JPH03274827A - Signal detector - Google Patents

Signal detector

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Publication number
JPH03274827A
JPH03274827A JP2075180A JP7518090A JPH03274827A JP H03274827 A JPH03274827 A JP H03274827A JP 2075180 A JP2075180 A JP 2075180A JP 7518090 A JP7518090 A JP 7518090A JP H03274827 A JPH03274827 A JP H03274827A
Authority
JP
Japan
Prior art keywords
compensation
electrostatic capacitance
electrode
capacitance
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.)
Granted
Application number
JP2075180A
Other languages
Japanese (ja)
Other versions
JPH0783299B2 (en
Inventor
Masao Fukuda
福田 昌夫
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.)
Anritsu Corp
Original Assignee
Anritsu Corp
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 Anritsu Corp filed Critical Anritsu Corp
Priority to JP7518090A priority Critical patent/JPH0783299B2/en
Publication of JPH03274827A publication Critical patent/JPH03274827A/en
Publication of JPH0783299B2 publication Critical patent/JPH0783299B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Tests Of Electronic Circuits (AREA)
  • Monitoring And Testing Of Transmission In General (AREA)

Abstract

PURPOSE:To detect the voltage waveform of a signal flowing on a communication line with fidelity by providing a means provided with a function to generate a capacitance value approximated to coupling electrostatic capacitance generated between an unbalanced type communication line that is a line targeted to be monitored and an electrode between the electrode and the ground, and attaching external electrostatic capacitance for compensation which performs band compensation. CONSTITUTION:A compensation conductor 2 is the one to supply the coupling electrostatic capacitance CC equivalent to the coupling electrostatic capacitance CC generated when the line 1 targeted to be monitored is sandwiched with the electrode 3 between the electrode 3 and the ground 6. The external electrostatic capacitance 4CE for compensation to be attached is electrostatic capacitance to be attached fixedly to further expand a low frequency band area. When the coupling electrostatic capacitance CC by the compensation conductor 2 is attached, flat loss is generated extending over a high frequency area, however, a flat part is extended in a low frequency area, which enables the making of the area into a wideband area. The increment of the loss in the flat part can be sufficiently amplified at a high input impedance differential amplifier, which remarkably increases the effect of compensation. When the external electrostatic capacitance 4CE for compensation is attached at the outside, the flat part in the low frequency area can be further expanded. A balanced type communication line can be set similarly as the line targeted to be monitored other than the unbalanced type communication line.

Description

【発明の詳細な説明】 〔産業上の利用分野〕 本発明は、監視対象線である通信線に直接に接続するこ
となく信号を検出する容量結合形の信号検出器に関する
ものである。
DETAILED DESCRIPTION OF THE INVENTION [Field of Industrial Application] The present invention relates to a capacitively coupled signal detector that detects a signal without being directly connected to a communication line that is a line to be monitored.

〔従来の技術〕[Conventional technology]

従来、監視対象線である通信線あるいは電力線に流れる
電圧、または電流波形を導体に接触せずに観測する場合
には、通信線等の観測対象となる線をトロイダルコイル
と電磁結合し電流波形を取出すか、または観測する線を
金属の電極で線の被覆上から挟み静電結合することによ
り電圧波形を取出す方法が採られる。特に、通信線を流
れる信号を観測する場合には伝送特性に影響を与えるこ
とが無いようにする必要があり、電磁結合でも静電結合
であっても可能な限り弱結合とし観測点に於ける信号の
損失、通信線上のインピーダンスの不均一が生じないよ
うに考慮しなければならない。
Conventionally, when observing the voltage or current waveform flowing in a communication line or power line, which is a line to be monitored, without touching the conductor, the line to be observed, such as a communication line, is electromagnetically coupled with a toroidal coil to measure the current waveform. A method is adopted in which the voltage waveform is extracted by capacitively coupling the wire to be extracted or observed between metal electrodes on the wire's coating. In particular, when observing signals flowing through a communication line, it is necessary to ensure that the transmission characteristics are not affected, so it is necessary to make the coupling as weak as possible, whether it is electromagnetic or electrostatic coupling, at the observation point. Consideration must be taken to prevent signal loss and impedance non-uniformity on the communication line.

従来、通信線に流れる信号を非接触で検出する場合、2
本で一対の通信線を1本ごとに心線の外液上から電極で
挟み静電結合で信号を取出し、これを高入力インピーダ
ンス差動増幅器で増幅し検出していた。第4図は静電結
合方式の概念図で、第5図は第4図の等価回路である。
Conventionally, when detecting signals flowing through communication lines without contact, 2
In this method, each pair of communication wires was sandwiched between electrodes above the external liquid of the core wire, and a signal was extracted through capacitive coupling, which was then amplified and detected using a high input impedance differential amplifier. FIG. 4 is a conceptual diagram of the electrostatic coupling method, and FIG. 5 is an equivalent circuit of FIG. 4.

第5図(a)は通信線と電極の結合静電容量を2Cとし
、高入力インピーダンス差動増幅器の入力インピーダン
スを含む対地負荷抵抗をR/2とした時の平衡形等価回
路である。第5図(b)は第5図(a)と全く等価な不
平衡等価回路である。従って、C,Rからなる検出系の
インピーダンスが通信線の特性インピーダンスρに比較
し極めて大きいため、ρは殆ど無視することができる。
FIG. 5(a) is a balanced equivalent circuit when the coupling capacitance between the communication line and the electrode is 2C, and the ground load resistance including the input impedance of the high input impedance differential amplifier is R/2. FIG. 5(b) is an unbalanced equivalent circuit completely equivalent to FIG. 5(a). Therefore, since the impedance of the detection system consisting of C and R is extremely large compared to the characteristic impedance ρ of the communication line, ρ can be almost ignored.

よって、信号源の電圧をE8、信号検出器の検出電圧を
vlとすると、電圧減衰量20Log (E s / 
V + )が下式で表されることは自明である。
Therefore, if the voltage of the signal source is E8 and the detection voltage of the signal detector is vl, the voltage attenuation amount is 20Log (E s /
It is obvious that V + ) is expressed by the following formula.

電圧減衰量= 20Log  (E s / V r 
)−10Log  ((1+ρ/R) +(1/ωCR) t) ’ilOLog  (1+ (1/ ωCR) ” )
・・・・・・(ρ(R) E、:信号源の電圧 Vl :信号検出器の検出電圧 ρ :通信線の特性インピーダンス R:検出系のインピーダンス C:通信線と電極の結合静電容量 ω :角周波数(2πf、f:周波数)〔発明が解決し
ようとする課題〕 即ち、第5図は機械的接触のため結合静電容量Cが不確
定な単純な高域通過フィルタであり、第6図に示すよう
に、伝達特性は低周波領域で大幅に変動する周波数特性
をもつ、この様な弱結合となる静電結合方式では結合静
電容量Cを大きくすることは物理的不可能で、低周波ま
で減衰特性が平坦な帯域を確保することは困難であった
。そのため、低周波酸分を含むディジタル信号などの広
帯域信号波形を非接触で忠実に検出し観測することが出
来なかった。
Voltage attenuation = 20Log (E s / V r
) −10Log ((1+ρ/R) + (1/ωCR) t) 'ilOLog (1+ (1/ωCR) ” )
......(ρ(R)) E,: Voltage of signal source Vl: Detection voltage of signal detector ρ: Characteristic impedance of communication line R: Impedance of detection system C: Coupling capacitance between communication line and electrode ω: angular frequency (2πf, f: frequency) [Problem to be solved by the invention] In other words, FIG. 5 shows a simple high-pass filter in which the coupling capacitance C is uncertain due to mechanical contact; As shown in Figure 6, it is physically impossible to increase the coupling capacitance C with such a weakly coupled capacitive coupling method, where the transfer characteristics have frequency characteristics that vary significantly in the low frequency region. , it was difficult to secure a band with flat attenuation characteristics down to low frequencies.As a result, it was not possible to faithfully detect and observe broadband signal waveforms such as digital signals containing low-frequency acid components without contact. .

本発明は、このよな事情に鑑みてなされたものであり、
弱結合により生しる問題点を解決し、通信線を流れる信
号の電圧波形を忠実に検出する信号検出器を提供するこ
とを課題とする。
The present invention has been made in view of these circumstances,
It is an object of the present invention to provide a signal detector that solves problems caused by weak coupling and faithfully detects the voltage waveform of a signal flowing through a communication line.

〔課題を解決するための手段〕[Means to solve the problem]

上記課題を解決するために本発明の信号検出器において
は、電極と対地間容量を積極的に利用することにより、
低周波領域を拡大し広帯域信号を忠実に検出する。すな
わち、 ■監視対象線である一対の平衡形通信線と電極間に生じ
る結合静電容量に近似した容量値を、二つの電極間に発
生する機能を持つ手段、具体的には電極に補償心線を挟
み込む。
In order to solve the above problems, in the signal detector of the present invention, by actively utilizing the capacitance between the electrode and the ground,
Expands the low frequency range and faithfully detects wideband signals. In other words, ■Means that have the function of generating a capacitance value that approximates the coupling capacitance that occurs between the pair of balanced communication lines that are the lines to be monitored and the electrodes, specifically, a compensation center in the electrodes. Insert the line.

■帯域補償を行う補償用外部静電容量を付加させた。■Added an external compensating capacitor to perform band compensation.

また、請求項(2)においては、 ■不衡形通信線の監視対象線と電極間に生じる結合静電
容量に近似した容量値を、電極と対地間に発生する機能
を持つ手段、具体的には電極に補償心線を挟み込む。
In addition, in claim (2), (1) a means having a function of generating a capacitance value close to the coupling capacitance generated between the electrode and the monitored line of the unbalanced communication line between the electrode and the ground; To do this, insert a compensating core wire between the electrodes.

■帯域補償を行う補償用外部静電容量を付加させた。■Added an external compensating capacitor to perform band compensation.

〔作用〕[Effect]

このように権威された信号検出器によれば、静電容量に
よる弱結合であっても100Hz程度の低周波数まで伝
達特性が平坦となる。
According to such an authoritative signal detector, the transfer characteristic is flat up to a low frequency of about 100 Hz even if there is weak coupling due to capacitance.

〔実施例〕〔Example〕

以下に、本発明の一実施例を図面を用いて説明する。第
1図は本発明の電極部分の接続を示したものであり、第
1図(a)は電極側面、第1図(b)は電極上面から見
た構成国、第2図は第1図の等価回路である。以下、第
1図の図面の引出し番号を()で示し対応を説明する。
An embodiment of the present invention will be described below with reference to the drawings. Figure 1 shows the connection of the electrode parts of the present invention; Figure 1 (a) is the side view of the electrode, Figure 1 (b) is the component country seen from the top of the electrode, and Figure 2 is the same view as Figure 1. This is the equivalent circuit of Hereinafter, the drawer numbers of the drawings in FIG. 1 will be indicated in parentheses and the correspondence will be explained.

補償心線(2)は、監視対象線(1)を電極(3)で挟
み込んだ時に生じる結合静電容量C8と等量の結合静電
容量CCを、電極(3)と対地(6)間に与えるための
ものである。追加する補償用外部静電容量(4)C,は
低周波帯域を更に広げるために固定的に付加する静電容
量である。
The compensating core wire (2) has a coupling capacitance CC between the electrode (3) and the ground (6) that is equivalent to the coupling capacitance C8 that occurs when the wire to be monitored (1) is sandwiched between the electrodes (3). It is intended to be given to The additional compensating external capacitance (4) C is a fixed capacitance added in order to further widen the low frequency band.

第1図の等価回路を第5図と同様に不平衡形で第2図に
示す。
The equivalent circuit of FIG. 1 is shown in FIG. 2 in an unbalanced form similar to FIG. 5.

第2図の電圧減衰量は下式で容易に表される。The voltage attenuation amount in FIG. 2 is easily expressed by the following formula.

電圧減衰量−20Log  (E s / V r )
=10Log  ([1+  (ρCs  + R(C
c 十C1))/RCsコ +[(ω”  Cs  (Cc + CE )ρR−1
)/Rωcs ]  ” ] ”;10Log  ([1+ (Cc +Ct ) /
 Cs ] ”+[1/Rωc、]  ”  ) (ρξO) :信号源の電圧 :信号検出器の検出電圧 :監視対象線の特性インピーダンス :検出系のインピーダンス :監視対象線との結合静電容量 :電極と補償心線による対地間結合静電容量 Cア:補償用外部静電容量 :角周波数(2zf、f :周波数) 3 ■ 算 ρ 8 Cc 第3図に電圧減衰量の周波数特性を示す、補償心線2に
よる結合静電容量Ccを付加すると、高周波領域にわた
り平坦な損失を生しるが平坦部分が低域に広がり広帯域
化が可能となる。平坦部分の損失の増加は高入力インピ
ーダンス差動増幅器(図示せず。)で十分増幅可能で補
償の効果は大である。外部に補償用外部静電容量(4)
Ctを追加すると更に低域の平坦部を拡大可能である。
Voltage attenuation - 20Log (Es/Vr)
=10Log ([1+ (ρCs + R(C
c 1 C1))/RCs + [(ω” Cs (Cc + CE) ρR-1
)/Rωcs] ” ] ”;10Log ([1+ (Cc +Ct) /
Cs ] ”+[1/Rωc,] ” ) (ρξO): Voltage of signal source: Detection voltage of signal detector: Characteristic impedance of monitored line: Impedance of detection system: Coupling capacitance with monitored line: Coupling capacitance between the electrode and the compensating wire to ground CA: External capacitance for compensation: Angular frequency (2zf, f: frequency) 3 ■ Calculation ρ 8 Cc Figure 3 shows the frequency characteristics of the voltage attenuation amount. Addition of the coupling capacitance Cc by the compensating core wire 2 causes a flat loss over the high frequency region, but the flat portion spreads to the low frequency range, making it possible to widen the band. The increase in loss in the flat portion can be sufficiently amplified by a high input impedance differential amplifier (not shown), and the compensation effect is large. External capacitance for compensation (4)
By adding Ct, it is possible to further expand the flat part of the low frequency range.

通常、監視対象線との結合静電容量C3は数pF以下、
監視対象線の特性インピーダンスρは数百Ω以下である
。CC+CEをC8の10倍にすると平坦部の損失は約
20dB増加するが、低域の周波数帯域は一桁広がり、
1QkHzから1kHzとなる。一方、高周波領域では
CC+CEを挿入したことにより、監視対象線の特性イ
ンピーダンスρが影響し損失が増加するが、C8の10
倍程度であれば100MHz程度まで平坦特性が得られ
問題ない、高入力インピーダンス差動増幅器の利得を4
0dBとすることは容易であり、Cc+C!はC8の1
00倍程度まで挿入でき、静電容量による弱結合であっ
ても100Hz程度の低周波数の信号まで平坦特性で検
出可能となる。
Usually, the coupling capacitance C3 with the line to be monitored is several pF or less,
The characteristic impedance ρ of the line to be monitored is several hundred ohms or less. If CC+CE is made 10 times that of C8, the loss in the flat part will increase by about 20 dB, but the low frequency band will expand by an order of magnitude.
It becomes 1kHz from 1QkHz. On the other hand, in the high frequency region, by inserting CC + CE, the characteristic impedance ρ of the monitored line is affected and the loss increases;
If the gain of a high input impedance differential amplifier is about 4, it can obtain flat characteristics up to about 100MHz without any problem.
It is easy to set it to 0 dB, and Cc+C! is C8 1
It can be inserted up to about 00 times, and even with weak coupling due to capacitance, signals with a low frequency of about 100 Hz can be detected with flat characteristics.

なお、本実施例では監視対象線として不平衡形通信線を
使用した例を説明したが、平衡形通信線についても同様
であることはいうまでもない。
In this embodiment, an example in which an unbalanced communication line is used as the line to be monitored has been described, but it goes without saying that the same applies to a balanced communication line.

〔効果〕〔effect〕

以上説明したように本発明の信号検出器によれば、監視
対象線である一対の平衡形通信線と電極間に生じる結合
静電容量に近似した容量値を、二つの電極間に発生する
機能を持つ手段と、帯域補償を行う補償用外部静電容量
を付加させた。
As explained above, the signal detector of the present invention has the function of generating a capacitance between two electrodes that approximates the coupling capacitance that occurs between the pair of balanced communication lines, which are the lines to be monitored, and the electrodes. In addition, we added a compensating external capacitor to perform band compensation.

また請求項(2)では、監視対象線である不衡形通信線
と電極間に生じる結合静電容量に近似した容量値を、電
極と対地間に発生する機能を持つ手段と、帯域補償を行
う補償用外部静電容量を付加させた。そのため、伝達特
性は低周波数まで平坦な特性となる。
Claim (2) also provides means for generating a capacitance between the electrode and ground, which approximates the coupling capacitance generated between the unbalanced communication line, which is the line to be monitored, and the electrode, and band compensation. An external capacitance was added for compensation. Therefore, the transfer characteristics are flat down to low frequencies.

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

第1図は、本発明の一実施例を示す電極部分の接続図、 第2図はその等価回路図、 第3図は第一の実施例による電圧減衰量の周波数特性図
、 第4図は従来の静電結合方式の概念図、第5図はその等
価回路図、 第6図は従来の方式による電圧減衰量の周波数特性図で
ある。 1・・・監視対象線、 2・・・補償心線、 3・・・電極、 4・・・補償用外部静電容量、 5・・・負荷抵抗、 6・・・地(アース)。
Fig. 1 is a connection diagram of the electrode portion showing one embodiment of the present invention, Fig. 2 is its equivalent circuit diagram, Fig. 3 is a frequency characteristic diagram of voltage attenuation according to the first embodiment, and Fig. 4 is A conceptual diagram of the conventional capacitive coupling method, FIG. 5 is its equivalent circuit diagram, and FIG. 6 is a frequency characteristic diagram of voltage attenuation amount by the conventional method. 1... Line to be monitored, 2... Compensating core wire, 3... Electrode, 4... External capacitance for compensation, 5... Load resistance, 6... Earth (earth).

Claims (2)

【特許請求の範囲】[Claims] (1)監視対象線である一対の平衡形通信線に静電結合
する二つの電極を備え、静電容量により結合する信号検
出器において、 前記監視対象線と前記電極間に生じる結合静電容量に近
似した容量値を前記二つの電極間に発生する機能を持つ
手段と、更に帯域補償を行う補償用外部静電容量を付加
させた信号検出器。
(1) In a signal detector that is equipped with two electrodes that are capacitively coupled to a pair of balanced communication lines that are monitored lines, the coupling capacitance that occurs between the monitored line and the electrodes. A signal detector having a function of generating a capacitance value approximating to between the two electrodes, and further adding an external compensating capacitance for band compensation.
(2)監視対象である不平衡形通信線に静電結合する電
極を備え、静電容量により結合する信号検出器において
、 前記監視対象線と前記電極間に生じる結合静電容量に近
似した容量値を前記電極と対地間に発生する機能を持つ
手段と、更に帯域補償を行う補償用外部静電容量を付加
させた信号検出器。
(2) In a signal detector that is equipped with an electrode that is capacitively coupled to an unbalanced communication line to be monitored and is coupled by capacitance, a capacitance that approximates the coupling capacitance that occurs between the line to be monitored and the electrode. A signal detector comprising means for generating a value between the electrode and the ground, and an external compensating capacitance for performing band compensation.
JP7518090A 1990-03-24 1990-03-24 Signal detector Expired - Fee Related JPH0783299B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP7518090A JPH0783299B2 (en) 1990-03-24 1990-03-24 Signal detector

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP7518090A JPH0783299B2 (en) 1990-03-24 1990-03-24 Signal detector

Publications (2)

Publication Number Publication Date
JPH03274827A true JPH03274827A (en) 1991-12-05
JPH0783299B2 JPH0783299B2 (en) 1995-09-06

Family

ID=13568751

Family Applications (1)

Application Number Title Priority Date Filing Date
JP7518090A Expired - Fee Related JPH0783299B2 (en) 1990-03-24 1990-03-24 Signal detector

Country Status (1)

Country Link
JP (1) JPH0783299B2 (en)

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006515678A (en) * 2003-01-17 2006-06-01 ヴァーサセンサ・エイビイ Sensor device
JP2012032202A (en) * 2010-07-29 2012-02-16 Toyo Networks & System Integration Co Ltd Signal extractor and signal measurement apparatus employing the same

Cited By (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006515678A (en) * 2003-01-17 2006-06-01 ヴァーサセンサ・エイビイ Sensor device
JP2012032202A (en) * 2010-07-29 2012-02-16 Toyo Networks & System Integration Co Ltd Signal extractor and signal measurement apparatus employing the same

Also Published As

Publication number Publication date
JPH0783299B2 (en) 1995-09-06

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