JPS6139634A - Higher harmonic noise removing method - Google Patents

Higher harmonic noise removing method

Info

Publication number
JPS6139634A
JPS6139634A JP15874484A JP15874484A JPS6139634A JP S6139634 A JPS6139634 A JP S6139634A JP 15874484 A JP15874484 A JP 15874484A JP 15874484 A JP15874484 A JP 15874484A JP S6139634 A JPS6139634 A JP S6139634A
Authority
JP
Japan
Prior art keywords
signal
circuit
sampling
wave
inputted
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
JP15874484A
Other languages
Japanese (ja)
Other versions
JPH0234531B2 (en
Inventor
Mitsuaki Fukushima
福島 光明
Satoshi Komazawa
駒沢 聰
Etsuro Nakayama
悦郎 中山
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.)
OSAKI DENKI KOGYO KK
Osaki Electric Co Ltd
Original Assignee
OSAKI DENKI KOGYO KK
Osaki 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 OSAKI DENKI KOGYO KK, Osaki Electric Co Ltd filed Critical OSAKI DENKI KOGYO KK
Priority to JP15874484A priority Critical patent/JPH0234531B2/en
Publication of JPS6139634A publication Critical patent/JPS6139634A/en
Publication of JPH0234531B2 publication Critical patent/JPH0234531B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B3/00Line transmission systems
    • H04B3/54Systems for transmission via power distribution lines
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B2203/00Indexing scheme relating to line transmission systems
    • H04B2203/54Aspects of powerline communications not already covered by H04B3/54 and its subgroups
    • H04B2203/5404Methods of transmitting or receiving signals via power distribution lines
    • H04B2203/5425Methods of transmitting or receiving signals via power distribution lines improving S/N by matching impedance, noise reduction, gain control
    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B2203/00Indexing scheme relating to line transmission systems
    • H04B2203/54Aspects of powerline communications not already covered by H04B3/54 and its subgroups
    • H04B2203/5462Systems for power line communications
    • H04B2203/5491Systems for power line communications using filtering and bypassing

Abstract

PURPOSE:To remove the higher harmonic wave of AC wave that becomes noises and to enable transmission of high-speed data in a system that uses a power line as a signal transmission line by subtracting a received signal of one period before of AC wave from the received signal. CONSTITUTION:Received signals inputted from an input terminal 1 are inputted to a sampling circuit 3 through a filter 2. The sampling circuit 3 makes sampling based on sampling pluse from a pulse generating circuit 5 and the result is inputted to a storing circuit 6 and an arithmetic circuit 7. The storing circuit 6 stores the input and outputs the result of sampling of one period before of AC wave based on inputted sampling pulse to an arithmetic discriminating circuit 7. The arithmetic discriminating circuit 7 subtracts the inputted signal from the storing circuit 6 from the inputted signals from the sampling circuit 3 and outputs to an output terminal 8.

Description

【発明の詳細な説明】 (発明の利用分野) 本発明は、電力線搬送信号の受信時に問題となる高調波
雑音の除去方法に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Field of Application of the Invention) The present invention relates to a method for removing harmonic noise that is a problem when receiving power line carrier signals.

(発明の背景) 交流波が印加される電力線路を信号伝送路とし、交流波
に信号を重畳させてデータの伝送゛を行う電力線搬送に
おいては、電力線路に接続される負荷機器などに起因す
る交流波の高調波雑音が存在し、信号の受信、復調時に
大きな障害となる。従来、この高調波雑音の除去方法と
しては、受信器側にフィルタを設け、伝送される信号の
周波数付近以外の周波数をもつ雑音をフィルタによりカ
ットする方法が一般に用いられている。ところが一方、
データ伝送速度は、信号の伝送帯蛾に比例する。すなわ
ち、データ伝送速度をあげるためには、受信器側のフィ
ルタの帯域幅を広く設定する必要がある。したがって、
データ伝送速度をあげ、かつ、高調波雑音を除去してS
/N比を許容値以上にするためには、フィルタに非常に
急峻なしゃ所持性を持たせる必要があるが、このような
特性を満足するフィルタを製作することは、素子数、形
状1価格、調整の点から、実現困難である。このことが
、現在の電力線搬送信号のデータ伝送速度が1〜10 
(bit/ sec )におさえられている大きな理由
の一つとなっている。
(Background of the Invention) In power line transmission, in which a power line to which alternating current waves are applied is used as a signal transmission path, and data is transmitted by superimposing signals on the alternating current waves, there are Harmonic noise of alternating current waves exists and becomes a major obstacle during signal reception and demodulation. Conventionally, as a method for removing harmonic noise, a method has generally been used in which a filter is provided on the receiver side and noise having a frequency other than the frequency of the transmitted signal is cut by the filter. However, on the other hand,
The data transmission rate is proportional to the signal transmission band. That is, in order to increase the data transmission speed, it is necessary to set the bandwidth of the filter on the receiver side to be wide. therefore,
Increase data transmission speed and remove harmonic noise
In order to make the /N ratio more than the allowable value, it is necessary for the filter to have extremely steep characteristics, but manufacturing a filter that satisfies such characteristics requires a small number of elements, shape, and price. , which is difficult to realize from the point of view of coordination. This means that the data transmission rate of current power line carrier signals is 1 to 10
This is one of the major reasons why it is kept at a low level (bit/sec).

(発明の目的) 本発明の目的は、上述した問題点を解決し、従来に比し
て高速度のデータ伝送を可能とする高調波雑音除去方法
を提供することである。
(Objective of the Invention) An object of the present invention is to provide a harmonic noise removal method that solves the above-mentioned problems and enables data transmission at a higher speed than conventional methods.

(線切の特徴) 上記目的を達成するために、本発明は、交流波が印加さ
れる電力線路を信号伝送路とし、交流波に重畳されて送
信されてくる信号を受信するに際して、受信信号から、
前記交流波の一周期分前の受信信号を減算するようにし
、以て、雑音となる交流波の高調波が基本波と同期して
いることを利用して、高調波のみを除去するようにした
ことを特徴とする。
(Characteristics of line cutting) In order to achieve the above object, the present invention uses a power line to which an alternating current wave is applied as a signal transmission path, and when receiving a signal superimposed on the alternating current wave and transmitted, the received signal from,
The received signal of one cycle of the alternating current wave is subtracted, and by taking advantage of the fact that the harmonics of the alternating current wave, which become noise, are synchronized with the fundamental wave, only the harmonics are removed. It is characterized by what it did.

(発明の実施例) 以下、本発明を図面を用いて詳細に説明する。(Example of the invention) Hereinafter, the present invention will be explained in detail using the drawings.

第2図ta>に、電力線路に印加される交流波の波形を
、第2図(b)に、交流波に混入する高調波雑音の波形
を示す。高調波雑音は、いくつかの異なる次数の高調波
の相であり、複雑な波形を示しているが、図示した通り
、基本波である交流波に位相的に同期している。したが
って受信信号から、交流波の一周期分前の受信信号を減
算すれば、高調波雑音が除去されることになる。
FIG. 2(a) shows the waveform of the AC wave applied to the power line, and FIG. 2(b) shows the waveform of harmonic noise mixed into the AC wave. Harmonic noise is a phase of harmonic waves of several different orders and has a complex waveform, but as shown in the figure, it is phase-synchronized with the alternating current wave that is the fundamental wave. Therefore, by subtracting the received signal of one cycle of the AC wave before the received signal, harmonic noise can be removed.

このことを式で表すと、次のとおりである。This can be expressed as follows.

8 (t)を伝送される信号、N(tlを高調波雑音と
すると、受信器側の受信信号’E(tlは次のように表
される。
8 (t) is the transmitted signal and N(tl is the harmonic noise), then the received signal 'E(tl) on the receiver side is expressed as follows.

E(tl = 5(t)+N(t)         
     (1)この受信信号E(t)から、交流波の
一周期分前の受信信号を減算して得られる信号E+(t
lは、交流波の周期をTとすると、 &(t)−E(tl  E(t  T)= 5(tl十
N(t) −(S(t−T )+N(t−T) ) (
2)ここで、高調波雑音N (t)は交流波に同期して
いるから、 N(t) = N (t−T )          
   (3)したがって式(2)1式(3)より。
E(tl = 5(t)+N(t)
(1) Signal E+(t
If the period of the alternating current wave is T, then &(t)-E(tl E(tT)=5(tl+N(t)-(S(t-T)+N(t-T))(
2) Here, since the harmonic noise N (t) is synchronized with the AC wave, N(t) = N (t-T)
(3) Therefore, from equation (2)1 equation (3).

El(t)=S(t)−8(t−’r )      
      (4)となり、高調波雑音N(t)が除去
される。なお、以上の説明及び第2図は、高調波雑音N
(tlが定常状態にある場合を示したが、実際には、高
調波雑音Nft)の原因となる電力線路の負荷の、接続
状態の変化により、高調波雑音Nft1が変動する場合
がある。しかし、この変動分は高調波雑音N(t)全体
に比べればわずかであり、減算した結果の信号1りに残
るのは交流波の一周期前からの変動分のみであるから、
大きな問題とはならず、S/Nは十分な値が得られる。
El(t)=S(t)-8(t-'r)
(4), and the harmonic noise N(t) is removed. The above explanation and FIG. 2 are based on the harmonic noise N
(Although the case where tl is in a steady state is shown, in reality, the harmonic noise Nft1 may fluctuate due to a change in the connection state of the load on the power line that causes the harmonic noise Nft). However, this variation is small compared to the entire harmonic noise N(t), and what remains in the subtracted signal is only the variation from one cycle before the AC wave.
This is not a major problem, and a sufficient S/N value can be obtained.

次に、式(4)で表される信号E+(t)によって、伝
送される信号5(tlによるデータが正しく伝えられる
ための条件を考える。
Next, we will consider the conditions for the data to be correctly transmitted by the signal 5 (tl) to be transmitted by the signal E+(t) expressed by equation (4).

まず条件の第1として、伝送される信号5(t)が、交
流波に同期していないようにすることがあげられる。も
し同期しているとすると、高調波雑音の場合と同様、信
号S (t)も、減算処理により除去されてしまい、式
(4)のEITt)の値が0になってしまうからである
The first condition is that the signal 5(t) to be transmitted is not synchronized with the alternating current wave. This is because if they were synchronized, the signal S (t) would also be removed by subtraction processing, as in the case of harmonic noise, and the value of EITt) in equation (4) would become 0.

次いで、信号E+ft)によるデータの符号値と。Then, the code value of the data according to the signal E+ft).

信号5(t)によるデータの符号値が一致するための条
件を考える。信号5(t)の例として、FSK信号(f
requency 5hift keying )の場
合を考える。すなわち、信号S (tlが としてり、えられる場合である(ω&l:マーク信号角
周波数、ω、ニスペース信号角周波数、A:信号振幅)
。この信号S (t)を、式(4)に適用した減算結果
El(tlは、次の4通りに分類される。
Consider the conditions for the code values of data based on signal 5(t) to match. As an example of signal 5(t), the FSK signal (f
Consider the case of 5hift keying). That is, this is the case where the signal S (tl is obtained) (ω & l: mark signal angular frequency, ω, space signal angular frequency, A: signal amplitude)
. The subtraction result El(tl) obtained by applying Equation (4) to this signal S (t) is classified into the following four types.

囚 信号S (tlの符号が、時刻tのときマー久1サ
イクル前の時刻t−Tのときもマークの場合。
Prison signal S (If the sign of tl is a mark at time t, it is also a mark at time t-T, one cycle before.

El (j) = Asln% t−As1aωm(t
T)(6)時刻tのときスペース、時刻t −Tのとき
もスペースの場合。
El (j) = Asln% t-As1aωm(t
T) (6) When time t is a space and time t -T is also a space.

El (il = As1aωg t −As1nω5
(tT)(O時刻tのときマーク、時刻t−Tのときス
ペースの場合。
El (il = As1aωg t −As1nω5
(tT) (O mark at time t, space at time t-T.

El(jl=Asincht−As1nω5(tT)■
 時刻tのときスペース、時刻t−Tのときマークの場
合。
El(jl=Asincht-As1nω5(tT)■
In the case of a space at time t and a mark at time t-T.

E+ (1= As1nω5t−As1aωc(t−’
r)ωg−ω1  ωMT = 2 As1a (−t +−) 減算結果から求まる信号E+(t)は、囚、@の場合は
それぞれ角周波数がωヨ又はω8に一義的に定まるため
、これから、もとの信号S (tlの符号の判別が可能
となる。ところが(0,0の場合はともに信号El (
t)の角周波数は一義的に定まらず、マーク周波数、ス
ペース周波数の中心周波数をもつ信号を振幅変調した波
形となるため、もとの信号S (t)の符号の判別がで
きない。この符号判別の不可能な区間の幅は、最大T(
交流波の一周期分)であるから、信号Et(tlから、
信号5(tlの符号を判別するための条件として、信号
5(tlの符号長は交流波の一周期分では不足で、最低
二周期分必要であることがわかる。第1図に、交流波及
び、信号S (t) 、信号g+(lの符号のタイミン
グ例を示した。fatが交流波、(blが信号S (t
)、tc+が交流波の1サイクル分前の信号5(t−T
)、(d)が、(blからfc)を減算して得られる信
号El(t)の符号である。ここには、信号S (t)
の符号長が交流波の三周切分である例を示し、た。
E+ (1= As1nω5t-As1aωc(t-'
r) ωg-ω1 ωMT = 2 As1a (-t +-) The signal E+(t) found from the subtraction result is uniquely determined to have an angular frequency of ωyo or ω8 in the case of @ and @, so from now on, It becomes possible to determine the sign of the signal S (tl). However, in the case of (0, 0, both the signal El (
The angular frequency of t) is not uniquely determined, and the waveform is obtained by amplitude modulating a signal having the center frequencies of the mark frequency and the space frequency, so the sign of the original signal S (t) cannot be determined. The width of this interval in which it is impossible to determine the sign is the maximum width T(
Since the signal Et (from tl,
As a condition for determining the sign of signal 5(tl), it can be seen that the code length of signal 5(tl is insufficient for one cycle of the AC wave, and requires at least two cycles. Also, timing examples of the signs of the signal S (t) and the signal g+(l are shown. fat is an AC wave, (bl is the signal S (t
), tc+ is the signal 5 (t-T
), (d) are the signs of the signal El(t) obtained by subtracting (bl from fc). Here, the signal S (t)
An example is shown in which the code length of is the third cycle of the alternating current wave.

さらに、信号El(tlにより信号S (t)の符号を
正確に判別するための、次の条件を考える。信号ltl
により信号S (t)の符号が判別可能な(4)、■)
2 As1n−”Z−である。符号の正確な判別には、
この振幅ができるだけ大きいことが望ましい。この振幅
は、fを交流波周波数、「ヨをマーク信号周波数、f、
をスペース信号周波数とすると、次のように書き直せる
Furthermore, consider the following conditions for accurately determining the sign of the signal S (t) using the signal El(tl. The signal ltl
The sign of the signal S (t) can be determined by (4), ■)
2 As1n-”Z-.To accurately determine the sign,
It is desirable that this amplitude be as large as possible. This amplitude is determined by where f is the alternating wave frequency, y is the mark signal frequency, f,
Letting be the space signal frequency, it can be rewritten as follows.

したがつ【、振幅なできるだけ大きくするには、  f
M/f及びra/rの値を、yc+%(rL:整数)に
できるだけ近くすることが必要である。
Therefore, to make the amplitude as large as possible, f
It is necessary to make the values of M/f and ra/r as close as possible to yc+% (rL: integer).

以上の条件をまとめて整理すると、次の通りである。The above conditions can be summarized as follows.

(1)  伝送される信号S (tlが交流波に同期し
ていないこと。
(1) The transmitted signal S (tl) is not synchronized with the AC wave.

(2)信号S (t)の符号長は、最低交流波の三周切
分とすること。
(2) The code length of the signal S (t) shall be the minimum of three cycles of the AC wave.

(3)マーク信号周波数fu、スペース信号周波数fm
の値は、交流波周波数fとの比fw / f 、 f+
 /fの値が、ともにル十%(ル:整数)にできるだけ
近くなるように定めること。
(3) Mark signal frequency fu, space signal frequency fm
The value of is the ratio fw/f to the alternating current wave frequency f, f+
The values of /f shall be determined so that both values are as close as possible to 10% (where 1 is an integer).

以上の条件下において、受信信号E (t)から。Under the above conditions, from the received signal E(t).

交流波の一周期分前の信号E(t−T)を減算して得ら
れる。高調波雑音の除去された信号E。
It is obtained by subtracting the signal E(t-T) of one cycle of the alternating current wave. Signal E with harmonic noise removed.

+11を用いれば、伝送される信号S (t)の符号を
正確に判別することができる。これによるデータ伝送速
度は、条件(2)によつ【、交流波の周期が50(Hz
)であれば、最高25 Cbit/sec )とナリ、
従来の1〜10 Cbit/sec 〕と比して格段に
上昇する。
+11, it is possible to accurately determine the sign of the transmitted signal S (t). The data transmission speed due to this is based on condition (2) [, and the period of the AC wave is 50 (Hz).
), the maximum is 25 Cbit/sec),
This is a significant increase compared to the conventional 1 to 10 Cbit/sec.

なお、前述した(1)〜(3)の条件を導く際、信号S
(りの例としてFSX信号の場合について説明したが1
本発明の信号S (t)は、FSK信号に限られるもの
ではなく、他の信号でも同様に適用できる。以下に、信
号5(t)にASK信号(amp l 1−tude 
5hift keying ) 、 P S K信号(
phase shiftkeying )を用いた場合
について、簡単に説明する。
In addition, when deriving the conditions (1) to (3) mentioned above, the signal S
(As an example, we explained the case of FSX signal, but 1
The signal S (t) of the present invention is not limited to the FSK signal, but can be similarly applied to other signals. Below, the ASK signal (amp l 1-tude
5hift keying), PSK signal (
A case in which phase shiftkeying is used will be briefly explained.

信号5(t)に1次の式で表されるASK信号を用いた
場合を考える。
Consider a case where an ASK signal expressed by a linear equation is used as the signal 5(t).

(ωC:信号角周波数、A;信号振幅)減算結果El(
tlは次の通りである。
(ωC: signal angular frequency, A: signal amplitude) Subtraction result El (
tl is as follows.

囚 時刻tのときマーク、時刻t−Tのときもマークの
場合 E+ (t) = As1IIωc t −As1aω
c(tT)(B)  時刻tのときスペース、時刻t−
Tのときもスペースの場合 El(t)=0 0=OQ4) 0 時刻tのときマーク、時刻t−Tのときスペースの
場合 ’& (it = As1nωc t −0= As1
nωc t       Q5)■ 時刻tのときスペ
ース、時刻t−Tのときマークの場合 El(リ−OAs1aωa(t−’r)”=  As1
aωc(t−’r)        (Ife囚の場合
の振幅2 As1a (ωCT/2)が2人となるよう
信号角周波数ω。を定め、スライスレベルをAとすると
、FSX信号の場合と同様に、囚がマーク、(6)がス
ペースと判別され、(Q、■は判別不可となる。
If there is a mark at time t and a mark at time t-T, then E+ (t) = As1IIωc t −As1aω
c(tT)(B) Space at time t, time t-
If T is also a space, then El (t) = 0 0 = OQ4) 0 If time is a mark, if time is t - T, if it is a space, '& (it = As1nωc t -0 = As1
nωc t Q5)■ In the case of a space at time t and a mark at time t-T, El(Le-OAs1aωa(t-'r)"= As1
aωc(t-'r) (amplitude 2 in case of Ife prisoners As1a (ωCT/2)) is determined so that there are two people, and the slice level is set to A. As in the case of the FSX signal, The prisoner is determined to be a mark, (6) is determined to be a space, and (Q, ■ cannot be determined).

また、信号S (tlに次の式で表されるPSK信号を
用いた場合を考える。
Also, consider a case where the signal S (tl is a PSK signal expressed by the following equation).

(ωC:信号角周波数、A:信号振幅)減算結果El 
(tlは次の通りである。
(ωC: Signal angular frequency, A: Signal amplitude) Subtraction result El
(tl is as follows.

囚 時刻tのときマーク、時刻t−Tのときもマークの
場合 El (t) ”= As1nωc t−A、si6ω
c(tT)■)時刻tのときスペース、時刻t−Tのと
きもスペースの場合 El (t) =AsinωcT (As1IIωc(
tT))0 時刻tのときマーク、時刻t−Tのときス
ペースの場合 El (tl = As1aωct(As1nωc(t
  T))0、時刻tのときスペース、時刻t−Tのと
きマークの場合 El (i) =  As1nωc t −As1aω
a(t−’r)(4)の場合の信号El(tlの位相が
マークであるとすると、(B)はスペースと判別され、
(0,0は判別不可となって、この場合もFSX信号の
場合と同様である。
If there is a mark at time t and a mark at time t-T, then El (t) ”= As1nωc t-A, si6ω
c(tT) ■) If there is a space at time t and a space at time t-T, then El (t) = AsinωcT (As1IIωc(
tT))0 Mark at time t, space at time t-T El (tl = As1aωct(As1nωc(t
T)) 0, space at time t, mark at time t-T El (i) = As1nωc t −As1aω
If the phase of the signal El (tl in the case of a(t-'r) (4) is a mark, then (B) is determined to be a space,
(0 and 0 cannot be distinguished, and this case is similar to the case of the FSX signal.

ここで、本発明の減算処理における、信号のサンプリン
グ方法について説明する。本発明においては、受信信号
を記憶しておき、時刻tの受信信号と、交流波の一周期
前の時刻t−T受信信号を対応させ、減算処理を行う必
要がある。
Here, a signal sampling method in the subtraction process of the present invention will be explained. In the present invention, it is necessary to store the received signal, make the received signal at time t correspond to the received signal at time t-T, which is one cycle before the alternating current wave, and perform subtraction processing.

ここで問題となるのが、交流波の周期Tが一定でないこ
とである。一般に電力を供給する交流波の周期は、発生
源が定周期数電源でない場合。
The problem here is that the period T of the AC wave is not constant. In general, the period of the AC wave that supplies power is when the source is not a constant frequency power supply.

数%の変動を見込まねばならない。したがって。A fluctuation of several percent must be expected. therefore.

本発明において、交流波の周期Tを定数として記憶し、
連続的に、時刻tと時刻t−Tの受信信号を減算処理し
た場合、時刻t−Tの受信信号が1時刻tの一周期前の
受信信号とのずれを生じ、高調波雑音の除去が正確にで
きなくなることがある。
In the present invention, the period T of the alternating current wave is stored as a constant,
If the received signals at time t and time t-T are continuously subtracted, the received signal at time t-T will deviate from the received signal one period before time t, and harmonic noise will not be removed. It may not be possible to do it accurately.

本発明は、以上の点を考慮し、受信信号のサンプリング
タイミングを次のように定めている。
In consideration of the above points, the present invention defines the sampling timing of the received signal as follows.

受信信号を、一定の周期τ、でサンプリングするとした
とき、第3図に示した通り、交流波の定位相(第3図で
は、交流波が負から正に極性をかえるゼロク四ス点の場
合を示した)ごとに、サンプリングを新たに開始する。
When the received signal is sampled at a constant period τ, as shown in Figure 3, the alternating current wave has a constant phase (in Figure 3, the alternating current wave changes polarity from negative to positive at the zero point). ), sampling is started anew.

すなわち、第3図(b)のD点、B点で、−周期ごとに
サンプリングを開始し、時刻tであり、B点からサンプ
リング周期τ8のn倍離れた点であるA点でサンプリン
グされた受信信号は、D点からサンプリンク周期τ、の
几倍離れた0点でサンプリングされた受信信号と対応さ
せられて、減算処理がなされる。このようにサンプリン
グタイミングを定めることにより、交流波の周期Tが変
動しても、交流波の一周期前の受信信号との対応がかな
りの程度正確に行われ、減算処理によって。
That is, sampling is started every - period at points D and B in Fig. 3(b), and sampling is performed at point A, which is time t and is n times the sampling period τ8 from point B. The received signal is made to correspond to a received signal sampled at a point 0, which is a multiple of the sampling link period τ, from point D, and a subtraction process is performed. By determining the sampling timing in this way, even if the period T of the AC wave changes, correspondence with the received signal one period before the AC wave can be made with a considerable degree of accuracy, and by the subtraction process.

高調波雑音の効果的な除去が可能となる。Effective removal of harmonic noise becomes possible.

第4図に示したのは、本発明を実施する高調波雑音除去
回路の一例のブロック図である。入力端子1から入力し
た受信信号は、サンプリング値をディジタル値に変換す
る際の分解能および復調時の信頼性の向上のため設けら
れた低次の簡便なフィルタ2を経て交流波および高い周
波数のランダム雑音が除かれ、サンプリング回路3へ入
力する。受信信号は、交流波位相検出回路4にも入力し
、ここであらかじめ決められた、交流波の定位相が検出
されると、その情報がサンプリングパルス発生回路5に
送られ、該情報が送られるごとに新たにサンプリングが
開始される。サンプリングパルス発生回路5から出力さ
れたサンプリングパルスは、サンプリング回路3と記憶
回路6に入力しており、サンプリング回路3では、サン
プリングパルスニ基づいてサンプリングが行われ、その
結果が記憶回路6と演算判別回路7に入力する。記憶回
路6はこの入力を記憶し、入力してくるサンプリングパ
ルスに基づいて、交流波の一周期分前のサンプリング結
果を演算判別回路7に出力する。
FIG. 4 is a block diagram of an example of a harmonic noise removal circuit implementing the present invention. The received signal input from the input terminal 1 is converted into an alternating current wave and a high frequency random signal through a simple low-order filter 2 provided to improve resolution when converting sampling values into digital values and reliability during demodulation. Noise is removed and the signal is input to the sampling circuit 3. The received signal is also input to the AC wave phase detection circuit 4, and when a predetermined constant phase of the AC wave is detected here, the information is sent to the sampling pulse generation circuit 5, where the information is sent. A new sampling starts each time. The sampling pulse outputted from the sampling pulse generation circuit 5 is input to the sampling circuit 3 and the memory circuit 6. In the sampling circuit 3, sampling is performed based on the sampling pulse 2, and the result is used for the memory circuit 6 and calculation discrimination. Input to circuit 7. The memory circuit 6 stores this input, and outputs the sampling result of one cycle of the AC wave before to the calculation/determination circuit 7 based on the input sampling pulse.

演算判別回路7は、サンプリング回路3からの入力信号
から、記憶回路6からの入力信号な減算し、その符号を
判別して出力端子8に出力する。
The arithmetic determination circuit 7 subtracts the input signal from the storage circuit 6 from the input signal from the sampling circuit 3, determines the sign thereof, and outputs it to the output terminal 8.

なお、本発明の方法は、信号として電圧、電流いずれを
用いる場合でも適用することができる。
Note that the method of the present invention can be applied regardless of whether voltage or current is used as the signal.

(発明の効果) 以上説明したように、本発明によれば、交流波が印加さ
れる電力線路を信号伝送路とし、交流波に重畳されて送
信されてくる信号を受信するに際して、受信信号から、
前記交流波の一周期分前の受信信号を減算するようにし
、以て、雑音となる交流波の高調波が基本波と同期して
いることを利用して、高調波のみを除去するようにした
から、データ伝送速度を制限するフィルタを通さずに済
み、高速度のデータ伝送を可能にすることができる。
(Effects of the Invention) As explained above, according to the present invention, a power line to which an alternating current wave is applied is used as a signal transmission path, and when receiving a signal transmitted superimposed on an alternating current wave, it is possible to ,
The received signal of one cycle of the alternating current wave is subtracted, and by taking advantage of the fact that the harmonics of the alternating current wave, which become noise, are synchronized with the fundamental wave, only the harmonics are removed. Therefore, there is no need to pass through a filter that limits data transmission speed, and high-speed data transmission can be achieved.

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

第1図は本発明によるFSK信号の高調波雑音除去方法
を説明する図、第2図は交流波と高調波雑音との関係を
示す波形図、第3図は本発明におけるサンプリングタイ
ミングの一例を示す図、第4図は本発明を実施する高調
波雑音除去回路の一例を示すブロック図である。 1・・・入力端子、3・・・サンプリング回路、6・・
・記憶回路、7・・・演算判別回路、8・・・出力端子
、τ、・・・サンプリング周期。
Fig. 1 is a diagram explaining the method for removing harmonic noise from an FSK signal according to the present invention, Fig. 2 is a waveform diagram showing the relationship between AC waves and harmonic noise, and Fig. 3 is an example of the sampling timing in the present invention. FIG. 4 is a block diagram showing an example of a harmonic noise removal circuit implementing the present invention. 1...Input terminal, 3...Sampling circuit, 6...
- Memory circuit, 7... Calculation discrimination circuit, 8... Output terminal, τ,... Sampling period.

Claims (1)

【特許請求の範囲】[Claims] 1、交流波が印加される電力線路を信号伝送路とし、交
流波に重畳されて送信されてくる信号を受信するに際し
て、受信信号から、前記交流波の一周期分前の受信信号
を減算するようにした高調波雑音除去方法。
1. A power line to which an alternating current wave is applied is used as a signal transmission path, and when receiving a signal superimposed on an alternating current wave and transmitted, the received signal of one cycle of the alternating current wave is subtracted from the received signal. This is a harmonic noise removal method.
JP15874484A 1984-07-31 1984-07-31 KOCHOHAZATSUON JOKYOHOHO Expired - Lifetime JPH0234531B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP15874484A JPH0234531B2 (en) 1984-07-31 1984-07-31 KOCHOHAZATSUON JOKYOHOHO

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP15874484A JPH0234531B2 (en) 1984-07-31 1984-07-31 KOCHOHAZATSUON JOKYOHOHO

Publications (2)

Publication Number Publication Date
JPS6139634A true JPS6139634A (en) 1986-02-25
JPH0234531B2 JPH0234531B2 (en) 1990-08-03

Family

ID=15678385

Family Applications (1)

Application Number Title Priority Date Filing Date
JP15874484A Expired - Lifetime JPH0234531B2 (en) 1984-07-31 1984-07-31 KOCHOHAZATSUON JOKYOHOHO

Country Status (1)

Country Link
JP (1) JPH0234531B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002347463A (en) * 2001-05-24 2002-12-04 Yanmar Agricult Equip Co Ltd Structure of main shift lever

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002347463A (en) * 2001-05-24 2002-12-04 Yanmar Agricult Equip Co Ltd Structure of main shift lever

Also Published As

Publication number Publication date
JPH0234531B2 (en) 1990-08-03

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