JPH0225856A - Development method - Google Patents

Development method

Info

Publication number
JPH0225856A
JPH0225856A JP17659588A JP17659588A JPH0225856A JP H0225856 A JPH0225856 A JP H0225856A JP 17659588 A JP17659588 A JP 17659588A JP 17659588 A JP17659588 A JP 17659588A JP H0225856 A JPH0225856 A JP H0225856A
Authority
JP
Japan
Prior art keywords
electric field
toner
magnetic
developer
carrier
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP17659588A
Other languages
Japanese (ja)
Other versions
JP2510247B2 (en
Inventor
Yuji Sakami
裕二 酒見
Masahiro Ito
政宏 伊藤
Akira Watanabe
渡辺 顕
Takahiro Kubo
貴裕 久保
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 JP63176595A priority Critical patent/JP2510247B2/en
Publication of JPH0225856A publication Critical patent/JPH0225856A/en
Application granted granted Critical
Publication of JP2510247B2 publication Critical patent/JP2510247B2/en
Anticipated expiration legal-status Critical
Expired - Fee Related legal-status Critical Current

Links

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  • Magnetic Brush Developing In Electrophotography (AREA)
  • Developing For Electrophotography (AREA)
  • Dry Development In Electrophotography (AREA)

Abstract

PURPOSE:To prepare an image excellent in evenness by superimposing a electric field to weaken the intensity of an electric field in either period of one part of the period to impress the electric field in a direction to cause a toner grain to transit or one part of the period to impress the electric field in the direction to drum the toner grain. CONSTITUTION:In at least either period of the period to impress the electric field to cause a toner 37 to transit from a developing sleeve 22 to a photosensitive body drum 1 or the period to impress the electric field in the direction to separate the toner 37 from the photosensitive body drum 1 to the contrary to the transition, the electric field to weaken the intensity of the electric field is superimposed. Thus, the image can be prepared which is rich in a gradation, in which a base fogging is small, in which the emphasis of an edge is properly executed, in which a density change in a half tone does not exist and which is excellent in the evenness.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は、電子写真法、静電記録法等によっ−で形成さ
れた静電潜像を現像する方法に関し、詳しくは現像剤担
持体と、静電潜像担持体間に交互電界を印加して2成分
現像剤を用いて現像を行なう現像方法に関するものであ
り、特に記録画像表示装置、複写機、プリンタ、ファク
シミリ等に好適な現像方法に関する。
Detailed Description of the Invention (Field of Industrial Application) The present invention relates to a method for developing an electrostatic latent image formed by electrophotography, electrostatic recording, etc. The present invention relates to a developing method in which an alternating electric field is applied between electrostatic latent image carriers and a two-component developer is used, and the developing method is particularly suitable for recording image display devices, copying machines, printers, facsimile machines, etc. Regarding the method.

(従来の技術) 従来、現像剤担持体の表面に、顕画剤としてのトナー粒
子と磁性キャリヤからなる乾式現像剤を担持させて搬送
させ、この現像剤を静電潜像を担持した静電潜像担持体
の表面近傍に搬送供給して該現像担持体上にこの現像剤
の磁気ブラシを形成させ、静電潜像担持体と現像剤担持
体の間に交互電界を印加しながら該静電潜像を顕画現像
する現像方法については知られている。この現像方法は
磁気ブラシ現像法と通称される場合が多い。
(Prior Art) Conventionally, a dry developer consisting of toner particles as a developing agent and a magnetic carrier is supported on the surface of a developer carrier and transported, and this developer is transferred to an electrostatic process carrying an electrostatic latent image. The developer is conveyed and supplied near the surface of the electrostatic latent image carrier to form a magnetic brush on the developer carrier, and while an alternating electric field is applied between the electrostatic latent image carrier and the developer carrier, the electrostatic developer is Developing methods for developing electrostatic latent images are known. This developing method is often commonly referred to as magnetic brush developing method.

なお上記現像剤担持体は一般に現像装置の現像スリーブ
として用いられる場合が多いので以下の説明では現像ス
リーブを総称するものとし、また静電潜像担持体は一般
に感光体ドラムとして用いられる場合が多いので以下の
説明では同様に感光体ドラムと総称するものとする。
The developer carrier described above is generally used as a developing sleeve of a developing device, so in the following explanation, the developing sleeve will be referred to generically, and the electrostatic latent image carrier is generally used as a photoreceptor drum in many cases. Therefore, in the following description, they will be collectively referred to as photosensitive drums.

この現像方法としては従来、例えば2成分系組成(キャ
リヤ粒子とトナー粒子)からなる現像剤により、内部に
磁石を配置した現像スリーブの表面に磁気ブラシを形成
させ、微小な現像間隙を保フて対向させた感光体ドラム
にこの磁気ブラシを摺擦ないし近接させ、現像スリーブ
と感光体ドラム間に連続的に交互電界を印加することで
、トナー粒子の現像スリーブ側から感光体ドラム側への
転位及び逆方向への逆転位を繰返し行なわせて現像を行
なういわゆる磁気ブラシ現像が知られ(特開昭55−3
2060号、同59−165082号等)、また簡易カ
ラー現像や多重現像を目的とした2成分現像剤を用いた
非接触方式の交互電界現像法も知られている(特開昭5
8−14268号、同58−68051号、同5B−1
44452号、同59−181362号、同60−17
8069号)。
Conventionally, this developing method uses a developer consisting of two components (carrier particles and toner particles) to form a magnetic brush on the surface of a developing sleeve with magnets arranged inside to maintain a minute development gap. By rubbing this magnetic brush against or bringing it close to the opposing photoreceptor drum and continuously applying an alternating electric field between the developing sleeve and the photoreceptor drum, the toner particles are transferred from the developing sleeve side to the photoreceptor drum side. So-called magnetic brush development is known in which development is carried out by repeatedly performing reverse displacement in the opposite direction (Japanese Patent Application Laid-Open No. 55-3).
No. 2060, No. 59-165082, etc.), and a non-contact alternating electric field development method using a two-component developer for the purpose of simple color development and multiple development is also known (Japanese Patent Laid-Open No.
No. 8-14268, No. 58-68051, No. 5B-1
No. 44452, No. 59-181362, No. 60-17
No. 8069).

(発明が解決しようとする課題) ところで上述した従来の交互電界を印加する方式の磁気
ブラシ現像法においては、感光体ドラムに形成されてい
る静電潜像の電界と印加する交互電界の作用で現像濃度
をあげ、またカブリを取除く現像方式のものであるため
、得られる顕画像の画像端部における鮮明度を上げるこ
とが困難である等の問題があった。
(Problems to be Solved by the Invention) In the above-mentioned conventional magnetic brush development method in which alternating electric fields are applied, the effect of the electric field of the electrostatic latent image formed on the photoreceptor drum and the alternating electric field applied Since the method uses a development method that increases the development density and removes fog, there are problems such as difficulty in increasing the sharpness of the image edges of the resulting developed image.

このような問題を解決するための方法としていくつかの
手段が考えられ、例えば感光体ドラムと現像スリーブの
間に印加する交互電界の周波数を上げて、濃度を上げカ
ブリを取り除く方法を採ることも考えられるが、このよ
うな方法では画像自身が硬調なものとなり、また非画像
部ばかりでなくこの非画像部の電位に近い画像部(いわ
ゆるハイライト部)におけるトナーの付着が減少し、再
現性が低下し易いという別の問題を招く。
Several methods can be considered to solve this problem, such as increasing the frequency of the alternating electric field applied between the photoreceptor drum and the developing sleeve to increase the density and eliminate fog. However, with this method, the image itself becomes high-contrast, and toner adhesion not only in non-image areas but also in image areas close to the potential of these non-image areas (so-called highlight areas) decreases, resulting in poor reproducibility. Another problem arises in that the amount of water tends to decrease.

このことは、静電潜像に対する画像濃度の特性として説
明される。一般にこの特性を示す曲線の勾配γにより画
像の階調性が判定できるが、上記交互電界の周波数を上
げた方式の現像では、この勾配γが極端に立ワた階調性
の不足気味の画像となり易い、これはキャリヤ粒子に付
着したトナー粒子や現像スリーブ上のトナー粒子が、交
互電界の周波数が高まってくると電界の動きに十分追従
できなくなり、ある閾値を境に、感光体ドラム上に飛翔
するかしないかの潜像に対する2値的な現像現象を呈す
る傾向が顕著になるためと考えられる。
This can be explained as a characteristic of image density for electrostatic latent images. Generally, the gradation of an image can be determined by the slope γ of the curve that indicates this characteristic, but in the developing method in which the frequency of the alternating electric field is increased, this slope γ is extremely steep, resulting in an image that lacks gradation. This is because as the frequency of the alternating electric field increases, the toner particles attached to the carrier particles and the toner particles on the developing sleeve cannot sufficiently follow the movement of the electric field, and after a certain threshold, the toner particles adhere to the photoreceptor drum. This is thought to be because the latent image tends to exhibit a binary development phenomenon of flying or not flying.

一方、上記とは反対に勾配γを小さくするために交互電
界の周波数を下げる(例えば数百Hz程度)と、トナー
粒子が感光体ドラムと現像スリーブの間を往復しながら
現像を行なうことになりて、階調性のよい画像が得られ
ることになるが、反面においてカブリの悪化や、キャリ
ヤが感光体ドラムに付着するどいフた問題もでてくる。
On the other hand, in contrast to the above, if the frequency of the alternating electric field is lowered (for example, to about several hundred Hz) in order to reduce the gradient γ, the toner particles will perform development while reciprocating between the photoreceptor drum and the developing sleeve. As a result, an image with good gradation can be obtained, but on the other hand, problems such as deterioration of fog and the possibility of the carrier adhering to the photoreceptor drum arise.

これは、上記周波数を下げることによって、トナー粒子
やキャリヤ粒子の電界の動きに対する追従性がよくなる
ものの、感光体ドラム上の非画像部に向フて飛翔したト
ナー粒子やキャリヤ粒子は、これを感光体ドラム側に転
位させる電界の印加時間の延長(周波数が低いので)の
ために該感光体ドラム上にトラップされてしまい、交互
電界による逆転位のための電界が作用してもこれを完全
に取り去ることが難かしくなるためと考えられる。
This is because by lowering the frequency, toner particles and carrier particles can better follow the movement of the electric field, but the toner particles and carrier particles that fly toward the non-image area on the photoreceptor drum are Due to the extended application time (because the frequency is low) of the electric field that causes transposition to the photosensitive drum side, it is trapped on the photosensitive drum, and even if the electric field for reverse transposition due to the alternating electric field acts, it cannot be completely eliminated. This is thought to be because it becomes difficult to remove.

このように、従来の2成分現像剤を用いて交互電界によ
り現像を行なう方法においては、得られる顕画画像につ
いて、カブリやキャリヤ付着を少なくすることと、階調
性に優れたものとすることを同時に満足させることが困
難であるという問題があった。
In this way, in the method of developing with an alternating electric field using a conventional two-component developer, it is necessary to reduce fog and carrier adhesion and to make the obtained microscopic image excellent in gradation. There was a problem in that it was difficult to simultaneously satisfy the following.

本発明は、以上のような2成分現像剤を用い、交互電界
を印加しながら現像を行なういわゆる磁気ブラシ現像法
において、従来の問題点を解消し、階調性に富み、地力
ブリが少なく高解像度で、中間調における濃度変化の少
ない均一性に優れた画像を形成できる現像方法を提供す
ることを目的とする。
The present invention solves the conventional problems in the so-called magnetic brush development method in which development is performed while applying an alternating electric field using a two-component developer as described above, and achieves high tonality, high tonality, and less blurring. It is an object of the present invention to provide a developing method capable of forming an image with excellent resolution and uniformity with little change in density in halftones.

また更に本発明の他の目的は、余分なトナーの転移を減
少させ、かつ顕画像を更に転写紙に転写させる際の負担
を軽減できると共に、少ない消費で高い濃度を得ること
ができる現像方法を提供するところにある。
Still another object of the present invention is to provide a developing method that can reduce transfer of excess toner, reduce the burden of further transferring a developed image onto transfer paper, and obtain high density with low consumption. It's there to provide.

(課題を解決するための手段) 本発明は以上の目的を実現するためになされたものであ
り、本発明現像方法の特徴の顕画像としてのトナー粒子
とキャリヤ粒子とからなる2成分現像剤を表面&:担持
して搬送する現像スリーブ(現像剤担持体)と、感光体
ドラム(静電潜像担持体)とを、微小な間隙を保ちつつ
移動する関係に配置すると共に。この間隙部で現像スリ
ーブ上に上記現像剤の磁気ブラシを形成させ、これら現
像スリー・ブと感光体ドラムの間に、現像スリーブから
感光体ドラムにトナー粒子を転移させる方向に電界?印
加する期間と、該転移とは反対に感光体ドラムからトナ
ー粒子を離脱させる方向に電界を印加する期間とを、交
互に繰返し印加しながら現像を行なう方式の現像方法に
おいで、上記トリー粒子を転移させる方向に電界を印加
する期間の一部、及びトナー粒子をドラムざぜる方向に
電界を印加する期間の一部の少なくともいずれか一方の
期間において、該電界を弱める1胛を1!宣させるよう
にしたところにある。
(Means for Solving the Problems) The present invention has been made to achieve the above objects, and uses a two-component developer consisting of toner particles and carrier particles as a developed image, which is a feature of the developing method of the present invention. Surface &: A developing sleeve (developer carrier) to be carried and conveyed and a photosensitive drum (electrostatic latent image carrier) are arranged in a moving relationship while maintaining a small gap. A magnetic brush of the developer is formed on the developing sleeve in this gap, and an electric field is applied between the developing sleeve and the photosensitive drum in the direction of transferring toner particles from the developing sleeve to the photosensitive drum. In a developing method in which development is performed while alternately and repeatedly applying an electric field in a direction in which the toner particles are applied and a period in which the electric field is applied in a direction in which the toner particles are detached from the photoreceptor drum in the opposite direction to the transfer, the above-mentioned tree particles are During at least one of a part of the period in which the electric field is applied in the direction of transferring the toner particles and a part of the period in which the electric field is applied in the direction of drumming the toner particles, the electric field is weakened by 1! This is what I tried to do to make it public.

本発明の方法は上述のように現像スリーブから感光体ド
ラムにトナーを転移させる方向に電界を印加する期間と
、該転移とは反対に感光体ドラムからトナー?離脱させ
る方向に電界を印加する期間の少なくともいすねかの期
間において、該電界を弱める電界を重畳させるものであ
ればよいが、これらを同時に行なう場合には本発明の効
果がより好ましく実現される。
As described above, the method of the present invention includes a period in which an electric field is applied in the direction of transferring the toner from the developing sleeve to the photoreceptor drum, and a period in which the electric field is applied in the direction in which the toner is transferred from the photoreceptor drum to the photoreceptor drum in the opposite direction. It is sufficient that an electric field that weakens the electric field is superimposed during at least part of the period in which the electric field is applied in the direction of separation, but the effects of the present invention are more preferably realized when these are applied simultaneously. .

本発明方法は、上述した2成分系の現像剤を用いたいわ
ゆる磁気ブラシ現像法に通用できる。
The method of the present invention can be applied to the so-called magnetic brush development method using the above-mentioned two-component developer.

本発明の構成において、感光体ドラムと現像スリーブの
間の交互電界は、基本となる交互電界および重畳する電
界のいずれについても、交流電圧の印加による方式、矩
形波のパルス電圧の印加による方式の他、三角波、鋸歯
状波、あるいは非対称波等のいずれによるものであって
もよく、特に限定されるものではない。
In the configuration of the present invention, the alternating electric field between the photoreceptor drum and the developing sleeve can be generated by applying an alternating current voltage or by applying a rectangular pulse voltage for both the basic alternating electric field and the superimposed electric field. In addition, it may be a triangular wave, a sawtooth wave, or an asymmetric wave, and is not particularly limited.

また上記構成において、現像スリーブから感光体ドラム
にトナーを転移させる方向に電界を印加する期間(主に
感光体ドラムの画像部を現像する方向に電界を印加する
期間であり、感光体ドラムの非画像部電位との関係で該
非画像部にもトナーが若干転移する)の・一部において
該電界を郭める電界を重畳するとは、例えばパルス合成
器等を用い、基本となる一つの交互電界として、300
H2〜2k)!zの電界を使用し、その電界に、その転
移期間で逆位相となる他の短いパルスを重畳させること
で行なうことができる。
Further, in the above configuration, a period in which an electric field is applied in a direction in which toner is transferred from a developing sleeve to a photoconductor drum (this is a period in which an electric field is applied in a direction in which an image area of the photoconductor drum is mainly developed; Toner is transferred to the non-image area to some extent due to the relationship with the potential of the image area).To superimpose the electric field that surrounds the electric field in a part of the area means to use a pulse synthesizer, etc., for example, to create one basic alternating electric field. as, 300
H2~2k)! This can be done by using an electric field in z and superimposing it with other short pulses that are in opposite phase during the transition.

また感光体ドラムから現像スリーブにトナーを逆転移さ
せる方向に電界を印加する期間(主に感光体ドラムの非
画像部に載りたトナーを剥11(逆転移)させる方向に
電界を印加する期間であり、感光体ドラムの画像部電位
との関係で該画像部のトナ・−も若干逆転移する)の一
部に該電界を弱める電界を重畳させるとは、上記と同様
にして例えば基本となる一つの交互電界に、その転移期
間で逆位相となる他の短いパルスを重畳させることによ
り、非画像部との間にトナーを転移させる強さを持たな
い電界を形成(即ち、スリーブに印加させる電圧は、感
光体の画像部、非画像部電位の間の値であって、かつ両
者間の中心よりも非画像部電位に近い値の直流成分とす
る)することにより行なうことができる。
Also, a period in which an electric field is applied in a direction to reversely transfer the toner from the photoreceptor drum to the developing sleeve (mainly a period in which an electric field is applied in a direction to peel off 11 (reverse transfer) the toner on the non-image area of the photoreceptor drum). The idea of superimposing an electric field that weakens the electric field on a part of the image area (the toner of the image area also undergoes a slight reverse transition in relation to the image area potential of the photoreceptor drum) is similar to the above, for example, as a basic idea. By superimposing one alternating electric field with another short pulse that has an opposite phase during the transition period, an electric field is created that does not have the strength to transfer toner between it and the non-image area (i.e., it is applied to the sleeve). The voltage may be a DC component having a value between the potential of the image area and the non-image area of the photoreceptor, and closer to the potential of the non-image area than the center between the two.

上記電界を弱める調整を行なう期間は、例えばトナーを
現像スリーブから感光体ドラムに転移させる期間の一部
においてその電界を弱める場合には、その初め、中間、
終りのいずれにおいても、あるいはこれらを複数に、設
けてもよい。トナーを感光体ドラムから現像スリーブに
逆転移させる場合に上記の調整の期間を設ける場合にも
同様である。電界を弱めるとは、一般的には感光体ドラ
ムの画像部電位と非画像部電位の間、特に交互電界と共
に重畳して印加する直流成分の電位(交互電界の上下ピ
ークの中間電位)に該印加電圧を移行させる場合を例示
することができるが、特にこれに限定されるものではな
い0例えば、電子写真法を用いた通常のアナログ複写機
では上記の電位ないしその近傍に移行させるのが好まし
い場合が多いが、コンピュータ機器等のプリンタとして
使用されるディジタル複写機(例えばレーザビームプリ
ンタ)では、トナーを転移させる期間においてその電界
を弱めるのに、画像部電位が概ね一定の電位として形成
されている等の理由からその画像電位ないしその近傍に
移行させることが好ましい場合が多い。
For example, when the electric field is weakened during a part of the period during which toner is transferred from the developing sleeve to the photoreceptor drum, the period during which the electric field is adjusted to weaken is the beginning, middle,
They may be provided at any end or in multiples. The same applies to the case where the above adjustment period is provided when the toner is reversely transferred from the photosensitive drum to the developing sleeve. Weakening the electric field generally refers to the potential between the image area potential and the non-image area potential of the photoreceptor drum, especially the potential of the DC component that is applied superimposed with the alternating electric field (midpoint potential between the upper and lower peaks of the alternating electric field). For example, in a normal analog copying machine using electrophotography, it is preferable to shift the applied voltage to or near the above potential. In many cases, in digital copying machines (for example, laser beam printers) used as printers for computer equipment, the image area potential is formed as a roughly constant potential in order to weaken the electric field during the period of toner transfer. In many cases, it is preferable to shift the image potential to or near that image potential.

本発明方法に用いられる2成分現像剤は、例えばフェラ
イト等の磁性体粒子の表面を樹脂コーティングした磁性
粒子であるキャリヤ粒子と、荷電制御剤、外添剤等を樹
脂で結着した非磁性粒子であるトナー粒子の組合せを例
示することができるが、特にこれに限定されるものでは
なく、いわゆる磁気ブラシ現像法に用いられる2成分現
像剤であればいずれのものでも使用することができる。
The two-component developer used in the method of the present invention includes carrier particles, which are magnetic particles whose surfaces are coated with a resin, such as magnetic particles such as ferrite, and non-magnetic particles, which are made by bonding a charge control agent, an external additive, etc. with a resin. Examples include combinations of toner particles, but the invention is not particularly limited thereto, and any two-component developer used in so-called magnetic brush development can be used.

本発明方法が適用される現像法は、代表的には、現像ス
リーブの内部に磁界発生である固定磁石を内装した回転
スリーブの表面で2成分現像剤を搬送させ、この現像ス
リーブが潜像担体である感光体ドラムと微小間隙を保っ
て対向する表面部分で、内部磁極により該現像スリーブ
上に現像剤の磁気ブラシ(穂立ち)を形成させて、この
磁気ブラシを感光体ドラムの表面に接触摺擦させるか、
近接させるかしながら駆動させて、トナー粒子の感光体
ドラムへの付着を行なわせる方法をいうが、特にこれに
限定されるものではなく、トナー粒子とキャリヤ粒子の
2成分現像剤を用いて接触ないし非接触の現像を行なう
方法であって、交互電界を印加することで有効な現像を
行なうことができるものであれば、磁気ブラシ現像法と
いう通称に限定されるものでもない。
In the developing method to which the method of the present invention is applied, a two-component developer is typically conveyed on the surface of a rotating sleeve equipped with a fixed magnet for generating a magnetic field inside the developing sleeve, and this developing sleeve is used as a latent image carrier. A magnetic brush of developer is formed on the developing sleeve by an internal magnetic pole at the surface facing the photoreceptor drum with a small gap, and this magnetic brush is brought into contact with the surface of the photoreceptor drum. Should I rub it?
This method refers to a method in which toner particles are caused to adhere to a photoreceptor drum by driving them while bringing them close to each other, but the method is not particularly limited to this method. The method is not limited to the common name "magnetic brush development" as long as it is a method of non-contact development and can perform effective development by applying an alternating electric field.

また電界を弱めるための重畳電界を印加することは、基
本となる電界を低く設定してこれを一部強める電界を重
畳するとしても実質的に同じであり、したがって本発明
において「電界を弱める電界を重畳する」とは上記の両
者の場合を包含するものとする。
Furthermore, applying a superimposed electric field to weaken the electric field is substantially the same even if the basic electric field is set low and an electric field that partially strengthens it is superimposed. ``overlapping'' shall include both of the above cases.

(作 用) 本発明の現像方法は、前記の構成をなすことにより、ト
ナーを現像スリーブから感光体ドラムに転移させる方向
に電界を印加する期間の一部において、電界を弱めるこ
とで、画像部へのトナーの過剰供給を調整し、また非画
像部にトナーが付着する傾向を弱めることができる。
(Function) With the above-described configuration, the developing method of the present invention weakens the electric field during a part of the period in which the electric field is applied in the direction of transferring the toner from the developing sleeve to the photoreceptor drum. It is possible to control excessive supply of toner to the image area and reduce the tendency of toner to adhere to non-image areas.

また感光体ドラムから現像スリーブ方向に逆転移させる
方向の電界を印加している期間の一部において、該電界
を弱めることで、階調性に富み、地力ブリが少なく、ま
たエツジの強調が適度に行なわれ中間調における濃度変
化のない均一性に優れた画像が形成できる。
In addition, by weakening the electric field during a part of the period in which the electric field is applied in the direction of reverse transfer from the photoreceptor drum toward the developing sleeve, it is possible to achieve rich gradation, less ground blur, and moderate edge emphasis. It is possible to form images with excellent uniformity without density changes in intermediate tones.

(実施例) 以下本発明を具体的な実施例に基づいて説明する。(Example) The present invention will be explained below based on specific examples.

実施例1 第1図は本発明の一実施例の現像装置の断面図である。Example 1 FIG. 1 is a sectional view of a developing device according to an embodiment of the present invention.

この図に招ける1は静電記録用絶縁ドラムあるいはa−
5e、Cds、ZnO,OPC,a−3Iの様な光導電
絶縁物質層を持つ感光体ドラム(もしくは感光ベルト)
である。この感光体ドラム1は図示しない駆動装置によ
って矢印a方向に回転される。22は感光体ドラム1に
近接されている現像スリーブであり、例えばアルミニウ
ム、5O5318等の非磁性材料で構成されている。
1 in this figure is an insulated drum for electrostatic recording or a-
Photoreceptor drum (or photoreceptor belt) with a layer of photoconductive insulating material such as 5e, Cds, ZnO, OPC, a-3I
It is. This photosensitive drum 1 is rotated in the direction of arrow a by a drive device (not shown). A developing sleeve 22 is located close to the photosensitive drum 1 and is made of a non-magnetic material such as aluminum or 5O5318.

この現像スリーブ22は、現像容器36の図の左下方壁
の位置で容器長手方向(図の奥行方向)、に形成した横
長開口から左略半周面を容器36内へ突入させ、左略半
周面を容器外へ露出させて回転自在に軸受けさせて回転
可能に横設してあり、矢印す方向に回転駆動される。
The developing sleeve 22 has its left approximately half circumferential surface thrust into the container 36 from a horizontally long opening formed in the container longitudinal direction (the depth direction in the figure) at the lower left wall of the developing container 36 in the figure. is exposed outside the container and rotatably mounted on a bearing, and is rotatably installed horizontally, and is driven to rotate in the direction of the arrow.

23は、現像スリーブ22内に図示の位置姿勢に位置決
め1ノて内装された固定磁界発生手段としての固定の永
久磁石(マグネット)であり、現像スリーブ22が回転
駆動されてもこの磁石23は図示の位置・姿勢にそのま
ま固定保持されている。本例のこの磁石23はN極の磁
極23a、S極の磁極23b 、 N極の磁極23cの
361!極を有する。なお磁石23は永久磁石に代えて
電磁石を配設してもよい。本例においては磁石23の表
面磁束密度の垂直成分の極大値を、23a、23c極が
約700ガウス、23b極が850ガウスとした。
Reference numeral 23 denotes a fixed permanent magnet (magnet) as a fixed magnetic field generating means, which is positioned inside the developing sleeve 22 in the position and orientation shown in the figure. It is held fixed in the same position and posture. This magnet 23 in this example has a north magnetic pole 23a, a south magnetic pole 23b, and a north magnetic pole 23c, 361! Has poles. Note that the magnet 23 may be an electromagnet instead of a permanent magnet. In this example, the maximum value of the vertical component of the surface magnetic flux density of the magnet 23 is approximately 700 Gauss for the poles 23a and 23c, and 850 Gauss for the pole 23b.

24は、非磁性ブレードであり、上記現像スリーブ22
を配設した現像剤供給器開口の下縁側に、基部を容器側
壁に固定し、先端側は開口下縁長手よりも容器36の外
側へ突出させて開口下縁長手に沿って配設させた現像剤
規制部材を構成している。この非磁性ブレード24は、
例えば5uS316を横断面からみて「への字」形に曲
げ加工し・たものである。
24 is a non-magnetic blade, and the developing sleeve 22
The base portion is fixed to the side wall of the container on the lower edge side of the opening of the developer supply device in which the developer supply device is disposed, and the tip side is arranged along the longitudinal length of the lower edge of the opening so as to protrude outward from the container 36 than the longitudinal length of the lower edge of the opening. It constitutes a developer regulating member. This non-magnetic blade 24 is
For example, it is made by bending 5uS316 into a ``H'' shape when viewed from a cross section.

27は2成分現像剤の一つの成分をなすキャリヤ粒子で
あり、一般的には粒径が20〜100μm、好ましくは
30〜80μmで抵抗値が107Ωca以上、好ましく
はXO’Ωc111以上のフェライト粒子(最大磁化3
0〜xooemu/g)を樹脂コーティングしたものが
用いられる場合が多く、本例においても後述のようにこ
の範囲のものを使用した。
27 is a carrier particle which is one component of a two-component developer, and is generally a ferrite particle (with a particle size of 20 to 100 μm, preferably 30 to 80 μm, and a resistance value of 107 Ωca or more, preferably XO'Ωc 111 or more). Maximum magnetization 3
0 to xooemu/g) is often used, and in this example, as will be described later, a resin coating was used.

37は2成分現像剤のもう一つの成分である非磁性トナ
ーを示している。
37 indicates a non-magnetic toner which is another component of the two-component developer.

62はトナー濃度検出センサーであり、このセンサー6
2の出力に応じて63のトナー補助ローラーの回転(矢
印C方向に回転する)及び停止を繰り返してトナー・・
の供給を行えるようにしている。
62 is a toner concentration detection sensor;
The toner auxiliary roller 63 repeatedly rotates (rotates in the direction of arrow C) and stops in accordance with the output of step 2, and the toner...
We are making it possible to supply the following.

66は矢印d方向に回転する攪拌部材であり、スクレー
バー67でスリーブ22上から剥離された現像剤と補給
トナーとを混合及び攪拌する。
A stirring member 66 rotates in the direction of arrow d, and mixes and stirs the developer peeled off from the sleeve 22 by the scraper 67 and the replenishment toner.

38はトナー貯蔵容器である。38 is a toner storage container.

以上の構成において、非磁性ブレード24によって規制
された現像剤はさらに補助規制板(図示せず)によって
規制されて現像領域に搬送される。現像後の現像剤はト
ナー濃度検出センサー62によって現像剤中のトナー濃
度が検出される。トナー濃度が低いと補給ローラー63
が回転始めて、トナーを供給する。
In the above configuration, the developer regulated by the non-magnetic blade 24 is further regulated by an auxiliary regulation plate (not shown) and transported to the development area. After development, the toner concentration in the developer is detected by a toner concentration detection sensor 62. If the toner concentration is low, the replenishment roller 63
starts rotating and supplies toner.

なお上記ブレード24としては厚さ1.5mmの非磁性
ステンレスを用い、スリーブ回転方向すに対して極23
aの下漬側に設けた。
The blade 24 is made of non-magnetic stainless steel with a thickness of 1.5 mm, and the pole 23 is made of stainless steel with a thickness of 1.5 mm.
It was installed on the lower side of a.

キャリヤ粒子としては表面にアクリルとフッ素との混合
樹脂を塗布した粒径70〜90μのフェライト(最大磁
化〜56 ea+u/g s抵抗値10’ 〜10’Ω
cm)を用いた。
As carrier particles, ferrite particles with a particle size of 70 to 90μ coated with a mixed resin of acrylic and fluorine on the surface (maximum magnetization ~56 ea+u/g s resistance value 10' to 10'Ω) are used.
cm) was used.

非磁トナーとしては、スチt/ン系樹脂90部にポリブ
ロビレンフ部、カーボンブラック4部を主体とする平均
粒径13μの[・ナー粉体を用いた。
As the non-magnetic toner, a [.-toner powder with an average particle diameter of 13 microns was used, which was mainly composed of 90 parts of a steel T/N resin, a polypropylene part, and 4 parts of carbon black.

更に、感光ドラム1とスリーブ22との間隙を約! m
m、スリーブ22とブレード24との間を0.8mmと
して現像装置を構成させた。
Furthermore, the gap between the photosensitive drum 1 and the sleeve 22 should be approximately ! m
The developing device was constructed with a distance of 0.8 mm between the sleeve 22 and the blade 24.

以上の現像装置を用い、現像条件として、感光ドラムの
潜像電位を画像部−650■、非画像部−150Vに設
定し、現像バイアスとして一200Vの直流電圧に第2
図に示したパルス波形(つまり単純に往復する)基本の
電界の・一部に電界を弱める電界を重畳したパルス波形
)を重畳して現像を行なフた。ここでt1〜1.の長さ
ヲ同一としおのおの60μSeC〜250μsecの範
囲にした時に良好な画像が得られた。言いかえると、1
サイクルの時間(T、=”z  t、)がIs+ 500μsec〜・3 n+secの範囲で良好な画が
得られた。本例の構成においでは、1サイクルのT。
Using the above developing device, the latent image potential of the photosensitive drum was set to -650V in the image area and -150V in the non-image area as the development conditions, and the developing bias was set to -200V DC voltage.
Development was carried out by superimposing the pulse waveform shown in the figure (that is, a pulse waveform in which an electric field that weakens the electric field is superimposed on a part of the basic electric field that simply reciprocates). Here, t1-1. Good images were obtained when the lengths were the same and each ranged from 60 .mu.Sec to 250 .mu.sec. In other words, 1
Good images were obtained when the cycle time (T, = "z t,) was in the range of Is+ 500 μsec to .3 n+sec. In the configuration of this example, T of 1 cycle.

が500μSeCより短かいと前述した従来例の単純な
交互電界を印加したのと類似して画像が硬調でγが立っ
て来る傾向となる。逆にT、が3 m5ec以上の時間
になるとトナーやキャリヤがパルスの変化に充分追従出
来ることになり、感光体ドラムに飛mしたまま戻らない
トナーやキャリヤが発生する結果としてカブリやキャリ
ヤ付着の発生する傾向がみられる。
If it is shorter than 500 μSeC, the image tends to be high contrast and γ tends to rise, similar to the case where a simple alternating electric field is applied in the conventional example described above. On the other hand, when T is longer than 3 m5ec, the toner and carrier can sufficiently follow the changes in the pulse, and as a result, toner and carrier fly to the photoreceptor drum and do not return, resulting in fogging and carrier adhesion. There is a tendency for this to occur.

ここで単に往復する交互電界のパルスを印加する場合と
、これに、弱める電界を重畳する本発明現像法の場合と
の差異を本例に促して説明する。
Here, the difference between the case where pulses of an alternating electric field are simply applied and the case where a weakening electric field is superimposed on the pulses of the present invention will be explained using this example.

交互電界を与える複数のパルス波形の電圧を60μse
c〜250μsecの短い周期で印加すると、現像剤に
は高周波の電界が加わる。ここでキャリヤとトナーは逆
極性に帯電しているので、キャリヤとトナーは逆方向に
上記の高周波で振動を繰り返し、電荷を与え合う、ここ
でキャリヤは現像スリーブ側の磁石による磁力で拘束さ
れており、しかもトナーよりも体積、比重が相当に大き
いので、キャリヤの回りをトナーの粒子がクラウド状に
覆フた状態となる。
The voltage of multiple pulse waveforms giving an alternating electric field is set at 60 μs.
When applied at a short period of c~250 μsec, a high frequency electric field is applied to the developer. Here, since the carrier and toner are charged with opposite polarities, the carrier and toner repeatedly vibrate in opposite directions at the above-mentioned high frequency and give each other electric charges.Here, the carrier is restrained by the magnetic force of the magnet on the developing sleeve side. Furthermore, since the volume and specific gravity of the carrier are considerably larger than that of the toner, toner particles surround the carrier in a cloud-like state.

一方従来単純な交互電界を印加した現像で上記の範囲に
周波数を上げたとすると、トナーはある閾値を境に二値
的に飛翔するか、しないかの動きを呈する傾向となり、
結果的にγの立った硬調な画像となる。これに対して本
実施例では、上述のように現像剤担持体側から、潜像担
持体にトナーが転位する期間の一部および逆転位の期間
の一部で電界が弱められているため、トナーのクラウド
が、現像スリーブと、感光体ドラムの間に亘って発生し
、ソフトタッチなりラウド現像に近い状態を繰り返すこ
とになる。
On the other hand, if the frequency is raised to the above range in conventional development by applying a simple alternating electric field, the toner tends to either fly or not fly in a binary manner after reaching a certain threshold.
The result is a high-contrast image with a strong γ. On the other hand, in this embodiment, as described above, the electric field is weakened during a part of the period in which toner is transferred from the developer carrier side to the latent image carrier and in a part of the period in which the toner is reversely transferred. A cloud occurs between the developing sleeve and the photoreceptor drum, and a state similar to soft touch or loud development is repeated.

しかも、トナーは前述した様に高周波のパルスによりト
ナーとキャリアとの摩擦回数を増してキャリヤによりし
っかり帯電しているのでカブリも発生しない、また短い
パルスで飛翔する信号が与えられているのでキャリヤは
低周波でパルスが加えられた場合に比較して飛翔する力
を受ける時間が短くなり極端にドラム側へ転位する傾向
は抑制され、キャリヤの付着もなくなるという効果も得
られる。
Moreover, as mentioned above, the toner is more firmly charged by the carrier by increasing the number of times of friction between the toner and the carrier using high-frequency pulses, so fogging does not occur.Also, since the toner is given a flying signal with short pulses, the carrier is Compared to the case where a pulse is applied at a low frequency, the time required for receiving the flying force is shortened, and the tendency to excessively displace to the drum side is suppressed, and the adhesion of carriers is also eliminated.

以上説明した様に、本実施例によって階調性があり、カ
ブリもキャリヤの付着しない高画質の画像が得られる様
になった。第9図に一例として、従来のバイアス(第1
0図)と本実施例のバイアス(第11図)でのD−Dカ
ーブを示す本実施例の前述した効果により、γの寝た階
調性のある画像が得られるようになフた事が分る。
As explained above, this embodiment makes it possible to obtain high-quality images with gradation, no fog, and no carrier adhesion. As an example, FIG. 9 shows the conventional bias (first
0) and the bias (Fig. 11) of this example. Due to the above-mentioned effects of this example, it was possible to obtain an image with a flat gradation of γ. I understand.

実施例2 第3図は本発明の他の実施例の現像装置の断面図を示し
ている。この第3図の例の装置は第1図の実施例1の装
置と異なり、現像スリーブ上で磁性粒子とトナー粒子と
を混合及び攪拌する方式の現像装置である。
Embodiment 2 FIG. 3 shows a sectional view of a developing device according to another embodiment of the present invention. The apparatus of the example shown in FIG. 3 is different from the apparatus of Embodiment 1 shown in FIG. 1, and is a developing apparatus of a type in which magnetic particles and toner particles are mixed and stirred on a developing sleeve.

以下、この装置に本発明を適用した場合を説明する。こ
の図に招ける101は静電記録用絶縁ドラムあるいはa
−5o、Cds、ZnO,OPC,a−51の様な光導
電絶縁物貫層を持つ感光体ドラム(もしくは感光ベルト
)である、この感光体ドラム101は図示しない駆動装
置によって矢印a方向に回転される。122は感光体ド
ラム101に近接されている現像スリーブであり、例え
ばアルミニウム、5O5318等の非磁性材料で構成さ
れている。この現像スリーブ122は、現像容器136
の図の左下方壁の位置で容器長手方向(図の奥行方向)
に形成した横長開口から右略半周面を容器136内へ突
入させ、左略半周面を容器外へ露出させて回転自在に軸
受けさせて回転可能に横設してあり、矢印す方向に回転
駆動される。
A case in which the present invention is applied to this device will be described below. 101 in this figure is an insulated drum for electrostatic recording or a
The photosensitive drum 101, which is a photosensitive drum (or photosensitive belt) having a photoconductive insulating layer such as -5o, Cds, ZnO, OPC, a-51, is rotated in the direction of arrow a by a drive device (not shown). be done. A developing sleeve 122 is located close to the photosensitive drum 101 and is made of a non-magnetic material such as aluminum or 5O5318. This developing sleeve 122 is connected to a developing container 136.
In the longitudinal direction of the container (in the depth direction of the figure) at the lower left wall in the figure.
The right half-circumferential surface is inserted into the container 136 through the horizontally elongated opening formed in the container 136, and the left half-circumferential surface is exposed to the outside of the container. be done.

123は、現像スリーブ122内に図示の位置姿勢に位
置決めして内装された固定磁界発生手段としての固定の
永久磁石(マグネット)であり、現像スリーブ122が
回転駆動されてもこの磁石123は図示の位置・姿勢に
そのまま固定保持されている0本例のこの磁石123は
N極の磁極123a、 S極の磁極123b、 N極の
磁極123c、 S極の磁極123dの4磁極を有する
。なお磁石123は永久磁石に代えて電磁石を配設して
もよい。
Reference numeral 123 denotes a fixed permanent magnet (magnet) as a fixed magnetic field generating means, which is positioned and housed in the developing sleeve 122 in the illustrated position and orientation. This example magnet 123, which is held fixed in its position and orientation, has four magnetic poles: an N-pole magnetic pole 123a, an S-pole magnetic pole 123b, an N-pole magnetic pole 123c, and an S-pole magnetic pole 123d. Note that the magnet 123 may be an electromagnet instead of a permanent magnet.

124は、非磁性ブレードであり、上記現像スリーブ1
22を配設した現像剤供給器開口の上縁側に、基部を容
器側壁に固定し、先端側は開口上縁位置よりも容器13
6の外側へ突出させ゛℃開口上縁長手に沿2て配設させ
た現像剤規制部材を構成している。この非磁性ブレード
124は、例えば5uS31Bを横断面からみて「への
字」形に曲げ加工したものである。
124 is a non-magnetic blade, which is attached to the developing sleeve 1
The base portion is fixed to the side wall of the container on the upper edge side of the opening of the developer supply device in which the developer supply device 22 is disposed, and the tip side is lower than the upper edge position of the opening.
A developer regulating member is arranged along the longitudinal direction of the upper edge of the opening. This non-magnetic blade 124 is made by bending, for example, 5uS31B into a "F" shape when viewed from a cross section.

126は非磁性ブレード124の下面側に上面を接触さ
せ前端面を現像剤案内面126aとした磁性粒子限定部
材である。
Reference numeral 126 denotes a magnetic particle limiting member whose upper surface is in contact with the lower surface side of the non-magnetic blade 124 and whose front end surface is a developer guiding surface 126a.

I27は2成分現偉剤の一つの成分をなすキャリヤ粒子
であり、本例の場合には粒径が30〜100μm1好ま
しくは40〜70μmで抵抗値が107Ωcm以上、好
ましくは工0°ΩCff1以上のフェライト粒子(最大
磁化a o emu/g )を樹脂コーティングしたも
のが好まし・く用いられ得る。
I27 is a carrier particle constituting one component of the two-component developing agent, and in this example, the particle size is 30 to 100 μm, preferably 40 to 70 μm, and the resistance value is 107 Ωcm or more, preferably 0°ΩCff1 or more. Ferrite particles (maximum magnetization a o emu/g) coated with a resin can be preferably used.

137は2成分現像剤のもう一つの成分である非磁性現
像剤トナーを示している。
137 indicates a non-magnetic developer toner which is another component of the two-component developer.

131は、現像スリーブ122を配設した現像容器13
6下部からのキャリヤ粒子12″lないしは非磁性トナ
ー粒子131の漏出を防止するために廓像容器下部内面
に現像スリーブ122に対向し°C配設された磁性体で
あり、例えば鉄板にメツキを施したもので形成される。
131 is a developing container 13 in which a developing sleeve 122 is arranged.
In order to prevent carrier particles 12''l or non-magnetic toner particles 131 from leaking from the lower part of the image container 6, it is a magnetic material placed on the inner surface of the lower part of the image container facing the developing sleeve 122. It is formed by what has been applied.

これにより磁性体131とS極性の磁i 123dとの
間の磁界でキャリヤ粒子127の回収と澗れ防止を達成
するシール効果が得られる。
As a result, a sealing effect is obtained in which the carrier particles 127 are recovered and prevented from sagging by the magnetic field between the magnetic body 131 and the S-polarity magnet i 123d.

139は現像スリーブ122内の固定磁極123により
形成されたキャリヤ粒子のブラシ部分へトナーを供給す
るトナー供給部材であり、回転自在に軸受した板金にゴ
ムシートを貼り付?づ現像容器下面を掃くが如くトナー
を搬送する。このトナー供給部材139には、トナー貯
蔵客器138中のトナー搬送部材(図示せず)Cよって
トナーが供給される。
Reference numeral 139 denotes a toner supply member that supplies toner to the brush portion of the carrier particles formed by the fixed magnetic pole 123 in the developing sleeve 122, and is made by pasting a rubber sheet on a rotatably bearing plate. The toner is conveyed as if sweeping the bottom surface of the developer container. Toner is supplied to the toner supply member 139 by a toner transport member (not shown) C in the toner storage device 138.

138.135はそれぞれトナー貯蔵容器、磁性粒子貯
蔵容器である。
138 and 135 are a toner storage container and a magnetic particle storage container, respectively.

140は現像容器136下部部分!=?:溜るトナーを
封止するシール部材であり、弾性を有していて現像スリ
ーブ122の回転方向に向って曲がっており、現像スリ
ーブ122表面を弾性的に押圧している。このシール部
材140は、現像剤の容器内部側への進入を許可するよ
うに、現像スリーブとの接触域で該現像スリーブ回転方
向下流側に端部を有している。
140 is the lower part of the developer container 136! =? : A sealing member that seals the accumulated toner, has elasticity, is bent toward the rotational direction of the developing sleeve 122, and elastically presses the surface of the developing sleeve 122. This sealing member 140 has an end on the downstream side in the rotational direction of the developing sleeve in a contact area with the developing sleeve so as to allow the developer to enter the inside of the container.

13Gは、現像工程で発生した浮遊現像剤を現像剤と同
極性の電圧を印加して感光体ドラム側に付看させ飛散を
防止する飛散防止電極板である。
Reference numeral 13G denotes a scattering prevention electrode plate that applies a voltage of the same polarity as the developer to the floating developer generated in the developing process to stick it to the photoreceptor drum side and prevent it from scattering.

又、S磁極123dは、磁性部材131との間に一方か
ら他方に磁騨を形成するための磁性シール用磁界発生手
段であり、磁性部材131に対して一部が対向する。磁
性部材131は現像側容器の現像剤収納部の実質的な端
部をなし、現像装置の下方に位置し、この周辺では、回
収された(磁性)キャリヤ粒子の移動に伴なフて、現像
スリーブ表面の現像剤中に、容器内下方に位置するトナ
ー粒子が取り込まれる。従って、キャリヤ粒子の安定し
た回収は、現像能力を安定化する効果をもたらすので、
この点でも本発明方法の有効性が期待できる。
Further, the S magnetic pole 123d is a magnetic field generating means for magnetic sealing to form a magnetic field from one side to the other between the S magnetic pole 123d and the magnetic member 131, and a part thereof faces the magnetic member 131. The magnetic member 131 constitutes a substantial end of the developer accommodating portion of the developer-side container, and is located below the developing device. Toner particles located in the lower part of the container are incorporated into the developer on the surface of the sleeve. Therefore, stable recovery of carrier particles has the effect of stabilizing the developing ability.
The effectiveness of the method of the present invention can also be expected in this respect.

この磁性部材131には、「<」あるいはr L J字
形状を有し、鉄等の永久磁化されでいない磁性体や非磁
性体を変形させることによって弱い磁性を帯びたものが
適用可能である。
This magnetic member 131 may have a "<" or r L J shape, and may be made of a magnetic material that is not permanently magnetized, such as iron, or that is made weakly magnetic by deforming a non-magnetic material. .

つまり、磁性部材131はキャリヤ粒子の拘束を行いつ
つキャリヤ粒子の損失を防止しさらにキャリヤ粒子の回
収を容易にするので、現像剤容器内のトナー粒子が容器
内から漏れるのを防止できる。
In other words, the magnetic member 131 restrains the carrier particles, prevents the loss of the carrier particles, and facilitates recovery of the carrier particles, so that the toner particles in the developer container can be prevented from leaking from inside the container.

前記構成において、磁極123dは前記のごとく配置す
ることによって、磁極123aとの関係で特に好ましい
効果が得られる。すなわち、容器136の収納部底部と
磁極123dとの上記関係によって、磁気ブラシが12
1内で(単に停滞している状態に比較して)粗の状態で
形成されないので、キャリヤ粒子中へのトナー粒子の取
込み量が過剰になることがない効果が得られる。過剰取
込みはトナーの帯電不足を招ぎ、かぶり発生の原因とな
る。
In the above configuration, by arranging the magnetic pole 123d as described above, a particularly favorable effect can be obtained in relation to the magnetic pole 123a. That is, due to the above relationship between the bottom of the container 136 and the magnetic pole 123d, the magnetic brush
Since the toner particles are not formed in a coarse state (compared to a merely stagnant state) within the carrier particles, an effect is obtained in which the amount of toner particles taken into the carrier particles does not become excessive. Excessive uptake results in insufficient charging of the toner, causing fogging.

なおこの構成は現像剤容器内にキャリヤ粒子と非磁性あ
るいは弱磁性のトナーが混在している場合にも有効であ
る。
Note that this configuration is also effective when carrier particles and nonmagnetic or weakly magnetic toner coexist in the developer container.

実験によると、現像スリーブ122と磁性部材131 
との距1112.5amで、キャリヤ粒子は完全に回収
され、トナー粒子の漏れは全く見られず、安定した現像
を達成できることが分る。
According to experiments, the developing sleeve 122 and the magnetic member 131
At a distance of 1112.5 am, the carrier particles are completely recovered and no leakage of toner particles is observed, indicating that stable development can be achieved.

非磁性ブレード124の端部と現像スリーブ122面と
の前記距* d2は50〜800 u m、好ましくは
150〜500μmである。この距離が50μmより小
さいとキャリヤ粒子がこの間に詰まり現像剤層にムラを
生じやすいと共に良好な現像を行うのに必要な現像剤を
塗布することが出来ず濃度の薄いムラの多い現像画像し
か得られない欠点がある。また800μmより大きいと
現像スリーブ122上へ塗布される現像剤量が増加し所
定の現像剤層厚の規制が行えず、感光体ドラムへのキャ
リヤ粒子付着が多くなると共に現像剤の循環、現像剤限
定部材126により現像規制が弱まりトナーのトリボが
不足しカプリやすくなる欠点がある。
The distance *d2 between the end of the non-magnetic blade 124 and the surface of the developing sleeve 122 is 50 to 800 μm, preferably 150 to 500 μm. If this distance is smaller than 50 μm, carrier particles tend to clog between the gaps, causing unevenness in the developer layer, and the developer necessary for good development cannot be applied, resulting in a developed image with a low density and a lot of unevenness. There are drawbacks that cannot be avoided. If the diameter is larger than 800 μm, the amount of developer applied onto the developing sleeve 122 increases, making it impossible to regulate the thickness of the developer layer to a predetermined value, increasing the amount of carrier particles attached to the photoreceptor drum, and increasing the circulation of the developer. The limiting member 126 weakens the development regulation, and there is a drawback that toner triboelectricity is insufficient and capping is likely to occur.

固定配置された磁極123aは、バッキング状態のキャ
リヤ粒子を磁力線に沿って再配置する。
The fixedly placed magnetic poles 123a reposition the bucking carrier particles along the magnetic field lines.

該空間でのバッキング状態はトリボ賦与に対しては不安
定なところがあり、安定化させるためには常に一定のバ
ッキング状態を必要とする。
The backing state in this space is unstable with respect to tribo-imposition, and a constant backing state is always required to stabilize it.

これは現像スリーブ122上をほぼ接線方向に搬送され
てきたキャリヤ粒子を該方向と直交する力で磁気ブラシ
を形成するため、キャリヤ粒子への攪拌効果はもちろん
のこと、はぐし効果も働鮒、上記トナーへのトリボ賦与
及びキャリヤ粒子層の塗布の均一化・安定化がさらに促
進される。この時、周辺の構成によって集中せしめられ
た現像剤が多大な圧力を受けたままであると現像剤がつ
まり過ぎる問題があるが、磁極123aの最大磁力を発
生する部分が案内面126aに対向することによって、
規制領域中における過大な圧力集中を防止し、現像剤の
集中と安定した高密度の磁性粒子存在割合を維持できる
ものと考えられる。
This is because a magnetic brush is formed by applying a force perpendicular to the direction of the carrier particles conveyed on the developing sleeve 122 in a substantially tangential direction, which not only has a stirring effect on the carrier particles but also has a peeling effect. The uniformity and stabilization of the tribo-imparting to the toner and the application of the carrier particle layer are further promoted. At this time, if the concentrated developer remains under great pressure due to the surrounding structure, there is a problem that the developer will become clogged. By,
It is believed that excessive pressure concentration in the regulated area can be prevented, and developer concentration and stable high-density magnetic particle existence ratio can be maintained.

上記の規制領域によって現像スリーブ表面には、安定し
た量のキャリヤ粒子と十分に帯電したトナー粒子とが現
像剤薄層として形成できる。従って現像領域での現像効
果は安定したものとなる0以上により現像部に搬送され
た現像剤の内掛なくとも前記現像スリーブ122表面に
担持されたトナー粒子を感光体ドラム101に転穆させ
るために、第4図に示した交互電界を前記現像部に印加
することで良好な現像を行なうことができる。本例の構
成において、潜像条件は実施例1と同一にし、交互電界
として、第4図に示した波形とした以外は実施例と同一
のパルスバイアスを印加したところ非常に良好な画像が
得られた。
Due to the above-mentioned restricted area, a stable amount of carrier particles and sufficiently charged toner particles can be formed as a thin layer of developer on the surface of the developer sleeve. Therefore, the development effect in the development area is stable.The toner particles carried on the surface of the development sleeve 122 are transferred to the photoreceptor drum 101 even if the developer conveyed to the development section does not fall within the range of 0 or more. Furthermore, by applying the alternating electric field shown in FIG. 4 to the developing section, good development can be performed. In the configuration of this example, the latent image conditions were the same as in Example 1, and when the same pulse bias as in Example was applied except for the alternating electric field and the waveform shown in Figure 4, a very good image was obtained. It was done.

なお第3図の構成は現像剤限定部材126の非磁性ブレ
ード124側に磁性体150を設置した場合として示し
であるが、この場合、磁性体150は磁極123aに対
向する位置に設けるのは好ましくない。なぜならば対向
していると、磁極123aとの間に強い集中磁界が発生
し、上記磁極123aによるキャリヤ粒子の攪拌及びほ
ぐし効果が低減するからである。しかし、規制部に磁性
体を設は現像スリーブ内部磁石123との間でキャリヤ
粒子の磁気的規制を行うことは規制部材のスリーブとの
間隙公差の拡大になり、有効的である。又、公差のみな
らず、規制部材とスリーブ間鎖長自体も拡大することが
でき、非磁性ブレードのみの場合よりも70〜100μ
程度拡大することができる。又、キャリヤ粒子ないしは
現像スリーブ122上に付着したトナーを比較すると、
現像スリーブ122上に付着したトナーの帯電電荷量は
キャリヤ粒子に付着したものよりも小さい。この理由は
現像スリーブ122の6動と供に、キャリヤ粒子も搬送
されるため、現像スリーブ122上のトナーがキャリヤ
粒子によって摺擦される機会が少なくなっているためで
ある。この現像スリーブ122上のトナーを所定の値に
まで持ち上げるためには、現像スリーブ122上のトナ
ーを積極的に摺擦してやる必要がある。即ち、現像スリ
ーブ表面近傍で該現像スリーブの移動に反して相対速度
のずれを生じさせるキャリヤ粒子の存在が必要となる。
Note that the configuration in FIG. 3 is shown in the case where the magnetic body 150 is installed on the non-magnetic blade 124 side of the developer limiting member 126, but in this case, it is preferable that the magnetic body 150 is installed at a position facing the magnetic pole 123a. do not have. This is because if they face each other, a strong concentrated magnetic field will be generated between them and the magnetic pole 123a, reducing the effect of stirring and loosening the carrier particles by the magnetic pole 123a. However, it is effective to provide a magnetic material in the regulating portion to magnetically regulate the carrier particles between the developing sleeve internal magnet 123 and the gap tolerance between the regulating member and the sleeve is increased. In addition, not only the tolerance but also the length of the chain between the regulating member and the sleeve itself can be expanded, which is 70 to 100μ compared to the case of only non-magnetic blades.
The degree can be expanded. Also, when comparing the toner deposited on the carrier particles or the developing sleeve 122,
The amount of charge on the toner deposited on the developer sleeve 122 is smaller than that on the carrier particles. The reason for this is that the carrier particles are also transported along with the six movements of the developing sleeve 122, so there is less chance that the toner on the developing sleeve 122 will be rubbed by the carrier particles. In order to lift the toner on the developing sleeve 122 to a predetermined value, it is necessary to actively rub the toner on the developing sleeve 122. That is, it is necessary to have carrier particles near the surface of the developing sleeve that cause a shift in relative velocity against the movement of the developing sleeve.

しかし、単純にキャリヤ粒子の搬送性を低下させること
は前述のトナーの取り込み作用を考慮すると不可能であ
る。又、規制部で上述の様にスリーブ内磁極123aに
対向して磁性体を配置し、集中磁界を発生させキャリヤ
粒子の現像スリーブ上への摺擦力を向上することも上述
の如く、現像剤循環規制部材26のつくる空間に磁極の
最大磁力発生部を配置する効果を低減させる。
However, it is impossible to simply reduce the transportability of carrier particles, considering the aforementioned toner uptake effect. In addition, as described above, a magnetic material may be disposed in the regulating portion facing the magnetic pole 123a in the sleeve to generate a concentrated magnetic field and improve the sliding force of the carrier particles on the developing sleeve. The effect of arranging the maximum magnetic force generating portion of the magnetic pole in the space created by the circulation regulating member 26 is reduced.

そこで本実施例において磁極123aよりも現像スリー
ブ回転方向に関して下流側に該磁性体150を設け、磁
極123aのブレード側の磁力線がほぼ現像スリーブ表
面の接線方向に集中する如く構成した。これにより現像
スリーブ表面近傍のみのキャリヤ粒子が現像スリーブ表
面に沿って磁気ブラシを形成し、現像スリーブ上のトナ
ーを摺擦し、現像スリーブ上のトナーのトリボ賦与を高
めることができる。
Therefore, in this embodiment, the magnetic body 150 is provided downstream of the magnetic pole 123a in the rotational direction of the developing sleeve, so that the lines of magnetic force on the blade side of the magnetic pole 123a are concentrated approximately in the tangential direction of the surface of the developing sleeve. As a result, the carrier particles only near the surface of the developing sleeve form a magnetic brush along the surface of the developing sleeve and rub the toner on the developing sleeve, thereby increasing the triboelectricity of the toner on the developing sleeve.

このような構成は、本発明方法の重畳した交互電界の印
加による効果と相まって一層優れた画像の形成に貢献す
るものとなる。
Such a configuration, in combination with the effect of applying superimposed alternating electric fields in the method of the present invention, contributes to the formation of even better images.

尚、磁極123aの磁束密度は600G以上、好ましく
は700 G以上が好ましい、これは磁性粒子層のトナ
ーコンテンツ変化に対して現像剤の塗布状態がカッi・
磁極の磁束密度が高い程安定する傾向にあるからである
。特にトナーコンテンツ維持のために自動トナー補給装
置を持たない現像装置に於いては800G以上の磁束密
度であることが好ましい。
The magnetic flux density of the magnetic pole 123a is preferably 600 G or more, preferably 700 G or more.
This is because the higher the magnetic flux density of the magnetic pole, the more stable it tends to be. In particular, in a developing device that does not have an automatic toner replenishment device to maintain toner content, it is preferable that the magnetic flux density be 800 G or more.

第3図に於いて1ift極123cは現像磁極であるが
、この現像磁極は、はぼ現像部に位置し、磁性粒子の潜
像への付着を防止する為、800 G以上の磁束密度と
するのが好ましい場合が多い。
In Figure 3, the 1ift pole 123c is a developing magnetic pole, which is located in the developing area and has a magnetic flux density of 800 G or more to prevent magnetic particles from adhering to the latent image. is often preferable.

実施例3 第5図に示した大略第1図と同様の構成の現像装置を用
い、感光体ドラム201と現像スリーブ222との距離
を500μmに設定し、現像剤層の厚さを感光体ドラム
201に最も接近する位置において400μmとなるよ
うに非磁性ブレード224で規制した(本例では非接触
現像が行なわれる)、現像剤には平均粒径8μmの(非
磁性)トナー粒子と(磁性)キャリヤを混合したものを
用い、トナー粒子の濃度比は30wt%にした。なお、
キャリヤ粒子中の磁性粉の含有率は70wt%にし、平
均粒径50μmの粒子を用いた。更に、磁極の配置は第
5図のように磁極間がドラムに対向した位置とし、磁極
N、とS、の磁界の強さを垂直方向の磁界成分が700
ガウスとなるように設定した。またこの時の磁極間の水
平方向の磁界の強さは610ガウスとした。
Example 3 Using a developing device shown in FIG. 5, which has roughly the same configuration as that in FIG. The developer contains (non-magnetic) toner particles with an average particle size of 8 μm and (magnetic) toner particles. A mixture of carrier was used, and the concentration ratio of toner particles was set to 30 wt%. In addition,
The content of magnetic powder in the carrier particles was 70 wt%, and particles with an average particle size of 50 μm were used. Furthermore, the magnetic poles are arranged so that the magnetic poles face the drum as shown in Figure 5, and the magnetic field strength of the magnetic poles N and S is such that the vertical magnetic field component is 700.
It was set to be Gaussian. Further, the strength of the horizontal magnetic field between the magnetic poles at this time was 610 Gauss.

この条件下で、画像部の潜像電位が一800V。Under this condition, the latent image potential of the image area is 1800V.

非画像部電位がOVの時、非磁性トナーには正極性に帯
電する粒子を用い、現像バイアス電圧として第6図に示
す波形のパルスバイアスを印加したところ良好な画像が
得られた。なお本実施例ではパルスの幅と値を実施例1
,2で示した接触現像の場合よりも大きく設定しである
When the non-image area potential was OV, positively charged particles were used as the non-magnetic toner, and a pulse bias having the waveform shown in FIG. 6 was applied as the developing bias voltage, and a good image was obtained. Note that in this example, the pulse width and value were set as in Example 1.
, 2 is set larger than the case of contact development shown in 2.

これは本例が非接触現像のものであることに対応して現
像効率を上げる為である。
This is to increase the development efficiency since this example uses non-contact development.

以上説明した各側では、転位、逆転位の各期間の中間で
重畳した電界を弱めるための重畳電界のパルス幅も設計
的には重要な要素の一つとなるが、本発明方法は、重畳
した交互電界によりクラウド現像に近い現像状態を作り
出すことを一つの特徴とするものであり、上記要素ある
いは交互電界の1サイクルの周期T、=Σt。
On each side explained above, the pulse width of the superimposed electric field to weaken the superimposed electric field in the middle of each period of dislocation and reverse transposition is also an important factor in design, but the method of the present invention One of the features is that a development state close to cloud development is created by alternating electric fields, and the period T, = Σt, of one cycle of the above elements or alternating electric fields.

直ml は必要な範囲で設計的に定めればよい。一般的には一サ
イクルを500 μsec 〜3 m5ecの範囲とし
、パルス電圧印加方式では電界を弱める重畳電界を転位
、逆転の各期間で1パルス以上とすることがよいが、何
パルスあっても良い。1サイクルの範囲での電位の値が
全て異なっていても良い勿論差支えないし、工法波形等
のものでもよい。
Direct ml may be determined by design within a necessary range. Generally, one cycle is in the range of 500 μsec to 3 m5ec, and in the pulse voltage application method, it is preferable that the superimposed electric field that weakens the electric field be one or more pulses in each period of transposition and reversal, but any number of pulses may be used. . It goes without saying that all the potential values within one cycle may be different, and a construction method waveform or the like may be used.

第7図、第8図は使用可能な変形の波形の例を示してい
る。
FIGS. 7 and 8 show examples of usable modified waveforms.

本発明は、上述した各構成の任意の組合せを含むことは
言うまでもない。
It goes without saying that the present invention includes any combination of the above-mentioned configurations.

また本発明は感光体に転移したトナーがスリーブ上に逆
転移するものばかりでなく、感光体から離脱してスリー
ブまで到達しないものにも適用できる。
Further, the present invention can be applied not only to a toner in which the toner transferred to the photoconductor is reversely transferred onto the sleeve, but also to a device in which the toner is separated from the photoconductor and does not reach the sleeve.

[発明の効果] 以上説明した様に、本発明の現像方法は、2成分現像剤
を用いて行なう現像方法において、現像スリーブと感光
体ドラムの間に交互電界を印加して現像スリーブから感
光体ドラムへのトナーの転位、およびこれとは反対方向
のトナー逆転位を与える場合に、これらのトナー転位、
逆転値の期間の一部に、電界を弱めるため重畳電界を与
えるようにしたものであり、これによりトナーの好まし
い往復参勤が現われ、結果としてカブリやキャリヤ付着
がなく、かつ階調性に優れた画像が得られるという効果
がある。
[Effects of the Invention] As explained above, the developing method of the present invention is a developing method using a two-component developer, in which an alternating electric field is applied between the developing sleeve and the photoreceptor drum to remove the photoreceptor from the developing sleeve. These toner dislocations provide for toner dislocation onto the drum and toner reverse translocation in the opposite direction;
A superimposed electric field is applied to weaken the electric field during a part of the period of the reversal value, and this results in a favorable reciprocating movement of the toner, resulting in no fogging or carrier adhesion, and excellent gradation. This has the effect that an image can be obtained.

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

第1図は本発明方法の実施に用いる現像装置の概要を示
した実施例1の説明図、 第2図は、第4図、第6図は各実施例1゜2.3のパル
ス電圧の波形説明図、 第3図及び第5図は実施例2.3の実施に用いる現像装
置の概要を示した説明図、第7図、第8rItJは本発
明方法で用いられる交互電界の他の例を示した図、第9
図は従来のバイアスと第1実施例のバイアスでのD−D
カーブを示す図、第10図および第11図はそれぞれ従
来および第1実施例のバイアスを示す図である。 である。 1・・・感光体ドラム、22・・・現像スリーブ、23
・・・磁石、    27−・・キャリヤ粒子、37・
・・トナー粒子、36・・・現像容器。 第1図 s 探乙 第3図 −rs −TS s 第9図 大すシ゛ナル11度 −by) ■/10第10図 第11図
FIG. 1 is an explanatory diagram of Example 1 showing an outline of the developing device used to carry out the method of the present invention, FIG. 2 is an explanatory diagram of Example 1, FIG. Waveform explanatory diagrams. Figures 3 and 5 are explanatory diagrams showing the outline of the developing device used in the implementation of Example 2.3. Figures 7 and 8 rItJ are other examples of alternating electric fields used in the method of the present invention. Figure 9 showing
The diagram shows D-D with the conventional bias and the bias of the first embodiment.
The diagrams showing the curves, FIG. 10 and FIG. 11 are diagrams showing the bias of the conventional method and the first embodiment, respectively. It is. 1... Photosensitive drum, 22... Developing sleeve, 23
...Magnet, 27-...Carrier particle, 37.
...Toner particles, 36...Developer container. Fig. 1 s Exploration Fig. 3 -rs -TS s Fig. 9 Large signal 11 degrees -by) ■/10 Fig. 10 Fig. 11

Claims (1)

【特許請求の範囲】 1 顕画剤としてのトナー粒子とキャリヤ粒子とからな
る2成分現像剤を表面に担持して搬送する現像剤担持体
と、静電潜像担持体とを、微小な間隙を保ちつつ移動す
る関係に配置すると共にこの間隙部で現像剤担持体上に
上記現像剤の磁気ブラシを形成させ、これら現像剤担持
体と静電潜像担持体の間に、現像剤担持体から静電潜像
担持体にトナー粒子を転移させる方向に電界を印加する
期間と、該転移とは反対にトナー粒子を静電像担持体か
ら離脱させる方向に電界を印加する期間とを、交互に繰
返し印加しながら現像を行なう方式の現像方法において
、 上記トナー粒子を転移させる方向に電界を印加する期間
の一部、及びトナー粒子を静電像担持体から離脱させる
方向に電界を印加する期間の一部に少なくともいずれか
一方の期間において該電界を弱める電界を重畳させるこ
とを特徴とする現像方法。
[Scope of Claims] 1. A developer carrier carrying and transporting a two-component developer consisting of toner particles and carrier particles as a developing agent on its surface and an electrostatic latent image carrier are separated by a minute gap. The magnetic brush of the developer is formed on the developer carrier in this gap, and the developer carrier is placed between the developer carrier and the electrostatic latent image carrier. A period in which an electric field is applied in a direction in which toner particles are transferred from the electrostatic latent image bearing member to the electrostatic latent image bearing member, and a period in which an electric field is applied in a direction in which the toner particles are separated from the electrostatic latent image bearing member in the opposite direction to the transfer are alternately applied. In a developing method in which development is performed while repeatedly applying an electric field, a part of the period during which the electric field is applied in the direction to transfer the toner particles, and a period during which the electric field is applied in the direction to separate the toner particles from the electrostatic image bearing member. A developing method characterized by superimposing an electric field that weakens the electric field in at least one period on a part of the electric field.
JP63176595A 1988-07-15 1988-07-15 Development method Expired - Fee Related JP2510247B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63176595A JP2510247B2 (en) 1988-07-15 1988-07-15 Development method

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63176595A JP2510247B2 (en) 1988-07-15 1988-07-15 Development method

Publications (2)

Publication Number Publication Date
JPH0225856A true JPH0225856A (en) 1990-01-29
JP2510247B2 JP2510247B2 (en) 1996-06-26

Family

ID=16016315

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63176595A Expired - Fee Related JP2510247B2 (en) 1988-07-15 1988-07-15 Development method

Country Status (1)

Country Link
JP (1) JP2510247B2 (en)

Cited By (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006184265A (en) * 2004-12-03 2006-07-13 Adonisu Denki:Kk Oral odor measuring instrument and method, and odor measuring instrument and method
JP2009204867A (en) * 2008-02-27 2009-09-10 Sharp Corp Developing device and image forming apparatus
JP2010097140A (en) * 2008-10-20 2010-04-30 Fuji Xerox Co Ltd Developing device and image forming apparatus

Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5553371A (en) * 1978-10-14 1980-04-18 Canon Inc Method and apparatus for electrophotographic development
JPS60134262A (en) * 1983-12-22 1985-07-17 Canon Inc Developing method

Patent Citations (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5553371A (en) * 1978-10-14 1980-04-18 Canon Inc Method and apparatus for electrophotographic development
JPS60134262A (en) * 1983-12-22 1985-07-17 Canon Inc Developing method

Cited By (7)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006184265A (en) * 2004-12-03 2006-07-13 Adonisu Denki:Kk Oral odor measuring instrument and method, and odor measuring instrument and method
JP2009204867A (en) * 2008-02-27 2009-09-10 Sharp Corp Developing device and image forming apparatus
US7974545B2 (en) 2008-02-27 2011-07-05 Sharp Kabushiki Kaisha Developing device and image forming apparatus that utilize a variable AC bias voltage
JP2010097140A (en) * 2008-10-20 2010-04-30 Fuji Xerox Co Ltd Developing device and image forming apparatus
JP4656223B2 (en) * 2008-10-20 2011-03-23 富士ゼロックス株式会社 Developing device and image forming apparatus
US8045895B2 (en) 2008-10-20 2011-10-25 Fuji Xerox Co., Ltd. Developing device and image forming device
KR101239815B1 (en) * 2008-10-20 2013-03-06 후지제롯쿠스 가부시끼가이샤 Developing device and image forming device

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