JPH0452467B2 - - Google Patents

Info

Publication number
JPH0452467B2
JPH0452467B2 JP58074911A JP7491183A JPH0452467B2 JP H0452467 B2 JPH0452467 B2 JP H0452467B2 JP 58074911 A JP58074911 A JP 58074911A JP 7491183 A JP7491183 A JP 7491183A JP H0452467 B2 JPH0452467 B2 JP H0452467B2
Authority
JP
Japan
Prior art keywords
photoreceptor
potential
current
constant
grid
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.)
Expired - Lifetime
Application number
JP58074911A
Other languages
Japanese (ja)
Other versions
JPS59201075A (en
Inventor
Koichi Noguchi
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.)
Ricoh Co Ltd
Original Assignee
Ricoh 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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP58074911A priority Critical patent/JPS59201075A/en
Publication of JPS59201075A publication Critical patent/JPS59201075A/en
Publication of JPH0452467B2 publication Critical patent/JPH0452467B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G15/00Apparatus for electrographic processes using a charge pattern
    • G03G15/02Apparatus for electrographic processes using a charge pattern for laying down a uniform charge, e.g. for sensitising; Corona discharge devices
    • G03G15/0266Arrangements for controlling the amount of charge

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  • Physics & Mathematics (AREA)
  • Engineering & Computer Science (AREA)
  • Plasma & Fusion (AREA)
  • General Physics & Mathematics (AREA)
  • Control Or Security For Electrophotography (AREA)

Description

【発明の詳細な説明】 (技術分野) 本発明は複写機の感光体の帯電電位の制御装置
に関するものである。
DETAILED DESCRIPTION OF THE INVENTION (Technical Field) The present invention relates to a control device for the charging potential of a photoreceptor in a copying machine.

(従来技術) 従来、この種帯電電位の制御装置としては以下
のものが公知となつている。
(Prior Art) Conventionally, the following devices are known as this type of charging potential control device.

1つは定電流コロナ放電装置であるがこれは感
光体のバラツキ、温度特性などにより電位が一定
にならないという欠点がある。
One is a constant current corona discharge device, but this has the disadvantage that the potential is not constant due to variations in the photoreceptor, temperature characteristics, etc.

またスコロトロンチヤージヤー装置は帯電に十
分時間をかけてグリツド電位により決まる電圧ま
で帯電すれば帯電電位は一定となるが時間がかか
り過ぎるので複写機としては、実用的でないとい
う欠点がある。尚この装置は普通は上述の様な使
い方をせず帯電ムラの防止として使うので電位の
制御としては不十分である。
In addition, the scorotron charger device has the disadvantage that it is not practical as a copying machine because it takes too much time, although the charging potential becomes constant if it takes a sufficient amount of time to charge to a voltage determined by the grid potential. Note that this device is usually not used as described above, but is used to prevent uneven charging, so it is insufficient for controlling potential.

さらに電位計を用い、この電位計の出力で高圧
電源、露光、現像バイアス制御などを行ない、電
位が変わつても複写画像の品質が一定になるよう
に制御する方式も公知である。しかしながらこの
方式では電位計が高価なこと、バイアス電圧、誘
起電圧により電位計が汚れ易いこと、高入力イン
ピーダンス回路なので電気的ノイズや雰囲気の影
響を受け易いこと等の欠点がある。また方式によ
つてはチヨツパーなどの機械的な振動部分があ
り、寿命、信頼性に欠けるという欠点もある。
Furthermore, a method is also known in which an electrometer is used and the output of the electrometer is used to control the high-voltage power supply, exposure, development bias, etc., so that the quality of the copied image remains constant even if the potential changes. However, this method has drawbacks such as the electrometer is expensive, the electrometer is easily contaminated by bias voltage and induced voltage, and the high input impedance circuit is easily affected by electrical noise and atmosphere. Additionally, some systems have mechanical vibrating parts such as choppers, which have the disadvantage of shortening lifespan and reliability.

(目的) 本発明は以上の様な従来例の欠点に鑑みてなさ
れたものであり、電位計のように特別の装置を用
いることなく、感光体のバラツキの影響を受ける
ことのない帯電電位制御装置を提供することを目
的とするものである。
(Purpose) The present invention has been made in view of the above-mentioned drawbacks of the conventional examples, and it is possible to control charging potential without using a special device such as an electrometer and without being affected by variations in photoreceptors. The purpose is to provide a device.

(構成) 以下、本発明の構成を図示の一実施例に基づき
説明する。
(Structure) Hereinafter, the structure of the present invention will be explained based on an illustrated embodiment.

第1図は一実施例に係る制御装置の機能図であ
る。チヤージヤー1はスコロトロンと呼ばれてい
るものと同じ構造をもち、コロノード2、シール
ド3、グリツド4より成る。この実施例ではグリ
ツド4は感光体の表面電位を検出する検出電極と
して作用する。コロノード2は高圧電源5の出力
に接続される。シールド3は接地される。チヤー
ジヤ1は感光体6に対向して置かれ、感光体6を
帯電させる。感光体6の背面電極は接地され、感
光体6を帯電するときに帯電させるための電流Ip
が流れる。感光体6は矢印の方向に回転し、チヤ
ージヤー1により順次全面が帯電される。検出電
極4は複数の導体のワイヤよりなり、相互に電気
的に接続されている。検出電極4は定電圧素子7
に接続され、定電圧素子7の他端は定電圧素子7
を流れる電流を検出するための電流検出抵抗8を
介して接地される。電流検出抵抗8に表われる電
圧を、定電圧素子7の電圧が数百から千ボルト程
度であるのに比較して、十分に低くなるようにす
る。このように抵抗値を選べば、直列抵抗を入れ
ることによる定電圧特性の悪化をさらけられる。
この電流検出抵抗8に発生する電圧は、定電圧素
子7を流れる電流に比例する。この検出された信
号は高圧電源5の比較回路9に入力される。コロ
ナ放電により流れる電流は交流成分を含むので、
実際に回路では信号の平均化処理をして直流に変
換後、比較回路9に入力している。比較回路9の
基準を与えるため、図で「電流設定」と書かれた
ブロツク10から基準電圧が比較回路9に入力さ
れる。「電流設定」からの基準と電流検出抵抗8
に発生する電圧の比較を行ない、差の信号を取り
出し、差の信号により高圧電源5の出力を制御す
る。図のパルス幅制御回路11とDC−DCコンバ
ータ12により、このような制御を行つている。
つまり、検出電極4に接続された定電圧素子7を
流れる電流を一定にするフイードバツク制御系が
構成される。
FIG. 1 is a functional diagram of a control device according to an embodiment. The charger 1 has the same structure as what is called a scorotron, and consists of a coronode 2, a shield 3, and a grid 4. In this embodiment, the grid 4 acts as a detection electrode for detecting the surface potential of the photoreceptor. The coronode 2 is connected to the output of the high voltage power supply 5. Shield 3 is grounded. The charger 1 is placed opposite the photoreceptor 6 and charges the photoreceptor 6. The back electrode of the photoconductor 6 is grounded, and when charging the photoconductor 6, a current I p is applied to charge the photoconductor 6.
flows. The photoreceptor 6 rotates in the direction of the arrow, and the entire surface is sequentially charged by the charger 1. The detection electrode 4 is made up of a plurality of conductor wires, which are electrically connected to each other. The detection electrode 4 is a constant voltage element 7
The other end of the constant voltage element 7 is connected to the constant voltage element 7.
It is grounded via a current detection resistor 8 for detecting the current flowing through it. The voltage appearing on the current detection resistor 8 is made to be sufficiently low compared to the voltage of the constant voltage element 7, which is approximately several hundred to one thousand volts. By selecting the resistance value in this way, it is possible to avoid deterioration of constant voltage characteristics caused by inserting a series resistor.
The voltage generated across this current detection resistor 8 is proportional to the current flowing through the constant voltage element 7. This detected signal is input to the comparison circuit 9 of the high voltage power supply 5. The current flowing due to corona discharge contains an alternating current component, so
In actuality, the circuit averages the signal and converts it to direct current, which is then input to the comparator circuit 9. In order to provide a reference for the comparator circuit 9, a reference voltage is input to the comparator circuit 9 from a block 10 labeled "Current Setting" in the figure. Reference from “Current setting” and current detection resistor 8
The voltages generated are compared, a difference signal is extracted, and the output of the high voltage power supply 5 is controlled by the difference signal. Such control is performed by the pulse width control circuit 11 and DC-DC converter 12 shown in the figure.
In other words, a feedback control system is configured to keep the current flowing through the constant voltage element 7 connected to the detection electrode 4 constant.

次に、定電圧素子7を流れる電流を一定にする
ことと、感光体6の帯電電位を一定にすることと
の関係を説明する。説明のための基準として、ま
ず第4図により公知のスコロトロンチヤージヤー
の機能について説明する。尚、符号中13はグリ
ツドバイヤス電源である。スコロトロンチヤージ
ヤーはグリツド4に一定の電位を与えながら高圧
電源5によるコロノード2のコロナ放電によつて
感光体6に電荷を与えるものである。グリツド4
に与えられた電圧によりグリツド4に沿つて等電
位面が形成される。コロノード2でコロナ放電が
起ると、コロノード2近傍でイオンが生成する。
生成したイオンはコロノード2とシールド3、コ
ロノード2と感光体6、コロノード2とグリツド
4間に形成される電界により加速され、それぞれ
に向かつて移動し、これによつて電流が流れ感光
体6の帯電が行なわれる。しかし感光体6の電位
の上昇により、感光体6グリツド4間の電界が弱
くなつてくる。弱くなるとグリツド4、感光体6
間でイオンを加速する度合が低下するので、感光
体6へ到達するイオンが減少し、感光体6の荷電
電流が減少する。減少した電流がグリツド4に流
れる。荷電電流が流れる間は感光体6の電位は上
昇する(ここでは簡単化のため感光体6のリーク
による電位の低下は無視できるものとする)。電
位の上昇により感光体6の電位とグリツド4の電
位が等しくなると、グリツド4、感光体6間では
イオンは加速されなくなる。このときでもイオン
がグリツド4により形成された等電圧面に達する
ときの初速度により一部のイオンは感光体6に到
達する。さらに感光体6の電圧が上るとグリツド
4感光体6間の電界は逆極性になり、コロノード
2、グリツド4間で加速されたイオンを逆方向に
加速するようになり、感光体6へは電荷が到達で
きなくなる。電荷の増加がなくなれば感光体6の
電圧は一定になる。これがスコロトロンチヤージ
ヤーによる感光体6の帯電電位の制御である。し
かし、グリツド4に与えた電位により帯電を制御
するには帯電に時間がかかりすぎて感光体6を移
動させながら帯電する静電複写機ではあまり実用
的でない。普通、静電複写機においてスコロトロ
ンチヤージヤーが使われるのは、感光体6を均一
に帯電するという目的をもつている。これは上の
説明からも分るように、帯電のムラを生じたと
き、電位の低い部分はグリツド4、感光体6間の
電位差が大きいので大きな電流が流れ、電位の高
い部分の電流が抑制されるためムラを緩和する作
用があるためである。そして次に前述の定電圧素
子と感光体との関係を第3図に基づき説明する。
Next, the relationship between keeping the current flowing through the constant voltage element 7 constant and keeping the charging potential of the photoreceptor 6 constant will be explained. As a basis for explanation, the function of a known scorotron charger will first be explained with reference to FIG. Note that the reference numeral 13 is a grid bias power source. The scorotron charger applies electric charge to the photoreceptor 6 by corona discharge of the coronode 2 by the high-voltage power supply 5 while applying a constant potential to the grid 4. grid 4
An equipotential surface is formed along the grid 4 by the voltage applied to the grid. When corona discharge occurs in the coronode 2, ions are generated near the coronode 2.
The generated ions are accelerated by the electric fields formed between the coronode 2 and the shield 3, between the coronode 2 and the photoconductor 6, and between the coronode 2 and the grid 4, and move toward each direction.This causes a current to flow and move toward the photoconductor 6. Charging is performed. However, as the potential of the photoreceptor 6 increases, the electric field between the photoreceptors 6 and the grid 4 becomes weaker. When it becomes weak, grid 4 and photoconductor 6
Since the degree of acceleration of ions is reduced between the two, the number of ions reaching the photoreceptor 6 is reduced, and the charging current of the photoreceptor 6 is reduced. A reduced current flows through grid 4. While the charging current flows, the potential of the photoconductor 6 increases (here, for the sake of simplicity, it is assumed that the decrease in potential due to leakage of the photoconductor 6 can be ignored). When the potential of the photoconductor 6 becomes equal to the potential of the grid 4 due to an increase in potential, ions are no longer accelerated between the grid 4 and the photoconductor 6. Even at this time, some of the ions reach the photoreceptor 6 due to the initial velocity when the ions reach the equal voltage surface formed by the grid 4. When the voltage of the photoreceptor 6 further increases, the electric field between the grid 4 and the photoreceptor 6 becomes of opposite polarity, and the ions accelerated between the coronode 2 and the grid 4 are accelerated in the opposite direction, and the charge on the photoreceptor 6 is becomes unreachable. When the charge no longer increases, the voltage of the photoreceptor 6 becomes constant. This is the control of the charging potential of the photoreceptor 6 by the scorotron charger. However, controlling the charging by the potential applied to the grid 4 takes too much time and is not very practical in an electrostatic copying machine in which the photoreceptor 6 is charged while being moved. Generally, a scorotron charger is used in an electrostatic copying machine for the purpose of uniformly charging the photoreceptor 6. As can be seen from the above explanation, when uneven charging occurs, a large current flows in areas with low potential due to the large potential difference between the grid 4 and photoreceptor 6, and the current in areas with high potential is suppressed. This is because it has the effect of alleviating unevenness. Next, the relationship between the above-mentioned constant voltage element and the photoreceptor will be explained based on FIG. 3.

第3図は第1図における特性グラフ、即ち、グ
リツド4に定電圧素子(1.0kV)をつけ、感光体
6のかわりに、外部からバイアスを与えたプレー
トをおいて、プレート電流Ipと定電圧素子7を流
れる電流Ivを測定したものを示す。図からわかる
ようにプレート電圧Vpの低いときはIpは多く流
れ、Vpの上昇とともにIpは減少している。逆にIv
はVpの上昇とともに上昇する。これはチヤージ
ヤー1の構造と感光体6との位置関係、及び定電
圧素子7の特性が一定ならば、Ivは感光体6の電
位により決定されることを示す。したがつて第1
図で示す構成によりIvを一定にするということは
感光体6の帯電電位を検出し、それを一定に制御
するのと同じ働きをすることになるのである。
Figure 3 shows the characteristic graph in Figure 1, that is, a constant voltage element (1.0 kV) is attached to the grid 4, a plate to which an external bias is applied is placed in place of the photoreceptor 6, and the plate current I p is determined. A measurement of the current I v flowing through the voltage element 7 is shown. As can be seen from the figure, a large amount of I p flows when the plate voltage V p is low, and I p decreases as V p rises. On the contrary, I v
increases as V p increases. This shows that I v is determined by the potential of the photoreceptor 6 if the structure of the charger 1 and the positional relationship with the photoreceptor 6 and the characteristics of the constant voltage element 7 are constant. Therefore, the first
Keeping Iv constant with the configuration shown in the figure has the same effect as detecting the charged potential of the photoreceptor 6 and controlling it to be constant.

次にグリツド4に定電圧素子7を使うことの意
味をいままでの説明の補足の意味で説明する。第
2図は定電圧素子のV,I特性を示す特性のaで
示す領域は電流が小さくて、定電圧特性を示して
いない。一般に高い抵抗値の抵抗体として近似で
きる。bは電流が流れ定電圧特性を示す領域であ
る。ここでは直線で近似する場合その直線の示す
抵抗値は低い。これを定電圧素子7の動作抵抗と
いう。この抵抗が低いということは、電流が変化
してもほぼ一定の電圧がかかつていることにな
る。これにより感光体6の電位の上昇に対する電
流の増加の感度が非常に高くなる。検出部の感度
が高いのは制御系の設計においても非常に有利で
あり、簡単な回路で、安定な制御系を構成でき
る。動作抵抗が高いと感光体6の電位の上昇によ
り、Ivが増加しても、これにより、定電圧素子7
の電圧も増加し、感光体6の電位上昇による変化
分を打ち消してしまうので感度が低下する。従つ
て動作抵抗は低くするのが望ましい。
Next, the meaning of using the constant voltage element 7 in the grid 4 will be explained as a supplement to the previous explanation. In FIG. 2, the region indicated by a of the characteristics showing the V, I characteristics of a constant voltage element has a small current and does not show constant voltage characteristics. In general, it can be approximated as a resistor with a high resistance value. b is a region where current flows and exhibits constant voltage characteristics. Here, when approximated by a straight line, the resistance value indicated by that straight line is low. This is called the operating resistance of the constant voltage element 7. The fact that this resistance is low means that a nearly constant voltage is applied even if the current changes. This makes the sensitivity of the current increase to a rise in the potential of the photoreceptor 6 extremely high. The high sensitivity of the detection section is also very advantageous in the design of a control system, and a stable control system can be constructed with a simple circuit. If the operating resistance is high, even if I v increases due to an increase in the potential of the photoreceptor 6, this will cause the constant voltage element 7 to
The voltage also increases, canceling out the change due to the increase in the potential of the photoreceptor 6, resulting in a decrease in sensitivity. Therefore, it is desirable to lower the operating resistance.

(効果) 以上本発明によれば電位計のように特別の装置
を使わないので実装上の制限がなく、チヤージヤ
ーの実装範囲内で電位を検知し制御することが出
来るし、検知部が単なる導体であるから、コスト
も安く、汚れなどの影響も受けにくい。
(Effects) As described above, according to the present invention, since no special device such as an electrometer is used, there are no restrictions on implementation, the potential can be detected and controlled within the mounting range of the charger, and the detection part is a simple conductor. Therefore, the cost is low and it is not easily affected by dirt.

また高インピーダンス回路ではないので電気的
ノイズ、雰囲気の影響の少ない装置とすることが
可能である。
Furthermore, since it is not a high impedance circuit, it is possible to create a device that is less affected by electrical noise and atmosphere.

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

第1図は本発明の一実施例に係る装置の機能説
明図、第2図は定電圧素子のV,I特性図、第3
図は本発明の一実施例に係るプレート電流と検出
電流の関係を示す特性図、第4図は本発明の前提
となるスコロトロンチヤージヤーを示す簡略図で
ある。 1……チヤージヤー、2……コロノード、4…
…検出電極、5……高圧電源、6……感光体、7
……定電圧素子、9……比較回路、11……パル
ス幅制御回路、12……DC−DCコンバータ。
FIG. 1 is a functional explanatory diagram of a device according to an embodiment of the present invention, FIG. 2 is a V, I characteristic diagram of a constant voltage element, and FIG.
The figure is a characteristic diagram showing the relationship between the plate current and the detected current according to an embodiment of the present invention, and FIG. 4 is a simplified diagram showing the scorotron charge which is the premise of the present invention. 1...Chargeer, 2...Coronode, 4...
...Detection electrode, 5...High voltage power supply, 6...Photoreceptor, 7
... Constant voltage element, 9 ... Comparison circuit, 11 ... Pulse width control circuit, 12 ... DC-DC converter.

Claims (1)

【特許請求の範囲】 1 感光体と対向しているチヤージヤと、 そのチヤージヤのコロノードと感光体との間に
設けられた検出電極と、 その検出電極とアースとの間に設置された定電
圧素子と、 その定電圧素子に流れる電流を検出する手段
と、 その電流の検知結果に基づいて、帯電用の高圧
電源の出力を制御し、前記定電圧素子に流れる電
流を一定に維持する手段とを備えたことを特徴と
する感光体の帯電電位制御装置。
[Scope of Claims] 1. A charger facing the photoreceptor, a detection electrode provided between the coronode of the charger and the photoreceptor, and a constant voltage element provided between the detection electrode and ground. a means for detecting a current flowing through the constant voltage element; and a means for controlling the output of a high voltage power supply for charging based on the detection result of the current to maintain a constant current flowing through the constant voltage element. A charging potential control device for a photoreceptor, characterized by comprising:
JP58074911A 1983-04-30 1983-04-30 Charged potential control device of photosensitive body Granted JPS59201075A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP58074911A JPS59201075A (en) 1983-04-30 1983-04-30 Charged potential control device of photosensitive body

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP58074911A JPS59201075A (en) 1983-04-30 1983-04-30 Charged potential control device of photosensitive body

Publications (2)

Publication Number Publication Date
JPS59201075A JPS59201075A (en) 1984-11-14
JPH0452467B2 true JPH0452467B2 (en) 1992-08-21

Family

ID=13561037

Family Applications (1)

Application Number Title Priority Date Filing Date
JP58074911A Granted JPS59201075A (en) 1983-04-30 1983-04-30 Charged potential control device of photosensitive body

Country Status (1)

Country Link
JP (1) JPS59201075A (en)

Families Citing this family (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62158456U (en) * 1986-03-31 1987-10-08
JPS63293564A (en) * 1987-05-26 1988-11-30 Sharp Corp Electrostatic charging device
JPH03170957A (en) * 1989-11-29 1991-07-24 Mita Ind Co Ltd Image forming operation controller for electronic image forming device
JP2714716B2 (en) * 1990-11-21 1998-02-16 富士写真フイルム株式会社 Silver halide photographic material
DE69321755T2 (en) * 1992-04-28 1999-04-22 Canon K.K., Tokio/Tokyo Imaging device with a charging element
JPH0635302A (en) * 1992-07-16 1994-02-10 Canon Inc Image forming device

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