JPS6250857A - Electrostatic charging device - Google Patents
Electrostatic charging deviceInfo
- Publication number
- JPS6250857A JPS6250857A JP18986085A JP18986085A JPS6250857A JP S6250857 A JPS6250857 A JP S6250857A JP 18986085 A JP18986085 A JP 18986085A JP 18986085 A JP18986085 A JP 18986085A JP S6250857 A JPS6250857 A JP S6250857A
- Authority
- JP
- Japan
- Prior art keywords
- voltage
- electrode
- discharge
- discharge electrode
- charging device
- 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
Abstract
Description
【発明の詳細な説明】
1亙上1
本発明は静電記録、電子写真装置などに使用可能な帯電
装置に関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a charging device that can be used in electrostatic recording, electrophotographic devices, and the like.
11藍遺
従来より、静電記録、電子写真装置においては、線径0
.1mm程度のワイヤーに高電圧を印加することにより
コロナ放電を行うコロナ帯電装置が広く用いられている
。しかしながら、このようなコロナ帯電装置では、ワイ
ヤーが細いため破損し易く、さらにはワイヤーの汚れに
より放電ムラが生じるため被帯電体への帯電が不均一と
なるという欠点があった。11 Ai Traditionally, in electrostatic recording and electrophotographic equipment, wire diameter 0
.. Corona charging devices that perform corona discharge by applying a high voltage to a wire of about 1 mm are widely used. However, such a corona charging device has the disadvantage that the wire is thin and easily damaged, and furthermore, dirt on the wire causes uneven discharge, resulting in non-uniform charging of the charged object.
また、ワイヤーとこれを包囲している導電性シールド部
材との距離をある程度以上に離す必要があり、コロナ帯
電装置の小型化にも限界があった。Furthermore, it is necessary to maintain a certain distance between the wire and the conductive shield member surrounding the wire, which limits the miniaturization of the corona charging device.
これに対して、他の帯電装置として誘電体を挾む電極間
に交流電圧を印加し、これにより一方の電極の端面との
誘電体との接合部分に正・負イオンを発生させ、外部電
界により所望の極性のイオンを抽出するもの(特開昭5
4−53537号公報、本件出願人による特願昭58−
187399号)がある。On the other hand, as another charging device, an alternating current voltage is applied between electrodes that sandwich a dielectric material, thereby generating positive and negative ions at the junction between the end face of one electrode and the dielectric material, and applying an external electric field. to extract ions of desired polarity (Unexamined Japanese Patent Publication No. 5
Publication No. 4-53537, patent application filed by the applicant in 1982
No. 187399).
第1図はこの形式の装置の基本構成を示し、放電部材1
は被帯電部材5に対して配置され、誘電体4、誘導電極
2、放電電極3を有している。誘導電極2と放電電極3
の間には交互電圧印加手段7により交互電圧が印加され
、一方、放電部材lに対して相対的に矢印Aの方向に移
動する被帯電部材5は導電体基体6上の絶縁体若しくは
光導電体であり、導電体基体6と放電電極3の間にはバ
イアス電圧印加手段7によりバイアス電圧が印加されて
いる。誘導電極2と放電電極3との間へ交互電圧を印加
することにより、放電電極3周辺から放電を起こさせ、
十分な正・負イオンを発生させたのち、放電電極3と導
電体基体6間に印加されているバイアス電圧による電界
で、上記圧又は負イオンを選択的に抽出して被帯電部材
5を帯電させるものである。FIG. 1 shows the basic configuration of this type of device, in which a discharge member 1
is arranged with respect to the charged member 5 and has a dielectric 4, an induction electrode 2, and a discharge electrode 3. Induction electrode 2 and discharge electrode 3
During this period, alternating voltages are applied by the alternating voltage applying means 7, while the charged member 5, which moves in the direction of arrow A relative to the discharge member 1, is an insulator or photoconductive member on a conductor base 6. A bias voltage is applied between the conductor base 6 and the discharge electrode 3 by a bias voltage applying means 7. By applying an alternating voltage between the induction electrode 2 and the discharge electrode 3, a discharge is caused from around the discharge electrode 3,
After generating sufficient positive and negative ions, the charged member 5 is charged by selectively extracting the above pressure or negative ions using an electric field caused by a bias voltage applied between the discharge electrode 3 and the conductive substrate 6. It is something that makes you
このような装置において1M電体4の厚みを薄くする(
例えば、厚みを500 pm以下、好ましくは20〜2
0 OILm位にする)ことによって、従来のコロナ帯
電装置に比して低い印加電圧(例えばピーク−ピーク値
で約1.5〜2.5KV )で安定した放電が得られる
。しかも、従来のコロナ帯電装置に比較して小型の帯電
装置とすることができる。In such a device, the thickness of the 1M electric body 4 is reduced (
For example, the thickness is 500 pm or less, preferably 20 to 2
0 OILm), stable discharge can be obtained with a lower applied voltage (for example, about 1.5 to 2.5 KV peak-to-peak) than in conventional corona charging devices. Furthermore, the charging device can be made smaller than the conventional corona charging device.
これは誘電体4の厚さを小さくすることにより、この誘
電体4を挾む2極間に印加する交互電圧が低くても2極
間の電界強度を高められるからである。このために、一
方の電極(放電電極)の縁の電界強度が放電するに十分
に高ければ、放電が可能となり、この電極が接する誘電
体4の表面に沿って沿面放電が生ずる。This is because by reducing the thickness of the dielectric 4, the electric field strength between the two electrodes can be increased even if the alternating voltage applied between the two electrodes sandwiching the dielectric 4 is low. For this reason, if the electric field strength at the edge of one electrode (discharge electrode) is high enough to cause a discharge, discharge is possible, and a creeping discharge occurs along the surface of the dielectric 4 in contact with this electrode.
この帯電装置では、従来のようなコロナ帯電装置のワイ
ヤに空気中の浮遊粒子が付着することによる。いわゆる
、ワイヤ汚れのような、放電電極の汚れは生じにくいの
で均一帯電に適するとされている。In this charging device, airborne particles adhere to the wire of a conventional corona charging device. It is said that it is suitable for uniform charging because it is difficult for the discharge electrode to become contaminated, such as so-called wire contamination.
しかしながら、この帯電装置は交互電圧電源とバイアス
電源の両方を必要とし、したがって装置が大きくなると
ともにコストが高く成るという欠点を有する。さらに、
この帯電装置で実際に帯電を行なうと、均一な帯電を得
るためには放電電極近傍の環境を無視できない、すなわ
ち、放電特性が周囲の環境(湿度、温度および気圧)、
とくに、湿度に依存して大きく変化し、比較的高い湿度
(例えば、相対湿度40%以上)の下では均一で安定し
た放電を得ることができない。However, this charging device has the disadvantage of requiring both an alternating voltage power supply and a bias power supply, thus increasing the size and cost of the device. moreover,
When actually charging with this charging device, in order to obtain uniform charging, the environment near the discharge electrode cannot be ignored.
In particular, it varies greatly depending on humidity, and uniform and stable discharge cannot be obtained under relatively high humidity (for example, relative humidity of 40% or more).
11立11
本発明は、したがって上記の形式の帯電装置であって、
小型で安価なものを提供することを第1の目的とする。11 The present invention therefore provides a charging device of the above type, comprising:
The primary objective is to provide something small and inexpensive.
本発明の他の目的は、環境の変化にもかかわらず、一定
な帯電可能な帯電装置を提供することである。Another object of the invention is to provide a charging device capable of constant charging despite changes in the environment.
11立且1
本発明によれば、誘電体と、該誘電体を挾んで延在する
誘導電極および放電電極と、該誘導電極と放電電極との
間に交互電圧を印加して放電電極・の近傍にイオンを発
生させる交互電圧と、放電電極と被帯電体との間に作用
し前記イオンを抽出して被帯電体を特定極性に帯電させ
る外部電界の両方を与えるトランス手段と、を有するこ
とを特徴とする帯電装置が提供されるので帯電装置全体
を小型廉価なものとすることができる。11 and 1 According to the present invention, a dielectric body, an induction electrode and a discharge electrode extending between the dielectric body, and a voltage applied alternately between the induction electrode and the discharge electrode to generate the discharge electrode. It has transformer means for applying both an alternating voltage that generates ions in the vicinity and an external electric field that acts between the discharge electrode and the charged object to extract the ions and charge the charged object to a specific polarity. Since a charging device characterized by the following is provided, the entire charging device can be made small and inexpensive.
実jL例 以下、本発明の実施例を図面に基づいて説明する。real jl example Embodiments of the present invention will be described below based on the drawings.
第2図は本発明による帯電装置の実施例を説明する概略
図である。放電部材lは第1図のものと同様に、誘電体
4、誘導電極2.放電電極3を有し、電子写真感光体な
どの被帯電部材5に対して配置されている。放電電極3
は線状で、誘導電極2誘導電極2の巾方向の中心線にほ
ぼ平行に配置されている。FIG. 2 is a schematic diagram illustrating an embodiment of the charging device according to the present invention. The discharge member l is the same as that in FIG. 1, and includes a dielectric material 4, an induction electrode 2. It has a discharge electrode 3 and is arranged with respect to a charged member 5 such as an electrophotographic photoreceptor. Discharge electrode 3
is linear, and is arranged substantially parallel to the center line in the width direction of the induction electrode 2.
ここで、誘電体4としては、セラミック、雲母、ガラス
等の比較的硬度の高い無機材料や、ポリイミド、四フッ
化エチレン、ポリエステル、アクリル、塩化ビニル、ポ
リエチレン等の柔軟性のある有機高分子材料等が用いら
れる。Here, as the dielectric material 4, relatively hard inorganic materials such as ceramic, mica, and glass, and flexible organic polymer materials such as polyimide, tetrafluoroethylene, polyester, acrylic, vinyl chloride, and polyethylene are used. etc. are used.
放電部材lに対して相対的に矢印Aの方向に移動する被
帯電部材5は導電体基体6上の絶縁体若しくは光導電体
である。The charged member 5, which moves in the direction of arrow A relative to the discharge member 1, is an insulator or photoconductor on a conductive substrate 6.
帯電方法としては、誘導電極2と放電電極3との間へ交
互電圧を印加することにより、放電電極3周辺から放電
を起こさせ、十分な正・負イオンを発生させ、放電電極
3と導電体基体6間に印加されているバイアス電圧によ
る電界で、上記圧又は負イオンを選択的に抽出して被帯
電部材5の絶縁体若しくは光導電体表面を特定極性に、
かつ所望の値に帯電させるものである。 ・誘導電
極2と放電電極3との間に印加する電圧波形としてはサ
イン波および矩形波、パルス状の波形などのいずれでも
よい。The charging method is to apply alternate voltages between the induction electrode 2 and the discharge electrode 3 to cause discharge from around the discharge electrode 3, generate enough positive and negative ions, and connect the discharge electrode 3 and the conductor. By selectively extracting the pressure or negative ions using an electric field caused by a bias voltage applied between the substrates 6, the insulator or photoconductor surface of the charged member 5 is made to have a specific polarity.
And it is charged to a desired value. - The voltage waveform applied between the induction electrode 2 and the discharge electrode 3 may be any of a sine wave, a rectangular wave, a pulsed waveform, etc.
本実施例においては、誘導電極2と放電電極3°の間へ
の交互電圧および導電体基体6と放電電極3の間へのバ
イアス電圧印加は電圧印加手段lOによって行なわれる
。In this embodiment, alternate voltage application between the induction electrode 2 and the discharge electrode 3° and bias voltage application between the conductor base 6 and the discharge electrode 3 are performed by voltage application means IO.
電圧印加手段10は昇圧用トランス12を有し、該トラ
ンスは入力側巻線13、誘導電極と放電電極との間に印
加される交互電圧を発生する第1の出力側巻線14およ
び放電電極3に印加されるバイアス電圧用の電力発生す
る第2の出力側巻線15を有する。第2の出力側巻線1
5は整流回路に接続され、該整流回路は、整流ダイオー
ド16、平糸化用コンデンサー17.抵抗18を有する
。抵抗18と並列にバリスタ21が接続され、これは直
流電位を一定に保持する。このようにして整流された後
の電圧が放電電極3に印加される。The voltage application means 10 has a step-up transformer 12, which includes an input winding 13, a first output winding 14 that generates an alternating voltage applied between an induction electrode and a discharge electrode, and a discharge electrode. The second output side winding 15 generates power for the bias voltage applied to the second output side winding 15. Second output winding 1
5 is connected to a rectifier circuit, which includes a rectifier diode 16, a flattening capacitor 17. It has a resistor 18. A varistor 21 is connected in parallel with the resistor 18, which keeps the DC potential constant. The voltage thus rectified is applied to the discharge electrode 3.
以上のごとく本実施例によれば単一のトランスによって
放電部材1が必要とする交互電圧および直流電圧が供給
されるので装置の小型化および低廉価が達成できる。As described above, according to this embodiment, since the alternating voltage and DC voltage required by the discharge member 1 are supplied by a single transformer, the device can be made smaller and less expensive.
本実施例においては、被帯電部材6と整流回路との間に
抵抗19が設けられ、さらにこれと並列に平滑化用コン
デンサー20が設けられている。In this embodiment, a resistor 19 is provided between the charged member 6 and the rectifier circuit, and a smoothing capacitor 20 is further provided in parallel with the resistor 19.
被帯電体5を流れた帯電電流はすべて抵抗19を通るの
で抵抗19の両端の電位を検出することによって帯電電
流を検知することができる。これによって検知された帯
電電流を示す信号は定電流制御回路21へ入力され、帯
電電流をあらかじめ設定された電流値と等しくするよう
な制御信号が交流発振回路22へ入力される。この定電
流制御回路からの信号によって一義的に決定される振幅
を有する交流信号が交流発振回路22から出力され、こ
れが電力増幅回路23を介して昇圧用トランスの入力側
巻線に入力される。Since all the charging current flowing through the charged object 5 passes through the resistor 19, the charging current can be detected by detecting the potential across the resistor 19. A signal indicating the detected charging current is input to the constant current control circuit 21, and a control signal for making the charging current equal to a preset current value is input to the AC oscillation circuit 22. An AC signal having an amplitude uniquely determined by the signal from the constant current control circuit is output from the AC oscillation circuit 22, and is input to the input winding of the step-up transformer via the power amplifier circuit 23.
第3図は各部の波形を示す。FIG. 3 shows the waveforms of each part.
25で示されるのは定電流制御回路21からの信号であ
り、前述のごとく抵抗19によって検知された帯電電流
にもとづいている。25 is a signal from the constant current control circuit 21, which is based on the charging current detected by the resistor 19 as described above.
波形26は第1の出力側巻線14から発生して放電部材
1に印加される交互電圧出力であり、定電流制御回路の
出力にしたがって電圧振幅が変調されている。The waveform 26 is an alternating voltage output generated from the first output winding 14 and applied to the discharge member 1, and the voltage amplitude is modulated according to the output of the constant current control circuit.
波形27は第2の出力側巻線の出力で、整流回路および
バリスタを通過した後の波形であり、図示のごとく一定
の電圧を得ることができる。The waveform 27 is the output of the second output winding, and is the waveform after passing through a rectifier circuit and a varistor, and as shown in the figure, a constant voltage can be obtained.
上記の定電流制御回路によって、温度、湿度などの環境
変化時においても安定でかつ一定の帯電量が得られる帯
電装置が提供される。しかも、何らかの原因によって外
部電界が変化した場合でも、この変化は電流検出部によ
って検出され、交互電圧の周波数を制御することによっ
て帯電電流を所定の値に保つことが可能である。The constant current control circuit described above provides a charging device that can provide a stable and constant amount of charge even when environmental changes such as temperature and humidity occur. Moreover, even if the external electric field changes for some reason, this change is detected by the current detection section, and by controlling the frequency of the alternating voltage, it is possible to maintain the charging current at a predetermined value.
11立差j
以上説明のごとく1本発明によれば単一のトランスによ
って放電部材が必要とする交互電圧および直流電圧の両
方が供給されるので装置の小型化および低廉価が達成で
きる。11 Standal difference j As explained above, according to the present invention, since both the alternating voltage and the DC voltage required by the discharge member are supplied by a single transformer, the device can be made more compact and inexpensive.
第1図は従来の帯電装置の基本構成を示し、第2図は本
発明の実施例による帯電装置を示し、
第3図は第2図の各部の電圧波形を示す。
符号の説明
lは放電部材、2は誘導電極、3は放電電極、4は誘電
体、5は被帯電体、7は交流電源、8はバイアス電圧印
加手段、lOはトランス手段、13は入力側巻線、14
は第1の出力側巻線、15は第2の出力側巻線である。
第1図
第3図FIG. 1 shows the basic configuration of a conventional charging device, FIG. 2 shows a charging device according to an embodiment of the present invention, and FIG. 3 shows voltage waveforms at various parts in FIG. Explanation of symbols 1 is a discharge member, 2 is an induction electrode, 3 is a discharge electrode, 4 is a dielectric, 5 is a charged object, 7 is an AC power source, 8 is a bias voltage application means, 1O is a transformer means, 13 is an input side winding, 14
15 is a first output side winding, and 15 is a second output side winding. Figure 1 Figure 3
Claims (1)
電極の近傍にイオンを発生させる交互電圧と、放電電極
と被帯電体との間に作用し前記イオンを抽出して被帯電
体を特定極性に帯電させる外部電界の両方を与えるトラ
ンス手段と、 を有することを特徴とする帯電装置[Claims] A dielectric, an induction electrode and a discharge electrode extending between the dielectric, and ions generated near the discharge electrode by applying alternating voltages between the induction electrode and the discharge electrode. and transformer means for applying both an alternating voltage to cause the charged object to be charged and an external electric field that acts between the discharge electrode and the charged object to extract the ions and charge the charged object to a specific polarity. Device
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18986085A JPS6250857A (en) | 1985-08-30 | 1985-08-30 | Electrostatic charging device |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP18986085A JPS6250857A (en) | 1985-08-30 | 1985-08-30 | Electrostatic charging device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPS6250857A true JPS6250857A (en) | 1987-03-05 |
Family
ID=16248391
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP18986085A Pending JPS6250857A (en) | 1985-08-30 | 1985-08-30 | Electrostatic charging device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS6250857A (en) |
-
1985
- 1985-08-30 JP JP18986085A patent/JPS6250857A/en active Pending
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