JPS6041333A - Transmitter for power line carrier - Google Patents
Transmitter for power line carrierInfo
- Publication number
- JPS6041333A JPS6041333A JP14979183A JP14979183A JPS6041333A JP S6041333 A JPS6041333 A JP S6041333A JP 14979183 A JP14979183 A JP 14979183A JP 14979183 A JP14979183 A JP 14979183A JP S6041333 A JPS6041333 A JP S6041333A
- Authority
- JP
- Japan
- Prior art keywords
- power line
- impedance
- output
- capacitor
- frequency
- 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
Links
Classifications
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B3/00—Line transmission systems
- H04B3/54—Systems for transmission via power distribution lines
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B2203/00—Indexing scheme relating to line transmission systems
- H04B2203/54—Aspects of powerline communications not already covered by H04B3/54 and its subgroups
- H04B2203/5404—Methods of transmitting or receiving signals via power distribution lines
- H04B2203/5416—Methods of transmitting or receiving signals via power distribution lines by adding signals to the wave form of the power source
-
- H—ELECTRICITY
- H04—ELECTRIC COMMUNICATION TECHNIQUE
- H04B—TRANSMISSION
- H04B2203/00—Indexing scheme relating to line transmission systems
- H04B2203/54—Aspects of powerline communications not already covered by H04B3/54 and its subgroups
- H04B2203/5404—Methods of transmitting or receiving signals via power distribution lines
- H04B2203/5425—Methods of transmitting or receiving signals via power distribution lines improving S/N by matching impedance, noise reduction, gain control
Landscapes
- Engineering & Computer Science (AREA)
- Power Engineering (AREA)
- Computer Networks & Wireless Communication (AREA)
- Signal Processing (AREA)
- Cable Transmission Systems, Equalization Of Radio And Reduction Of Echo (AREA)
Abstract
Description
【発明の詳細な説明】
産業上の利用分野
本発明(は電力線に所定周波数の搬送波信号を重畳させ
ることにより通信を行う電力線搬送用送信機に関するも
のである。DETAILED DESCRIPTION OF THE INVENTION Field of the Invention The present invention relates to a power line carrier transmitter that performs communication by superimposing a carrier signal of a predetermined frequency on a power line.
従来例の構成とその問題点
従来の電力線搬送用送信機は、第1図に示す様に、発振
器1の出力を増幅器2で増幅し、その出力を出カドラン
ス3を用いて、電力線4とインピーダンスマツチングを
行い、コンデンサ6により商用周波数のカットを行い、
搬送波信号を電力線4に重畳させていた。一般に電力線
4の高周波インピーダンスは数オーム(最悪の場合は1
Ω以下)と低いため、送信機の出力インピーダンスを低
くしないと、送信効率が低下してしまう。ところが、い
くら出カドランス3を調整してインビータンスを低下さ
せても、出カドランス3と電力線4の間にコンデンサ5
があるため、出力インビータンスはコンデンサ5のイン
ピーダンスよりも下げることができない。コンデンサ6
は商用周波数をカットすることが目的であるから、商用
周波数におけるインピーダンスは十分大きくなければな
らない。Configuration of the conventional example and its problems In the conventional power line carrier transmitter, as shown in FIG. Matching is performed, and the commercial frequency is cut using capacitor 6.
A carrier signal was superimposed on the power line 4. Generally, the high frequency impedance of the power line 4 is several ohms (in the worst case, 1
Ω or less), so unless the output impedance of the transmitter is lowered, the transmission efficiency will decrease. However, no matter how much you adjust the output transformer 3 to lower the impedance, the capacitor 5 remains between the output transformer 3 and the power line 4.
Therefore, the output impedance cannot be lowered below the impedance of the capacitor 5. capacitor 6
Since the purpose of this is to cut commercial frequencies, the impedance at commercial frequencies must be sufficiently large.
したがって、極端に容量を大きくすることもできない。Therefore, it is not possible to increase the capacity extremely.
加えて商用電源が印加されるために耐電圧も大きくなけ
ればならない。つまり、大容量、高耐圧の高価なコンデ
ンサを使用しても、出力インピーダンスをあ址り下げる
ことができない。その結果、電力線4のインピーダンス
変化に応じて、出力電圧が変化し、インピーダンスが低
い時は出力電圧が小さくなり、伝送距離が短かくなり、
インピーダンスが高い時は出力電圧が大きくなり、所定
の伝送範囲外にまで信号が漏洩すること力玉アる。In addition, since commercial power is applied, the withstand voltage must be high. In other words, even if an expensive capacitor with a large capacity and high voltage resistance is used, the output impedance cannot be lowered. As a result, the output voltage changes according to the impedance change of the power line 4, and when the impedance is low, the output voltage becomes small and the transmission distance becomes short.
When the impedance is high, the output voltage becomes large, causing signal leakage outside the specified transmission range.
発明の目的
本発明は、これらの欠点を解決したもので、出力インピ
ーダンスの低下と、商用周波数カット用コンデンサの小
型化が可能な、電力線搬送用送信機を提供することを目
的としている。OBJECTS OF THE INVENTION The present invention solves these drawbacks, and aims to provide a power line carrier transmitter that can reduce the output impedance and downsize the commercial frequency cutting capacitor.
発明の構成
本発明の電力線搬送用送信機は、電力線に所定周波数の
搬送波信号を重畳させて送信を行う送信機の出力と、電
力線の間に前記所定周波数を共振する直列共振回路を接
続したものである。Structure of the Invention The power line carrier transmitter of the present invention has a series resonant circuit connected between the output of a transmitter that superimposes a carrier signal of a predetermined frequency on a power line and transmits the same, and the power line to resonate the predetermined frequency. It is.
実施例の説明
以下、第2図にもとづいて本発明の一実施例を説明する
。搬送信号を発生する発振器6の出力信号を増幅する増
幅器7の出力インピーダンスは、電力線12の信号周波
数に於けるインピーダンスに比べるとか々り高いので出
カドランス8を使用し、出カドランス8の2次fAII
の出力インピーダンスを信号周波数に於ける電力線12
のインピーダンスとほぼ同じ、数オームに設定する。コ
イル9とコンデンサ1oの直列接続からなる直列共振回
路11ば、送信機の出力と、電力純量に接続しておシ、
その共振周波数は信号周波数と一致させである。したが
って直列共振回路11のインピーダンスは、出カドラン
ス8の出力インピーダンスよりも小さくなる。このため
、この送信機の総合的な出力インピーダンスはラインイ
ンピーダンスとほぼ等しくなる。つまり送信機の出力イ
ンピーダンスと電力線12のインピーダンスの整合がと
れていることになり出力効率が改善される。以下に実際
に数値を代入して効率を割算する。DESCRIPTION OF THE EMBODIMENTS An embodiment of the present invention will be described below with reference to FIG. The output impedance of the amplifier 7 that amplifies the output signal of the oscillator 6 that generates the carrier signal is much higher than the impedance at the signal frequency of the power line 12.
The output impedance of the power line 12 at the signal frequency
Set the impedance to several ohms, which is approximately the same as the impedance. A series resonant circuit 11 consisting of a series connection of a coil 9 and a capacitor 1o is connected to the output of the transmitter and the pure amount of electric power.
Its resonant frequency should match the signal frequency. Therefore, the impedance of the series resonant circuit 11 is smaller than the output impedance of the output transformer 8. Therefore, the overall output impedance of this transmitter is approximately equal to the line impedance. In other words, the output impedance of the transmitter and the impedance of the power line 12 are matched, and output efficiency is improved. Substitute the actual values below and divide the efficiency.
例として、電源周波数eoHz、電源電圧100V、搬
送波信号周波数120KHz、搬送波信号周波数に於け
る電力線インピーダンス1Ω、出カドランス8の出力イ
ンピーダンス1Ωと仮定する。As an example, it is assumed that the power supply frequency is eoHz, the power supply voltage is 100V, the carrier wave signal frequency is 120 KHz, the power line impedance at the carrier wave signal frequency is 1Ω, and the output impedance of the output transformer 8 is 1Ω.
従来例の場合、コンデンサ6の容量を0.1μFとすれ
ば、コンデンサ5の120KH2に於けるインピーダン
スは、
1/2XyrX120X105X0.lX10 ’4=
13.26(Ω)となり、総合的な出力インピーダンス
の絶対値はバエ■震3’=13.3(Ω)
となる。従って、出カドランス802次側に0.1■の
信号が発生していた場合の電力線に注入される信号は、
o、1×□二〇、007(V)
13.3 +’1 +1
となり、非常に弱いものである。In the case of the conventional example, if the capacitance of the capacitor 6 is 0.1 μF, the impedance of the capacitor 5 at 120KH2 is 1/2XyrX120X105X0. lX10'4=
13.26 (Ω), and the absolute value of the overall output impedance is 3' = 13.3 (Ω). Therefore, when a signal of 0.1■ is generated on the secondary side of the output transformer 80, the signal injected into the power line is o, 1 x 20, 007 (V) 13.3 +'1 +1, It is very weak.
一方、本発明を利用した場合は、直列共振回路11のイ
ンピーダンスを1Ωとしても、総合的な出力インピーダ
ンスは
1+1=2(Ω)
となり、出力電圧0,1 Vの時の電力線への注入電圧
は、
1+、+1−0.o3(v)
トナシ、従来例に比へ4.3倍も改善されることがわか
る。On the other hand, when the present invention is used, even if the impedance of the series resonant circuit 11 is 1Ω, the overall output impedance is 1+1=2(Ω), and the voltage injected into the power line when the output voltage is 0.1 V is , 1+, +1-0. It can be seen that o3(v) is improved by 4.3 times compared to the conventional example.
従来例の場合の注入電圧では、電力線上の雑音との区別
ができなくなるので出カドランスの2次側の出力電圧を
大きくしておくことが必要となる。With the injection voltage used in the conventional example, it becomes impossible to distinguish noise from noise on the power line, so it is necessary to increase the output voltage on the secondary side of the output transformer.
そうした場合、電力線のインピーダンスが上昇した時に
は、その電圧が、減衰することなく電力線に注入される
ので所定の範囲外にまで信号が到達し、他のシステムに
防害を与える可能性もある。In such a case, when the impedance of the power line increases, the voltage is injected into the power line without attenuation, and the signal may reach outside the predetermined range, potentially harming other systems.
直列共振回路11の共振時のインピーダンスは実際には
コンデンサ10の値が大きい程、小さくなるが、従来例
の様な大容量のコンデンサは必要でなく、発明者の実験
によると、コンデンサ1゜の値はコンデンサ5の値の1
/10程度でも十分な機能を果すことが確かめられてい
る。The impedance of the series resonant circuit 11 during resonance actually decreases as the value of the capacitor 10 increases, but a capacitor with a large capacity as in the conventional example is not necessary, and according to the inventor's experiments, a capacitor of 1° The value is 1 of the value of capacitor 5
It has been confirmed that even a ratio of about /10 can function satisfactorily.
また、搬送波の信号波形が完全な正弦波でない場合、搬
送波の高周波、低周波に対する直列共振回路11のイン
ピーダンスは大きいだめ、基本波以外の成分は、直列共
振回路11を通過できず、電力線12に注入される電圧
が小さくなる。このだめ、増幅器7の直線性もあまI)
要求されない。Furthermore, if the signal waveform of the carrier wave is not a perfect sine wave, the impedance of the series resonant circuit 11 with respect to the high and low frequencies of the carrier wave is large, and components other than the fundamental wave cannot pass through the series resonant circuit 11 and are transmitted to the power line 12. The injected voltage becomes smaller. Unfortunately, the linearity of amplifier 7 is also poor.
Not required.
発明の詳細
な説明したように、本発明の電力線搬送用送信機は、電
力線のインピーダンスが変化しても、信号注入電圧があ
まり変化なく、注入効率が非常に高く、小型の商用周波
数カット用のコンデンサでよく、回路全体が小さく安価
なものとすることができる。As described in detail, the power line carrier transmitter of the present invention has very high injection efficiency, with the signal injection voltage not changing much even when the impedance of the power line changes, and is suitable for use in small commercial frequency cutting applications. A capacitor may be sufficient, and the entire circuit can be made small and inexpensive.
第1図は従来例を示す回路図、第2図は本発明の一実施
例を示す電力線搬送用送信機の回路図である。
9・・・・・コイル、10・・・・・コンデンサ、11
・・・・・直列共振回路、12・・・・・・電力線。
代理人の氏名 弁理士 中 尾 敏 男 ほか1名第1
図FIG. 1 is a circuit diagram showing a conventional example, and FIG. 2 is a circuit diagram of a power line carrier transmitter showing an embodiment of the present invention. 9... Coil, 10... Capacitor, 11
...Series resonant circuit, 12...Power line. Name of agent: Patent attorney Toshio Nakao and 1 other person No. 1
figure
Claims (1)
う送信機の出力と電力線の間に前記所定周波数で共振す
る直列共振回路を接続した電力線搬送用送信機。A power line carrier transmitter comprising a series resonant circuit that resonates at the predetermined frequency connected between the power line and the output of a transmitter that transmits by superimposing a carrier signal of a predetermined frequency on the power line.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14979183A JPS6041333A (en) | 1983-08-17 | 1983-08-17 | Transmitter for power line carrier |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP14979183A JPS6041333A (en) | 1983-08-17 | 1983-08-17 | Transmitter for power line carrier |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6041333A true JPS6041333A (en) | 1985-03-05 |
Family
ID=15482791
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP14979183A Pending JPS6041333A (en) | 1983-08-17 | 1983-08-17 | Transmitter for power line carrier |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6041333A (en) |
-
1983
- 1983-08-17 JP JP14979183A patent/JPS6041333A/en active Pending
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