JPS58209236A - Signal extracting system - Google Patents

Signal extracting system

Info

Publication number
JPS58209236A
JPS58209236A JP9229682A JP9229682A JPS58209236A JP S58209236 A JPS58209236 A JP S58209236A JP 9229682 A JP9229682 A JP 9229682A JP 9229682 A JP9229682 A JP 9229682A JP S58209236 A JPS58209236 A JP S58209236A
Authority
JP
Japan
Prior art keywords
coil
signal
distribution line
magnetic field
voltage
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
Application number
JP9229682A
Other languages
Japanese (ja)
Inventor
Kazuhiro Ohashi
一弘 大橋
Masao Tsukada
塚田 正男
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.)
Fuji Electric Co Ltd
Fuji Facom Corp
Original Assignee
Fuji Electric Co Ltd
Fuji Facom Corp
Fuji Electric Manufacturing 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 Fuji Electric Co Ltd, Fuji Facom Corp, Fuji Electric Manufacturing Co Ltd filed Critical Fuji Electric Co Ltd
Priority to JP9229682A priority Critical patent/JPS58209236A/en
Publication of JPS58209236A publication Critical patent/JPS58209236A/en
Pending legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H04ELECTRIC COMMUNICATION TECHNIQUE
    • H04BTRANSMISSION
    • H04B3/00Line transmission systems
    • H04B3/54Systems for transmission via power distribution lines
    • H04B3/56Circuits for coupling, blocking, or by-passing of signals
    • 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
    • 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
    • H04B2203/5483Systems for power line communications using coupling circuits
    • H04B2203/5487Systems for power line communications using coupling circuits cables

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

PURPOSE:To extract a signal superimposed on a distribution line or the like based on a voltage induced in a coil, by providing the coil contactlessly with a core wire of the distribution line or the like at a location subject to the effect of a magnetic ield produced around the distribution line. CONSTITUTION:The magnetic field H at a distance (r) to the coil 6 is expressed as H=I/2pir [AT/m]. The total magnetic flux phi is expressed as Equation 1, where B=muH [wb/m<2>] is magnetic flux density and (a) is radius of the coil 6 in [m]. Further, a voltage E induced in the coil 6 is expressed in Equation 2, where N is the number of windings of the coil 6. The induced voltage E is in- creased with the coil 6 wound on a ferromagnetic substance 7. Since the relation of E0/E=f0/f is established, where f[Hz] is commercial frequency, f0[Hz] is signal frequency, and E[V], E0[V] are output voltages at respective magnetic field, a signal superimosed is detected on the basis of the induced voltage of the coil 6.

Description

【発明の詳細な説明】 本発明は配電線に重畳された高周波信号を抽出するため
の信号抽出方式に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a signal extraction method for extracting high frequency signals superimposed on power distribution lines.

伝送路として配電線を利用し.この配電線に高周波信号
を重畳させて信号伝送を行なうことは良く知られている
。このような信号伝送方式において,配電線に重畳され
る高周波信号t−取シ出せ抽出方式としてはコンデンサ
を使用する方式が一般的である。すなわち、この方式に
は配電線の芯線に直接コンテンサを接続する方式と.配
電線の絶縁物を電極で覆い.芯線との間にコンデンサを
対地間に接続されたインピーダンスと直列に接続して信
号を佃出するいわゆる分圧方式がある。第1図はこのよ
うな従来の方式のうち、配電線の芯線に直接コンデンサ
を接続する方式を示している。
Power distribution lines are used as transmission lines. It is well known that signal transmission is performed by superimposing a high frequency signal on the power distribution line. In such a signal transmission method, a method using a capacitor is generally used as a method for extracting the high frequency signal superimposed on the power distribution line. In other words, this method involves connecting the capacitor directly to the core wire of the distribution line. Cover the insulation of the distribution line with electrodes. There is a so-called voltage division method in which a capacitor is connected in series with an impedance connected between the core wire and the ground to output a signal. Among these conventional methods, FIG. 1 shows a method in which a capacitor is directly connected to the core wire of a power distribution line.

図において1は配電線%2は結合コンデンサ、3は整合
変成器,4は受信装置を示している。結合コンデンサ2
は系統周波数の電流に対しては高いインピータンス金保
有するが重畳される高周波信号に対しては低いインピー
ダンスを保有するものが選択され、これにより高周波信
号成分が整合変成器3に供給されて受信装置4に入力さ
れる。
In the figure, 1 indicates a distribution line, 2 indicates a coupling capacitor, 3 indicates a matching transformer, and 4 indicates a receiving device. Coupling capacitor 2
is selected to have a high impedance to the current at the grid frequency, but a low impedance to the superimposed high frequency signal, so that the high frequency signal component is supplied to the matching transformer 3 and received. It is input into the device 4.

しかし、コンデンサを用いるいずれの方式も必ず接地を
とらねばならず、任意に抽出場所を変え、早急に処理す
ることが不可能であるという欠点を有している。また、
コンデンサを配電線の芯線に接続する方式では数が多く
なると対地充電々流が増加するため、変電所内に設置さ
れた保護リレーなどの誤動作の原因となっていた。
However, all methods using capacitors have the disadvantage that they must be grounded and that it is impossible to arbitrarily change the extraction location and process quickly. Also,
In the method of connecting capacitors to the core wires of power distribution lines, as the number of capacitors increases, the ground charging current increases, causing malfunctions of protective relays installed in substations.

本発明は上記に鑑み、作業性の同上、ならびに供給信頼
度の同上をはかることが可能な信号抽出方式を提供する
ことを目的とする。
In view of the above, an object of the present invention is to provide a signal extraction method that can improve workability and supply reliability.

この目的は本発明によれば配電線等の周囲に生ずる磁界
の影響を受ける位置に配電線等の芯線とは非接触にてコ
イルを設け、このコイルに誘起される電圧に基づいて前
記配電線等に重畳された信号を抽出することによシ達成
される。
According to the present invention, a coil is provided at a position affected by the magnetic field generated around the distribution line, etc., without contact with the core wire of the distribution line, etc., and the voltage induced in the coil is This is achieved by extracting the signal superimposed on the

以下、本発明を図に示す実施例に基づ4いて詳細に説明
する。
Hereinafter, the present invention will be explained in detail based on embodiments shown in the drawings.

第2図は配電線と本発明による信号抽出方式に用いられ
る磁気センサの相対位置関係を示している。図において
5は配電線、6はコイル、7は強磁性体である。第2図
において、紙の表から裏へ。
FIG. 2 shows the relative positional relationship between the power distribution line and the magnetic sensor used in the signal extraction method according to the present invention. In the figure, 5 is a power distribution line, 6 is a coil, and 7 is a ferromagnetic material. In Figure 2, from the front to the back of the paper.

周波数f [Hz :] 、 ’を流ICA)が流れて
いるものとすると、コイル6までの距離r(m〕に2け
る磁界Hはアンペア周回路の法則より。
Assuming that a current ICA) is flowing at a frequency f [Hz:], ', the magnetic field H at 2 at a distance r (m) to the coil 6 is from the ampere circuit law.

■ となる。したがって、磁束密度B=μHcwb/I′I
′1′〕よシ、コイル6の牛径arm〕とすれば、磁束
の総数Φは、 Φ=π・a!・B=π・a2@μH となる。そこでコイル6に誘起される電圧Eは、コイル
6の巻数をNとすると、 となる。コイル6が強磁性体7に巻かれている場合には
強磁性体7に磁束が吸い寄せられるような現象が生ずる
ので、空心コイルの場合に較べて(3)式の誘起電圧E
が大きくなる。したがって配電線5に重畳されている信
号を抽出する際に、商用周波数DHz〕、i号周波数f
。[Hz]とした場合に各々の磁界による出力電圧をE
〔V)、BO[V)とすると(3)式より、 の関係が本質的に成立するので、信号周波数f。の値を
適切な値に選択することによシコイル6の誘起電圧に基
づいて重畳されている信号を検出することができ、信号
抽出が可能となる。
■ It becomes. Therefore, magnetic flux density B=μHcwb/I′I
'1'], the diameter of the coil 6 is arm], then the total number of magnetic fluxes Φ is Φ=π・a!・B=π・a2@μH. Therefore, the voltage E induced in the coil 6 is as follows, where N is the number of turns of the coil 6. When the coil 6 is wound around the ferromagnetic material 7, a phenomenon in which magnetic flux is attracted to the ferromagnetic material 7 occurs, so that the induced voltage E in equation (3) is lower than in the case of an air-core coil.
becomes larger. Therefore, when extracting the signal superimposed on the distribution line 5, the commercial frequency DHZ], the i frequency f
. [Hz], the output voltage due to each magnetic field is E
[V) and BO[V], from equation (3), the relationship essentially holds true, so the signal frequency f. By selecting an appropriate value for , the superimposed signal can be detected based on the induced voltage of the coil 6, and signal extraction becomes possible.

また、第2図に示すようにコイル6に並列に並  4列
共振条件となるコンデンサ8を付加すれば、必要な信号
周波数の゛電圧のみを強調して取り出せることになる。
Furthermore, as shown in FIG. 2, if a capacitor 8 is added in parallel to the coil 6 to provide a four-row resonance condition, only the voltage at the required signal frequency can be extracted with emphasis.

この時の共振周波数fは次式で表わさせる。The resonance frequency f at this time is expressed by the following equation.

このように本発明によれば、配電線等の周囲に生ずる磁
界中にコイルを設置することによシ配電線の芯線に非接
触でかつ接地等を必要とせずに信号を抽出することがで
きる。第3図は配電線の周囲の磁界中にコイルを設置す
るための一実施例を示すものであ勺、配電線5に引っ掛
けられる部分を有する支持体9を絶縁物で構成し、この
支持体9の内部にコイル6と強磁性体7を埋設したもの
である。このような構成とすれば配電線の任意の箇所に
おいて支持体9を引っ掛けるだけで信号を抽出すること
ができるーなお1本発明は配電線に限らす、信号電流に
より線路の周囲に磁界が゛発生するような信号伝送に巾
広く応用が可能である。
As described above, according to the present invention, by installing the coil in the magnetic field generated around the distribution line, it is possible to extract the signal without contacting the core wire of the distribution line and without the need for grounding. . FIG. 3 shows an embodiment for installing a coil in a magnetic field around a power distribution line. A coil 6 and a ferromagnetic material 7 are embedded inside the coil 9. With such a configuration, a signal can be extracted by simply hooking the support 9 at any point on the power distribution line. However, the present invention is limited to power distribution lines, and the signal current creates a magnetic field around the line. It can be widely applied to signal transmissions such as those that occur.

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

第1Nは従来の信号抽出方式の実施例を示す構成図、第
2因は本発明による磁気センサと配電線の相対位置関係
を示す因、第3図は磁気七ンサ會配電線の周囲の磁界中
に設置させるための一実施例を示す図でおる。 1.5・・・配電線、2・・・結合コンデンサ、3・・
・結合装置、4・・・受信装置、6・・・コイル、7・
・・強磁性体、8・・・同調コンデンサ、9・・・支持
体。
1N is a configuration diagram showing an example of a conventional signal extraction method, the second factor is a factor showing the relative positional relationship between the magnetic sensor and the power distribution line according to the present invention, and FIG. 3 is a diagram showing the magnetic field around the power distribution line. This is a diagram showing an embodiment for installing the device inside the device. 1.5... Distribution line, 2... Coupling capacitor, 3...
・Coupling device, 4... Receiving device, 6... Coil, 7.
...Ferromagnetic material, 8...Tuning capacitor, 9...Support.

Claims (1)

【特許請求の範囲】 1)配電線等に重畳されている信号を抽出するためのも
のにおいて,配電線等の周囲に生ずる磁界の影響を受け
る位置K前記配電線等の芯線とは非接触にてコイルを設
け、前記磁界により前記コイルに誘起される電圧に基づ
いて前記信号を抽出することを特徴とする信号抽出方式
。 2)%許請求の範囲第1項に記載の信号抽出方式におい
て前記コイルは信号周波数に対して共振条件となる並列
接続コンデンサを有し,前記コイルに誘起される電圧よ
り前記信号成分のみを強調して抽出することを特徴とす
る信号抽出方式。 3)特許請求の範囲第1項または第2項に記載の信号抽
出方式において、前記コイルは配電線等に引っ掛けられ
る絶縁物からなる支持体に埋設されることを特徴とする
信号抽出方式。
[Scope of Claims] 1) In a device for extracting a signal superimposed on a distribution line, etc., a position K that is affected by a magnetic field generated around the distribution line, etc. is not in contact with the core wire of the distribution line, etc. A signal extraction method characterized in that a coil is provided in the coil, and the signal is extracted based on a voltage induced in the coil by the magnetic field. 2) % Allowance In the signal extraction method according to claim 1, the coil has a parallel-connected capacitor that provides a resonance condition with respect to the signal frequency, and only the signal component is emphasized by the voltage induced in the coil. A signal extraction method characterized by extracting signals by 3) The signal extraction method according to claim 1 or 2, wherein the coil is embedded in a support made of an insulator that is hooked onto a power distribution line or the like.
JP9229682A 1982-05-31 1982-05-31 Signal extracting system Pending JPS58209236A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP9229682A JPS58209236A (en) 1982-05-31 1982-05-31 Signal extracting system

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP9229682A JPS58209236A (en) 1982-05-31 1982-05-31 Signal extracting system

Publications (1)

Publication Number Publication Date
JPS58209236A true JPS58209236A (en) 1983-12-06

Family

ID=14050447

Family Applications (1)

Application Number Title Priority Date Filing Date
JP9229682A Pending JPS58209236A (en) 1982-05-31 1982-05-31 Signal extracting system

Country Status (1)

Country Link
JP (1) JPS58209236A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51147107A (en) * 1975-06-11 1976-12-17 Toyo Commun Equip Co Ltd Electromagnetic communication method using open magnetic coupler

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS51147107A (en) * 1975-06-11 1976-12-17 Toyo Commun Equip Co Ltd Electromagnetic communication method using open magnetic coupler

Similar Documents

Publication Publication Date Title
US3963975A (en) Electromagnetically shielded electrical power supply with reduced common mode electromagnetic interference output
US6563296B2 (en) Closely-coupled multiple-winding magnetic induction-type sensor
SE515388C2 (en) Device for sensing electrical discharges in a sample object
US4622535A (en) Receiving circuit for a data transmission system
JPS61245511A (en) Dc and ac current transformer
US5536978A (en) Net current control device
EP3709320A1 (en) Current transformer
US20070263335A1 (en) Single-phase filter for reducing harmonics
US2381097A (en) Magnetic pickup device
JPH10294589A (en) Device for improvement of quality of audio and/or video signal
EP0302746B1 (en) Apparatus for and method of discriminating signals
MY106734A (en) Generator for generating an electric voltage.
JPS58209236A (en) Signal extracting system
JPH09152462A (en) Partial discharge detection method for transformer
CN106653301B (en) Ring-shaped inductors and its manufacturing method
US5068636A (en) Current shunting
CN213275740U (en) Flexible current sensor with multiple characteristic quantity measurement
JPH03296313A (en) Single phase three wire blocking filter for power line carrier communication
JPS6238033A (en) Information transmission system
JPH062259Y2 (en) Noise shielding transformer
JP2021196259A (en) Current sensor
JP2001319815A (en) Signal input and output device
JPH0677065A (en) Differential transformer
JPH01221929A (en) Signal discrimination method
JPS61229312A (en) Air-core current transformer