JPH0124454B2 - - Google Patents

Info

Publication number
JPH0124454B2
JPH0124454B2 JP57213762A JP21376282A JPH0124454B2 JP H0124454 B2 JPH0124454 B2 JP H0124454B2 JP 57213762 A JP57213762 A JP 57213762A JP 21376282 A JP21376282 A JP 21376282A JP H0124454 B2 JPH0124454 B2 JP H0124454B2
Authority
JP
Japan
Prior art keywords
signal
optical
converter
electrical
output
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
JP57213762A
Other languages
Japanese (ja)
Other versions
JPS59103438A (en
Inventor
Tadashi Asahara
Masaji Ooshima
Akio Kitamura
Hiroshi Kunyasu
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.)
Kansai Electric Power Co Inc
Nissin Electric Co Ltd
Original Assignee
Nissin Electric Co Ltd
Kansai Denryoku KK
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 Nissin Electric Co Ltd, Kansai Denryoku KK filed Critical Nissin Electric Co Ltd
Priority to JP57213762A priority Critical patent/JPS59103438A/en
Publication of JPS59103438A publication Critical patent/JPS59103438A/en
Publication of JPH0124454B2 publication Critical patent/JPH0124454B2/ja
Granted legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/50Transmitters
    • H04B10/501Structural aspects
    • H04B10/502LED transmitters
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B10/00Transmission systems employing electromagnetic waves other than radio-waves, e.g. infrared, visible or ultraviolet light, or employing corpuscular radiation, e.g. quantum communication
    • H04B10/50Transmitters
    • H04B10/58Compensation for non-linear transmitter output

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Signal Processing (AREA)
  • Nonlinear Science (AREA)
  • Light Guides In General And Applications Therefor (AREA)
  • Optical Communication System (AREA)

Description

【発明の詳細な説明】 この発明は、アナログ光変成装置に関し、さら
に詳しくは、電圧電流変成器の二次側電気出力を
発光ダイオードにより光信号に変換し、光フアイ
バ等によりアナログ伝送し、フオト・ダイオード
等により再び電気信号に戻して出力するアナログ
光変成装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to an analog optical conversion device, and more specifically, it converts the secondary electrical output of a voltage-current transformer into an optical signal using a light emitting diode, transmits it in analog form using an optical fiber, etc., and converts it into an optical signal. -Related to an analog optical conversion device that converts the signal back into an electrical signal using a diode or the like and outputs the signal.

信号を光で伝送する光変成装置は、電気伝送方
式の変成装置と比べ絶縁が容易なため小形軽量化
が可能であり、測定量を信号伝送するに際して光
フアイバを使用することで誘導問題が解消される
など大きなメリツトを有している。このような光
変成装置で電気信号を光信号に変換するのに、幅
広い線型性を持つことから発光ダイオードが多く
用いられているが、発光ダイオードは、発光閾値
電圧のため交流零交差点近傍を光変換できない欠
点があり、このためアナログ伝送の際、波形歪が
大きくなる問題がある。
Optical transformation devices that transmit signals using light can be made smaller and lighter because they are easier to insulate than electrical transmission type transformation devices, and the use of optical fibers to transmit signals of measured quantities solves the problem of guidance. It has great merits such as: Light-emitting diodes are often used to convert electrical signals into optical signals in such optical conversion devices because they have a wide range of linearity. It has the disadvantage that it cannot be converted, which causes a problem of large waveform distortion during analog transmission.

この発明は、上記問題の解決を目的とするもの
で、端的に述べれば、発光ダイオードを用いた通
常の信号伝送部とは別途に設けた飽和変成器の交
流零交差点位相検出パルスの光伝送により、これ
に同期した補正信号を光受信側で発生させ、これ
を通常の信号伝送部の信号に加算することによ
り、発光ダイオードの発光閾値に起因する波形歪
を精度よく補正するアナログ光変成装置を提供す
るものである。
The purpose of this invention is to solve the above-mentioned problem. To put it simply, this invention uses optical transmission of AC zero-crossing phase detection pulses of a saturation transformer provided separately from a normal signal transmission section using light emitting diodes. By generating a correction signal synchronized with this on the optical receiving side and adding it to the signal of the normal signal transmission section, we have created an analog optical conversion device that accurately corrects waveform distortion caused by the light emission threshold of the light emitting diode. This is what we provide.

以下、図に示す実施例に基いて、この発明を詳
説する。なお、これによりこの発明が限定される
ものではない。
Hereinafter, this invention will be explained in detail based on embodiments shown in the drawings. Note that this invention is not limited to this.

第1図に示す30は、この発明のアナログ光変
成装置の一実施例であり、主信号伝送部27と補
正信号伝送部28と補正演算部29とからなつて
いる。
Reference numeral 30 shown in FIG. 1 is an embodiment of the analog optical conversion device of the present invention, which is composed of a main signal transmission section 27, a correction signal transmission section 28, and a correction calculation section 29.

主信号伝送部27は、主変成器1、電気―光変
換器3、光フアイバ5,6、光―電気変換器7お
よび差動増幅器11からなつている。
The main signal transmission section 27 includes a main transformer 1 , an electric-to-optical converter 3 , optical fibers 5 and 6 , an optical-to-electrical converter 7 and a differential amplifier 11 .

補正信号伝送部28は、飽和変成器2、電気―
光変換器4、光フアイバ8,9、光―電気変換器
10、増幅器12,13および双安定マルチバイ
ブレータ14,15からなつている。
The correction signal transmission unit 28 includes the saturation transformer 2, the electrical
It consists of an optical converter 4, optical fibers 8, 9, an optical-to-electrical converter 10, amplifiers 12, 13 and bistable multivibrators 14, 15.

補正演算部29は、AGC増幅器16,17、
差動増幅器18,19、ダイオード20,21、
反転増幅器22および加算増幅器23からなつて
いる。
The correction calculation unit 29 includes AGC amplifiers 16, 17,
Differential amplifiers 18, 19, diodes 20, 21,
It consists of an inverting amplifier 22 and a summing amplifier 23.

一次電流iが正弦波交流であるとすると、主変
成器1の出力波形は第2図2―aに示される正弦
波形、飽和変成器2の出力波形は第2図2―bに
示されるような三角パルス状波形となる。変成器
のインピーダンスおよび負荷インピーダンスを適
切に選択することにより、飽和変成器2の出力信
号は、主変成器1の出力信号の零交差点にピーク
を有する位相となる。
Assuming that the primary current i is a sine wave alternating current, the output waveform of the main transformer 1 is the sine waveform shown in Fig. 2-2-a, and the output waveform of the saturation transformer 2 is the sine-waveform shown in Fig. 2-2-b. The result is a triangular pulse-like waveform. By appropriately selecting the transformer impedance and the load impedance, the output signal of the saturation transformer 2 will have a phase that has a peak at the zero crossing point of the output signal of the main transformer 1.

主変成器1の出力は、電気―光変換器3で正負
別々の発光ダイオードにより光出力に変換され、
2本の光フアイバ5,6により正負別々に光受信
側に伝送される。これら光信号は、光―電気変換
器7で正負別々のPINフオトダイオードにより電
気出力に変換され、差動増幅器11で合成および
増幅され、第3図3―aに示される脈流となる。
図中のθは、発光ダイオードの発光閾値電圧に起
因する発光遅れ角で、閾値電圧をEth、発光ダイ
オードに印加される交流最大値をEmaxとすれ
ば、 θ=Sin-1 Eth/Emax で示され、交流最大値Emaxにほぼ逆比例する。
これは、一次電流iの最大値にほぼ逆比例するこ
とを意味する。
The output of the main transformer 1 is converted into optical output by separate positive and negative light emitting diodes in the electrical-to-optical converter 3.
Positive and negative signals are separately transmitted to the optical receiving side through two optical fibers 5 and 6. These optical signals are converted into electrical outputs by separate positive and negative PIN photodiodes in the opto-electrical converter 7, and are combined and amplified by the differential amplifier 11, resulting in the pulsating flow shown in FIG. 3-a.
θ in the figure is the light emission delay angle caused by the light emission threshold voltage of the light emitting diode. If the threshold voltage is Eth and the maximum AC value applied to the light emitting diode is Emax, then θ=Sin -1 Eth/Emax. and is almost inversely proportional to the maximum AC value Emax.
This means that it is approximately inversely proportional to the maximum value of the primary current i.

飽和変成器2の出力も、電気―光変換器4で正
負別々の発光ダイオードにより光出力に変換さ
れ、2本の光フアイバ8,9により正負別々に受
信側の光―電気変換器10に伝送される。光―電
気変換器10の電気出力は、増幅器12,13で
各々増幅され、双安定マルチバイブレータ14,
15を駆動し、第3図3―b,3―cに示される
矩形波を発生させる。
The output of the saturation transformer 2 is also converted into optical output by separate positive and negative light emitting diodes in the electric-to-optical converter 4, and transmitted separately to the optical-to-electrical converter 10 on the receiving side through two optical fibers 8 and 9. be done. The electrical output of the optical-to-electrical converter 10 is amplified by amplifiers 12 and 13, respectively, and bistable multivibrators 14 and
15 to generate the rectangular waves shown in FIG. 3-b and 3-c.

一方、増幅器12,13の出力は、AGC増幅
器16,17により矩形波電圧ERと等しい尖頭
値ER′の第3図3―d,3―eに示すような三角
波に整形される。三角波のパルス幅θ′は、前記θ
と同様一次電流iの最大値にほぼ逆比例するの
で、飽和変成器2のコア材料と断面寸法を適宜選
定することにより、常に前記θの2倍となるよう
にされる。
On the other hand, the outputs of the amplifiers 12 and 13 are shaped by the AGC amplifiers 16 and 17 into triangular waves as shown in FIGS. 3-d and 3-e with a peak value ER ' equal to the rectangular wave voltage ER . The pulse width θ′ of the triangular wave is the above-mentioned θ
Similarly, it is almost inversely proportional to the maximum value of the primary current i, so by appropriately selecting the core material and cross-sectional dimensions of the saturation transformer 2, it is always made to be twice the above-mentioned θ.

これら三角波は、差動増幅器18,19の反転
端子に夫々加えられ、非反転端子に加えられた双
安定マルチバイブレータ14,15の出力電圧と
夫々減算され、増幅器11の出力において発光値
に対応する電圧に振幅Ecが合致するよう増幅さ
れて出力される。そこで差動増幅器18の出力に
は第3図3―f、差動増幅器19の出力には第3
図3―gの波形が得られる。
These triangular waves are applied to the inverting terminals of the differential amplifiers 18 and 19, respectively, and are subtracted from the output voltages of the bistable multivibrators 14 and 15, which are applied to the non-inverting terminals, respectively, so that the output voltage of the amplifier 11 corresponds to the luminescence value. It is amplified and output so that the amplitude Ec matches the voltage. Therefore, the output of the differential amplifier 18 is set to 3-f in FIG. 3, and the output of the differential amplifier 19 is set to the third
The waveform shown in Figure 3-g is obtained.

これら差動増幅器18,19の出力は、ダイオ
ード20,21で夫々負側のスパイク電圧をカツ
トし、ダイオード21出力電圧を反転増幅器22
で極性反転した後、ダイオード20出力電圧と共
に加算増幅器23により、差動増幅器11の出力
と加え合わされる。注意すべきことは、ダイオー
ド20,21の肩電圧より充分大きな電圧レベル
でこれらの演算を行うべきことである。
The outputs of these differential amplifiers 18 and 19 are outputted by diodes 20 and 21, respectively, to cut negative side spike voltages, and the output voltage of the diode 21 is transferred to an inverting amplifier 22.
After the polarity is inverted at , the output voltage of the diode 20 is added to the output of the differential amplifier 11 by the summing amplifier 23 . What should be noted is that these calculations should be performed at a voltage level that is sufficiently higher than the shoulder voltage of the diodes 20 and 21.

差動増幅器23の出力には第3図3―hのよう
な正弦波交流が得られるが、これは光受信側で作
成した補正電圧(斜線部分)で、主信号伝送部2
7の出力に含まれる発光ダイオードの閾値歪を補
正した信号である。
A sine wave alternating current as shown in Figure 3-3-h is obtained at the output of the differential amplifier 23, but this is a correction voltage (shaded area) created on the optical receiving side, and the main signal transmission section 2
This is a signal obtained by correcting the threshold distortion of the light emitting diode included in the output of No. 7.

変形実施例としては、主変成器1および飽和変
成器2を電圧変成器としたものなどが挙げられ
る。
As a modified example, the main transformer 1 and the saturation transformer 2 may be used as voltage transformers.

以上の説明から理解されるように、この発明の
アナログ光変成装置によれば、一次交流信号を精
度よく復元できるので、周波数特性、位相特性に
制限なく、JEC―190で定められた1級の規格を
満足できるようになる。
As can be understood from the above explanation, the analog optical conversion device of the present invention can accurately restore the primary AC signal, so there are no restrictions on the frequency characteristics and phase characteristics, and the analog optical conversion device of the present invention is Be able to meet the standards.

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

第1図はこの発明のアナログ光変成装置の一実
施例の構成を示すブロツクダイヤグラム、第2図
は主変成器1と飽和変成器2の出力波形を示す波
形図、第3図は第1図に示す装置の各主要部分の
信号波形図である。 1……主変成器、2……飽和変成器、3,4…
…電気―光変換器、5,6,8,9……光フアイ
バ、7,10……光―電気変換器、11,18,
19……差動増幅器、14,15……双安定マル
チバイブレータ、16,17……AGC増幅器、
23……加算増幅器、30……アナログ光変成装
置。
FIG. 1 is a block diagram showing the configuration of an embodiment of the analog optical transformer of the present invention, FIG. 2 is a waveform diagram showing the output waveforms of the main transformer 1 and the saturation transformer 2, and FIG. 3 is the same as that shown in FIG. FIG. 3 is a signal waveform diagram of each main part of the device shown in FIG. 1... Main transformer, 2... Saturation transformer, 3, 4...
...Electric-optical converter, 5,6,8,9...Optical fiber, 7,10...Optical-electrical converter, 11,18,
19...differential amplifier, 14,15...bistable multivibrator, 16,17...AGC amplifier,
23... Addition amplifier, 30... Analog optical conversion device.

Claims (1)

【特許請求の範囲】 1 (a) 一次側交流電気信号に応じて二次側に電
気信号を出力する変成器、その変成器の出力電
気信号を発光ダイオードにより光信号に変換し
て出力する電気―光変換器およびその電気―光
変換器の光信号を受光素子により電気信号に変
換して出力する光―電気変換器からなる主信号
伝送部、 (b) 前記一次側交流電気信号の零交差点近傍部分
の信号に応じて二次側に三角パルス状の電気信
号を出力する飽和変成器、その飽和変成器の出
力電気信号を発光素子により光信号に変換して
出力する電気―光変換器、その電気―光変換器
の光信号を受光素子により電気信号に変換して
出力する光―電気変換器およびその光―電気変
換器の出力信号をトリガとして反転する双安定
マルチバイブレータ回路からなる補正信号伝送
部、および (c) 前記補正信号伝送部の光―電気変換器の出力
と双安定マルチバイブレータ回路の出力とで台
形交流状の電気信号を合成しかつこれと前記主
信号伝送部の光―電気変換器の出力とで前記一
次側交流電気信号に忠実な電気信号を合成する
演算回路からなる補正演算部、 を具備してなるアナログ光変成装置。
[Scope of Claims] 1 (a) A transformer that outputs an electrical signal to the secondary side in response to an AC electrical signal on the primary side, and an electricity that converts the output electrical signal of the transformer into an optical signal using a light emitting diode and outputs it. - Optical converter and its electricity - A main signal transmission section consisting of an optical-to-electrical converter that converts the optical signal of the optical converter into an electrical signal by a light receiving element and outputs it, (b) Zero crossing point of the primary side AC electrical signal A saturation transformer that outputs a triangular pulse-shaped electrical signal to the secondary side in response to a signal in the vicinity, an electric-to-optical converter that converts the output electrical signal of the saturation transformer into an optical signal using a light emitting element and outputs it. A correction signal consisting of an optical-to-electrical converter that converts the optical signal of the electric-to-optical converter into an electric signal using a light receiving element and outputs it, and a bistable multivibrator circuit that inverts using the output signal of the optical-to-electrical converter as a trigger. a transmission section; and (c) a trapezoidal AC-shaped electric signal is synthesized with the output of the optical-to-electrical converter of the correction signal transmission section and the output of the bistable multivibrator circuit, and this and the optical signal of the main signal transmission section are combined. An analog optical conversion device comprising: a correction calculation unit comprising a calculation circuit that synthesizes an electric signal faithful to the primary side AC electric signal with the output of an electric converter.
JP57213762A 1982-12-06 1982-12-06 Analog optical transforming device Granted JPS59103438A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57213762A JPS59103438A (en) 1982-12-06 1982-12-06 Analog optical transforming device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57213762A JPS59103438A (en) 1982-12-06 1982-12-06 Analog optical transforming device

Publications (2)

Publication Number Publication Date
JPS59103438A JPS59103438A (en) 1984-06-14
JPH0124454B2 true JPH0124454B2 (en) 1989-05-11

Family

ID=16644601

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57213762A Granted JPS59103438A (en) 1982-12-06 1982-12-06 Analog optical transforming device

Country Status (1)

Country Link
JP (1) JPS59103438A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
KR100819147B1 (en) 2007-10-11 2008-04-03 유호전기공업주식회사 Optical signal converter and optical signal conversion method

Also Published As

Publication number Publication date
JPS59103438A (en) 1984-06-14

Similar Documents

Publication Publication Date Title
KR830007003A (en) Optical receiver circuit
JPH0124454B2 (en)
US5097229A (en) Modulator - demodulator transformer coupled d.c. to one mhz information channel
RU2365922C1 (en) Optical-electronic current sensor
CN201285432Y (en) Magnetic field current uploading apparatus for electricity generator
CN202488450U (en) Ultra-wideband pulse sequence optical generating device
RU75887U1 (en) OPTICAL ELECTRONIC SENSOR
JPH0136372Y2 (en)
JP3155866B2 (en) Isolation amplifier
JPH04116618A (en) Optical modulating device
JPH0516749Y2 (en)
JPS5527756A (en) Fault position measuring system for communication balanced cable line
EP0099232A3 (en) Burst length modulation for switching power supplies
SU859939A1 (en) Method of electric energy measuring
JPH04337944A (en) Optically balanced transmission circuit
JPS598439A (en) Optical transformer
JPH02108349A (en) Optical receiver
SU1180862A1 (en) D.c.stabilizer
JPS6220000A (en) Insulated transmission circuit
SU1564570A1 (en) Converter of mutual inductance
RU2018139C1 (en) Ac voltage-to absolute value converter
JPS6116638A (en) Optical receiver
JPH0184070U (en)
JPS5533606A (en) Surge detector
SU1637005A1 (en) Bipolar pulse driver