JPH0736252A - Photoconductor charging device - Google Patents

Photoconductor charging device

Info

Publication number
JPH0736252A
JPH0736252A JP23230893A JP23230893A JPH0736252A JP H0736252 A JPH0736252 A JP H0736252A JP 23230893 A JP23230893 A JP 23230893A JP 23230893 A JP23230893 A JP 23230893A JP H0736252 A JPH0736252 A JP H0736252A
Authority
JP
Japan
Prior art keywords
magnetic
charging
photoconductor
magnetic field
sleeve
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
Application number
JP23230893A
Other languages
Japanese (ja)
Other versions
JP3087934B2 (en
Inventor
Shigeki Tsukahara
茂樹 塚原
Susumu Kikuchi
進 菊地
Tatsuji Imoo
龍士 芋生
Yasuo Nishiguchi
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 JP05232308A priority Critical patent/JP3087934B2/en
Priority to US08/245,281 priority patent/US5596394A/en
Publication of JPH0736252A publication Critical patent/JPH0736252A/en
Application granted granted Critical
Publication of JP3087934B2 publication Critical patent/JP3087934B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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Abstract

(57)【要約】 【目的】 粒子帯電において長期帯電によっても帯電剤
が劣化する事なく安定した帯電能を確保し得る帯電装置 【構成】 感光体帯電領域下流側に、感光体1を挟んで
その背面側と表面側に夫々磁性体若しくは磁石体からな
る磁界発生手段2A、5A(5A’)をほぼ対向配置
し、感光体法線方向に垂直磁場4Aを形成し、一方感光
体帯電領域上流側に、前記磁性粒子群4の循環手段2
B、11、9を配し、該循環手段2B、11、9と垂直
磁場4A形成位置間で帯電域に位置する磁性粒子群4を
循環可能に構成する。
(57) [Abstract] [Purpose] A charging device capable of ensuring stable charging ability without deteriorating the charging agent even during long-term charging in particle charging [Configuration] The photosensitive member 1 is sandwiched on the downstream side of the photosensitive member charging area. Magnetic field generating means 2A, 5A (5A ') made of a magnetic body or a magnet body are arranged substantially opposite to each other on the back side and the front side, and a vertical magnetic field 4A is formed in the photoconductor normal direction, while the photoconductor charging area is upstream. On the side, the circulation means 2 for the magnetic particle group 4
B, 11, and 9 are arranged so that the magnetic particle group 4 located in the charging area can be circulated between the circulation means 2B, 11, and 9 and the vertical magnetic field 4A formation position.

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.

【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】又前記従来技術では、磁石集成体102の
磁極Sが帯電領域に固定状態にあるために、該帯電領域
にある磁性粒子群が移動することなく帯電を継続する構
造となるために、長期帯電動作により前記磁性粒子が劣
化し帯電能が低下するという問題が生じる。
Further, in the above-mentioned prior art, since the magnetic pole S of the magnet assembly 102 is fixed in the charging area, the magnetic particles in the charging area are structured to continue charging without moving. The long-term charging operation causes a problem that the magnetic particles are deteriorated and the charging ability is lowered.

【0008】かかる欠点を防止するために、前記磁石集
成体を回転させる方式もあるが、かかる方式では駆動系
の構造が複雑となる上に、磁極が高速で移動するため
に、渦電流の発生、磁性粒子の飛散等の問題が生じる。
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が最
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101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。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。
In order to prevent such a drawback, there is a method of rotating the magnet assembly. However, in this method, the structure of the drive system is complicated and the magnetic pole moves at a high speed, so that eddy current is generated. However, problems such as scattering of magnetic particles occur.
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 groups 104 are charged by being rubbed with each other or with the photosensitive drum 101 by being rubbed in the charging region. Therefore, when the photosensitive drum 101 is rotated in this state, a centrifugal force acts on the surface of the drum 101, and the magnetic particles 104 electrostatically attached to the photosensitive drum 101 are retained by the fixed magnet assembly 102. A force acts against the (magnetic field) in the direction away from the magnetic brush, that is, the charged area, and the particles 104a attached to the photosensitive drum 101 adversely affect the exposure and development in the next step. 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.

【0009】本発明はかかる従来技術の欠点に鑑み、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と提供す
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
装置を提供する事を目的とする。更に本発明の他の目的
は、長期帯電によっても帯電剤が劣化する事なく安定し
た帯電能を確保し得る帯電装置を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 which can maintain a stable charging ability without being affected by the fluctuation of the charging gap and the assembly error. Another object of the present invention is to provide a charging device which can effectively prevent leakage of magnetic particles to the outside of the charging region with a simple structure. Still another object of the present invention is to provide a charging device capable of ensuring stable charging ability without deterioration of the charging agent even after long-term charging.

【0010】[0010]

【課題を解決する為の手段】本発明は、図1に示すよう
に磁性粒子群4を磁気的に担持させる磁界発生手段2
A、5A(5A’)、即ち磁石体若しくは磁性体を、非
磁性スリーブ3背面側のみではなく、感光体1背面側に
も配置した点を第1の特徴とする。この場合前記垂直磁
場を形成する位置におけるスリーブ3表面磁力が感光体
表面磁力より大になるように構成するのがよい。これに
より磁性粒子の磁気保持を行なう磁極が帯電ギャップの
片側にのみ配置されているのではなく、両側に配置され
る事になるために、帯電ギャップ間の磁化力(ΔH/Δ
t)をほぼ均一に設定でき、結果として前記帯電ギャッ
プの多少の組み立て誤差等があっても又ギャップ公差を
大きく取っても、更には感光体ドラム1や非磁性スリー
ブ3の偏心等を考慮する事なく、安定した磁性粒子群4
の磁気保持力を維持できる。
According to the present invention, a magnetic field generating means 2 for magnetically carrying a magnetic particle group 4 as shown in FIG.
A first feature is that A, 5A (5A ′), that is, a magnet body or a magnetic body is arranged not only on the back side of the non-magnetic sleeve 3 but also on the back side of the photoconductor 1. In this case, the surface magnetic force of the sleeve 3 at the position where the vertical magnetic field is formed is preferably larger than the surface magnetic force of the photosensitive member. As a result, the magnetic poles for magnetically retaining the magnetic particles are not arranged on only one side of the charging gap but on both sides thereof, so that the magnetizing force (ΔH / Δ) between the charging gaps is increased.
t) can be set substantially evenly, and as a result, even if there is some assembly error in the charging gap or a large gap tolerance is taken into consideration, the eccentricity of the photosensitive drum 1 or the non-magnetic sleeve 3 is taken into consideration. Stable magnetic particle group 4
The magnetic holding power of can be maintained.

【0011】又組み立て公差や偏心量等を粗く設定でき
る事は組立工数や製造コストの低減につながる。この場
合前記磁界発生手段2A、5A(5A’)は、逆極性の
磁石体、又磁石体と磁性体の組合せの何れでも可であ
る。又前記磁性粒子群4は一般には、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
で構成するのがよく、そして該粒子群4にスリーブ3若
しくはブレードを介して帯電バイアス8を印加可能に構
成する。
Further, the rough setting of the assembly tolerance, the amount of eccentricity, etc. leads to a reduction in the assembly man-hour and the manufacturing cost. In this case, the magnetic field generating means 2A, 5A (5A ′) may be magnet bodies of opposite polarities or a combination of magnet bodies and magnetic bodies. Further, it is generally preferable that the magnetic particle group 4 is composed of conductive magnetic particles or a mixed particle group of conductive particles and magnetic particles, and the particle group 4 is charged through the sleeve 3 or the blade. The bias 8 can be applied.

【0012】第2の特徴は前記磁界発生手段2A、5A
(5A’)をほぼ対向させて配置し、感光体法線方向に
垂直磁場を形成すると共に、前記非磁性スリーブ3を感
光体移動方向に対し反対方向すなわちアゲインスト方向
に回転可能に構成した事にある。即ち感光体1の法線方
向における垂直磁場4Aを帯電領域下流側に配すること
により、いわゆる垂直磁気バリアが帯電領域の下流側に
形成できるために、感光体1に静電的に付着した磁性粒
子が帯電領域外へ洩出するのを防ぐ事が出来、結果とし
て前記従来技術に用いたようなブレードや該ブレードに
付着した磁性粒子を回収する機構が不要になり、構成が
簡単化する。而も本発明は前記非磁性スリーブ3を感光
体に対しアゲインスト方向に回転させる事により、前記
垂直磁場4A上で滞留した磁性粒子群を帯電域上流側へ
循環させることが出来る。
The second characteristic is that the magnetic field generating means 2A, 5A.
(5A ') are arranged so as to face each other to form a vertical magnetic field in the normal direction of the photoconductor, and the non-magnetic sleeve 3 is rotatable in the opposite direction to the moving direction of the photoconductor, that is, in the against direction. It is in. That is, by arranging the vertical magnetic field 4A in the normal direction of the photoconductor 1 on the downstream side of the charging region, a so-called vertical magnetic barrier can be formed on the downstream side of the charging region, so that the magnetic force electrostatically attached to the photoconductor 1 is formed. It is possible to prevent the particles from leaking out of the charged area, and as a result, the blade used in the above-mentioned prior art and the mechanism for collecting the magnetic particles attached to the blade are not required, and the structure is simplified. Further, according to the present invention, by rotating the non-magnetic sleeve 3 in the against direction with respect to the photoconductor, the magnetic particle group retained on the vertical magnetic field 4A can be circulated to the upstream side of the charging area.

【0013】この場合前記垂直磁場4Aを形成する位置
におけるスリーブ表面磁力が感光体表面磁力より大にな
るように構成することにより前記循環が一層円滑に行な
うことが出来る。これにより長期帯電を行なっても前記
磁性粒子が劣化し帯電能が低下する事がない。そして好
ましくは、前記垂直磁場4A形成位置より感光体移動方
向上流側に磁性粒子群4を循環若しくは攪拌させる手段
2B、11、9を設ける事により、前記垂直磁場4Aに
より磁気封止された磁性粒子群4が帯電領域内を一層円
滑に循環若しくは攪拌させることが出来る。尚、前記循
環手段2B、11、9は例えば非磁性スリーブ3内の固
定磁石集成体に設けた反発磁界により、帯電域上流側の
非磁性スリーブ3上に無磁力帯を形成し、該無磁力帯か
らなる磁気的開放手段2A、2Bにより前記非磁性スリ
ーブ3上に担持された磁性粒子群4の磁気的拘束を解
き、感光体側に落下させるように構成してもよく、又非
磁性スリーブ3上に担持された磁性粒子群4を、前記帯
電域上流側で機械的に剥離させるフィルムやブレード等
の機械的剥離手段9を用いてもよい。
In this case, the circulation can be performed more smoothly by constructing the sleeve surface magnetic force at the position where the vertical magnetic field 4A is formed to be larger than the photosensitive member surface magnetic force. As a result, the magnetic particles are not deteriorated and the charging ability is not deteriorated even after long-term charging. And preferably, by providing means 2B, 11 and 9 for circulating or stirring the magnetic particle group 4 on the upstream side in the moving direction of the photoconductor from the position where the vertical magnetic field 4A is formed, the magnetic particles magnetically sealed by the vertical magnetic field 4A. The group 4 can circulate or stir more smoothly in the charging area. The circulation means 2B, 11 and 9 form a non-magnetic field on the non-magnetic sleeve 3 on the upstream side of the charging area by, for example, a repulsive magnetic field provided in a fixed magnet assembly in the non-magnetic sleeve 3. The magnetic releasing means 2A, 2B formed of a band may be configured to release the magnetic restraint of the magnetic particle group 4 carried on the non-magnetic sleeve 3 and drop it on the photoreceptor side. A mechanical peeling means 9 such as a film or a blade that mechanically peels the magnetic particle group 4 supported on the upstream side of the charging area may be used.

【0014】又前記の作用を円滑に営むためには、例え
ば 感光体帯電領域下流側に、感光体1を挟んでその背
面側と表面側に夫々磁性体若しくは磁石体からなる磁界
発生手段2A、5A(5A’)をほぼ対向配置し、感光
体法線方向に垂直磁場4Aを形成し、一方感光体帯電領
域上流側に、前記磁性粒子群4の循環手段2B、11、
9を配し、該循環手段2B、11、9と垂直磁場4A形
成位置間で帯電域に位置する磁性粒子群4を循環可能に
構成する事により、必ずしも非磁性スリーブ3を用いな
くても達成可能である。
In order to smoothly carry out the above-mentioned operation, for example, on the downstream side of the charging area of the photoreceptor, magnetic field generating means 2A composed of a magnetic body or a magnet body on the back side and the front side of the photoreceptor 1 with the photoreceptor 1 sandwiched therebetween, 5A (5A ′) are arranged substantially opposite to each other to form a vertical magnetic field 4A in the normal direction of the photoconductor, while on the upstream side of the photoconductor charging area, circulation means 2B, 11 for the magnetic particle group 4 are provided.
9 is arranged and the magnetic particles 4 located in the charging area can be circulated between the circulating means 2B, 11 and 9 and the position where the vertical magnetic field 4A is formed, so that the non-magnetic sleeve 3 is not necessarily used. It is possible.

【0015】[0015]

【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。
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.

【0016】図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。帯電装置20は前記し
たよう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(0.5mm)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固定配置した固
定磁石体2Aと、該固定磁石体2Aの帯電領域上流方
向、言換えればスリーブ回転方向下流側に、前記固定磁
石体2Aと同極性の反発磁石体2Bを配設する。尚、8
は不図示の導電ブレード若しくは非磁性スリーブ3を介
して導電性磁性粒子群4に現像バイアスを印加させるバ
イアス電源である。
The structure of the charging device according to the first embodiment of the present invention will be described with reference to the drawings. As described above, the charging device 20 is arranged so that the photoconductor drum 1 rotating to the right in the figure has a charging gap (0.5 mm) with respect to the photoconductor drum 1.
A non-magnetic sleeve 3 is rotatably provided in the rotation direction and the opposite direction (left direction in the drawing), and a fixed magnet body 2A fixedly arranged on the downstream side of the charging area on the back side of the non-magnetic sleeve 3; A repulsive magnet body 2B having the same polarity as that of the fixed magnet body 2A is arranged on the upstream side of the charging area of the fixed magnet body 2A, in other words, on the downstream side in the sleeve rotation direction. Incidentally, 8
Is a bias power source for applying a developing bias to the conductive magnetic particle group 4 via a conductive blade or a non-magnetic sleeve 3 not shown.

【0017】そして前記帯電領域上には導電性磁性粒子
群4を介在させる。該磁性粒子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30μm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。
A group of conductive magnetic particles 4 is interposed on the charged area. The magnetic particles are not particularly limited as long as they are conductive, but they are composed of conductive magnetic particles such as ferrite, iron powder, magnetite or the like coated on the surface of a magnetic core with a conductive resin, or a mixture of conductive particles and magnetic particles. It may be composed of the particle group 4. For example, a magnetic particle base material having an average particle size of about 30 μm and a conductive particle material having an average particle size of about 15 μm may be mixed in an appropriate ratio. In this embodiment, the average particle size is 20 to 35 μm and the resistivity is 10 3.
Ferrite core particles having a density of about 10 6 Ω · cm are used, and magnetic properties thereof are set to 60 to 70 emu / g (1 k Oe).

【0018】一方、感光体ドラム1の背面側には、帯電
領域下流側に位置する前記固定磁石体2Aとほぼ対向さ
せて第1の磁石体5Aと、前記第1の磁石体5Aに隣接
させて帯電領域上流側に第2の磁石体5Bとを隣接配置
すると共に、第1の磁石体5Aは前記固定磁石体2Aと
逆極性のS極に設定し、第2の磁石体5Bは該第1の磁
石体5Aと逆極性のN極に設定し、両磁石体5A、5B
間の感光体ドラム1上に水平磁場を形成する。即ち、具
体的には前記対向配置される第1の磁石体5Aと固定磁
石体2を感光体ドラム1回転方向における帯電領域下流
側に配し、両磁石体2A、5A間に形成された垂直磁場
4Aにより前記磁性粒子群4Aを磁気保持させ、又第2
の磁石体5Bは前記第1の磁石体5Aに隣接させて帯電
領域上流側に配置させ、前記第1の磁石体5Aと第2の
磁石体5B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4Bを感光体ドラム1上に密着させる。
On the other hand, on the rear surface side of the photosensitive drum 1, the first magnet body 5A and the first magnet body 5A are arranged so as to be substantially opposed to the fixed magnet body 2A located on the downstream side of the charging area. The second magnet body 5B is disposed adjacent to the upstream side of the charging area, the first magnet body 5A is set to the S pole having a polarity opposite to that of the fixed magnet body 2A, and the second magnet body 5B is set to the first magnet body 5B. The magnet body 5A of No. 1 is set to the N pole having the opposite polarity, and both magnet bodies 5A, 5B
A horizontal magnetic field is formed on the photosensitive drum 1 in between. That is, specifically, the first magnet body 5A and the fixed magnet body 2 which are opposed to each other are arranged on the downstream side of the charging area in the rotation direction of the photosensitive drum 1, and the vertical direction formed between the two magnet bodies 2A and 5A. The magnetic particles 4A are magnetically held by the magnetic field 4A, and
The magnet body 5B is arranged adjacent to the first magnet body 5A on the upstream side of the charging area, and the magnetic particles are generated by the horizontal magnetic field mainly formed between the first magnet body 5A and the second magnet body 5B. The group 4B is brought into close contact with the photosensitive drum 1.

【0019】そして固定磁石体2Aと同極性のN極に設
定した反発磁石体2Bは、両者間で形成される反発磁界
による無磁力帯が帯電領域上流側に位置するようにレイ
アウトし、これにより前記非磁性スリーブ3に担持され
て垂直磁場4A位置より帯電領域上流側に搬送された磁
性粒子群4Cを磁気的に開放し、感光体ドラム1側に落
下するように構成する。そして前記夫々の磁石体の磁力
は、前記固定磁石体2Aでは感光体ドラム1と対峙する
N極の端面で例えば1200〜1400ガウス前後に、
又前記第1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、前記磁石体5
A上の感光体ドラム1表面で300〜400ガウス前後
の磁力を得る事が出来、又スリーブ3上で800〜10
00ガウスの磁力が得られた。
The repulsive magnet body 2B set to the N pole having the same polarity as the fixed magnet body 2A is laid out so that the non-magnetic field due to the repulsive magnetic field formed between the two is located on the upstream side of the charging area. The magnetic particle group 4C carried on the non-magnetic sleeve 3 and conveyed to the upstream side of the charging area from the position of the vertical magnetic field 4A is magnetically released and dropped to the photosensitive drum 1 side. The magnetic force of each of the magnet bodies is, for example, about 1200 to 1400 Gauss at the end face of the N pole facing the photosensitive drum 1 in the fixed magnet body 2A,
Further, when the first magnet body 5A is set to, for example, 800 gauss on the end face of the S pole on the side of the photosensitive drum 1, the magnet body 5A
A magnetic force of about 300 to 400 gauss can be obtained on the surface of the photosensitive drum 1 on A, and 800 to 10 on the sleeve 3.
A magnetic force of 00 Gauss was obtained.

【0020】又第2の磁石体5Bの磁力を第1の磁石体
5Aとほぼ同等に設定する事により感光体ドラム1表面
で300〜400ガウス前後の磁力を得る事が出来、更
に反発磁石体2Bの磁力はその直上位置でのスリーブ3
上で800〜1000ガウスの磁力が得られるように設
定する。即ち第1及び第2の磁石体5A、5Bの感光体
表面磁力は均一帯電と密着性の向上の為に出来る限り大
きくしたほうがよいが、垂直磁場4A上で感光体ドラム
1側から非磁性スリーブ3側への粒子の移動を円滑にす
るために、感光体ドラム1側よりスリーブ3側の磁力を
強くする必要がある。
By setting the magnetic force of the second magnet body 5B to be substantially equal to that of the first magnet body 5A, a magnetic force of about 300 to 400 gauss can be obtained on the surface of the photosensitive drum 1, and the repulsive magnet body can be obtained. The magnetic force of 2B is applied to the sleeve 3 immediately above it.
It is set so that a magnetic force of 800 to 1000 gauss is obtained above. That is, the magnetic force on the surface of the photoconductor of the first and second magnet bodies 5A and 5B should be as large as possible in order to achieve uniform charging and improve the adhesion, but the nonmagnetic sleeve from the side of the photoconductor drum 1 on the vertical magnetic field 4A. In order to facilitate the movement of the particles to the 3 side, it is necessary to make the magnetic force on the sleeve 3 side stronger than on the photosensitive drum 1 side.

【0021】従って限界値は感光体ドラム1表面の夫々
の磁石体の直上位置で、第1の磁石体5Aと第2の磁石
体5Bが、夫々1000ガウス以下、固定磁石体2Aと
反発磁石体2Bが夫々1200ガウス以下に設定するの
がよい。かかる実施例によれば、前記感光体ドラム1上
の水平磁場上で磁性粒子群4B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4A位置まで移動し、こ
こで該垂直磁場4Aにより微粒子群4A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4A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
域上流側に移動する。ここで反発磁石体2Bとの間の反
発磁界による無磁力帯上に磁性粒子群4Cが達すると、
前記非磁性スリーブ3に担持されて磁性粒子群4Cが磁
気的に開放され、感光体ドラム1側に落下し、以下前記
動作を繰り返す。
Therefore, the limit value is the position directly above each magnet body on the surface of the photosensitive drum 1, the first magnet body 5A and the second magnet body 5B are each 1000 gauss or less, the fixed magnet body 2A and the repulsive magnet body. 2B is preferably set to 1200 gauss or less. According to this embodiment, the fine particle group in which the surface of the photosensitive drum 1 is smoothly charged while the magnetic particle group 4B is brought into close contact with the horizontal magnetic field on the photosensitive drum 1 has a vertical magnetic field according to the rotation of the photosensitive drum 1. 4A, where the vertical magnetic field 4A magnetically seals the fine particle group 4A 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 magnetic particle group 4A 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. Here, when the magnetic particle group 4C reaches the non-magnetic band due to the repulsive magnetic field with the repulsive magnet body 2B,
The magnetic particle group 4C carried by the non-magnetic sleeve 3 is magnetically released, drops to the photosensitive drum 1 side, and the above-mentioned operations are repeated.

【0022】従って前記帯電領域上の磁性粒子4は例え
水平磁場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
記実施例を弊社のLEDプリンタ(商品名:エコシス)
に組込んで2万枚印刷して感光体ドラム1の帯電電位の
劣化状態を調べた所、初期印刷時と全く変らない帯電電
位が得られた。
Therefore, the magnetic particles 4 on the charged area are always circulated even if they are in close contact with each other due to the horizontal magnetic field, and there is no room for deterioration of the charged particles even after long-term use. In addition, the above-mentioned embodiment is our LED printer (trade name: ECOSYS)
When 20,000 sheets of paper were incorporated in the above-mentioned printer and the deterioration state of the charging potential of the photosensitive drum 1 was examined, a charging potential which was completely the same as that at the initial printing was obtained.

【0023】図2は前記実施例の変形例で、前記第1の
磁石体の代りにフェライトその他の磁性体5A’を用い
て構成する。かかる構成にてもフェライト5A’と固定
磁石体2Aの間で垂直磁場4Aからなる閉回路が、又感
光体ドラム1側よりスリーブ3側の磁力を強くする事が
出来、更には感光体ドラム1背面側で隣接するフェライ
ト5A’と第2の磁石体5Bの間で水平磁場からなる閉
回路が夫々形成される。
FIG. 2 shows a modification of the above embodiment, in which ferrite or other magnetic material 5A 'is used instead of the first magnet. Even with such a configuration, the closed circuit composed of the vertical magnetic field 4A between the ferrite 5A 'and the fixed magnet body 2A can further strengthen the magnetic force on the sleeve 3 side from the photosensitive drum 1 side, and further, the photosensitive drum 1 A closed circuit composed of a horizontal magnetic field is formed between the ferrite 5A 'and the second magnet body 5B which are adjacent to each other on the back side.

【0024】図3は前記実施例の更に他の変形例で、反
発磁石体2Bを設けずに且つ前記第1の磁石体の代りに
フェライトその他の磁性体5A’を用いて構成すると共
に、帯電領域始端近傍にブレードやフィルム等の粒子剥
離手段9を配置し、スリーブ3に担持されて垂直磁場4
Aより帯電領域上流側に搬送されてきた磁性粒子群4C
を感光体ドラム1側に落下させるように構成する。
FIG. 3 shows another modification of the above-described embodiment, which is constructed without using the repulsive magnet body 2B and using ferrite or other magnetic body 5A 'in place of the first magnet body, and charging A particle peeling means 9 such as a blade or a film is arranged in the vicinity of the starting point of the area, and is supported by the sleeve 3 to support the vertical magnetic field 4
A group of magnetic particles 4C that has been conveyed to the upstream side of the charging area from A
Is dropped to the photosensitive drum 1 side.

【0025】図4は非磁性スリーブ3を用いない本発明
の第2実施例に係る帯電装置を組込んだプリンタで、そ
の構成について説明する。同図(A)において、感光体
ドラム1の周囲に回転方向に沿って本発明の要旨たる帯
電装置20、LEDユニットからなる露光手段40、現
像スリーブ等からなる現像ユニット50、転写ローラ6
0及びクリーニング手段30からなり、前記攪拌手段1
1を介して帯電バイアスが印加された導電性の磁性粒子
群4を感光体ドラム1表面を均一帯電させた後、露光手
段40により潜像を形成して現像ユニット50により現
像させたトナー像を転写ローラ60を介して記録紙70
側に転写し、該未定着トナー像を不図示の定着ローラに
て画像定着し、一方前記転写ローラ60に転写しきれな
かった残留トナーはクリーニングブレード31により除
去し、以下前記動作を繰り返すように構成されている。
そして前記帯電装置20とクリーニング手段は、扇形の
枠体21に一体的に組込まれており、該枠体21のほぼ
中央部を仕切壁21aにより仕切り、感光体ドラム1の
回転方向上流側の仕切空間内に、前記仕切壁21aにク
リーニングブレード31を取り付けて、クリーニング手
段30を構成する。
FIG. 4 shows a printer incorporating a charging device according to the second embodiment of the present invention which does not use the non-magnetic sleeve 3, and its construction will be described. In FIG. 1A, a charging device 20, which is the gist of the present invention, an exposure unit 40 including an LED unit, a developing unit 50 including a developing sleeve, and the like, and a transfer roller 6 around the photosensitive drum 1 along the rotation direction.
0 and a cleaning means 30, and the stirring means 1
After uniformly charging the surface of the photosensitive drum 1 with the conductive magnetic particle group 4 to which the charging bias is applied via 1, the latent image is formed by the exposing means 40 and the toner image developed by the developing unit 50 is formed. Recording paper 70 through transfer roller 60
Side, and the unfixed toner image is fixed by a fixing roller (not shown). On the other hand, the residual toner that could not be transferred to the transfer roller 60 is removed by the cleaning blade 31, and the above operation is repeated. It is configured.
The charging device 20 and the cleaning means are integrally incorporated in a fan-shaped frame body 21, and a substantially central portion of the frame body 21 is partitioned by a partition wall 21a to partition the photosensitive drum 1 on the upstream side in the rotation direction. The cleaning blade 30 is attached to the partition wall 21a in the space to form the cleaning means 30.

【0026】一方帯電装置20は、同図(B)に示すよ
うに前記枠体21の感光体ドラム1回転方向最下流端よ
り感光体ドラム1側に向け、法線方向に延設させて棒状
固定磁石体2Aを配設するとともに、該固定磁石体2A
とほぼ対向させて、第1の磁石体5Aと、該第1の磁石
体5Aに隣接させて帯電領域上流側に第2の磁石体5B
を夫々感光体ドラム1内に配設する。そして前記第1の
磁石体5Aと第2の磁石体5B間の感光体ドラム1上方
の収納空間内に攪拌部材11が矢印方向に回転可能に配
設されている。尚、本実施例においては前記攪拌部材1
1に現像バイアス電源80を接続し、該攪拌部材11を
介して現像バイアスを磁性粒子群4に印加可能に構成し
ている。
On the other hand, as shown in FIG. 1B, the charging device 20 is rod-shaped so as to extend in the normal direction from the most downstream end of the frame 21 in the rotation direction of the photosensitive drum 1 toward the photosensitive drum 1 side. The fixed magnet body 2A is provided and the fixed magnet body 2A is provided.
And a first magnet body 5A, and a second magnet body 5B adjacent to the first magnet body 5A on the upstream side of the charging area.
Are arranged in the photosensitive drum 1, respectively. A stirring member 11 is disposed in the storage space above the photosensitive drum 1 between the first magnet body 5A and the second magnet body 5B so as to be rotatable in the arrow direction. In this embodiment, the stirring member 1
1 is connected to a developing bias power source 80, and a developing bias can be applied to the magnetic particle group 4 via the stirring member 11.

【0027】又前記導電性磁性粒子には平均粒径が35
μm、抵抗率を5×102・Ω・cmのフェライトコア
粒子を用い、5kOe(エールステッド)の磁場での最
大磁化を55〜80emu/g、又1kOeの磁場での
最大磁化を45〜60emu/gに設定する。尚、前記
夫々の磁石体の磁力は前記実施例とほぼ同様に、前記固
定磁石体2A2では感光体ドラム1と対峙するN極の端
面で例えば1000〜1200ガウス前後に、又前記第
1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、前記磁石体5A上の感
光体ドラム1表面で300〜400ガウス前後の磁力を
得る事が出来、又第2の磁石体5Bの磁力を第1の磁石
体5Aとほぼ同等に設定する事により帯電領域の感光体
ドラム1表面で300〜400ガウス前後の磁力を得る
事が出来る。又攪拌部材11は非磁性材で形成され、磁
性粒子群4の循環と水平磁場域での攪拌を容易にするた
めに細径で且つ矢印方向に回転させるのがよい。
The conductive magnetic particles have an average particle size of 35.
The maximum magnetization in a magnetic field of 5 kOe (Oersted) is 55 to 80 emu / g, and the maximum magnetization in a magnetic field of 1 kOe is 45 to 60 emu using ferrite core particles having a resistivity of 5 × 10 2 Ω · cm. / G. The magnetic force of each of the magnet bodies is approximately the same as in the above-described embodiment, in the fixed magnet body 2A2, for example, about 1000 to 1200 gauss at the end face of the N pole facing the photosensitive drum 1, and the first magnet. When the body 5A is set to, for example, 800 gauss on the end surface of the S pole on the photoconductor drum 1 side, a magnetic force of about 300 to 400 gauss can be obtained on the surface of the photoconductor drum 1 on the magnet body 5A. By setting the magnetic force of the magnet body 5B to be substantially equal to that of the first magnet body 5A, a magnetic force of about 300 to 400 gauss can be obtained on the surface of the photosensitive drum 1 in the charging area. The stirring member 11 is made of a non-magnetic material, and it is preferable that the stirring member 11 has a small diameter and is rotated in the direction of the arrow in order to facilitate the circulation of the magnetic particle group 4 and the stirring in the horizontal magnetic field region.

【0028】かかる実施例によれば前記攪拌部材11が
前記感光体ドラム1上の水平磁場上で密着されている磁
性粒子群4Bの攪拌を行ないつつ、その下流側の垂直磁
場4Aで磁気的に封止されている帯電領域内の磁性粒子
群4Aを緩やかに一点鎖線の矢印方向に泳動させ、帯電
領域内での循環及び入替えが可能となる。この場合前記
攪拌部材11の回転は帯電動作中常時行なってもよく、
又非印字時に適宜行なっても良い。
According to this embodiment, the stirring member 11 stirs the magnetic particle group 4B which is in close contact with the horizontal magnetic field on the photosensitive drum 1 while magnetically generating the magnetic field 4A on the downstream side. The magnetic particle groups 4A in the sealed charging area are gently migrated in the direction of the alternate long and short dash line to allow circulation and replacement in the charging area. In this case, the stirring member 11 may be rotated at all times during the charging operation,
Further, it may be appropriately performed at the time of non-printing.

【0029】[0029]

【効果】以上記載のごとく本発明によれば、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、これにより安定した帯電
能とともに磁性粒子の感光体ドラム側への付着洩出を阻
止し得るとともに、帯電領域内で磁性粒子が円滑に循環
且つ攪拌され長期に亙って帯電剤の劣化を阻止し得る。
等の種々の著効を有す。
[Effect] As described above, according to the present invention, without being affected by the fluctuation of the charging gap and the assembly error,
A uniform magnetic field can always be obtained, which can prevent the magnetic particles from adhering and leaking to the photosensitive drum side with stable charging ability, and the magnetic particles can be smoothly circulated and stirred within the charging area for a long time. Therefore, deterioration of the charging agent can be prevented.
It has various remarkable effects.

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

【図1】本発明の第1実施例にかかる帯電装置の全体概
略図(A)とその要部拡大図(B)である。
FIG. 1 is an overall schematic view (A) of a charging device according to a first embodiment of the present invention and an enlarged view (B) of its main part.

【図2】図1の変形例を示す要部拡大図である。FIG. 2 is an enlarged view of a main part showing a modified example of FIG.

【図3】図1の変形例を示す要部拡大図である。FIG. 3 is an enlarged view of an essential part showing a modified example of FIG.

【図4】本発明の第2実施例に係る帯電装置を組込んだ
プリンタの構成を示す全体概略図(A)とその要部拡大
図(B)である。
FIG. 4 is an overall schematic view (A) showing an arrangement of a printer incorporating a charging device according to a second embodiment of the present invention and an enlarged view (B) of a main part 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.

【符号の説明】[Explanation of symbols]

1 感光体ドラム 2A、5A(5A’) 垂直磁場形成手段 3 非磁性スリーブ 4 磁性粒子群 80 帯電バイアス電源 2B、11、9 磁性粒子群の循環若しくは攪拌手段 DESCRIPTION OF SYMBOLS 1 Photosensitive drum 2A, 5A (5A ') Vertical magnetic field forming means 3 Non-magnetic sleeve 4 Magnetic particle group 80 Charging bias power supply 2B, 11, 9 Circulation or stirring means of magnetic particle group

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 (6)

【特許請求の範囲】[Claims] 【請求項1】 感光体と対面する非磁性スリーブ間に磁
性粒子群を担持させ、該粒子群を介して感光体を帯電可
能に構成した帯電装置において、 感光体帯電領域下流側に位置する感光体背面側と非磁性
スリーブ背面側に夫々磁性体若しくは磁石体からなる磁
界発生手段をほぼ対向させて配置し、感光体法線方向に
垂直磁場を形成すると共に、前記非磁性スリーブを感光
体の移動方向に対しアゲインストに回転可能に構成した
事を特徴とする感光体の帯電装置
1. A charging device in which magnetic particles are carried between a non-magnetic sleeve facing a photoconductor and the photoconductor can be charged through the particles, and a photoconductor located downstream of a charging region of the photoconductor. Magnetic field generating means composed of a magnetic body or a magnet body are arranged substantially opposite to each other on the back side of the body and the back side of the non-magnetic sleeve to form a vertical magnetic field in the direction normal to the photoreceptor, and the non-magnetic sleeve is attached to the photoreceptor. Charging device for photoconductor characterized by being configured to be able to rotate against the moving direction
【請求項2】 前記垂直磁場形成位置より感光体移動方
向上流側に磁性粒子群を循環若しくは攪拌させる手段を
設け、前記垂直磁場により磁気封止された磁性粒子群が
帯電領域内を循環若しくは攪拌可能に構成した請求項1
記載の感光体の帯電装置
2. A means for circulating or stirring magnetic particle groups upstream of the vertical magnetic field forming position in the moving direction of the photosensitive member, wherein magnetic particle groups magnetically sealed by the vertical magnetic field circulate or stir in a charging region. Claim 1 constituted as possible
Charging device for photoreceptor
【請求項3】 前記循環手段が前記帯電域上流側の非磁
性スリーブ上に形成された磁気的開放手段である請求項
2記載の感光体の帯電装置
3. A charging device for a photosensitive member according to claim 2, wherein the circulating means is a magnetic opening means formed on a non-magnetic sleeve on the upstream side of the charging area.
【請求項4】 前記循環手段が、非磁性スリーブ上に担
持された磁性粒子群を、前記帯電域上流側で機械的に剥
離させる剥離手段である請求項2記載の帯電装置
4. The charging device according to claim 2, wherein the circulation means is a peeling means for mechanically peeling the magnetic particle group carried on the non-magnetic sleeve on the upstream side of the charging area.
【請求項5】 前記垂直磁場上におけるスリーブ表面磁
力が感光体表面磁力より大になるように前記磁石体の磁
力密度を設定した請求項1記載の帯電装置。
5. The charging device according to claim 1, wherein the magnetic force density of the magnet body is set so that the magnetic force on the surface of the sleeve on the vertical magnetic field is larger than the magnetic force on the surface of the photoconductor.
【請求項6】 感光体表面と摺擦する磁性粒子群を介し
て感光体を帯電可能に構成した帯電装置において、 感光体帯電領域下流側に、感光体を挟んでその背面側と
表面側に夫々磁性体若しくは磁石体からなる磁界発生手
段をほぼ対向配置し、感光体法線方向に垂直磁場を形成
し、 一方感光体帯電領域上流側に、前記磁性粒子群の循環手
段を配し、該循環手段と垂直磁場形成位置間で帯電域に
位置する磁性粒子群を循環可能に構成した事を特徴とす
る感光体の帯電装置
6. A charging device configured to charge a photoconductor through a group of magnetic particles that rub against the surface of the photoconductor. The photoconductor charging area has a downstream side, and a back side and a front side thereof sandwiching the photoconductor. Magnetic field generating means composed of a magnetic body or a magnet body are arranged substantially opposite to each other to form a vertical magnetic field in the normal direction of the photoconductor, and on the other hand, circulation means for the magnetic particle group is arranged on the upstream side of the photoconductor charging area, A charging device for a photoconductor, characterized in that a group of magnetic particles located in a charging region can be circulated between a circulation means and a position for forming a vertical magnetic field.
JP05232308A 1993-05-20 1993-08-25 Photoconductor charging device Expired - Fee Related JP3087934B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP05232308A JP3087934B2 (en) 1993-05-20 1993-08-25 Photoconductor charging device
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
JP5-139831 1993-05-20
JP13983193 1993-05-20
JP05232308A JP3087934B2 (en) 1993-05-20 1993-08-25 Photoconductor charging device

Publications (2)

Publication Number Publication Date
JPH0736252A true JPH0736252A (en) 1995-02-07
JP3087934B2 JP3087934B2 (en) 2000-09-18

Family

ID=26472529

Family Applications (1)

Application Number Title Priority Date Filing Date
JP05232308A Expired - Fee Related JP3087934B2 (en) 1993-05-20 1993-08-25 Photoconductor charging device

Country Status (1)

Country Link
JP (1) JP3087934B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP4368702B2 (en) 2004-03-11 2009-11-18 株式会社リコー Charging device, process cartridge, image forming apparatus

Also Published As

Publication number Publication date
JP3087934B2 (en) 2000-09-18

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