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JPS6339055B2 - - Google Patents
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JPS6339055B2 - - Google Patents

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Publication number
JPS6339055B2
JPS6339055B2 JP5884580A JP5884580A JPS6339055B2 JP S6339055 B2 JPS6339055 B2 JP S6339055B2 JP 5884580 A JP5884580 A JP 5884580A JP 5884580 A JP5884580 A JP 5884580A JP S6339055 B2 JPS6339055 B2 JP S6339055B2
Authority
JP
Japan
Prior art keywords
toner
developer
latent image
magnetic
developing
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
Application number
JP5884580A
Other languages
Japanese (ja)
Other versions
JPS56154771A (en
Inventor
Nobuo Tsukada
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.)
Canon Inc
Original Assignee
Canon Inc
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 Canon Inc filed Critical Canon Inc
Priority to JP5884580A priority Critical patent/JPS56154771A/en
Publication of JPS56154771A publication Critical patent/JPS56154771A/en
Publication of JPS6339055B2 publication Critical patent/JPS6339055B2/ja
Granted legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G15/00Apparatus for electrographic processes using a charge pattern
    • G03G15/06Apparatus for electrographic processes using a charge pattern for developing
    • G03G15/08Apparatus for electrographic processes using a charge pattern for developing using a solid developer, e.g. powder developer
    • G03G15/09Apparatus for electrographic processes using a charge pattern for developing using a solid developer, e.g. powder developer using magnetic brush

Landscapes

  • Physics & Mathematics (AREA)
  • General Physics & Mathematics (AREA)
  • Magnetic Brush Developing In Electrophotography (AREA)

Description

【発明の詳細な説明】 一成分系現像方法に属する所謂ジヤンピング現
像法として、シート等の担持体にトナーを均一に
塗布した後、これを静電像保持面に小間隙を保つ
て対向させ、静電像の有する電荷によりトナーを
その担持体から静電像保持面に吸引し付着させて
現像する方法が知られている(特公昭41−9475号
公報、米国特許第2839400号明細書等)。この方法
は、静電荷のない非画像部には、トナーが吸引さ
れないばかりか、トナーと非画像部とが接触しな
いので、他の一成分系現像方法に比べて地カブリ
が出にくいという長所を有している。
DETAILED DESCRIPTION OF THE INVENTION As a so-called jumping development method belonging to one-component development method, toner is uniformly applied to a carrier such as a sheet, and then the toner is opposed to an electrostatic image holding surface with a small gap maintained. A method is known in which toner is attracted from the carrier to the electrostatic image holding surface by the electric charge of the electrostatic image and developed (Japanese Patent Publication No. 41-9475, U.S. Pat. No. 2,839,400, etc.). . This method has the advantage that not only toner is not attracted to the non-image area where there is no static charge, but also there is no contact between the toner and the non-image area, so background fog is less likely to occur compared to other one-component developing methods. have.

しかしながらこの方法は次に述べる欠点のため
に未だ実用化された事がない。その理由のひとつ
は支持体にトナーを均一に塗布することが困難で
ある。均一に塗布するために剛体が弾性体ブレー
ドを用いる方法があるが、液体を塗布する場合と
異なり塗布ムラが生じやすい。
However, this method has not yet been put into practical use due to the following drawbacks. One of the reasons for this is that it is difficult to uniformly apply toner to the support. There is a method of using a rigid and elastic blade to uniformly apply the coating, but unlike the case of applying a liquid, uneven coating is likely to occur.

また比較的均一に塗布された場合でも、現像工
程においてトナー担持体からの均一なトナー離脱
が困難であつた。さらにトナーの離脱の際トナー
の持つお互いの反発する電荷により潜像面との距
離が広がると現像された画像には乱れが生じやす
かつた。
Furthermore, even when the toner is applied relatively uniformly, it is difficult to uniformly separate the toner from the toner carrier during the development process. Furthermore, when the toner is separated from the toner and the distance from the latent image surface increases due to the mutually repelling charges of the toner, the developed image tends to be disturbed.

本出願人はかかる欠点を除去し忠実性が高く画
質の安定した静電像現像装置を提供した(例えば
特開昭52−43037号、同55−18659号等)。
The present applicant has provided an electrostatic image developing device which eliminates such drawbacks and exhibits high fidelity and stable image quality (for example, Japanese Patent Application Laid-open Nos. 52-43037 and 55-18659).

これらの発明は次を目的としている。 These inventions are aimed at:

(1) 均一なトナー層を簡便な装置によつて得る。(1) Obtain a uniform toner layer using a simple device.

(2) きわめて薄く且つ層厚の均一なトナー層を現
像部において維持する。
(2) Maintain an extremely thin toner layer with uniform thickness in the developing section.

(3) 対向する静電潜像面に対して均一なトナー離
脱が可能なトナー層を得る。
(3) Obtain a toner layer that allows uniform toner separation from opposing electrostatic latent image surfaces.

これらにより非画像部ではトナー層が該非画像
部に接触しないようにして地カブリ現像を全く除
去し、且つ画像部には均一で高解像力のトナー画
像が得られるように、トナー粒子をその担持体か
の転移を生ぜしめるように構成した現像装置を提
供する事を目的としている。例えば上記特開昭52
−43037号の発明は、第1図に例示するように、
静電像を有する静電像保持手段1に対向して設け
られた現像剤支持手段(スリーブ)2と該静電像
保持手段1と現像剤支持手段2の間隙を一定に保
つ手段と、該現像剤支持手段2上に、磁性現像剤
6を供給する手段と、該現像剤支持手段2上の現
像剤の厚みを少くとも現像部に於て静電像保持手
段の非画像部に現像剤が接しない厚みに規制する
ため磁界発生手段(磁石)3と、該磁界発生手段
による磁界中で現像剤支持手段に近接して設けら
れ磁界により起立した現像剤の厚みを規制する手
段(磁性ブレード)4を有することを特徴とする
静電像現像装置である。図中5はホツパー7は静
電潜像支持体1とスリーブ2の間に交流バイアス
を印加し画像の階調、ラインの再現性を良くする
ための補助的な装置である。
As a result, in the non-image area, the toner layer is prevented from coming into contact with the non-image area, completely eliminating background fog development, and in the image area, a uniform and high-resolution toner image is obtained. It is an object of the present invention to provide a developing device configured to cause such a transition. For example, the above-mentioned Japanese Patent Application Publication No. 52
The invention of No.-43037, as illustrated in Figure 1,
a developer supporting means (sleeve) 2 provided opposite to the electrostatic image holding means 1 having an electrostatic image; a means for maintaining a constant gap between the electrostatic image holding means 1 and the developer supporting means 2; A means for supplying the magnetic developer 6 onto the developer support means 2, and a means for supplying the magnetic developer 6 onto the developer support means 2, and a thickness of the developer on the developer support means 2 such that the developer is applied to the non-image area of the electrostatic image holding means at least in the developing section. A magnetic field generating means (magnet) 3 is provided to regulate the thickness of the developer so that it does not come into contact with the developer, and a means (magnetic blade) is provided close to the developer supporting means in the magnetic field generated by the magnetic field generating means to regulate the thickness of the developer that stands up due to the magnetic field. ) 4. In the figure, a hopper 7 denoted by 5 is an auxiliary device for applying an alternating current bias between the electrostatic latent image support 1 and the sleeve 2 to improve image gradation and line reproducibility.

この実施例をより具体的に説明をすると、静電
像保持体は特に制限はなく、通常カルーソンプロ
セスで使われている感光体はいずれも使える。又
磁気的記録媒体をも使用可能である。例えば80μ
厚さのセレン感光板上に500Vの潜像電位(コン
トラスト)をつくり、スリーブと感光板との距離
を0.5mmに保つた。
To explain this embodiment more specifically, there is no particular restriction on the electrostatic image holder, and any photoreceptor commonly used in the Caruson process can be used. It is also possible to use magnetic recording media. For example 80μ
A latent image potential (contrast) of 500 V was created on a thick selenium photosensitive plate, and the distance between the sleeve and the photosensitive plate was maintained at 0.5 mm.

またスリーブ表面と磁性ブレードとの距離を
0.3mmに保ち、磁極3aから約600ガウスの磁界を
発生させると、約70ミクロンの厚さの均一なトナ
ー塗布層が形成された。この際使用した磁性トナ
ーは粒径約10ミクロン径で、形成されたトナー層
の電位は約30Vであつた。
Also, the distance between the sleeve surface and the magnetic blade is
When the magnetic field was maintained at 0.3 mm and a magnetic field of about 600 Gauss was generated from the magnetic pole 3a, a uniform toner coating layer with a thickness of about 70 microns was formed. The magnetic toner used at this time had a particle size of about 10 microns, and the potential of the formed toner layer was about 30V.

このような条件で本出願人は二成分系、一成分
系でかつて実現出来なかつた、安定した良好な画
像を再現出来た。
Under these conditions, the applicant was able to reproduce stable and good images, which had not been possible with two-component systems or one-component systems.

しかるにこの方法において問題となるのは、現
像工程で作用する「力」のバランスが複雑なため
安定した画像を維持するのが困難な事である。即
ち現像時トナーのスリーブ2に対する付着力は、
トナーの持つ電荷によるスリーブ表面への吸引力
及びトナーの持つ磁気によるスリーブ表面方向へ
の吸引力、また付着した事によるトナー同志、或
はトナーとスリーブ間の吸引力である。一方潜像
方向へは潜像のつくる電界により引かれる静電力
及び現像バイアス7による静電力である。またト
ナーの持つ運動エネルギー(遠心力)が接線方向
に働いている。
However, a problem with this method is that it is difficult to maintain a stable image because the balance of "forces" acting during the developing process is complicated. That is, the adhesion force of the toner to the sleeve 2 during development is:
These are the attraction force toward the sleeve surface due to the charge of the toner, the attraction force toward the sleeve surface due to the magnetism of the toner, and the attraction force between the toners or between the toners and the sleeve due to adhesion. On the other hand, in the direction of the latent image, there is an electrostatic force drawn by the electric field created by the latent image and an electrostatic force due to the developing bias 7. Furthermore, the kinetic energy (centrifugal force) of the toner acts in the tangential direction.

これらの複雑な「力」のバランスが保たれて良
い画像が維持される事になるが、我々の実験では
次の欠点が明らかになつた。即ち現像を長時間行
うことにより画像濃度の低下が顕著になつた。さ
らにこの現象は現像バイアスが直流方式の時に顕
著であつた。この原因の非常に大きなもののひと
つに現像時に磁界を作用させている為である事が
明らかになつた。つまり現像時トナーに作用する
磁気力が強ければそれだけ潜像方向へ移動するト
ナーは少なくなる。長時間使用した時比較的強く
帯磁したトナーの比率が高くなり、現像特性の劣
化がみられる。或は現像時持つトリボと磁化され
る事による、電気、磁気力のバランスがくずれる
事が明らかとなつた。現像時トナーの持つ磁気量
はトナーに分散されている磁性体の含有率、或は
トナーの大きさ(磁性体の量)、或は磁性体の磁
化特性によつてはスリーブを回転し且つ磁気カツ
トブレードに接触摩擦する事で次第に磁気を帯び
るようになる事等により、トナーに作用している
磁気力は常に変化してゆく事を示している。
A good image is maintained by maintaining the balance of these complex "forces," but our experiments revealed the following drawbacks. That is, when development was carried out for a long time, the image density decreased significantly. Furthermore, this phenomenon was remarkable when the developing bias was a direct current system. It has become clear that one of the major causes of this is that a magnetic field is applied during development. In other words, the stronger the magnetic force acting on the toner during development, the less toner moves toward the latent image. When used for a long time, the ratio of relatively strongly magnetized toner increases, resulting in deterioration of development characteristics. It has also become clear that the balance between electric and magnetic forces is disrupted due to the tribo and magnetization during development. The amount of magnetism that the toner has during development depends on the content of the magnetic material dispersed in the toner, the size of the toner (amount of magnetic material), or the magnetization characteristics of the magnetic material. This shows that the magnetic force acting on the toner is constantly changing, as the toner gradually becomes magnetic due to contact friction with the cut blade.

我々の実験ではこのような不安定な要因をなく
すこと、つまり現像時作用している磁界をなくす
事で前記した現像特性の劣化をなくす事が出来
た。
In our experiments, we were able to eliminate the aforementioned deterioration in development characteristics by eliminating such unstable factors, that is, by eliminating the magnetic field that acts during development.

即ちスリーブ上に均一な層のトナーコーテイン
グを行う上に磁気カツトブレード方式は非常に有
効な手段であるが、現像工程で磁界を作用させる
長所があまり認められなかつた。本出願人の提案
している例えば特開昭54−43037号では現像工程
磁界を作用させトナーの「ほだち」現象を利用し
トナーを飛ばしやすくする説明がなされている
が、この事は特に必須の事項ではなく、潜像面と
スリーブとの距離、両者間の潜像、現像バイアス
条件等の選択で良い画像を持続させる事が出来
た。
That is, although the magnetic cut blade method is a very effective means for coating the sleeve with a uniform layer of toner, the advantage of applying a magnetic field during the developing process has not been well recognized. For example, in Japanese Patent Laid-Open No. 54-43037 proposed by the present applicant, there is an explanation of applying a magnetic field during the developing process to make use of the toner "hodachi" phenomenon to make it easier to blow the toner away, but this is particularly important. Although these are not essential, it was possible to maintain a good image by selecting the distance between the latent image surface and the sleeve, the latent image between them, the developing bias conditions, etc.

本発明は、以上のような技術背景に於て実験研
究の結果開発されたもので、第1図示のような現
像方法に於て、実質的に潜像を現像する領域に磁
界を作用させないことを特徴とするものである。
The present invention was developed as a result of experimental research against the above-mentioned technical background, and in the developing method shown in Figure 1, the present invention is based on the fact that no magnetic field is applied to the area where the latent image is to be developed. It is characterized by:

即ち本発明は、潜像保持手段に対向して設けら
れた現像剤支持手段と、該現像剤支持手段上に各
粒子が帯電している磁性現像剤を供給する手段
と、該現像剤支持手段上の現像剤の厚みを少なく
とも現像部に於て潜像保持手段の非画像部に現像
剤が接しない厚みに規制する手段を有する現像方
法において、実質的に潜像を現像する領域に磁界
を作用させない事を特徴とする現像方法である。
That is, the present invention provides a developer support means provided opposite to a latent image holding means, a means for supplying magnetic developer in which each particle is charged onto the developer support means, and a developer support means. In a developing method having a means for regulating the thickness of the upper developer at least in the developing section to a thickness such that the developer does not come into contact with the non-image area of the latent image holding means, a magnetic field is applied to the area where the latent image is substantially developed. This is a developing method characterized by the fact that it does not act.

第2図は本発明の基本的構成を示すもので、ス
リーブ2に均一なトナー層をコーテイングするた
めの磁性ブレード4に対向する位置だけに磁極8
を配置し、スリーブ2と感光ドラム1との対向す
る現像領域には磁界を有しない構成である。この
場合スリーブ2のトナーくみ上げ搬送に必要な磁
極を、ブレード4に対しスリーブ回転方向後方に
必要に応じ設けることもある。
FIG. 2 shows the basic configuration of the present invention, in which a magnetic pole 8 is located only at a position facing the magnetic blade 4 for coating the sleeve 2 with a uniform toner layer.
, and there is no magnetic field in the developing area where the sleeve 2 and the photosensitive drum 1 face each other. In this case, a magnetic pole necessary for pumping up and conveying the toner in the sleeve 2 may be provided at the rear of the blade 4 in the rotational direction of the sleeve, if necessary.

第3図はカツト磁極8の位置を通過した後トナ
ーに充分トリボを与えるために複数個の搬送磁極
1〜9oを置いた例である。
FIG. 3 shows an example in which a plurality of transport magnetic poles 9 1 to 9 o are provided in order to give sufficient triboelectricity to the toner after passing through the position of the cut magnetic pole 8.

本発明に於ては、トナーが飛び易くなつている
が、なお第1図例と同様電源7から交流バイアス
を印加して現像剤の往復運動による現像促進を行
わせることは、本発明に於ても併用することは好
ましい。そのバイアスは直流でもよい。
In the present invention, the toner is more likely to fly, but it is preferable in the present invention to apply an AC bias from the power supply 7 to accelerate development by reciprocating the developer as in the example shown in FIG. However, it is preferable to use them together. The bias may be direct current.

実施例 感光層の表面に30μのマイラ(商標名)層を形
成した感光ドラムに500Vの潜像を形成し、スリ
ーブ2と300μの間隙で対向させ、同方向に回転
させる。
Example A 500V latent image is formed on a photosensitive drum having a 30μ Mylar (trade name) layer formed on the surface of the photosensitive layer, and the drum is opposed to the sleeve 2 with a gap of 300μ and rotated in the same direction.

鉄製ブレード4をスリーブ2と150μの間隙で
700ガウスの磁石8と向い合せた。その間隙にト
ナー粒子の約5層のトナー層の形成が顕微鏡で観
察された。なおトナーは下記の組成で平均粒径約
15〜20μである。
Iron blade 4 is connected to sleeve 2 with a gap of 150μ.
It faced magnet 8 of 700 gauss. The formation of a toner layer of about 5 toner particles in the interstices was observed under a microscope. The toner has the following composition and an average particle size of approximately
It is 15-20μ.

ポリスチレン(ピコラステイツクD―125)
100部 荷電制御剤(ザボンフアーストブラツクB)
2〃 カーボンブラツク(リーガル400R) 6〃 マグネタイト(戸田工業製EPT―500) 40〃 これらの組合せで現像を繰り返すと第4図に示
すような傾向が確認された。カーブ1は第1図の
現像磁極3a(800ガウス)を置いた時の濃度変
化、2はその現像磁極がない本発明の場合のもの
で長時間現像を継続しても濃度低下が小さいこと
を表わしている。
Polystyrene (Picola Stik D-125)
100 parts Charge control agent (Pomelo First Black B)
2. Carbon black (Regal 400R) 6. Magnetite (Toda Kogyo EPT-500) 40. When development was repeated using these combinations, the tendency shown in Figure 4 was confirmed. Curve 1 shows the density change when the developing magnetic pole 3a (800 Gauss) shown in Figure 1 is placed, and curve 2 shows the density change in the case of the present invention without the developing magnetic pole, which shows that the density drop is small even if development is continued for a long time. It represents.

第5図は第1図例における現像スリーブ上に残
るトナーの残留磁気(帯磁量)を表わすもので、
時間がたつにつれてトナーの平均帯磁量は増加し
ている。スリーブ回転で強く帯磁したもの、はじ
めから強く帯磁しているもの、の割合が増加して
いる為と思われる。
Figure 5 shows the residual magnetism (amount of magnetization) of the toner remaining on the developing sleeve in the example shown in Figure 1.
As time passes, the average amount of magnetization of toner increases. This seems to be due to the increase in the proportion of those that are strongly magnetized by rotation of the sleeve and those that are strongly magnetized from the beginning.

第4図のカーブ1と2の差は、第5図のトナー
の帯磁量の変化のみで説明されるものではなく、
例えば第6図に示すカーブの意味するものも大切
である。第6図は現像器5にトナーを約1000g入
れ5時間コピーをした時、最後に残つたトナーと
初期のトナーの粒度分布を示している。初期のト
ナーはカーブ1のように中心値が約13μφ付近で
5μ以下、20μ以上のトナーはかなり少なくいわゆ
る正規分布に近いものである。しかし残留トナー
の分布を調べるとカーブ2のように数μ以下20μ
以上のトナーのしめる比率が高くなる。
The difference between curves 1 and 2 in FIG. 4 is not explained only by the change in the amount of magnetization of the toner in FIG.
For example, the meaning of the curve shown in FIG. 6 is also important. FIG. 6 shows the particle size distribution of the toner remaining at the end and the initial toner when approximately 1000 g of toner was put into the developing device 5 and copying was carried out for 5 hours. The initial toner has a center value around 13μφ as shown in curve 1.
The amount of toner below 5μ and above 20μ is quite small and is close to the so-called normal distribution. However, when examining the distribution of residual toner, as shown in curve 2, it is less than a few microns or less than 20 microns.
The tightening ratio of the above toner increases.

第6図中の領域のトナーは比較的粒径の小さ
いものであり、この領域のトナーは電気的にも、
また物理的にも強くスリーブに付着する傾向にあ
る。即ちトナーのもつトリボによるスリーブとの
間の鏡像力は小さいトナー程大きい傾向がある。
またスリーブ表面の凹凸部に接触する面積チヤン
スも多くなり、潜像側へ飛び出しづらい。
The toner in the area in FIG. 6 has a relatively small particle size, and the toner in this area is also electrically
It also tends to physically adhere strongly to the sleeve. That is, the smaller the toner, the larger the mirror image force between the toner and the sleeve due to the triboelectric toner.
In addition, the chance of contacting the uneven portions of the sleeve surface increases, making it difficult for the sheet to protrude toward the latent image side.

一方の領域のトナーは粒径大であり質量も大
なので、飛びづらい傾向はあるが、この種の一成
分系現像のトナーは絶縁性のトナーであり、スリ
ーブ上で充分回転しないのでトリボ量が粒径に比
例して大きくはならない事が確認されている。
The toner in one region has a large particle size and mass, so it tends to be difficult to fly, but the toner in this type of one-component developer is insulating and does not rotate sufficiently on the sleeve, so the amount of tribo is low. It has been confirmed that the particle size does not increase in proportion to the particle size.

一方トナーの磁気量はほぼ粒径の3乗に近い程
度に増大していく、従つて大きい粒径のトナーは
しだいに現像に寄与することなく残留し、結果と
して耐久的にみると次第に現像濃度の低下が避け
られない。組成的にも粒径が均一ならばこのよう
な問題は生じないが、実際的には無理であり、現
像濃度変動は避けられなかつた。
On the other hand, the amount of magnetism in toner increases to a degree close to the cube of the particle size. Therefore, toner with a large particle size gradually remains without contributing to development, and as a result, from a durable perspective, the development density gradually decreases. decline is inevitable. Such a problem would not occur if the particle size was uniform in terms of composition, but this is practically impossible, and fluctuations in development density are unavoidable.

本発明による現像磁極なしの系あるいは磁界を
弱めていく系では、第6図カーブ3のようにほぼ
初期の分布カーブ1に近いものが得られている。
この場合粒径の小さなトナーはやはり残る傾向に
あるが、大きい粒子が有効に現像されるので、視
覚的には濃度が高くなり、現像上有利に作用して
いる。
In the system without a developing magnetic pole or the system in which the magnetic field is weakened according to the present invention, a distribution curve 3 similar to the initial distribution curve 1 in FIG. 6 is obtained.
In this case, toner with small particle size still tends to remain, but since large particles are effectively developed, the density visually becomes higher, which is advantageous in terms of development.

【図面の簡単な説明】[Brief explanation of the drawing]

第1図は本発明の前提となる現像装置の構成
図、第2図は本発明方法を実施する装置の構成
図、第3図は本発明の他の実施例の構成図、第4
図は現像濃度―現像時間の関係を表わす曲線図、
第5図は帯磁量―現像時間の関係曲線図、第6図
は現像初期と長時間現像後のトナー粒度分布曲線
図。 1は潜像保持手段、2は現像剤支持手段、3,
8,9は磁石、4は磁性ブレード、5は現像器、
6はトナー、7はバイアス電源。
Fig. 1 is a block diagram of a developing device which is a premise of the present invention, Fig. 2 is a block diagram of an apparatus for carrying out the method of the present invention, Fig. 3 is a block diagram of another embodiment of the present invention, and Fig. 4 is a block diagram of a developing device that is a premise of the present invention.
The figure is a curve diagram showing the relationship between development concentration and development time.
FIG. 5 is a graph showing the relationship between magnetization amount and development time, and FIG. 6 is a graph showing the toner particle size distribution curve at the initial stage of development and after long-term development. 1 is a latent image holding means, 2 is a developer supporting means, 3,
8 and 9 are magnets, 4 is a magnetic blade, 5 is a developer,
6 is toner, 7 is bias power supply.

Claims (1)

【特許請求の範囲】 1 潜像保持手段に対向して設けられた現像剤支
持手段と、該現像剤支持手段上に各粒子が帯電し
ている磁性現像剤を供給する手段と、該現像剤支
持手段上の現像剤の厚みを少なくとも現像部に於
て潜像保持手段の非画像部に現像剤が接しない厚
みに規制する手段を有する現像方法において、実
質的に潜像を現像する領域に磁界を作用させない
事を特徴とする現像方法。 2 特許請求の範囲第1項において、潜像保持手
段と現像剤支持手段との間に交流電圧を印加する
事を特徴とする現像方法。 3 特許請求の範囲第1項に於て、潜像保持手段
と現像剤支持手段との間に直流電圧を印加する事
を特徴とする現像方法。
[Scope of Claims] 1. A developer support means provided opposite to the latent image holding means, means for supplying a magnetic developer in which each particle is electrically charged onto the developer support means, and the developer In a developing method having means for controlling the thickness of the developer on the supporting means to a thickness that does not allow the developer to come into contact with the non-image area of the latent image holding means at least in the developing section, A developing method characterized by not applying a magnetic field. 2. The developing method according to claim 1, characterized in that an alternating current voltage is applied between the latent image holding means and the developer supporting means. 3. A developing method according to claim 1, characterized in that a DC voltage is applied between the latent image holding means and the developer supporting means.
JP5884580A 1980-05-02 1980-05-02 Developing method Granted JPS56154771A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP5884580A JPS56154771A (en) 1980-05-02 1980-05-02 Developing method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP5884580A JPS56154771A (en) 1980-05-02 1980-05-02 Developing method

Publications (2)

Publication Number Publication Date
JPS56154771A JPS56154771A (en) 1981-11-30
JPS6339055B2 true JPS6339055B2 (en) 1988-08-03

Family

ID=13095992

Family Applications (1)

Application Number Title Priority Date Filing Date
JP5884580A Granted JPS56154771A (en) 1980-05-02 1980-05-02 Developing method

Country Status (1)

Country Link
JP (1) JPS56154771A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS59137968A (en) * 1983-01-27 1984-08-08 Mita Ind Co Ltd Recording method using photoconductive toner

Also Published As

Publication number Publication date
JPS56154771A (en) 1981-11-30

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