is frequency modulated and transmitted as optical output without using a power supply in the detection part, so it is reliable. It has high resistance to noise, is unaffected by loss in the optical transmission system, and can perform highly accurate voltage measurements.

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

図はこの発明の一実施例を示す構成図である。 図において、(1)は導体(充電部’) 、(21(3
)は一極、(4) (5)はエレクトロルミネセンス素
子(発光素子)、@α3は光ファイバ、04αωは受光
素子、αQα力は波形整形回路、α1は変換回路である
。 代理人   葛 野 信 −
The figure is a configuration diagram showing an embodiment of the present invention. In the figure, (1) is a conductor (live part'), (21 (3
) is a single pole, (4) and (5) are electroluminescent elements (light emitting elements), @α3 is an optical fiber, 04αω is a light receiving element, αQα is a waveform shaping circuit, and α1 is a conversion circuit. Agent Shin Kuzuno −

Claims (1)

【特許請求の範囲】 (131m!気機器の充電部から所定の距離を隔てて設
けらnた一対のIII!l、この各電極と基準電位との
間に接続さnた発光素子、この発光素子の発光を受ける
ように配箪し、電気的に前記発光素子の両端に接続され
た第1の受光素子、前記発光素子の発光を受けて遠隔地
に伝送する光ファイバ、前記光ファイバの光を受光する
第2の受光素子、この第2の受光素子の電気出力信号を
波形整形する波形整形回路、この波形整形回路の周波数
を電圧に変換する変換囲路からなる。ことを特徴とする
電圧測定装置。 (2、特許請求の範囲第1項において、発光素子として
、エレクトロルミネセンス素子を用いたことを特徴とす
る電圧測定装置。 (3)特許請求の範囲第1項において、発光素子として
発光ダイオードを用いたことを特徴とする電圧測定装置
。 (4)特許請求の範囲第1項において、第1の受光素子
として、フォトトランジスタあるいはフォトダイオード
を用いたことを特徴とする電圧測定装置。 (5)特許請求の範囲第1項において、第1の受光素子
として、カドニウムセル等の光によシ抵抗が小さくなる
素子を用いることを特徴とする電圧測定装置。
[Scope of Claims] (131m!) A pair of III!l provided at a predetermined distance from a live part of the device, a light emitting element connected between each electrode and a reference potential, and a light emitting element connected between each electrode and a reference potential; a first light receiving element arranged to receive light emitted from the light emitting element and electrically connected to both ends of the light emitting element; an optical fiber that receives the light emitted from the light emitting element and transmits it to a remote location; light of the optical fiber; A second light-receiving element that receives light, a waveform shaping circuit that shapes the waveform of the electrical output signal of the second light-receiving element, and a conversion circuit that converts the frequency of this waveform shaping circuit into a voltage. Measuring device. (2. In claim 1, a voltage measuring device characterized in that an electroluminescent element is used as a light emitting element. (3) In claim 1, a voltage measuring device characterized in that an electroluminescent element is used as a light emitting element. A voltage measuring device characterized by using a light emitting diode. (4) A voltage measuring device according to claim 1, characterized in that a phototransistor or a photodiode is used as the first light receiving element. (5) A voltage measuring device according to claim 1, characterized in that an element such as a cadmium cell whose resistance decreases due to light is used as the first light receiving element.
JP56198282A 1981-12-04 1981-12-04 Voltage measuring device Pending JPS5897664A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP56198282A JPS5897664A (en) 1981-12-04 1981-12-04 Voltage measuring device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP56198282A JPS5897664A (en) 1981-12-04 1981-12-04 Voltage measuring device

Publications (1)

Publication Number Publication Date
JPS5897664A true JPS5897664A (en) 1983-06-10

Family

ID=16388528

Family Applications (1)

Application Number Title Priority Date Filing Date
JP56198282A Pending JPS5897664A (en) 1981-12-04 1981-12-04 Voltage measuring device

Country Status (1)

Country Link
JP (1) JPS5897664A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59222651A (en) * 1983-06-01 1984-12-14 Mazda Motor Corp Control device in automatic transmission
JPS61149865A (en) * 1984-12-24 1986-07-08 Hitachi Cable Ltd Detecting device for charging state of electric wire
EP0635725A3 (en) * 1993-07-22 1997-04-09 Schneider Electric Sa Electronic circuit for monitoring the presence of a voltage and for comparing the phase in conductors of electric lines.

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59222651A (en) * 1983-06-01 1984-12-14 Mazda Motor Corp Control device in automatic transmission
JPS61149865A (en) * 1984-12-24 1986-07-08 Hitachi Cable Ltd Detecting device for charging state of electric wire
EP0635725A3 (en) * 1993-07-22 1997-04-09 Schneider Electric Sa Electronic circuit for monitoring the presence of a voltage and for comparing the phase in conductors of electric lines.

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