JPS59204772A - Surface potential meter - Google Patents

Surface potential meter

Info

Publication number
JPS59204772A
JPS59204772A JP8019483A JP8019483A JPS59204772A JP S59204772 A JPS59204772 A JP S59204772A JP 8019483 A JP8019483 A JP 8019483A JP 8019483 A JP8019483 A JP 8019483A JP S59204772 A JPS59204772 A JP S59204772A
Authority
JP
Japan
Prior art keywords
electrode
potential
measured
vibrator
linear
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
JP8019483A
Other languages
Japanese (ja)
Inventor
Tadashi Ishikawa
正 石川
Koji Suzuki
鈴木 孝二
Joji Nagahira
譲二 永平
Kazuyoshi Takahashi
一義 高橋
Kunio Yoshihara
吉原 邦男
Toshiaki Matsui
松井 俊明
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP8019483A priority Critical patent/JPS59204772A/en
Publication of JPS59204772A publication Critical patent/JPS59204772A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To set the condition of forming the optimum image by arranging a first electrode with the length almost the same as the width of an object to be measured in parallel near the body being measured to measure the potential with respect to a second electrode connected electrically to the first electrode. CONSTITUTION:A linear electrode 8 is arranged entirely on the length of a photosensitive body 6, namely, on almost the entire width of a manuscript. An electrode 9 is arranged immediate before a vibrator 2 on the side of the photosensitive body 6 while a measuring electrode 10 opposite to the electrode 9 sandwitching flat plate sections 2a and 2a of the vibrator. Fine parts composing the linear electrode 8 is given a potential directivity characteristic having such a gaus distribution as to maximize the surface potential detected at position where it is in front of the fine part in the surface of the photosensitive body 6 with respect to angle or distance and a only a potential thereof is measured facing the fine part of the photosensitive body. The entire electrode 8 provides the sum or the integration of the measured potentials at fine parts. Connecting the linear electrode 8 and the electrode 9, the electrode 9 is given a potential measured with the linear electrode 8.

Description

【発明の詳細な説明】 技術分野 本発明は表面電位計に係り、さらに詳しくは複写機等の
感光体表面等の被測定体の電位を測定する表面電位計に
関するものである。
DETAILED DESCRIPTION OF THE INVENTION TECHNICAL FIELD The present invention relates to a surface electrometer, and more particularly to a surface electrometer for measuring the potential of an object to be measured, such as the surface of a photoreceptor in a copying machine or the like.

従来技術 一般に電子複写機な、どに使用される光導電物質を使用
した感光体は、経時変化等による感度シフトが生じ易い
。そこでこの感度シフトを補償するために感光体表面電
位を制御する手段を付加して表面電位を常時一定範囲内
に設定しておく方法が知られている。
2. Description of the Related Art Generally, photoreceptors using photoconductive materials, such as those used in electronic copying machines, are susceptible to sensitivity shifts due to changes over time. Therefore, in order to compensate for this sensitivity shift, a method is known in which a means for controlling the surface potential of the photoreceptor is added so that the surface potential is always set within a certain range.

このためには感光体表面の電位を測定する表面電位計が
用いられている。
For this purpose, a surface electrometer is used to measure the potential on the surface of the photoreceptor.

表面電位計としては、被測定体とそれに対向して配置さ
れた電位測定電極との間に生じる電界を断続的に遮蔽す
ることにより、被測定体表面と測定電極の差電圧に比例
した振幅を持つ交流信号を測定電極に誘起させ、これに
より表面電位を知る構造のものが提案されている。
As a surface electrometer, by intermittently shielding the electric field generated between the object to be measured and the potential measurement electrode placed opposite it, it is possible to generate an amplitude proportional to the voltage difference between the surface of the object to be measured and the measurement electrode. A structure has been proposed in which the surface potential is determined by inducing an alternating current signal in the measuring electrode.

このような表面電位計は、電位測定電極回路及び測定電
極と被測定体との間を断続的に遮蔽するチョップ手段か
ら構成されており、両者は外部電界、ノイズを防止する
ため金属製のシールドによって覆われている。
Such a surface electrometer consists of a potential measuring electrode circuit and a chopping means that intermittently shields between the measuring electrode and the object to be measured, and both are covered with a metal shield to prevent external electric fields and noise. covered by.

この金属製のシールドには、感光体の被測定部に対して
対向して配置された電位測定用のff1ll定窓が形成
されており、この測定窓を通して感光体の電位が測定さ
れる。
This metal shield is formed with an ff1ll constant window for potential measurement, which is placed opposite to the portion to be measured of the photoreceptor, and the potential of the photoreceptor is measured through this measurement window.

チョップ手段としては直流モータを使用するものも提案
されているが、小型で、簡単に作成できるという面から
圧電素子を使用したものが提案されている。
Although it has been proposed to use a DC motor as the chopping means, it has been proposed to use a piezoelectric element because it is small and easy to manufacture.

このようなチョップ手段は第1図及び第2図に示すよう
に構成されている。
Such chopping means is constructed as shown in FIGS. 1 and 2.

各図において、符号′1で示すものは取付基板で、この
基板1の側面には音叉の形状をした振動子2が固定され
ている。振動子2は音叉の形状をしており、U字状に形
成された自由端側には平板部2aが形成されており、こ
の平板部2aが図示していない測定電極の被測定体と対
向する端面の手前側に平行に配置される。この振動子2
のU字状の折曲部の上下面には圧電素子3,3が固定さ
れている。振動子2のU字状の折曲部の端部にはピン3
aが取付基板1側に向って突設されており、このピン3
aは取付基板l内に埋め込まれ、下方に“向って屈曲し
、取付基板1の下端から露出され、図示していないプリ
ント基板側に接続される。このピン3aはアースをとる
ためのものである。
In each figure, the reference numeral '1 indicates a mounting board, and a tuning fork-shaped vibrator 2 is fixed to the side surface of this board 1. The vibrator 2 has a tuning fork shape, and a flat plate part 2a is formed on the free end side of the U-shape, and this flat plate part 2a faces the object to be measured of a measurement electrode (not shown). It is placed parallel to the front side of the end face. This vibrator 2
Piezoelectric elements 3, 3 are fixed to the upper and lower surfaces of the U-shaped bent portion. A pin 3 is attached to the end of the U-shaped bent part of the vibrator 2.
a protrudes toward the mounting board 1 side, and this pin 3
A is embedded in the mounting board 1, bent downward, exposed from the bottom end of the mounting board 1, and connected to the printed circuit board (not shown).This pin 3a is for grounding. be.

ま・た、取付基板1側にはリードピン4.5が設けられ
ており、それぞれは前記圧電素子3,3に接続されてい
る。これらリードピン4,5は圧電素子3を駆動するた
めの信号を導くもので、ピン3aと同様に図示していな
いプリント基板側に接続される。
Additionally, lead pins 4.5 are provided on the mounting board 1 side, and each is connected to the piezoelectric elements 3, 3. These lead pins 4 and 5 guide signals for driving the piezoelectric element 3, and are connected to a printed circuit board (not shown) similarly to the pin 3a.

このような構造を有するチョップ手段は、圧電素子3.
3に第1図において上下方向に電圧を印加すると、圧電
素子3,3は面方向の歪みを生じ、この歪みにより振動
子5の二叉状の各辺は第1図において上下方向の振動を
生じる。
The chopping means having such a structure includes a piezoelectric element 3.
3, when a voltage is applied in the vertical direction in FIG. 1, the piezoelectric elements 3, 3 produce distortion in the plane direction, and due to this distortion, each side of the bifurcated vibrator 5 vibrates in the vertical direction in FIG. arise.

このような振動が生じると、図示していない測定電極に
加わる電界の総面積が変動し、振動子2の振動周波数と
同じ周波数で被測定体と測定電極との間に電位差に比例
した振幅を持つ交流信号が測定電極側に誘起される。
When such vibration occurs, the total area of the electric field applied to the measurement electrode (not shown) changes, and an amplitude proportional to the potential difference between the object to be measured and the measurement electrode is generated at the same frequency as the vibration frequency of the vibrator 2. An alternating current signal with this voltage is induced on the measurement electrode side.

ところで、第3図は被測定体である複写機の感光体と表
面電位計との配置関係を説明するもので、符号6は感光
体を示し、符号7は表面電位計を示す。
By the way, FIG. 3 explains the arrangement relationship between a photoreceptor of a copying machine, which is an object to be measured, and a surface electrometer. Reference numeral 6 indicates the photoreceptor, and reference numeral 7 indicates a surface electrometer.

表面電位計7は測定電極及び測定窓が正確に位置決めさ
れて感光体6に対して配置され、感光体6の特定の部分
に対向するように配置されている。
The surface electrometer 7 is placed with respect to the photoreceptor 6 with its measurement electrode and measurement window accurately positioned, and is placed so as to face a specific portion of the photoreceptor 6.

この結果、第3図からも明らかなように表面電位計7は
感光体6の測定すべき部分のごく一部の表面電位を測定
しているにすぎない結果となった。
As a result, as is clear from FIG. 3, the surface potential meter 7 only measured the surface potential of a small portion of the photoreceptor 6 to be measured.

このため、原稿全体を一度走査して感光体6上に潜像を
形成させ、この潜像の表面電位を測定して最適な画像形
成条件を決定するに際し、原稿走査方向、すなわち、感
光体6の軸線方向にコントラストが大きな原稿や写真な
どの特殊な被複写物に対しては必ずしも最適な画像形成
条件の決定を行なっているとは限らなかった。
Therefore, when scanning the entire document once to form a latent image on the photoreceptor 6, and determining the optimal image forming conditions by measuring the surface potential of this latent image, it is necessary to Optimum image forming conditions have not always been determined for special objects to be copied, such as originals or photographs, which have a large contrast in the axial direction.

目   的 本発明は以上のような従来の欠点を除去するために成さ
れたもので、原稿が幅方向に対して大きなコントラスト
を持つ場合にも有効な画像形成条件を決定することがで
きるように構成した表面電位計を提供することを目的と
している。
Purpose The present invention has been made in order to eliminate the above-mentioned drawbacks of the conventional art, and to make it possible to determine effective image forming conditions even when a document has a large contrast in the width direction. The object of the present invention is to provide a surface electrometer configured according to the present invention.

実施例 第4図(a)、(b)は本発明の一実施例を説明するも
ので、図中第1図〜第3図と同一部分には同一符号を付
し、その説明は省略する。
Embodiment FIGS. 4(a) and 4(b) illustrate an embodiment of the present invention. In the figures, the same parts as in FIGS. 1 to 3 are denoted by the same reference numerals, and the explanation thereof will be omitted. .

図において、符号8で示すものは直線状電極で、感光体
6の長手方向、すなわち、原稿の幅方向のほぼ全長にわ
たって配置されている。
In the figure, the reference numeral 8 indicates a linear electrode, which is arranged over almost the entire length of the photoreceptor 6 in the longitudinal direction, that is, in the width direction of the document.

一方、振動子2の感光体6側の直前には、電極9が配置
されており、振動子2の平板部2a、2aを挟んで電極
9と反対側には測定電極10が配置されている。測定電
極10には増幅回路11が接続されている。
On the other hand, an electrode 9 is disposed immediately in front of the photoreceptor 6 side of the vibrator 2, and a measurement electrode 10 is disposed on the opposite side of the electrode 9 across the flat plate portions 2a, 2a of the vibrator 2. . An amplifier circuit 11 is connected to the measurement electrode 10.

以上のような構造のもとに直線状電極8によって感光体
6の表面全体の表面電位を検出する。
Based on the structure described above, the surface potential of the entire surface of the photoreceptor 6 is detected by the linear electrode 8.

直線状電極8を構成する微小部分は感光体6の表面の微
小部分と角度あるいは距離に対して正面となる位置にお
いて検出した表面電位が最大値となるような強いガウス
分布を有する電位指向特性を与えられている。
The minute portion constituting the linear electrode 8 has a potential directivity characteristic having a strong Gaussian distribution such that the detected surface potential has a maximum value at a position facing the minute portion on the surface of the photoreceptor 6 with respect to the angle or distance. It is given.

従って、直線状型fl!8の微小部分はこれに対向する
感光体の微小部分の電位のみを測定していることになる
Therefore, the linear type fl! The minute portion 8 measures only the potential of the minute portion of the photoreceptor that faces it.

直線状電極8はこのような微小部分の集合体と考えられ
るため、直線状電極8全体では各微小部分での測定電位
の総和あるいは積分量である電位が得られる。
Since the linear electrode 8 is considered to be a collection of such minute portions, the potential of the linear electrode 8 as a whole is the sum or integral of the potentials measured at each minute portion.

この直線状電極8とチョップ手段である振動子2の手前
側に位置する電極9とを接続しておけば、直線状電極8
によって測定した電位が電極9に与えられる。
If this linear electrode 8 is connected to an electrode 9 located on the front side of the vibrator 2, which is a chopping means, the linear electrode 8
A potential measured by is applied to the electrode 9.

測定電極lOはアースされているため、Ovであり、振
動子2も前述したようにアースされているため、Ovで
ある。
The measurement electrode IO is grounded, so it is Ov, and the vibrator 2 is also grounded, as described above, so it is Ov.

この結果、直線状電極8及び電極9は感光体6の表面電
位に応じた電位となる。
As a result, the linear electrode 8 and the electrode 9 have a potential corresponding to the surface potential of the photoreceptor 6.

この結果、電極9と測定電極10との間に電界が発生し
、この電界を振動子2がチョップするため、測定電位1
0に加わる電界の総面積が変動し、振動子2の振動周波
数と同じ周波数で電極9と測定電極10との間の電位差
に比例した振幅をもつ交流信号が測定電極10に誘起さ
れる。
As a result, an electric field is generated between the electrode 9 and the measurement electrode 10, and the vibrator 2 chops this electric field, so that the measurement potential 1
The total area of the electric field applied to the oscillator 2 changes, and an alternating current signal having the same frequency as the vibration frequency of the vibrator 2 and an amplitude proportional to the potential difference between the electrode 9 and the measurement electrode 10 is induced in the measurement electrode 10.

電極9は直線状電極8と同電位であり、しかも直線状電
極8は被測定体である感光体の表面電位に比例した電位
であるため、測定電極lOに誘起された交流信号の振幅
は被測定体の表面電位に比例していることになる。
Since the electrode 9 has the same potential as the linear electrode 8, and the linear electrode 8 has a potential proportional to the surface potential of the photoreceptor, which is the object to be measured, the amplitude of the AC signal induced in the measurement electrode 10 is It is proportional to the surface potential of the measuring object.

この結果、特殊なコントラストを有する表面電位を被測
定体の全面にわたって測定することができ、あらゆる種
類の被複写物の潜像の表面電位を測定でき、最適な画像
形成条件を設定できる。
As a result, the surface potential having a special contrast can be measured over the entire surface of the object to be measured, the surface potential of latent images of all kinds of objects to be copied can be measured, and the optimum image forming conditions can be set.

効  果 以上の説明から明らかなように、本発明によれば、被測
定体の近傍に被測定体の幅と同程度の長さを持つ第1の
電極λ平行に配置し、この第1の電極と電気的に接続さ
れた第2の電極に対して電位の測定を行なう構造を採用
しているため、測定方向に大きなコントラストを有する
特殊な被複写物を含めてあらゆる種類の被複写物の潜像
の表面電位を測定でき、最適な画像形成条件を設定する
ことができる。
Effects As is clear from the above explanation, according to the present invention, a first electrode λ having a length comparable to the width of the measured object is arranged near the measured object, and the first electrode λ is arranged in parallel with the measured object. Since it uses a structure in which the potential is measured with respect to a second electrode that is electrically connected to the electrode, it can be used for all kinds of copies, including special copies that have a large contrast in the measurement direction. The surface potential of the latent image can be measured, and the optimal image forming conditions can be set.

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

第1図及び第2図は本発明に適用されるチョップ手段の
正面図及び平面図、第3図(A)。 (B)は従来構造の表面電位の被測定体との間の配置関
係を説明する側面図及び正面図、第4図(A)、(B)
は本発明の一実施例を説明する側面図及び正面図である
1 and 2 are a front view and a plan view of a chopping means applied to the present invention, and FIG. 3(A). (B) is a side view and a front view illustrating the arrangement relationship between the surface potential of the conventional structure and the measured object, and FIGS. 4 (A) and (B)
1 is a side view and a front view illustrating an embodiment of the present invention. FIG.

Claims (1)

【特許請求の範囲】[Claims] 被測定体の電位を測定する表面電位計において、前記被
測定体近傍に前記被測定体の幅と同程度の長さを有する
第1の電極を平行に配置し、前記第1の電極と電気的に
接続された第2の電極に対して電位を測定することを特
徴とする表面電位計。
In a surface electrometer that measures the potential of a measured object, a first electrode having a length comparable to the width of the measured object is arranged in parallel near the measured object, and the first electrode and the electrical potential are arranged in parallel. 1. A surface electrometer, characterized in that the potential is measured with respect to a second electrode connected to the surface.
JP8019483A 1983-05-10 1983-05-10 Surface potential meter Pending JPS59204772A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8019483A JPS59204772A (en) 1983-05-10 1983-05-10 Surface potential meter

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8019483A JPS59204772A (en) 1983-05-10 1983-05-10 Surface potential meter

Publications (1)

Publication Number Publication Date
JPS59204772A true JPS59204772A (en) 1984-11-20

Family

ID=13711570

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8019483A Pending JPS59204772A (en) 1983-05-10 1983-05-10 Surface potential meter

Country Status (1)

Country Link
JP (1) JPS59204772A (en)

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