JPH0284679A - Developing device - Google Patents
Developing deviceInfo
- Publication number
- JPH0284679A JPH0284679A JP9501789A JP9501789A JPH0284679A JP H0284679 A JPH0284679 A JP H0284679A JP 9501789 A JP9501789 A JP 9501789A JP 9501789 A JP9501789 A JP 9501789A JP H0284679 A JPH0284679 A JP H0284679A
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- JP
- Japan
- Prior art keywords
- developer
- developing
- area
- magnetic field
- 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.)
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- Magnetic Brush Developing In Electrophotography (AREA)
Abstract
Description
【発明の詳細な説明】
[産業上の利用分野]
本発明は静電潜像を現像する装置、特に現像領域に於い
て現像剤層の厚みが像担持体と現像剤支持体との間隙よ
りも薄い現像剤層を像担持体に対向させて〈替像を現像
する現像装置に関する。Detailed Description of the Invention [Industrial Application Field] The present invention relates to an apparatus for developing an electrostatic latent image, particularly in a developing area where the thickness of the developer layer is greater than the gap between the image carrier and the developer support. The present invention also relates to a developing device that develops a replacement image by placing a thin developer layer facing an image carrier.
[従来技術と問題点]
従来、この種の現像装置は像担持体に外周面を対向して
配置され、その外周面に磁性を有する現像剤を支持する
非磁性の回転体を有している。そして像担持体と回転体
の最近接部を含む現像域に於いて、回転体から像担持体
に現像剤が飛翔転移し、これによって静電潜像が現像さ
れる。[Prior Art and Problems] Conventionally, this type of developing device has a non-magnetic rotating body that is disposed with its outer circumferential surface facing an image carrier and supports a magnetic developer on its outer circumferential surface. . In a developing area including the closest portion between the image carrier and the rotating body, the developer is transferred by flying from the rotating body to the image carrier, thereby developing the electrostatic latent image.
この場合、上記回転体の表面に現像剤を磁気的に吸引す
る手段として、回転体の内部に磁極を複数有する磁石が
固定設置されている。そして、この複数の磁極のうち一
磁極は、現像領域の範囲内にあって像担持体と回転体と
の近接部に対応する位置の近傍に配設され、現像領域の
略中央部で法線方向磁界成分(上記回転体の表面に対す
る法線方向の磁界成分)の最大密度点を有するように磁
化設定されている。この法線方向磁界成分か、現像領域
の範囲内で回転体外周面に現像剤を磁気的に拘束してい
わゆる「゛穂立ち」を形成させ、上記像担持体へ現像剤
を移行せしめている。In this case, a magnet having a plurality of magnetic poles is fixedly installed inside the rotary body as a means for magnetically attracting the developer to the surface of the rotary body. One of the plurality of magnetic poles is located within the range of the development area and near a position corresponding to the proximity of the image carrier and the rotating body, and is located approximately at the center of the development area and has a normal line. The magnetization is set to have the maximum density point of the directional magnetic field component (magnetic field component in the normal direction to the surface of the rotating body). This normal magnetic field component magnetically restrains the developer on the outer circumferential surface of the rotating body within the range of the development area to form a so-called "stiffness" and transfer the developer to the image carrier. .
ところが、現像領域の両端側へと向うにしたがい上記法
線方向磁界成分の密度が徐々に減少し、逆に接線方向磁
界成分(上記回転体の外周面に対する接線方向の磁界成
分)の密度が徐々に増す。However, as one moves toward both ends of the developing area, the density of the normal magnetic field component gradually decreases, and conversely, the density of the tangential magnetic field component (the magnetic field component in the tangential direction to the outer peripheral surface of the rotating body) gradually decreases. increase to
その結実現像領域の両端側になるほど現像剤の穂か回転
体側に傾斜してしまい、そのためその部分での現像がな
された画像には種々の障害が生じる。例えば第9図(A
)に示されるように、「尾引き」と称され、像担持体の
移動方向とは逆方向に画像から現像剤が線状に延びて尾
を引いているように見える状態や、「飛び散り」と称さ
れ上記「尾引き」がさらに悪化して複写画像の周近部に
まで現像剤の粒子が飛び敗る状態などの画像形成に悪影
響を与える。The closer the developer is to both ends of the image area, the more the developer tip is inclined toward the rotating body, causing various problems in the image developed in that area. For example, Fig. 9 (A
), this is called "tailing" and is a condition in which the developer appears to be trailing in a linear manner from the image in the opposite direction to the direction of movement of the image carrier, or "splatter". The above-mentioned "tailing" is further worsened, and this adversely affects image formation, such as a state in which developer particles are scattered even near the periphery of the copied image.
このときの現像領域を拡大し、現像剤の穂立ちの様子を
示したのが第8図(A)である。同図において現像剤相
持体としての現像スリーブ2上に現像剤10が担持され
ている。また、像担持体としての感光ドラムi上には静
電潜像(第8図では参照符号11のマイナス極性として
表わされている)が担持されている。そして感光ドラム
1と現像スリーブ2との最近接部(図示の場合、現像領
域の中央部)では現像スリーブ2上で穂立ちした現像剤
lOが電気的吸引力を受けて感光ドラム1側へ移動する
。しかし、現像領域中央部から両端側の非現像領域へと
向うにしたがい、水平磁界成分の影響を受けて穂が徐々
に傾斜するようになってくる。この傾向は、参照符号1
2で示されるごとく現像領域両端部においてはかなり顕
著に表われている。例えば、第8図(A)に示された現
像領域の左側部分においては、現像スリーブ2上で傾斜
している現像剤10の穂の一部が、感光ドラム1と現像
スリーブ2との間隔が大きくなる傾向にあるにも拘らず
、矢印W方向に電気的に感光ドラム1へ吸引されていく
ために、回転している感光ドラム1上では感光ドラム回
転方向Bとは逆方向に現像剤10のずれが生じてしまう
。この現像剤10のずれか複写画像上では後方に線状と
なって延びる上述の1尾引き」である。また、上記穂の
一部が飛行中、或いはドラムに衝突した衝撃でばらばら
になると、前記「飛びちり」現象が生ずる。FIG. 8(A) shows an enlarged view of the developing area at this time, showing the appearance of spikes of developer. In the figure, a developer 10 is supported on a developing sleeve 2 serving as a developer carrier. Further, an electrostatic latent image (represented by reference numeral 11 of negative polarity in FIG. 8) is carried on the photosensitive drum i as an image carrier. Then, at the closest part between the photosensitive drum 1 and the developing sleeve 2 (in the case shown, the central part of the developing area), the developer lO that has stood up on the developing sleeve 2 is moved toward the photosensitive drum 1 by the electric attraction force. do. However, from the center of the developing area toward the non-developing areas at both ends, the ears gradually become inclined due to the influence of the horizontal magnetic field component. This trend can be seen with reference numeral 1
As shown in 2, it is quite noticeable at both ends of the development area. For example, in the left side portion of the developing area shown in FIG. Even though it tends to increase in size, it is electrically attracted to the photosensitive drum 1 in the direction of the arrow W, so the developer 10 is drawn onto the rotating photosensitive drum 1 in a direction opposite to the photosensitive drum rotation direction B. A misalignment will occur. This deviation of the developer 10 is the above-mentioned "tail" that extends linearly backward on the copied image. Furthermore, when a portion of the ears breaks apart during flight or due to the impact of collision with a drum, the above-mentioned "floating off" phenomenon occurs.
[発明の[1的と概要コ
本発明の目的は、前述の「尾引き」、「飛びちり」の発
生を防止できる現像装置の提供を目的とする。[1.Object and Overview of the Invention] An object of the present invention is to provide a developing device that can prevent the above-mentioned "tailing" and "flying dust" from occurring.
本発明に於いては、現像領域に於いて現像剤の穂を現像
剤支持部材上で起立させるll11極を有する固定磁石
が設けられ、そして上記磁極は、現像剤支持円筒表面で
の法線方向磁界成分の支持円筒回転方向についての変化
率の絶対値が、30ガウス/度以上の極大値を有する磁
界を形成する。In the present invention, a fixed magnet having 11 poles is provided in the development region to make the ears of developer stand up on the developer support member, and the magnetic poles are arranged in the normal direction on the surface of the developer support cylinder. A magnetic field is formed in which the absolute value of the rate of change of the magnetic field component with respect to the rotational direction of the supporting cylinder has a maximum value of 30 Gauss/degree or more.
[実施例]
第3図に於いて、電子写真感光ドラム1は矢印方向Bに
回転し、ドラム1に形成された静電潜像が、ドラム1と
円筒状のアルミニウム、ステンレス絹等の非磁性スリー
ブ2とが微小間+41を間にして対向する現像域りに到
来する。スリーブ2は矢印六方向に回転する。即ち、現
像域りに於いてドラム1とスリーブ2は同方向に回転す
る。スリーブ2は現像剤を支持して現像域Oに搬送する
。現像領域りに於いて現像剤が感光トラムlに供給され
る。[Example] In FIG. 3, the electrophotographic photosensitive drum 1 is rotated in the direction of the arrow B, and the electrostatic latent image formed on the drum 1 is attached to the drum 1 and a cylindrical non-magnetic material such as aluminum or stainless steel silk. The sleeve 2 arrives at the developing area opposite to each other with a minute distance +41 in between. The sleeve 2 rotates in six directions indicated by arrows. That is, the drum 1 and the sleeve 2 rotate in the same direction in the developing area. The sleeve 2 supports and conveys the developer to the development area O. A developer is supplied to the photosensitive tram 1 in the development area.
スリーブ2が回転可能に設けられている容器8には一成
分磁性現像剤(磁性トナー)10が収容されている。撹
拌棒6は現像剤10を現像スリーブ2の方向へ、搬送す
るべく矢印P方向に回転運動している。補助撹拌棒7は
、撹拌棒6方向へ現像剤を搬送すべく矢印Q方向に回転
運動する。A one-component magnetic developer (magnetic toner) 10 is contained in a container 8 in which the sleeve 2 is rotatably provided. The stirring rod 6 rotates in the direction of arrow P to convey the developer 10 toward the developing sleeve 2 . The auxiliary stirring rod 7 rotates in the direction of arrow Q to convey the developer in the direction of the stirring rod 6.
スリーブ2に供給された現像剤は、スリーブ2の中に固
定配置された磁石3の磁力により、スリーブ2の外周面
上に吸引される。磁石3には図では4つの磁石部a、b
、c、dが設けられていて、各磁石部の各1つの磁極(
図にN、Sで示されている)は、磁石の外周部に存在す
る。そして磁極31は現像領域りに対向して配置された
現像1ifl 44であり、6A1極32は現像剤の層
J7を規制する鉄等の磁・ヒ[ブ1ノート4にス4向す
る現像剤層厚規制磁極であり、6ハ極33,34は現像
剤搬送磁極である。The developer supplied to the sleeve 2 is attracted onto the outer peripheral surface of the sleeve 2 by the magnetic force of the magnet 3 fixedly disposed within the sleeve 2 . The magnet 3 has four magnet parts a and b in the figure.
, c, d are provided, and each one magnetic pole (
(indicated by N and S in the figure) are present at the outer periphery of the magnet. The magnetic pole 31 is a developer 1ifl 44 disposed facing the developing area, and the 6A1 pole 32 is a magnetic material such as iron that regulates the developer layer J7. These are layer thickness regulation magnetic poles, and the 6th poles 33 and 34 are developer transporting magnetic poles.
磁性ブレート4には社1極32からの磁界が集中し、こ
れによっ°C磁性現像剤10の薄層がスリーブ2上に形
成される。(特公、昭59−8831号公報参照)スリ
ーブ2上に形成された現像剤層は、現像領域りに於いて
、トラムlとスリーブ2の最小間隙より薄い層厚を有し
ている。尚、スリーブ2上に上記現像剤薄層を形成する
手段としては、特公昭63−16736号公報に記載の
ように、スリーブ2に当接した弾性プレートも使用でき
る。また磁性ブレード4の代りに非IIu性ブレードを
使用してもよい。The magnetic field from the magnetic pole 32 concentrates on the magnetic plate 4, thereby forming a thin layer of °C magnetic developer 10 on the sleeve 2. (Refer to Japanese Patent Publication No. 59-8831) The developer layer formed on the sleeve 2 has a thickness smaller than the minimum gap between the tram l and the sleeve 2 in the developing area. As a means for forming the thin layer of developer on the sleeve 2, an elastic plate that is in contact with the sleeve 2 can also be used, as described in Japanese Patent Publication No. 16736/1983. Moreover, a non-IIu blade may be used instead of the magnetic blade 4.
現像剤は現像領域りに於いては磁8i31の形成する磁
界の法線方向成分によりスリーブ表面上にその穂が起立
せしめられる。即ち磁気ブラシが形成される。そして現
像領域りに於いて現像剤はスリーブ2から飛翔し、ドラ
ム1に付着して静電潜像を現像する。この飛翔を助ける
為に、′心証5によってスリーブ2に直流バイアス電圧
(好ましくは光の露光された潜像部の電位、即ち明部電
位と、光が露光されなかつた潜像部の電位、即ち暗部電
位の間の値の電圧)を印加することが好ましい。或いは
、更に画質を改善する為に、′7ff、源5によりスリ
ーブ2に交番バイアス電圧を印加し、現像領域りに撮動
電界を形成してもよい。この振動電界中で現像剤がドラ
ム1に繰り返して付着、離脱する工程を経て、最終的に
高画質画像が得られる。(特公昭58−32377号公
報参照)尚、交番バイアス電圧は、前記明部電位と暗部
電位の間の値の直流電圧成分を含んだものであることが
好ましい。In the developing area, the developer is caused to stand up on the surface of the sleeve by the normal component of the magnetic field formed by the magnet 8i31. That is, a magnetic brush is formed. Then, in the developing area, the developer flies from the sleeve 2, adheres to the drum 1, and develops the electrostatic latent image. In order to facilitate this flight, DC bias voltage (preferably the potential of the latent image area exposed to light, i.e. bright area potential) and the potential of the latent image area not exposed to light, i.e. It is preferable to apply a voltage with a value between the dark potential. Alternatively, in order to further improve the image quality, an alternating bias voltage may be applied to the sleeve 2 by the source 5 to form a photographing electric field in the developing area. A high-quality image is finally obtained through a process in which the developer repeatedly adheres to and leaves the drum 1 in this oscillating electric field. (Refer to Japanese Patent Publication No. 58-32377.) It is preferable that the alternating bias voltage includes a DC voltage component having a value between the bright area potential and the dark area potential.
第4図で、現像スリーブ2の回転中心2a、感光ドラム
1の回転中心1aを結ぶ線部を基準線りとし、現像スリ
ーブ2上の点をXとする。この基準Pj! Lと現像ス
リーブ2の外周面及び感光ドラム1の外周面との交点を
それぞれXo、 Yoとする。距11fXoYoは現像
スリーブ2と感光ドラム1が対向した最短距菌であり、
XOは現像領域の略中夫に位置することとなる。In FIG. 4, a line connecting the rotation center 2a of the developing sleeve 2 and the rotation center 1a of the photosensitive drum 1 is defined as a reference line, and a point on the developing sleeve 2 is defined as X. This standard Pj! Let the intersections of L and the outer circumferential surface of the developing sleeve 2 and the outer circumferential surface of the photosensitive drum 1 be Xo and Yo, respectively. The distance 11fXoYo is the shortest distance between the developing sleeve 2 and the photosensitive drum 1,
The XO is located approximately in the middle of the development area.
現像スリーブ2上の現像剤により感光ドラムl上の静電
潜像を現像可能とする限界としての、現像スリーブと感
光ドラムとの最長距離を11 may、とする。The maximum distance between the developing sleeve and the photosensitive drum, which is the limit at which the electrostatic latent image on the photosensitive drum l can be developed by the developer on the developing sleeve 2, is 11 may.
このIt maxと等しい長さで、線分X。YOと平行
な、現像スリーブ2と感光体lの表面を結ぶ線分をX、
Y、とする。この線分XIY、は、第4図に示されるご
とくx。を挟む二位置に存在し、現像可能範囲内では対
向する現像スリーブ2と感光ドラム1の対向距離の最長
である。すなわち、この2本の線分に!Yl−XIYI
に挟まれた周方向範囲が現像領域りとして設定し得る範
囲といえる。ここで、It raaxの値は磁界強度等
の設計条件によって変わるので、現像領域として設定し
得る最大範囲(周方向での範囲)もこれに伴ない変動す
ることになるが、本発明者の試験結果によると通常は1
1 wax≦2000μmである。上記した第4図の現
像スリーブ2上の周方向の任意位置Xと現像スリーブ2
の回転中心2aを結んだ線分か、基IV線りとのなず角
度をαとする。また、このときの位置X、の基準線から
の角度をαI+laxとする。ここで、現像領域りは、
角度αによって表わすならばlαmax l以下の範
囲内である。A line segment X with a length equal to this It max. The line segment parallel to YO that connects the developing sleeve 2 and the surface of the photoreceptor l is X,
Let's say Y. This line segment XIY is x as shown in FIG. The distance between the opposing developing sleeve 2 and the photosensitive drum 1 is the longest within the developing range. In other words, these two line segments! Yl-XIYI
It can be said that the circumferential range sandwiched between is the range that can be set as the development area. Here, since the value of It raax changes depending on design conditions such as magnetic field strength, the maximum range (range in the circumferential direction) that can be set as the development area also changes accordingly. According to the results, usually 1
1 wax≦2000 μm. Arbitrary position X in the circumferential direction on the developing sleeve 2 shown in FIG. 4 and the developing sleeve 2
The angle between the line segment connecting the center of rotation 2a and the base IV line is α. Further, the angle of the position X from the reference line at this time is αI+lax. Here, the development area is
If expressed by angle α, it is within the range of lαmax l.
第5図にスリーブ2外周面上での6R界強度、即ち磁束
密度の分イDを極座標的に示した。即ち、スリーブ2の
回転中心2aを中心とした極座標グラフの各角度位置に
、その位置の磁束密度を半径方向にプロットしたもので
ある。但し、円Zは0ガウス線を示す。而して曲線3a
、3b、3c、3dは夫々磁極31,32,33.34
に対応する法線方向磁界成分の強度分布を示す。FIG. 5 shows the 6R field strength on the outer peripheral surface of the sleeve 2, that is, the division D of the magnetic flux density in polar coordinates. That is, at each angular position of a polar coordinate graph centered on the rotation center 2a of the sleeve 2, the magnetic flux density at that position is plotted in the radial direction. However, the circle Z indicates the 0 Gauss line. Therefore, curve 3a
, 3b, 3c, and 3d are magnetic poles 31, 32, 33, and 34, respectively.
The intensity distribution of the normal magnetic field component corresponding to is shown.
第5図にも示されているように、磁極31による法線方
向磁界成分の最大値となる位置、即ち磁極31の中心は
、直線り上、又はこの近傍に位置している。そして、法
線方向磁界成分の強度は上記最大値となる位置から、ス
リーブ回転方向についての上流側、及び下流側に向けて
、夫々次第に弱くなって行く。As shown in FIG. 5, the position where the normal magnetic field component due to the magnetic pole 31 has a maximum value, that is, the center of the magnetic pole 31, is located on or near a straight line. Then, the strength of the normal direction magnetic field component gradually becomes weaker from the position at the maximum value toward the upstream side and the downstream side in the sleeve rotation direction.
占うまでもなく 、 6A1極31に対応する法線方向
671界成分か最大重1°lとなる位置は現像域り内に
存在する。Needless to say, the position where the normal direction 671 field component corresponding to the 6A1 pole 31 has a maximum weight of 1°l exists within the development area.
尚、参考までに、第6図にスリーブ外周を位置座標fq
bとし、直線りを磁界強度座標11ilI+とした場合
の、磁極31にス・i応する法線方向けl異成分の強度
分イ1を摸式的に示した。For reference, Fig. 6 shows the sleeve outer circumference as position coordinate fq.
b, and the intensity component i1 of the l different component in the normal direction corresponding to the magnetic pole 31 is schematically shown when the straight line is taken as the magnetic field intensity coordinate 11ilI+.
さて、前述したように、1尾引き」、「飛び敗り」の発
生は、現像剤の穂がスリーブ上でゆっくりと傾斜して行
くこと、或いはゆっくりと起立して行くことに起因する
ことをつきとめた。そして現像剤の穂の傾斜して行く場
合、起立して行く度合は、法線方向磁界成分の強度の変
化率に対応する。というのは、法線方向磁界成分が現像
剤の穂をスリーブ上に起立させるのに寄与するからであ
る。Now, as mentioned above, the occurrence of "one tail trailing" and "flying failure" is caused by the developer spike slowly tilting on the sleeve or slowly rising up. I found out. When the ears of developer tilt, the degree to which they stand up corresponds to the rate of change in the intensity of the normal magnetic field component. This is because the normal magnetic field component contributes to causing the spikes of developer to stand up on the sleeve.
而して、発明者の種々実験の結果次の事が判明した。即
ち、第7図に示すように、スリーブ回転中心から見た単
位中心角度当りのスリーブ表面に於ける法線方向磁界成
分の強度(磁束密度)の変化量が絶対値で30ガウス/
度より小ではr1弓き」、「飛び散り」の発生が多く、
画質が劣化する場合が多かった。As a result of various experiments conducted by the inventor, the following was discovered. That is, as shown in Fig. 7, the amount of change in the strength (magnetic flux density) of the normal direction magnetic field component on the sleeve surface per unit center angle as seen from the sleeve rotation center is 30 Gauss/
If it is smaller than 1 degree, there will be a lot of "r1 bowing" and "splashing".
Image quality often deteriorated.
そこで、6n8i31に対応する法線方向磁界成分の変
化率の絶対値に極大値を与λ、かつこの極大値を30ガ
ウス/度以上とすることにより、この極大値の存在する
位置近傍で、現像剤はスリーブ上に急激に穂立ち、或い
は急激に倒れ、前述のr尾引き」、「飛び散り」のない
第9図(B)のような画像が得られた。Therefore, by giving a maximum value λ to the absolute value of the rate of change of the normal direction magnetic field component corresponding to 6n8i31, and making this maximum value 30 Gauss/degree or more, development can be performed near the position where this maximum value exists. The agent suddenly stood up or fell down on the sleeve, and an image as shown in FIG. 9(B) was obtained without the above-mentioned "tailing" or "splatter".
以下では、さらに詳しく本実鹿例装置の現像6B極31
が形成する法線方向磁界成分の磁束密度分布状態を図を
もって具体的に説明する。第2図は、法線方向磁界成分
の磁束密度分布を、本発明実施例装置の現像磁極につい
ては実線3aで、従来装置の現像極については二点鎖線
eでそれぞれ示した図である。横軸は、第3図に示され
る磁極31と、現像スリーブ2の回転方向Aにおいて上
流側に位置する磁極32との中間位置にあって、磁極3
1の現像極の法線方向磁界成分の密度が0ガウスとなる
位置をノ、(型位置θ0とし、現像スリーブ2の回転中
心2aに対して下流側へf、(+度θをもって示されて
いる。縦軸は現像スリーブ2の表面での法線方向磁界成
分磁束密度G(ガウス)で表わしている。同図において
、本実施例と従来装置の両者を比較すると本実施例の場
合(実線3a)の方が従来装置(二欝」f1線e)より
も磁極中央位置(角度θ=50度近辺)の最大磁束密度
点Sの近傍では密度の変化率が比較的安定しており、中
央値Isから両側へ所定距列となる位置で変化率が大き
くなっている。−上記の関係をより明らかにするため第
2図のMi1袖の垂直磁界成分の磁束密度(G(ガウス
))を上記角度θで微分し、角度θに対する変化率を縦
軸にとったものが第1図である。3a’が曲線3aの変
化率、eoが曲線eの変化率である。この両者を比較す
ると、中央位置Sから両側へ所定距離となる位置で、変
化率が大きく、極大値N及び極小値N2(絶対値で見る
と極大値となる)が明瞭となっている。そして極大値N
1.及び極小値N2の絶対値lN21はいずれも30ガ
ウス/度より大である。従って、第8図(B)に示され
ているように、N、、 N2の位置近傍に於いて、現像
剤の穂はスリーブ2上に急激に起立する、換言すれば起
立領域の外側で穂はスリーブ2上に急激に倒れる。この
ように穂がスリーブ2Lに起立した領域とスリーブ外周
面に対する接線方向の磁界成分により穂がスリーブ2に
沿って寝た領域との境界部が相対的に明瞭になる。そし
てスリーブ2に沿って穂が寝た領域の現像剤は感光ドラ
ムに向けての飛翔が抑制されるので、第8図(B)の状
態に於いては、スリーブ回転方向に関しN3点の上流側
、N2点の下流側の現像剤の感光ドラムへの飛翔は生じ
にくい。一方、N1点、N2点の間の領域では現像剤の
穂はスリーブに対して大きな、或いはスリーブに対し垂
直に近角度をもって起立していて現像剤の個々の粒子が
整然と配列されているので、この領域では現像剤はドラ
ム1に向って飛翔、付着しやすく、かつ「尾引き」や「
飛び散り」となるような飛翔、付着の仕方は抑制される
。Below, in more detail, the development 6B pole 31 of the Honjishika example device will be described.
The magnetic flux density distribution state of the normal direction magnetic field component formed by will be specifically explained using diagrams. FIG. 2 is a diagram in which the magnetic flux density distribution of the normal direction magnetic field component is shown by a solid line 3a for the developing magnetic pole of the apparatus according to the embodiment of the present invention, and by a two-dot chain line e for the developing pole of the conventional apparatus. The horizontal axis is located at an intermediate position between the magnetic pole 31 shown in FIG. 3 and the magnetic pole 32 located on the upstream side in the rotation direction A of the developing sleeve 2.
The position where the density of the magnetic field component in the normal direction of the developing pole 1 is 0 Gauss is defined as the (mold position θ0), and the position where the density of the magnetic field component in the normal direction of the developing pole 1 becomes 0 Gauss is expressed as f, (+ degrees θ) toward the downstream side with respect to the rotation center 2a of the developing sleeve 2. The vertical axis represents the normal direction magnetic field component magnetic flux density G (Gauss) on the surface of the developing sleeve 2. In the figure, when comparing both the present embodiment and the conventional device, the present embodiment (solid line) In 3a), the rate of change in density is relatively stable near the maximum magnetic flux density point S at the center position of the magnetic pole (near angle θ = 50 degrees) than in the conventional device (F1 line e); The rate of change becomes large at positions where there is a predetermined distance sequence on both sides from the value Is. - To clarify the above relationship, the magnetic flux density (G (Gauss)) of the vertical magnetic field component of the Mi1 sleeve in Fig. 2 is Figure 1 shows the differentiation with respect to the angle θ and the rate of change with respect to the angle θ is plotted on the vertical axis. 3a' is the rate of change of curve 3a, and eo is the rate of change of curve e. Comparing these two, , at positions a predetermined distance from the center position S to both sides, the rate of change is large, and the local maximum value N and local minimum value N2 (the local maximum value when viewed in absolute value) are clear.Then, the local maximum value N
1. and the absolute value lN21 of the minimum value N2 are both greater than 30 Gauss/degree. Therefore, as shown in FIG. 8(B), near the positions N, N2, the spikes of developer suddenly rise on the sleeve 2, in other words, the spikes of developer rise outside the rising area. suddenly falls onto sleeve 2. In this way, the boundary between the area where the ears stand up on the sleeve 2L and the area where the ears lie down along the sleeve 2 becomes relatively clear due to the magnetic field component in the tangential direction to the outer peripheral surface of the sleeve. Since the developer in the area where the spikes lie along the sleeve 2 is suppressed from flying toward the photosensitive drum, in the state shown in FIG. , the developer downstream of the N2 point is unlikely to fly to the photosensitive drum. On the other hand, in the region between points N1 and N2, the ears of developer are large relative to the sleeve, or stand up at a near angle perpendicular to the sleeve, and the individual particles of developer are arranged in an orderly manner. In this area, the developer tends to fly toward the drum 1 and adhere to it, causing "tailing" and "
Flying and adhering methods that result in "splatter" are suppressed.
而してN、点は現像域りの入口側端部E近傍、即ち現像
域りのスリーブ回Iliム方向上流側の端部の近傍に、
N2点は現像域りの出口側端部F近傍、即ち現像域りの
スリーブ回転方向下流側の端部の近傍に配置するのが好
ましい。N3点を現像域りの入口側端部Eを中心に、ス
リーブ回転方向上流側、下流側に夫々1mm以内の範囲
に位置させ、またN2点は現像域りの出口側端部Fを中
心に、スリーブ回転方向上流側、下流側に夫々II以内
の範囲に位置させると、「尾引き」 「飛び散り」防止
に良好な結果が得られる。Therefore, the point N is near the inlet side end E of the developing area, that is, near the upstream end of the developing area in the sleeve rotation direction.
It is preferable that point N2 be placed near the outlet side end F of the developing area, that is, near the end of the developing area on the downstream side in the rotational direction of the sleeve. Point N3 is located within 1 mm on the upstream and downstream sides of the sleeve rotation direction, centering on the entrance end E of the developing area, and point N2 is located around the exit end F of the developing area. If the sleeve is located within II on the upstream and downstream sides in the rotational direction of the sleeve, good results can be obtained in preventing "tailing" and "splashing".
また、N3点、N7点は、磁極31の中心Sから、スリ
ーブ回転方向に関して上流側、下流側に夫々30度以内
に設けることが好ましい。また、現像剤を感光ドラムに
対して飛翔、付着させるにはドラムとスリーブ間の間隙
が一般的に2000μm以下であることが好ましいので
、N3点s N2点はドラムとスリーブ間の間隙が20
00μm以下となる領域に位置させることが好ましい。Further, it is preferable that the points N3 and N7 are provided within 30 degrees on the upstream side and the downstream side, respectively, from the center S of the magnetic pole 31 with respect to the rotational direction of the sleeve. In addition, in order for the developer to fly and adhere to the photosensitive drum, it is generally preferable that the gap between the drum and the sleeve is 2000 μm or less, so for the N3 point s, the gap between the drum and the sleeve is 20 μm or less.
It is preferable to locate it in a region where the thickness is 00 μm or less.
ところで、現像領域の入口側近傍の現像剤は出口側近傍
の現像剤に比へて感光ドラムに対して相対的に飛翔しに
くい。従って入口近傍に於いて現像剤か第8図(A)に
示す状態であっても、それに起因する「尾引き」、「飛
び敗り」は比較的軽微である。それ故、現像領域りの出
口側端部Fの近傍にのみ、法線方向磁界成分の強度の変
化率の絶対値が極大値(30ガウス/度以上)が存在す
るように、磁石を磁化させてもよい。この場合、現像域
りの入口近傍では第2図(A)のような現像剤の穂の状
態となり、出口近傍では第8図(B)に示すような穂の
状態となる。Incidentally, the developer near the entrance side of the developing area is less likely to fly toward the photosensitive drum than the developer near the exit side. Therefore, even if the developer is in the state shown in FIG. 8(A) near the entrance, "tailing" and "flying away" caused by this are relatively minor. Therefore, the magnet is magnetized so that the absolute value of the rate of change in the intensity of the normal direction magnetic field component has a maximum value (30 Gauss/degree or more) only in the vicinity of the exit side end F of the developing area. It's okay. In this case, near the entrance of the developing area, the developer will be in a spiked state as shown in FIG. 2(A), and near the exit, the developer will be in a spiked state as shown in FIG. 8(B).
次に、本発明の他の実施例装置として現像スリーブ2と
感光ドラムlの間に隔絶板を設けた装置について説明す
る。ただし、本実施例装置は上述第一の実施例装置とそ
の多くを共通とするので、第4図に本実施例の特徴であ
る隔絶板14を同図において二点鎖線で示し、他の部分
については説明を省略する。本実施例装置は、現像領域
両端部の傾斜した現像剤が現像に関与せぬよう隔絶板1
4を設けた。この隔絶板14は、少なくともX、X、の
範囲内に先H,iMかイ装置するように現像スリーブ2
と感光体1との間でスリーブ2の長平方向に配設されて
いる。その材質は使用する現像剤の性質や周辺部材によ
り非磁性、磁性、絶縁性、導伝性等について選択が可能
である。またその形状についても第4図に示されるごと
く先端部を尖状形と1/−rもよいし、矩形としてもよ
い。第4図のごとく隔絶板14を先端部を現像領域の出
口端部F近傍に設置した場合には、例えば(lrnay
、=2000μmの場合基部での厚さが5〜1500
limのポリエチレン テレフタレートやステンレス鋼
板が使用できる。第4図では隔絶板14を現像領域出口
端部Fにのみ設けたが、入口端部Eのみに設けることも
可能であるし、両方に設けることも可能である。以上の
ような本実施例装置によるならば現像領域の端部での傾
斜が大きい現像剤の穂立ちによる現像をざらに確実に防
止できる。Next, as another embodiment of the present invention, an apparatus in which a separating plate is provided between the developing sleeve 2 and the photosensitive drum 1 will be described. However, since the device of this embodiment has many of the same features as the device of the first embodiment described above, the isolation plate 14, which is a feature of this embodiment, is shown in FIG. The explanation will be omitted. In this embodiment, the device has a partition plate 1 to prevent the inclined developer at both ends of the development area from participating in the development.
4 was established. This isolation plate 14 is arranged so that the developing sleeve 2 is located within the range of at least X,
and the photoreceptor 1 in the longitudinal direction of the sleeve 2 . The material can be selected from non-magnetic, magnetic, insulating, conductive, etc., depending on the properties of the developer used and surrounding materials. Also, regarding its shape, the tip may be pointed or 1/-r as shown in FIG. 4, or it may be rectangular. As shown in FIG.
, = 2000 μm, the thickness at the base is 5 to 1500 μm
Polyethylene terephthalate and stainless steel plates can be used. In FIG. 4, the isolation plate 14 is provided only at the exit end F of the developing area, but it is also possible to provide it only at the entrance end E, or it is also possible to provide it at both. According to the apparatus of this embodiment as described above, it is possible to roughly and reliably prevent development due to spikes of developer having a large slope at the end of the development area.
なお、以上説明した本発明装置に使用する磁石としては
貼り合せタイプ、埋め込みタイプ、フェライト焼結タイ
プ、磁性粉含有樹脂の一体成形タイブ等広く適用可能で
ある。特に一体成形樹脂磁石は小径化か可1ヒであり、
廉価、軽量でもあるので有用である。The magnets used in the above-described apparatus of the present invention may be of a bonded type, an embedded type, a ferrite sintered type, an integrally molded type made of resin containing magnetic powder, etc. In particular, the diameter of integrally molded resin magnets can be reduced,
It is useful because it is inexpensive and lightweight.
また、現像磁極磁化設定も、法線方向磁界成分の強度分
布がその最大磁束密度点を中央とし左右対称である必要
はなく、非対称であっても、また歪んだ形状のものであ
るようにしてもよい。In addition, the development magnetic pole magnetization setting is such that the intensity distribution of the normal direction magnetic field component does not have to be symmetrical with the maximum magnetic flux density point at the center, but may be asymmetrical or have a distorted shape. Good too.
また、−成分磁性現像剤のみならず、磁性キャリアとト
ナーを有する二成分現像剤を使用する装置にも本発明は
適用できる。Furthermore, the present invention can be applied not only to a one-component magnetic developer but also to an apparatus using a two-component developer having a magnetic carrier and a toner.
[効果]
本発明では、現像剤の穂を急激に寝かせることによって
、画像上に1尾引き」、「飛び散り」が発生するのを防
止できるものである。[Effect] According to the present invention, by rapidly laying down the spikes of developer, it is possible to prevent the occurrence of "tails" and "splatters" on the image.
第1図は法線方向磁界成分の変化率の説明図、第2図は
現像スリーブ表面上での法線方向磁界成分分布の説明図
、第3図は本発明の一実施例の説明図、第4図は現像領
域の説明図、第5図は法線方向磁界成分の強度分布の説
明図、第6図は法線方向6点1界成分の強度分布の他の
説明図、第7図は効果の説明図、第8図(A)・は従来
例に於ける現像剤の状態の説明図、第8図(B)に本発
明に於ける現像剤の状態の説明図、第9図(A)は従来
例による現像画像の説明図、第9図(B)は本発明によ
る現像画像の説明図、である。
1は電子写真感光体ドラム、2は現像スリーブ、3は磁
石、31,32,33.34は磁極、N2は極小値であ
る。
(θ、ノ
P120
l
良
す
θ
10 ご 30 ω タ 1t11dクー1弘鐵’
7頗ALに族′分の厖矛τ崖斐化宰0糸已灯を黒5fE
l
(A)
第6図(已)FIG. 1 is an explanatory diagram of the rate of change of the normal direction magnetic field component, FIG. 2 is an explanatory diagram of the normal direction magnetic field component distribution on the surface of the developing sleeve, and FIG. 3 is an explanatory diagram of an embodiment of the present invention. Fig. 4 is an explanatory diagram of the development area, Fig. 5 is an explanatory diagram of the intensity distribution of the magnetic field component in the normal direction, Fig. 6 is another explanatory diagram of the intensity distribution of the field component at 6 points in the normal direction, and Fig. 7 8(A) is an explanatory diagram of the effect, FIG. 8(A) is an explanatory diagram of the state of the developer in the conventional example, FIG. 8(B) is an explanatory diagram of the state of the developer in the present invention, and FIG. 9(A) is an explanatory diagram of a developed image according to a conventional example, and FIG. 9(B) is an explanatory diagram of a developed image according to the present invention. 1 is an electrophotographic photosensitive drum, 2 is a developing sleeve, 3 is a magnet, 31, 32, 33, 34 are magnetic poles, and N2 is a minimum value. (θ, ノP120 l good θ 10 go 30 ω ta 1t11dku 1 Kotetsu'
7 AL, the tribe's sword, τ Gai, and the black 5fE.
l (A) Figure 6 (已)
Claims (9)
る現像剤を支持して現像領域に搬送する可回転現像剤支
持部材と、 上記現像剤支持部材上の現像剤層の厚みを、それが現像
領域に於いて、像担持体と現像剤支持部材間の最小間隙
よりも薄くなるように規制する層厚規制部材と、 上記現像剤支持部材の内側に固定配置され、上記現像領
域に於いて現像剤の穂を現像剤支持部材上で起立させる
磁石と、 を有し、 上記磁石は、現像剤支持部材表面での法線方向磁界成分
の現像剤支持部材回転方向についての変化率の絶対値が
極大値となる位置が上記現像領域の出口側端部近傍であ
るような磁界を形成し、かつ前記極大値は30ガウス/
度以上であることを特徴とする現像装置。(1) A rotatable developer support member that faces the image carrier in the development area, supports a magnetic developer, and transports it to the development area; and the thickness of the developer layer on the developer support member. , a layer thickness regulating member that regulates the layer thickness to be thinner than the minimum gap between the image carrier and the developer supporting member in the developing area; and a layer thickness regulating member fixedly arranged inside the developer supporting member, the developing area a magnet for causing ears of developer to stand up on a developer support member; A magnetic field is formed such that the position where the absolute value of
A developing device characterized in that the temperature is higher than 100%.
る現像剤を支持して現像領域に搬送する可回転現像剤支
持部材と、 上記現像剤支持部材上の現像剤層の厚みを、それが現像
領域に於いて、像担持体と現像剤支持部材間の最小間隙
よりも薄くなるように規制する層厚規制部材と、 上記現像剤支持部材の内側に固定配置され、上記現像領
域に於いて現像剤の穂を現像剤支持部材上で起立させる
磁石と、 を有し、 上記磁石は、現像剤支持部材表面での法線方向磁界成分
の現像剤支持部材回転方向についての変化率の絶対値が
、上記現像領域の入口側端部近傍で第1の極大値をとり
、出口側端部近傍で第2の極大値をとるような磁界を形
成し、かつ前記第1と第2の極大値は夫々30ガウス/
度以上であることを特徴とする現像装置。(2) A rotatable developer support member that faces the image carrier in the development area and supports a magnetic developer and transports it to the development area, and a thickness of the developer layer on the developer support member. , a layer thickness regulating member that regulates the layer thickness to be thinner than the minimum gap between the image carrier and the developer supporting member in the developing area; and a layer thickness regulating member fixedly arranged inside the developer supporting member, the developing area a magnet for causing ears of developer to stand up on a developer support member; A magnetic field is formed in which the absolute value of the developing area takes a first maximum value near the entrance end of the development area and a second maximum value near the exit end of the development area, and the first and second The maximum value of each is 30 Gauss/
A developing device characterized in that the temperature is higher than 100%.
る現像剤を支持して現像領域に搬送する可回転現像剤支
持円筒と、 上記現像剤支持円筒上の現像剤層の厚みを、それが現像
領域に於いて、像担持体と現像剤支持部材間の最小間隙
よりも薄くなるように規制する層厚規制部材と、 上記現像剤支持円筒の内側に固定配置され、上記現像領
域に於いて現像剤の穂を現像剤支持円筒上で起立させる
磁極を有する磁石と、 を有し、 上記磁極は、現像剤支持円筒表面での法線方向磁界成分
の支持円筒回転方向についての変化率の絶対値が、30
ガウス/度以上の極大値を有する磁界を形成することを
特徴とする現像装置。(3) A rotatable developer support cylinder that faces the image carrier in the development area and supports a magnetic developer and transports it to the development area; and the thickness of the developer layer on the developer support cylinder. , a layer thickness regulating member that regulates the layer thickness to be thinner than the minimum gap between the image carrier and the developer supporting member in the developing area; and a layer thickness regulating member fixedly arranged inside the developer supporting cylinder, the developing area a magnet having a magnetic pole that causes ears of developer to stand up on the developer supporting cylinder; The absolute value of the rate is 30
A developing device characterized by forming a magnetic field having a maximum value of Gauss per degree or more.
対して現像剤支持円筒回転方向についての下流側の位置
である請求項(3)に記載の現像装置。(4) The developing device according to claim 3, wherein the position where the maximum value exists is a position downstream of the center of the magnetic pole in the rotational direction of the developer support cylinder.
、前記磁極の中心から現像剤支持円筒回転方向下流側に
向けて減少して行く請求項(4)に記載の現像装置。(5) The developing device according to claim 4, wherein the strength of the normal component of the magnetic field formed by the magnetic pole decreases from the center of the magnetic pole toward the downstream side in the rotational direction of the developer support cylinder.
回転方向についての変化率の絶対値が30ガウス/度以
上の第2の極大値を、磁極の中心に対して現像剤支持円
筒回転方向についての上流側の位置に有する磁界を形成
する請求項(4)に記載の現像装置。(6) The magnetic pole has a second maximum value of 30 Gauss/degree or more in which the absolute value of the rate of change of the normal direction magnetic field component in the direction of rotation of the developer support cylinder is set to a second maximum value of 30 Gauss/degree or more. The developing device according to claim 4, wherein the developing device forms a magnetic field at an upstream position in the rotation direction.
記磁極の中心から現像剤支持円筒回転方向についての上
流側、下流側に向けて、夫々減少して行く請求項(6)
に記載の現像装置。(7) The strength of the magnetic field formed by the magnetic pole in the normal direction decreases from the center of the magnetic pole toward the upstream side and the downstream side in the rotational direction of the developer supporting cylinder.
The developing device described in .
る手段、を有する請求項(3)乃至(7)のいずれかに
記載の現像装置。(8) The developing device according to any one of claims (3) to (7), further comprising means for applying an alternating bias voltage to the developer supporting cylinder.
る手段、を有する請求項(3)乃至(7)のいずれかに
記載の現像装置。(9) The developing device according to any one of claims (3) to (7), further comprising means for applying a DC bias voltage to the developer supporting cylinder.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9501789A JPH0284679A (en) | 1988-04-15 | 1989-04-14 | Developing device |
Applications Claiming Priority (4)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP9126688 | 1988-04-15 | ||
JP63-91266 | 1988-04-15 | ||
JP63-154954 | 1988-06-24 | ||
JP9501789A JPH0284679A (en) | 1988-04-15 | 1989-04-14 | Developing device |
Publications (1)
Publication Number | Publication Date |
---|---|
JPH0284679A true JPH0284679A (en) | 1990-03-26 |
Family
ID=26432718
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP9501789A Pending JPH0284679A (en) | 1988-04-15 | 1989-04-14 | Developing device |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPH0284679A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1235119A2 (en) * | 2001-02-26 | 2002-08-28 | Canon Kabushiki Kaisha | Developer-carrying member, and developing apparatus and image forming apparatus including the member |
Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60146274A (en) * | 1984-01-10 | 1985-08-01 | Canon Inc | Developing device |
JPS61151578A (en) * | 1984-12-26 | 1986-07-10 | Casio Comput Co Ltd | Developing device |
-
1989
- 1989-04-14 JP JP9501789A patent/JPH0284679A/en active Pending
Patent Citations (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
JPS60146274A (en) * | 1984-01-10 | 1985-08-01 | Canon Inc | Developing device |
JPS61151578A (en) * | 1984-12-26 | 1986-07-10 | Casio Comput Co Ltd | Developing device |
Cited By (2)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
EP1235119A2 (en) * | 2001-02-26 | 2002-08-28 | Canon Kabushiki Kaisha | Developer-carrying member, and developing apparatus and image forming apparatus including the member |
EP1235119A3 (en) * | 2001-02-26 | 2005-12-14 | Canon Kabushiki Kaisha | Developer-carrying member, and developing apparatus and image forming apparatus including the member |
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