JPH0225873A - Developing device - Google Patents

Developing device

Info

Publication number
JPH0225873A
JPH0225873A JP17497188A JP17497188A JPH0225873A JP H0225873 A JPH0225873 A JP H0225873A JP 17497188 A JP17497188 A JP 17497188A JP 17497188 A JP17497188 A JP 17497188A JP H0225873 A JPH0225873 A JP H0225873A
Authority
JP
Japan
Prior art keywords
magnetic field
developing
rotating body
area
developer
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Granted
Application number
JP17497188A
Other languages
Japanese (ja)
Other versions
JPH087500B2 (en
Inventor
Takao Honda
本田 孝男
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 JP63174971A priority Critical patent/JPH087500B2/en
Publication of JPH0225873A publication Critical patent/JPH0225873A/en
Publication of JPH087500B2 publication Critical patent/JPH087500B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Abstract

PURPOSE:To prevent image troubles such as a tailing and a scattering by setting the change rate of the magnetic flux density of the horizontal magnetic field components of a developing pole at both edges of a developing area in correcting it so that it can be enlarged. CONSTITUTION:The developing pole is magnetize-set so that the absolute value of the density change rate of the horizontal magnetic field components at both edges of the developing area can be made into a maximum value. Namely, when a developing device is activated, a developer 10 made into a thin layer on the surface of a rotor 2 is carried to the close area of an electrostatic latent image carrier 1 and the rotor 2. The developer 10 is arranged in the close area of the rotor 2, it is napped by the magnetic field of a magnetic pole set so as to form both edges of the developing area in a position and the vicinity where the absolute value of the change rate of the density of the horizontal magnetic field components to the circumference direction distance of the rotor 2 is made into the maximum value, and a visible image is prepared according to the charge of an electrostatic latent image carried by the electrostatic latent image carrier 1. Thus, the adverse effects in an image preparation such as the tailing and scattering can be eliminated.

Description

【発明の詳細な説明】 [産業上の利用分野] この発明は静電潜像を現像剤にて現像する技術の分野に
おいて利用され、特に現像剤を磁気力で拘束して現像を
行なう現像装置に関する。
[Detailed Description of the Invention] [Field of Industrial Application] The present invention is utilized in the field of technology for developing electrostatic latent images with a developer, and in particular, a developing device that performs development by restraining the developer with magnetic force. Regarding.

[従来の技術] 従来、この種の現像装置は静電潜像担持体と、この静電
潜像担持体と近接領域を形成するように外周面を対向し
て配設し、その外周面に磁性を有する現像剤を担持する
非磁性の回転体とで構成されている。そして、上記近接
領域内において、この両者の外周面対向距離が一定値以
下となる所定域、すなわち一定の磁界強度の領域を現像
領域としている。
[Prior Art] Conventionally, this type of developing device has an electrostatic latent image carrier and an electrostatic latent image carrier, which is disposed with its outer circumferential surface facing each other so as to form a close area with the electrostatic latent image carrier. It is composed of a non-magnetic rotating body that carries a magnetic developer. A predetermined area within the above-mentioned proximity area where the distance between the two outer peripheral surfaces facing each other is equal to or less than a certain value, that is, an area where the magnetic field strength is constant is defined as a development area.

この場合、上記回転体の表面で現像剤を担持する手段と
して、回転体の内部に−・磁極が回転体外周面側に向く
よう磁石を複数項する磁界発生体が固定設置されている
。そして、この磁界発生体を構成する複数の磁石のうち
一磁石は、上記静電潜像体と上記回転体の近接領域の範
囲内にあって最近接部に対応する位置の近傍に配設され
、回転体外周面側の一磁極が現像領域の略中央部で垂直
磁界成分(上記回転体の表面に対し垂直な磁界成分)の
最大密度点を有するように磁化設定されている。この垂
直磁界成分が、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、
上記静電潜像担持体へ現像剤を移行せしめている。
In this case, as a means for supporting the developer on the surface of the rotating body, a magnetic field generating body including a plurality of magnets is fixedly installed inside the rotating body so that the magnetic poles are directed toward the outer peripheral surface of the rotating body. One of the plurality of magnets constituting the magnetic field generator is disposed in the vicinity of a position corresponding to the closest portion within the range of the vicinity of the electrostatic latent image body and the rotary body. The magnetization is set such that one magnetic pole on the outer circumferential surface of the rotating body has a maximum density point of a perpendicular magnetic field component (a magnetic field component perpendicular to the surface of the rotating body) approximately at the center of the developing area. This perpendicular magnetic field component magnetically restrains the developer on the outer circumferential surface of the rotating body within the range of the development area, forming a so-called "standing spike".
The developer is transferred to the electrostatic latent image carrier.

[発明が解決しようとする課題] しかしながら、従来の現像装置にあフては、現像領域の
両端側へと向うにしたがい磁石の上記垂直磁界成分の密
度か徐々に減少し、逆に水平磁界成分(上記回転体の周
方向の磁界成分)の密度が徐々に増す。その結実現像領
域の両端側になるほど現像剤の穂立ちが傾斜してしまい
、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、「尾引き」と称され、上記回転
体の回転に伴ない画像形成の方向(画像が形成される記
録材の搬送方向)とは逆方向に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
まで現像剤の粒子か飛び散る状態などの画像形成に悪影
響を与える。
[Problems to be Solved by the Invention] However, in the conventional developing device, the density of the vertical magnetic field component of the magnet gradually decreases toward both ends of the developing area, and conversely, the density of the horizontal magnetic field component decreases toward both ends of the developing area. (The magnetic field component in the circumferential direction of the rotating body) gradually increases in density. The developer spikes become more inclined towards both ends of the formed image area, and various problems occur in the image developed in those areas. For example, this is called "tailing", and as the rotating body rotates, the developer extends linearly in a direction opposite to the direction of image formation (the direction of conveyance of the recording material on which the image is formed), creating a tail. This adversely affects image formation, such as a state in which developer particles appear to be floating, or a state in which the above-mentioned "tailing" (referred to as "splatter") is further worsened and developer particles are scattered 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7図である。同図において現像剤担持体と
しての現像スリーブ2.1:に現像剤10が担持されて
いる。また、静電潜像担持体としての感光ドラムl上に
は静電潜像(第7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l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10が電気的吸引力を受けて感光ドラムl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立
ち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12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0例えば、第7図に示された
現像領域の左側部分に8いては、現像スリーブ2上で傾
斜している現像剤lOの穂立ちの一部が、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lへ吸引され
ていくために、回転している感光ドラム1上では画像形
成方向Aに現像剤10のずれが生じてしまう、この現像
剤10のずれが複写画像上では後方に線状となりで延び
る上述の「尾引き」である。
FIG. 7 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 carried on a developing sleeve 2.1 as a developer carrier. Further, an electrostatic latent image (represented by reference numeral 11 of negative polarity in FIG. 7) is carried on the photosensitive drum l serving as an electrostatic latent image carrier. Then, at the closest part between the photosensitive drum l and the developing sleeve 2 (in the case shown, the central part of the developing area), the developer 10 that has stood up on the developing sleeve 2 is moved toward the photosensitive drum l side by the electric attraction force. do. However, as you move from the center of the developing area to the non-developing areas at both ends, the spikes gradually become inclined due to the influence of the horizontal magnetic field component. This tendency is quite noticeable at both ends of the developing area as shown by reference numeral 12.For example, at the left side of the developing area shown in FIG. Some of the spikes of the developer lO are on the photosensitive drum 1.
Even though the distance between the developing sleeve 2 and the developing sleeve 2 tends to increase, the image forming direction A is generated on the rotating photosensitive drum 1 because it is electrically attracted to the photosensitive drum l in the direction of the arrow W. This deviation of the developer 10 causes the above-mentioned "tailing" which extends in a linear shape backwards on the copied image.

本発明は、従来のこのような現像装置の有していた「尾
引き」、「飛び散りjなどの画像形成における悪影響を
解決することを目的とする。
The object of the present invention is to solve the adverse effects in image formation such as "tailing" and "splatter" that conventional developing devices have.

[課題を解決するための手段] 本発明の現像装置は、上記目的達成のために、静電潜像
担持体と、内部に磁界発生体を有する現像剤担持体とし
ての回転体を、両者の外周面間に最近接部をもつ近接領
域を形成するように配設し、 上記磁界発生体は、上記回転体の上記最近接部に、回転
体表面に垂直な磁界成分の最大密度点を生せしめる位置
に磁極を配され、 上記回転体表面に磁性現像剤を担持し、上記近接領域内
で上記垂直磁界成分により、上記磁性現像剤を穂立ち状
態に形成せしめて現像を行なう現像装置において、 上記磁極が形成する水平磁界成分は、上記回転体の周方
向距離に対する密度の変化率の絶対値が極大値をとる位
置及びその近傍で、現像領域の両端部を形成している。
[Means for Solving the Problems] In order to achieve the above object, the developing device of the present invention includes an electrostatic latent image carrier and a rotating body as a developer carrier having a magnetic field generating member inside. The magnetic field generating body is arranged so as to form a proximate area having the closest portion between the outer circumferential surfaces, and the magnetic field generating body generates a maximum density point of a magnetic field component perpendicular to the surface of the rotating body at the closest portion of the rotating body. In a developing device, a developing device is provided with a magnetic pole at a position where the rotating body is exposed to the rotating body, carries magnetic developer on the surface of the rotating body, and performs development by forming the magnetic developer into a standing state by the perpendicular magnetic field component in the adjacent region, The horizontal magnetic field components formed by the magnetic poles form both ends of the developing area at and near a position where the absolute value of the rate of change in density with respect to the circumferential distance of the rotating body takes a maximum value.

ことによって構成される。It consists of

[作用] 上記のように構成された現像装置が起動するど、回転体
の表面上に薄層化された現像剤が静電潜像担持体と回転
体の近接領域に搬送される。該現像剤は、上記回転体の
近接領域に配設され1回転体の周方向距離に対する水平
磁界成分の密度の変化率の絶対値が極大値をとる位置及
びその近傍で現像領域の両端部を形成するように設定さ
れた磁極の磁界によって穂立ちし、静電潜像担持体に担
持された静1!潜像の電荷に応じて可視像を形成させる
[Operation] When the developing device configured as described above is activated, the developer formed in a thin layer on the surface of the rotating body is transported to an area near the electrostatic latent image carrier and the rotating body. The developer is disposed in the vicinity of the rotating body, and is applied to both ends of the developing area at and near a position where the absolute value of the rate of change in the density of the horizontal magnetic field component with respect to the circumferential distance of the rotating body takes a maximum value. The electrostatic latent image bearing member carries the electrostatic latent image 1! A visible image is formed depending on the charge of the latent image.

[実施例] 以下、添付図面にもとづいて、本発明の実施例装置を説
明する。
[Example] Hereinafter, an example device of the present invention will be described based on the accompanying drawings.

第1図(A)は、一実施例装置としての現像装置で現像
剤担持体としての現像スリーブの周辺を示す断面図であ
り、第1図(B)は第1図(A)の現像スリーブと静電
潜像担持体としての感光ドラムが形成する近接領域を拡
大し、該近接領域内の垂直磁界成分の分布の様子を模式
的に示した図である。
FIG. 1(A) is a sectional view showing the periphery of a developing sleeve as a developer carrier in a developing device as an embodiment, and FIG. 1(B) is a sectional view of the developing sleeve of FIG. 1(A). FIG. 3 is an enlarged view of a close area formed by a photosensitive drum as an electrostatic latent image carrier, and schematically shows the distribution of perpendicular magnetic field components in the close area.

第1図(A)において、現像スリーブ2は、感光ドラム
lに所定間隙をもって対向する位置に入方向に回転自在
に配設されている。該現像スリーブ2の内部には、四つ
の磁石a、b、c、dを周部に有する磁界発生体3が所
定位置に固定設置されている。各磁石は、その対をなす
二磁極の一方の磁極が現像スリーブ2の周面に向くよう
に配置されており、磁石aが現像極を、磁石l)が現像
剤規制様(カフェ・極)を、磁石C及びdが現像剤搬送
極を、それ・ぞれ形成している。
In FIG. 1(A), the developing sleeve 2 is disposed at a position facing the photosensitive drum 1 with a predetermined gap therebetween so as to be freely rotatable in the entrance direction. Inside the developing sleeve 2, a magnetic field generator 3 having four magnets a, b, c, and d around its periphery is fixedly installed at a predetermined position. Each magnet is arranged so that one of its pair of two magnetic poles faces the circumferential surface of the developing sleeve 2, with magnet a serving as a developing pole and magnet l serving as a developer regulating pole (café pole). , magnets C and d form developer transport poles, respectively.

また、現像スリーブ2の上部には、現像剤10の穂立ち
高さを規制して現像スリーブ」二の現像剤を薄層化する
ためのブレード4が上記磁石すに対向した位置に配設さ
れている。現像スリーブ2の右側は、開口にて上該現像
スリーブ2の左部分を突出状態で配置し、かつ該現像ス
リーブ2へ供給する現像剤10を収容するための容器8
となっている。なお、2aは現像スリーブ2の回転中心
であると共に磁界発生体3の固定中心でもある。
Further, a blade 4 is disposed on the upper part of the developing sleeve 2 at a position facing the magnet 2 for regulating the height of the spikes of the developer 10 and thinning the developer in the developing sleeve 2. ing. A container 8 is disposed on the right side of the developing sleeve 2 with the left side of the developing sleeve 2 protruding from the opening, and is used to store the developer 10 to be supplied to the developing sleeve 2.
It becomes. Note that 2a is the center of rotation of the developing sleeve 2 and also the center of fixation of the magnetic field generator 3.

第1図(B)は、上記第1図(A)における近接領域を
拡大して示しており、同図では、磁石aの周表面側の磁
極である現像極(本実施例ではN極)の垂直磁界成分の
分布の様子を、現像スリーブ2の周表面位置での磁束密
度を矢印の長さで示している。
FIG. 1(B) shows an enlarged view of the adjacent area in FIG. 1(A), and in the same figure, the developing pole (in this example, the N pole) is the magnetic pole on the circumferential surface side of the magnet a. The distribution of the perpendicular magnetic field component is shown by the length of the arrow indicating the magnetic flux density at the circumferential surface position of the developing sleeve 2.

周知のように磁石aの磁界は、磁石aを中心として全方
向に形成される。したがって、現像スリーブ2の表面に
は垂直磁界成分と水平磁界成分とが形成され、現像剤の
穂立ちの方向は図中に示された垂直磁界成分と、図示さ
れていない水平磁界成分とによりて決まる。ここで、水
平磁界成分というのは、スリーブ円周での接線の方向に
ついての磁界成分である。
As is well known, the magnetic field of magnet a is formed in all directions with magnet a as the center. Therefore, a vertical magnetic field component and a horizontal magnetic field component are formed on the surface of the developing sleeve 2, and the direction of the developer spikes is determined by the vertical magnetic field component shown in the figure and the horizontal magnetic field component not shown. It's decided. Here, the horizontal magnetic field component is a magnetic field component in the direction of a tangent to the circumference of the sleeve.

この現像極の水平磁界成分の密度分布状態を修正するこ
とにより、既述した従来装置の問題点として指摘した現
像領域の両端部で生じる、現像剤の傾斜した穂立ちによ
る現像を防止することができる。
By correcting the density distribution state of the horizontal magnetic field component of this development pole, it is possible to prevent the development caused by the slanted spikes of developer that occur at both ends of the development area, which is the problem of the conventional device mentioned above. can.

すなわち、現像領域の両端部での、現像極の水平磁界成
分の磁束密度の変化率を大きくなるよう修正して設定す
ることにより上述問題点か解消される。
That is, the above-mentioned problem can be solved by correcting and setting the rate of change of the magnetic flux density of the horizontal magnetic field component of the development pole at both ends of the development area to be large.

以下は、本実施例において、問題点の解消のためにどの
ように現像領域で水平磁界成分の密度分布を形成したか
について詳述する。そこで、先ず1本実施例装置にあフ
て上述近接領域内において現像領域として設定し得る最
大範囲を明らかにするが、これに先立ち、本実施例装訝
の回転体としての現像スリーブ2は略円筒であるので、
現像スリーブ2の周面上に形成される現像領域は、現像
スリーブ2の回転中心2aに対する中心角に対応させて
説明する。
In the following, a detailed description will be given of how the density distribution of the horizontal magnetic field component was formed in the development area in order to solve the problem in this embodiment. Therefore, first of all, we will clarify the maximum range that can be set as the developing area within the above-mentioned proximity area in the apparatus of this embodiment. Since it is a cylinder,
The developing area formed on the circumferential surface of the developing sleeve 2 will be explained in correspondence with the central angle with respect to the rotation center 2a of the developing sleeve 2.

第2図は第1図(B)と同様に現像スリーブ2と感光ト
ラムlの近接領域を表わしている。ここで現像スリーブ
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
。この基準線りと現像スリーブ2の外周面及び感光ドラ
ムlの外周面との交点をそ゛れぞれX、、 Y、とする
、距離X。Y、は現像スリーブ2と感光ドラム1が対向
した最短距離であり、Xoは現像領域の中央に位置する
こととなる。
Similar to FIG. 1(B), FIG. 2 shows the vicinity area between the developing sleeve 2 and the photosensitive tram l. Here, 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. Distance X, where the intersections of this reference line and the outer circumferential surface of the developing sleeve 2 and the outer circumferential surface of the photosensitive drum l are respectively X and Y. Y is the shortest distance between the developing sleeve 2 and the photosensitive drum 1, and Xo is located at the center of the developing area.

この位置X0を含む周方向での近傍にて上述の現像極の
垂直磁界成分の密度がほぼ最大で、かつ水平磁界成分が
ほぼ最小となり、該部分を最近接部として以下説明する
In the vicinity of this position X0 in the circumferential direction, the density of the vertical magnetic field component of the above-mentioned development pole is approximately the maximum, and the horizontal magnetic field component is approximately the minimum, and this portion will be described below as the closest portion.

上述のような最近接部を近接領域のほぼ中央にもつ本実
施例装置にあって、現像スリーブz上の現像剤により感
光ドラム1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2と感光トラム1との最長距離を文■a
xとする。
In the apparatus of this embodiment, which has the above-mentioned closest portion at approximately the center of the adjacent area, the developing speed is the limit for developing the electrostatic latent image on the photosensitive drum 1 with the developer on the developing sleeve z. The longest distance between sleeve 2 and photosensitive tram 1 is written in sentence a.
Let it be x.

この!l wax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1の表面を結ぶ線分なX、
Y□とする。この線分x、y、は、第2図に示されるご
と<XOを挾む二位置に存在し、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lの対向距離の最長
である。すなわち、この2本の線分XtYt、X□Y、
に挾まれた周方向範囲が現像領域として設定し得る範囲
といえる。ここで、l wax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fLwa
x≦2000 u、■であり、その前提で現像領域とし
て設定することが多くの場合好ましい。
this! Line segment X with length equal to l wax. A line segment X connecting the developing sleeve 2 and the surface of the photoreceptor 1 parallel to Yo,
Let Y□. As shown in FIG. 2, the line segments x and y exist at two positions sandwiching <XO, and are the longest facing distance between the opposing developing sleeve 2 and the photosensitive drum l within the developing range. In other words, these two line segments XtYt, X□Y,
It can be said that the circumferential range between the two is the range that can be set as the development area. Here, since the value of l wax 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 fLwa
x≦2000 u, ■, and in many cases it is preferable to set it as the development area on that premise.

次に、上記現像領域における現像極の水平磁界成分の密
度分布について説明する。上記した第2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を結んだ線分が、基準線りどのなす角度なαとす
る。また、このときの位置xlの基準線からの角度をα
■axとする。
Next, the density distribution of the horizontal magnetic field component of the development pole in the development area will be explained. The angle α formed by the line segment connecting the circumferential arbitrary position X on the developing sleeve 2 shown in FIG. Also, the angle of the position xl from the reference line at this time is α
■Let it be ax.

ここで、現像領域は、角度αによって表わすならば1α
wax l以下の範囲内である。この角度αによって表
わされる現像領域内において、回転体の周方向距離に対
する密度の変化率として現像スリーブ2の回転中心2a
に対する単位中心角当りの水平磁界成分の密度変化率(
ガウス7度)の絶対値の極大値で現像領域の両端部を形
成するように現像極を磁化設定する。
Here, the development area is 1α if expressed by the angle α
It is within the range of wax l or less. Within the developing area represented by this angle α, the rotation center 2a of the developing sleeve 2 is expressed as the rate of change in density with respect to the circumferential distance of the rotating body.
The density change rate of the horizontal magnetic field component per unit central angle for
The development poles are magnetized so as to form both ends of the development area at the maximum absolute value of Gauss (7 degrees).

すなわち、現像領域として設定し得る最大範囲の両端の
位1tXt、Lにより挟まれる中央位!!x0を包む範
囲内で、中央位置から両側へ所定距離となる位置を現像
領域の両端部とすべく現像極を磁化設定する。なお第3
図に示されるごとく1回転体中心に対する単位中心角度
当りの水平磁界成分の密度変化線が30ガウス以下では
多くの場合、「尾引き」、「飛び散り」等の画像障害の
発生が確認されており、一般に、密度変化率の絶対値の
極大値は30ガウス/度以上となるよう磁化設定するこ
とが好ましい。
In other words, the center position between the two end positions 1tXt and L of the maximum range that can be set as the development area! ! Within the range surrounding x0, the development poles are magnetized so that positions at a predetermined distance from the center position to both sides are set as both ends of the development area. Furthermore, the third
As shown in the figure, if the density change line of the horizontal magnetic field component per unit center angle with respect to the center of one rotating body is less than 30 Gauss, image disturbances such as "tailing" and "splatter" are often observed to occur. Generally, it is preferable to set the magnetization so that the maximum absolute value of the density change rate is 30 Gauss/degree or more.

以下では、さらに詳しく本実施例装置の現像極が形成す
る垂直及び水平磁界成分の密度分布状態を図をもって具
体的に説明する。第4図には、垂直磁界成分及び水平磁
界成分の密度分布が示されている。
In the following, the density distribution state of the vertical and horizontal magnetic field components formed by the developing pole of the apparatus of this embodiment will be specifically explained with reference to the drawings. FIG. 4 shows the density distribution of the vertical magnetic field component and the horizontal magnetic field component.

なお、図中の実線及び破線は、本実施例による装置の現
像極の垂直磁界成分及び水平磁界成分の密度分布を示し
、また二点鎖線及び−点鎖線は従来の装置の現像極の垂
直磁界成分及び水平磁界成分を示している。
In addition, the solid line and the broken line in the figure show the density distribution of the vertical magnetic field component and the horizontal magnetic field component of the developing pole of the apparatus according to this embodiment, and the dashed-two dotted line and the dashed-dotted line indicate the vertical magnetic field of the developing pole of the conventional apparatus. component and horizontal magnetic field component.

横軸は、第1図(A)に示される磁石a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石すとの
中間位置にあって、磁石aの現像極の垂直磁界成分の密
度がOガウスとなる位置を基準位置θ。とじ、現像スリ
ーブ2の回転中心2aに対して下流側(現像極側)へ角
度θをもって示されている。縦軸は現像スリーブ2の表
面での垂直磁界成分密度及び水平磁界成分密度なG(ガ
ウス)で表わしている。同図において、本実施例と従来
装置の垂直磁界成分密度を比較すると、本実施例の場合
(実線)の方が従来装置(二点鎖線)よりも中央位置(
角度θ=50度近辺)の最大密度点Sを頂点としてその
近傍では密度の変化率が比較的安定しており、中央位置
から両側へ所定距離となる位置て変化率が大きくなって
いる。また、水平磁界成分密度を比較すると、本実施例
(破線)の装置の方が従来の装置(−点鎖線)よりも−
F、記中央位置を最小密度点としてその近傍で密度の変
化率が安定し、中央位置から両側へ上記所定の距離とな
る位置で変化率が大ぎくなっていることがわかる。上記
の関係をより明らかにするため、第4図の縦軸の水平磁
界成分の密度(G(ガウス))を上記角度O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5図であ
る。この両者を比較すると、中央位置から両側へ所定距
離となる位置で、変化率が大きく、極大値(最大値)及
び極小値(最小値)が明瞭となっている。
The horizontal axis is located at an intermediate position between magnet a shown in FIG. The reference position θ is the position where the density is O Gauss. The binding is shown at an angle θ toward the downstream side (towards the developing pole) with respect to the rotation center 2a of the developing sleeve 2. The vertical axis represents the vertical magnetic field component density and the horizontal magnetic field component density G (Gauss) on the surface of the developing sleeve 2. In the figure, when comparing the perpendicular magnetic field component density of this example and the conventional device, it is found that the density of the vertical magnetic field component in the case of this example (solid line) is higher at the center position (double-dashed line) than in the conventional device (two-dot chain line).
The rate of change in density is relatively stable in the vicinity of the maximum density point S at the angle θ = 50 degrees (nearly 50 degrees), and the rate of change increases at positions a predetermined distance away from the center position on both sides. Also, when comparing the horizontal magnetic field component density, the device of this example (dashed line) is -
F. It can be seen that the rate of change in density is stable in the vicinity of the center position as the minimum density point, and that the rate of change becomes large at positions at the predetermined distance from the center position to both sides. In order to clarify the above relationship, the density (G (Gauss)) of the horizontal magnetic field component on the vertical axis in Fig. 4 is differentiated by the angle O, and
FIG. 5 shows the rate of change with respect to the angle θ on the vertical axis. Comparing the two, the rate of change is large at positions a predetermined distance from the center position to both sides, and the local maximum value (maximum value) and local minimum value (minimum value) are clear.

これは、−上述したごとく本実施例装置の現像極は、現
像領域の中央位置から所定距離となる位置(すなわち、
現像領域の両端部となる位置)で、水平磁界成分の密度
変化率の絶対値が極大となるよう設定されているからで
ある。
- As mentioned above, the development pole of the present embodiment apparatus is located at a predetermined distance from the center of the development area (i.e.,
This is because the absolute value of the density change rate of the horizontal magnetic field component is set to be maximum at the positions (positions that are both ends of the development area).

以上説明したごとくに磁化設定された現像極を有する本
実施例装置の現像領域を拡大した現像剤の穂立ちの状態
を示したのが第6図である。現像領域の両端部Nt、 
N、で垂直及び水平の磁界成分の密度の変化率が大きい
ので該現像領域の端部での穂立ちの有無かはっきりとし
ている。その結果。
FIG. 6 is an enlarged view of the developing area of the apparatus of this embodiment, which has developing poles magnetized as described above, and shows the state of developer spikes. Both ends Nt of the development area,
Since the rate of change in the density of the vertical and horizontal magnetic field components is large at N, it is clear whether or not there is a spike at the edge of the development area. the result.

スリーブ2上で垂直に穂立ちした現像剤が現像領域内で
整然と配列されている。その結果、現像剤10は乱れる
ことなく感光ドラムlに吸引移行して「尾引き」、「飛
び散り」等の画像障害を生じない。
The developer particles that stand up vertically on the sleeve 2 are arranged in an orderly manner within the development area. As a result, the developer 10 is attracted and transferred to the photosensitive drum 1 without being disturbed, and image defects such as "tailing" and "splatter" do not occur.

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2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
端部の傾斜した親書剤が現像に関与せぬよう隔絶板14
を設けた。この隔絶板14は、少なくともX、X、の範
囲内に先端か位置するように現像スリーブ2と感光体l
との間でスリーブ2の長手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2図に示されるごとく先端部を
尖状形とbてもよいし、矩形としてもよい。第2図のご
とく隔絶板14の先端部を現像領域の端部近傍に設置し
た場合には、例えば交wax m 2000ル霧の場合
基部での厚さが5〜1500IL閣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2図ては
隔絶板14を現像スリーブ2の回転方向Aの下流側の現
像領域端部にのみ設けたが、上流側のみに設けることも
可能であるし、上流及び下流側に設けることも可能であ
る0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さら
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 above-mentioned first embodiment, 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 separating plate 14 to prevent the inclined letter agent at the end of the developing area from being involved in the development.
has been established. The separating plate 14 is connected to the developing sleeve 2 and the photoreceptor l such that the tip is located within the range of at least X, X.
The sleeve 2 is disposed in the longitudinal direction between the sleeve 2 and the sleeve 2. The material may be non-magnetic, depending on the properties of the developer used and surrounding materials.
It is possible to select magnetism, insulation, conductivity, etc. Regarding its shape, the tip may be pointed or rectangular as shown in FIG. When the tip of the separating plate 14 is installed near the end of the developing area as shown in Fig. 2, for example, in the case of a 2000 m thick wax, a polyethylene terephthalate or stainless steel plate with a thickness of 5 to 1500 IL at the base is used. can be used. In FIG. 2, the isolation plate 14 is provided only at the end of the development area on the downstream side in the rotational direction A of the developing sleeve 2, but it is also possible to provide it only on the upstream side, or it can be provided on the upstream and downstream sides. If the apparatus of this embodiment has a number of 0 or more, it is possible to more 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の磁界発生体に配設する
磁石としてはフェライト焼結タイプ、樹脂性の一体成形
タイブ等広く適用可能である。また、現像極磁化設定も
垂直成分の最大密度点を中央とし左右対称である必要は
なく、非対称であってもよい。
The magnets to be disposed in the magnetic field generating body of the device of the present invention described above can be widely used, such as a sintered ferrite type or an integrally molded resin type. Further, the development pole magnetization setting does not need to be symmetrical with the maximum density point of the vertical component at the center, but may be asymmetrical.

[発明の効果] 以上説明したように、本発明に係る現像装置の現像極は
、現像領域の両端部で、水平磁界成分の密度変化率の絶
対値が極大値となるよう磁化設定したので、現像領域の
両端部において水平磁界成分の密度が急激に変化するこ
ととなり、現像剤の穂立ちの有無をはっきりさせること
かできる。
[Effects of the Invention] As explained above, the developing poles of the developing device according to the present invention are magnetized so that the absolute value of the rate of change in density of the horizontal magnetic field component is the maximum value at both ends of the developing area. The density of the horizontal magnetic field component changes rapidly at both ends of the development area, making it possible to clearly see whether or not the developer is bristling.

よって、傾斜した現像剤により現像がなされるという事
態がなくなり、従来装置の有していた「尾引き」、「飛
び散り」等の画像障害を防止でき、常に高品質の画像を
提供できるという効果をもたらす、磁界発生体は、固定
磁石と樹脂との一体成形によって製作可能であり、フェ
ライト焼結ターイブ磁石、張り合せタイプ、埋め込みタ
イプの磁石に比較して大幅な廉価化及び軽量化も可能と
なる。
Therefore, there is no longer a situation where the developer is slanted during development, and it is possible to prevent image defects such as "tailing" and "splatters" that were present in conventional devices, and it is possible to always provide high-quality images. The resulting magnetic field generator can be manufactured by integrally molding a fixed magnet and resin, making it possible to significantly reduce the cost and weight compared to ferrite sintered tabe magnets, bonded type magnets, and embedded type magnets. .

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

第1図(A)は本発明一実施例装置の概要構成断面図、
第1図(8)は第1図(A)の近接領域を拡大して該領
域での垂直磁界成分密度分布を示した図、第2図は現像
剤担持体と静電潜像担持体の近接領域を示L/、さらに
第二実施例を二点iln線により示した図、第3図は水
平磁界成分密度の変化率と画像障害発生状態との関係を
示す図、第4図は本発明の一実施例装置の現像極と従来
装置の現像極の垂直磁界成分及び水平磁界成分の密度分
布を示した図、第5図は第4図の水Y磁界成分について
回転体の中心角に対する変化率を示した図、第6図は本
発明装置の現像領域を拡大して現像剤の穂立ちの状態を
示した図、第7図は従来装置の現像領域を拡大して現像
剤の穂立ちの状態を示した図である。 l・・・・・・・・・静電潜像担持体(感光ドラム)2
・・・・・・・−・現像剤担持用回転体(現像スリーブ
)3・・・・・・・・・磁界発生体 1ト・・・・・・・・現像剤
FIG. 1(A) is a schematic cross-sectional view of a device according to an embodiment of the present invention;
Fig. 1 (8) is an enlarged view of the adjacent region of Fig. 1 (A) to show the perpendicular magnetic field component density distribution in this region, and Fig. 2 is a diagram showing the density distribution of the perpendicular magnetic field component in the adjacent region of Fig. 1 (A). 3 is a diagram showing the relationship between the rate of change in the horizontal magnetic field component density and the state of occurrence of image disturbance, and FIG. A diagram showing the density distribution of the vertical magnetic field component and the horizontal magnetic field component of the developing pole of an embodiment of the invention and the developing pole of a conventional device. FIG. Figure 6 is a diagram showing the rate of change, and Figure 6 is an enlarged view of the development area of the device of the present invention to show the state of developer spikes. Figure 7 is an enlargement of the development area of the conventional device, showing the state of developer spikes. It is a diagram showing a standing state. l...... Electrostatic latent image carrier (photosensitive drum) 2
・・・・・・・・・・Developer carrying rotating body (developing sleeve) 3・・・・・・・・・Magnetic field generator 1t・・・・・・・・・Developer

Claims (4)

【特許請求の範囲】[Claims] (1)静電潜像担持体と、内部に磁界発生体を有する現
像剤担持体としての回転体を、両者の外周面間に最近接
部をもつ近接領域を形成するように配設し、 上記磁界発生体は、上記回転体の上記最近接部に、回転
体表面に垂直な磁界成分の最大密度点を生ぜしめる位置
に磁極を配され、 上記回転体表面に磁性現像剤を担持し、上記近接領域内
で上記垂直磁界成分により、上記磁性現像剤を穂立ち状
態に形成せしめて現像を行なう現像装置において、 上記磁極が形成する水平磁界成分は、上記回転体の周方
向距離に対する密度の変化率の絶対値が極大値をとる位
置及びその近傍で、現像領域の両端部を形成している、 ことを特徴とする現像装置。
(1) An electrostatic latent image carrier and a rotating body as a developer carrier having a magnetic field generating member inside are arranged so as to form a proximate region having the closest portion between the outer circumferential surfaces of both, The magnetic field generating body has a magnetic pole disposed at the closest portion of the rotating body at a position that produces a maximum density point of a magnetic field component perpendicular to the surface of the rotating body, and supports a magnetic developer on the surface of the rotating body, In a developing device that performs development by forming the magnetic developer into a spiked state using the perpendicular magnetic field component in the adjacent region, the horizontal magnetic field component formed by the magnetic pole has a density of A developing device characterized in that a position where the absolute value of the rate of change takes a maximum value and its vicinity form both ends of a developing area.
(2)現像領域の両端部における、水平磁界成分の回転
体の中心角に対する密度変化率は、30ガウス毎度以上
であることとする請求項(1)に記載の現像装置。
(2) The developing device according to claim 1, wherein the density change rate of the horizontal magnetic field component with respect to the center angle of the rotating body at both ends of the developing area is 30 Gauss per degree or more.
(3)現像領域は、静電潜像担持体と回転体の表面対向
距離が2000ミクロンメートル以下であることとする
請求項(1)または(2)に記載の現像装置。
(3) The developing device according to claim 1 or 2, wherein in the developing region, the distance between the surfaces of the electrostatic latent image carrier and the rotating body is 2000 micrometers or less.
(4)静電潜像担持体と回転体とを隔絶する隔絶手段が
、上記静電潜像担持体と回転体とが形成する近接領域に
おける現像領域の端部近傍に配設されていることとする
請求項(1)ないし(3)のいずれかに記載の現像装置
(4) An isolation means for isolating the electrostatic latent image carrier and the rotating body is disposed near the end of the developing area in the close area formed by the electrostatic latent image carrier and the rotating body. The developing device according to any one of claims (1) to (3).
JP63174971A 1988-07-15 1988-07-15 Development device Expired - Lifetime JPH087500B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63174971A JPH087500B2 (en) 1988-07-15 1988-07-15 Development device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63174971A JPH087500B2 (en) 1988-07-15 1988-07-15 Development device

Publications (2)

Publication Number Publication Date
JPH0225873A true JPH0225873A (en) 1990-01-29
JPH087500B2 JPH087500B2 (en) 1996-01-29

Family

ID=15987941

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63174971A Expired - Lifetime JPH087500B2 (en) 1988-07-15 1988-07-15 Development device

Country Status (1)

Country Link
JP (1) JPH087500B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5320791A (en) * 1991-04-30 1994-06-14 Mitsui Mining Company, Limited Method for preparing molded articles of high-purity alumina fibers

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57168278A (en) * 1981-04-10 1982-10-16 Fuji Xerox Co Ltd Magnetic brush developing device
JPS5814169A (en) * 1981-07-18 1983-01-26 Konishiroku Photo Ind Co Ltd Magnet device for development
JPS60146274A (en) * 1984-01-10 1985-08-01 Canon Inc Developing device

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS57168278A (en) * 1981-04-10 1982-10-16 Fuji Xerox Co Ltd Magnetic brush developing device
JPS5814169A (en) * 1981-07-18 1983-01-26 Konishiroku Photo Ind Co Ltd Magnet device for development
JPS60146274A (en) * 1984-01-10 1985-08-01 Canon Inc Developing device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US5320791A (en) * 1991-04-30 1994-06-14 Mitsui Mining Company, Limited Method for preparing molded articles of high-purity alumina fibers

Also Published As

Publication number Publication date
JPH087500B2 (en) 1996-01-29

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