JPH0458277A - Image forming device - Google Patents

Image forming device

Info

Publication number
JPH0458277A
JPH0458277A JP17076390A JP17076390A JPH0458277A JP H0458277 A JPH0458277 A JP H0458277A JP 17076390 A JP17076390 A JP 17076390A JP 17076390 A JP17076390 A JP 17076390A JP H0458277 A JPH0458277 A JP H0458277A
Authority
JP
Japan
Prior art keywords
toner
image
image forming
charging
polarity
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.)
Pending
Application number
JP17076390A
Other languages
Japanese (ja)
Inventor
Toshihiko Minato
湊 敏彦
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.)
Toshiba Corp
Original Assignee
Toshiba 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 Toshiba Corp filed Critical Toshiba Corp
Priority to JP17076390A priority Critical patent/JPH0458277A/en
Publication of JPH0458277A publication Critical patent/JPH0458277A/en
Pending legal-status Critical Current

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  • Discharging, Photosensitive Material Shape In Electrophotography (AREA)
  • Electrostatic Charge, Transfer And Separation In Electrography (AREA)

Abstract

PURPOSE:To obtain a stable image without the unevenness of density by providing an electrified substance capturing means having the same discharge polarity as an electrifying means in an area between the electrifying means and a developing means. CONSTITUTION:When an image forming device 1 is actuated, a part of toner TN in developer D on a magnetic roller 5A starts to scatter to the outside of a developing means 5. A part of Si which is exteriorly added to the toner TN also starts to scatter to the outside of the means 5. the discharged toner TN and the Si initially suspend on the periphery of the means 5 and electrostatically attracted by the (-) potential of a conductive member 13 positioned near the means 5, start to move toward the member 13 and adhere to the member 13 soon. Since the toner TN and the Si are mostly captured by the member 13 in such a way, they do not adhere to the electrifying means 3. As a result, the irregularity of the electric discharge in the means 3 is eliminated and the unevenness of image density at the time of forming the image, furthermore, is eliminated.

Description

【発明の詳細な説明】 [発明の目的コ (産業上の利用分野) 本発明は、電子写真方式を用いた画像形成装置に関する
DETAILED DESCRIPTION OF THE INVENTION [Object of the Invention (Field of Industrial Application) The present invention relates to an image forming apparatus using an electrophotographic method.

(従来の技術) 電子写真方式を用いた画像形成装置は、第3図に示すよ
うに像担持体としてのドラム状の感光体2周辺に、帯電
手段3.露光手段4.現像手段5を配置し、さらに図示
していないが、転写、剥離手段、クリーニング手段、除
電ランプ等が配置され、帯電と像露光により感光体2の
周面に形成されたトナー像(静電潜像)を現像手段5中
の現像剤りにより可視像に変換し、その後転写手段から
の放電電荷により感光体2の周面上のトナー像を転写紙
に転写し、さらに転写紙上のトナー像を熱又は圧力によ
り定着させ、転写紙上に所望の画像を得るものである。
(Prior Art) As shown in FIG. 3, an image forming apparatus using an electrophotographic method includes charging means 3. Exposure means 4. A developing means 5 is disposed, and although not shown, a transfer means, a peeling means, a cleaning means, a static elimination lamp, etc. are also disposed, and a toner image (electrostatic latent) formed on the circumferential surface of the photoreceptor 2 by charging and image exposure is disposed. image) is converted into a visible image by the developer in the developing means 5, and then the toner image on the circumferential surface of the photoreceptor 2 is transferred to a transfer paper by the discharge charge from the transfer means, and then the toner image on the transfer paper is converted into a visible image. is fixed by heat or pressure to obtain a desired image on transfer paper.

ここで帯電手段3は、感光体2の帯電極性に応じて(+
)又は(−)の放電電荷が発生するようになっている。
Here, the charging means 3 charges (+) according to the charging polarity of the photoreceptor 2.
) or (-) discharge charges are generated.

特に感光体2として(−)帯電極性を持つ電子写真複写
機等の場合、帯電手段3にはグリッド7を用いたスコロ
トロン方式が一般的に用いられている。スコロトロン方
式は、グリッド7に感光体2の帯電極性と同一極性の電
位を持たせることにより、チャージ用のワイヤ10から
の放電電流を一定に制御し、常に安定で均一な放電を実
現する方式である。グリッド7に印加する電位の大きさ
は、感光体2の表面電位V。の大きさとほぼ同等となっ
ている。
Particularly in the case of an electrophotographic copying machine or the like in which the photoreceptor 2 has (-) charging polarity, a scorotron system using a grid 7 as the charging means 3 is generally used. The scorotron method is a method that controls the discharge current from the charging wire 10 to a constant level by giving the grid 7 a potential of the same polarity as the charging polarity of the photoreceptor 2, thereby realizing stable and uniform discharge at all times. be. The magnitude of the potential applied to the grid 7 is the surface potential V of the photoreceptor 2. It is almost the same size as .

感光体2の周りの各プロセスユニットの配置において、
帯電手段3と現像手段5との中間の領域には、通常、露
光光学系を通って結像された、光像を感光体2に露光す
る露光手段4が設けられている。
In the arrangement of each process unit around the photoreceptor 2,
In a region intermediate between the charging means 3 and the developing means 5, an exposure means 4 is usually provided which exposes the photoreceptor 2 to a light image formed through an exposure optical system.

また、一部の画像形成装置においては、感光体2上の非
画像領域における帯電電荷を打消すためのランプユニッ
ト(通常LEDアレイを用いている)を、帯電手段3の
後(下流側)で露光手段−4の前(上流側)に設けてい
る場合もある。
Furthermore, in some image forming apparatuses, a lamp unit (usually using an LED array) for canceling the electrical charges in the non-image area on the photoreceptor 2 is installed after the charging means 3 (on the downstream side). In some cases, it is provided before (upstream side) the exposure means-4.

それ以外に帯電手段3と現像手段5の間に何らかのユニ
ットを設けている例は従来の画像形成装置において見当
らないのが現状である。
Currently, there are no examples of conventional image forming apparatuses in which any other unit is provided between the charging means 3 and the developing means 5.

一般的に感光体2の周りの現像手段5の周囲では、現像
手段5からの現像剤り中のトナーTN等の飛散、浮遊が
非常に多くなる。トナーTNのような帯電物(絶縁物)
がもし帯電手段3の中まで流れていき、そのケース12
.ワイヤ10あるいはグリッド7に付着すると付着部の
放電条件が他の部分と異なってしまうため、感光体2へ
の帯電ムラ(VOムラ)が生じ、結果的に、例えばハー
フトーン画像などで部分的な濃度ムラが発生してくる。
Generally, around the developing means 5 around the photoreceptor 2, toner TN and the like in the developer from the developing means 5 scatters and floats in a large amount. Charged objects (insulators) such as toner TN
If it flows into the charging means 3, the case 12
.. If it adheres to the wire 10 or the grid 7, the discharge conditions of the attached part will be different from those of other parts, resulting in uneven charging of the photoreceptor 2 (VO unevenness), and as a result, for example, partial unevenness in halftone images, etc. Density unevenness occurs.

特にスコロトロン方式の場合、グリッド7に何らかの絶
縁物が付着すると、グリッド7上の付着部の抵抗が高く
なるため、グリッド7の電位が局部的に設定値より高く
なる(グリッド7上で電位ムラが発生する)。これによ
り感光体2の帯電ムラ(V Oムラ)が生じるため、結
果的に、帯電物の付着部に対応する位置で、画像の濃度
が他の部分より高くなくことが確認されている。
Particularly in the case of the scorotron method, if some kind of insulator adheres to the grid 7, the resistance of the attached part on the grid 7 increases, causing the potential of the grid 7 to locally become higher than the set value (potential unevenness on the grid 7). Occur). This causes uneven charging of the photoreceptor 2 (V O unevenness), and as a result, it has been confirmed that the density of the image is not higher at the position corresponding to the portion to which the charged object is attached than at other parts.

トナーTN等の帯電物の付着は、現像手段5周変に飛散
、浮遊したものが画像形成装置内の気流の動き(風の流
れ)によって帯電手段3周辺部まで移動し物理的付着す
る場合が多い。しかし、これとは別に、例えばトナーT
Nなどがある極性を持った状態で飛散、浮遊した場合を
考える。トナーTNは一般に帯電手段の放電極性と逆極
性に帯電しているため、現像手段5周辺に飛散、浮遊し
たトナーTNは、気流の動きによってだけでなく静電的
な力によって帯電手段3周辺部まで移動することがある
。特にスコロトロン方式でグリッド7を用いている場合
、グリッド7がトナーTNと逆極性の電位を持っており
しかも広い面積に亘って配置されているため、極性を持
った(帯電している)トナーTNを引きつける力は非常
に強くなり、グリッド7へのトナー付着の確率は非常に
高くなる。
The adhesion of charged substances such as toner TN may be caused by scattering and floating substances during the five rotations of the developing means, which may move to the periphery of the charging means 3 due to the movement of the air current (wind flow) within the image forming apparatus and become physically attached. many. However, apart from this, for example, toner T
Let us consider a case where N or the like is scattered or floating in a state with a certain polarity. Since the toner TN is generally charged with a polarity opposite to the discharge polarity of the charging means, the toner TN scattered and floating around the developing means 5 is not only caused by the movement of airflow but also by electrostatic force to the surrounding area of the charging means 3. It may move up to. In particular, when the grid 7 is used in the scorotron method, the grid 7 has a potential of opposite polarity to the toner TN and is arranged over a wide area, so the toner TN with polarity (charged) The attracting force becomes very strong, and the probability of toner adhesion to the grid 7 becomes very high.

グリッド7やワイヤ10と逆の極性を持った浮遊帯電物
はトナーTsだけではない。即ちトナーTNの流動性を
向上させるため、一般的にトナーTNに外添されている
Stも強い極性を持っている。通常外添されるStは、
トナーTNの帯電極性と同一極性を示すものを用いる(
例えば(+)トナーTNなら(+)極性のSiといった
様に)ので、トナーTNと同様にSiも帯電手段3周辺
へ静電的に引っばられグリッド7、ワイヤ10等に付着
する(外添していたSiは物理的にトナー母体より遊離
することがあるためSi単体で現像手段5周辺に浮遊す
ることがある)。
The toner Ts is not the only floating charged object having a polarity opposite to that of the grid 7 and the wire 10. That is, in order to improve the fluidity of toner TN, St, which is generally externally added to toner TN, also has strong polarity. St, which is usually added externally, is
Use one that has the same charged polarity as the toner TN (
For example, (+) toner TN has (+) polarity Si), so like toner TN, Si is also electrostatically drawn around the charging means 3 and adheres to the grid 7, wire 10, etc. Since the previously used Si may be physically liberated from the toner matrix, Si alone may float around the developing means 5).

(発明が解決しようとする課題) 上述したように従来においてはトナーやSi等の帯電物
が帯電手段に移動、付着し、このため帯電手段の放電ム
ラが生じて画像濃度の均一化を生じるという問題がある
(Problem to be Solved by the Invention) As mentioned above, in the conventional method, charged substances such as toner and Si move and adhere to the charging means, which causes uneven discharge of the charging means and causes uniform image density. There's a problem.

そこで、本発明は、像担持体の周囲の構成を改良するこ
とによって帯電手段の放電の均一化2画像濃度の均一化
を図ることができる画像形成装置を提供することを目的
とするものである。
SUMMARY OF THE INVENTION Therefore, an object of the present invention is to provide an image forming apparatus that can achieve uniform discharge of a charging means and uniform image density by improving the configuration around an image carrier. .

[発明の構成コ (課題を解決するための手段) 本発明は、画像形成に供する静電潜像を担持する像担持
体の周囲に帯電手段と現像手段とを備える画像形成装置
において、前記帯電手段と現像手段との間の領域に帯電
手段と同一の放電極性を有する帯電物捕獲手段を備えた
ものである。
[Structure of the Invention (Means for Solving the Problems) The present invention provides an image forming apparatus including a charging means and a developing means around an image bearing member carrying an electrostatic latent image to be used for image formation. A charged object capturing means having the same discharge polarity as the charging means is provided in a region between the means and the developing means.

(作 用) 上述した構成の画像形成装置によれば、現像手段周辺に
飛散、浮遊した帯電物が、帯電手段と同一の放電極性を
有する帯電物捕獲手段により捕獲されるので、帯電手段
への帯電物の付着が回避される。
(Function) According to the image forming apparatus configured as described above, charged objects scattered or floating around the developing means are captured by the charged object capturing means having the same discharge polarity as the charging means, so that the charged objects are not affected by the charging means. Adhesion of charged objects is avoided.

(実施例) 以下に本発明の実施例を詳細に説明する。(Example) Examples of the present invention will be described in detail below.

第1図に示す画像形成装置1は、像担持体としてのドラ
ム状の感光体2の周囲に沿って帯電手段3、露光手段4
.現像手段5を所定の間隔で順次配置している。
The image forming apparatus 1 shown in FIG.
.. The developing means 5 are sequentially arranged at predetermined intervals.

前記帯電手段3は、スコロトロン方式で、グリッド7、
放電用のワイヤ10.ケース12を備えるとともに、ワ
イヤ10に高圧電源9を接続し、ワイヤ10から負(−
)の電荷を放電するようになっている。また、グリッド
7はツェナーダイオード8を介して接地されている。
The charging means 3 is a scorotron type, and includes a grid 7,
Discharge wire 10. A case 12 is provided, a high voltage power supply 9 is connected to the wire 10, and a negative (-) is connected to the wire 10.
) is designed to discharge the electric charge. Furthermore, the grid 7 is grounded via a Zener diode 8.

従って、ワイヤ10からの(−)の電荷によりグリッド
7には(−)の電位が生じることになる。
Therefore, a (-) potential is generated on the grid 7 due to the (-) charge from the wire 10.

前記露光手段3と現像手段5との間には第1図。There is a space between the exposing means 3 and the developing means 5 as shown in FIG.

第2図に示すような帯電物捕獲手段11が配置されてい
る。
Charged object capturing means 11 as shown in FIG. 2 is arranged.

この帯電物捕獲手段11は、感光体2の軸方向に沿って
配置した板状で絶縁体製の支持体6と、この支持体6に
よって支持された前記グリッド7と同様な構成の導電部
材13とを具備し、この導電部材13をリード線14に
より前記グリッド7の一端に接続している。即ち、導電
部材13は、支持体6が絶縁体製であるため電気的に非
接地状態で、かつ、グリッド7と同様な(−)の電位(
同電位)に保たれるようになっている。
This charged object capturing means 11 includes a plate-shaped insulating support 6 disposed along the axial direction of the photoreceptor 2, and a conductive member 13 having the same structure as the grid 7 supported by the support 6. The conductive member 13 is connected to one end of the grid 7 by a lead wire 14. That is, the conductive member 13 is electrically ungrounded because the support body 6 is made of an insulator, and is at a negative potential (-) similar to that of the grid 7.
are kept at the same potential).

次に、前記画像形成装置1の作用を説明する。Next, the operation of the image forming apparatus 1 will be explained.

画像形成装置1が作動すると、現像手段5中の磁気ロー
ラ5Aが回転を始め、磁気ローラ5A上にあった現像剤
り中のトナーTNの一部が現像手段5の外部に飛散しだ
す。またトナーTNに外添されていたSiの一部が、ト
ナーTNの母体より遊離し、これもまた、現像手段5の
外部に飛散し始める。トナーTNやSiは、帯電手段3
の放電極性と反対極性(+)に帯電しているため、飛散
し現像手段5の外部に排出したトナーTN、Siも弱く
であるが極性(この場合は(+)極性)を帯びている。
When the image forming apparatus 1 is operated, the magnetic roller 5A in the developing means 5 starts rotating, and a part of the toner TN in the developer on the magnetic roller 5A begins to scatter to the outside of the developing means 5. Further, a part of the Si externally added to the toner TN is released from the toner TN matrix, and this also begins to scatter to the outside of the developing means 5. Toner TN and Si are charged by charging means 3.
Since the toner TN and Si are charged to the opposite polarity (+) to the discharge polarity, the toner TN and Si that are scattered and discharged to the outside of the developing means 5 also have a weak polarity (in this case, (+) polarity).

排出されたトナーTN、Siは最初現像手段5の周辺に
浮遊しているが、現像手段5の近傍に位置する導電部材
13の(−)電位によって静電的に引かれ、その方向に
移動しはじめ、やがて導電部材13に付着する。この状
態を第1図に示す。この様にして、トナーTN、Siの
ほとんどが導電部材13により捕獲されるため、帯電手
段3には、トナーTN、Siの付着が起きず、この結果
、帯電手段3の放電ムラが無くなり、さらには、画像形
成時の画像濃度のムラも無くなる。
The discharged toners TN and Si are initially floating around the developing means 5, but are electrostatically attracted by the (-) potential of the conductive member 13 located near the developing means 5 and move in that direction. At first, it eventually adheres to the conductive member 13. This state is shown in FIG. In this way, most of the toner TN and Si are captured by the conductive member 13, so that the toner TN and Si do not adhere to the charging means 3, and as a result, uneven discharge of the charging means 3 is eliminated. Also, unevenness in image density during image formation is eliminated.

尚、上述した実施例では、導電部材13とグリッド7と
に共通の高圧電源9を用いているので、導電部材13専
用の電源は不要となる。
In the embodiment described above, the common high-voltage power supply 9 is used for the conductive member 13 and the grid 7, so a dedicated power supply for the conductive member 13 is not required.

本発明は上述した実施例のほか、その要旨の範囲内で種
々の変形が可能である [発明の効果コ 以上詳述した本発明によれば、前記帯電物捕獲手段を設
けたことにより、帯電手段の帯電ムラ、さらには画像の
濃度ムラの無い安定した画像形成を行うことができる画
像形成装置を提供することができる。
In addition to the embodiments described above, the present invention can be modified in various ways within the scope of the gist thereof. It is possible to provide an image forming apparatus that can perform stable image formation without uneven charging of the device and uneven density of the image.

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

第1図は本発明の実施例装置の概略断面図、第2図は同
装置の帯電物捕獲手段の切欠斜視図、第3図は従来装置
の概略断面図である。
FIG. 1 is a schematic sectional view of an apparatus according to an embodiment of the present invention, FIG. 2 is a cutaway perspective view of a charged object capturing means of the same apparatus, and FIG. 3 is a schematic sectional view of a conventional apparatus.

Claims (1)

【特許請求の範囲】[Claims] 画像形成に供する静電潜像を担持する像担持体の周囲に
帯電手段と現像手段とを備える画像形成装置において、
前記帯電手段と現像手段との間の領域に帯電手段と同一
の放電極性を有する帯電物捕獲手段を備えたことを特徴
とする画像形成装置。
An image forming apparatus including a charging means and a developing means around an image bearing member carrying an electrostatic latent image to be used for image formation,
An image forming apparatus characterized in that a charged object capturing means having the same discharge polarity as the charging means is provided in a region between the charging means and the developing means.
JP17076390A 1990-06-28 1990-06-28 Image forming device Pending JPH0458277A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP17076390A JPH0458277A (en) 1990-06-28 1990-06-28 Image forming device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP17076390A JPH0458277A (en) 1990-06-28 1990-06-28 Image forming device

Publications (1)

Publication Number Publication Date
JPH0458277A true JPH0458277A (en) 1992-02-25

Family

ID=15910927

Family Applications (1)

Application Number Title Priority Date Filing Date
JP17076390A Pending JPH0458277A (en) 1990-06-28 1990-06-28 Image forming device

Country Status (1)

Country Link
JP (1) JPH0458277A (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002006592A (en) * 2000-06-27 2002-01-09 Katsuragawa Electric Co Ltd Electrification device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2002006592A (en) * 2000-06-27 2002-01-09 Katsuragawa Electric Co Ltd Electrification device

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