JP2002365321A - Field sensor - Google Patents
Field sensorInfo
- Publication number
- JP2002365321A JP2002365321A JP2001174928A JP2001174928A JP2002365321A JP 2002365321 A JP2002365321 A JP 2002365321A JP 2001174928 A JP2001174928 A JP 2001174928A JP 2001174928 A JP2001174928 A JP 2001174928A JP 2002365321 A JP2002365321 A JP 2002365321A
- Authority
- JP
- Japan
- Prior art keywords
- electric field
- waveform
- field sensor
- conductor
- space
- 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
Landscapes
- Details Of Aerials (AREA)
Abstract
Description
【0001】[0001]
【発明の属する技術分野】この発明は、ダイポールアン
テナでもって空間の電界を検出する電界センサに関し、
特に、高周波ノイズの入らない電界センサに関する。BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to an electric field sensor for detecting an electric field in a space by using a dipole antenna.
In particular, it relates to an electric field sensor that does not contain high-frequency noise.
【0002】[0002]
【従来の技術】図3は、従来の電界センサを示し、
(A)はその構成を示す斜視図、(B)は図3の(A)
の等価回路図である。図3の(A)において、従来の電
界センサにおけるダイポールアンテナ1は、互いに逆方
向に向けて直線状に空間7に配された導体棒1A,1B
からなり、導体棒1A,1Bが対向する側の端部8が差
動増幅器3の入力端に接続され、差動増幅器3の出力端
が波形表示装置4の入力端に接続されている。差動増幅
器3には導体棒1A,1Bによって拾われたそれぞれの
電波信号が入力され、差動増幅器3がその電波信号の差
を取ることによって空間7の電界に比例する信号を出力
する。波形表示装置4が差動増幅器3から出力される信
号を波形にして表示するようになっている。FIG. 3 shows a conventional electric field sensor.
(A) is a perspective view showing the configuration, (B) is (A) of FIG.
3 is an equivalent circuit diagram of FIG. In FIG. 3A, a dipole antenna 1 in a conventional electric field sensor includes conductor rods 1A and 1B linearly arranged in a space 7 in opposite directions.
The end 8 on the side facing the conductor bars 1A and 1B is connected to the input terminal of the differential amplifier 3, and the output terminal of the differential amplifier 3 is connected to the input terminal of the waveform display device 4. Each of the radio signals picked up by the conductor bars 1A and 1B is input to the differential amplifier 3, and the differential amplifier 3 outputs a signal proportional to the electric field in the space 7 by taking the difference between the radio signals. The waveform display device 4 displays the signal output from the differential amplifier 3 as a waveform.
【0003】図3の(B)において、太線が導体棒1
A,1Bに対応し、キャパシタンスCは導体棒1A,1
Bと接地Eとの間にそれぞれ分布する浮遊容量、抵抗R
は差動増幅器3の入力抵抗である。ダイポールアンテナ
1を電界センサとする場合には、抵抗Rとしてその抵抗
値の大きいものが用いられ、キャパシタンスCと抵抗R
とで導体棒1A,1Bからの電波信号が積分されるよう
になっている。[0003] In FIG. 3 (B), a thick line represents a conductor bar 1.
A, 1B, and the capacitance C is the conductor rod 1A, 1B.
Stray capacitance and resistance R distributed between B and ground E, respectively.
Is the input resistance of the differential amplifier 3. When the dipole antenna 1 is an electric field sensor, a resistor having a large resistance value is used as the resistor R, and the capacitance C and the resistor R
Thus, the radio signals from the conductor bars 1A and 1B are integrated.
【0004】[0004]
【発明が解決しようとする課題】しかしながら、前述し
たような従来の電界センサは、高周波ノイズが入るとい
う問題があった。図4は、図3の従来の電界センサによ
る電界の波形観測結果を示し、(A)は波形表示装置で
得られた電界の波形図、(B)は空間に発生させた電界
の波形図であり、いずれも横軸が時間(100ns/d
iv)、縦軸が電界である。すなわち、図3において、
電界の波形観測においては、ダイポールアンテナ1を図
示されていない電界発生装置の空間7内に配し、その空
間7に数百nsで立ち上がる電界を発生させた。図4の
(B)における波形6Bは、電界発生装置から電界を形
成させるために用いられた電圧の波形であり、その波形
6Bが空間7中に形成された真の電界波形に対応する。
図4の(A)における波形6Aは、図3における電界セ
ンサによるものであるが、波形に高周波ノイズが重畳し
波形観測の精度が悪かった。However, the conventional electric field sensor as described above has a problem that high frequency noise is introduced. 4A and 4B show results of electric field waveform observation by the conventional electric field sensor of FIG. 3, wherein FIG. 4A is a waveform chart of an electric field obtained by a waveform display device, and FIG. 4B is a waveform chart of an electric field generated in space. In each case, the horizontal axis represents time (100 ns / d
iv), the vertical axis is the electric field. That is, in FIG.
In the observation of the electric field waveform, the dipole antenna 1 was disposed in the space 7 of an electric field generator (not shown), and an electric field rising in the space 7 for several hundred ns was generated. A waveform 6B in FIG. 4B is a waveform of a voltage used for forming an electric field from the electric field generator, and the waveform 6B corresponds to a true electric field waveform formed in the space 7.
The waveform 6A in FIG. 4A is from the electric field sensor in FIG. 3, but the high-frequency noise was superimposed on the waveform and the accuracy of waveform observation was poor.
【0005】この発明の目的は、高周波ノイズの入らな
い電界センサを提供することにある。An object of the present invention is to provide an electric field sensor free from high-frequency noise.
【0006】[0006]
【課題を解決するための手段】上記目的を達成するため
に、この発明によれば、2本の導体棒が互いに逆方向に
向けて直線状に空間に配されてなるダイポールアンテナ
の前記導体棒が対向する側の端部から検出される信号の
差を前記空間の電界とする電界センサにおいて、前記導
体棒がそれぞれが外部導体で覆われてなるようにすると
よい。それによって、外部導体と導体棒との間に分布す
る浮遊容量が電波信号を積分するので高周波ノイズが減
衰するようになる。According to the present invention, there is provided a dipole antenna in which two conductor rods are linearly arranged in space in opposite directions to each other. In an electric field sensor in which the difference between signals detected from the ends on the opposite side is an electric field in the space, it is preferable that each of the conductor bars is covered with an external conductor. Thus, the stray capacitance distributed between the outer conductor and the conductor bar integrates the radio signal, so that high-frequency noise is attenuated.
【0007】[0007]
【発明の実施の形態】以下、この発明を実施例に基づい
て説明する。図1は、この発明の実施例にかかる電界セ
ンサを示し、(A)はその構成を示す斜視図、(B)は
図1の(A)の等価回路図である。図1の(A)におい
て、導体棒1A,1Bがそれぞれ同軸の円筒状の外部導
体2A,2Bで覆われている。また、図1の(B)にお
いて、キャパシタンスC0 は、太線で示す外部導体2
A,2Bと、導体棒1A,1Bとの間にそれぞれ分布す
る浮遊容量である。図1のその他は、図3の従来の場合
と同じであり、従来と同じ部分は同一参照符号を付ける
ことによって詳細な説明は省略する。DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described below with reference to embodiments. 1A and 1B show an electric field sensor according to an embodiment of the present invention, in which FIG. 1A is a perspective view showing the configuration, and FIG. 1B is an equivalent circuit diagram of FIG. In FIG. 1A, conductor rods 1A and 1B are covered with coaxial cylindrical outer conductors 2A and 2B, respectively. In FIG. 1B, the capacitance C 0 is the external conductor 2 indicated by a thick line.
A, 2B and the stray capacitance distributed between the conductor rods 1A, 1B, respectively. Other parts of FIG. 1 are the same as the conventional case of FIG. 3, and the same parts as those of the conventional case are denoted by the same reference numerals, and the detailed description is omitted.
【0008】図2は、図1の電界センサによる電界の波
形観測結果を示し、(A)は波形表示装置で得られた電
界の波形図、(B)は空間に発生させた電界の波形図で
あり、いずれも横軸が時間(100ns/div)、縦
軸が電界である。すなわち、図1において、電界の波形
観測においては、ダイポールアンテナ1を図示されてい
ない電界発生装置の空間7に配し、その空間7に数百n
sで立ち上がる電界を発生させた。図2の(B)におけ
る波形5Bは、図4の(B)における波形6Bと同様
で、電界発生装置から電界を形成させるために用いられ
た電圧の波形であり、真の電界波形に対応する。図2の
(A)における波形5Aは、図1における電界センサに
よるものであるが、高周波ノイズが除去され波形観測の
精度が従来より向上している。これは、外部導体2A,
2Bと導体棒1A,1Bとの間にそれぞれ分布するキャ
パシタンスC0 に並列に形成される抵抗が無限大と高い
ため、その外部導体2A,2Bと導体棒1A,1Bとの
間で電波信号がそれぞれ積分され、高周波ノイズが減衰
することによる。FIGS. 2A and 2B show the results of electric field waveform observation by the electric field sensor of FIG. 1, wherein FIG. 2A is a waveform chart of an electric field obtained by a waveform display device, and FIG. In each case, the horizontal axis represents time (100 ns / div), and the vertical axis represents electric field. That is, in FIG. 1, in observing the waveform of the electric field, the dipole antenna 1 is arranged in a space 7 of an electric field generator (not shown), and several hundred n
An electric field rising at s was generated. The waveform 5B in FIG. 2B is the same as the waveform 6B in FIG. 4B, the waveform of the voltage used to generate the electric field from the electric field generator, and corresponds to the true electric field waveform. . The waveform 5A in FIG. 2A is from the electric field sensor in FIG. 1, but the high-frequency noise has been removed and the accuracy of waveform observation has been improved compared to the related art. This is the outer conductor 2A,
Since the resistance formed in parallel with the capacitance C 0 distributed between the outer conductors 2A and 2B and the conductor rods 1A and 1B is infinite and high, a radio signal is transmitted between the outer conductors 2A and 2B and the conductor rods 1A and 1B. Each is integrated and the high frequency noise is attenuated.
【0009】[0009]
【発明の効果】この発明は前述のように、導体棒がそれ
ぞれが外部導体で覆われるようにすることによって、高
周波ノイズが除去され電界波形観測の精度が向上するよ
うになった。As described above, according to the present invention, by covering each of the conductor rods with an external conductor, high-frequency noise is removed and the accuracy of electric field waveform observation is improved.
【図面の簡単な説明】[Brief description of the drawings]
【図1】この発明の実施例にかかる電界センサを示し、
(A)はその構成を示す斜視図、(B)は図1の(A)
の等価回路図FIG. 1 shows an electric field sensor according to an embodiment of the present invention;
(A) is a perspective view showing the configuration, (B) is (A) of FIG.
Equivalent circuit diagram of
【図2】図1の電界センサによる電界の波形観測結果を
示し、(A)は波形表示装置で得られた電界の波形図、
(B)は空間に発生させた電界の波形図2A and 2B show the results of an electric field waveform observed by the electric field sensor of FIG. 1; FIG. 2A is a waveform diagram of the electric field obtained by a waveform display device;
(B) is a waveform diagram of the electric field generated in the space.
【図3】従来の電界センサを示し、(A)はその構成を
示す斜視図、(B)は図3の(A)の等価回路図3A and 3B show a conventional electric field sensor, in which FIG. 3A is a perspective view showing a configuration thereof, and FIG. 3B is an equivalent circuit diagram of FIG.
【図4】図3の電界センサによる電界の波形観測結果を
示し、(A)は波形表示装置で得られた電界の波形図、
(B)は空間に発生させた電界の波形図4A and 4B show results of electric field waveform observation by the electric field sensor shown in FIG. 3, wherein FIG.
(B) is a waveform diagram of the electric field generated in the space.
1:ダイポールアンテナ、1A,1B:導体棒、2A,
2B:外部導体、8:端部1: dipole antenna, 1A, 1B: conductor rod, 2A,
2B: outer conductor, 8: end
Claims (1)
状に空間に配されてなるダイポールアンテナの前記導体
棒が対向する側の端部から検出される信号の差を前記空
間の電界とする電界センサにおいて、前記導体棒がそれ
ぞれが外部導体で覆われてなることを特徴とする電界セ
ンサ。1. A dipole antenna in which two conductor rods are linearly arranged in opposite directions in a space, and a difference between signals detected from an end of the dipole antenna on a side opposite to the conductor rods is determined. An electric field sensor for an electric field, wherein each of the conductor bars is covered with an external conductor.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2001174928A JP2002365321A (en) | 2001-06-11 | 2001-06-11 | Field sensor |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP2001174928A JP2002365321A (en) | 2001-06-11 | 2001-06-11 | Field sensor |
Publications (1)
Publication Number | Publication Date |
---|---|
JP2002365321A true JP2002365321A (en) | 2002-12-18 |
Family
ID=19016143
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP2001174928A Pending JP2002365321A (en) | 2001-06-11 | 2001-06-11 | Field sensor |
Country Status (1)
Country | Link |
---|---|
JP (1) | JP2002365321A (en) |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006295712A (en) * | 2005-04-13 | 2006-10-26 | Yagi Antenna Co Ltd | Onboard antenna incorporated with door |
JP2015001458A (en) * | 2013-06-17 | 2015-01-05 | 株式会社日立製作所 | Probe for near electric field measurement and near electric field measurement system using the same |
-
2001
- 2001-06-11 JP JP2001174928A patent/JP2002365321A/en active Pending
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JP2006295712A (en) * | 2005-04-13 | 2006-10-26 | Yagi Antenna Co Ltd | Onboard antenna incorporated with door |
JP2015001458A (en) * | 2013-06-17 | 2015-01-05 | 株式会社日立製作所 | Probe for near electric field measurement and near electric field measurement system using the same |
Similar Documents
Publication | Publication Date | Title |
---|---|---|
US7298140B2 (en) | Three-dimensional magnetic direction sensor, and magneto-impedance sensor element | |
US6831457B2 (en) | Two-dimensional magnetic sensor including magneto-impedance sensor elements | |
EP1426772B1 (en) | Impedance measuring circuit, its method, and capacitance measuring circuit | |
US7482814B2 (en) | Electric/magnetic field sensor | |
US6184693B1 (en) | Electromagnetic noise measurement apparatus | |
JPS59231909A (en) | Piezoelectric crystal vibrator | |
JP2002365321A (en) | Field sensor | |
Tiep et al. | Tilt sensor based on three electrodes dielectric liquid capacitive sensor | |
JP2009094849A (en) | Capacitance change detection circuit, touch panel and determining method | |
EP2040086B1 (en) | Sensor for non-contact electric field measurements | |
JP2002048836A (en) | Method of detecting partial discharge in power cable | |
JP2015152505A (en) | magnetic detection device | |
CN103969566B (en) | SMU RF transistor stability devices | |
JP7067920B2 (en) | Tablet | |
JP2000028661A (en) | Grounding resistance measurement method and device thereof | |
JPS59148855A (en) | Measuring device for conductance of epidermal horny layer | |
JPS6278901A (en) | Oscillation device | |
TWI579569B (en) | Multimeter with wireless transmission function | |
JPS5822137Y2 (en) | High frequency probe device | |
JPH0744093Y2 (en) | Wide wavelength band receiving antenna | |
CN106154191B (en) | Magnetic resonance imaging device, power amplifier module and power synthesizer | |
JP3047514U (en) | Simple high-frequency power meter | |
JP2020183878A (en) | High-speed and high-sensitivity magnetic sensor | |
JP3024616B2 (en) | Variable resistor for high voltage | |
JPH0682538A (en) | Nmr probe |