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JPH087500B2 - Development device - Google Patents
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JPH087500B2 - Development device - Google Patents

Development device

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Publication number
JPH087500B2
JPH087500B2 JP63174971A JP17497188A JPH087500B2 JP H087500 B2 JPH087500 B2 JP H087500B2 JP 63174971 A JP63174971 A JP 63174971A JP 17497188 A JP17497188 A JP 17497188A JP H087500 B2 JPH087500 B2 JP H087500B2
Authority
JP
Japan
Prior art keywords
developing
magnetic field
developer
field component
area
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
JP63174971A
Other languages
Japanese (ja)
Other versions
JPH0225873A (en
Inventor
孝男 本田
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

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  • Magnetic Brush Developing In Electrophotography (AREA)

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と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
の行なう現像装置に関する。
DETAILED DESCRIPTION OF THE INVENTION [Industrial field of application] The present invention is used in the field of technology for developing with an electrostatic latent image and a developer, and in particular, a developing device for carrying out development by restraining the developer with a 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、その静
電潜像担持体と近接領域力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, in this type of developing device, an electrostatic latent image carrier and an outer peripheral surface thereof are disposed so as to face each other so as to form a proximity area force with the electrostatic latent image carrier. And a non-magnetic rotating body carrying a developer having magnetism. In the proximity area, a predetermined area in which the distance between the outer peripheral surfaces facing each other is equal to or less than a certain value, that is, an area having a certain magnetic field strength is defined as a developing 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、回転体の内部に一磁極が回転体外周面側に向く
よう磁石を複数有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 carrying the developer on the surface of the rotating body, a magnetic field generator having a plurality of magnets is fixedly installed inside the rotating body so that one magnetic pole faces the outer peripheral surface side of the rotating body. One of the plurality of magnets forming the magnetic field generator is disposed in the vicinity of the position closest to the closest portion within the range of the proximity area between the electrostatic latent image body and the rotating body. , One magnetic pole on the outer peripheral surface side of the rotating body is a vertical magnetic field component in a substantially central portion of the developing area (magnetic field component perpendicular to the surface of the rotating body)
The magnetization is set so as to have a maximum density point of. This vertical magnetic field component magnetically restrains the developer on the outer peripheral surface of the rotating body within the range of the developing region to form a so-called "brush", and transfers the developer 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っては、現像領域
の両端側へと向うようにしたがい磁石の上記垂直磁界成
分の密度が徐々に減少し、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。その結果
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
称される上記「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 the both ends of the developing region, and conversely the horizontal magnetic field component. The density of (the magnetic field component in the circumferential direction of the rotating body) gradually increases. As a result, the spikes of the developer are inclined toward the both ends of the developing area, which causes various troubles in the image developed in that portion. For example, it is called “tailing”, and the developer linearly extends in a direction opposite to the image forming direction (conveying direction of the recording material on which the image is formed) along with the rotation of the rotating body, and the tail is drawn. The image formation is adversely affected by such a state as if it appears to be present or the above-mentioned "tailing" called "scattering" is further deteriorated and the developer particles are scattered to the peripheral portion 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上に現像剤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1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
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
10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。例えば、第7図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の穂立ちの一部が、感光ドラム1と現像スリ
ーブ2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。この現像相10のずれが
複写画像上では後方に線状となって延びる上述の「尾引
き」である。
FIG. 7 shows a state in which the developing region at this time is enlarged and the spikes of the developer are raised. In the figure, the developer 10 is carried on the developing sleeve 2 as the developer carrying member. An electrostatic latent image (represented by a negative polarity of reference numeral 11 in FIG. 7) is carried on the photosensitive drum 1 as the electrostatic latent image carrier. Then, at the closest portion between the photosensitive drum 1 and the developing sleeve 2 (in the central portion of the developing area in the figure), the developer that stands on the developing sleeve 2
10 receives the electric attraction force and moves to the photosensitive drum 1 side.
However, as it goes from the central portion of the developing area to the non-developing areas on both ends, the spikes gradually incline due to the influence of the horizontal magnetic field component. This trend has a reference
As shown by 12, it appears considerably at both ends of the development area. For example, in the left side portion of the developing area shown in FIG. 7, a part of the spikes of the developer 10 inclined on the developing sleeve 2 tends to increase the distance between the photosensitive drum 1 and the developing sleeve 2. However, since the toner is electrically attracted to the photosensitive drum 1 in the arrow W direction, the developer 10 is displaced in the image forming direction A on the rotating photosensitive drum 1. This deviation of the development phase 10 is the above-mentioned "tailing" that extends linearly rearward 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」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。
An object of the present invention is to solve the adverse effects in image formation such as "tailing" and "scattering" which the conventional developing device has.

[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、内部に
磁界発生体を有し、磁性現像剤を担持して移動する現像
剤担持体を移動方向に所定幅の現像領域をなすように静
電潜像担持体に対向させ、磁界発生体は現像領域内に現
像剤担持体表面に垂直な垂直磁界成分の最大磁束密度点
を形成する現像磁極を有する現像装置において、 上記現像磁極が形成する現像剤担持体表面の接線方向
の水平磁界成分の磁束密度分布は現像領域の端部位置も
しくはその近傍で極大値をとる、 ことによって構成される。
[Means for Solving the Problems] In order to achieve the above-mentioned object, the developing device of the present invention has a magnetic field generator inside and a developer carrier for carrying a magnetic developer and moving the developer carrier in a predetermined direction. A development having a developing magnetic pole facing the electrostatic latent image carrier so as to form a developing area of width, and the magnetic field generator forming a maximum magnetic flux density point of a vertical magnetic field component perpendicular to the surface of the developer carrier in the developing area. In the apparatus, the magnetic flux density distribution of the horizontal magnetic field component in the tangential direction on the surface of the developer carrier formed by the developing magnetic pole has a maximum value at or near the end position of the developing area.

[作用] 上記のように構成された現像装置が起動すると、回転
体の表面上に薄層化された現像剤が現像領域に搬送され
る。該現像剤は、上記現像領域に配設され回転体の周方
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電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 thinned on the surface of the rotating body is conveyed to the developing area. The developer is disposed in the developing region so that both ends of the developing region are formed at and near the position where the absolute value of the change rate of the density of the horizontal magnetic field component with respect to the circumferential distance of the rotating body has a maximum value. It stands by the magnetic field of the set magnetic pole,
A visible image is formed according to the charge of the electrostatic latent image carried by the electrostatic latent image carrier.

[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。
[Embodiment] Hereinafter, an embodiment of the present invention will be described with reference to 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 cross-sectional view showing the periphery of a developing sleeve as a developer carrying member in the developing device as one embodiment, and FIG. 1 (B) is the developing sleeve of FIG. 1 (A). FIG. 3 is a diagram schematically showing an enlarged proximity region formed by a photosensitive drum as an electrostatic latent image carrier, and showing a distribution state of a vertical magnetic field component in the proximity region.

第1図(A)において、現像スリーブ2は、感光ドラ
ム1に所定間隙をもって対向する位置にA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bが現像剤規制
極(カット極)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. 1A, the developing sleeve 2 is disposed rotatably in the A direction at a position facing the photosensitive drum 1 with a predetermined gap. Inside the developing sleeve 2, a magnetic field generator 3 having four magnets a, b, c, d in its peripheral portion is fixedly installed at a predetermined position. Each of the magnets is arranged such that one of the two magnetic poles forming the pair faces the peripheral surface of the developing sleeve 2. The magnet a is the developing pole, the magnet b is the developer regulating pole (cutting pole), The magnets c and d form the developer carrying 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上の現像剤を薄層化するた
めのブレード4が上記磁石b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 for regulating the height of spikes of the developer 10 and thinning the developer on the developing sleeve 2 is provided above the developing sleeve 2 at a position facing the magnet b. There is. The right side of the developing sleeve 2 is a container 8 in which the upper portion of the developing sleeve 2 is arranged in a projecting state at the opening and the developer 10 to be supplied to the developing sleeve 2 is accommodated. 2a is the rotation center of the developing sleeve 2 and the fixed center 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) is an enlarged view of the proximity area in FIG. 1 (A). In FIG. 1 (B), the developing pole (N pole in this embodiment) which is the magnetic pole on the peripheral surface side of the magnet a is shown. The distribution of the vertical magnetic field component is indicated by the magnetic flux density at the peripheral surface position of the developing sleeve 2 by the length of the arrow.

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って決まる。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 the magnet a is formed in all directions centering on the magnet a. 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 spike of the developer is determined by the vertical magnetic field component shown in the drawing and the horizontal magnetic field component not shown. . here,
The horizontal magnetic field component is a magnetic field component in the direction of the tangent line on 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 the developing pole, it is possible to prevent the development caused by the sloping spikes of the developer, which has been pointed out as a problem of the above-described conventional apparatus, which occurs at both ends of the developing area. it 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が解消される。
That is, the above-mentioned problems can be solved by correcting and setting the change rate of the magnetic flux density of the horizontal magnetic field component of the developing pole at both ends of the developing area so as 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、本実施例装置にあ
っ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
置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, in this embodiment, how the density distribution of the horizontal magnetic field component is formed in the developing region in order to solve the problem will be described in detail. Therefore, first, the maximum range that can be set as the developing area in the above-mentioned proximity area in the apparatus of the present embodiment will be clarified. Prior to this, the developing sleeve 2 as the rotating body of the apparatus of the present embodiment has a substantially cylindrical shape. Therefore, the developing area formed on the peripheral surface of the developing sleeve 2 is
The description will be made in correspondence with the central angle of the developing sleeve 2 with respect to the rotation center 2a.

第2図は第1図(B)と同様に現像スリーブ2と感光
ドラム1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Lとし、現像スリーブ2の上の点をXとす
る。この基準線Lと現像スリーブ2の外周面及び感光ド
ラム1の外表面との交点をそれぞれX0,Y0とする。距離
X0Y0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、X0は現像領域の中央に位置することとなる。
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。
Similar to FIG. 1B, FIG. 2 shows a proximity area between the developing sleeve 2 and the photosensitive drum 1. Here, a line connecting the rotation center 2a of the developing sleeve 2 and the rotation center 1a of the photosensitive drum 1 is a reference line L, and a point on the developing sleeve 2 is X. The intersections of the reference line L and the outer peripheral surface of the developing sleeve 2 and the outer surface of the photosensitive drum 1 are defined as X 0 and Y 0 , respectively. distance
X 0 Y 0 is the shortest distance where the developing sleeve 2 and the photosensitive drum 1 face each other, and X 0 is located at the center of the developing area.
In the vicinity of the position X 0 in the circumferential direction, the density of the vertical magnetic field component of the above-described developing pole is almost maximum and the horizontal magnetic field component is almost 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2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と感光ドラム1との最長距離をlmax
とする。
In the apparatus of the present embodiment having the closest portion as described above in the approximate center of the proximity area, the development as the limit that allows the electrostatic latent image on the photosensitive drum 1 to be developed by the developer on the developing sleeve 2. The maximum distance between the sleeve 2 and the photosensitive drum 1 is lmax
And

このlmaxと等しい長さで、線分X0Y0と平行な、現像ス
リーブ2と感光体1の表面を結ぶ線分をX1Y1とする。こ
の線分X1Y1は、第2図に示されるごとくX0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1の対向距離の最長である。すなわち、こ
の2本の線分X1Y1、X1Y1に挟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、lmax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lmax≦2000μm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。
A line segment connecting the developing sleeve 2 and the surface of the photoconductor 1 and having a length equal to this lmax and parallel to the line segment X 0 Y 0 is defined as X 1 Y 1 . This line segment X 1 Y 1 exists at two positions sandwiching X 0 as shown in FIG. 2, and the developing sleeve 2 facing each other within the developable range.
Is the longest facing distance of the photosensitive drum 1. That is, it can be said that the circumferential range sandwiched between these two line segments X 1 Y 1 and X 1 Y 1 can be set as the development region. Here, since the value of lmax varies 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, but the test results of the present inventor According to the above, usually, lmax ≦ 2000 μm, and on the assumption that it is often preferable to set as the developing region.

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Lとのなす角度をαとす
る。また、このときの位置X1の基準線からの角度をαma
xとする。
Next, the density distribution of the horizontal magnetic field component of the developing pole in the developing area will be described. The angle between the reference line L and the line segment connecting the arbitrary position X in the circumferential direction on the developing sleeve 2 in FIG. 2 and the rotation center 2a of the developing sleeve 2 is α. In addition, the angle of position X 1 from the reference line at this time is αma
Let x.

ここで、現像領域は、角度αによって表わすならば|
αmax|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
/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。
If the development area is represented by the angle α, then |
It is within the range of αmax | In the developing area represented by this angle α, the absolute rate of change in density (gauss / degree) of the horizontal magnetic field component per unit central angle with respect to 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 development poles are magnetized so that both ends of the development area are formed at the maximum value.

すなわち、現像領域として設定し得る最大範囲の両端
の位置X1,X1により挟まれる中央位置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、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量が30ガウス以下では大きく
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。
That is, within the range that encloses the central position X 0 sandwiched by the positions X 1 and X 1 at both ends of the maximum range that can be set as the developing region, the positions that are a predetermined distance from the central position to both sides are the both ends of the developing region. Therefore, the developing pole is magnetized. As shown in Fig. 3, if the density variation of the horizontal magnetic field component per unit central angle with respect to the center of the rotating body is large below 30 Gauss, image defects such as "tailing" and "scattering" are confirmed. Therefore, it is generally preferable to set the magnetization so that the maximum value of the 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 described in detail with reference to the drawings. FIG. 4 shows the density distributions 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、また二点鎖線及び一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。
The solid and broken lines in the figure show the density distributions 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 two-dot chain line and the one-dot chain line show the vertical magnetic field component of the developing pole of the conventional apparatus. And a 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b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0ガウスとなる位置を基準位置θoとし、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を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で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(一点鎖線)よりも上
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
置で変化率が大き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。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。
The horizontal axis is an intermediate position between the magnet a shown in FIG. 1 (A) and the magnet b located on the upstream side in the rotation direction A of the developing sleeve 2, and represents the vertical magnetic field component of the developing pole of the magnet a. The position where the density is 0 gauss is defined as a reference position θ o, and the angle θ is shown downstream (development pole side) 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 on the surface of the developing sleeve 2 by G (Gauss). In the figure, comparing the vertical magnetic field component densities of this embodiment and the conventional device, in the case of this embodiment (solid line), the central position (angle θ = near 50 degrees) is better than that of the conventional device (two-dot chain line). The rate of change of the density is relatively stable in the vicinity of the maximum density point S as the apex, and the rate of change becomes large at the position where the distance is a predetermined distance from the central position. Further, comparing the horizontal magnetic field component densities, the device of the present embodiment (dashed line) has a stable density change rate in the vicinity of the minimum density point at the central position as compared with the conventional device (dashed line). It can be seen that the rate of change increases at the position where the above-mentioned predetermined distance is from the position to both sides. In order to clarify the above relationship, the density of the horizontal magnetic field component (G (Gauss)) on the vertical axis in FIG. 4 is differentiated by the angle θ, and the rate of change with respect to the angle θ is plotted on the vertical axis. It is FIG.
Comparing the two, the rate of change is large and the maximum value (maximum value) and the minimum value (minimum value) are clear at the positions that are a predetermined distance from the center position to both sides. As described above, this is because the developing pole of the apparatus of this embodiment has an absolute value of the density change rate of the horizontal magnetic field component at a position at a predetermined distance from the center position of the developing region (that is, at both ends of the developing region). Is set to be maximum.

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N1,N2
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がはっきりとしてい
る。その結果、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1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。
FIG. 6 shows the state of the spikes of the developer in which the developing area of the apparatus of this embodiment having the developing pole with the magnetization set as described above is enlarged. Both ends of development area N 1 , N 2
Since the rate of change in the density of the vertical and horizontal magnetic field components is large, the presence or absence of spikes at the edge of the developing area is clear. As a result, the developer that stands vertically on the sleeve 2 is arranged in an orderly manner in the developing area. As a result, the developer 10 is suction-transferred to the photosensitive drum 1 without being disturbed, and image defects such as "tailing" and "scattering" 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1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
両端部の傾斜した現像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X1X1の範囲内に
先端が位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
としてもよいし、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lmax=2000μmの場合基部での厚さが5〜15
00μm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図では隔絶板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。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 device of the present invention, the developing sleeve 2
An apparatus in which a separating plate is provided between the photosensitive drum 1 and the photosensitive drum 1 will be described. However, since the device of this embodiment shares much of it with the device of the first embodiment described above, the isolation plate 14 that is a feature of this embodiment is shown in FIG. 2 by a chain double-dashed line in FIG. The description is omitted. In the apparatus of this embodiment, the separating plate 14 is provided so that the inclined developer at both ends of the developing area does not participate in the development.
Was set up. The separating plate 14 is arranged in the longitudinal direction of the sleeve 2 between the developing sleeve 2 and the photoconductor 1 so that the tip thereof is located at least within the range of X 1 X 1 . The material is non-magnetic, magnetic, depending on the properties of the developer used and the surrounding materials.
Insulation, conductivity, etc. can be selected. As for the shape, the tip may have a pointed shape as shown in FIG. 2 or a rectangular shape. When the tip of the isolation plate 14 is installed near the edge of the developing area as shown in FIG. 2, for example, when lmax = 2000 μm, the thickness at the base is 5-15.
00 μm polyethylene terephthalate or stainless steel plate can be used. In FIG. 2, the isolation plate 14 is provided only on the downstream end of the developing area in the rotational direction A of the developing sleeve 2, but it may be provided only on the upstream side, or on the upstream and downstream sides. Is. According to the apparatus of this embodiment as described above, it is possible to more reliably prevent the development due to the spike of the developer having a large inclination at the end portion 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
形タイプ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。
As the magnet arranged in the magnetic field generator of the device of the present invention described above, a ferrite sintered type, a resin integrally molded type, etc. can be widely applied. Also, the setting of the developing pole magnetization does not need to be symmetric with respect to the maximum density point of the vertical component as the center, and may be asymmetric.

[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
とができる。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、フェライト焼結タイプ磁石、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。
[Advantages of the Invention] As described above, since the developing pole of the developing device according to the present invention is magnetized so that the absolute value of the density change rate of the horizontal magnetic field component has a maximum value at both ends of the developing region, The density of the horizontal magnetic field component changes abruptly at both ends of the developing area, so that the presence or absence of spikes of the developer can be made clear. Therefore, the situation in which the development is performed by the inclined developer is eliminated, and the image troubles such as “tailing” and “scattering” which the conventional apparatus has can be prevented, and the effect of always providing a high quality image can be obtained. Bring The magnetic field generator can be manufactured by integral molding of a fixed magnet and resin, a ferrite sintered type magnet, a laminated type,
Compared with embedded magnets, the price and weight can be reduced significantly.

【図面の簡単な説明】[Brief description of drawings]

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(B)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し、さらに第
二実施例を二点鎖線により示した図、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図の水平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。 1……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 10……現像剤 a……現像磁極を形成する磁石
FIG. 1 (A) is a schematic sectional view of an apparatus according to an embodiment of the present invention,
FIG. 1 (B) is an enlarged view of the adjacent region of FIG. 1 (A) showing the vertical magnetic field component density distribution in that region, and FIG. 2 is a diagram of the developer carrier and the electrostatic latent image carrier. FIG. 3 is a diagram showing a proximity region and further showing the second embodiment by a chain double-dashed line, FIG. 3 is a diagram showing the relationship between the rate of change of the horizontal magnetic field component density and the image failure occurrence state, and FIG. The figure which shows the density distribution of the vertical magnetic field component and the horizontal magnetic field component of the developing pole of the Example apparatus and the developing pole of the conventional apparatus, FIG. 5 shows the rate of change with respect to the central angle of a rotating body about the horizontal magnetic field component of FIG. FIG. 6 is a diagram showing the developing area of the device of the present invention by enlarging the developing area, and FIG. 7 is the developing area of the conventional apparatus by enlarging the developing area of the developer. It is the figure shown. 1 ... Electrostatic latent image carrier (photosensitive drum) 2 ... Rotating member for carrying developer (developing sleeve) 3 ... Magnetic field generator 10 ... Developer a ... Magnet for forming developing magnetic pole

Claims (4)

【特許請求の範囲】[Claims] 【請求項1】内部に磁界発生体を有し、磁性現像剤を担
持して移動する現像剤担持体を移動方向に所定幅の現像
領域をなすように静電潜像担持体に対向させ、磁界発生
体は現像領域内に現像剤担持体表面に垂直な垂直磁界成
分の最大磁束密度点を形成する現像磁極を有する現像装
置において、 上記現像磁極が形成する現像剤担持体表面の接線方向の
水平磁界成分の磁束密度分布は現像領域の端部位置もし
くはその近傍で極大値をとることを特徴とする現像装
置。
1. A magnetic field generator is provided inside, and a developer carrying member carrying and moving a magnetic developer is opposed to the electrostatic latent image carrying member so as to form a developing region of a predetermined width in the moving direction, The magnetic field generator has a developing magnetic pole which forms a maximum magnetic flux density point of a vertical magnetic field component perpendicular to the surface of the developer carrier in the developing area, and in the tangential direction of the surface of the developer carrier formed by the developing magnetic pole. The developing device characterized in that the magnetic flux density distribution of the horizontal magnetic field component has a maximum value at or near the end position of the developing area.
【請求項2】現像領域の両端部における、水平磁界成分
の現像剤担持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 central angle of the developer carrying member at both ends of the developing area is 30 gauss per degree or more.
【請求項3】現像領域は、静電潜像担持体と現像剤担持
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)または請求項(2)に記載の現像
装置。
3. The developing device according to claim 1, wherein in the developing area, the surface facing distance between the electrostatic latent image carrier and the developer carrier is 2000 μm or less. .
【請求項4】静電潜像担持体と現像剤担持体とを隔絶す
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)ないし請求項(3)のいずれか一つに記載の現
像装置。
4. A separating means for separating the electrostatic latent image bearing member and the developer bearing member is disposed near the end of the developing area formed by the electrostatic latent image bearing member and the rotating member. 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 JPH0225873A (en) 1990-01-29
JPH087500B2 true 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)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2959683B2 (en) * 1991-04-30 1999-10-06 三井鉱山株式会社 Method for producing high-purity alumina fiber molded body

Family Cites Families (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

Also Published As

Publication number Publication date
JPH0225873A (en) 1990-01-29

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