JPS598439A - Optical transformer - Google Patents

Optical transformer

Info

Publication number
JPS598439A
JPS598439A JP57118264A JP11826482A JPS598439A JP S598439 A JPS598439 A JP S598439A JP 57118264 A JP57118264 A JP 57118264A JP 11826482 A JP11826482 A JP 11826482A JP S598439 A JPS598439 A JP S598439A
Authority
JP
Japan
Prior art keywords
output
transformer
optical
light emitting
signal
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
JP57118264A
Other languages
Japanese (ja)
Other versions
JPH0148704B2 (en
Inventor
Akio Kitamura
北村 章夫
Hiroshi Kuniyasu
國安 廣
Tadashi Asahara
浅原 正
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
Kansai Electric Power Co Inc
Nissin Electric 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 Kansai Electric Power Co Inc, Nissin Electric Co Ltd filed Critical Kansai Electric Power Co Inc
Priority to JP57118264A priority Critical patent/JPS598439A/en
Publication of JPS598439A publication Critical patent/JPS598439A/en
Publication of JPH0148704B2 publication Critical patent/JPH0148704B2/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
    • H04B10/25Arrangements specific to fibre transmission

Landscapes

  • Physics & Mathematics (AREA)
  • Electromagnetism (AREA)
  • Engineering & Computer Science (AREA)
  • Computer Networks & Wireless Communication (AREA)
  • Signal Processing (AREA)
  • Optical Communication System (AREA)

Abstract

PURPOSE:To reproduce a sinusoidal wave faithful to an original waveform, by giving a secondary output of a transformer to a light emitting diode, transmitting an optical signal corresponding to a positive and a negative voltage and adding a level proportional to the threshold value of a diode for eliminating high harmonic components. CONSTITUTION:A secondary output (a) between terminals 1, 2 of the transformer Tr is applied to light emitting diodes D1, D2 via a temperature cmpensating circuit 2 comprising resistors R1, R2 and a thermister Rt to light respectively the diodes D1, D2 in response to the positive and the negative voltage. This optical signal is transmitted to photodiodes D3, D4 at receiving side on optical fibers F1, F2 to convert the optical signal into an electric signal. A pulsive output is generated at load resistors R3, R4 with this signal to output a pulsive output (b) at an output load resistor R7 of an operational amplifier IC1 to be supplied to operational amplifiers IC2, IC4 to output respective rectangular wave signals C, C'. The signals C, C' are added to the output (b) proportional to a threshold voltage inherent to the diodes D1, D2, the high harmonic components are eliminated and a sinusoidal wave faithful to the original waveform is outputted.

Description

【発明の詳細な説明】 本発明は光変成器に関する。。[Detailed description of the invention] The present invention relates to optical transformers. .

通常発光ダイオードをアナログ信号の光源に使用する場
合、適当なバイアス電圧を加え、直線性の良好な範囲内
で電気信号による光出力の振1」変調を行っている。し
カルこの発光ダイオードを光変成器の光源に使用する場
合はいわゆる高電圧部位に設けられるところから、安定
なバイアス電圧を供給することが困難となる。このため
従来は、正極性電圧を分担するダイオードと負極性電圧
を分担するダイオードとを組み合わせ、交流の半周期ご
とにそれぞれのダイオードを発光させて得られる光信号
を2本の光ファイバで別々に伝送し、光信号受信側で光
電変換した後交流に復元している。
Normally, when a light emitting diode is used as a light source for an analog signal, an appropriate bias voltage is applied and the optical output is modulated by an electric signal within a range with good linearity. However, when this light emitting diode is used as a light source of an optical transformer, it is difficult to supply a stable bias voltage because it is installed in a so-called high voltage region. For this reason, in the past, a diode that shared the positive polarity voltage and a diode that shared the negative polarity voltage were combined, and the optical signals obtained by making each diode emit light every half cycle of AC were transmitted separately using two optical fibers. The signal is transmitted, and after photoelectric conversion on the receiving side, the signal is restored to alternating current.

しかしながら、発光ダイオードをこのように使うと、当
然ダイオードに固有の閾値電圧の8題が発生し、正弦波
交流の零点から閾値電圧に達するまでの時間帯は発光せ
ず、従って、光ファイバを経て伝送されてきた光信号を
受信側で電気信号に復元してもそのままでは脈流が得ら
れるだけで正弦波交流を再現させることができない。
However, when a light emitting diode is used in this way, there are of course eight problems with the threshold voltage inherent to the diode, and it does not emit light during the time period from the zero point of the sine wave alternating current until the threshold voltage is reached, and therefore it cannot be used via an optical fiber. Even if the transmitted optical signal is restored to an electrical signal on the receiving side, only a pulsating current will be obtained and it will not be possible to reproduce a sinusoidal alternating current.

本発明は、上述の事柄に留意してなされたもので、変成
器の二次側出力を発光ダイオードに与え、正極性電圧、
負極性電圧に対応してそれぞれ得られる光信号を光ファ
イバを用いてアナログ伝送するようにしたものにおいて
、前記光ファイバの受信側で前記光信号に基づく電気信
号を合成して得られる脈流出力に同期しtコ矩形波信号
を発生させ・、この矩形波信号を前記発光ダイオードに
固有の閾値電圧に比例した適当なレベルで前記脈流出力
に加算し、この加算によって得られる波形から高調波成
分を除去するようにしtコもので、原波形に忠実な正弦
波交流を再現しようとするものである。
The present invention has been made with the above-mentioned matters in mind, and the secondary side output of the transformer is applied to the light emitting diode, and the positive polarity voltage,
A pulsating output obtained by synthesizing electrical signals based on the optical signals on the receiving side of the optical fiber, in which optical signals obtained in response to negative polarity voltages are transmitted in analog form using optical fibers. A square wave signal is generated in synchronization with t, and this square wave signal is added to the pulsating output at an appropriate level proportional to the threshold voltage specific to the light emitting diode, and harmonics are calculated from the waveform obtained by this addition. This method removes components and attempts to reproduce a sinusoidal alternating current that is faithful to the original waveform.

以下、本発明を図面に示す実施例に従って説明する。第
1図は、本発明の一実施例を示す回路構成図である。T
rは高電位部に設けられtこ変成器で、その端子1.2
に現われる二次側出力aは、第2図(a)に示すような
波形であって、抵抗孔1、R2、サーミスタ几tにより
構成された温度補償回路を経て発光ダイオードD1、D
2に与えられろ。この発光ダイオードDI、D2はそれ
ぞれ正極性電圧、負極性電圧に対応して発光するよう接
続されている。その出力である光信号は光ファイバF1
、F2を経て受信側に導かれる。D3、D4は受信側に
設けられたフォトダイオードで、IiJ記光記号信号の
ダイオードD3、D4によって電気信号に変換される。
Hereinafter, the present invention will be explained according to embodiments shown in the drawings. FIG. 1 is a circuit diagram showing an embodiment of the present invention. T
r is a transformer installed in the high potential section, and its terminals 1.2
The secondary side output a appearing in the waveform shown in FIG.
Be given to 2. The light emitting diodes DI and D2 are connected to emit light in response to positive and negative voltages, respectively. The output optical signal is transmitted through optical fiber F1
, F2 to the receiving side. D3 and D4 are photodiodes provided on the receiving side, and the IiJ optical symbol signals are converted into electrical signals by the diodes D3 and D4.

乙の信号により負荷抵抗R5、山の両端に脈流出力が発
生し、オペアンプIC1の出力負荷抵抗R7の両端には
第2図書に示す如き波形の脈流出力bが得られる。この
脈流出力す波形と変成器’rrの二次側出力aの波形と
の位相関係1よ、矢印で示すように、発光ダイオードD
1、D2に固有の閾値電圧Vthにより決まる。
The signal B generates a pulsating output at both ends of the load resistor R5, and a pulsating output b having a waveform as shown in Figure 2 is obtained at both ends of the output load resistor R7 of the operational amplifier IC1. According to the phase relationship 1 between this pulsating output waveform and the waveform of the secondary output a of the transformer 'rr, as shown by the arrow, the light emitting diode D
1, determined by the threshold voltage Vth specific to D2.

再び第1図に戻り、抵抗R3はフォトダイオードD5、
D4の出力電圧の平衡をとるため可変抵抗とし、抵抗R
5、R4、几5およびR6の各抵抗値の間にはR5/R
3= R6/R4t、x ;S関係’e モタセ”Ch
 7)。ICz、IC3、IC4およびICsはオペア
ンプである。オペアンプIO2は非反転帰還形のオペア
ンプで、抵抗Re 、R9によりオペアンプIC1の出
方電圧を1十R9/几8倍に増巾し、その出力を抵抗孔
10SA11テ分圧し、ダイオードD5により正の半波
のみを結合コンデンサC1を介して矩形波発振用マルチ
バイブレータとして作用するオペアンプICsに同期信
号として供給している。マルチバイブレークIC3の1
発振RKATは、コンデンサC2の容量値と抵抗Rsz
、R13、R14Mよび几15の抵抗値によりT=20
zR1zln 1+H−A  Nのように決まる。この
発振周期Tを第2図(a)に示す変成器Trの二次側出
力aの正弦波交流の周期と一致するように選んでおけば
、マルチバイブレータIC5の出力として、第2図(e
)に示すように、前記脈流出力すに同期した繰返し周期
Tの矩形波信号Cが得られる。この矩形波信号Cを抵抗
16.17により適当なレベルに分圧して矩形波信号C
′を得る。この矩形波信号C′と前記差動増巾器工C1
がらの脈流出力すとをオペアンプIC4に入力して差動
増巾すると、第2図ゆに示すJうに、奇数次高調波を含
有した歪波形交流dが得られる。なお、抵抗R18、R
19は次に述べるローパスアクティブフィルタFを飽和
させないよう低抵抗を使用する。このローパスアクティ
ブフィルタFは抵抗孔20.R21およびR22、コン
デンサ03.04とオペアンプ■C5とで構成されてい
て、そのしゃ新局波数は100Hzである。そして、商
用周波数の交流の第6高調波以上は減衰が大きく、基本
波成分のみが設定利得で出力されるため、抵抗R20と
コンデンサc5との積分時定数(c5・IL2o)で決
まる位相遅延をコンデンサC5と抵抗孔25とで構成さ
れる微分回路DFにより補正してやると、第2 図(e
) ニ示スような出力波形eが出力端子6とアース間に
得られる。
Returning to FIG. 1 again, the resistor R3 is a photodiode D5,
In order to balance the output voltage of D4, a variable resistor is used, and the resistor R
5, R4, R5/R between each resistance value of 5 and R6.
3= R6/R4t, x; S relation'e Motase"Ch
7). ICz, IC3, IC4 and ICs are operational amplifiers. The operational amplifier IO2 is a non-inverting feedback type operational amplifier, which amplifies the output voltage of the operational amplifier IC1 by 10R9/8 times using the resistors Re and R9, divides the output voltage into the resistor hole 10SA11, and uses the diode D5 to amplify the output voltage of the operational amplifier IC1. Only the half wave is supplied as a synchronizing signal to the operational amplifier ICs acting as a multivibrator for rectangular wave oscillation via the coupling capacitor C1. Multi-by-break IC3 1
Oscillation RKAT is determined by the capacitance value of capacitor C2 and resistance Rsz
, T=20 due to the resistance values of R13, R14M and 几15.
It is determined as zR1zln 1+H-A N. If this oscillation period T is selected to match the period of the sine wave alternating current of the secondary output a of the transformer Tr shown in FIG. 2(a), the output of the multivibrator IC5 is
), a rectangular wave signal C with a repetition period T that is synchronized with the pulsatile output is obtained. This rectangular wave signal C is divided into an appropriate level by resistors 16 and 17 to form a rectangular wave signal C.
′ is obtained. This square wave signal C' and the differential amplifier C1
When the pulsating current output from the filter is input to the operational amplifier IC4 and differentially amplified, a distorted waveform AC d containing odd harmonics is obtained as shown in FIG. In addition, the resistors R18, R
19 uses a low resistance so as not to saturate a low-pass active filter F, which will be described next. This low-pass active filter F has a resistor hole 20. It is composed of R21 and R22, a capacitor 03.04, and an operational amplifier C5, and its new station frequency is 100Hz. Since the 6th harmonic of AC at the commercial frequency and higher attenuation is large, and only the fundamental wave component is output with the set gain, the phase delay determined by the integral time constant (c5・IL2o) of resistor R20 and capacitor c5 is When the correction is made by the differential circuit DF consisting of the capacitor C5 and the resistor hole 25, the result shown in Fig. 2 (e
) An output waveform e as shown in the figure is obtained between the output terminal 6 and the ground.

この出力波形は変成器Trの二次側出力aの正弦波形と
全く相似である。
This output waveform is completely similar to the sine waveform of the secondary output a of the transformer Tr.

つまり、マルチバイブレータICsの出方である矩形波
出力Cを発光ダイオードDI、D2に特有の閾値電圧v
thに見合った適当な値に設定しておけば、変成器Tr
の出力が広範囲に変動しても常に比例関係を保つことが
できる。
In other words, the rectangular wave output C, which is the output of the multivibrator ICs, is converted to the threshold voltage v specific to the light emitting diodes DI and D2.
If you set it to an appropriate value commensurate with th, the transformer Tr
Even if the output varies over a wide range, a proportional relationship can always be maintained.

本発明によれば、変成器の二次側出方を発光ダイオード
に与え、正極性電圧、負極性電圧に対応してそれぞれ得
られる光信号を光ファイバを介してアナログ送信し、こ
の光信号を光ファイバの受信側で光電変換して得られた
電気信号を合成して得られる脈流出力に同期した矩形波
信号を発光ダイオードに固有の閾値電圧に比例しtコレ
ベルで前記脈流出力に加算し、この加算によって得らる
波形から高周波成分を除去するようにしtコので、変成
器の二次側出力に相似した歪の全くない正弦波交流を再
現することが可能となり、従って、精度の高い検出が可
能となる。
According to the present invention, the secondary side output of the transformer is applied to the light emitting diode, and the optical signals obtained in response to the positive polarity voltage and the negative polarity voltage are transmitted in analog form via the optical fiber, and the optical signals are transmitted in analog form through the optical fiber. A rectangular wave signal synchronized with the pulsating output obtained by combining the electrical signals obtained by photoelectric conversion on the receiving side of the optical fiber is added to the pulsating output at a level t in proportion to the threshold voltage specific to the light emitting diode. However, since high-frequency components are removed from the waveform obtained by this addition, it is possible to reproduce a completely distortion-free sine wave alternating current similar to the secondary output of the transformer, and therefore the accuracy is improved. High detection is possible.

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

第1図は、本発明の一実施例を示す回路図、第2図は本
発明の詳細な説明するための波形図である。 Tr・・・変成器   Dl、D2・・・発光ダイオー
ドF1、F2・・・光ファイバ、 a・・・変成器の二
次側出力b・・・脈流出力   c、 c’・・・矩形
波信号e・・・出力波形 特許出願人 日新電機株式会社 (ほか1名)
FIG. 1 is a circuit diagram showing one embodiment of the present invention, and FIG. 2 is a waveform diagram for explaining the present invention in detail. Tr... Transformer Dl, D2... Light emitting diodes F1, F2... Optical fiber a... Secondary output of transformer b... Pulsating output c, c'... Square wave Signal e...Output waveform Patent applicant Nissin Electric Co., Ltd. (and one other person)

Claims (1)

【特許請求の範囲】[Claims] 変成器の二次側出力を発光ダイオードに与え正極性電圧
、負極性電圧に対応してそれぞれ得られる光信号を光フ
ァイバを用いてアナログ伝送するようにし1こものにお
いて、前記光ファイバの受信側で前記光信号に基づく電
気信号を合成して得られる脈流出力に同期した矩形波信
号を発生させ、この矩形波信号を前記発光ダイオードに
固有の閾値電圧に比例したレベルで前記脈流出力に加算
し、この加算によって得られる波形から高調波成分を除
去することにより前記二次側出力に相似した出力波形を
得るようにしてなる光変成器。
The secondary output of the transformer is applied to a light emitting diode, and the optical signals obtained in response to positive polarity voltage and negative polarity voltage are transmitted in analog form using an optical fiber. generates a rectangular wave signal synchronized with the pulsating output obtained by combining electrical signals based on the optical signal, and applies this rectangular wave signal to the pulsating output at a level proportional to a threshold voltage specific to the light emitting diode. An optical transformer that obtains an output waveform similar to the secondary side output by adding the above-mentioned secondary side outputs and removing harmonic components from the waveform obtained by the addition.
JP57118264A 1982-07-06 1982-07-06 Optical transformer Granted JPS598439A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP57118264A JPS598439A (en) 1982-07-06 1982-07-06 Optical transformer

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP57118264A JPS598439A (en) 1982-07-06 1982-07-06 Optical transformer

Publications (2)

Publication Number Publication Date
JPS598439A true JPS598439A (en) 1984-01-17
JPH0148704B2 JPH0148704B2 (en) 1989-10-20

Family

ID=14732321

Family Applications (1)

Application Number Title Priority Date Filing Date
JP57118264A Granted JPS598439A (en) 1982-07-06 1982-07-06 Optical transformer

Country Status (1)

Country Link
JP (1) JPS598439A (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63200888A (en) * 1987-02-16 1988-08-19 Unitika Ltd Removal of phosphorus contained in water
JPH02309828A (en) * 1989-05-25 1990-12-25 Mitsubishi Electric Corp Drive method for laser diode and laser diode module

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63200888A (en) * 1987-02-16 1988-08-19 Unitika Ltd Removal of phosphorus contained in water
JPH0712477B2 (en) * 1987-02-16 1995-02-15 ユニチカ株式会社 How to remove phosphorus in water
JPH02309828A (en) * 1989-05-25 1990-12-25 Mitsubishi Electric Corp Drive method for laser diode and laser diode module

Also Published As

Publication number Publication date
JPH0148704B2 (en) 1989-10-20

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