JPH0584903B2 - - Google Patents

Info

Publication number
JPH0584903B2
JPH0584903B2 JP60217212A JP21721285A JPH0584903B2 JP H0584903 B2 JPH0584903 B2 JP H0584903B2 JP 60217212 A JP60217212 A JP 60217212A JP 21721285 A JP21721285 A JP 21721285A JP H0584903 B2 JPH0584903 B2 JP H0584903B2
Authority
JP
Japan
Prior art keywords
toner
sleeve
magnetic particles
developing
magnetic
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 - Lifetime
Application number
JP60217212A
Other languages
Japanese (ja)
Other versions
JPS6275653A (en
Inventor
Atsushi Hosoi
Hatsuo Tajima
Norihisa Hoshika
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 JP60217212A priority Critical patent/JPS6275653A/en
Publication of JPS6275653A publication Critical patent/JPS6275653A/en
Publication of JPH0584903B2 publication Critical patent/JPH0584903B2/ja
Granted legal-status Critical Current

Links

Landscapes

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

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は粉体現像剤を供給して潜像担持体を現
像する現像装置に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a developing device that supplies a powder developer to develop a latent image carrier.

本発明は、現像装置が利用される複写機、プリ
ンター、印刷機等の記録一般に適用されるもので
ある。
INDUSTRIAL APPLICATION This invention is applicable to the recording of copying machines, printers, printing machines, etc. which use a developing device in general.

(従来技術) 現像容器部と、この現像容器部に、静電潜像担
持体に対向して配置され、内部に磁石を有する回
転現像スリーブと、を備え、上記現像容器部内で
現像スリーブに沿つて磁性粒子層を形成し、現像
スリーブの回転により上記磁性粒子層の磁性粒子
を上昇移動し次いで反転して下降移動する循環運
動させ、この磁性粒子の運動により磁性粒子層の
外側のトナー層から磁性粒子層内にトナーを取り
込む現像装置に於いては、上記磁性粒子層上に多
量のトナーが存在すると、その重量により磁性粒
子の前記循環運動が不活発となつて磁性粒子層内
へのトナーの取り込みが不安定となり、また磁性
粒子層内でのトナーの摩擦帯電が不足する。この
ようなことから、現像画像の画質が劣化する。
(Prior art) A developing container section, a rotary developing sleeve disposed in the developing container section facing the electrostatic latent image carrier and having a magnet therein, and a rotating developing sleeve disposed in the developing container section facing the electrostatic latent image carrier and having a magnet therein. The rotation of the developing sleeve causes the magnetic particles in the magnetic particle layer to move upwards, then reverse and move downwards in a circular motion, and the movement of the magnetic particles causes the toner layer outside the magnetic particle layer to In a developing device that takes toner into the magnetic particle layer, if a large amount of toner exists on the magnetic particle layer, the circulation movement of the magnetic particles becomes inactive due to the weight of the toner, causing the toner to enter the magnetic particle layer. The uptake of the toner becomes unstable, and the frictional charging of the toner within the magnetic particle layer becomes insufficient. Because of this, the quality of the developed image deteriorates.

(発明の目的) 本発明の目的は、如上の現像装置に於いて、現
像スリーブの周面に沿つて形成された磁性粒子層
の磁性粒子の循環運動を阻害しないで、トナー層
からのトナーの磁性粒子層内への取り込みを安定
化させ、かつトナーの磁性粒子層内での摩擦帯電
を向上させ、そしてトナーの負荷を軽減できる現
像装置を提供することである。
(Objective of the Invention) An object of the present invention is to remove toner from the toner layer without inhibiting the circulation movement of the magnetic particles in the magnetic particle layer formed along the circumferential surface of the developing sleeve in the above-mentioned developing device. It is an object of the present invention to provide a developing device that can stabilize the uptake of toner into a magnetic particle layer, improve triboelectric charging of toner within the magnetic particle layer, and reduce the load of toner.

(目的を達する為の手段) 本発明の現像装置は、 現像容器部と、この現像容器部に、静電潜像担
持体に対向して配置され、内部に磁石を有する回
転現像スリーブと、を備え、上記現像容器部内で
現像スリーブに沿つて磁性粒子層を形成し、現像
スリーブの回転により上記磁性粒子層の磁性粒子
を上昇移動し次いで反転して下降移動する循環運
動させ、この磁性粒子の運動により磁性粒子層の
外側のトナー層から磁性粒子層内にトナーを取り
込む現像装置に於いて、上記現像容器の水平方向
側方に配置されたトナー収容容器部と、このトナ
ー収容容器部と上記現像容器部を現像スリーブ回
転中心よりも低い位置で連通するスリツト状のト
ナー通路部と、上記トナー収容容器部内で回転し
てトナー収容容器部内のトナーを上記トナー通路
部に送り込み、トナー通路部にトナーの蓄積部を
形成するトナー搬送部材と、回転軌跡の一部が上
記トナーの蓄積部内を通過するように現像容器部
内で回転し、このトナーの蓄積部から、このトナ
ーの蓄積部を消滅させない程度の少量ずつ掻き取
つて、前記磁性粒子の循環運動領域の下部部分に
送るトナー供給部材と、を備えたことを特徴とす
る現像装置である。
(Means for Achieving the Object) The developing device of the present invention includes a developing container portion, and a rotating developing sleeve disposed in the developing container portion facing the electrostatic latent image carrier and having a magnet therein. A magnetic particle layer is formed along a developing sleeve in the developing container, and by rotation of the developing sleeve, the magnetic particles in the magnetic particle layer are moved upwardly, then reversed and moved downwardly in a circular motion. In a developing device that takes toner from a toner layer outside the magnetic particle layer into the magnetic particle layer by movement, a toner storage container section disposed on the horizontal side of the developer container, this toner storage container section and the above-mentioned toner storage container section are provided. A slit-shaped toner passage section that communicates the developer container section at a position lower than the center of rotation of the development sleeve; A toner conveying member forming a toner accumulation portion rotates within the developer container portion such that a portion of its rotation locus passes through the toner accumulation portion, and does not eliminate the toner accumulation portion from the toner accumulation portion. and a toner supplying member that scrapes off the magnetic particles little by little and sends the toner to a lower part of the circulation movement area of the magnetic particles.

(実施例) 以下図面を用いて本発明の実施例を説明する。(Example) Embodiments of the present invention will be described below with reference to the drawings.

第1図現像装置は、静電潜像担持体としての不
図示のドラムの右斜め上方に位置し、現像時の状
態を表わしている。lは現像時の水平面を表わす
直線で、以下の高さ関係の基準である。
The developing device in FIG. 1 is located diagonally above and to the right of a drum (not shown) serving as an electrostatic latent image carrier, and shows the state during development. l is a straight line representing the horizontal plane during development, and is a reference for the following height relationship.

第1図例は、現像容器41内に磁性粒子と非磁
性トナーを有し、現像剤担持体としての非磁性ス
リーブの表面にトナー及び磁性粒子を付着させて
現像を行う方式(第3図で説明する)の装置を示
している。
The example in FIG. 1 is a method in which magnetic particles and non-magnetic toner are contained in the developer container 41, and development is carried out by adhering the toner and magnetic particles to the surface of a non-magnetic sleeve serving as a developer carrier (see FIG. 3). (described).

現像されるべき潜像を有する潜像担持体2とし
ては、静電記録用絶縁ドラムあるいはα−Se,
Cds,ZnO2,OPC,α−Siの様な光導電絶縁物
質層を持つ感光ドラムもしくは感光ベルトであ
る。現像スリーブ3は潜像担持体2に接触もしく
は近接されている。現像スリーブ3は例えばアル
ミニウム等の非磁性スリーブであり、現像容器4
1の左側壁の横長開口に、右略半周面を容器41
内へ突入させ、左略半周面を容器外へ露出させて
いる。現像スリーブ3は回転駆動される無端ベル
ト形態の現像剤担持体でも良い。
The latent image carrier 2 having the latent image to be developed may be an insulated drum for electrostatic recording or α-Se,
It is a photosensitive drum or photosensitive belt with a layer of photoconductive insulating material such as Cds, ZnO 2 , OPC, α-Si. The developing sleeve 3 is in contact with or close to the latent image carrier 2. The developing sleeve 3 is a non-magnetic sleeve made of aluminum, for example, and the developing container 4
Insert approximately half the right side of the container 41 into the horizontally long opening of the left side wall of 1.
The container is inserted into the container, and approximately the left half circumferential surface is exposed to the outside of the container. The developing sleeve 3 may be a developer carrier in the form of an endless belt that is rotationally driven.

36は現像スリーブ3内に挿入し、図示の位
置・姿勢に位置決め保持した固定磁界発生手段と
しての固定の永久磁石(マグネツト)であり、現
像スリーブ3が矢印方向に回転駆動されてもこの
磁石36は図示の位置・姿勢にそのまま固定保持
される。38は非磁性材からなる規制ブレード
で、スリーブ3の回転方向に関して上流側に位置
する磁石Nとの位置関係から磁性粒子7を容器4
1内に拘束する。従つて、非磁性トナーはこの拘
束下の磁性粒子の間を通過して、スリーブ3表面
上にトナー薄層として形成される。このトナー薄
層は、不図示の交番電界下で、ドラム2の表面に
対して往復運動をして静電潜像を現像する。
Reference numeral 36 denotes a fixed permanent magnet (magnet) as a fixed magnetic field generating means that is inserted into the developing sleeve 3 and held in the position and orientation shown in the figure.Even when the developing sleeve 3 is rotationally driven in the direction of the arrow, is fixedly held in the position and posture shown in the figure. Reference numeral 38 denotes a regulating blade made of a non-magnetic material, which controls the magnetic particles 7 into the container 4 due to its positional relationship with the magnet N located on the upstream side with respect to the rotational direction of the sleeve 3.
Constrain within 1. Therefore, the non-magnetic toner passes between the constrained magnetic particles and is formed as a thin toner layer on the surface of the sleeve 3. This toner thin layer reciprocates against the surface of the drum 2 under an alternating electric field (not shown) to develop the electrostatic latent image.

ここで現像例としてのトナーの供給について構
成を説明しながら説明する。
Here, toner supply as an example of development will be explained while explaining the configuration.

61は現像剤保有部としてのトナー貯蔵容器
で、全体に微粒子トナーを保有している。41は
現像剤受容部としての現像容器で、トナー貯蔵容
器61の側方に並設されている。8は時計方向に
回転して、貯蔵容器61内のトナーを搬送する搬
送部材で、その外側には布製のシート81が取付
けられている。搬送部材8は容器の長手方向にわ
たつて存在する板状で、その回転半径方向に短い
幅を有する。シート81はトナー貯蔵容器の球状
の底全体に当接しながら移動する。部材8、シー
ト81は、現像剤搬送部材として機能する。39
は、貯蔵容器61、現像容器41との間に形成さ
れ、現像剤としてのトナーが通過する開口部で、
運搬時又は装置使用開始前にはシール材(不図
示)で封鎖されている。開口部39はシール材を
除去することで開放される。30は開口部39の
上方にあつて、トナー貯蔵容器61内に設けられ
た現像剤案内部材としての分流部材で、容器61
内部から開口部39へ向かい、重力方向へ傾斜し
ている現像剤案内面301を備えている。この案
内面301は、搬送部材8と弾性シート81が搬
送してくるトナーを受けて、実質的にトナーを開
口部39側の矢印B方向と、容器61内部側の矢
印C方向とに分流せしめる。開口部39は容器内
に突出する境界部100の上面にトナー搬送方向
に関して長さLの平面部を有し、この平面部から
の高さHが開口部39の実質のトナー通過許可領
域である。この平面部はトナーの山積状蓄積部E
の低面として利用される。
Reference numeral 61 denotes a toner storage container as a developer holding section, which holds fine particle toner throughout. A developing container 41 serves as a developer receiving section, and is arranged side by side with the toner storage container 61. A conveying member 8 rotates clockwise to convey the toner in the storage container 61, and a cloth sheet 81 is attached to the outside thereof. The conveyance member 8 has a plate shape that extends in the longitudinal direction of the container, and has a short width in the rotation radius direction. The sheet 81 moves while contacting the entire spherical bottom of the toner storage container. The member 8 and the sheet 81 function as a developer conveying member. 39
is an opening formed between the storage container 61 and the developer container 41, through which toner as a developer passes;
It is sealed with a sealing material (not shown) during transportation or before the start of use of the device. The opening 39 is opened by removing the sealing material. Reference numeral 30 denotes a flow dividing member as a developer guiding member provided in the toner storage container 61 above the opening 39;
A developer guiding surface 301 is provided which extends from the inside toward the opening 39 and is inclined in the direction of gravity. The guide surface 301 receives the toner conveyed by the conveying member 8 and the elastic sheet 81 and substantially divides the toner into the direction of arrow B on the opening 39 side and the direction of arrow C on the inside of the container 61. . The opening 39 has a flat part having a length L in the toner transport direction on the upper surface of the boundary part 100 that projects into the container, and the height H from this flat part is the actual toner passage permitting area of the opening 39. . This plane part is a pile-like accumulation part E of toner.
It is used as a lower surface.

又、34は現像剤搬送部材8,81の回転中心
で、水平面からの高さは、案内面301とほぼ同
等かそれよりも低く、開口部39の位置レベルに
ある。
Reference numeral 34 denotes the center of rotation of the developer conveying members 8 and 81, and its height from the horizontal plane is approximately equal to or lower than the guide surface 301, and is at the level of the opening 39.

37は、開口部39の近傍にあつて、搬送部材
8,81から供給されたトナーをさらに現像スリ
ーブ3の矢印方向へ搬送するトナー供給部材であ
る。トナー供給部材37は、時計回転方向の回転
中心373に対して端部側に布状のトナー掻き取
り板371を有し、その回転半径による回転領域
372は図中の円内である。この回転領域372
は、前記山積状蓄積部Eと共通領域を有してお
り、トナー供給部材の回転により山積状蓄積部E
のトナーが磁性部材40側にトナーの供給を達成
せしめる。
A toner supply member 37 is located near the opening 39 and further conveys the toner supplied from the conveyance members 8 and 81 in the direction of the arrow of the developing sleeve 3. The toner supply member 37 has a cloth-like toner scraping plate 371 on the end side with respect to the rotation center 373 in the clockwise direction, and a rotation area 372 according to the rotation radius is within a circle in the figure. This rotation area 372
has a common area with the pile-shaped accumulation part E, and the pile-shaped accumulation part E is formed by rotation of the toner supply member.
toner is supplied to the magnetic member 40 side.

前記搬送部材8,81とトナー供給部材37は
その間に常に山積状の蓄積部Eを形成し続けるよ
うに、その回転が制御される。具体的には搬送部
材によつて形成された蓄積部を維持しながら、ト
ナー供給部材によつてのみその一部が磁性粒子循
環部に与えられるように、それらの回転速度を定
めれば良い。
The rotation of the conveying members 8, 81 and the toner supplying member 37 is controlled so that a heap-shaped accumulation portion E is always formed between them. Specifically, their rotational speeds may be determined so that only a portion of the toner supply member is supplied to the magnetic particle circulation unit while maintaining the storage unit formed by the conveyance member.

前記搬送部材8,81のようにトナー容器内の
搬送手段によつてのみトナー供給を行なうと過剰
な供給となるばかりでなく、トナーの融着、負荷
圧力が高まり、帯電過多の問題も発生するので好
ましくない。このような観点から、1〜5rpm程
度の低速で山積状の蓄積部Eを維持できる搬送力
であることが好ましい。
If toner is supplied only by the conveying means in the toner container, such as the conveying members 8 and 81, not only will excessive supply occur, but also problems of toner fusion, increased load pressure, and excessive charging will occur. So I don't like it. From this point of view, it is preferable that the conveyance force be such that the heaped accumulation portion E can be maintained at a low speed of about 1 to 5 rpm.

本実施例のようにトナー搬送部材の回転中心が
開口部39の上限よりも低い場合は、山積状の蓄
積部Eの高さは開口部の高さHによつて決定され
る。又、山積状の蓄積部Eの低面Lの大きさは、
トナーの流動性、安息角、トナー搬送部材の搬送
力、トナー残量によつて決定されるが、本例のよ
うに搬送部材の搬送力が小さいときはほぼトナー
の流動性、安息角によつて決定される。この場合
には、トナー供給部材の回転領域の有効供給範囲
内にトナーがなく山積状の蓄積部Eが小さく形成
されてしまう場合が見られた。このような問題を
解決する条件として前記L,HにL<2Hの関係
が見たされれば良い。これによつて、確実なトナ
ー供給量を得ることができ、少量供給を達成でき
る。従つて、後述する現像方式においては磁性粒
子層の循環が負荷を軽減した状態で安定してしか
も長期に渡つて維持できるので、形成される画像
の画質を良好ならしめる。
When the rotation center of the toner conveying member is lower than the upper limit of the opening 39 as in this embodiment, the height of the heaped accumulation portion E is determined by the height H of the opening. In addition, the size of the lower surface L of the mountain-like accumulation portion E is as follows:
It is determined by the fluidity of the toner, the angle of repose, the transporting force of the toner transporting member, and the amount of toner remaining, but when the transporting force of the transporting member is small as in this example, it is determined mostly by the fluidity of the toner and the angle of repose. will be determined. In this case, there have been cases where there is no toner within the effective supply range of the rotational region of the toner supply member, and the pile-like accumulation portion E is formed in a small size. As a condition for solving such a problem, it is sufficient if the relationship L<2H is satisfied for the above-mentioned L and H. Thereby, a reliable amount of toner supply can be obtained, and a small amount of toner supply can be achieved. Therefore, in the development method described below, the circulation of the magnetic particle layer can be stably maintained with a reduced load and can be maintained for a long period of time, thereby improving the quality of the image formed.

本実施例では、時計方向回転の回転中心373
をスリーブ中心O及び搬送部材8の回転中心34
よりも低い位置レベルにある。前述した基準平面
lからの垂直距離を、夫々中心34がl1、中心3
72がl2、スリーブ中心Oがls、ドラム中心がlD
とすると、 l2≦l1,l2<lsである。又、lDはlD<l2と設定され
ている。
In this embodiment, the rotation center 373 of clockwise rotation is
The sleeve center O and the rotation center 34 of the conveying member 8
is at a lower position level. The perpendicular distance from the reference plane l described above is determined by the center 34 being l 1 and the center 3 being l 1 , respectively.
72 is l 2 , sleeve center O is l s , drum center is l D
Then, l 2 ≦l 1 and l 2 <l s . Also, l D is set as l D < l 2 .

この中心の位置関係は、開口39を通過した現
像トナーをトナー供給部材37が現像容器内に存
在するスリーブ3の進入領域に確実に供給すると
共にトナー貯蔵容器からのトナー補給を安定化し
ているのでトナーが進入領域で不足状態になるこ
とを防止できる。そして、安定したトナー量が、
進入してきたスリーブ表面側へ搬送されると共に
スリーブ表面に予め形成されている磁性粒子層に
対して安定した接触期間を保てるのでトナーの帯
電が安定化される。そしてスリーブ表面上のトナ
ー薄層は現像行程中はもとより現像装置の使用期
間中も安定した帯電、層厚状態を維持でき現像像
の解像度を良好ならしめることができる。
This center positional relationship allows the toner supply member 37 to reliably supply the developed toner that has passed through the opening 39 to the entry area of the sleeve 3 present in the developer container, and also stabilizes the supply of toner from the toner storage container. It is possible to prevent toner from becoming insufficient in the entry area. And a stable amount of toner,
As the toner is transported to the surface of the sleeve that has entered the toner, a stable period of contact with the magnetic particle layer previously formed on the sleeve surface can be maintained, so that the toner is stably charged. The thin toner layer on the sleeve surface can maintain stable charging and layer thickness not only during the development process but also during the period of use of the developing device, and the resolution of the developed image can be improved.

尚、本例では、予め磁性粒子7が、現像スリー
ブ表面域に磁極Nにより拘束と磁性ブレード38
と磁極Nとにより容器41内への拘束と磁性粒子
7の循環を助ける粒子反転部材35とによつて、
矢印eで示す時計方向への循環を行つている。こ
の循環はスリーブ内の磁極配置、数、粒子7の流
動性、磁気特性を適宜選ぶことによつて、磁気
力、重力、摩擦力の兼ね合いで形成できる。従つ
て、本例では、磁性粒子7がスリーブ表面に対し
て循環を始める地点にトナーの取込み部を形成
し、この取込み部へトナー供給部材37が積極的
にトナーを供給するので、現像上の上述した特有
の効果がより一層確実となる。本例ではさらに、
トナー層の重さを磁性粒子層に与えることがない
ので、この循環を阻害することなく安定したトナ
ーの取り込みが可能となり、融着、凝集の問題で
使用できなかつた軽圧力定着性トナーの使用を可
能にする。
In this example, the magnetic particles 7 are previously restrained by the magnetic poles N on the surface area of the developing sleeve and the magnetic blades 38
and the magnetic pole N to restrain the magnetic particles 7 in the container 41 and the particle reversing member 35 that helps circulate the magnetic particles 7.
Circulation is performed in a clockwise direction as indicated by arrow e. This circulation can be created by appropriately selecting the arrangement and number of magnetic poles in the sleeve, the fluidity of the particles 7, and the magnetic properties to balance magnetic force, gravity, and frictional force. Therefore, in this example, a toner intake part is formed at the point where the magnetic particles 7 start circulating with respect to the sleeve surface, and the toner supply member 37 actively supplies toner to this intake part, so that there is no problem in development. The above-mentioned unique effects are further ensured. In this example, further
Since the weight of the toner layer is not applied to the magnetic particle layer, stable toner uptake is possible without interfering with this circulation, allowing the use of light-pressure fixing toner, which previously could not be used due to problems of fusion and aggregation. enable.

また、トナー取り込み口付近にトナーを送るこ
とにより、磁性粒子循環に伴つて磁性粒子層とト
ナー層間に生じる隙間を効果的につぶすことが可
能となり、磁性粒子層へのトナーの取り込みが安
定し、現像画像も均一なものとなる。
In addition, by feeding the toner near the toner intake port, it is possible to effectively close the gap that occurs between the magnetic particle layer and the toner layer as the magnetic particles circulate, and the toner intake into the magnetic particle layer is stabilized. The developed image also becomes uniform.

一般に回転型のトナー搬送部材8では第2図に
示されているように回転中心34と部材8を結ぶ
直線と回転中心34を通る鉛直線とのなす角を
θ、部材8の回転によるトナー総合搬送力をF、
水平方向の搬送力をFλ、垂直方向の搬送力をFy
とすると、このトナー搬送部材8によりトナーの
受ける力は送り部材回転円の接線方向を向いてい
るので水平方向にトナーの受ける搬送力FxはFx
=Fxcos θである。すなわちθ=0°の時トナー
の水平搬送力Fxは最大となり、θ=90°では最小
となる。
In general, in a rotary type toner conveying member 8, as shown in FIG. Conveying force is F,
The horizontal conveying force is Fλ, and the vertical conveying force is Fy.
Then, since the force exerted on the toner by this toner conveying member 8 is directed in the tangential direction of the rotating circle of the conveying member, the conveying force Fx exerted on the toner in the horizontal direction is Fx
=Fxcos θ. That is, when θ=0°, the toner horizontal conveyance force Fx is maximum, and when θ=90°, it is minimum.

従つて第1図の現像装置に戻つて現像容器11
とトナー貯蔵容器12が概略水平に設けられた場
合、トナー貯蔵容器から現像容器へのトナーの搬
送は主に前述のθで−90≦θ≦90の範囲(特に0
≦θ≦90)で行われる。
Therefore, returning to the developing device shown in FIG.
When the toner storage container 12 is installed approximately horizontally, the toner is transported from the toner storage container to the developer container mainly within the range of -90≦θ≦90 (particularly 0
≦θ≦90).

このような関係から、前述した構成の位置レベ
ルは、トナー搬送部材8,81とトナー供給部材
9とスリーブ3との供給、搬送上の関係を安定し
た供給搬送状態にならしめることができる。
Because of this relationship, the position level of the above-mentioned configuration can bring the supply and conveyance relationship between the toner conveying members 8, 81, toner supply member 9, and sleeve 3 into a stable supply and conveyance state.

本例ではさらに、案内部材30を設けることに
より、トナー貯蔵容器内のトナーを無駄なく供給
でき、狭小の開口でも上述した供給搬送状態を維
持させることができる。
In this example, by further providing the guide member 30, the toner in the toner storage container can be supplied without waste, and the above-mentioned supply and conveyance state can be maintained even with a narrow opening.

各回転の速度は画像形成上設定されるものであ
るが、現像スリーブ、ドラムを120mm/sec、トナ
ー供給部材9を13rpm、トナー搬送部材を3rpm
として通常の現像を行なつたところ、トナー供給
は安定しトナー帯電状態も安定化して優れた画像
を2000枚の耐久実験でも安定して得ることができ
た。尚、この実験では磁性粒子として平均粒径
100μmの鉄球にアクリル/フツソ系樹脂の混合物
をコーテイングしたものを用い、非磁性現像剤と
してスチレン/ブタジエン共重合体系樹脂100部
に銅フタロシアニン系顔料5部からなる平均粒系
12μmのトナー粉体にコロイダルシリカ1.0%を外
添したブルートナーを用い、N極を800Gとした。
The speed of each rotation is set for image formation, and is 120 mm/sec for the developing sleeve and drum, 13 rpm for the toner supply member 9, and 3 rpm for the toner transport member.
When normal development was carried out, the toner supply was stabilized, the toner charging state was also stabilized, and excellent images could be stably obtained even in a 2000-sheet durability test. In addition, in this experiment, the average particle size of the magnetic particles was
A 100 μm iron ball coated with a mixture of acrylic/futsuso resin is used, and an average particle system consisting of 100 parts of styrene/butadiene copolymer resin and 5 parts of copper phthalocyanine pigment is used as the non-magnetic developer.
A blue toner in which 1.0% colloidal silica was externally added to 12 μm toner powder was used, and the north pole was set to 800G.

又、実験上の現像バイアスは1.8KHz、
1.3KVppの交番電界に直流−260Vを重畳し、画
像部−680V、非画像部−220V、スリーブとドラ
ム間を400μmとした。
Also, the experimental development bias was 1.8KHz,
DC -260V was superimposed on an alternating electric field of 1.3KVpp, the image area was -680V, the non-image area -220V, and the distance between the sleeve and the drum was 400 μm.

これによつて良好なブルーの画像が得られた。 This resulted in a good blue image.

上記実施例では、現像時2成分の粒子を用いて
現像を行なうものであるが、非磁性ブレード38
の代わりに磁性ブレードを用いて現像時1成分の
現像を行なうようにしても良い。
In the above embodiment, development is performed using two-component particles during development, but the non-magnetic blade 38
Instead, a magnetic blade may be used to develop one component during development.

磁性粒子は抵抗値が107Ωcm以上、好ましくは
108Ωcm以上でフエライト等の磁性材料に樹脂コ
ーテイングしたものが用いられる。そしてこの磁
性粒子7は先ずはじめに磁性粒子収納部5より現
像容器41内に投入することにより、その磁性粒
子7が容器41内に臨んでいるスリーブ面領域
(即ち、スリーブ3を配設した現像容器41から
の磁性粒子ないしはトナー漏出を防止する部材4
0から現像剤量規制ブレード38の先端部までの
スリーブ面領域)各部にスリーブ3内の磁石36
による磁界により吸着保持される。これは磁性粒
子層として該スリーブ面領域を全体的に覆つた状
態になる。この時磁性粒子層には所定量のトナー
を含むことが好ましい。
The magnetic particles have a resistance value of 10 7 Ωcm or more, preferably
A magnetic material such as ferrite coated with resin and having a resistance of 10 8 Ωcm or more is used. The magnetic particles 7 are first introduced into the developer container 41 from the magnetic particle storage section 5, so that the magnetic particles 7 are exposed to the area of the sleeve surface facing into the container 41 (i.e., the developer container in which the sleeve 3 is disposed). Member 4 for preventing magnetic particles or toner from leaking from 41
0 to the tip of the developer amount regulating blade 38).
It is attracted and held by the magnetic field. This forms a layer of magnetic particles that completely covers the sleeve surface area. At this time, it is preferable that the magnetic particle layer contains a predetermined amount of toner.

スリーブ3を矢印b方向に回転させた時、磁極
N1,S2の配置位置と磁性粒子7の流動性及び磁
気特性を適宜選ぶことによつて磁気ブラシは磁極
N1の付近で矢印e方向に循環し、循環層を形成
する。この磁性粒子の循環により磁気ブラシ中に
周囲のトナーを取り込み、磁性粒子あるいはスリ
ーブとの摺擦によりトナーは摩擦帯電を受け、ス
リーブの回転に伴つて磁性粒子と共に現像領域へ
搬送され現像に供される。
When sleeve 3 is rotated in the direction of arrow b, the magnetic pole
By appropriately selecting the arrangement positions of N 1 and S 2 and the fluidity and magnetic properties of the magnetic particles 7, the magnetic brush can be made into a magnetic pole.
It circulates in the direction of arrow e near N1 , forming a circulation layer. Through the circulation of the magnetic particles, the surrounding toner is taken into the magnetic brush, and the toner is triboelectrically charged due to the friction between the magnetic particles and the sleeve, and as the sleeve rotates, the toner is transported to the development area together with the magnetic particles and subjected to development. Ru.

本図例において、特異点としては、トナー供給
部材37が磁性粒子収納部5よりも下方にあるた
め、磁性粒子の落下開口面積が広くとれ、磁性粒
子の投入を容易にすると共に、現像スリーブ3内
の固定磁極で拘束されず現像容器11下部面に堆
積した磁性粒子もトナー供給部材9の回転により
現像スリーブ3側へ送られて無駄な磁性粒子がな
くなり極めて効率が良い。
In this example, the peculiar point is that since the toner supply member 37 is located below the magnetic particle storage section 5, the opening area for the magnetic particles to fall is wide, making it easy to introduce the magnetic particles, and the developing sleeve 3 Magnetic particles that are not restrained by the fixed magnetic poles inside and have accumulated on the lower surface of the developer container 11 are also sent to the developer sleeve 3 side by the rotation of the toner supply member 9, eliminating unnecessary magnetic particles, resulting in extremely high efficiency.

尚、第1図で、ブレード38は本実施例では、
少なくともその先端が例えばアルミニウムなどの
非磁性材料製であり、容器部41の開口の上部近
傍でスリーブ3の長手方向に延在し、その基部は
容器部41に固定され、先端側はスリーブ3の表
面に間隙をもつて対向している。ブレード24の
先端とスリーブ3の表面との間隙は50〜500μm、
好ましくは100〜350μmであり、本実施例では
250μmである。この間隙が50μmより小さいと、
磁性粒子がこの間隙部に詰まり易く、500μmを越
えると、磁性粒子およびトナーが多量に間隙を通
過し、スリーブ3上に適当な厚さの現像剤層が形
成できない。
In addition, in FIG. 1, the blade 38 in this embodiment is
At least its tip is made of a non-magnetic material such as aluminum and extends in the longitudinal direction of the sleeve 3 near the top of the opening of the container section 41, its base is fixed to the container section 41, and its tip side is made of a non-magnetic material such as aluminum. They face each other with a gap between the surfaces. The gap between the tip of the blade 24 and the surface of the sleeve 3 is 50 to 500 μm,
Preferably it is 100 to 350 μm, and in this example
It is 250μm. If this gap is smaller than 50μm,
Magnetic particles tend to clog this gap, and if the diameter exceeds 500 μm, a large amount of magnetic particles and toner will pass through the gap, making it impossible to form a developer layer of an appropriate thickness on the sleeve 3.

以下第3図で第1図の装置の現像部での現像を
説明するが、第3図では現像スリーブを符号22
で、磁石を符号23で示した。
The development in the developing section of the apparatus shown in FIG. 1 will be explained below with reference to FIG. 3. In FIG.
The magnet is designated by the reference numeral 23.

電源34は感光ドラム1とスリーブ22との間
に電圧を印加して、それらの間の空隙に交互電界
を形成させ、スリーブ22上の現像剤からトナー
を感光ドラム1に転移させる。電源34による電
圧は正側と負側のピーク電圧が同じである対称型
交互電圧でも、このような交互電圧に直流電圧を
重畳した形の非対称交互電圧でもよい。具体的な
電圧値としては、例えば暗部電位−600V、明部
電位−200Vの静電潜像に対して、一例として、
直流電圧−300Vを重畳してピーク・ピーク電圧
を300〜2000Vpp、周波数200〜3000Hz交互電圧を
スリーブ22側に印加し、感光ドラム1を接地電
位に保持する。
The power supply 34 applies a voltage between the photosensitive drum 1 and the sleeve 22 to form an alternating electric field in the gap therebetween, thereby transferring the toner from the developer on the sleeve 22 to the photosensitive drum 1. The voltage from the power supply 34 may be a symmetrical alternating voltage in which the peak voltages on the positive side and the negative side are the same, or an asymmetrical alternating voltage in which a DC voltage is superimposed on such an alternating voltage. As a specific voltage value, for example, for an electrostatic latent image with a dark area potential of -600V and a bright area potential of -200V, for example,
A direct current voltage of -300 V is superimposed to apply a peak-to-peak voltage of 300 to 2000 Vpp and an alternating voltage of a frequency of 200 to 3000 Hz to the sleeve 22 side, and the photosensitive drum 1 is held at the ground potential.

第3図は現像部における挙動を説明するための
拡大断面図である。感光ドラム1は潜像を構成す
る電荷を担持し、本実施例においては静電潜像を
構成する電荷は負極性であり、トナーは正極性に
帯電している。また、この実施例においては感光
ドラム1とスリーブ22とは同一周方向移動とな
るように矢印のごとく回転する。これらの間の空
間には電源34によつて前述の交互電圧が印加さ
れ、交互電界が形成される。一方、感光ドラム1
とスリーブ22との最近接部に対応してスリーブ
22の内部には磁石23の磁極23bがある。
FIG. 3 is an enlarged sectional view for explaining the behavior in the developing section. The photosensitive drum 1 carries charges constituting a latent image. In this embodiment, the charges constituting the electrostatic latent image have a negative polarity, and the toner is charged to a positive polarity. Further, in this embodiment, the photosensitive drum 1 and the sleeve 22 rotate as shown by the arrows so as to move in the same circumferential direction. The above-mentioned alternating voltage is applied to the space between these by the power supply 34, and an alternating electric field is formed. On the other hand, photosensitive drum 1
There is a magnetic pole 23b of the magnet 23 inside the sleeve 22 corresponding to the closest portion between the sleeve 22 and the sleeve 22.

この空間には、前述のごとくスリーブ22の回
転によつて搬送されてきた磁性粒子27とトナー
28との混合物である現像剤がある。ここに磁性
粒子27が存在する点において前記のいわゆる一
成分非磁性現像剤薄層による現像方法の場合(特
開昭58−143360号および同59−101680号明細書)
とは本質的に異なつている。また、この部分にお
ける磁性粒子の体積比率(後述)の関係から、存
在する磁性粒子の量は通常のいわゆる磁気ブラシ
現像方法に比較して、はるかに少なく、この点に
おいて磁気ブラシ現像方法とも本質的に異なる。
この少ない磁性粒子27が磁極23aの作用で、
鎖状に連なつた穂51を粗の状態、すなわち疎ら
な状態で形成する。
In this space, there is a developer, which is a mixture of magnetic particles 27 and toner 28, which have been conveyed by the rotation of the sleeve 22 as described above. In the case of the development method using the so-called one-component non-magnetic developer thin layer, the magnetic particles 27 are present here (Japanese Patent Application Laid-open Nos. 143360/1982 and 101680/1980).
It is essentially different. Furthermore, due to the relationship of the volume ratio of magnetic particles in this area (described later), the amount of magnetic particles present is much smaller than in the usual so-called magnetic brush development method, and in this respect, it is essentially different from the magnetic brush development method. different.
This small number of magnetic particles 27 is due to the action of the magnetic pole 23a,
The ears 51 connected in a chain are formed in a coarse state, that is, in a sparse state.

現像部における磁性粒子27の挙動は自由度が
増加しているので、特殊なものとなつている。
The behavior of the magnetic particles 27 in the developing section is special because the degree of freedom is increased.

つまり、このまばらな磁性粒子の穂は均一な分
布を磁力線方向に形成すると共に、スリーブ表面
と磁性粒子表面の両方の開放することができるた
め、磁性粒子表面の付着トナーを穂に阻害される
ことなく感光ドラムへ供給でき、スリーブ表面の
均一な開放表面の形成によつて、スリーブ表面に
付着したトナーが交番電界でスリーブ表面から感
光ドラム表面へ飛翔できる。
In other words, these sparse spikes of magnetic particles form a uniform distribution in the direction of the magnetic field lines and can open both the sleeve surface and the magnetic particle surface, so that the toner adhering to the surface of the magnetic particles is not blocked by the spikes. By forming a uniform open surface on the sleeve surface, toner adhering to the sleeve surface can fly from the sleeve surface to the photosensitive drum surface by an alternating electric field.

ここで磁性粒子の挙動及びトナー粒子の飛翔に
ついて説明する。
Here, the behavior of magnetic particles and the flight of toner particles will be explained.

第1図に示されるように、本実施例においては
静電潜像は負電荷(画像暗部)によつて構成され
ているので、静電潜像による電界は矢印aで示す
方向である。交互電界による電界の方向は交互に
変化するが、スリーブ22側に正成分が印加され
ている位相では、これによる電界の方向は潜像に
よる電界の方向と一致している。この時に電界に
よつて穂51に注入される電荷の量は最大とな
り、したがつて、穂51は図示のごとく最大起立
状態となつて、長い穂は感光ドラム1表面に伸び
る。
As shown in FIG. 1, in this embodiment, the electrostatic latent image is composed of negative charges (image dark areas), so the electric field due to the electrostatic latent image is in the direction indicated by arrow a. The direction of the electric field due to the alternating electric field changes alternately, but in the phase where the positive component is applied to the sleeve 22 side, the direction of the electric field due to this matches the direction of the electric field due to the latent image. At this time, the amount of charge injected into the ears 51 by the electric field becomes maximum, so the ears 51 are in the maximum standing state as shown in the figure, and the long ears extend over the surface of the photosensitive drum 1.

一方、スリーブ22および磁性粒子27の表面
上のトナー28は前述のごとく正極性に帯電して
いるので、この空間に形成されている電界によつ
て感光ドラム1に転移する。このときに穂51は
粗の状態で起立しているので、スリーブ22表面
は露出しており、トナー28はスリーブ22表面
および穂51の表面の両方から離脱する。加え
て、穂51にはトナー28と同極性の電荷が存在
するため、穂51表面上のトナー28は電気的反
発力によつてさらに移動し易い。
On the other hand, since the toner 28 on the surfaces of the sleeve 22 and the magnetic particles 27 is positively charged as described above, it is transferred to the photosensitive drum 1 by the electric field formed in this space. At this time, since the ears 51 stand up in a rough state, the surface of the sleeve 22 is exposed, and the toner 28 separates from both the sleeve 22 surface and the surface of the ears 51. In addition, since the spikes 51 are charged with the same polarity as the toner 28, the toner 28 on the surface of the spikes 51 is more likely to move due to electrical repulsion.

交互電圧成分の負の成分がスリーブ22に印加
される位相では、交互電圧による電界(矢印b)
は静電潜像による電界(矢印a)と逆方向であ
る。したがつてこの空間部での電界は逆方向に強
くなり、電荷の注入量は相対的に少なくなり、穂
51は電荷注入量に応じて縮んだ接触状態とな
る。
In the phase in which the negative component of the alternating voltage component is applied to the sleeve 22, the electric field due to the alternating voltage (arrow b)
is in the opposite direction to the electric field (arrow a) due to the electrostatic latent image. Therefore, the electric field in this space becomes strong in the opposite direction, the amount of charge injection becomes relatively small, and the ears 51 are brought into a contracted contact state in accordance with the amount of charge injection.

一方、感光ドラム1上のトナー28は前述のご
とく正極性に帯電しているので、この空間に形成
されている電界によつてスリーブ22あるいは磁
性粒子27に逆転移する。このようにしてトナー
28は感光ドラム1とスリーブ22表面あるいは
トナー28表面との間を往復運動し、感光ドラム
1およびスリーブ22の回転によつて、これらの
間の空間が広がるにつれて、電界が弱くなるとと
もに現像作用が完了する。
On the other hand, since the toner 28 on the photosensitive drum 1 is positively charged as described above, it is reversely transferred to the sleeve 22 or the magnetic particles 27 by the electric field formed in this space. In this way, the toner 28 moves back and forth between the photosensitive drum 1 and the surface of the sleeve 22 or the surface of the toner 28, and as the space between them expands due to the rotation of the photosensitive drum 1 and sleeve 22, the electric field becomes weaker. The developing action is completed at the same time.

穂51にはトナー28との摩擦帯電電荷もしく
は鏡映電荷、感光ドラム1上の静電潜像電荷およ
び感光ドラム1とスリーブ22との間の交互電界
によつて注入される電荷が存在するが、その状態
は磁性粒子27の材質その他によつて決定される
電荷の充放電時定数によつて変化する。
There are charges injected into the spikes 51 by frictional charges or mirror charges with the toner 28, electrostatic latent image charges on the photosensitive drum 1, and alternating electric fields between the photosensitive drum 1 and the sleeve 22. , the state changes depending on the charging/discharging time constant of the charge determined by the material of the magnetic particles 27 and other factors.

以上のごとく、磁性粒子27の穂51は上述の
交互電界によつて微小なしかし激しい振動状態と
なる。
As described above, the ears 51 of the magnetic particles 27 are brought into a state of slight but intense vibration due to the above-mentioned alternating electric field.

ここで、現像部における磁性粒子の体積比率に
ついて説明する。「現像部」とはスリーブ22か
ら感光ドラム1へトナーが転移あるいは供給され
る部分である。「体積比率」とはこの現像部の容
積に対するその中に存在する磁性粒子の占める体
積の百分率である。本件発明者は種々の実験およ
び考察の結果、上記現像装置においてはこの体積
比率が重要な影響を有すること、およびこれを
1.5〜30%特に2.6〜26%とすることが極めて好ま
しいことを見出した。
Here, the volume ratio of magnetic particles in the developing section will be explained. The "developing section" is a section where toner is transferred or supplied from the sleeve 22 to the photosensitive drum 1. The "volume ratio" is the percentage of the volume occupied by the magnetic particles present in the developing area relative to the volume of the developing area. As a result of various experiments and considerations, the inventor of the present invention has found that this volume ratio has an important influence on the above-mentioned developing device, and that this
It has been found that a content of 1.5 to 30%, particularly 2.6 to 26%, is extremely preferable.

1.5%未満では、現像像濃度の低下が認められ
ること、スリーブゴーストが発生すること、穂5
1が存在する部分としない部分との間で顕著な濃
度差が発生すること、スリーブ22表面上に形成
される現像剤層の厚さが全体的に不均一となるこ
と、などの点で好ましくない。
If it is less than 1.5%, a decrease in the density of the developed image will be observed, sleeve ghost will occur, and panicle 5
This is preferable in that a noticeable difference in density occurs between the part where 1 is present and the part where it is not, and the thickness of the developer layer formed on the surface of the sleeve 22 becomes non-uniform as a whole. do not have.

30%を越えると、スリーブ面を閉鎖する度合が
増大し、かぶりが発生すること、などの点で好ま
しくない。
If it exceeds 30%, the degree of closure of the sleeve surface increases, which is undesirable because fogging may occur.

特に、本発明は体積比率の増加あるいは減少に
したがつて画質が単調に劣化または増加するので
はなく、1.5〜30%の範囲で十分な画像濃度が得
られ、1.5%未満でも30%を越えても、画質低下
が発生し、しかもこの画質が十分な上記数値の範
囲ではスリーブゴーストもかぶりも発生しないと
いう発明者が見出した事実に基づくものである。
前者の画質低下は負性特性によるものと思われ、
後者は磁性粒子の存在量が大きくなつてスリーブ
22表面を開放できなくなりスリーブ22表面か
らのトナー供給量が大幅に減少することから生ず
ると考えられる。
In particular, in the present invention, the image quality does not monotonically deteriorate or increase as the volume ratio increases or decreases, but sufficient image density can be obtained in the range of 1.5 to 30%, and even if it is less than 1.5%, it can exceed 30%. This is based on the fact that the inventor has discovered that in the range of the above numerical values where the image quality is sufficient, neither sleeve ghost nor fogging occurs.
The deterioration in image quality in the former is thought to be due to the negative characteristic;
The latter is thought to occur because the amount of magnetic particles present becomes large and the surface of the sleeve 22 cannot be opened, resulting in a significant decrease in the amount of toner supplied from the surface of the sleeve 22.

又、1.5%未満では、線画像の再現性に劣り、
画質濃度の低下が顕著である。逆に30%を越えた
場合は磁性粒子が感光ドラム面を傷つける問題、
画像の一部として付着して行くために生じる転
写、定着の問題がある。
Also, if it is less than 1.5%, the reproducibility of line images will be poor,
There is a noticeable decrease in image quality and density. On the other hand, if it exceeds 30%, the magnetic particles may damage the photosensitive drum surface.
There are transfer and fixing problems that occur because the image is attached as part of the image.

そして、磁性粒子の存在が1.5%に近い場合は、
大面積の一様高濃度画像(ベタ黒)の再現時に、
「あらび」と称せられる部分的現像ムラが発生す
る場合(特別環境下等)があるので、これらが発
生しにくい体積比率とすることが好ましい。この
数値は現像部に対して磁性粒子の体積比率が2.6
%以上であることで、この範囲はより好ましい範
囲となる。又、磁性粒子の存在が30%に近い場合
は、磁性粒子の穂が接する部分の周辺にスリーブ
面からのトナー補給が遅れる場合(現像速度大の
時等)があり、ベタ黒再現時にうろこ状の濃度ム
ラを生じる可能性がある。これを防止する確実な
範囲としては、磁性粒子の上記体積比率が26%以
下がより好ましいものとなる。
And if the presence of magnetic particles is close to 1.5%,
When reproducing large area uniform high density images (solid black),
Since partial development unevenness called "roughness" may occur (under special circumstances, etc.), it is preferable to set a volume ratio that makes it difficult for this to occur. This value indicates that the volume ratio of magnetic particles to the developing area is 2.6.
% or more, this range becomes a more preferable range. Also, if the presence of magnetic particles is close to 30%, there may be a delay in toner replenishment from the sleeve surface around the area where the ears of magnetic particles come into contact (such as when the development speed is high), and scales may appear when solid black is reproduced. This may result in uneven density. As a reliable range for preventing this, it is more preferable that the volume ratio of the magnetic particles is 26% or less.

体積比率が1.5〜30%の範囲であれば、スリー
ブ22表面上に穂51が好ましい程度に疎らな状
態で形成され、スリーブ22および穂51上の両
方のトナーが感光ドラム1に対して十分に開放さ
れ、スリーブ上のトナーも交互電界で飛翔転移す
るので、ほとんどすべてのトナーが現像に消費可
能な状態となることから高い現像効率(現像部に
存在するトナーのうち現像に消費され得るトナー
の割合)および高画像濃度が得られる。好ましく
は、微小なしかし激しい穂の振動を生じさせ、こ
れによつて磁性粒子およびスリーブ22に付着し
ているトナーがほぐされる。いずれにせよ磁気ブ
ラシの場合などのような掃目むらやゴースト像の
発生を防止できる。さらに、穂の振動によつて、
磁性粒子27とトナー28との摩擦接触が活発に
なるのでトナー28への摩擦帯電を向上させ、か
ぶり発生を防止できる。なお、現像効率が高いこ
とは現像装置の小型化に適する。
If the volume ratio is in the range of 1.5 to 30%, the spikes 51 are formed on the surface of the sleeve 22 in a preferable sparse state, and the toner on both the sleeve 22 and the spikes 51 is sufficiently applied to the photosensitive drum 1. Since the toner on the sleeve is released and the toner on the sleeve is also transferred by flight due to the alternating electric field, almost all of the toner is in a state that can be consumed for development. ratio) and high image density. Preferably, slight but strong vibrations of the ears are generated, thereby loosening the magnetic particles and the toner adhering to the sleeve 22. In any case, it is possible to prevent uneven sweeping and ghost images that occur in the case of magnetic brushes. Furthermore, due to the vibration of the ears,
Since the frictional contact between the magnetic particles 27 and the toner 28 becomes active, the frictional electrification of the toner 28 can be improved and fogging can be prevented. Note that high developing efficiency is suitable for downsizing of the developing device.

上記現像部に存在する磁性粒子27の体積比率
は (M/h)×(1/ρ)×[(C/(T+C)] で求めることができる。ここで、Mはスリーブの
単位面積当りの現像像(混合物……非穂立時)の
塗布量(g/cm2)、hは現像部空間の高さ(cm)、
ρは磁性粒子の真密度g/cm3、C/(T+C)は
スリーブ上の現像剤中の磁性粒子の重量割合であ
る。
The volume ratio of the magnetic particles 27 existing in the developing area can be determined as (M/h) x (1/ρ) x [(C/(T+C)]. Here, M is the volume ratio per unit area of the sleeve. Coating amount (g/cm 2 ) of the developed image (mixture...when not standing), h is the height of the developing area space (cm),
ρ is the true density of the magnetic particles in g/cm 3 , and C/(T+C) is the weight ratio of the magnetic particles in the developer on the sleeve.

なお、上記定義の現像部において磁性粒子に対
するトナーの割合は4〜40重量%が好ましい。
In addition, in the developing section defined above, the ratio of toner to magnetic particles is preferably 4 to 40% by weight.

上記実施例のように交番電界が強い(変化率が
大きいまたはVppが大きい)場合、穂51がスリ
ーブ22からあるいはその基部から離脱し、離脱
した磁性粒子27はスリーブ22と感光ドラム1
との間の空間で往復運動する。この往復運動のエ
ネルギーは大きいので、上述の振動による効果が
さらに促進される。
When the alternating electric field is strong (the rate of change is large or Vpp is large) as in the above embodiment, the spikes 51 separate from the sleeve 22 or from its base, and the separated magnetic particles 27 are attached to the sleeve 22 and the photosensitive drum 1.
It moves back and forth in the space between. Since the energy of this reciprocating motion is large, the effect of the vibration described above is further promoted.

以上の挙動は高速度カメラ(日立製作所製)で
8000コマ/秒の撮影を行なつて確認された。
The above behavior was observed using a high-speed camera (manufactured by Hitachi).
This was confirmed by shooting at 8000 frames per second.

感光ドラム1表面とスリーブ22表面との間隙
を小さくして、感光ドラム1と穂51との接触圧
力を高め、振動を小さくした場合でも、現像部の
入口側および出口側では空隙は大きいので、十分
な振動が起り、上述の効果が奏される。
Even if the gap between the surface of the photosensitive drum 1 and the surface of the sleeve 22 is reduced to increase the contact pressure between the photosensitive drum 1 and the brush 51 and to reduce vibration, the gap is large at the entrance and exit sides of the developing section. Sufficient vibration occurs to produce the above-mentioned effects.

逆に、感光ドラム1とスリーブ22との間隙を
大きくして、磁界を印加しない状態で穂51は感
光ドラム1に接触しないが、印加した場合は接触
するような距離とすることが好ましい。
Conversely, it is preferable to increase the gap between the photosensitive drum 1 and the sleeve 22 so that the ears 51 do not contact the photosensitive drum 1 when no magnetic field is applied, but do come into contact when a magnetic field is applied.

なお、前記の比較的低い抵抗値の磁性粒子27
を使用する場合、感光ドラム1とスリーブ22と
の間に印加する交互電圧は、そのピーク値の際に
潜像の暗部、明部のいずれにおいても間隙放電が
発生しないように設定する必要がある。一方、比
較的高い抵抗値の穂51を使用する場合は、交互
電圧の周波数と穂51の充放電時定数を適切に選
択することによつて、間隙電圧が放電開始電圧に
到達しないようにすることが好ましい。
Note that the magnetic particles 27 having a relatively low resistance value
When using an alternating voltage applied between the photosensitive drum 1 and the sleeve 22, it is necessary to set the alternating voltage applied between the photosensitive drum 1 and the sleeve 22 so that no gap discharge occurs in either the dark or bright areas of the latent image when the voltage reaches its peak value. . On the other hand, when using ears 51 with a relatively high resistance value, the gap voltage does not reach the discharge starting voltage by appropriately selecting the frequency of the alternating voltage and the charging/discharging time constant of the ears 51. It is preferable.

これらを考慮した場合、穂51全体の抵抗とし
ては、感光ドラム1に現像ブラシが接触した状態
で穂51の高さ方向の抵抗が1015〜106Ωcmの程
度が好ましく、現像電極効果を期待する場合は
1010〜106Ωcm程度が好ましい。
Taking these into consideration, the resistance of the entire spike 51 in the height direction of the spike 51 with the developing brush in contact with the photosensitive drum 1 is preferably in the range of 10 15 to 10 6 Ωcm, and a developing electrode effect is expected. If you do
Approximately 10 10 to 10 6 Ωcm is preferable.

磁性粒子27は平均粒径が30〜100μ、好まし
くは40〜80μである。一般的に平均粒径の小さい
もの程、スリーブ22上でのトナーの摩擦帯電特
性が優れ、スリーブゴースト(ベタ黒原稿を現像
した直後のスリーブ回転による現像で濃度が低く
なる現象あるいはスリーブの回転ごとに現像濃度
が低下する現象として現れる)が発生しなくな
る。しかし粒径が小さい場合は、静電保持体への
磁性粒子の付着を発生する傾向がある。この付着
位置は磁性粒子の抵抗値によつて異なり、例えば
比較的低抵抗なものでは画像部に付着し、高抵抗
なものでは非画像部に付着する。これは一般的傾
向で、実際には磁性粒子の磁気的特性、表面形
状、表面処理材(樹脂コートを含む)も多少影響
する。
The magnetic particles 27 have an average particle size of 30 to 100 microns, preferably 40 to 80 microns. In general, the smaller the average particle size, the better the triboelectric charging characteristics of the toner on the sleeve 22, and the sleeve ghost (a phenomenon in which the density decreases due to the rotation of the sleeve immediately after developing a solid black original, or every rotation of the sleeve). (which appears as a phenomenon in which the developing density decreases) will no longer occur. However, if the particle size is small, there is a tendency for the magnetic particles to adhere to the electrostatic holder. The position of this adhesion differs depending on the resistance value of the magnetic particles; for example, those with relatively low resistance will adhere to the image area, and those with high resistance will adhere to the non-image area. This is a general tendency, and in reality, the magnetic properties of the magnetic particles, the surface shape, and the surface treatment material (including resin coating) also have some influence.

現像部のスリーブ上の磁界が600〜900Gの商業
的電子写真現像装置においては、粒径が30μ以下
では磁性粒子の付着が増大する。又100μ以上で
はスリーブゴーストが目立つ。したがつて上記範
囲が好ましい。
In commercial electrophotographic development equipment where the magnetic field on the sleeve of the developer section is 600 to 900 G, adhesion of magnetic particles increases when the particle size is less than 30 microns. Also, sleeve ghosts are noticeable at 100μ or more. Therefore, the above range is preferable.

本現像装置においては従来用いられていた2成
分系の50〜100μ程度の比較的高抵抗のキヤリア
を用いることができる。
In this developing device, a conventional two-component carrier having a relatively high resistance of about 50 to 100 μm can be used.

各磁性粒子は磁性材料のみから成るものでも、
磁性材料と非磁性材料との結合体でも良いし、磁
性粒子全体としては二種類以上の磁性粒子の混合
物でも良い。
Each magnetic particle may consist only of magnetic material,
The magnetic particles may be a combination of a magnetic material and a non-magnetic material, or the magnetic particles as a whole may be a mixture of two or more types of magnetic particles.

つぎに、前記角度θについてはθ<2°の範囲で
は磁性粒子27の塊が発生、あるいはスリーブ上
に現像剤が均一な層として形成されない。これは
ブレード24の近傍で磁力線に沿つて磁性粒子が
粗の状態で並ぶことになり、一定以上の磁性粒子
がここに貯つたのちに初めて出ていくことによる
と考えられる。一方θ>40°では磁性粒子27の
量の規制効果が著しく劣る。したがつて2°≦θ≦
40°が好ましく、5°≦θ≦20°が特に好ましいこと
が見出された。
Next, when the angle θ is in a range of θ<2°, agglomerates of the magnetic particles 27 occur or the developer is not formed as a uniform layer on the sleeve. This is thought to be due to the fact that the magnetic particles are arranged in a coarse manner along the lines of magnetic force in the vicinity of the blade 24, and only after a certain number of magnetic particles have accumulated here do they leave. On the other hand, when θ>40°, the effect of regulating the amount of magnetic particles 27 is significantly inferior. Therefore, 2°≦θ≦
It has been found that 40° is preferred and 5°≦θ≦20° is particularly preferred.

なお角度θと現像剤通過量との関係は、θを小
さくすると通過量は減少し、したがつて現像部に
おける体積比率は減少し、θを大きくすると逆の
傾向となる。スリーブ22表面上に塗布されるト
ナーの量はθに影響されずほぼ一定である。
Regarding the relationship between the angle θ and the amount of developer passing through, as θ is decreased, the amount of developer passing through decreases, and therefore the volume ratio in the developing section decreases, and as θ is increased, the opposite tendency occurs. The amount of toner applied onto the surface of the sleeve 22 is not affected by θ and remains approximately constant.

つぎに、第1図の現像装置を用いた具体例につ
いて述べる。第1図において、スリーブ22とし
て直径20mmのアルミスリーブの表面を、アランダ
ム砥粒により不定型サンドブラスト処理したもの
を用い、磁石23として4極着磁でN極、S極が
交互に第1図で示されるようなものを用いた。磁
石23による表面磁束密度の最大値は約900ガウ
スであつた。
Next, a specific example using the developing device shown in FIG. 1 will be described. In Fig. 1, the sleeve 22 is an aluminum sleeve with a diameter of 20 mm, the surface of which has been subjected to irregular sandblasting with Alundum abrasive grains, and the magnet 23 is 4-pole magnetized with N and S poles alternately shown in Fig. 1. I used something like the one shown in . The maximum value of the surface magnetic flux density due to the magnet 23 was about 900 Gauss.

ブレード24としては1.2mm厚の非磁性ステン
レスを用い、上記角度θは15°とした。
The blade 24 was made of nonmagnetic stainless steel with a thickness of 1.2 mm, and the angle θ was 15°.

磁性粒子としては、表面にシリコン樹脂コート
した粒径70〜50μ(250/300メツシユ)のフエラ
イト(最大磁化60emu/g)を用いた。
As the magnetic particles, ferrite (maximum magnetization 60 emu/g) with a particle size of 70 to 50 μm (250/300 mesh) whose surface was coated with silicone resin was used.

非磁性トナーとしては、スチレン/ブタジエン
共重合体系樹脂100部に銅フタロシアニン系顔料
5部から成る平均粒径10μのトナー粉体にコロイ
ダルシリカ0.6%を外添したブルートナーを用い
たところ、スリーブ22表面上にコーテイング厚
約20〜30μmのトナー塗布層を得、さらにその上
層として100〜200μの磁性粒子層を得た。各磁性
粒子の表面上には上記トナーが付着している。
As a non-magnetic toner, blue toner was used, which was made by externally adding 0.6% of colloidal silica to toner powder with an average particle size of 10μ, which was made of 100 parts of styrene/butadiene copolymer resin and 5 parts of copper phthalocyanine pigment. A toner coating layer with a coating thickness of about 20 to 30 μm was obtained on the surface, and a magnetic particle layer with a thickness of 100 to 200 μm was obtained as an upper layer. The toner is attached to the surface of each magnetic particle.

このときのスリーブ22上の磁性粒子と全トナ
ーとの合計重量は約2.43×10-2g/cm2であつた。
At this time, the total weight of the magnetic particles and all the toner on the sleeve 22 was approximately 2.43×10 −2 g/cm 2 .

磁性粒子は現像部およびその近傍でスリーブ2
2内の磁極23bにより磁界によつて穂立ちし
て、最大長約0.9mm程の穂立ちブラシを形成して
いた。
The magnetic particles are placed in the sleeve 2 in the developing area and its vicinity.
The brushes were raised by the magnetic field generated by the magnetic pole 23b in the brush 2, forming a raised brush with a maximum length of about 0.9 mm.

帯電量をブローオフ法で測定したところスリー
ブ上及び磁性粒子上のトナーのトリボ電荷量が+
10μC/gであつた。
When the amount of charge was measured using the blow-off method, the amount of triboelectric charge of the toner on the sleeve and on the magnetic particles was +
It was 10μC/g.

この現像装置をキヤノン(株)製PC−10型複写機
に組み込み、感光ドラム3(有機感光材料製)と
スリーブ22の表面との間隙を350μmとした。こ
の条件で体積比率を求めると、約10%であつた
(h=350μm、M=2.43×10-2g/cm2、ρ=5.5
g/cm3、T/(T+C)=20.4%)。バイアス電源
34として周波数1600Hz、ピーク対ピーク値
1300Vの交流電圧に−300Vの直流電圧を重畳さ
せたものを用いて現像を行なつたところ、良好な
ブルー色の画像を得た。
This developing device was installed in a PC-10 type copying machine manufactured by Canon Inc., and the gap between the photosensitive drum 3 (made of an organic photosensitive material) and the surface of the sleeve 22 was set to 350 μm. When the volume ratio was calculated under these conditions, it was approximately 10% (h = 350 μm, M = 2.43 × 10 -2 g/cm 2 , ρ = 5.5
g/cm 3 , T/(T+C)=20.4%). Frequency 1600Hz as bias power supply 34, peak-to-peak value
When development was carried out using an AC voltage of 1300V superimposed with a DC voltage of -300V, a good blue image was obtained.

また、ベタ黒画像について現像し、現像後のス
リーブ面を観察したところ、磁性粒子に付着した
トナー及びスリーブ上のトナーはほとんど消費さ
れ100%近い現像効率で現像が行なわれていた。
Further, when a solid black image was developed and the sleeve surface after development was observed, it was found that most of the toner attached to the magnetic particles and the toner on the sleeve were consumed, and development was performed with nearly 100% development efficiency.

(効果) 本発明は、現像剤収容部から現像剤受容部へそ
して現像剤担持体上への現像剤供給の安定化を達
成し、現像剤の安定した帯電状態を形成できるの
で再現された画質を良好ならしめる。又、現像条
件の設定や使用材料の選定範囲を広げる効果もあ
る。
(Effects) The present invention achieves stabilization of developer supply from the developer accommodating section to the developer receiving section and onto the developer carrier, and forms a stable charging state of the developer, thereby improving reproduced image quality. make it good. It also has the effect of widening the range of development conditions and selection of materials used.

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

第1図は本発明実施例の要部説明図、第2図は
第1図中のトナー搬送部材の移動説明図、第3図
は本発明を適用した現像装置の概要説明図であ
る。 8は搬送部材、30は案内部材、41は現像容
器、39は開口部、61は貯蔵容器、81はシー
ト、l1,l2,ls,lD,L1,L2,Ls,LDは距離。
FIG. 1 is an explanatory diagram of essential parts of an embodiment of the present invention, FIG. 2 is an explanatory diagram of movement of the toner conveying member in FIG. 1, and FIG. 3 is a schematic explanatory diagram of a developing device to which the present invention is applied. 8 is a conveyance member, 30 is a guide member, 41 is a developer container, 39 is an opening, 61 is a storage container, 81 is a sheet, l 1 , l 2 , l s , l D , L 1 , L 2 , L s , L D is distance.

Claims (1)

【特許請求の範囲】[Claims] 1 現像容器部と、この現像容器部に、静電潜像
担持体に対向して配置され、内部に磁石を有する
回転現像スリーブと、を備え、上記現像容器部内
で現像スリーブに沿つて磁性粒子層を形成し、現
像スリーブの回転により上記磁性粒子層の磁性粒
子を上昇移動し次いで反転して下降移動する循環
運動させ、この磁性粒子の運動により磁性粒子層
の外側のトナー層から磁性粒子層内にトナーを取
り込む現像装置に於いて、上記現像容器の水平方
向側方に配置されたトナー収容容器部と、このト
ナー収容容器部と上記現像容器部を現像スリーブ
回転中心よりも低い位置で連通するスリツト状の
トナー通路部と、上記トナー収容容器部内で回転
してトナー収容容器部内のトナーを上記トナー通
路部に送り込み、トナー通路部にトナーの蓄積部
を形成するトナー搬送部材と、回転軌跡の一部が
上記トナーの蓄積部内を通過するように現像容器
部内で回転し、このトナーの蓄積部から、このト
ナーの蓄積部を消滅させない程度の少量ずつ掻き
取つて、前記磁性粒子の循環運動領域の下部部分
に送るトナー供給部材と、を備えたことを特徴と
する現像装置。
1. A developing container section, and a rotating developing sleeve disposed in the developing container section facing the electrostatic latent image carrier and having a magnet therein, and magnetic particles are distributed along the developing sleeve within the developing container section. The rotation of the developing sleeve causes the magnetic particles in the magnetic particle layer to move upwards, then reverse and move downwards in a circular motion, and the movement of the magnetic particles causes the magnetic particles to move from the toner layer outside the magnetic particle layer to the magnetic particle layer. In a developing device that takes toner into the developing device, a toner storage container portion disposed on the horizontal side of the developer container, and the toner storage container portion and the developer container portion communicate with each other at a position lower than the center of rotation of the developer sleeve. a slit-shaped toner passage section; a toner conveying member that rotates within the toner storage container section to feed the toner in the toner storage container section to the toner passage section to form a toner accumulation section in the toner passage section; and a rotation locus. The magnetic particles rotate in the developing container so that a part of the toner particles pass through the toner accumulation area, and are scraped off from the toner accumulation area little by little to the extent that the toner accumulation area does not disappear. A developing device comprising: a toner supply member that supplies toner to a lower portion of the area.
JP60217212A 1985-09-30 1985-09-30 Method and device for supplying developer in developing device Granted JPS6275653A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP60217212A JPS6275653A (en) 1985-09-30 1985-09-30 Method and device for supplying developer in developing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP60217212A JPS6275653A (en) 1985-09-30 1985-09-30 Method and device for supplying developer in developing device

Publications (2)

Publication Number Publication Date
JPS6275653A JPS6275653A (en) 1987-04-07
JPH0584903B2 true JPH0584903B2 (en) 1993-12-03

Family

ID=16700618

Family Applications (1)

Application Number Title Priority Date Filing Date
JP60217212A Granted JPS6275653A (en) 1985-09-30 1985-09-30 Method and device for supplying developer in developing device

Country Status (1)

Country Link
JP (1) JPS6275653A (en)

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2006267933A (en) * 2005-03-25 2006-10-05 Fuji Xerox Co Ltd Developing device, and process cartridge and image forming apparatus using the same
EP2071849A4 (en) 2006-11-07 2010-08-04 Sony Corp Receiver, delayed information transmitting method for receivers, audio output device, and delay control method for audio output devices

Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5723548B2 (en) * 1975-10-09 1982-05-19
JPS5848901A (en) * 1981-09-18 1983-03-23 日本特殊陶業株式会社 High temperature thermistor
JPS6134567A (en) * 1984-07-26 1986-02-18 Ricoh Co Ltd Container of developing agent
JPS61129668A (en) * 1984-11-28 1986-06-17 Toshiba Corp Developing device

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS55121252U (en) * 1979-02-19 1980-08-28
JPS5723548U (en) * 1980-07-10 1982-02-06

Patent Citations (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5723548B2 (en) * 1975-10-09 1982-05-19
JPS5848901A (en) * 1981-09-18 1983-03-23 日本特殊陶業株式会社 High temperature thermistor
JPS6134567A (en) * 1984-07-26 1986-02-18 Ricoh Co Ltd Container of developing agent
JPS61129668A (en) * 1984-11-28 1986-06-17 Toshiba Corp Developing device

Also Published As

Publication number Publication date
JPS6275653A (en) 1987-04-07

Similar Documents

Publication Publication Date Title
JP2554249B2 (en) Development device
JP2668781B2 (en) Development method
JP2517579B2 (en) Development device
JPH0584903B2 (en)
JP2505800B2 (en) Development device
JPS62192757A (en) Developing method
JP2644489B2 (en) Developing device
JP2505814B2 (en) Development device
JPS6275687A (en) Developing device
JPS63225269A (en) Developing device
JPS634281A (en) Developing device
JPH0279863A (en) Developing method
JPS63225261A (en) Developing device
JPH0664396B2 (en) Development device
JPS6361272A (en) Developing device
JPS63225274A (en) Developing device
JPH0279878A (en) Developing device
JPS63225262A (en) Developing method
JPH03138674A (en) Developing device
JPS63225268A (en) Developing device
JPS63225272A (en) Developing device
JPH0575113B2 (en)
JPS6361271A (en) Developing device
JPS63225263A (en) Developing device
JPS6275685A (en) Developing device

Legal Events

Date Code Title Description
EXPY Cancellation because of completion of term