JPH0736253A - Photosensitive member charging device and charging method - Google Patents
Photosensitive member charging device and charging methodInfo
- Publication number
- JPH0736253A JPH0736253A JP23883993A JP23883993A JPH0736253A JP H0736253 A JPH0736253 A JP H0736253A JP 23883993 A JP23883993 A JP 23883993A JP 23883993 A JP23883993 A JP 23883993A JP H0736253 A JPH0736253 A JP H0736253A
- Authority
- JP
- Japan
- Prior art keywords
- magnetic
- photoconductor
- charging
- magnetic field
- region
- Prior art date
- Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
- Granted
Links
Landscapes
- Electrostatic Charge, Transfer And Separation In Electrography (AREA)
Abstract
(57)【要約】
【目的】 本発明は、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粒子
帯電装置を提供する。
【構成】 前記感光体の帯電領域背面側に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。及び帯電領域下流
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。
(57) [Summary] [Object] The present invention provides a particle charging device capable of effectively ensuring a charging region and a charging density even when the diameter of a photosensitive drum is reduced. Two magnetic field generating means are arranged adjacent to each other on the back side of the charged area of the photoconductor, and the magnetic particle group is brought into close contact with the photoconductor by a horizontal magnetic field mainly formed between the two magnetic field generation means. To be charged. And a repulsive magnetic field composed of a pair of adjacent magnetic poles of the same polarity on the back side of the photoconductor located on the downstream side of the charging region, and the repulsive magnetic field forms a non-magnetic band at the downstream end of the charging region on the photoconductor. It is configured to prevent leakage of magnetic particles.
Description
【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 therefor.
【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, process means for exposing, developing, transferring, cleaning (removing residual toner), discharging, 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 light-transmitting conductive layer and a photoconductor layer are laminated on a cylindrical light-transmitting support to form a photosensitive drum, and an optical output corresponding to image information is provided in the drum. At the same time as or immediately after the exposure means (for example, an LED head) to be generated is inserted, and the light output of the exposure means is exposed through the focusing lens on the photosensitive drum charged on the photosensitive drum using a predetermined charging means. Image formation in which the latent image is formed into a toner image (developed) through a developing sleeve facing the photosensitive drum, and then the toner image can be transferred onto a recording sheet through a transfer roller or other transfer means. Apparatuses (Japanese Patent Laid-Open No. 58-153957, etc.) 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 system in which a high voltage is applied to a thin tungsten wire to carry out corona discharge, or a conductive roller is charged with a voltage of several hundreds of volts to contact and charge the photosensitive drum. In addition, there is one in which a voltage is applied to a conductive brush so that the brush is charged while being in contact with the photosensitive drum. However, the corotron method uses a high voltage, and in terms of safety such as generating ozone,
There are many environmental problems. Further, since the charging roller is in line contact with the photosensitive drum, charging is unstable. Further, in the brush charging method, since the drum and the brush contact each other to perform charging, the charging deterioration of the brush is likely to occur.
【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 drawback, 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, a magnetic particle group 104 is attached to the magnetic particle group 3, the brush-shaped magnetic brush is rubbed against the photosensitive drum 101, and a charging bias 108 is applied to the magnetic particle group 104 via the sleeve 103 to perform charging. Is proposed.
(JP-A-59-133569, JP-A-63-18726
7 and 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 the charging method, in order to uniformly charge the photosensitive drum 101 with the conductive fine particles, it is necessary to make the contact area and the contact density between the magnetic particle group 104 and the photosensitive drum 101 in the charging region sufficient conditions. But,
The contact area of the magnetic brush is 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 faster the rotation speed of the photosensitive drum 101, the more likely the contact nip becomes unstable. Therefore, in order to ensure the stability of the contact nip, the gap tolerance between the photosensitive drum 101 and the non-magnetic sleeve 103 is set to be strict. However, with this configuration, the number of assembling steps and the like increase, which leads to an increase in cost. In addition, the magnetic force and the magnetic flux density fluctuate due to an assembly error such as eccentricity between the fixed magnet assembly 102 and the non-magnetic sleeve 103 and expansion / contraction due to heat and other environmental factors, so that 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 above-mentioned prior art, when a magnetic ear is 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, and therefore the position on the surface of the photosensitive drum 101 is reduced. The magnetic coercive force of the magnetic particles is weakest. On the other hand, the magnetic particle group 104
Are in the charging area between the particles or the photosensitive drum 1
It rubs against and becomes charged and has an electric charge. Therefore, when the photosensitive drum 101 is rotated in this state, the drum 101
The centrifugal force acts on the surface, and the magnetic particles 104 electrostatically adhering to the photosensitive drum 101 are separated from the magnetic brush, that is, the charged area against the magnetic coercive force (magnetic field) from the fixed magnet assembly 102. Force acts in the direction of
The particles 104a attached to the surface adversely affect exposure and development in the next process. However, the above-mentioned drawbacks become more serious as the particle size of the magnetic particles is made smaller and the linear velocity of the photosensitive drum 101 is made faster in order to increase the number of printed sheets per hour. For this reason, in the above-mentioned conventional technique, a blade is arranged on the downstream side of the charging region in the moving direction of the photoconductor to collect the magnetic particles. A mechanism for collecting the magnetic particles attached to the blade is required, which complicates the configuration.
【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 prior art, since the magnet assembly or the charging sleeve including the assembly is arranged so as to face the photosensitive drum, the charging device portion is largely projected on the photosensitive drum. Therefore, even if the size of the photosensitive drum is reduced, the size of the entire apparatus cannot be 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。In view of the above-mentioned drawbacks of the prior art, it is an object of the present invention to provide a charging device capable of effectively ensuring the charging area and the charging density even when the diameter of the photosensitive drum is reduced. Another object of the present invention is to maintain a stable charging ability even when the magnet assembly or the charging sleeve containing the assembly is removed, preferably facing the photoconductor drum, and these can be maintained. An object of the present invention is to provide a charging device capable of maintaining 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 opposed to the above. Another object of the present invention is to provide a charging device capable of effectively preventing leakage of magnetic particles to the outside of the charging region with a simple structure.
【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。In order to achieve such a technical problem, charging of a photoconductor is configured so that the photoconductor can be charged through a group of magnetic particles held on a charged region of the photoconductor by a magnetic force. In the device, on the back side of the charged area of the photoconductor,
Two magnetic field generating means composed of two magnet bodies having different polarities or a combination of the magnet body and the magnetic body are adjacently arranged along the moving direction of the photoconductor, and a horizontal magnetic field mainly formed between the two magnetic field generating means is used. It is characterized in that the magnetic particles are charged while being brought into close contact with the photoreceptor. As a result, by the horizontal magnetic field, the magnetic particle group can be brought into close contact with the photoconductor only by the two magnetic field generating means arranged on the back side of the photoconductor, irrespective of the fixed magnet body and the like arranged opposite to each other on the photoconductor drum. . Further, even when the diameter of the photosensitive drum is reduced, not only can the charging contact area and the charging density with which the magnetic particle groups come into contact effectively be secured, but also when the magnet assembly or the charging sleeve is removed facing the photosensitive drum. Can maintain a stable charging ability. As a result, the charging device portion does not largely project on the photosensitive drum, and therefore the photosensitive drum can be downsized and the entire device can be easily downsized.
【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, in the case of the above configuration, since the magnetic particles are held only by the magnetic force on the back side of the photoconductor, leakage of the magnetic particles from the charging 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 surface side of the photoconductor located on the downstream side of the charging area,
The repulsive magnetic field forms a non-magnetic band at the downstream end of the charged area on the photoconductor, thereby preventing leakage of magnetic particles. Of course, such a configuration is also effective when the magnet assembly or the charging sleeve is provided so as to face the photoconductor drum, but in this case, a vertical magnetic field in which the magnetic force lines extend in the photoconductor normal direction on the downstream side of the photoconductor charging area. It is better to have a structure that forms a. As such a vertical magnetic field forming means, specifically, of the two magnetic field generating means located on the back side of the charging area of the photoconductor, it substantially opposes the first magnetic field generating means located on the downstream side in the moving direction of the photoconductor. This can be achieved by arranging a vertical magnetic field forming means composed of a magnetic body or a magnet body having a polarity opposite to that of the first magnetic field generating means 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 more preferable magnetic particle leakage prevention means, of the two magnetic field generating means located on the back side of the charging area of the photoconductor, the first magnetic field generating means located on the downstream side in the moving direction of the photoconductor is formed by a magnet body. On the other hand, a second magnet body having a polarity opposite to that of the first magnetic field generating means is disposed above the photoconductor so as to be substantially opposed to the first magnetic field generating means, and
The magnetic substance is further disposed by arranging the magnetic substance adjacent to the magnetic field generating means or the side face on the downstream side in the charging direction of the second magnet substance, and forming a closed circuit of the vertical magnetic field between any of the magnet substances and the magnetic substance. Is effective. The magnetic particle group is composed 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 so that the linear velocity of the photoreceptor can be increased. Sufficient charging can be ensured even if the charging area is narrowed due to the reduction in 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。Embodiments of the present invention will now be illustratively described in detail with reference to the drawings. However, the dimensions, materials, shapes, relative positions and the like of the components described in this embodiment are not intended to limit the scope of the present invention thereto, but are merely examples, unless otherwise specified. Not too much. Figure 1
The configuration of the charging device according to the first exemplary embodiment of the present invention will be described based on FIG. This apparatus shows an embodiment in which a charging sleeve and a fixed magnet assembly are not arranged opposite to each other on the photosensitive drum, but are arranged only on the rear surface side of the photosensitive drum. Reference numeral 1 denotes a photoconductor drum that rotates clockwise. On the drum back side corresponding to the charging area, the first magnet body 5B having an N pole is provided on the upstream side and the downstream side is provided so as to divide the charging area almost in two. And a second magnet body 5A having an S pole of opposite polarity are arranged adjacent to each other,
A horizontal magnetic field 6A is formed on the photosensitive drum 1 between A and 5B. Then, a repulsive magnet body 5C having an S pole having the same polarity as that of the second magnet body 5A is arranged 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. The non-magnetic band 6D due to the repulsive magnetic field 6C formed between the two 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 forces of the respective magnets are set to 800 gauss at the end faces of the magnetic poles on the side of the photoconductor drum 1 when the magnetic particles described later are used, and the magnets 5A are set.
It is preferable to set the magnetic force of about 300 to 400 gauss on the surface of the photosensitive drum 1 immediately above. The conductive magnetic particles 4 interposed on the charging area are not particularly limited as long as they are conductive, but are composed of conductive magnetic particles such as ferrite, iron powder, magnetite, etc., whose surface is coated with a conductive resin. Alternatively, it may be composed of a mixed particle group 4 of conductive particles and magnetic particles. For example, the average particle size is 30
It is also possible to use a mixture of a magnetic particle base material having a particle size of about μm and a conductive particle material having an average particle size of about 15 μm in an appropriate ratio.
In this embodiment, ferrite core particles having an average particle size of 20 to 35 μm and a resistivity of 10 3 to 10 6 Ω · cm are used, and magnetic properties of which are set to 60 to 70 emu / g (1 k Oe) are used. . Reference numeral 8 is a bias power source 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 magnetic pole layout. As can be understood from this figure, the vertical magnetic field 6B is formed directly above each magnetic pole and the charging area is formed. There is a strong horizontal magnetic field 6A between the N and S pole magnet bodies 5A and 5B, and between the S pole and the second magnet body 5A of the S pole on the lower end side of the charging area and the repulsive magnet body 5C. A repulsive magnetic field 6C is formed by dividing the two horizontal magnetic fields 6A, and as a result, a non-magnetic field 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 is adhered and adhered onto the photosensitive drum 1 on the horizontal magnetic field 6A between the N and S magnets 5A and 5B. Vertical magnetic field 6B on the downstream side of the charging area deviated from the horizontal magnetic field 6A
In the 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 particle group is formed by the repulsive magnet body 5C. The vertical magnetic field 6 without being transported downstream due to the non-magnetic field 6D
There is no choice but to escape vertically due to B. The magnetic particle group oriented in the vertical direction is composed of the first and second magnet bodies 5A and 5A.
The magnetic field of B is returned to the horizontal magnetic field 6A side, and the circulation is repeated thereafter. Therefore, according to this embodiment, the smooth charging is performed without the magnetic particles leaking 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 opposite to a photosensitive drum, and the difference from the above embodiment will be mainly described. In this embodiment, a vertical magnetic field 6B for preventing leakage is formed by the rod-shaped fixed magnet body 2 standing upright from the photosensitive drum 1 in the normal direction through a predetermined gap without providing the repulsive magnet body 5C of the above embodiment. In another embodiment, 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 arranged to face each other are rotated. Placed on the downstream side 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 on the upstream side of the charging area. The magnetic particle group 4 is brought into close contact with the photosensitive drum 1 by the 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 such a structure, the magnetic force of each of the magnet bodies is, for example, about 1200 gauss at the end face of the N pole facing the photosensitive drum 1 in the fixed magnet body 2, and the second magnet body 5A is exposed to light. When the end face of the S pole on the body drum 1 side is set to, for example, 800 Gauss, the two magnet bodies 2, 5A
It was confirmed that a magnetic force of about 300 Gauss could be obtained on the surface of the upper photosensitive drum 1, and a sufficient magnetic holding force of the magnetic particle group 4 could be obtained on the surface of the photosensitive drum 1. The first
It was also confirmed that an effective horizontal magnetic field 6A can be obtained by setting the magnetic force of the magnet body 5A of No. 1 to be almost equal to that of the second magnet body 5B. Further, the stirring means 11 is disposed in the magnetic particle group 4 in the charging area so that the particle group 4 is replaced by mechanical stirring, and the charging bias power source 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 such an embodiment, the fine particle group in which the surface of the photosensitive drum 1 is smoothly charged while the magnetic particle group 4 is closely contacted on the horizontal magnetic field 6A on the photosensitive drum 1 is According to the rotation, it moves to the position of the vertical magnetic field 6B, where the vertical magnetic field 6B magnetically seals the fine particle group 4 to prevent the particles from leaking out of the charging region, and is fixed from the photosensitive drum 1 side by the magnetic force difference. The magnetic particle group 4 is adsorbed on the magnet body side, and is then returned to the horizontal magnetic field 6A side while moving to the charging area upstream side by rotating the stirring means in the arrow direction, 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,
There is no room for deterioration of charged particles even after long-term use.
For the replacement or circulation, the second magnet body 5B or the first magnet body 5A is formed of an electromagnet body, and for example, by using the voltage changer 12 of the DC power supply 13 or the like when no printing is performed or predetermined printing is performed. By appropriately changing the polarity or changing the applied voltage for each number of sheets, the first magnet body 5A
Alternatively, the second magnet body 5B may be appropriately swung by a predetermined angle to exchange and circulate the particle group 4. A vertical magnetic field 6B is similarly formed even if a magnetic material is used instead of the fixed magnet body 2, and in this embodiment, the same operation as in the above embodiment can be achieved, and the developing bias power supply 8 is made a 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, focusing on the difference from the embodiment of FIG. 3, in which the charging gap is set with respect to the photosensitive drum 1 rotating in the right direction in the drawing. (0.5
mm), the non-magnetic sleeve 3 is disposed rotatably in the rotation direction of the photoconductor drum 1 and in the against direction (left direction in the drawing), and on 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 charging area of the fixed magnet body 2 to form a closed circuit of the vertical magnetic field 6B. . According to such an embodiment, the fine particle group in which the surface of the photosensitive drum 1 is smoothly charged while the magnetic particle group 4 is brought into close contact with the horizontal magnetic field 6A on the photosensitive drum 1 becomes vertical as the photosensitive drum 1 rotates. The magnetic field 6B is moved to a position where the vertical magnetic field 6B magnetically seals the fine particle group 4 to prevent leakage to the outside of the charging area, and due to the magnetic force difference, from the photosensitive drum 1 side to the sleeve 3 side. The directed magnetic particle group 4 is adsorbed, and is moved to the upstream side of the charging area while being held by the sleeve 3 by the against rotation of the non-magnetic sleeve 3, and is dropped to the photosensitive drum 1 side by the magnetic force of the horizontal magnetic field 6A. Then, the above operation is repeated thereafter.
【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 body is disposed adjacent to the fixed magnet body to form the closed circuit of the vertical magnetic field 6B, the magnetic shield effect is further enhanced. In this case, the same action is achieved even if the magnetic body is arranged adjacent to the downstream side surface of the second magnet body 5A facing the fixed magnet body in the drum rotation direction. Further, in order to promote the circulation of particles from the developing sleeve 3, a scraper 14 may be provided so that the scraper 14 is mechanically separated and drops onto 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, the horizontal magnetic field can secure a charging area in a predetermined width range. Therefore, even when the diameter of the photosensitive drum is reduced, the magnet assembly is provided so as to face the photosensitive drum. Stable charging ability can be maintained even when the body or the charging sleeve containing the assembly is removed. Further, even when the charging sleeve and the like are arranged opposite to each other on the photosensitive drum, the stable charging ability can be maintained without being affected by the fluctuation of the charging gap and the assembly error. Further, it is possible to always obtain a uniform magnetic field without being affected by the fluctuation of the charging gap and the assembly error. Further, the present invention can effectively prevent the leakage of magnetic particles to the outside of the charging area with a simple structure by utilizing a vertical magnetic field or a non-magnetic field. It has various remarkable effects.
【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 body 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 magnetic force lines in 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 view of a charging device according to a conventional technique.
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 1 Photoconductor 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 Non-magnetic band
フロントページの続き (72)発明者 芋生 龍士 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 (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Front Page Continuation (72) Inventor Ryushi Imo 2-14-9 Tamagawadai, Setagaya-ku, Tokyo Kyocera Corporation Tokyo Yoga Works (72) Inventor Yasuo Nishiguchi 2-14-9 Tamagawadai, Setagaya-ku, Tokyo No. Kyocera Corporation Tokyo Yoga Works
Claims (8)
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 photoconductor, comprising a magnetic particle group held on the charging region of the photoconductor by a magnetic force so that the photoconductor can be charged. Two magnetic fields having different polarities along the body moving direction, or two magnetic field generating means composed of a combination of a magnet and a magnetic body are arranged adjacent to each other, and a horizontal magnetic field formed mainly between the two magnetic field generating means A charging device for a photoconductor, characterized in that the magnetic particles are charged while being in close contact with the photoconductor.
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 composed of a pair of adjacent magnetic poles of the same polarity is formed on the back side of the photoconductor located on the downstream side of the charging region, and the repulsive magnetic field forms a non-magnetic band at the downstream end of the charging region on the photoconductor. The charging device for the photoconductor according to claim 1, which is formed.
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. A charging device for a photosensitive member according to claim 1, wherein a vertical magnetic field having magnetic force lines along the photosensitive member normal direction is formed on the downstream side of the photosensitive member charging area.
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してなる請求項3記載の感
光体の帯電装置4. A magnetic body or a magnetic body located above the photoconductor substantially facing the first magnetic field generation means located downstream of the photoconductor moving direction in the two magnetic field generation means located on the back side of the photoconductor charging area. 4. A charging device for a photosensitive member according to claim 3, wherein a vertical magnetic field forming means composed of a magnet body having a polarity opposite to that of the first magnetic field generating means is arranged.
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. 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 moving direction of the photoconductor is formed of a magnet body, and the first magnetic field is formed. A second magnet body having a polarity opposite to that of the first magnetic field generating means is arranged at a position above the photoconductor so as to be substantially opposed to the generating means, and
A magnetic body is disposed adjacent to a downstream side surface of the first magnetic field generating means or the second magnet body in the charging direction, and a closed circuit of a vertical magnetic field is formed between any one of the magnet bodies and the magnetic body. 3. The charging device for the photoconductor according to item 3.
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 composed 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
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、 前記感光体表面の帯電領域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
帯電させるとともに、該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 by a magnetic force through a group of magnetic particles held on the charged region of the photoconductor by a magnetic force, comprising: a horizontal magnetic field formed mainly in the charged region of the surface of the photoconductor. By this, the magnetic particle group is charged while being brought into close contact with the photoconductor, and a non-magnetic field is formed on the surface of the photoconductor on the downstream end side of the charging region to prevent leakage of the magnetic particles located on the charging region. Charging method for a photoconductor characterized in that
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、 前記感光体表面の帯電領域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
帯電させるとともに、該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. A method of charging a photoconductor by magnetic force through a group of magnetic particles held on the charged region of the photoconductor, comprising: a horizontal magnetic field mainly formed in the charged region of the surface of the photoconductor. The magnetic particle group is charged while being brought into close contact with the photoconductor, and a magnetic leakage block region mainly composed of a vertical magnetic field is formed on the surface of the photoconductor on the downstream end side of the charging region by using the block region. A method of charging a photoconductor, characterized in that it acts so as to prevent leakage of magnetic particles located on the charging area.
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 true JPH0736253A (en) | 1995-02-07 |
| JP3142034B2 JP3142034B2 (en) | 2001-03-07 |
Family
ID=26472530
Family Applications (1)
| Application Number | Title | Priority Date | Filing Date |
|---|---|---|---|
| JP05238839A Expired - Fee Related JP3142034B2 (en) | 1993-05-20 | 1993-08-31 | Apparatus and method for charging photoreceptor |
Country Status (1)
| Country | Link |
|---|---|
| JP (1) | JP3142034B2 (en) |
-
1993
- 1993-08-31 JP JP05238839A patent/JP3142034B2/en not_active Expired - Fee Related
Also Published As
| Publication number | Publication date |
|---|---|
| JP3142034B2 (en) | 2001-03-07 |
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