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JPH0237735B2 - SHINGODENSOHOHOOYOBISOCHI - Google Patents
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JPH0237735B2 - SHINGODENSOHOHOOYOBISOCHI - Google Patents

SHINGODENSOHOHOOYOBISOCHI

Info

Publication number
JPH0237735B2
JPH0237735B2 JP10249780A JP10249780A JPH0237735B2 JP H0237735 B2 JPH0237735 B2 JP H0237735B2 JP 10249780 A JP10249780 A JP 10249780A JP 10249780 A JP10249780 A JP 10249780A JP H0237735 B2 JPH0237735 B2 JP H0237735B2
Authority
JP
Japan
Prior art keywords
signal
phase
zero
output
distribution line
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 - Lifetime
Application number
JP10249780A
Other languages
Japanese (ja)
Other versions
JPS5728435A (en
Inventor
Atsuhiro Yoshizaki
Eizaburo Sakawa
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.)
Hitachi Ltd
Original Assignee
Hitachi 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 Hitachi Ltd filed Critical Hitachi Ltd
Priority to JP10249780A priority Critical patent/JPH0237735B2/en
Publication of JPS5728435A publication Critical patent/JPS5728435A/en
Publication of JPH0237735B2 publication Critical patent/JPH0237735B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

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
    • H04B2203/5416Methods of transmitting or receiving signals via power distribution lines by adding signals to the wave form of the power source

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)

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は配電線を伝送路として使用する信号伝
送方法及び装置に関わり、特に非接地系配電線に
て対地帰路伝送を行なうに好適な信号伝送方法及
び装置に関する。
[Detailed Description of the Invention] [Industrial Application Field] The present invention relates to a signal transmission method and device that use power distribution lines as transmission lines, and in particular, to a signal transmission method and device that uses power distribution lines as transmission lines, and in particular, a signal transmission method and device that is suitable for return-to-ground transmission through ungrounded power distribution lines. The present invention relates to a transmission method and device.

〔従来の技術〕[Conventional technology]

一般に配電線系統の多くは非接地系であり、第
1図に示す如く変圧器1によつて変圧された電圧
が母線2を介してフイーダ3,4,5にそれぞれ
送られるように構成されている。このような非接
地系の配電線系統において、いわゆる零相回路の
電流、電圧を信号として利用する信号伝送装置が
特公昭49−38495号等で知られている。この公知
例ではフイーダ5に零相電流検出器を設け、この
零相電流検出器から検出される零相電流12を伝
送信号として用いる親局6が設けられている。ま
た、親局6の近くのフイーダ5の一線にはインピ
ーダンス7を介してスイツチ8が接続されてお
り、親局6からの信号によつてこのスイツチ8が
閉じられるとスイツチ8の他端が接地される。一
方、この親局6に対して適当な距離離れた位置
に、フイーダ上の零相電流を検出して親局6から
の伝送信号をキヤツチする子局9が設けられてい
る。この子局9も親局6と同様にフイーダ5の1
線をインピーダンス10を介してスイツチ11に
よつて1線地絡をおこさせるように構成されてい
る。このように構成されているから、いま、親局
6にてフイーダ5の1線をインピーダンス7を通
しスイツチ8によつて「1、0」の伝送コード信
号によつて間閉し、インピーダンス7による1線
地絡をおこして微小な零相電圧に変換し信号伝送
することができる。この親局6からの伝送に対し
て、子局9はこれを受信し、必要に応じてインピ
ーダンス10とスイツチ11により前記と同様な
方法によつて親局6に対しアンサー出力を伝送す
る。親局6は子局9からの信号を零相電流12に
より受信する。
Generally, most distribution line systems are ungrounded, and are configured so that the voltage transformed by a transformer 1 is sent to feeders 3, 4, and 5 via a bus 2, as shown in FIG. There is. In such an ungrounded power distribution line system, a signal transmission device that uses current and voltage of a so-called zero-phase circuit as a signal is known from Japanese Patent Publication No. 49-38495. In this known example, a feeder 5 is provided with a zero-sequence current detector, and a master station 6 is provided that uses the zero-sequence current 12 detected from the zero-sequence current detector as a transmission signal. Further, a switch 8 is connected to one line of the feeder 5 near the master station 6 via an impedance 7, and when this switch 8 is closed by a signal from the master station 6, the other end of the switch 8 is grounded. be done. On the other hand, a slave station 9 is provided at an appropriate distance away from the master station 6 to detect the zero-sequence current on the feeder and catch the transmission signal from the master station 6. Similarly to the master station 6, this slave station 9 also has 1 of the feeder 5.
It is configured such that a one-wire ground fault is caused by a switch 11 via an impedance 10 in the wire. Since it is configured in this way, one line of the feeder 5 is now passed through the impedance 7 at the master station 6 and closed by the transmission code signal of "1, 0" by the switch 8. It is possible to cause a one-line ground fault and convert it into a minute zero-sequence voltage for signal transmission. The slave station 9 receives this transmission from the master station 6, and transmits an answer output to the master station 6 using the impedance 10 and switch 11 as necessary in the same manner as described above. The master station 6 receives a signal from the slave station 9 using a zero-phase current 12.

この特公昭49−38495号のシステムにおいては、
伝送信号用の電源として低周波電源を準備し、受
信側では低周波信号のみを弁別して受信信号とし
ている。
In this system of Special Publication No. 49-38495,
A low frequency power source is prepared as a power source for the transmission signal, and on the receiving side, only the low frequency signal is discriminated and used as a received signal.

〔発明が解決しようとする問題点〕[Problem that the invention seeks to solve]

この公知のシステムでは、特に子局装置の大形
化が問題となり、電信柱の上あるいは各家庭に実
装するには適当でない。
This known system is particularly problematic in that it increases the size of the slave station, and is not suitable for installation on telephone poles or in individual homes.

つまり、低周波電源を得るためには、配電線の
電圧を変圧器にて絶縁しながら降圧し、変換器に
て直流に変換し再度低周波電圧を作り出すことが
不可欠であり、変圧器、変換器、整流用コンデン
サ、増巾器等を必要とすることから装置の大形化
をまぬがれることができない。
In other words, in order to obtain a low-frequency power source, it is essential to step down the voltage on the distribution line while insulating it with a transformer, convert it to DC with a converter, and then create the low-frequency voltage again. Since this method requires a rectifying capacitor, a rectifying capacitor, an amplifier, etc., it is impossible to avoid increasing the size of the device.

また、信号伝送に利用する配電線の零相回路に
は、変圧器1の負荷側の配電系統の構成によつて
固定的に定まる零相電圧や零相電流(以下これら
を残留零相成分という)が発生しており、配電線
の保護継電器は残留零相成分の変化を検出して配
電線の事故検出をしている。このため、零相回路
に伝送信号を注入するにしても、保護継電器を不
要動作させるものであつてはいけないし、かとい
つてS/N比を向上させるには注入信号を大きく
することが不可欠となる。
In addition, the zero-sequence circuit of the distribution line used for signal transmission contains zero-sequence voltage and zero-sequence current (hereinafter referred to as residual zero-sequence components) that are fixedly determined depending on the configuration of the distribution system on the load side of the transformer 1. ) has occurred, and the distribution line's protective relay detects a change in the residual zero-sequence component to detect an accident on the distribution line. Therefore, even if a transmission signal is injected into the zero-phase circuit, it must not cause unnecessary operation of the protective relay, and it is essential to increase the injection signal to improve the S/N ratio. becomes.

以上のことから本発明の目的とするところは、
小型の装置でかつ高精度に信号伝送することので
きる信号伝送方法及び装置を提供することを目的
とする。
From the above, the purpose of the present invention is to
It is an object of the present invention to provide a signal transmission method and device that can transmit signals with high accuracy using a small device.

〔問題点を解決するための手段〕[Means for solving problems]

本発明においては、送信側では配電線の一線と
大地間にインピーダンスとスイツチを直列に設け
伝送する信号に応じて適宜スイツチを開閉する。
また受信側では零相電流または零相電圧(以下零
相信号という)と相電圧または線間電圧(以下基
準信号という)とを検出しこの2つの成分の積演
算によつて求めた信号成分から第2高調波成分を
除去し、残余の信号成分の変化分を情報信号とし
て得ることにより良好なS/N比を得たものであ
る。
In the present invention, on the transmitting side, an impedance and a switch are connected in series between one line of the power distribution line and the ground, and the switch is opened and closed as appropriate in accordance with the transmitted signal.
Also, on the receiving side, the zero-sequence current or zero-sequence voltage (hereinafter referred to as zero-sequence signal) and the phase voltage or line voltage (hereinafter referred to as reference signal) are detected, and from the signal component obtained by multiplying these two components. A good S/N ratio is obtained by removing the second harmonic component and obtaining a change in the remaining signal component as an information signal.

〔作用〕[Effect]

受信端における受信信号である零相信号零相電
圧または零相電流の受信波形は、第2図に示す如
く送信端でのスイツチ開閉によつて発生した零相
の信号成分である信号ベクトル14と配電線に定
常的に発生している残留零相成分である定常誤差
ベクトル13とのベクトル和15となつている。
従つて、定常誤差ベクトル13の波形を交流的に
記憶し、ベクトル和15からアナログ的に引き算
すると信号ベクトル14のみを情報信号として検
出することができる。しかし、波形の交流的記憶
は回路的に複雑であるため、本発明では信号ベク
トル14と一定の位相関係の基準ベクトル16を
導入し、基準ベクトル16と受信波形のベクトル
15の積演算をし、その出力に含まれる第2高調
波成分を除去し、残余の信号成分の変化分を信号
ベクトル14の成分として分離することにより簡
単に高いS/N比を確保できるようにしたもので
ある。
The received waveform of a zero-phase signal, zero-phase voltage, or zero-phase current, which is a received signal at the receiving end, is a signal vector 14, which is a zero-phase signal component, generated by the opening and closing of a switch at the transmitting end, as shown in FIG. The vector sum is 15 with a steady error vector 13 which is a residual zero-sequence component constantly occurring in the distribution line.
Therefore, by storing the waveform of the steady error vector 13 in an alternating current manner and subtracting it from the vector sum 15 in an analog manner, only the signal vector 14 can be detected as an information signal. However, since alternating current storage of waveforms is complicated in terms of circuitry, the present invention introduces a reference vector 16 having a constant phase relationship with the signal vector 14, and calculates the product of the reference vector 16 and the received waveform vector 15. By removing the second harmonic component included in the output and separating the variation in the remaining signal component as a component of the signal vector 14, a high S/N ratio can be easily ensured.

〔実施例〕〔Example〕

以下本発明の一実施例について説明する。 An embodiment of the present invention will be described below.

一般に子局9側にてスイツチ11を開閉した時
の状態を対称座標法の零相回路で示すと、第3図
Aのようになる。すなわち、子局9の接地点でイ
ンピーダンス10を通し3相配電線の1線(例え
ばa相)をスイツチ11で接地すると、a相の相
電圧Vaと零相インピーダンス10,17で定ま
る零相電流を流すことのできる零相回路をa相と
大地間に構成する。この零相回路の零相インピー
ダンス17は、当該子局9接地のフイーダ18以
外の全フイーダの零相インピーダンスを代表して
示している。非接地の配電線系統では零相インピ
ーダンス17は、全フイーダの対地容量できまる
容量性インピーダンスである。今、インピーダン
ス10を零相インピーダンス17の容量に比べ充
分小さいコンデンサとすると、フイーダ18を流
れる零相電流は零相電源16に対し第3図Bに示
す如く進み90゜の電流として、零相CT19の2次
側に検出される。
In general, when the switch 11 is opened and closed on the slave station 9 side, the state shown in FIG. 3A is shown in a zero-phase circuit using symmetrical coordinates. In other words, when one wire of the three-phase distribution line (for example, the a phase) is grounded by the switch 11 through the impedance 10 at the grounding point of the slave station 9, the zero-sequence current determined by the phase voltage V a of the a-phase and the zero-sequence impedances 10 and 17 A zero-phase circuit that can flow is constructed between the a-phase and the ground. The zero-phase impedance 17 of this zero-phase circuit is shown as a representative of the zero-phase impedance of all feeders other than the feeder 18 connected to the slave station 9. In an ungrounded distribution line system, the zero-sequence impedance 17 is a capacitive impedance determined by the ground capacity of all feeders. Now, if the impedance 10 is a capacitor that is sufficiently smaller than the capacitance of the zero-sequence impedance 17, the zero-sequence current flowing through the feeder 18 advances with respect to the zero-sequence power supply 16 as shown in FIG. is detected on the secondary side of

この零相CT19から検出した零相信号に基づ
く信号復調装置の一実施例が第4図に示されてい
る。本実施例では一例として相電圧Vaを基準信
号として使用している。今、子局9のスイツチ1
1が閉の時流れる零相電流をI0として、零相CT
19より出力されるものとする。但し、ここでは
説明の都合上、まず零相電流I0には常時の残留誤
差分を含まない理想状態を考える。前述の如く相
電圧Vaに対し零相電流I0は90゜進みとなつている。
すなわち、相電圧ベクトルV〓aおよび零相電圧ベ
クトルI〓0は、それぞれ V〓a=Vasin(ωt) ……(1) I〓0=I0sin(ωt+90゜) ……(2) という関係にある。
An embodiment of a signal demodulation device based on the zero-phase signal detected from this zero-phase CT 19 is shown in FIG. In this embodiment, as an example, the phase voltage V a is used as the reference signal. Now switch 1 of slave station 9
The zero-sequence current that flows when 1 is closed is I 0 , and the zero-sequence CT
19. However, for convenience of explanation, first consider an ideal state in which the zero-sequence current I 0 does not include any residual error at any time. As mentioned above, the zero-sequence current I 0 leads the phase voltage V a by 90°.
In other words, the phase voltage vector V〓 a and the zero-phase voltage vector I〓 0 are respectively V〓 a =V a sin(ωt) ……(1) I〓 0 =I 0 sin(ωt+90゜) ……(2) This is the relationship.

ここで、Va、I0は夫々の最大値であり、ωは角
速度である。そして、Vaは既に知られた一定値
である。
Here, V a and I 0 are their respective maximum values, and ω is the angular velocity. And V a is a known constant value.

図において、V〓aを90゜進み移相回路20を通し
I〓0との乗算回路22に与え、I〓0を90゜遅れ移相回路
21を通しV〓aとの乗算回路23に入力する。こ
の乗算回路22と乗算回路23の両出力を加算回
路24によつて加算する。すなわち加算回路24
の出力は前記(1)、(2)式より、 Vasin(ωt+90゜)×I0sin(ωt+90゜)+Vasi
n(ωt)×I0sin(ωt) VaI0(cos2ωt+sin2ωt)=VaI0 ……(3) となる。すなわち、このことは加算回路24の出
力が基準信号の大きさVaと零相電流の大きさI0
積として定まる信号成分として復調できることを
示している。ここで、基準信号Vaは既知の値で
あり、VaI0は、I0つまり送信端のスイツチの開閉
信号で定まる。
In the figure, V = a is advanced by 90° and passed through the phase shift circuit 20.
I〓 0 is applied to a multiplier circuit 22 with I〓 0, and I〓 0 is inputted to a multiplier circuit 23 with V〓 a through a 90° delay phase shift circuit 21 . The outputs of the multiplier circuit 22 and the multiplier circuit 23 are added together by an adder circuit 24. That is, the addition circuit 24
From equations (1) and (2) above, the output of is V a sin (ωt + 90°) × I 0 sin (ωt + 90°) + V a si
n (ωt) × I 0 sin (ωt) V a I 0 (cos 2 ωt + sin 2 ωt) = V a I 0 ...(3). That is, this shows that the output of the adder circuit 24 can be demodulated as a signal component determined as the product of the magnitude of the reference signal V a and the magnitude of the zero-sequence current I 0 . Here, the reference signal V a is a known value, and V a I 0 is determined by I 0 , that is, the open/close signal of the switch at the transmitting end.

一方、零相CT19の出力には実際には零相の
定常残留誤差分として第2図の13で示したI〓εが
ある。従つて、 I〓e=Ie sin(ωt+) ……(4) 但し:V〓aとI〓eの位相差 とすると、零相CT19の出力は(2)式と(4)式の和
で考える必要がある。この時、加算回路24から
の出力は Vasin(ωt+90゜)×{I0sin((ωt+90゜)+Ie sin
(ωt+)}+Vasinωt ×{I0sin(ωt)+Ie sin(ωt+−90゜)}=Va
×I0{cos2ωt+sin2ωt} +Va×Ie{cosωt sin(ωt+)−sinωt cos(ωt
+)}=Va×I0+Va×Ie sin……(5) となる。
On the other hand, the output of the zero-phase CT 19 actually contains I〓ε shown by 13 in FIG. 2 as a zero-phase steady-state residual error. Therefore, I〓e=Ie sin(ωt+)...(4) However: If the phase difference between V〓a and I〓e, the output of zero-phase CT19 is the sum of equations (2) and (4). I need to think about it. At this time, the output from the adder circuit 24 is V a sin (ωt + 90°) × {I 0 sin ((ωt + 90°) + Ie sin
(ωt+)}+V a sinωt × {I 0 sin(ωt)+Ie sin(ωt+−90°)}=V a
×I 0 {cos 2 ωt+sin 2 ωt} +V a ×Ie {cosωt sin(ωt+)−sinωt cos(ωt
+)}=V a ×I 0 +V a ×Ie sin……(5).

この(5)式の第1項Va×I0は信号成分(3)式そのも
ので、信号送信中可変となる値であるに対し、第
2項Va×Ie sinは残留零相成分に相当し配電系
統の構成により定まる一定の直流成分である。こ
のことから、受信タイミングとなる直前に加算回
路24の出力(Va×Ie sin)の直流値をアナロ
グ的なホールド回路25でホールドし、受信期間
中加算回路24の出力とホールド回路25の出力
を減算回路26に印加すると、(4)式の誤差分が定
常的に発生していても減算回路26の出力として
は受信信号成分の内のVa×I0のみを復調出力とし
て抽出することができる。
The first term V a ×I 0 in equation (5) is the signal component in equation (3) itself, and is a value that changes during signal transmission, whereas the second term V a ×Ie sin is the residual zero-phase component. It is a constant DC component determined by the configuration of the power distribution system. From this, the DC value of the output (V a ×Ie sin) of the adder circuit 24 is held in the analog hold circuit 25 immediately before the reception timing, and the output of the adder circuit 24 and the output of the hold circuit 25 during the reception period. is applied to the subtraction circuit 26, even if the error in equation (4) occurs constantly, the subtraction circuit 26 extracts only V a ×I 0 of the received signal components as the demodulated output. Can be done.

従つて本発明によれば、残留零相成分に無関係
に伝送信号のみを取り出すことのできる復調回路
を構成することができる。
Therefore, according to the present invention, it is possible to construct a demodulation circuit that can extract only the transmission signal regardless of the residual zero-phase component.

また、本実施例によれば交流信号が「1、0」
の直流信号変換は整流後の直流化回路のような時
定数回路を用いていないため瞬時に復調信号を得
ることができ高速化が計れる。さらに本実施例に
よれば、基準信号との位相差を判別する機能があ
るため、自フイーダ子局と他フイーダ子局の設置
信号電流の区別をすることができるため、一斉ポ
ーリングで同時に各フイーダの各子局が親局にア
ンサー出力を伝送することができる。
Further, according to this embodiment, the AC signal is "1, 0"
Since the DC signal conversion does not use a time constant circuit like the DC conversion circuit after rectification, the demodulated signal can be obtained instantaneously and the speed can be increased. Furthermore, according to this embodiment, since there is a function to determine the phase difference with the reference signal, it is possible to distinguish between the installation signal current of the own feeder slave station and that of other feeder slave stations. Each slave station can transmit an answer output to the master station.

以上第4図を参照し、設置インピーダンスをコ
ンデンサとし、a相接地時Vaを基準ベクトルと
する実施例について説明してきたがここで本発明
の基本思想について説明すると、本発明では2つ
の基本周波ベクトルの乗算を行うと直流分と第2
高調波分ができることを利用している。このこと
を第5図を参照して説明する。同図においてaは
配電線路の零相電流を表わしており、このうちIe
は残留誤差電流として常時流れている成分であり
配電系統が定まれば固定的に定まる。これに対
し、I0は本発明の配電線利用伝送により零相回路
に印加された信号としての零相成分である。従つ
て、信号伝送時にはIe+I0、そうでない時はIeな
る零相電流が流れる。なお、一般にはI0>Ieであ
り、S/N比の悪い信号伝送方式である点で、他
の信号伝送方式とは異なる。一方、零相信号と乗
算される基準信号(同図b)は配電系統のいずれ
の電流電圧を利用してもよく、図示の例ではVa
なる任意位相の信号としている。これらを乗算し
た信号は同図cのように、乗ずるいずれかの信号
が零レベルのとき零となり、乗ずる信号の極性が
不一致のとき負レベルとなり、極性が一致すると
き正レベルの信号となる。この積後の信号は図示
から明らかなように適宜のバスアス値を有し、積
前の信号に比し2倍の周波数の信号である。V〓a
とI〓eを夫々上記(1)(4)式で表わし、I〓0を次の(6)式

一般的に表わしたとき、積後の信号は(7)式で表わ
される。
With reference to FIG. 4, we have described an embodiment in which the installation impedance is a capacitor and the reference vector is V a when phase a is grounded.The basic idea of the present invention will now be explained. By multiplying the frequency vector, the DC component and the second
It takes advantage of the fact that harmonic components are generated. This will be explained with reference to FIG. In the figure, a represents the zero-sequence current of the distribution line, of which Ie
is a component that constantly flows as a residual error current, and is fixedly determined once the power distribution system is determined. On the other hand, I 0 is a zero-phase component as a signal applied to a zero-phase circuit by transmission using a power distribution line according to the present invention. Therefore, a zero-sequence current of Ie+I 0 flows during signal transmission, and Ie flows otherwise. Note that this signal transmission method is different from other signal transmission methods in that generally I 0 >Ie and the signal transmission method has a poor S/N ratio. On the other hand, the reference signal (b in the same figure) to be multiplied by the zero-phase signal may use any current or voltage in the power distribution system, and in the illustrated example, V a
The signal has an arbitrary phase. The signal obtained by multiplying these signals becomes zero when either signal to be multiplied is zero level, becomes a negative level when the polarities of the multiplied signals do not match, and becomes a positive level signal when the polarities match, as shown in FIG. As is clear from the figure, the signal after the product has an appropriate bass value and has twice the frequency of the signal before the product. V〓 a
and I〓e are respectively expressed by the above equations (1) and (4), and I〓 0 is generally expressed by the following equation (6), then the signal after the product is expressed by the equation (7).

I〓0=I0sin(ωt+θ) ……(6) θ:V〓aとの間の位相差 (I〓0+I〓e)・V〓a={I0sin(ωt+θ)+Ie sin(
ωt+)}・Vasinωt =I0・Vasin(ωt+θ)・sinωt+Ie・Vasin(ωt+
)・sinωt =I0・Va/2{−cos(2ωt+θ)+cosθ}+Ie・Va
/2{−cos(2ωt+)+cos}……(7) この(7)式は、配電線を利用した信号伝送中に受
信される信号を表わし、信号を送つていないとき
は第2項の成分のみ受信される。そして、当式中
cos(2ωt+θ)、cos(2ωt+)が第5図cの第2
高調波成分、cosθ、cosがバイアスとしての値
である。この中で復調により取り出したい情報
は、I0・Va/2cosθである。このため、まず第2高 調波成分を除去する。前述の第4図の実施例で
は、このフイルタ作用を、回路22,20による
第1の乗算と回路21,23による第2の乗算を
行ない1つの乗算で生じた第2高調波成分が他の
もう1つの乗算で生じる第2高調波成分で打ち消
されるよう加算器24で加算することにより達成
したものである。従つて一般に周知の第2高調波
除去フイルタを用いてバイアス成分のみを抽出で
きることは言うまでもない。係るフイルタリング
後には(8)式の出力が得られる。
I〓 0 = I 0 sin (ωt + θ) ... (6) θ: V〓 Phase difference between a (I〓 0 + I〓e)・V〓 a = {I 0 sin (ωt + θ) + Ie sin (
ωt+)}・V a sinωt =I 0・V a sin(ωt+θ)・sinωt+Ie・V a sin(ωt+
)・sinωt =I 0・V a /2 {−cos(2ωt+θ)+cosθ}+Ie・V a
/2{−cos(2ωt+)+cos}……(7) This equation (7) represents the signal received during signal transmission using the distribution line, and when no signal is being sent, the second term is Only components are received. And during this ceremony
cos(2ωt+θ) and cos(2ωt+) are the second
The harmonic components, cosθ, and cos are values as bias. Among these, the information to be extracted by demodulation is I 0 ·V a /2cosθ. For this reason, first the second harmonic component is removed. In the embodiment shown in FIG. 4 described above, this filter action is performed by performing a first multiplication by circuits 22 and 20 and a second multiplication by circuits 21 and 23, and the second harmonic component generated by one multiplication is This is achieved by adding in the adder 24 so that it is canceled by the second harmonic component generated by another multiplication. Therefore, it goes without saying that only the bias component can be extracted using a generally known second harmonic removal filter. After such filtering, the output of equation (8) is obtained.

I0・Ia/2cosθ+Ie・Va/2cos ……(8) しかし、真の情報は第1項であり、第1項は第
2項に比し十分に小さいため、このままでは満足
な復調とならない。そこで本発明では(8)式の第2
項が一定であることに着目しその変化分を伝送信
号として取出すことにしたものである。
I 0・I a /2cosθ+Ie・V a /2cos ……(8) However, the true information is the first term, and the first term is sufficiently small compared to the second term, so the demodulation as it is is satisfactory. It won't happen. Therefore, in the present invention, the second
We focused on the fact that the term is constant, and decided to extract the change as a transmission signal.

以上説明したように本発明によれば良好なS/
N比を得ることができる。
As explained above, according to the present invention, good S/
The N ratio can be obtained.

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

第1図は非接地系の配電線系統を示す図、第2
図は信号受信時の受信信号のベクトル図、第3図
Aは子局側のスイツチ開閉時における対称座標方
の零相回路図、第3図Bは第3図A図示フイーダ
を流れる零相電流のベクトル図、第4図は本発明
に係る信号受信復調装置の実施例を示す回路図、
第5図は本発明の動作原理説明図である。 19……零相CT、20……90゜進み移相回路、
21……90゜遅れ移相回路、22,23……乗算
回路、24……加算回路、25……ホールド回
路、26……減算回路。
Figure 1 is a diagram showing an ungrounded distribution line system, Figure 2
The figure is a vector diagram of the received signal when the signal is received, Figure 3A is a zero-phase circuit diagram in symmetrical coordinates when the switch on the slave station side is opened and closed, and Figure 3B is the zero-phase current flowing through the feeder shown in Figure 3A. 4 is a circuit diagram showing an embodiment of the signal receiving and demodulating device according to the present invention,
FIG. 5 is an explanatory diagram of the operating principle of the present invention. 19...Zero phase CT, 20...90° advance phase shift circuit,
21...90° delay phase shift circuit, 22, 23...multiplication circuit, 24...addition circuit, 25...hold circuit, 26...subtraction circuit.

Claims (1)

【特許請求の範囲】 1 配電線の一線と大地間にインピーダンスとス
イツチとを直列接続しスイツチ開閉時の零相信号
を伝送信号として利用する配電線利用信号伝送方
式の信号伝送方法において、 前記配電線における零相信号とこの配電線から
得られる基準ベクトルの位相を90゜進ませた信号
とを積演算し、前記零相信号の位相を90゜遅らせ
た信号とこの配電線から得られた前記基準ベクト
ルとを積演算し、積演算して得た2つの信号を加
算して直流信号成分を得、所定時間記憶した直流
信号成分と現在時刻にえられた直流信号成分の差
を求めこれを情報信号とすることを特徴とする信
号伝送方法。 2 配電線の一線と大地間にインピーダンスとス
イツチとを直列接続しスイツチ開閉時の零相信号
を伝送信号として利用する配電線利用信号伝送方
式の信号伝送装置において、 前記配電線における人工的1線地絡時に発生す
る零相信号を検出する第1の手段、該第1の手段
の出力信号の位相を90゜遅らせる第2の手段、配
電線から得られる基準ベクトルの位相を90゜進ま
せる第3の手段、前記第1の手段の出力信号と前
記第3の手段の出力信号とを積演算する第4の手
段、前記第2の手段の出力信号と前記基準ベクト
ルとを積演算する第5の手段、前記第4の手段の
出力と前記第5の手段の出力とを加算して直流信
号成分を出力する第6の手段、伝送受信直前に第
6の手段から出力される値を記憶ホールドする第
7の手段、前記伝送受信中に第6の手段から出力
される信号から前記第7の手段によつてホールド
されている値を減算する第8の手段とから成るこ
とを特徴とする信号伝送装置。
[Scope of Claims] 1. A signal transmission method using a distribution line-based signal transmission system in which an impedance and a switch are connected in series between one line of a distribution line and the ground, and a zero-phase signal when the switch is opened/closed is used as a transmission signal, comprising: The zero-phase signal in the electric wire and the signal obtained by leading the phase of the reference vector obtained from this distribution line by 90 degrees are multiplied, and the signal obtained by delaying the phase of the zero-phase signal by 90 degrees and the signal obtained from this distribution line are calculated. Multiply the reference vector and add the two signals obtained by the product to obtain a DC signal component. Find the difference between the DC signal component stored for a predetermined time and the DC signal component obtained at the current time. A signal transmission method characterized in that the signal is an information signal. 2. In a signal transmission device using a distribution line signal transmission method, in which an impedance and a switch are connected in series between one line of a distribution line and the ground, and a zero-phase signal when the switch is opened/closed is used as a transmission signal, an artificial one wire on said distribution line A first means for detecting a zero-phase signal generated at the time of a ground fault, a second means for delaying the phase of the output signal of the first means by 90 degrees, and a second means for advancing the phase of the reference vector obtained from the distribution line by 90 degrees. a fourth means for multiplying the output signal of the first means and the output signal of the third means; a fifth means for multiplying the output signal of the second means and the reference vector; means, a sixth means for adding the output of the fourth means and the output of the fifth means to output a DC signal component, and storing and holding the value output from the sixth means immediately before transmission reception. and eighth means for subtracting the value held by the seventh means from the signal output from the sixth means during transmission and reception. Transmission device.
JP10249780A 1980-07-28 1980-07-28 SHINGODENSOHOHOOYOBISOCHI Expired - Lifetime JPH0237735B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP10249780A JPH0237735B2 (en) 1980-07-28 1980-07-28 SHINGODENSOHOHOOYOBISOCHI

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP10249780A JPH0237735B2 (en) 1980-07-28 1980-07-28 SHINGODENSOHOHOOYOBISOCHI

Publications (2)

Publication Number Publication Date
JPS5728435A JPS5728435A (en) 1982-02-16
JPH0237735B2 true JPH0237735B2 (en) 1990-08-27

Family

ID=14329042

Family Applications (1)

Application Number Title Priority Date Filing Date
JP10249780A Expired - Lifetime JPH0237735B2 (en) 1980-07-28 1980-07-28 SHINGODENSOHOHOOYOBISOCHI

Country Status (1)

Country Link
JP (1) JPH0237735B2 (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH061909B2 (en) * 1986-01-24 1994-01-05 株式会社日立製作所 Power line carrier signal transmission device
JPS62171236A (en) * 1986-01-24 1987-07-28 Hitachi Ltd Power line carrier transmission equipment

Also Published As

Publication number Publication date
JPS5728435A (en) 1982-02-16

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