JP3142034B2 - Apparatus and method for charging photoreceptor - Google Patents

Apparatus and method for charging photoreceptor

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Publication number
JP3142034B2
JP3142034B2 JP05238839A JP23883993A JP3142034B2 JP 3142034 B2 JP3142034 B2 JP 3142034B2 JP 05238839 A JP05238839 A JP 05238839A JP 23883993 A JP23883993 A JP 23883993A JP 3142034 B2 JP3142034 B2 JP 3142034B2
Authority
JP
Japan
Prior art keywords
magnetic field
magnetic
generating means
charging
photoreceptor
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 - Fee Related
Application number
JP05238839A
Other languages
Japanese (ja)
Other versions
JPH0736253A (en
Inventor
茂樹 塚原
進 菊地
龍士 芋生
泰夫 西口
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.)
Kyocera Corp
Original Assignee
Kyocera Corp
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 Kyocera Corp filed Critical Kyocera Corp
Priority to JP05238839A priority Critical patent/JP3142034B2/en
Priority to US08/245,281 priority patent/US5596394A/en
Publication of JPH0736253A publication Critical patent/JPH0736253A/en
Application granted granted Critical
Publication of JP3142034B2 publication Critical patent/JP3142034B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Description

【発明の詳細な説明】DETAILED DESCRIPTION OF THE INVENTION

【0001】[0001]

【産業上の利用分野】本発明は粒子帯電によりベルト状
若しくはドラム状感光体を帯電させる電子写真装置に於
ける帯電装置とその帯電方法に関する。
BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a charging device in an electrophotographic apparatus for charging a belt-shaped or drum-shaped photosensitive member by particle charging, and a charging method thereof.

【0002】[0002]

【従来の技術】従来より感光体ドラム外周面上に、露
光、現像、転写、クリーニング(残留トナー除去)、除
電、及び帯電の各プロセス手段を配置し、所定の電子写
真プロセスにより画像形成を行なう、いわゆるカールソ
ンプロセスに基づく画像形成装置は周知である。
2. Description of the Related Art Conventionally, respective process means of exposure, development, transfer, cleaning (removal of residual toner), charge elimination and charging are arranged on the outer peripheral surface of a photosensitive drum, and an image is formed by a predetermined electrophotographic process. Image forming apparatuses based on the so-called Carlson process are well known.

【0003】又近年円筒状の透光性支持体上に透光性導
電層と光導電体層を積層して感光体ドラムを形成すると
共に、該ドラム内に、画像情報に対応した光出力を生成
する露光手段(例えばLEDヘッド)を内挿し、所定の
帯電手段を用いて感光体ドラム上に帯電させた感光体ド
ラム上に前記露光手段の光出力を集束レンズを通して露
光すると同時若しくはその直後に前記感光体ドラムと対
面配置させた現像スリーブを介して前記潜像をトナー像
化(現像)した後、該トナー像を転写ローラその他の転
写手段を介して記録紙に転写可能に構成した画像形成装
置(特開昭58−153957号他)も公知である。
In recent years, a photoconductive drum is formed by laminating a light-transmitting conductive layer and a photoconductive layer on a cylindrical light-transmitting support, and a light output corresponding to image information is formed in the drum. Exposure means (for example, an LED head) to be generated is interpolated, and the light output of the exposure means is exposed on a photosensitive drum charged on the photosensitive drum using a predetermined charging means through a converging lens, or simultaneously or immediately after the exposure. An image forming apparatus configured to form the latent image into a toner image (development) through a developing sleeve facing the photosensitive drum and transfer the toner image to recording paper via a transfer roller or other transfer means; Apparatuses (JP-A-58-153957 and others) are also known.

【0004】この種の装置に用いる帯電手段は一般に細
いタングステン線に高電圧を印加してコロナ放電を行な
うコロトロン方式、又導電ローラに数百ボルトの電圧を
かけて感光体ドラムと接触帯電させるもの、又導電性ブ
ラシに電圧を印加して感光体ドラムに接触させながら帯
電を行なうもの等が存在する。しかしながらコロトロン
方式は高電圧を使用し、又オゾンを発生する等安全上、
環境上の問題が多い。又帯電ローラは感光体ドラムとの
接触が線接触であるために帯電が不安定である。更にブ
ラシ帯電方式はドラムとブラシが接触して帯電を行なう
為に、ブラシの帯電劣化が生じやすい。
The charging means used in this type of apparatus is generally a corotron type in which a high voltage is applied to a thin tungsten wire to perform corona discharge, or a charging means in which a conductive roller is charged in contact with a photosensitive drum by applying a voltage of several hundred volts. In addition, there is a type in which a voltage is applied to a conductive brush while being brought into contact with a photosensitive drum to charge the conductive brush. However, the corotron method uses high voltage and generates ozone for safety reasons.
Many environmental problems. Further, the charging roller is unstable in charging because the contact with the photosensitive drum is a line contact. Further, in the brush charging method, the charging of the brush is likely to occur because the drum and the brush are in contact with each other to perform charging.

【0005】かかる欠点を解消するために、図5に示す
ように、感光体ドラム101と磁石集成体102を内挿
した非磁性スリーブ103を用い、該スリーブ103に
帯電バイアス108を印加した状態で、該スリーブ10
3に磁性粒子群104を付着させて刷子状の磁気穂を感
光体ドラム101に摺擦させてスリーブ103を介して
帯電バイアス108を磁性粒子群104に印加させて帯
電を行なう、いわゆる粒子帯電法が提案されている。
(特開昭59ー133569、特開昭63ー18726
7他)
In order to eliminate such a defect, as shown in FIG. 5, a non-magnetic sleeve 103 having a photosensitive drum 101 and a magnet assembly 102 inserted therein is used, and a charging bias 108 is applied to the sleeve 103. , The sleeve 10
3 is a so-called particle charging method in which a magnetic particle group 104 is adhered to the brush 3 and a brush-shaped magnetic spike is rubbed against the photosensitive drum 101 to apply a charging bias 108 to the magnetic particle group 104 via a sleeve 103 to perform charging. Has been proposed.
(JP-A-59-133569, JP-A-63-18726)
7 others)

【0006】かかる帯電法において導電性微粒子により
感光体ドラム101を均一帯電させるには前記帯電領域
における磁性粒子群104と感光体ドラム101との接
触面積及び接触密度を十分な条件にする必要があるが、
磁気刷子の接触面積は感光体ドラム1と磁石集成体10
2を内挿した非磁性スリーブ103の外径によって決っ
てしまい、この為前記感光体ドラム101やスリーブ1
03を小型にすればするほど接触ニップが狭くなり、而
も感光体ドラム101の回転速度も大になるために、接
触ニップが不安定化しやすい。この為前記接触ニップの
安定性を図る為に、感光体ドラム101と非磁性スリー
ブ103間のギャップ公差を厳しく設定しているが、こ
のように構成すると組立工数等が増大し、コストアップ
につながるのみならず、固定磁石集成体102と非磁性
スリーブ103間の偏心等の組み立て誤差や熱その他の
環境要因による膨張/収縮等により磁力及び磁束密度等
が変動し、安定した帯電が出来ない。
In order to uniformly charge the photosensitive drum 101 with the conductive fine particles in such a charging method, the contact area and the contact density between the magnetic particle group 104 and the photosensitive drum 101 in the charged area must be set to sufficient conditions. But,
The contact area of the magnetic brush depends on the photosensitive drum 1 and the magnet assembly 10.
2 is determined by the outer diameter of the non-magnetic sleeve 103 in which the photosensitive drum 101 and the sleeve 1 are inserted.
The smaller the size of 03, the narrower the contact nip and the higher the rotation speed of the photosensitive drum 101, the more easily the contact nip becomes unstable. For this reason, the gap tolerance between the photosensitive drum 101 and the non-magnetic sleeve 103 is strictly set in order to ensure the stability of the contact nip. However, such a configuration increases the number of assembling steps and the like, leading to an increase in cost. In addition, the magnetic force and the magnetic flux density fluctuate due to assembly errors such as eccentricity between the fixed magnet assembly 102 and the non-magnetic sleeve 103 and expansion / contraction due to heat or other environmental factors, and stable charging cannot be performed.

【0007】次に磁性粒子の感光体ドラム付着(粒子引
き)の問題がある。又、前記従来技術においては、固定
磁石集成体102により磁気穂を形成した場合、該固定
磁石集成体102よりの距離の2乗に比例して磁界が減
衰し、従って感光体ドラム101表面に位置する磁性粒
子の磁気保持力は最も弱い。一方前記磁性粒子群104
は前記帯電領域内で粒子相互に若しくは感光体ドラム1
との間で摺擦し、帯電して電荷を持つ。従ってこの状態
で感光体ドラム101を回転させると、該ドラム101
表面に遠心力が働き、静電的に感光体ドラム101に付
着している磁性粒子104は固定磁石集成体102より
の磁気保持力(磁界)に抗して前記磁気穂、即ち帯電領
域から離脱する方向に力が働き、該感光体ドラム101
に付着した粒子104aが次工程の露光及び現像等に悪
影響を及ぼす。而も前記欠点は磁性粒子の粒径を小さく
すればするほど、又時間当りの印刷枚数を増やすため
に、感光体ドラム101の線速を早くすればするほど大
きくなる。この為前記従来技術は前記帯電領域の感光体
移動方向下流側にブレードを配して磁性粒子を回収する
ように構成しているが、かかる構成を取ると、長期使用
を可能にする為に前記ブレードに付着した磁性粒子を回
収する機構が必要になり、構成が煩雑化する。
Next, there is a problem that magnetic particles adhere to the photosensitive drum (particle pulling). Further, in the prior art, when the magnetic spikes are formed by the fixed magnet assembly 102, the magnetic field is attenuated in proportion to the square of the distance from the fixed magnet assembly 102. Magnetic particles have the weakest magnetic coercive force. On the other hand, the magnetic particle group 104
Are particles in the charged area or the photosensitive drum 1
And rubs between them to become charged and have electric charge. Therefore, when the photosensitive drum 101 is rotated in this state,
Centrifugal force acts on the surface, and the magnetic particles 104 electrostatically attached to the photosensitive drum 101 are separated from the magnetic chain, that is, the charged area, against the magnetic coercive force (magnetic field) from the fixed magnet assembly 102. The photosensitive drum 101
The particles 104a adhered to the surface adversely affect exposure and development in the next step. However, the above-mentioned disadvantage increases as the particle size of the magnetic particles decreases and as the linear speed of the photosensitive drum 101 increases in order to increase the number of prints per time. For this reason, the prior art is configured to collect the magnetic particles by arranging a blade downstream of the charging area in the photoconductor moving direction. A mechanism for collecting the magnetic particles attached to the blade is required, and the configuration becomes complicated.

【0008】更に前記従来技術は感光体ドラムと対向さ
せて磁石集成体若しくは該集成体を内包した帯電スリー
ブを配置する構成を取るために、感光体ドラム上に帯電
装置部分が大きく突設することになり、この為例え感光
体ドラムの小型化を図っても装置全体の小型化につなが
らない。
Further, in the above-mentioned prior art, in order to adopt a configuration in which a magnet assembly or a charging sleeve containing the assembly is disposed so as to be opposed to the photosensitive drum, a charging device portion is protruded largely on the photosensitive drum. For this reason, even if the size of the photosensitive drum is reduced, the size of the entire apparatus is not reduced.

【0009】本発明はかかる従来技術の欠点に鑑み、感
光体ドラムを小径化した場合においても、帯電領域と帯
電密度を有効に確保し得る帯電装置を提供する事を目的
とする。本発明の他の目的は、好ましくは感光体ドラム
と対向させて磁石集成体若しくは該集成体を内包した帯
電スリーブを削除した場合においても安定した帯電能を
維持し得、又これらを感光体ドラム上に対向配置した場
合においても前記帯電ギャップの変動及び組み立て誤差
等に影響される事なく、安定した帯電能を維持し得る帯
電装置を提供する事を目的とする。又本発明の他の目的
は簡単な構成で帯電領域外への磁性粒子の洩出を有効に
阻止し得る帯電装置と提供する事を目的とする。
SUMMARY OF THE INVENTION In view of the drawbacks of the prior art, it is an object of the present invention to provide a charging device capable of effectively securing a charging area and a charging density even when the diameter of a photosensitive drum is reduced. Another object of the present invention is to stably maintain the charging ability even when the magnet assembly or the charging sleeve containing the assembly is removed so as to face the photoconductor drum. It is an object of the present invention to provide a charging device that can maintain a stable charging ability without being affected by the fluctuation of the charging gap, an assembly error, and the like even when the charging device is disposed facing the upper side. Another object of the present invention is to provide a charging device which can effectively prevent magnetic particles from leaking out of the charging region with a simple configuration.

【0010】[0010]

【課題を解決する為の手段】かかる技術的課題を達成す
る為に、磁気力により感光体の帯電領域上に保持された
磁性粒子群を介して感光体を帯電可能に構成した感光体
の帯電装置において、前記感光体の帯電領域背面側に、
感光体移動方向に沿って極性の異なる2つの磁石体、若
しくは磁石体と磁性体の組合せからなる2つの磁界発生
手段を隣接配置し、該2つの磁界発生手段間に主として
形成される水平磁場により、前記磁性粒子群を感光体上
に密着させながら帯電させることを特徴とするものであ
る。この結果前記水平磁場により、感光体ドラム上に対
向配置した固定磁石体等と無関係に感光体背面側に配し
た2つの磁界発生手段のみで前記磁性粒子群を感光体上
に密着させる事ができる。又感光体ドラムを小径化した
場合においても有効に磁性粒子群が接触する帯電接触面
積と帯電密度を確保できるのみならず、感光体ドラムと
対向させて磁石集成体若しくは帯電スリーブを削除した
場合においても安定した帯電能を維持し得る。これによ
り感光体ドラム上に帯電装置部が大きく突設することに
なく、この為感光体ドラムの小型化と共に、装置全体の
小型化を容易に図れる。
SUMMARY OF THE INVENTION In order to achieve the above technical object, a photoreceptor is structured such that the photoreceptor can be charged by magnetic force via magnetic particles held on a charged area of the photoreceptor. In the apparatus, on the back side of the charged area of the photoconductor,
Two magnetic bodies having different polarities along the photoconductor moving direction or two magnetic field generating means composed of a combination of a magnet and a magnetic substance are arranged adjacent to each other, and a horizontal magnetic field mainly formed between the two magnetic field generating means is used. The magnetic particles are charged while being brought into close contact with the photoreceptor. As a result, due to the horizontal magnetic field, the magnetic particle group can be brought into close contact with the photoreceptor by only the two magnetic field generating means disposed on the back side of the photoreceptor, irrespective of the fixed magnet body and the like arranged opposite to the photoreceptor drum. . Even when the diameter of the photoconductor drum is reduced, not only can the charging contact area and the charging density with which the magnetic particles are effectively contacted be ensured, but also the case where the magnet assembly or the charging sleeve is removed in opposition to the photoconductor drum. Can also maintain stable charging ability. As a result, the charging device section does not protrude largely on the photosensitive drum, and therefore, the size of the photosensitive drum and the size of the entire apparatus can be easily reduced.

【0011】しかしながら前記の構成を取った場合感光
体背面側の磁力のみで磁性粒子を保持する構成を取るた
めに、帯電領域よりの磁性粒子の洩出を避けられない。
そこで本発明は帯電領域下流側に位置する感光体背面側
に、一対の同極性の隣接磁極からなる反発磁界を設け、
該反発磁界により感光体上の帯電領域下流端に無磁力帯
を形成し、これにより磁性粒子の洩出を阻止する構成を
取る。勿論かかる構成は感光体ドラムと対向させて磁石
集成体若しくは帯電スリーブを配設した場合にも有効で
あるが、この場合は感光体帯電領域下流側に感光体法線
方向に磁力線が沿う垂直磁場を形成する構成を取るのが
良い。そしてこの様な垂直磁場形成手段としては、具体
的には感光体帯電領域背面側に位置する2つの磁界発生
手段の内、感光体移動方向下流側に位置する第1の磁界
発生手段とほぼ対向させて感光体上方位置に磁性体若し
くは第1の磁界発生手段と逆極性の磁石体からなる垂直
磁場形成手段を配置することにより達成し得る。
However, when the above configuration is adopted, the configuration is such that the magnetic particles are held only by the magnetic force on the back side of the photoreceptor, so that leakage of the magnetic particles from the charged area cannot be avoided.
Therefore, the present invention provides a repulsive magnetic field composed of a pair of adjacent magnetic poles of the same polarity on the back side of the photoconductor located downstream of the charging area,
The repelling magnetic field forms a non-magnetic force zone at the downstream end of the charged area on the photoconductor, thereby preventing leakage of the magnetic particles. Of course, such a configuration is also effective when a magnet assembly or a charging sleeve is provided so as to face the photoconductor drum, but in this case, a perpendicular magnetic field in which the magnetic field lines extend in the normal direction of the photoconductor downstream of the photoconductor charging area. It is good to take the structure which forms. As such a vertical magnetic field forming means, specifically, of the two magnetic field generating means located on the back side of the photoconductor charging area, the first magnetic field generating means located on the downstream side in the photoconductor moving direction is substantially opposed to the first magnetic field generating means. This can be achieved by arranging a vertical magnetic field forming means made of a magnetic material or a magnet having a polarity opposite to that of the first magnetic field generating means at a position above the photoconductor.

【0012】そして更に好ましい磁性粒子漏洩阻止手段
として感光体帯電領域背面側に位置する2つの磁界発生
手段の内、感光体移動方向下流側に位置する第1の磁界
発生手段を磁石体で形成し、一方該第1の磁界発生手段
とほぼ対向させて感光体上方位置に第1の磁界発生手段
と逆極性の第2の磁石体を配置するとともに、前記第1
の磁界発生手段若しくは第2の磁石体の帯電方向下流側
側面に磁性体を隣接配置し、前記何れかの磁石体と磁性
体間で垂直磁場の閉回路を形成する事により一層磁性粒
子の阻止が有効となる。尚前記磁性粒子群を、導電性磁
性粒子で構成するか若しくは導電性粒子と磁性粒子の混
合粒子群で構成し、該粒子群に帯電バイアスを印加可能
に構成する事により感光体の線速を早くしても又感光体
ドラム小径化により帯電領域が狭くなっても十分なる帯
電を確保し得る。
As a further preferred magnetic particle leakage preventing means, of the two magnetic field generating means located on the back side of the photosensitive member charging area, the first magnetic field generating means located on the downstream side in the photosensitive member moving direction is formed by a magnet. On the other hand, a second magnet body having a polarity opposite to that of the first magnetic field generating means is arranged at a position above the photosensitive member so as to substantially face the first magnetic field generating means, and
A magnetic substance is disposed adjacent to the magnetic field generating means or the second magnet body on the downstream side in the charging direction, and a magnetic field is further prevented by forming a closed circuit of a vertical magnetic field between any one of the magnet bodies and the magnetic body. Becomes effective. In addition, the magnetic particles may be formed of conductive magnetic particles or a mixed particle of conductive particles and magnetic particles, and the linear velocity of the photoconductor may be reduced by applying a charging bias to the particles. Sufficient charging can be ensured even when the charging speed is increased and the charging area is reduced due to the reduction in the diameter of the photosensitive drum.

【0013】[0013]

【実施例】以下、図面に基づいて本発明の実施例を例示
的に詳しく説明する。但しこの実施例に記載されている
構成部品の寸法、材質、形状、その相対配置などは特に
特定的な記載がない限りは、この発明の範囲をそれのみ
に限定する趣旨ではなく単なる説明例に過ぎない。図1
に基づいて本発明の第1実施例に係る帯電装置の構成に
ついて説明する。本装置は感光体ドラム上に帯電スリー
ブや固定磁石集成体を対向配置する事なく、感光体ドラ
ム背面側のみに配置した実施例を示す。1は時計廻りに
回転する感光体ドラムで、その帯電領域と対応するドラ
ム背面側には、該帯電領域をほぼ2分するごとく、その
上流側にN極の第1の磁石体5B及び下流側に逆極性の
S極の第2の磁石体5Aとを隣接配置し、両磁石体5
A、5B間の感光体ドラム1上に水平磁場6Aを形成す
る。そして前記第2の磁石体5Aに隣接させて感光体ド
ラム1回転方向における帯電領域下流端を越えた位置
に、第2の磁石体5Aと同極性のS極に設定した反発磁
石体5Cを配設し、両者間で形成される反発磁界6Cに
よる無磁力帯6Dが帯電領域下流端に位置するように配
設する。
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a block diagram showing an embodiment of the present invention; However, unless otherwise specified, the dimensions, materials, shapes, relative arrangements, and the like of the components described in this embodiment are not intended to limit the scope of the present invention, but are merely illustrative examples. Not just. FIG.
The configuration of the charging device according to the first embodiment of the present invention will be described based on FIG. This embodiment shows an embodiment in which a charging sleeve and a fixed magnet assembly are not arranged on the photosensitive drum but opposed to each other, and are arranged only on the back side of the photosensitive drum. Reference numeral 1 denotes a photosensitive drum which rotates clockwise. On the back side of the drum corresponding to the charged area, an N-pole first magnet body 5B and a downstream side are provided on the upstream side so as to substantially divide the charged area into two. And a second magnet body 5A having an S pole having the opposite polarity is disposed adjacent to the second magnet body 5A.
A horizontal magnetic field 6A is formed on the photosensitive drum 1 between A and 5B. At a position adjacent to the second magnet body 5A and beyond the downstream end of the charging area in the rotation direction of the photosensitive drum 1, a repulsion magnet body 5C having the same polarity as the second magnet body 5A and having the S pole is disposed. And a non-magnetic force zone 6D formed by the repulsive magnetic field 6C formed therebetween is located at the downstream end of the charging area.

【0014】そして前記夫々の磁石体の磁力は、例えば
後記する磁性粒子を用いた場合、感光体ドラム1側の磁
極の端面で夫々800ガウスに設定し、前記磁石体5A
直上の感光体ドラム1表面で300〜400ガウス前後
の磁力を得るように設定するのが好ましい。そして前記
帯電領域上に介在させる導電性磁性粒子4は導電性であ
れば特に限定されないが、フェライトや鉄粉、マグネタ
イト等の磁性コアの表面に導電性樹脂で被覆した導電性
磁性粒子で構成するか若しくは導電性粒子と磁性粒子の
混合粒子群4で構成してもよい。例えば平均粒径が30
μm前後の磁性粒子母材と、平均粒径が15μm前後の
導電粒子材を適宜割合で配合したものを用いても良い。
尚、本実施例においては平均粒径が20〜35μm、抵
抗率103〜106Ω・cmのフェライトコア粒子を用
い、磁気特性を60〜70emu/g(1k Oe)に設定した
ものを用いる。8は線状電極を介して導電性磁性粒子群
4に帯電バイアスを印加させるバイアス電源である。
The magnetic force of each of the magnet bodies is set to 800 gauss at the end face of the magnetic pole on the photosensitive drum 1 side, for example, when magnetic particles described later are used.
It is preferable that a magnetic force of about 300 to 400 Gauss be obtained on the surface of the photosensitive drum 1 immediately above. The conductive magnetic particles 4 interposed on the charged region are not particularly limited as long as they are conductive, but are formed of conductive magnetic particles having a magnetic resin surface coated with a conductive resin such as ferrite, iron powder, or magnetite. Alternatively, it may be composed of a mixed particle group 4 of conductive particles and magnetic particles. For example, if the average particle size is 30
A mixture of a magnetic particle base material having a particle size of about 15 μm and a conductive particle material having an average particle size of about 15 μm at an appropriate ratio may be used.
In this example, ferrite core particles having an average particle diameter of 20 to 35 μm and a resistivity of 10 3 to 10 6 Ω · cm are used, and magnetic characteristics set to 60 to 70 emu / g (1 k Oe) are used. . Reference numeral 8 denotes a bias power supply for applying a charging bias to the conductive magnetic particle group 4 via the linear electrode.

【0015】図2は前記磁極レイアウトにおける垂直磁
場6Bと水平磁場6Aの磁気作用を示し、本図より理解
される通り、各磁極の直上位置に夫々垂直磁場6Bが形
成されると共に、帯電領域に位置するN極とS極の両磁
石体5A、5B間に強い水平磁場6Aが、又前記S極と
帯電領域下端側のS極の第2の磁石体5Aと反発磁石体
5Cとの間に、2つの水平磁場6Aが分断された反発磁
界6Cが形成され、結果として2つの磁極5A、5C間
に無磁力帯域6Dが形成される。
FIG. 2 shows the magnetic action of the vertical magnetic field 6B and the horizontal magnetic field 6A in the above-described magnetic pole layout. As can be understood from FIG. 2, the vertical magnetic field 6B is formed immediately above each magnetic pole, and the charged area is formed. A strong horizontal magnetic field 6A is located between the N-pole and S-pole magnet bodies 5A and 5B located between the S-pole and the S-pole second magnet body 5A and the repulsion magnet body 5C at the lower end of the charged area. A repulsive magnetic field 6C in which the two horizontal magnetic fields 6A are separated is formed, and as a result, a non-magnetic force zone 6D is formed between the two magnetic poles 5A and 5C.

【0016】この結果前記帯電領域に付着される磁性粒
子群4は、N極とS極の両磁石体5A、5B間の水平磁
場6A上で感光体ドラム1上に密着して付着し、又前記
水平磁場6Aから外れた帯電領域下流側の垂直磁場6B
上では、粗の状態で感光体ドラム1法線方向に立つよう
に付着される。この状態で感光体ドラム1が回転する
と、水平磁場6A上で感光体ドラム1への帯電を行ない
ながら水平磁場6Aから垂直磁場6B上に移動し、更に
磁性粒子群は反発磁石体5Cにより形成される無磁力帯
域6Dにより下流側に搬送されることなく、垂直磁場6
Bにより垂直方向に逃げるしかない。そして垂直方向に
向った磁性粒子群は、第1及び第2の両磁石体5A、5
Bからなる磁界に引戻され、水平磁場6A側に引戻さ
れ、以下繰り返し循環を行なう。従ってかかる実施例に
よれば帯電領域下流側に磁性粒子が漏洩することなく円
滑な帯電が行なわれる。
As a result, the magnetic particle group 4 adhered to the charged area adheres closely to the photosensitive drum 1 on the horizontal magnetic field 6A between the N-pole and S-pole magnets 5A and 5B. The vertical magnetic field 6B on the downstream side of the charged area deviating from the horizontal magnetic field 6A
Above, it is attached so as to stand in the normal direction of the photosensitive drum 1 in a rough state. When the photoconductor drum 1 rotates in this state, the photoconductor drum 1 moves from the horizontal magnetic field 6A to the vertical magnetic field 6B while charging the photoconductor drum 1 on the horizontal magnetic field 6A, and the magnetic particles are formed by the repulsive magnet 5C. Without being transported downstream by the non-magnetic force zone 6D.
B has to escape in the vertical direction. The magnetic particle group oriented in the vertical direction is composed of the first and second magnet bodies 5A, 5A,
The magnetic field is returned to the magnetic field composed of B, and then returned to the horizontal magnetic field 6A side, and thereafter, circulation is repeatedly performed. Therefore, according to this embodiment, smooth charging is performed without leakage of the magnetic particles to the downstream side of the charging area.

【0017】図3は固定磁石を感光体ドラムに対向配置
させた他の実施例で、前記実施例との差異を中心に説明
する。本実施例は、前記実施例の反発磁石体5Cを設け
ずに、感光体ドラム1より所定ギャップを介して法線方
向に立設する棒状固定磁石体2により漏洩阻止用の垂直
磁場6Bを形成した他の実施例で、前記固定磁石体2は
感光体ドラム1と対峙する側にN極を位置させ、そして
前記対向配置される第2の磁石体5Bと固定磁石体2を
感光体ドラム回転方向における帯電領域下流側に配し、
両磁石体2、5B間に垂直磁場6Bにより前記磁性粒子
群4を磁気保持させ、又第1の磁石体5Aは前記第2の
磁石体5Bに隣接させて帯電領域上流側に配置させ、前
記第2の磁石体5Bと第1の磁石体5A間に主として形
成される水平磁場6Aにより前記磁性粒子群4を感光体
ドラム1上に密着させる。
FIG. 3 shows another embodiment in which a fixed magnet is arranged to face the photosensitive drum, and a description will be given focusing on differences from the above embodiment. In this embodiment, the vertical magnetic field 6B for preventing leakage is formed by the bar-shaped fixed magnet 2 erected in the normal direction from the photosensitive drum 1 via a predetermined gap without providing the repulsion magnet 5C of the above-described embodiment. In another embodiment described above, the fixed magnet body 2 has an N-pole located on the side facing the photosensitive drum 1, and the second magnet body 5B and the fixed magnet body 2 disposed opposite to each other are rotated by the photosensitive drum. Arranged downstream of the charging area in the direction,
The magnetic particle group 4 is magnetically held by a vertical magnetic field 6B between the two magnet bodies 2 and 5B, and the first magnet body 5A is arranged adjacent to the second magnet body 5B and on the upstream side of the charging area. The magnetic particle group 4 is brought into close contact with the photosensitive drum 1 by a horizontal magnetic field 6A mainly formed between the second magnet body 5B and the first magnet body 5A.

【0018】かかる構成において、前記夫々の磁石体の
磁力を、前記固定磁石体2では感光体ドラム1と対峙す
るN極の端面で例えば1200ガウス前後に、又前記第
2の磁石体5Aは感光体ドラム1側のS極の端面で例え
ば800ガウスに設定した場合、前記両磁石体2、5A
上の感光体ドラム1表面で300ガウス前後の磁力を得
る事が出来、該感光体ドラム1表面上で磁性粒子群4の
十分なる磁気保持力が得られる事が確認された。又第1
の磁石体5Aの磁力を第2の磁石体5Bとほぼ同等に設
定する事により有効な水平磁場6Aが得られる事も確認
出来た。更に前記帯電領域中に磁性粒子群4中に攪拌手
段11を配置して、機械的な攪拌により粒子群4の入替
えを行なうように構成すると共に、該攪拌手段に帯電バ
イアス電源8を接続させる。
In this configuration, the magnetic force of each of the magnets is set to, for example, about 1200 gauss at the end face of the N pole facing the photosensitive drum 1 in the fixed magnet 2, and the second magnet 5A When the end face of the south pole on the body drum 1 side is set to, for example, 800 gauss, the two magnet bodies 2, 5A
A magnetic force of about 300 Gauss could be obtained on the surface of the upper photosensitive drum 1, and it was confirmed that a sufficient magnetic coercive force of the magnetic particles 4 could be obtained on the surface of the photosensitive drum 1. Also the first
It was also confirmed that an effective horizontal magnetic field 6A could be obtained by setting the magnetic force of the magnet body 5A to be substantially equal to that of the second magnet body 5B. Further, a stirring means 11 is arranged in the magnetic particle group 4 in the charging region, and the particle group 4 is replaced by mechanical stirring, and a charging bias power supply 8 is connected to the stirring means.

【0019】かかる実施例によれば、前記感光体ドラム
1上の水平磁場6A上で磁性粒子群4を密着させながら
感光体ドラム1表面を円滑に帯電させた微粒子群は、感
光体ドラム1の回転に従って垂直磁場6B位置まで移動
し、ここで該垂直磁場6Bにより微粒子群4が磁気的に
封止され、帯電領域外への漏洩を阻止すると共に、磁力
差により、感光体ドラム1側より固定磁石体側に磁性粒
子群4が吸着され、そして前記攪拌手段を矢印方向に回
転させる事により帯電領域上流側に移動しながら水平磁
場6A側に戻入され、以下前記動作を繰り返す。
According to this embodiment, the fine particles whose surface is smoothly charged while the magnetic particles 4 are brought into close contact with each other on the horizontal magnetic field 6A on the photosensitive drum 1 It moves to the position of the vertical magnetic field 6B according to the rotation, where the fine particle group 4 is magnetically sealed by the vertical magnetic field 6B, preventing leakage outside the charged area, and fixed from the photosensitive drum 1 side by the magnetic force difference. The magnetic particle group 4 is attracted to the magnet body side, and is returned to the horizontal magnetic field 6A side while moving to the upstream of the charging area by rotating the stirring means in the direction of the arrow, and the above operation is repeated.

【0020】従って前記帯電領域上の磁性粒子4は例え
水平磁場6Aにより密着状態にあっても常に循環され、
長期使用しても帯電粒子の劣化が生じる余地がない。
尚、前記入替え若しくは循環は前記第2の磁石体5B若
しくは第1の磁石体5Aを電磁石体で形成し、例えば直
流電源13の電圧可変器12等を利用して非印字時、若
しくは所定印字枚数毎に適宜極性変換若しくは印加電圧
の変更を行なう事により、更には前記第1の磁石体5A
若しくは第2の磁石体5Bを、適宜所定角度揺動させて
粒子群4の入替え及び循環を行なってもよい。尚、前記
固定磁石体2の代わりに磁性体を用いても同様に垂直磁
場6Bが形成され、かかる実施例において前記実施例と
同様な作用が達成し得ると共に、現像バイアス電源8を
磁性体に接続してもよい。
Therefore, the magnetic particles 4 on the charged area are always circulated even if they are in close contact with each other by the horizontal magnetic field 6A,
Even if used for a long time, there is no room for deterioration of the charged particles.
The replacement or circulation is performed by forming the second magnet body 5B or the first magnet body 5A with an electromagnet body, and using a voltage variable device 12 of a DC power supply 13 or the like to perform non-printing or predetermined printing. By appropriately changing the polarity or changing the applied voltage for each sheet, the first magnet body 5A
Alternatively, the replacement and circulation of the particle groups 4 may be performed by appropriately swinging the second magnet body 5B by a predetermined angle. Note that a vertical magnetic field 6B is similarly formed even when a magnetic material is used in place of the fixed magnet body 2. In this embodiment, the same operation as that of the embodiment can be achieved, and the developing bias power supply 8 is connected to the magnetic material. You may connect.

【0021】図4(A)(B)は本発明の他の実施例で
図3の実施例との差異を中心に説明するに、図上右方向
に回転する感光体ドラム1に対し帯電ギャップ(0.5
mm)を介して前記感光体ドラム1の回転方向とアゲイ
ンスト方向(図上左方向)に回転可能により非磁性スリ
ーブ3を配設すると共に、該非磁性スリーブ3の背面側
の帯電領域下流側にN極の固定磁石体2を第2の磁石体
5Aと対向して配置すると共に、該固定磁石体2の帯電
領域下端側に磁性体2aを隣接配置し、垂直磁場6Bの
閉回路を形成する。かかる実施例によれば、前記感光体
ドラム1上の水平磁場6A上で磁性粒子群4を密着させ
ながら感光体ドラム1表面を円滑に帯電させた微粒子群
は、感光体ドラム1の回転に従って垂直磁場6B位置ま
で移動し、ここで該垂直磁場6Bにより微粒子群4が磁
気的に封止され、帯電領域外への漏洩を阻止すると共
に、磁力差により、感光体ドラム1側よりスリーブ3側
へ向け磁性粒子群4が吸着され、そして非磁性スリーブ
3のアゲインスト回転により該スリーブ3に担持された
まま帯電領域上流側に移動し、水平磁場6Aの磁気力に
より、感光体ドラム1側に落下し、以下前記動作を繰り
返す。
FIGS. 4A and 4B show another embodiment of the present invention. The difference from the embodiment of FIG. 3 will be mainly described. (0.5
mm) so as to be rotatable in the rotational direction of the photosensitive drum 1 and in the opposite direction (left direction in the drawing), and at the downstream side of the charging area on the back side of the non-magnetic sleeve 3. The N-pole fixed magnet body 2 is arranged to face the second magnet body 5A, and the magnetic body 2a is arranged adjacent to the lower end side of the charged area of the fixed magnet body 2 to form a closed circuit of the vertical magnetic field 6B. . According to this embodiment, the fine particles that smoothly charge the surface of the photosensitive drum 1 while closely contacting the magnetic particles 4 on the horizontal magnetic field 6 </ b> A on the photosensitive drum 1 become vertical as the photosensitive drum 1 rotates. It moves to the position of the magnetic field 6B, where the vertical magnetic field 6B magnetically seals the fine particle group 4 to prevent leakage outside the charged area, and also causes the magnetic force difference to move from the photosensitive drum 1 side to the sleeve 3 side. The magnetic particles 4 are attracted, move toward the upstream side of the charging area while being carried on the non-magnetic sleeve 3 by the against rotation of the non-magnetic sleeve 3, and fall to the photosensitive drum 1 side by the magnetic force of the horizontal magnetic field 6A. Then, the above operation is repeated.

【0022】この場合、固定磁石体には磁性体が隣接配
置され垂直磁場6Bの閉回路が形成されている為に、磁
気シールド効果が一層増大する。この場合、前記磁性体
は前記固定磁石体と対向する第2に磁石体5Aのドラム
回転方向下流端側面に隣接配置しても同様な作用を営
む。又前記現像スリーブ3よりの粒子の循環を促すため
に、スクレーパ14を設け、機械的に剥離させて水平磁
場6A上の感光体ドラム1側に落下するように構成して
もよい。
In this case, since the magnetic material is arranged adjacent to the fixed magnet and a closed circuit of the vertical magnetic field 6B is formed, the magnetic shielding effect is further increased. In this case, the same operation is achieved even when the magnetic body is disposed adjacent to the second magnet body 5A on the downstream side in the drum rotation direction, facing the fixed magnet body. Further, in order to promote the circulation of the particles from the developing sleeve 3, a scraper 14 may be provided so that the scraper 14 is mechanically peeled off and falls on the photosensitive drum 1 side on the horizontal magnetic field 6A.

【0023】[0023]

【効果】以上記載のごとく本発明によれば、前記水平磁
場により所定幅域の帯電領域を確保できるために、感光
体ドラムを小径化した場合においても、又感光体ドラム
と対向させて磁石集成体若しくは該集成体を内包した帯
電スリーブを削除した場合においても安定した帯電能を
維持し得る。又前記帯電スリーブ等を感光体ドラム上に
対向配置した場合においても前記帯電ギャップの変動及
び組み立て誤差等に影響される事なく、安定した帯電能
を維持し得る。又前記帯電ギャップの変動及び組み立て
誤差等に影響される事なく、常に均一磁場を得る事が出
来る。又本発明は垂直磁場若しくは無磁力帯等を利用し
て簡単な構成で帯電領域外への磁性粒子の洩出を有効に
阻止し得る。等の種々の著効を有す。
As described above, according to the present invention, it is possible to secure a charging area of a predetermined width range by the horizontal magnetic field. Therefore, even when the diameter of the photosensitive drum is reduced, the magnet assembly is opposed to the photosensitive drum. Even when the body or the charging sleeve containing the assembly is omitted, stable charging ability can be maintained. Further, even when the charging sleeve and the like are arranged on the photosensitive drum so as to face each other, stable charging ability can be maintained without being affected by the fluctuation of the charging gap and assembly errors. Further, a uniform magnetic field can always be obtained without being affected by the fluctuation of the charging gap and the assembly error. Further, according to the present invention, it is possible to effectively prevent the leakage of the magnetic particles to the outside of the charged region with a simple configuration utilizing a vertical magnetic field or a non-magnetic force zone. And so on.

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

【図1】感光体ドラムの背面側のみに磁石体を配置した
本発明の実施例を示す概略図である。
FIG. 1 is a schematic view showing an embodiment of the present invention in which a magnet is arranged only on the back side of a photosensitive drum.

【図2】図1の磁力線の作用図である。FIG. 2 is an operation diagram of the magnetic force lines of FIG.

【図3】本発明の第2実施例に係る慨略図である。FIG. 3 is a schematic diagram according to a second embodiment of the present invention.

【図4】(A)は本発明の第3実施例に係る慨略図、
(B)はその拡大図である。
FIG. 4A is a schematic diagram according to a third embodiment of the present invention,
(B) is an enlarged view thereof.

【図5】従来技術にかかる帯電装置の全体概略図であ
る。
FIG. 5 is an overall schematic diagram of a charging device according to the related art.

【符号の説明】[Explanation of symbols]

1 感光体ドラム 2 固定磁石体 5A 第1の磁石体 5B 第2の磁石体 5C 反発磁石体 2a 磁性体 4 導電性磁性粒子群 6B 垂直磁場 6A 水平磁場 6C 反発磁界 6D 無磁力帯域 REFERENCE SIGNS LIST 1 photosensitive drum 2 fixed magnet body 5A first magnet body 5B second magnet body 5C repulsive magnet body 2a magnetic body 4 conductive magnetic particle group 6B vertical magnetic field 6A horizontal magnetic field 6C repulsive magnetic field 6D nonmagnetic field

───────────────────────────────────────────────────── フロントページの続き (72)発明者 西口 泰夫 東京都世田谷区玉川台2丁目14番9号 京セラ株式会社東京用賀事業所内 (56)参考文献 特開 平5−181347(JP,A) (58)調査した分野(Int.Cl.7,DB名) G03G 15/02 G03G 15/09 ──────────────────────────────────────────────────続 き Continuation of the front page (72) Inventor Yasuo Nishiguchi 2-14-9 Tamagawadai, Setagaya-ku, Tokyo Kyocera Corporation Tokyo Yoga Office (56) References JP-A-5-181347 (JP, A) ( 58) Field surveyed (Int. Cl. 7 , DB name) G03G 15/02 G03G 15/09

Claims (8)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】 磁気力により感光体の帯電領域上に保持
された磁性粒子群を介して感光体を帯電可能に構成した
感光体の帯電装置において、 前記感光体の帯電領域背面側に、感光体移動方向に沿っ
て極性の異なる2つの磁石体、若しくは磁石体と磁性体
の組合せからなる2つの磁界発生手段を隣接配置し、該
2つの磁界発生手段間に主として形成される水平磁場に
より、前記磁性粒子群を感光体上に密着させながら帯電
させることを特徴とする感光体の帯電装置。
1. A charging device for a photoreceptor configured to be able to charge a photoreceptor via a magnetic particle group held on a charging region of the photoreceptor by a magnetic force, wherein a photosensitive element is provided on the back side of the charging region of the photoreceptor. Two magnet bodies having different polarities along the body movement direction, or two magnetic field generating means composed of a combination of a magnet body and a magnetic substance are arranged adjacently, and a horizontal magnetic field mainly formed between the two magnetic field generating means, A charging device for a photoconductor, wherein the magnetic particles are charged while being brought into close contact with the photoconductor.
【請求項2】 帯電領域下流側に位置する感光体背面側
に、一対の同極性の隣接磁極からなる反発磁界を形成
し、該反発磁界により感光体上の帯電領域下流端に無磁
力帯域を形成した請求項1記載の感光体の帯電装置。
2. A repulsive magnetic field comprising a pair of adjacent magnetic poles of the same polarity is formed on the back side of the photoreceptor located on the downstream side of the charged area, and a non-magnetic force band is formed at the downstream end of the charged area on the photoreceptor by the repulsive magnetic field. The charging device for a photoreceptor according to claim 1 formed.
【請求項3】 感光体帯電領域下流側の前記感光体の帯
電領域背面側に第1の磁界発生手段を設け、該第1の磁
界発生手段に対向させて感光体帯電領域表面側に第2の
磁界発生手段を配置し、前記第1の磁界発生手段を磁石
体とし、前記第2の磁界発生手段を前記磁石体と逆極性
の磁石体もしくは磁性体で構成し、 感光体帯電領域下流側に感光体法線方向に磁力線が沿う
垂直磁場を形成した請求項1記載の感光体の帯電装置。
(3)The belt of the photoconductor downstream of the photoconductor charging area
A first magnetic field generating means is provided on the back side of the
A second surface facing the photoreceptor charged area facing the field generating means;
Magnetic field generating means is arranged, and the first magnetic field generating means is a magnet
And the second magnetic field generating means has a polarity opposite to that of the magnet.
Composed of a magnet or magnetic material  Magnetic field lines along the photoconductor normal direction downstream of photoconductor charging area
2. The charging device for a photoconductor according to claim 1, wherein a vertical magnetic field is formed.
【請求項4】 前記感光体の帯電領域背面側と表面側に
互いに対向して2つの磁界発生手段を配置し、背面側に
配置された第1の磁界発生手段を磁性体とし、第2の磁
界発生手段を前記第1の磁界発生手段に隣接配置された
磁石体と同極性の磁石体として、感光体帯電領域下流側
に感光体法線方向に磁力線が沿う垂直磁場を形成した請
求項1記載の感光体の帯電装置。
4. A method according to claim 1, wherein said photosensitive member has a charged area on the back side and on the front side.
Two magnetic field generating means are arranged facing each other, and on the back side
The first magnetic field generating means disposed is made of a magnetic material, and the second magnetic field
A field generating means disposed adjacent to the first magnetic field generating means;
As a magnet body of the same polarity as the magnet body, downstream of the photoconductor charging area
A vertical magnetic field with a magnetic field line in the normal direction of the photoconductor
The charging device for a photoreceptor according to claim 1 .
【請求項5】 前記感光体の帯電領域背面側に位置する
2つの磁界発生手段の内、感光体移動方向下流側に位置
する第1の磁界発生手段を磁石体で形成し、一方該第1
の磁界発生手段とほぼ対向させて感光体上方位置に第1
の磁界発生手段と逆極性の第2の磁石体を配置するとと
もに、前記第1の磁界発生手段若しくは第2の磁石体の
帯電方向下流側側面に磁性体を隣接配置し、前記何れか
の磁石体と磁性体間で垂直磁場の閉回路を形成してなる
請求項3記載の感光体の帯電装置。
5. A magnetic field generating means, wherein the first magnetic field generating means located on the downstream side in the moving direction of the photoreceptor is formed of a magnet, among the two magnetic field generating means located on the back side of the charged area of the photoreceptor.
And a first position above the photoreceptor substantially opposed to the magnetic field generating means.
A second magnet body having a polarity opposite to that of the first magnetic field generating means, and a magnetic body adjacently arranged on the charging direction downstream side of the first magnetic field generating means or the second magnet body; 4. The charging device for a photoreceptor according to claim 3, wherein a closed circuit of a vertical magnetic field is formed between the body and the magnetic body.
【請求項6】 前記磁性粒子群を、導電性磁性粒子で構
成するか若しくは導電性粒子と磁性粒子の混合粒子群で
構成し、該粒子群に帯電バイアスを印加可能に構成した
請求項1記載の感光体の帯電装置。
6. The magnetic particle group is formed of conductive magnetic particles or a mixed particle group of conductive particles and magnetic particles, and a charging bias can be applied to the particle group. Photoconductor charging device.
【請求項7】 磁気力により感光体の帯電領域上に保持
された磁性粒子群を介して感光体を帯電させる感光体の
帯電方法において、 前記感光体の帯電領域背面側に、感光体移動方向に沿っ
て極性の異なる2つの磁石体もしくは磁石体と磁性体の
組み合わせからなる2つの磁界発生手段を隣接配置して
前記感光体表面の帯電領域に主として形成される水平磁
を形成し、前記磁性粒子群を感光体上に密着させなが
ら帯電させるとともに、前記帯電領域下流側の感光体背面側に、一対の同極性の
隣接磁極からなる反発磁界を形成して、該反発磁界によ
り前記 帯電領域下流端側の感光体表面上に無磁力帯域を
形成し、帯電領域上に位置する磁性粒子の漏洩を阻止す
るように作用させた事を特徴とする感光体の帯電方法。
7. A method of charging a photoconductor, wherein the photoconductor is charged by a magnetic force via a group of magnetic particles held on the charged area of the photoconductor. Along
And two magnets with different polarities or a magnet and a magnetic
Two magnetic field generating means consisting of a combination
Said photosensitive member to form a horizontal magnetic field is mainly formed on the charged area of the surface, the magnetic particles with charging while in close contact on the photosensitive member, the photosensitive member back side of the charging area downstream, a pair of the same polarity of
A repulsive magnetic field consisting of adjacent magnetic poles is formed, and
A non-magnetic force zone is formed on the surface of the photoreceptor at the downstream end side of the charging area to prevent leakage of magnetic particles located on the charging area.
【請求項8】 磁気力により感光体の帯電領域上に保持
された磁性粒子群を介して感光体を帯電させる感光体の
帯電方法において、感光体移動方向に沿って極性の異なる2つの磁石体もし
くは磁石体と磁性体の組み合わせからなる2つの磁界発
生手段を隣接配置して、 前記感光体表面の帯電領域に主
として形成される水平磁場を形成し、前記磁性粒子群を
感光体上に密着させながら帯電させるとともに、前記帯電領域下流側の感光体背面側に、第1の磁界発生
手段を配置し、該第1の磁界発生手段にほぼ対向させて
感光体上方位置に第2の磁界発生手段を配置するととも
に、 前記第1の磁界発生手段が磁石体の場合は第2磁界発生
手段は磁性体とし、 前記第1の磁界発生手段が磁性体の場合は第2の磁界発
生手段は磁石体とし、これら第1及び第2の磁界発生手
段により、前記 帯電領域下流端側の感光体表面上に主と
して垂直磁場からなる磁気漏洩阻止域を形成し、該阻止
域を利用して帯電領域上に位置する磁性粒子の漏洩を阻
止するように作用させた事を特徴とする感光体の帯電方
法。
8. Holding on a charged area of a photoreceptor by magnetic force
Of the photoreceptor that charges the photoreceptor via the magnetic particles
In the charging method,If two magnets with different polarities along the photoconductor movement direction
Or two magnetic fields consisting of a combination of magnet and magnetic material
Place the raw means adjacent, Mainly in the charged area on the photoreceptor surface
Horizontal magnetic field formed asTo formThe magnetic particle group
While being charged while closely contacting the photoreceptor,A first magnetic field is generated on the photoreceptor back side downstream of the charging area.
Means is disposed and substantially opposed to said first magnetic field generating means.
The second magnetic field generating means is arranged above the photoconductor.
To When the first magnetic field generating means is a magnet, a second magnetic field is generated.
The means is a magnetic material, When the first magnetic field generating means is a magnetic material, a second magnetic field generating means is provided.
The generating means is a magnet body, and the first and second magnetic field generating means are used.
Step by step Mainly on the photoconductor surface at the downstream end side of the charging area
To form a magnetic leakage stop zone consisting of a perpendicular magnetic field.
Area to prevent leakage of magnetic particles located on the charged area
The method of charging a photoreceptor, characterized in that it acts to stop
Law.
JP05238839A 1993-05-20 1993-08-31 Apparatus and method for charging photoreceptor Expired - Fee Related JP3142034B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP05238839A JP3142034B2 (en) 1993-05-20 1993-08-31 Apparatus and method for charging photoreceptor
US08/245,281 US5596394A (en) 1993-05-20 1994-05-18 Charging apparatus for charging a photo-sensitive member by magnetically holding magnetic particles in a charging zone

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
JP13983193 1993-05-20
JP5-139831 1993-05-20
JP05238839A JP3142034B2 (en) 1993-05-20 1993-08-31 Apparatus and method for charging photoreceptor

Publications (2)

Publication Number Publication Date
JPH0736253A JPH0736253A (en) 1995-02-07
JP3142034B2 true JP3142034B2 (en) 2001-03-07

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Family Applications (1)

Application Number Title Priority Date Filing Date
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Country Link
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