JPS60152959A - Potential sensor - Google Patents

Potential sensor

Info

Publication number
JPS60152959A
JPS60152959A JP882284A JP882284A JPS60152959A JP S60152959 A JPS60152959 A JP S60152959A JP 882284 A JP882284 A JP 882284A JP 882284 A JP882284 A JP 882284A JP S60152959 A JPS60152959 A JP S60152959A
Authority
JP
Japan
Prior art keywords
output
potential sensor
distance
electrodes
output voltages
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
JP882284A
Other languages
Japanese (ja)
Other versions
JPH0320709B2 (en
Inventor
Hiroaki Yamada
博章 山田
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.)
NEC Corp
Original Assignee
NEC Corp
Nippon 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 NEC Corp, Nippon Electric Co Ltd filed Critical NEC Corp
Priority to JP882284A priority Critical patent/JPS60152959A/en
Publication of JPS60152959A publication Critical patent/JPS60152959A/en
Publication of JPH0320709B2 publication Critical patent/JPH0320709B2/ja
Granted legal-status Critical Current

Links

Abstract

PURPOSE:To enable the measurement of a correct electrostatic field by a differential amplification of output voltages from two electrodes. CONSTITUTION:Two detection electrodes 3a and 3b are arranged on a substrate 8 so as to be varied in the height and output voltages Va and Vb outputted from output terminals 5a and 5b of the electrodes 3a and 3b are supplied to amplifiers 11 and 12 of a differential amplification section. The output voltages Va and Vb of the terminal 5a and 5b have different distance characteristics and hence, output voltages V1 and V2 of the amplifiers 11 and 12 are inputted into a differential amplifier 13 through a resistance R1. The output voltage V3 thereof 13 indicates a surface potential of an object to be measured free from distance by setting the voltages V1 and V2 here and the resistance ratio R1/R2 at specified values respectively.

Description

【発明の詳細な説明】 (孜術分野) 不発明は電位センv1特に静電界の強度検出や帯′電量
の測定等に使用する電位センサに関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Science and Technology) The present invention relates to a potential sensor v1, particularly a potential sensor used for detecting the strength of an electrostatic field, measuring the amount of charge, etc.

(従来技術) 一般に電位センナは被測足vIJから放射される電気力
線を導入するための検出孔を待つケースと、ケース内に
入ってくる′電気力線を一定の周期で切るチ四ツバ部と
、この切らrtた電気力lIMを受けて交泥信号を取り
出すだめの1極とから構成さtている。
(Prior art) In general, potential sensors have two types: one that waits for a detection hole to introduce the lines of electric force radiated from the foot to be measured vIJ, and the other that waits for a detection hole to introduce the lines of electric force radiated from the foot to be measured, and the other that waits for a detection hole to introduce the lines of electric force that enter the case. It consists of a part and one pole for receiving this cut electric force lIM and taking out an exchange signal.

第1図(a)および(b)はそfl;f:n−従来の′
電位センサの一例を示す平面断面図ひよび側面断面図で
るる。
FIGS. 1(a) and (b) are fl;f:n-conventional'
1 is a plan sectional view and a side sectional view showing an example of a potential sensor.

同図において、チョッパ部には駆動用の圧電セラミック
ス6を接着した音叉2を使用して2す、音叉2の元端部
2aνよび2bで電気力線7が切ら動用端子4.出力端
子5および接地端子9が取り付けられ、音叉駆動用端子
4と圧電セラミック6間は所要の内部配線が施ざnてい
る。
In the figure, a tuning fork 2 to which piezoelectric ceramics 6 for driving is bonded is used in the chopper part, and lines of electric force 7 are cut at the base ends 2aν and 2b of the tuning fork 2 to drive terminals 4. An output terminal 5 and a ground terminal 9 are attached, and necessary internal wiring is provided between the tuning fork drive terminal 4 and the piezoelectric ceramic 6.

次に第2図は第1図に寂ける電位センサの距離tF!j
性の一例を示す特性図で、は位センブは蛍シしている被
測定物からの距離りにょシ出カ端子5(第1図に図示)
からの出力電圧■が変化する。すなわち、同一表面電位
で帯電している複数の被測定物でめっても各被測定物か
ら電位センサまでの距離(測定距離)Dによって出力電
圧■の値は異なってくる。従って第1図に2いて、電位
センサを被測定物からめる一定の距離に固定した後に被
測定物に既知の表面電位を、印加して校正してPく必要
がめシ、しかも電位センサの取付位置によって出力電圧
が大きくばらつくのでその取付精度が厳しく要求さnる
という欠点がめった。
Next, Figure 2 shows the distance tF of the potential sensor that is missing in Figure 1! j
This is a characteristic diagram showing an example of the characteristics of the output terminal 5 (shown in Figure 1).
The output voltage from ■ changes. That is, even if a plurality of objects to be measured are charged with the same surface potential, the value of the output voltage (2) will differ depending on the distance (measurement distance) D from each object to the potential sensor. Therefore, as shown in Figure 1, it is necessary to fix the potential sensor at a certain distance from the object to be measured and then calibrate it by applying a known surface potential to the object. Since the output voltage fluctuates greatly due to this, the mounting accuracy is often required to be very strict.

(発明の目的) 不発明の目的は、2つの電極からの出力電圧を差動増幅
することによシ上記欠点を除去し、正しい静電界の測定
等を行えるようにした電位センサを提供することにめる
(Object of the invention) The object of the invention is to provide a potential sensor that eliminates the above drawbacks by differentially amplifying the output voltage from two electrodes, and that enables accurate measurement of electrostatic fields, etc. Smell.

(発明の構成) 不発明によnば、被測定物から放射さnる電気力線を一
定の周期で切るチロツバ部と、該チ■ツバ部により切ら
n几電気力線を受ける電極部と、前記テ冒ツバ部および
前記電極部を搭載する基板と、前記電気力線を導入する
だめの検出孔を有し前記基板を収容するケースとを備え
る電位センサに2いて、前記電極部は互いに異なる高さ
に前記基板に配置さnた2つの電極から構成さn且っ該
電極からの出力電圧を差動増幅手段に接続するこする。
(Structure of the Invention) According to the invention, there is provided a chiro-flange part that cuts the electric lines of force radiated from the object to be measured at regular intervals, and an electrode part that receives the electric flux lines cut by the chiro-flange part. , a potential sensor including a substrate on which the teat flange portion and the electrode portion are mounted, and a case housing the substrate and having a detection hole for introducing the electric line of force, the electrode portions being mutually connected to each other. It consists of two electrodes placed on the substrate at different heights, and the output voltage from the electrodes is connected to differential amplification means.

第3図(a)、 (b)および(C)はそnぞn本発明
の電位センサに2けるセンサ部の一実施例を示す平面断
面図、側面断面図および斜視図でるるP砲において、第
1図と同一の参照符号は従来例と同一の構成要素を示す
。本実施例においては、基板8に2つの検出電極3a、
3bおよびチョッパ部でめる音叉2が取)付けらtL、
検出電極3aおよび3bはそnぞ−n高さが異なるよう
に配置さnている。従って検出゛電極3aおよび3bで
検出さn出力端子5aおよび5bから出力さnる出力電
圧はそnぞn異なっ交互lli特性を有することになる
FIGS. 3(a), (b) and (C) are a plan sectional view, a side sectional view and a perspective view showing one embodiment of the sensor portion of the potential sensor of the present invention, respectively, in the P gun. , the same reference numerals as in FIG. 1 indicate the same components as in the conventional example. In this embodiment, the substrate 8 includes two detection electrodes 3a,
3b and the tuning fork 2 attached at the chopper part) are attached tL,
The detection electrodes 3a and 3b are arranged at different heights. Therefore, the output voltages detected by the detection electrodes 3a and 3b and outputted from the output terminals 5a and 5b are different from each other and have alternating characteristics.

続いて不発明の電位センナによシ距離特性を除去する方
法について説明する。第2図に示した従来の電位センサ
の距離特性は次式で表さnる。
Next, a method for removing the distance characteristic using an uninvented potential sensor will be explained. The distance characteristic of the conventional potential sensor shown in FIG. 2 is expressed by the following equation.

V=E(−十b)・・・・・・・・・・・・・・・(1
)ここでVは出力電圧、Eは被測定物の表面電位、Dは
被測定物と電位センナの距離およびa、 bは定数でめ
る。
V=E(-10b)・・・・・・・・・・・・(1
) Here, V is the output voltage, E is the surface potential of the object to be measured, D is the distance between the object to be measured and the potential sensor, and a and b are constants.

従って、距離りを変化させて2点以上の測定を行えば定
数のa、bが決定さ扛、第2図に示し友ような距離特性
が一義的に決定さnる。不実施例に2いても出力端子5
a、5bからそn−5rt、出力される出力電圧va、
Vbは上記と同様の距離特性を有するが、該出力電圧v
a、Vbを組み合わせることによシ距離りに依存せずに
被測定物の表面電位を測定することができる。検出電極
3aおよび3bでの距離特性を表わす式は七牡ぞn ■a =”’ Cn +bl )・・・・・・・・・・
・・(2Vb=E (B+bz)・・・・・・・・・・
・・・(3)でめり、こしら(2)式および(3)式か
ら距離りを消去すると が得られる。すなわち(4)式によれば表面電位EH2
つの検出電極の出力電圧va、Vbによシ簡単な式で表
わさnることが分かる。ここでale ”2ab1*J
は定数なので、出力電圧va、Vbが分かれば距離りに
関係することなく被測定物の表面電位Eが決定される。
Therefore, by changing the distance and measuring at two or more points, the constants a and b are determined, and the distance characteristic shown in FIG. 2 is uniquely determined. Output terminal 5 even if it is 2 in non-implemented example
a, 5b to n-5rt, output voltage va,
Vb has the same distance characteristics as above, but the output voltage v
By combining a and Vb, the surface potential of the object to be measured can be measured without depending on the distance. The formula expressing the distance characteristics at the detection electrodes 3a and 3b is as follows.
・・・(2Vb=E (B+bz)・・・・・・・・・・
...(3), and by eliminating the distance from equations (2) and (3), we obtain. That is, according to equation (4), the surface potential EH2
It can be seen that the output voltages va and Vb of the two detection electrodes can be expressed by a simple equation. Here ale “2ab1*J
are constants, so if the output voltages va and Vb are known, the surface potential E of the object to be measured can be determined regardless of the distance.

この(4)式を実現する丸めには不発明の電位センサー
に例えば第4図に示す差動増幅手段を接続すねはよい。
For rounding to realize this equation (4), for example, the differential amplification means shown in FIG. 4 may be connected to the uninvented potential sensor.

第4図は不発明の電位センサにおける差動増幅部の一実
施例を示す回路図でめる。同図において、差動増幅部は
センサ部の出力端子5a、5bからの各出力電圧V、、
Vbをそnぞn増幅する一般的な増幅器11.12と。
FIG. 4 is a circuit diagram showing an embodiment of the differential amplifier section in the potential sensor according to the invention. In the same figure, the differential amplification section has each output voltage V from the output terminals 5a, 5b of the sensor section,
General amplifiers 11 and 12 each amplify Vb.

該増幅器11.12の各出力電圧Vl、Vl をそれぞ
n抵抗R1を介して−0士湘子に入力する一般的な差動
増幅器13とから成シ、差動増幅器13の出力端子から
出力電圧vs″t”取り出すとともに。
It consists of a general differential amplifier 13 which inputs the output voltages Vl and Vl of the amplifiers 11 and 12 to the -0 signal through resistors R1, respectively, and the output voltage from the output terminal of the differential amplifier 13. vs"t" and take it out.

抵抗R2を介して前記一端子に接続さnている。It is connected to the one terminal via a resistor R2.

不回路において、出力電圧Y1.V2 および抵抗比R
t/Rz kそれぞniloazVB、 vz=alV
b>よびR1/Rz=alb2−asJ(*だL/ ”
 1m ” L bisb2は(4)式に示し次定数)
に定めnば前記(4)式により出力電圧v3 は被測定
物の表面電位Eを示すことになるのは明白である。
In the non-circuit, the output voltage Y1. V2 and resistance ratio R
t/Rz k respectively niroazVB, vz=alV
b> and R1/Rz=alb2-asJ(*daL/”
1m ” L bisb2 is shown in equation (4) and is the following constant)
It is clear that if n is defined as n, the output voltage v3 will indicate the surface potential E of the object to be measured according to the above equation (4).

(発明の効果) 以上の説明によシ明らかなように本発明の電位センサに
よりば、2つの電極からの出力電圧を簡単な差動増幅手
段に接続することによって電位センサの有する距離特性
の影響を除去できるので、被測定物の表面電位を正しく
且つ容易に測定できるという効果が生じる。
(Effects of the Invention) As is clear from the above explanation, according to the potential sensor of the present invention, the distance characteristics of the potential sensor can be influenced by connecting the output voltages from the two electrodes to a simple differential amplification means. can be removed, resulting in the effect that the surface potential of the object to be measured can be measured accurately and easily.

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

第1図(a)2よび〜)はそn(Jn従来の電位センサ
の一例を示す平面断面図2よび側面断面図、第2図は第
1図に2ける電位センナの距離特性の一例を示す特性図
、第3図(a)、 (b)、 (c)はそnぞn不発明
の電位センサにおけるセンサ部の一実施例を示す平面断
面図、側面断面図、斜視図および第4図は本発明の電位
センサにおける差動増幅部の一実施例を示す回路図でる
る。 図において、1・・・・・・ケース、2・旧・・音叉、
2a。 2b・・・・・・先端部、3.3a、 ab・・・・・
・検出電極、4・・・・・・音叉駆動用端子、5s 5
a、5b・・・・・・出力端子、6・・・・・・圧電セ
ラはツク、7・・・・・・電気力線、8・・・・・・基
板、9・・・・・・接地端子% 1o・・・・・・検出
孔、11゜12・・・・・・増幅器、13・・・・・・
差動増幅器。 茅10 ¥−5絽 キ4−回 2
Figure 1 (a) 2 and ~) is a plan sectional view 2 and a side sectional view showing an example of a conventional potential sensor. Figure 2 shows an example of the distance characteristics of the potential sensor 2 in Figure 1. The characteristic diagrams shown in FIGS. 3(a), 3(b), and 3(c) are a plan sectional view, a side sectional view, a perspective view, and a fourth The figure is a circuit diagram showing an embodiment of the differential amplifier section in the potential sensor of the present invention. In the figure, 1...case, 2...old tuning fork,
2a. 2b... tip, 3.3a, ab...
・Detection electrode, 4... Tuning fork drive terminal, 5s 5
a, 5b... Output terminal, 6... Piezoelectric ceramic is connected, 7... Lines of electric force, 8... Substrate, 9...・Grounding terminal% 1o...Detection hole, 11゜12...Amplifier, 13...
Differential amplifier. Kaya 10 ¥-5 Koki 4-times 2

Claims (1)

【特許請求の範囲】[Claims] 被1411定物から放射さnる電気力線を一定の周期で
切るテ田ツバ部と、ぎチョッパ部により切らn友゛嵯気
力Nを受ける電極部と、前記テ璽ツバ部および前記電極
部を搭載する基板と、前aa ’!電気力線導入するた
めの検出孔を有し@記基板を収容するケースとを備える
′這位セン′り′にpいて、前S己電極部は互いに異な
る高さに前記基板に配置さ牡た2つの磁極から構成さn
1且つ該′嵯極からの出力′磁圧を差動増幅手段に接続
することを特徴とする電位センサ。
1411 A tape collar portion that cuts electric lines of force radiated from a fixed object at a constant cycle, an electrode portion that receives the cutting force N by a chopper portion, the wire collar portion and the electrode portion. The board that carries the and the front aa'! The front electrode portions are arranged on the substrate at different heights from each other in a ``vertical sensor'' which has a detection hole for introducing electric lines of force and a case for accommodating the substrate. Consisting of two magnetic poles
1, and the output magnetic pressure from the top pole is connected to differential amplification means.
JP882284A 1984-01-20 1984-01-20 Potential sensor Granted JPS60152959A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP882284A JPS60152959A (en) 1984-01-20 1984-01-20 Potential sensor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP882284A JPS60152959A (en) 1984-01-20 1984-01-20 Potential sensor

Publications (2)

Publication Number Publication Date
JPS60152959A true JPS60152959A (en) 1985-08-12
JPH0320709B2 JPH0320709B2 (en) 1991-03-20

Family

ID=11703493

Family Applications (1)

Application Number Title Priority Date Filing Date
JP882284A Granted JPS60152959A (en) 1984-01-20 1984-01-20 Potential sensor

Country Status (1)

Country Link
JP (1) JPS60152959A (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH028755A (en) * 1988-01-27 1990-01-12 Nec Corp Potential sensor
JPH02201173A (en) * 1989-01-30 1990-08-09 Nec Corp Potential sensor
JP2014186018A (en) * 2013-02-25 2014-10-02 Ricoh Co Ltd Potential detector and image forming apparatus

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH028755A (en) * 1988-01-27 1990-01-12 Nec Corp Potential sensor
JPH02201173A (en) * 1989-01-30 1990-08-09 Nec Corp Potential sensor
JP2014186018A (en) * 2013-02-25 2014-10-02 Ricoh Co Ltd Potential detector and image forming apparatus

Also Published As

Publication number Publication date
JPH0320709B2 (en) 1991-03-20

Similar Documents

Publication Publication Date Title
US20070044370A1 (en) Coil, coil module and method of manufacturing the same, current sensor and method of manufacturing the same
KR100750439B1 (en) Magnetic sensor
US11143719B2 (en) Magnetic sensor and current sensor
US4176555A (en) Signal amplifier system for controlled carrier signal measuring sensor/transducer of the variable impedance type
EP1424563B1 (en) Capacitance measuring circuit, capacitance measuring instrument, and microphone device
US3882387A (en) Electrical current detector
JPS582084A (en) Hall element device
JPS60152959A (en) Potential sensor
JPS6211184A (en) Method and device for measuring current
JP2003075487A (en) Impedance detection apparatus and capacitance detection apparatus
US6989623B2 (en) Method and apparatus for measurement using piezoelectric sensor
JP2001153659A (en) Angular velocituy sensor
JP2003156551A (en) Method for calibrating capacitance meter, calibrating standard capacitance box, method for measuring electrostatic capacity, box for measuring capacity and capacitance meter
US4908575A (en) Circuit for measuring diffusion-limited current
JPS626171B2 (en)
US6861717B2 (en) Device for defecting a magnetic field, magnetic field measure and current meter
JP3157907B2 (en) Acceleration detector
CN110987223B (en) Improved high-precision platinum resistor temperature measuring circuit
JPH0747742Y2 (en) Current detector
JPS58204313A (en) Detecting head of linear scale
JP2003315089A (en) Strain gauge
SU1064156A1 (en) Semiconducor temperature pickup
JPS6361961A (en) Current detector
JPH052865Y2 (en)
JPH0628702Y2 (en) Current detector