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JP3087936B2 - Charging device - Google Patents
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JP3087936B2 - Charging device - Google Patents

Charging device

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Publication number
JP3087936B2
JP3087936B2 JP05239040A JP23904093A JP3087936B2 JP 3087936 B2 JP3087936 B2 JP 3087936B2 JP 05239040 A JP05239040 A JP 05239040A JP 23904093 A JP23904093 A JP 23904093A JP 3087936 B2 JP3087936 B2 JP 3087936B2
Authority
JP
Japan
Prior art keywords
magnet body
magnetic
magnet
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
JP05239040A
Other languages
Japanese (ja)
Other versions
JPH0736255A (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 JP05239040A priority Critical patent/JP3087936B2/en
Priority to US08/245,281 priority patent/US5596394A/en
Publication of JPH0736255A publication Critical patent/JPH0736255A/en
Application granted granted Critical
Publication of JP3087936B2 publication Critical patent/JP3087936B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

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  • Electrostatic Charge, Transfer And Separation In Electrography (AREA)

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, 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) via 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 voltage of several hundred volts is applied to a conductive roller to contact and charge a photosensitive drum. 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4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。
In such a charging method, when a magnetic spike 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. The magnetic coercive force of the magnetic particles located is the weakest. On the other hand, the magnetic particle group 104 slidably rubs between particles or with the photosensitive drum 1 in the charged area, and is charged to have a charge. Therefore, when the photosensitive drum 101 is rotated in this state, a centrifugal force acts on the drum surface, and the magnetic particles 4 electrostatically adhered to the photosensitive drum 101 cause the magnetic coercive force ( magnetic field)
A force acts in the direction away from the magnetic chain, that is, the charged region, and the particles 104a attached to the photosensitive drum adversely affect the exposure and development in the next step.

【0007】又、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、磁性粒子の漏洩のみなら
ず飛散が一層増大する。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105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10
5に付着した磁性粒子104aを回収する機構が必要に
なり、構成が煩雑化する。
There is also a method of rotating the magnet assembly. However, such a method requires a complicated drive system structure,
Since the magnetic pole moves at high speed, not only leakage but also scattering of magnetic particles is further increased. For this reason, the prior art is configured to collect the magnetic particles by arranging the blade 105 on the downstream side of the charging area in the photoconductor moving direction. The blade 10
A mechanism for collecting the magnetic particles 104a attached to the surface 5 is required, and the configuration becomes complicated.

【0008】本発明はかかる従来技術の欠点に鑑み、簡
単な構成で帯電領域外への磁性粒子の洩出及び飛散を有
効に阻止し得、更には感光体ドラムの小型化を図った場
合にも更には帯電スリーブ等の組立誤差等が生じても安
定して帯電が可能な帯電装置を提供する事を目的とす
る。
In view of the drawbacks of the prior art, the present invention can effectively prevent the magnetic particles from leaking and scattering outside the charged area with a simple structure, and can further reduce the size of the photosensitive drum. Still another object of the present invention is to provide a charging device capable of stably charging even if an assembly error of a charging sleeve or the like occurs.

【0009】[0009]

【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
の帯電装置に関するもので、その第一の特徴とする所
は、感光体背面側に一又は複数の磁石体(以下第1の磁
石体という)を配置し、該磁石体若しくは他の磁石体と
の協動作用により感光体表面の帯電領域上に磁性粒子群
を磁気的に担持させる点にある。即ち、より具体的には
後記実施例に示すように、感光体の背面側に逆極性の複
数の磁極を配して水平磁場を形成し、該水平磁場により
感光体表面上に磁性粒子を密着させて帯電させてもよ
く、又感光体を挟んで感光体の背面側と両面側に逆極性
の複数の磁極を配して磁場を形成し、該磁場により感光
体表面上に磁性粒子を担持させて帯電させてもよいが、
いずれにしても感光体背面側に少なくとも一の磁極が存
在することが前提となる。
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. The first feature of the apparatus is that one or a plurality of magnets (hereinafter, referred to as a first magnet) are arranged on the back side of the photoreceptor and cooperate with the magnet or another magnet. The point is that the magnetic particles are magnetically supported on the charged area on the surface of the photoreceptor by operation. That is, more specifically, as shown in the examples described later, a plurality of magnetic poles having opposite polarities are arranged on the back side of the photoreceptor to form a horizontal magnetic field, and the horizontal magnetic field adheres the magnetic particles on the surface of the photoreceptor. The magnetic field may be formed by arranging a plurality of magnetic poles having opposite polarities on the back side and both sides of the photoconductor with the photoconductor interposed therebetween, and the magnetic field carries the magnetic particles on the photoconductor surface. May be charged,
In any case, it is assumed that at least one magnetic pole exists on the back surface of the photoconductor.

【0010】この結果、磁性粒子の磁気保持を行なう磁
石体が感光体表面上の帯電スリーブ内にのみ配置されて
いるのではなく、感光体の背面側に配置されている為
に、従来技術に比較して感光体表面上の帯電領域の磁場
を強くすることが出来、これにより帯電領域上の磁性粒
子の飛散等を防止できると共に、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
リーブの偏心等を考慮する事なく、安定した磁性粒子群
の磁気保持力を維持できる。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。又感光体ドラムを小径化した場合においても有
効に帯電磁場を確保できる。
As a result, the magnet body for holding the magnetic particles magnetically is arranged not only in the charging sleeve on the surface of the photoreceptor but on the back side of the photoreceptor. By comparison, the magnetic field of the charged area on the photoreceptor surface can be increased, thereby preventing the scattering of magnetic particles on the charged area and the like.As a result, even if there is some assembly error of the charging gap, etc. Even if the gap tolerance is set large, it is possible to maintain a stable magnetic coercive force of the magnetic particles without considering the eccentricity of the photosensitive drum 1 and the non-magnetic sleeve. The fact that the assembly tolerance and the eccentricity can be set roughly leads to a reduction in the number of assembly steps and manufacturing costs. Even when the diameter of the photosensitive drum is reduced, a charging magnetic field can be effectively secured.

【0011】そして本発明の第二の特徴とするところ
は、感光体移動方向下流側の感光体背面側若しくは表面
上に前記磁石体と同極性の第2の磁石体を形成し、該第
2の磁石体と、前記第1の磁石体の内、感光体帯電領域
下流側に位置する一の磁石体間により形成される反発磁
界を利用して帯電領域下端側で磁性粒子群の磁気シール
ドを図った事にある。即ち、具体的には感光体帯電領域
下流側に位置する磁石体と隣接させて、感光体背面側に
前記第2の磁石体を配設してもよく、又感光体帯電領域
下流側に位置する磁石体と感光体を挟んでほぼ対向する
ごとく感光体の表面側に感光体移動方向と直交する方向
に延在させて、前記第2の磁石体を配設してもよい。
A second feature of the present invention is that a second magnet body having the same polarity as the magnet body is formed on the back surface or the surface of the photosensitive body downstream in the movement direction of the photosensitive body. And a magnetic shield of a group of magnetic particles at the lower end side of the charged area using a repulsive magnetic field formed between the magnet body of the first magnet body and one of the first magnet bodies located on the downstream side of the photoconductor charged area. I have done it. That is, specifically, the second magnet body may be provided on the back side of the photoconductor adjacent to the magnet body located on the downstream side of the photoconductor charging area, or may be provided on the downstream side of the photoconductor charging area. The second magnet body may be provided so as to extend in a direction orthogonal to the photosensitive body moving direction on the surface side of the photosensitive body so as to be substantially opposed to the magnet body to be sandwiched by the photosensitive body.

【0012】これにより一対の同極性の隣接磁極からな
る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、該無磁力帯により感光体ドラム側への磁性粒
子の漏洩を阻止し帯電領域側に粒子を維持することが可
能であるために、ブレード等を用いなくても帯電領域か
らの洩出を有効に阻止し得る。この場合好ましくは、感
光体背面側の帯電領域下流側に第1の磁石体、該第1の
磁石体と対向する非磁性スリーブ背面側に第1の磁石体
と逆極性の第3の磁石体、感光体移動方向下流側の感光
体背面側若しくは表面上に前記第1の磁石体と同極性の
第2の磁石体を夫々配設すると共に、前記第1の磁石体
の感光体表面上の磁力密度より、前記第2の磁石体の磁
力密度を大に設定する。この結果、前記反発磁界により
感光体上の帯電領域下流端に形成した無磁力帯により感
光体ドラム表面上で帯電領域外への洩出を阻止された磁
性粒子は磁力差により第2の磁石体側、即ち非磁性スリ
ーブ側に向い、帯電領域内での循環が可能となる。この
場合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することにより、磁性粒子群
を帯電域上流側へ循環させることが一層容易に行われ
る。
Thus, a repulsive magnetic field consisting of a pair of adjacent magnetic poles having the same polarity forms a non-magnetic force band at the downstream end of the charged area on the photoreceptor, and the non-magnetic force band prevents leakage of magnetic particles to the photoreceptor drum. In addition, since particles can be maintained on the charged area side, leakage from the charged area can be effectively prevented without using a blade or the like. In this case, preferably, a first magnet body is provided on the downstream side of the charged area on the back side of the photoconductor, and a third magnet body having a polarity opposite to that of the first magnet body is provided on the back side of the non-magnetic sleeve opposed to the first magnet body. A second magnet body having the same polarity as that of the first magnet body is disposed on the back surface or the surface of the photosensitive body on the downstream side in the movement direction of the photosensitive body, and the second magnet body is disposed on the surface of the photosensitive body of the first magnet body. The magnetic force density of the second magnet body is set higher than the magnetic force density. As a result, the magnetic particles that have been prevented from leaking out of the charged area on the surface of the photoreceptor drum by the non-magnetic force band formed at the downstream end of the charged area on the photoreceptor due to the repulsive magnetic field are caused by the magnetic force difference. That is, it is possible to circulate in the charging region toward the non-magnetic sleeve. In this case, by arranging the non-magnetic sleeve so as to be rotatable against the moving direction of the photoconductor, it is easier to circulate the magnetic particles to the upstream side of the charging area.

【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
(A)(B)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)を介して帯電領域位置で前記感光体
ドラム1と互いに反対方向、即ちアゲインスト方向(図
上左方向、尚回転軸から見た場合はいずれも同一回転方
向となる。)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磁石集成体2内に固定磁石体2Aを
配設して構成する。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。
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 (A) and (B). As described above, the charging device is opposite to the photosensitive drum 1 at the charging area position via the charging gap (0.5 mm) with respect to the photosensitive drum 1 rotating rightward in the drawing, that is, in the opposite direction (see FIG. The non-magnetic sleeve 3 is rotatably provided in the upper left direction, and when viewed from the rotation axis, the rotation direction is the same. In addition, the non-magnetic sleeve 3 is fixed and disposed on the back side of the non-magnetic sleeve 3 downstream of the charging area. The fixed magnet body 2A is disposed in the magnet assembly 2 thus formed. Reference numeral 8 denotes a bias power supply for applying a developing bias to the conductive magnetic particle group 4 via a conductive blade or a non-magnetic sleeve 3 (not shown).

【0014】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水平磁場形成用磁石体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、水平磁場形成用磁石体
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。
On the other hand, on the back side of the photosensitive drum 1, a first magnet body 5A is substantially opposed to the fixed magnet body 2A located on the downstream side of the charging area, and is adjacent to the first magnet body 5A. The horizontal magnetic field forming magnet 5B is disposed adjacent to the charging area upstream side, the first magnet 5A is set to the S pole having the opposite polarity to the fixed magnet 2A, and the horizontal magnetic field forming magnet 5B is The first magnetic body 5A is set to have an N pole having a polarity opposite to that of the first magnet body 5A, and a horizontal magnetic field is formed on the photosensitive drum 1 between the two magnet bodies 5A and 5B.

【0015】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
に垂直磁場6Aにより前記磁性粒子群4を磁気保持さ
せ、又水平磁場形成用磁石体5Bは前記第1の磁石体5
A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と水平磁場形成用磁石体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4を感光体ドラ
ム1上に密着させる。
That is, specifically, the first opposedly arranged first
5A and the fixed magnet 2 are disposed downstream of the charged area in the rotation direction of the photosensitive drum 1, and the magnetic particles 4 are magnetically held by a vertical magnetic field 6A between the two magnets 2A and 5A. The forming magnet body 5B is the first magnet body 5
A, and the magnetic particle group 4 is closely attached to the photosensitive drum 1 by a horizontal magnetic field mainly formed between the first magnet body 5A and the horizontal magnetic field forming magnet body 5B. Let it.

【0016】又前記非磁性スリーブ3と感光体ドラム1
間の帯電領域上には導電性磁性粒子群4を介在させると
ともに、又現像領域下流端より僅かに感光体ドラム1移
動方向下流側の空域に前記固定磁石体2A及び第1の磁
石体5Aと対向する位置に円棒状の若しくは略台形状の
S極の磁石体5Cを配設する。
The non-magnetic sleeve 3 and the photosensitive drum 1
The conductive magnet particles 4 are interposed on the charged area between the fixed magnet body 2A and the first magnet body 5A in an air space slightly downstream of the downstream end of the developing area in the moving direction of the photosensitive drum 1. An S-pole or substantially trapezoidal S-pole magnet body 5C is disposed at an opposing position.

【0017】前記磁性粒子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。
The magnetic particles 4 are not particularly limited as long as they are conductive. However, the magnetic particles 4 may be made of conductive magnetic particles coated with a conductive resin on the surface of a magnetic core such as ferrite, iron powder, magnetite or the like. Mixed particle group 4 of magnetic particles
May be configured. For example, a mixture of 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 used. In this example, the average particle diameter was 20 to 35 μm, and the resistivity was 10 3 to 10 μm.
Use is made of ferrite core particles of 10 6 Ω · cm with magnetic properties set to 60 to 70 emu / g (1 k Oe).

【0018】又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と対峙するスリーブ3上で
800〜1000ガウスの磁力が得られ、又前記第1の
磁石体5Aは、該磁石体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るよう
に磁力密度を設定し、又水平磁場形成用磁石体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、更に前記S極の磁石体5Cは前記第1の
磁石体5Aの感光体ドラム表面上の磁力密度より大なる
磁力密度、例えば600〜800ガウス程度に設定す
る。
The magnetic force of each of the magnet bodies is 800 to 1000 gauss on the sleeve 3 facing the photosensitive drum 1 in the fixed magnet body 2A, and the first magnet body 5A is The magnetic force density is set so that a magnetic force of about 300 to 400 Gauss can be obtained on the surface of the photosensitive drum 1 on the magnet body 5A, and the magnetic force of the horizontal magnetic field forming magnet body 5B is set to be equal to that of the first magnet body 5A. By setting them substantially equal, a magnetic force of about 300 to 400 gauss can be obtained on the surface of the photosensitive drum 1, and the magnetic body 5C of the S pole has a magnetic force on the photosensitive drum surface of the first magnet 5A. The magnetic force density is set higher than the density, for example, about 600 to 800 Gauss.

【0019】尚、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6A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。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
と水平磁場形成用磁石体5Bが、夫々1000ガウス以
下、固定磁石体2Aのスリーブ上での磁力密度と反発磁
石体2Bが夫々1200ガウス以下に設定するのがよ
い。
Although the surface magnetic force of the photoreceptor of the first and second magnet bodies 5A and 5B should be as large as possible for uniform charging and improvement of adhesion, the photoreceptor drum 1 side on a vertical magnetic field 6A is preferable. In order to smoothly move particles from the photosensitive drum 1 to the non-magnetic sleeve 3 side, it is necessary to increase the magnetic force on the sleeve 3 side with respect to the photosensitive drum 1 side. Therefore, the limit value is the position just above each magnet body on the surface of the photosensitive drum 1 and the first magnet body 5A
And the horizontal magnetic field forming magnet 5B are preferably set to 1000 gauss or less, and the magnetic force density on the sleeve of the fixed magnet 2A and the repulsion magnet 2B are preferably set to 1200 gauss or less.

【0020】又S極の磁石体5Cは、前記第1の磁石体
とS極の磁石体5C間で形成された反発磁界により帯電
領域外への移動が阻止された磁界粒子が固定磁石体2A
側に円滑に吸着可能に構成するために、前記S極の磁石
体5Cは前記第1の磁石体5Aの感光体ドラム1表面上
の磁力密度より大なる磁力密度に設定するのがよい。
The S-pole magnet body 5C is composed of a fixed magnet body 2A that is prevented from moving outside the charged area by the repulsive magnetic field formed between the first magnet body and the S-pole magnet body 5C.
In order to make it possible to smoothly attract to the side, the magnetic body 5C of the S pole is preferably set to a magnetic force density larger than the magnetic force density on the surface of the photosensitive drum 1 of the first magnet body 5A.

【0021】かかる実施例によれば、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上で感光体ドラムへの帯電
を行ないながら該垂直磁場6Bから垂直磁場6B上に移
動し、更に磁性粒子群4はS極の磁石体5Cとの間の反
発磁界で感光体ドラム1上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6B
により垂直方向に逃げる。
According to this embodiment, the magnetic particle group 4 adhered to the charged area is composed of both N-pole and S-pole magnet bodies 5A,
On the vertical magnetic field 6B downstream from the horizontal magnetic field 6A on the charged area, which adheres closely to the photosensitive drum on the horizontal magnetic field 6A between 5B, and coarsely in the normal direction of the photosensitive drum 1 It is attached to stand. In this state, the photosensitive drum 1
Rotates, the photosensitive drum is charged on the horizontal magnetic field 6A while moving from the vertical magnetic field 6B to the vertical magnetic field 6B, and the magnetic particles 4 are repelled by the repulsive magnetic field between the S magnetic pole and the magnet body 5C. The vertical magnetic field 6B is not transferred to the downstream side by the non-magnetic force zone 6D formed by the photosensitive drum 1.
Escapes in the vertical direction.

【0022】そして垂直方向に向った磁性粒子群4は、
今度は逆にS極の磁石体5Cと固定磁石体との吸引力に
よりスリーブ3側に付着し、その後スリーブ3の回転に
従って帯電領域上流側の水平磁場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4が漏洩することなく円滑な
帯電が行なわれる。
The magnetic particle group 4 oriented in the vertical direction is
This time, on the contrary, the magnetic field adheres to the sleeve 3 side by the attractive force of the S-pole magnet body 5C and the fixed magnet body, and thereafter, is returned to the horizontal magnetic field 6A side on the upstream side of the charging area according to the rotation of the sleeve 3, and thereafter the circulation is repeated. Do. Therefore, according to this embodiment, the smooth charging is performed without the magnetic particles 4 leaking to the downstream side of the charging area.

【0023】尚、前記S極の磁石体5Cは図2に示すよ
うに現像するスリーブ3背面側に配置してもよい。そし
て本実施例においては、特に本図及び図1(A)に示す
ように固定磁石体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。そして固定磁石体2A
と同極性のN極に設定した前記反発磁石体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側に落下し、磁性粒子の循環と漏洩
阻止が一層円滑に行なわれる。
The S-pole magnet body 5C may be arranged on the back side of the developing sleeve 3, as shown in FIG. In this embodiment, as shown in FIG. 1 and FIG. 1A, repulsion having the same polarity as the fixed magnet body 2A is provided in the upstream direction of the charging area of the fixed magnet body 2A, in other words, in the downstream side of the sleeve rotation direction. The magnet body 2B is provided. And the fixed magnet body 2A
The repulsion magnet body 2B, which is set to have the same polarity as the N pole, is laid out such that the non-magnetic force zone due to the repulsion magnetic field formed between the two is located on the upstream side of the charging area, and is thereby carried on the non-magnetic sleeve 3. Then, the magnetic particles 4C conveyed to the upstream side of the charging area from the position of the vertical magnetic field 4A are magnetically released, fall to the photosensitive drum 1 side, and the circulation and leakage prevention of the magnetic particles are performed more smoothly.

【0024】図3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極の水平磁場形成用磁石体5B及び下流側に逆極性
のS極の第1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1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1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。
FIG. 3 shows an embodiment in which the charging sleeve and the fixed magnet assembly are not arranged on the photosensitive drum but opposed to each other, and are arranged only on the rear surface 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 region, an N-pole horizontal magnetic field forming magnet body 5B and a downstream are arranged on the upstream side so as to substantially divide the charged region into two. The first magnet body 5A of the S pole having the opposite polarity is disposed adjacent to the first 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 first 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 first magnet body 5A and having the S pole is arranged. 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.

【0025】そして前記磁性粒子の漏洩を一層円滑に阻
止するために、前記無磁力帯入口端の感光体ドラム1上
に自由端側が接するごとく非磁性導電性薄膜7aを導電
性支持部材7bより感光体ドラム法線方向に垂下させ、
更に前記支持部材7bを介してバイアス電源8を接続す
る。図4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極の第1及び第2
の磁石体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1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、5
C間に無磁力帯域6Dが形成される。この結果水平磁場
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6Bにより垂直方
向に移動するが、前記薄膜7aによりバイアス電源8が
印加されつつその漏洩が更に機械的に阻止されながらり
前記磁性粒子の循環が円滑に行なわれる。
In order to more smoothly prevent the leakage of the magnetic particles, the non-magnetic conductive thin film 7a is exposed from the conductive support member 7b so that the free end side contacts the photosensitive drum 1 at the entrance end of the non-magnetic force zone. Droop in the body drum normal direction,
Further, a bias power source 8 is connected via the support member 7b. FIG. 4 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 FIG. 4, a vertical magnetic field 6B is formed immediately above each magnetic pole, and N Pole and S pole first and second
A strong horizontal magnetic field 6A between the magnet bodies 5A and 5B
A repulsive magnetic field 6C, in which two horizontal magnetic fields 6A are separated, is formed between the first pole 5A and the repulsive magnet 5C of the S pole on the lower end side of the charged area, and as a result, the two magnetic poles 5A, 5A
A nonmagnetic zone 6D is formed between C. As a result, the magnetic field moves from the horizontal magnetic field 6A to the vertical magnetic field 6B, and the magnetic particles move in the vertical direction by the vertical magnetic field 6B without being transported downstream by the non-magnetic force zone 6D formed by the repulsive magnet 5C. However, while the bias power 8 is applied by the thin film 7a, the leakage is further mechanically prevented, and the circulation of the magnetic particles is smoothly performed.

【0026】[0026]

【効果】以上記載のごとく本発明によれば、複数の磁極
の対向配置という簡単な構成で帯電領域外への磁性粒子
の洩出阻止及び帯電領域内の循環を円滑に達成し得る。
更に本発明は感光体ドラムの小型化を図った場合にも更
には帯電スリーブ等の組立誤差等が生じても安定して帯
電が可能となる。等の種々の著効を有す。
As described above, according to the present invention, it is possible to smoothly prevent magnetic particles from leaking out of the charged area and smoothly circulate in the charged area with a simple configuration in which a plurality of magnetic poles are opposed to each other.
Further, according to the present invention, even when the size of the photosensitive drum is reduced, charging can be stably performed even if an assembly error of the charging sleeve or the like occurs. And so on.

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

【図1】本発明の第1実施例にかかる帯電装置の概略図
で、印字状態(A)と非印字状態(B)を夫々示す。
FIG. 1 is a schematic view of a charging device according to a first embodiment of the present invention, showing a printing state (A) and a non-printing state (B), respectively.

【図2】図1の変形例を示す概略図である。FIG. 2 is a schematic diagram showing a modification of FIG.

【図3】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. 3 is a schematic diagram showing an embodiment of the present invention in which a magnet body is arranged only on the back side of the photosensitive drum.

【図4】図3の磁力線の作用図である。FIG. 4 is an operation diagram of the magnetic field lines of FIG. 3;

【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 2A 固定磁石体(第3の磁石体) 5A 第1の磁石体 5C S極の磁石体(第2の磁石体) 5B 水平磁場形成用磁石体 4 導電性磁性粒子群 Reference Signs List 1 photoconductor drum 2A fixed magnet body (third magnet body) 5A first magnet body 5C S pole magnet body (second magnet body) 5B horizontal magnetic field forming magnet body 4 conductive magnetic particle group

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) 特開 昭59−228675(JP,A) (58)調査した分野(Int.Cl.7,DB名) G03G 15/02 101 G03G 15/09 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) JP-A Sho-59 -228675 (JP, A) (58) Fields investigated (Int. Cl. 7 , DB name) G03G 15/02 101 G03G 15/09

Claims (6)

(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、 感光体背面側に一又は複数の磁石体(以下第1の磁石体
という)を配置し、該磁石体若しくは他の磁石体との協
動作用により感光体表面の帯電領域上に磁性粒子群を磁
気的に担持させると共に、感光体移動方向下流側の感光
体背面側若しくは表面上に前記磁石体と同極性の第2の
磁石体を形成し、該第2の磁石体と、前記第1の磁石体
の内、感光体帯電領域下流側に位置する一の磁石体間に
より形成される反発磁界を利用して帯電領域下端側で磁
性粒子群の磁気シールドを図った事を特徴とする帯電装
1. A charging device for a photoreceptor configured to be capable of charging a photoreceptor via a group of magnetic particles held on a charging area of the photoreceptor by a magnetic force, wherein one or a plurality of magnets are provided on the back side of the photoreceptor. (Hereinafter, referred to as a first magnet body), magnetic particles are magnetically supported on a charged area on the surface of the photoconductor by cooperating with the magnet body or another magnet body, and the moving direction of the photoconductor is changed. A second magnet body having the same polarity as the magnet body is formed on the back surface or the surface of the downstream photosensitive body, and the second magnet body and the first magnet body, and the downstream side of the photosensitive body charging area. A charging device characterized by using a repulsive magnetic field formed by a single magnet body positioned at the lower end to magnetically shield a group of magnetic particles at the lower end of the charging area.
【請求項2】 感光体帯電領域下流側に位置する磁石体
と隣接させて、感光体背面側に前記第2の磁石体を配設
した事を特徴とする請求項1記載の帯電装置
2. The charging device according to claim 1, wherein the second magnet is disposed on the back side of the photoconductor adjacent to a magnet located downstream of the photoconductor charging area.
【請求項3】 感光体帯電領域下流側に位置する磁石体
と感光体を挟んでほぼ対向するごとく感光体の表面側に
感光体移動方向と直交する方向に延在させて、前記第2
の磁石体を配設した事を特徴とする請求項1記載の帯電
装置
A second magnet extending in a direction orthogonal to a moving direction of the photosensitive member on a surface of the photosensitive member so as to be substantially opposed to the magnet member located on the downstream side of the photosensitive member charging area with the photosensitive member interposed therebetween;
The charging device according to claim 1, wherein the magnet body is disposed.
【請求項4】 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、 感光体背面側の帯電領域下流側に第1の磁石体、該第1
の磁石体と対向する非磁性スリーブ背面側に第1の磁石
体と逆極性の第3の磁石体、帯電領域を僅かに外れた感
光体移動方向下流側に前記第1の磁石体と同極性の第2
の磁石体を夫々配設した事を特徴とする帯電装置
4. A charging device in which a magnetic particle group is carried between a non-magnetic sleeve facing a photoreceptor and the photoreceptor can be charged via the particle group. A first magnet body, the first magnet body;
A third magnet body having a polarity opposite to that of the first magnet body on the back side of the non-magnetic sleeve opposite to the magnet body, and a same polarity as the first magnet body on the downstream side in the photoconductor moving direction slightly out of the charged area. Second
Charging device characterized in that each magnet body is disposed.
【請求項5】 前記第1の磁石体の感光体表面上の磁力
密度より、前記第2の磁石体の磁力密度を大に設定した
事を特徴とする請求項4記載の帯電装置
5. The charging device according to claim 4, wherein the magnetic force density of the second magnet body is set to be larger than the magnetic force density of the first magnet body on the photoreceptor surface.
【請求項6】 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
る請求項4記載の帯電装置
6. The charging device according to claim 4, wherein said non-magnetic sleeve is configured to be rotatable against the moving direction of the photosensitive member.
JP05239040A 1993-05-20 1993-08-31 Charging device Expired - Fee Related JP3087936B2 (en)

Priority Applications (2)

Application Number Priority Date Filing Date Title
JP05239040A JP3087936B2 (en) 1993-05-20 1993-08-31 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
JP13983193 1993-05-20
JP5-139831 1993-05-20
JP05239040A JP3087936B2 (en) 1993-05-20 1993-08-31 Charging device

Publications (2)

Publication Number Publication Date
JPH0736255A JPH0736255A (en) 1995-02-07
JP3087936B2 true JP3087936B2 (en) 2000-09-18

Family

ID=26472532

Family Applications (1)

Application Number Title Priority Date Filing Date
JP05239040A Expired - Fee Related JP3087936B2 (en) 1993-05-20 1993-08-31 Charging device

Country Status (1)

Country Link
JP (1) JP3087936B2 (en)

Also Published As

Publication number Publication date
JPH0736255A (en) 1995-02-07

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