JPS5852583B2 - Self-bias developing device - Google Patents

Self-bias developing device

Info

Publication number
JPS5852583B2
JPS5852583B2 JP50041042A JP4104275A JPS5852583B2 JP S5852583 B2 JPS5852583 B2 JP S5852583B2 JP 50041042 A JP50041042 A JP 50041042A JP 4104275 A JP4104275 A JP 4104275A JP S5852583 B2 JPS5852583 B2 JP S5852583B2
Authority
JP
Japan
Prior art keywords
potential
latent image
bias
developing
electrode
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
JP50041042A
Other languages
Japanese (ja)
Other versions
JPS51115830A (en
Inventor
誠一 宮川
進 辰己
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.)
Ricoh Co Ltd
Original Assignee
Ricoh Co Ltd
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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP50041042A priority Critical patent/JPS5852583B2/en
Publication of JPS51115830A publication Critical patent/JPS51115830A/en
Publication of JPS5852583B2 publication Critical patent/JPS5852583B2/en
Expired legal-status Critical Current

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  • Developing For Electrophotography (AREA)
  • Wet Developing In Electrophotography (AREA)
  • Dry Development In Electrophotography (AREA)
  • Control Or Security For Electrophotography (AREA)

Description

【発明の詳細な説明】 本発明は、バイアス現像装置、より詳しくは、静電潜像
の電位に応じた電位を現像電極に誘起させて該潜像を現
像する自己バイアス現像装置に関する。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a bias developing device, and more particularly to a self-bias developing device that develops an electrostatic latent image by inducing a potential in a developing electrode that corresponds to the potential of the latent image.

従来、画像の縁端部にのみ多量の現像剤が付着する、い
わゆるエツジ効果を避けるため、現像電極を用いてバイ
アス現像を行っていた。
Conventionally, bias development has been performed using a development electrode in order to avoid the so-called edge effect, in which a large amount of developer adheres only to the edges of an image.

しかし、被写体である原稿には、原稿内の画像面積の大
小、線画像が多いかあるいは連続階調の画像が多いか等
、さまざまなものがあり、これらの原稿から作成された
静電潜像もそれぞれ状態が異なるため、同一の現像条件
では適切な画像が作像されなかった。
However, there are various types of originals that are the subject, such as the size of the image area within the original, whether there are many line images or many continuous tone images, etc., and the electrostatic latent image created from these originals Since the conditions of each are different, an appropriate image could not be formed under the same development conditions.

また、原稿画像を感光体表面に投影露光して静電潜像を
形成するものにおいては、感光体の疲労度や周囲の環境
条件等により静電潜像の電位が微妙に左右され、現像画
像に地肌汚れが生じたり画像濃度が低くなったりする。
In addition, in devices that form an electrostatic latent image by projecting and exposing the original image onto the surface of a photoreceptor, the potential of the electrostatic latent image is slightly affected by the degree of fatigue of the photoreceptor, surrounding environmental conditions, etc., and the developed image The background may become smudged or the image density may become low.

従って、操作者は、そのつと露光光量等の作像条件を調
節しなげればならないが、実際には、そのために試しに
画像を作成し、これによって調節を繰返しており、これ
らの試しに作成した画像(例えば電子写真複写機の1は
、複写紙に形成された複写画像)は全くの無駄になって
しまう。
Therefore, the operator must adjust the image forming conditions such as the exposure light amount, but in reality, the operator creates a trial image for this purpose and repeats the adjustment based on this. The resulting image (for example, the image 1 of an electrophotographic copying machine is a copy image formed on copy paper) is completely wasted.

この欠点を除去するために、現像電極に静電潜像の電位
に応じた電位を導くようにした装置がいくつか提案され
ている。
In order to eliminate this drawback, several devices have been proposed in which a potential corresponding to the potential of the electrostatic latent image is introduced to the developing electrode.

その代表的なものとして、フロート現像電極方式の自己
バイアス現像装置およびオートバイアス方式の強制バイ
アス現像装置が挙げられる。
Typical examples include a self-bias developing device using a float developing electrode and a forced bias developing device using an auto-bias method.

前者は、他から電気的に絶縁をした、いわゆるフロート
現像電極を用いるもので、現像電極には、この現像電極
と対向した静電潜像の平均電位が誘起される。
The former uses a so-called floating developing electrode that is electrically insulated from others, and the average potential of the electrostatic latent image facing the developing electrode is induced in the developing electrode.

この方式によれば、きわめて簡単にバイアス現像を行う
ことができるという利点があるが、現像電極に誘起され
る電位が潜像の平均電位であるため、地肌部が多(て像
領域の少ない原稿や、逆に像領域が多くて地肌部の少な
い原稿を用いた場合、現像電極に誘起される電位と静電
潜像の地肌部あるいは画像領域の電位との電位差が小さ
くなってしまうため、地肌汚れが生じたり、画像濃度が
下ったりしてしまう。
This method has the advantage of being able to perform bias development very easily, but since the potential induced in the development electrode is the average potential of the latent image, the background area is large (and the original has a small image area). Conversely, when using an original with many image areas and few background areas, the potential difference between the potential induced in the developing electrode and the potential of the background area or image area of the electrostatic latent image becomes small, resulting in This may cause stains or lower image density.

この欠点を緩和するものとして、現像電極を一方向整流
器を介して電源に接続したものも提案されている。
In order to alleviate this drawback, a method in which the developing electrode is connected to a power source via a one-way rectifier has also been proposed.

これは、感光体の疲労等によって地肌電位が高い場合に
はある程度効を奏するが、地肌電位が低い場合は、画像
部の濃度が必要以上に低くなってしまい、原稿が薄い鉛
筆書きのようなものの場合には、画像がほとんど消えて
しまう場合もある。
This is effective to some extent when the background potential is high due to fatigue of the photoreceptor, but when the background potential is low, the density of the image area becomes lower than necessary, causing the original to look like thin pencil writing. In some cases, the image may almost disappear.

また、潜像が電源電圧よりも高電位の部分に関しては、
電源に接続したことによる効果は全く得られない。
Also, regarding the part where the latent image has a higher potential than the power supply voltage,
There is no effect of connecting to a power source.

後者のオートバイアス方式は、特願昭4952010号
、特願昭49−67714号に記載されるように、静電
潜像の地肌部に相当する電位を検出し、これを演算処理
して、最適のバイアス電位を現像電極に印加するように
したもので、きわめて確実な作用が得られる。
The latter auto-bias method, as described in Japanese Patent Application No. 4952010 and Japanese Patent Application No. 49-67714, detects the potential corresponding to the background of the electrostatic latent image, performs arithmetic processing on this, and determines the optimal By applying a bias potential of 1 to the developing electrode, an extremely reliable effect can be obtained.

しかし、電位検出装置や演算処理装置の構成が複雑高価
であるという欠点がある。
However, there is a drawback that the configurations of the potential detection device and the arithmetic processing device are complicated and expensive.

本発明の目的は、フロート現像電極方式のように構造が
簡単で、かつ、オートバイアス方式のように作用が確実
な自己バイアス現像装置を提供することにある。
SUMMARY OF THE INVENTION An object of the present invention is to provide a self-bias developing device which has a simple structure like a float developing electrode type and has reliable operation like an auto bias type.

以下、本発明を図面を参照して説明する。Hereinafter, the present invention will be explained with reference to the drawings.

第1図は、本発明が適用された電子写真複写機各部を示
す構成図で、表面に光導電性絶縁層を有する感光体ドラ
ム1が、軸2に支承されて矢印の方向に定速回転すると
、まず、コロナ放電器3によりその表面が一様に帯電さ
れる。
FIG. 1 is a configuration diagram showing each part of an electrophotographic copying machine to which the present invention is applied, in which a photosensitive drum 1 having a photoconductive insulating layer on its surface is supported by a shaft 2 and rotates at a constant speed in the direction of the arrow. Then, first, the surface of the corona discharger 3 is uniformly charged.

コロナ放電器3の極性は、感光体表面の光導電性絶縁層
の特性に応じて適宜選ばれる。
The polarity of the corona discharger 3 is appropriately selected depending on the characteristics of the photoconductive insulating layer on the surface of the photoreceptor.

次に、露光光学系4により、複写されるべき原稿の画像
が、一様に帯電された感光体表面に投影され、感光体表
面の電荷が、影像光線のために選択的に消散し、静電潜
像が形成される。
Next, the image of the document to be copied is projected by the exposure optical system 4 onto the uniformly charged photoreceptor surface, and the charge on the photoreceptor surface is selectively dissipated due to the image beam, and the image becomes static. A latent image is formed.

このようにして感光体表面に形成された静電潜像は、現
像部5においてトナー粒子と接触することにより可視像
化される。
The electrostatic latent image thus formed on the surface of the photoreceptor is made into a visible image by coming into contact with toner particles in the developing section 5.

現像部5は、トナー粒子が分散された現像液6を貯留し
た液槽7と、現像液を現像電極8に供給するためのポン
プ(図示されず)その他の部材からなる。
The developing section 5 includes a liquid tank 7 storing a developer 6 in which toner particles are dispersed, a pump (not shown) for supplying the developer to the developing electrode 8, and other members.

現像電極8は、スイッチ9、抵抗R2を介して、コロナ
放電器3の内部に設けられた電極板10および一端を接
地されたバリスター11に接続されている。
The developing electrode 8 is connected via a switch 9 and a resistor R2 to an electrode plate 10 provided inside the corona discharger 3 and a varistor 11 whose one end is grounded.

電極板10から高電圧の放電電流が取り出され、これを
バリスター11によって定電圧化し7、これを現像電極
8にバイアス印加するための定電圧電源としている。
A high-voltage discharge current is taken out from the electrode plate 10 and is made into a constant voltage by a varistor 11 7, which is used as a constant voltage power source for applying a bias to the developing electrode 8.

このような電源のかわりに、通常のバイアス電源を用い
てもよいことはもちろんである。
Of course, a normal bias power source may be used instead of such a power source.

現像後、感光体表面に付着する余分の現像液は、スクイ
ズローラ12により掻き落とされて鮮明な現像画像が得
られる。
After development, excess developer adhering to the surface of the photoreceptor is scraped off by the squeeze roller 12, resulting in a clear developed image.

この現像画像は、転写部13において、案内板14に案
内されてきた転写紙15に重ねられ、現像画像を形成し
ているトナー粒子を十分引きつげるだけの電荷をコロナ
放電器16かも受けることにより、感光体表面から転写
紙15へ転写される。
This developed image is superimposed on the transfer paper 15 guided by the guide plate 14 in the transfer section 13, and the corona discharger 16 also receives an electric charge sufficient to sufficiently tighten the toner particles forming the developed image. , is transferred from the surface of the photoreceptor to the transfer paper 15.

像を転写された転写紙15は、排出ローラ17により排
出される。
The transfer paper 15 on which the image has been transferred is discharged by a discharge roller 17.

転写紙に転写しないで感光体表面に残留するトナーは、
クリーニングローラ18およびクリーニングブレード1
9により除去され、感光体は再使用可能となる。
Toner that remains on the surface of the photoreceptor without being transferred to the transfer paper is
Cleaning roller 18 and cleaning blade 1
9, the photoreceptor can be reused.

この実施例において、スイッチ9を開いたときには、現
像電極8はフロートの状態になり、スイッチ9を閉じた
ときには、現像電極8はバイアス電源に接続された状態
になる。
In this embodiment, when the switch 9 is opened, the developing electrode 8 is in a floating state, and when the switch 9 is closed, the developing electrode 8 is connected to the bias power supply.

本発明はスイッチ9を閉じたときに係わり、このときの
、この現像装置の電気的等価回路を第2図に示す。
The present invention relates to when the switch 9 is closed, and an electrical equivalent circuit of the developing device at this time is shown in FIG.

Vsは感光体の平均潜像電位と等価的に置きかえた直流
電源の電位、R1は感光体表面と現像電極8との間に介
在する現像剤の抵抗、vDは現像電極電位、R2は現像
電極8と電源20との間に接続された外部抵抗、Vaは
現像電極8に印加されるバイアス定電位にそれぞれ対応
する。
Vs is the potential of the DC power supply equivalent to the average latent image potential of the photoreceptor, R1 is the resistance of the developer interposed between the photoreceptor surface and the developing electrode 8, vD is the developing electrode potential, and R2 is the developing electrode An external resistor Va connected between the developing electrode 8 and the power source 20 corresponds to a bias constant potential applied to the developing electrode 8, respectively.

そして、実際には、抵抗Raが、電源出力インピーダン
スにマツチングするよう電源20に並列に、そして抵抗
R2に直列に接続される。
In practice, a resistor Ra is connected in parallel to the power supply 20 and in series to the resistor R2 to match the power supply output impedance.

コピーの地肌汚れに対する現像電極電位VDと感光体の
平均潜像電位Vsとの関係は第3図に示される。
The relationship between the developing electrode potential VD and the average latent image potential Vs of the photoreceptor with respect to background stains on copies is shown in FIG.

この図において、一点鎖線21で示す直線は、現像電極
電位VDと平均潜像電位Vsとが等しい場合の関係を示
し、静電潜像全体が均一電位である場合の現像画像の地
肌汚れの発生領域を分岐するものである。
In this figure, a straight line indicated by a dashed-dotted line 21 indicates the relationship when the developing electrode potential VD and the average latent image potential Vs are equal, and the occurrence of background stains on the developed image when the entire electrostatic latent image has a uniform potential. It branches out areas.

すなわち、現像電極電位■Dが平均潜像電位Vsより大
きい範囲では、トナー粒子が感光体表面から現像電極に
吸着される電界が生ずるので、現像画像の地肌汚れは生
じることなく、これに対し、現像電極電位■。
That is, in a range where the developing electrode potential ■D is greater than the average latent image potential Vs, an electric field is generated that attracts toner particles from the photoreceptor surface to the developing electrode, so that background staining of the developed image does not occur. Development electrode potential ■.

が平均潜像電位Vsより小さい範囲では、トナー粒子が
現像電極から感光体表面に吸着される電界が生ずるので
、現像画像の地肌汚れが生じる。
In a range where V is smaller than the average latent image potential Vs, an electric field is generated that attracts toner particles from the developing electrode to the surface of the photoreceptor, resulting in background staining of the developed image.

この直線21は、地肌汚れに関する理論的分岐線である
が、フロート現像電極方式における特性曲線と一致し、
実際に現われる現象とよく一致することが確認されてい
る。
This straight line 21 is a theoretical branch line regarding background stains, but it coincides with the characteristic curve in the float developing electrode method,
It has been confirmed that the results match well with actual phenomena.

一方、本発明にかかる現像電極電位■。On the other hand, the developing electrode potential (■) according to the present invention.

と平均潜像電位Vsとの関係は実線で示す直線22によ
り示され、これは次式で表わされる。
The relationship between Vs and the average latent image potential Vs is shown by a solid straight line 22, which is expressed by the following equation.

いま、静電潜像の画像領域がきわめて小さく、平均潜像
電位Vsがバイアス定電位Vaよりも小さい場合を考え
る。
Now, consider a case where the image area of the electrostatic latent image is extremely small and the average latent image potential Vs is smaller than the bias constant potential Va.

このときの平均潜像電位Vsは、静電潜像の地肌部電位
にきわめて近い低電位であるため、フロート現像電極方
式の場合には、地肌部にトナーが付着しないような電界
がほとんど発生せず、現像画像に地肌汚れを生じやすい
The average latent image potential Vs at this time is a low potential that is extremely close to the background potential of the electrostatic latent image, so in the case of the float developing electrode method, almost no electric field is generated to prevent toner from adhering to the background area. Also, background stains are likely to occur in the developed image.

これに対し本発明によれば、第3図に示すように直線2
2は直線21の上方に位置し、現像電極電位vDが平均
潜像電位Vsより大きくなるので、静電潜像の地肌部に
トナーが付着しない電界が生じ、現像画像の地肌汚れは
防止される。
On the other hand, according to the present invention, as shown in FIG.
2 is located above the straight line 21, and the developing electrode potential vD is larger than the average latent image potential Vs, so an electric field is generated that prevents toner from adhering to the background of the electrostatic latent image, and background staining of the developed image is prevented. .

次に、静電潜像の画像領域が大きく、平均潜像電位Vs
がバイアス定電位Vaよりも大きい場合も考える。
Next, the image area of the electrostatic latent image is large, and the average latent image potential Vs
Also consider the case where is larger than the bias constant potential Va.

このときの平均潜像電位Vsは、相対的に静電潜像の画
像領域電位に近くなっており、フロート現像電極方式に
よると、現像画像の地肌汚れは防止できるが、画像濃度
が低くなってしまう。
The average latent image potential Vs at this time is relatively close to the image area potential of the electrostatic latent image. According to the float developing electrode method, background staining of the developed image can be prevented, but the image density becomes low. Put it away.

これに対し本発明によれば、直線22は、第3図で示さ
れるように直線21の下方に位置し、平均潜像電位Vs
より低い電位が現像電極に誘起される。
On the other hand, according to the present invention, the straight line 22 is located below the straight line 21 as shown in FIG. 3, and the average latent image potential Vs
A lower potential is induced at the developer electrode.

従ってフロート電極方式のような画像濃度の低下は生じ
ない。
Therefore, there is no reduction in image density as in the float electrode method.

また、現像電極電位vDの絶対値自体は、平均潜像電位
Vsの上昇に伴って上昇させているので、平均潜像電位
Vsの上昇が着色原稿の使用や感光体の疲労等による静
電潜像の地肌部電位の上昇に起因するものであったとし
ても、現像画像の地肌汚れは防止される。
Furthermore, since the absolute value of the developing electrode potential vD itself is increased as the average latent image potential Vs increases, the increase in the average latent image potential Vs is due to the electrostatic potential caused by the use of colored originals, fatigue of the photoreceptor, etc. Even if it is caused by an increase in the background potential of the image, background staining of the developed image is prevented.

第3図の直線23は、第2図においてバイアス定電位V
aを零としたときの直線である。
The straight line 23 in FIG. 3 corresponds to the bias constant potential V in FIG.
This is a straight line when a is set to zero.

図からも明らかなように、直線23は、直線22と傾き
が等しく、バイアス定電位Va=Oの点で直線21と交
わる。
As is clear from the figure, the straight line 23 has the same slope as the straight line 22, and intersects the straight line 21 at the point where the bias constant potential Va=O.

また、抵抗R2の大きさを変化させれば直線22および
23の傾きが変化する。
Furthermore, if the magnitude of the resistance R2 is changed, the slopes of the straight lines 22 and 23 will change.

従って、装置の使用条件、感光体や現像剤の種類、ある
いは得ようとする画像の品質に応じて、バイアス定電位
Vaおよび抵抗R2を適宜設定すればよい。
Therefore, the bias constant potential Va and the resistance R2 may be appropriately set depending on the usage conditions of the apparatus, the type of photoreceptor and developer, or the quality of the image to be obtained.

また、これらの値を任意に切換えるようにすることもで
きる。
Moreover, these values can also be switched arbitrarily.

なお、直線21および23は原点を中心に点対称であり
、従って各電位の符号が入れかわっても、まったく同様
の作用を営むことは容易に理解できよう。
It should be noted that the straight lines 21 and 23 are point symmetrical with respect to the origin, and therefore it is easy to understand that even if the signs of the respective potentials are reversed, they operate in exactly the same way.

上述の実施例では、平均潜像電位Vsが上昇すれば現像
電極電位■。
In the above embodiment, if the average latent image potential Vs increases, the developing electrode potential becomes ■.

はこれに伴ってどこまでも上昇する。will rise accordingly.

しかし、平均潜像電位Vsが静電潜像の地肌電位の上昇
に起因して上昇するのには限度があり、平均潜像電位V
sがある程度以上まで上昇するのは、通常は静電潜像の
画像領域が大きいことに起因する。
However, there is a limit to how much the average latent image potential Vs can increase due to an increase in the background potential of the electrostatic latent image, and the average latent image potential Vs
The reason why s increases above a certain level is usually due to the fact that the image area of the electrostatic latent image is large.

この場合には現像電極電位■。をそれほど高くする必要
はなく、平均潜像電位Vsがある程度以上の場合には現
像電極電位■。
In this case, the developing electrode potential ■. There is no need to make the developing electrode potential so high, and if the average latent image potential Vs is above a certain level, the developing electrode potential (■) is set.

を一定値に保つようにすればよい=第4図はその構成を
示したもので、上記実施例に、新たに定電圧素子24が
、その一端を抵抗R2と現像電極8との接続点に、他の
一端を接地されて接続されており、上限バイアス定電位
■1がそこに設定されている。
Figure 4 shows its configuration. In the above embodiment, a constant voltage element 24 is added with one end connected to the connection point between the resistor R2 and the developing electrode 8. , the other end is connected to ground, and an upper limit bias constant potential 1 is set there.

第5図は、この実施例における現像電極電位VDと感光
体の平均潜像電位Vsとの関係を実線25で示した図で
ある。
FIG. 5 is a diagram showing the relationship between the developing electrode potential VD and the average latent image potential Vs of the photoreceptor in this embodiment using a solid line 25.

一般に、画像の少ない被写体は、はとんど平均潜像電位
をその地肌電位とみてさしつかえなく、このような場合
、平均潜像電位Vsが、上限バイアス定電位■1 より
小さければ地肌汚れを生じないので、通常の地肌電位に
応じて上限バイアス電位V1 を定めればよい。
Generally, for objects with few images, it is safe to regard the average latent image potential as the background potential.In such cases, if the average latent image potential Vs is smaller than the upper limit bias constant potential 1, background staining will occur. Therefore, the upper limit bias potential V1 may be determined according to the normal background potential.

第5図に示すように、上限バイアス定電位v1 をバイ
アス定電位Vaよりも小さく選ぶことにより、画像の多
い場合でも画像濃度が下がらないようにすることができ
る。
As shown in FIG. 5, by selecting the upper limit bias constant potential v1 to be smaller than the bias constant potential Va, it is possible to prevent the image density from decreasing even when there are many images.

もちろん上限バイアス電位V、の値は、装置の条件に応
じて定めればよく、上限バイアス電位■、をバイアス定
電位Vaより大きい値に設定してもよい。
Of course, the value of the upper limit bias potential V, may be determined according to the conditions of the apparatus, and the upper limit bias potential (2) may be set to a value greater than the constant bias potential Va.

さらに、本発明を効果的に用いるために、現像電極を高
絶縁性の樹脂類で包んで、電気的に完全に絶縁すれば、
特に優れた効果を発揮する。
Furthermore, in order to effectively use the present invention, if the developing electrode is completely electrically insulated by wrapping it in a highly insulating resin,
Particularly effective.

抵抗R2の値は、抵抗R1の値よりも大きい方が好まし
く、上述の液体現像法の実施例において、抵抗R1を約
200MΩ、抵抗R2を約600MΩに保ち、バイアス
定電位を約+400■で、セレン感光体を用いて実験し
たところ、地肌汚れも画像濃度の低下もない各種のコピ
ーを得ることができた。
The value of the resistor R2 is preferably larger than the value of the resistor R1. In the example of the liquid development method described above, the resistor R1 is kept at about 200 MΩ, the resistor R2 is kept at about 600 MΩ, and the bias constant potential is set at about +400 ■. In experiments using a selenium photoreceptor, we were able to obtain various types of copies without background smudges or decreases in image density.

本発明は、いうまでもなく、液体現像法にのみ適用され
るものではなく、乾式現像法においても同様の効果を得
ることができる。
Needless to say, the present invention is not only applicable to liquid development methods, but also can obtain similar effects in dry development methods.

以上、本発明によれば、現像電極に抵抗を接続し、バイ
アス定電位を強制的に印加するたげの簡単な方法により
、潜像に応じてバイアス電位を変化させ、地肌汚れも画
像濃度の低下もないコピーを得ることができる。
As described above, according to the present invention, by connecting a resistor to the developing electrode and forcibly applying a constant bias potential, the bias potential can be changed according to the latent image, and background stains can also be reduced in image density. You can even get a copy.

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

第1図は、本発明が適用された電子写真複写機の全体を
示す構成図、第2図は、本発明が適用された現像装置に
おける電気的等価回路図、第3図は本発明が適用された
現像装置における現像電極電位と感光体の平均潜像電位
との関係を示すグラフ、第4図は、本発明が適用された
現像装置の別の実施例を示す部分構成図、第5図は、第
4図に示す現像装置における現像電極電位と感光体の平
均潜像電位との関係を示すグラフである。 R1:感光体表面と現像電極との間に介在する現像剤の
抵抗、R2:現像電極と電源との間に接続された抵抗、
Va:バイアス定電位、vD:現像電極電位、■s:感
光体の平均潜像電位。
FIG. 1 is a block diagram showing the entire structure of an electrophotographic copying machine to which the present invention is applied, FIG. 2 is an electrical equivalent circuit diagram of a developing device to which the present invention is applied, and FIG. 3 is a diagram to which the present invention is applied. FIG. 4 is a graph showing the relationship between the developing electrode potential and the average latent image potential of the photoreceptor in the developed developing device, and FIG. 5 is a partial configuration diagram showing another embodiment of the developing device to which the present invention is applied. 4 is a graph showing the relationship between the developing electrode potential and the average latent image potential of the photoreceptor in the developing device shown in FIG. 4. FIG. R1: resistance of the developer interposed between the photoreceptor surface and the developing electrode, R2: resistance connected between the developing electrode and the power source,
Va: bias constant potential, vD: developing electrode potential, ■s: average latent image potential of the photoreceptor.

Claims (1)

【特許請求の範囲】 1 現像電極に対向する静電潜像面の平均表面電位に対
応した現像電極電位を、前記静電潜像面と前記現像電極
との間に介在する現像剤の抵抗および前記現像電極と接
地との間に介在させたバイアス抵抗との間において分配
誘起させることにより、前記静電潜像の現像を行なう自
己バイアス現像装置において、前記バイアス抵抗と接地
との間に前記静電潜像面の平均表面電位が低い場合に必
要な現像電極電位を得るための電源装置を接続したこと
を特徴とする自己バイアス現像装置。 2 現像電極に対向する静電潜像面の平均表面電位に対
応した現像電極電位を、前記静電潜像面と前記現像電極
との間に介在する現像剤の抵抗および前記現像電極と接
地との間に介在させたバイアス抵抗との間において分配
誘起させることにより。 前記静電潜像の現像を行なう自己バイアス現像装置にお
いて、前記バイアス抵抗と接地との間に前記静電潜像面
の平均表面電位が低い場合に必要な現像電極電位を得る
ための電源装置を接続するとともに、前記現像電極を定
電圧素子を介して接地することを特徴とする自己バイア
ス現像装置。
[Scope of Claims] 1. A developing electrode potential corresponding to the average surface potential of an electrostatic latent image surface facing the developing electrode is determined by the resistance of the developer interposed between the electrostatic latent image surface and the developing electrode, and In a self-bias developing device that develops the electrostatic latent image by inducing a distribution between the bias resistor interposed between the developing electrode and ground, the electrostatic latent image is distributed between the bias resistor and ground. A self-bias developing device characterized in that a power supply device is connected to obtain a necessary developing electrode potential when the average surface potential of the latent image surface is low. 2 The development electrode potential corresponding to the average surface potential of the electrostatic latent image surface facing the development electrode is determined by the resistance of the developer interposed between the electrostatic latent image surface and the development electrode, and between the development electrode and ground. By inducing a distribution between the bias resistor and the bias resistor interposed between the two. In the self-bias developing device for developing the electrostatic latent image, a power supply device is provided between the bias resistor and ground for obtaining a necessary developing electrode potential when the average surface potential of the electrostatic latent image surface is low. A self-bias developing device characterized in that the developing electrode is connected to the developing electrode and grounded via a constant voltage element.
JP50041042A 1975-04-03 1975-04-03 Self-bias developing device Expired JPS5852583B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP50041042A JPS5852583B2 (en) 1975-04-03 1975-04-03 Self-bias developing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP50041042A JPS5852583B2 (en) 1975-04-03 1975-04-03 Self-bias developing device

Publications (2)

Publication Number Publication Date
JPS51115830A JPS51115830A (en) 1976-10-12
JPS5852583B2 true JPS5852583B2 (en) 1983-11-24

Family

ID=12597335

Family Applications (1)

Application Number Title Priority Date Filing Date
JP50041042A Expired JPS5852583B2 (en) 1975-04-03 1975-04-03 Self-bias developing device

Country Status (1)

Country Link
JP (1) JPS5852583B2 (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS56113149A (en) * 1980-02-13 1981-09-05 Toshiba Corp Copying density change-over device

Also Published As

Publication number Publication date
JPS51115830A (en) 1976-10-12

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