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JP2773151B2 - Developing device - Google Patents
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JP2773151B2 - Developing device - Google Patents

Developing device

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Publication number
JP2773151B2
JP2773151B2 JP63228590A JP22859088A JP2773151B2 JP 2773151 B2 JP2773151 B2 JP 2773151B2 JP 63228590 A JP63228590 A JP 63228590A JP 22859088 A JP22859088 A JP 22859088A JP 2773151 B2 JP2773151 B2 JP 2773151B2
Authority
JP
Japan
Prior art keywords
magnetic field
developer
developing
field component
density
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
JP63228590A
Other languages
Japanese (ja)
Other versions
JPH0277772A (en
Inventor
孝男 本田
克彰 小林
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 JP63228590A priority Critical patent/JP2773151B2/en
Publication of JPH0277772A publication Critical patent/JPH0277772A/en
Application granted granted Critical
Publication of JP2773151B2 publication Critical patent/JP2773151B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

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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。
Description: BACKGROUND OF THE INVENTION The present invention is used in the field of technology for developing an electrostatic latent image with a developer, and in particular, a developing device that performs development while restraining the developer with a magnetic force. About.

[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 outer peripheral surface facing each other so as to form an area close to the electrostatic latent image carrier. And a non-magnetic rotating body that carries a magnetic developer. In the proximity region, a predetermined region in which the distance between the outer peripheral surfaces of the two adjacent surfaces is equal to or less than a predetermined value, that is, a region having a constant magnetic field strength is defined as a development region.

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手段としての磁界発生体
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 as a magnetic field generating means having a plurality of magnets such that one magnetic pole faces the outer peripheral surface side of the rotating body is fixedly installed inside the rotating body. I have. One of the plurality of magnets constituting the magnetic field generator is disposed in the range of the proximity area between the electrostatic latent image body and the rotator and near the position corresponding to the closest part. The magnetization is set such that one magnetic pole on the outer peripheral surface side of the rotating body has a maximum density point of a vertical magnetic field component (a magnetic field component perpendicular to the surface of the rotating body) substantially at the center of the developing region. This vertical magnetic field component magnetically constrains the developer on the outer peripheral surface of the rotating body within the range of the development area to form a so-called “spike”, 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(上記回転体表
面に平行な磁界成分)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 both ends of the developing area, and conversely, the horizontal magnetic field component ( The density of the magnetic field component parallel to the surface of the rotator gradually increases. As a result, the spikes of the developer are inclined toward both ends of the development area, so that various obstacles occur in the image developed in that part. For example, it is referred to as “tailing”, and the developer linearly extends in the direction opposite to the direction of image formation accompanying the rotation of the rotator (the direction of transport of the recording material on which an image is formed) and trails. The image formation has an adverse effect on the image formation, such as a state in which the developer particles appear to be scattered, and a state in which the "tailing", which is called "scattering", is further deteriorated, and the particles of the developer scatter to 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6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6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6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って延びる上述の「尾引
き」である。
FIG. 6 is an enlarged view of the development area at this time, showing the appearance of the ears of the developer. In FIG. 1, a developer 10 is carried on a developing sleeve 2 as a developer carrying member. Further, an electrostatic latent image (represented as a negative polarity of reference numeral 11 in FIG. 6) is carried on the photosensitive drum 1 as an electrostatic latent image carrier. At the closest portion between the photosensitive drum 1 and the developing sleeve 2 (in the case of the drawing, the central portion of the developing area), the developer which has risen on the developing sleeve 2
10 moves to the photosensitive drum 1 side under the electric suction force.
However, in the direction from the central part of the developing area to the non-developing areas at both ends, the ears gradually become inclined under the influence of the horizontal magnetic field component. This trend is referenced
As shown by reference numeral 12, it is quite noticeable at both ends of the development area. For example, in the left part of the developing area shown in FIG. 6, a part of the rising of the developer 10 inclined on the developing sleeve 2 has a large distance between the photosensitive drum 1 and the developing sleeve 2. Despite the tendency, the developer is electrically attracted to the photosensitive drum 1 in the direction of the arrow W, so that the developer 10 shifts in the image forming direction A on the rotating photosensitive drum 1. This displacement of the developer 10 is the above-mentioned “tailing” that extends linearly rearward on the copy 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。
SUMMARY OF THE INVENTION An object of the present invention is to solve adverse effects on image formation, such as "tailing" and "scattering", of such a conventional developing device.

[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、該静電潜像担持体とで現像領域を
形成し非磁性円筒からなる現像剤担持体と、該現像剤担
持体内に設けられた磁界発生手段とを有する現像装置に
おいて、 上記磁界発生手段は現像領域内に単一の磁極を有し、
該磁極により形成される現像剤担持体上の磁界は、現像
領域の略中央で現像剤担持体の径方向の磁界成分が磁束
密度の最大を成し、現像剤担持体表面の接線方対値の極
大点が現像領域内に存在し、現像剤担持体表面の接線方
向の磁界成分の変化率の絶対値の極大値は30ガウス/度
以上である、 ことによって構成される。
[Means for Solving the Problems] To achieve the above object, a developing device of the present invention comprises a non-magnetic cylinder in which a developing area is formed by an electrostatic latent image carrier and the electrostatic latent image carrier. In a developing device having a developer carrier and a magnetic field generating means provided in the developer carrier, the magnetic field generating means has a single magnetic pole in a development area,
The magnetic field on the developer carrier formed by the magnetic poles is such that the magnetic field component in the radial direction of the developer carrier substantially at the center of the development area has the maximum magnetic flux density, and the tangential direction of the surface of the developer carrier is Is present in the developing region, and the maximum value of the absolute value of the absolute value of the rate of change of the magnetic field component in the tangential direction on the surface of the developer carrier is 30 gauss / degree or more.

[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静電潜像担持体と回
転体の近接領域に搬送される。一方、回転体に配設され
た磁極のうち少なくとも一つは、静電潜像担持体と回転
体の近接領域に現像可能領域を形成し、さらにその磁極
が形成する回転体表面に平行な磁界成分は、回転体の単
位回転角に対する密度変化率の絶対値の極大値が該現像
可能領域内に存在するように設定されている。したがっ
て、上記現像剤は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 started, the developer thinned on the surface of the rotating body is transported to a region near the electrostatic latent image carrier and the rotating body. On the other hand, at least one of the magnetic poles disposed on the rotating body forms a developable area in an area near the electrostatic latent image carrier and the rotating body, and a magnetic field parallel to the rotating body surface formed by the magnetic pole. The components are set such that the maximum value of the absolute value of the density change rate with respect to the unit rotation angle of the rotator exists in the developable region. Therefore, the developer rises due to the magnetic field of the magnetic pole, and forms a visible image according to the charge of the electrostatic latent image carried on 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] An embodiment of the present invention will be described below 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. 1A is a cross-sectional view showing the periphery of a developing sleeve as a developer carrier in a developing device as one embodiment of the present invention, and FIG. 1B is a developing sleeve of FIG. 1A. FIG. 3 is a diagram schematically illustrating a distribution state of a vertical magnetic field component in the proximity region formed by a photosensitive drum serving as an electrostatic latent image carrier formed by enlarging a 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, a developing sleeve 2 is rotatably arranged in a direction A 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, and d on its periphery is fixedly installed at a predetermined position. Each magnet is arranged so that one of the two magnetic poles forming a pair faces the peripheral surface of the developing sleeve 2, the magnet a serves as a developing pole, the magnet b serves as a developer regulating pole (cut pole), The 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。
In addition, a blade 4 for regulating the height of the rising edge of the developer 10 to make the developer on the developing sleeve thinner is disposed at a position facing the magnet b above the developing sleeve 2. I have. On the right side of the developing sleeve 2 is a container 8 in which the left portion of the developing sleeve 2 is disposed so as to protrude at the opening, and stores a developer 10 to be supplied to the developing sleeve 2. 2a is the center of rotation 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 region in FIG. 1 (A). In FIG. 1 (B), a developing pole (N pole in this embodiment) which is a magnetic pole on the peripheral surface side of the magnet a is shown. The vertical magnetic field component distribution is shown by the length of the arrow indicating the magnetic flux density at the peripheral 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
には該表面に垂直な垂直磁界成分と該表面に平行な水平
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、現像スリーブ2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 around the magnet a. Therefore, a vertical magnetic field component perpendicular to the surface and a horizontal magnetic field component parallel to the surface are formed on the surface of the developing sleeve 2, and the direction of the ears of the developer is the vertical magnetic field component shown in FIG. It is determined by a horizontal magnetic field component not shown. Here, the horizontal magnetic field component is a magnetic field component in a tangential direction on the circumference of the developing sleeve 2.

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 inclined spikes of the developer occurring at both ends of the developing area, which has been pointed out as a problem of the conventional apparatus described above. it can.

すなわち、現像可能領域内において、現像極である磁
石aの水平磁界成分の磁束密度の変化率が大きくなるよ
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 problem is solved by correcting and setting the change rate of the magnetic flux density of the horizontal magnetic field component of the magnet a as the developing pole in the developable region.

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、上記現像極として
の磁石aの磁化設定条件について説明する。第3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。
Hereinafter, 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 magnetization setting condition of the magnet a as the developing pole will be described. FIG. 3 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 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 the present 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 the 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θ0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。
The horizontal axis is at 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 at which the density becomes 0 Gauss is defined as a reference position θ 0, and the angle θ is shown downstream (developing pole side) with respect to the rotation center 2 a 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).

磁石aは、感光ドラム1と現像スリーブ2の最近接点
で現像スリーブ2表面に垂直な磁界成分の最大密度点
(第3図,S点)を形成し、最大密度点を中心として現像
スリーブ2の上流側及び下流側に約30°の角度をもって
現像領域を形成するように設定されている。磁石aはさ
らに、上記現像領域内に、水平磁界成分の磁束密度変化
量の最大値及び最小値が存在するように設定されてい
る。
The magnet a forms the maximum density point (point S, FIG. 3) of the magnetic field component perpendicular to the surface of the developing sleeve 2 at the closest contact point between the photosensitive drum 1 and the developing sleeve 2, and the developing sleeve 2 It is set so that the development area is formed at an angle of about 30 ° on the upstream side and the downstream side. The magnet a is further set so that the maximum value and the minimum value of the change amount of the magnetic flux density of the horizontal magnetic field component exist in the development area.

なお、第2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/度以上となるよう強化設
定することが好ましい。
In addition, as shown in FIG. 2, when the amount of change in the density of the horizontal magnetic field component per unit center angle with respect to the center of the rotating body is 30 Gauss or less, the occurrence of image defects such as “tailing” and “scattering” often occurs. It has been confirmed that, in general, it is preferable to strengthen and set the maximum value of the absolute value of the density change rate to be 30 gauss / degree or more.

ところで、現像可能領域とは、現像スリーブ2上の現
像剤が感光ドラム1上の潜像を現像し得る領域のことを
表わしているが、この現像領域は以下に示した関係にお
いて最良条件となることが明らかとなった。
By the way, the developable region indicates a region where the developer on the developing sleeve 2 can develop the latent image on the photosensitive drum 1, and this developing region is the best condition in the following relationship. It became clear.

θ=2cos -1{[(d−G)/r]+1}…(1) ここでθ(°)は現像可能領域の設定角度であり、d
(mm)は垂直磁界成分の最大密度点である感光ドラム1
と現像スリーブ2の表面対向距離の最近接距離を示して
いる。また、G(mm)は現像が可能となる感光ドラム1
と現像スリーブ2の表面対向距離である。このGは現像
剤の種類等の条件によって異なるが約2000μm以下であ
ることが好ましい。なお、(1)式の関係は、静電潜像
担持体あるいは現像剤担持体が本実施例のように円筒状
のものに限らず、例えばベルト状に形成されたものにお
いても適用が可能である。
θ = 2 cos −1 {[(d−G) / r] +1} (1) where θ (°) is a set angle of the developable area, and d
(Mm) is the photosensitive drum 1 which is the maximum density point of the vertical magnetic field component
And the closest distance between the surface facing distance of the developing sleeve 2 and the developing sleeve 2. G (mm) is a photosensitive drum 1 that can be developed.
And the surface facing distance of the developing sleeve 2. This G varies depending on conditions such as the type of developer, but is preferably about 2000 μm or less. Note that the relationship of the expression (1) is not limited to a cylindrical electrostatic latent image carrier or a developer carrier as in the present embodiment, but can be applied to, for example, a belt-shaped electrostatic latent image carrier or developer carrier. is there.

第3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3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4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。
In FIG. 3, the vertical magnetic field component density of the present embodiment is compared with that of the conventional device. In the case of the present embodiment (solid line), the center position (angle θ = around 50 degrees) is higher than that of the conventional device (two-dot chain line).
, The rate of change of density is relatively stable near the maximum density point S, and the rate of change increases at a position at a predetermined distance from the center position to both sides. Further, comparing the horizontal magnetic field component densities, the device of the present embodiment (broken line) has the above-mentioned center position as the minimum density point and the change rate of the density in the vicinity thereof is more stable than that of the conventional device (dashed line). It can be seen that the rate of change is greater at the position at the above-mentioned predetermined distance from the 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. 3 is differentiated by the angle θ, and the rate of change with respect to the angle θ is plotted on the vertical axis. FIG. Comparing the two, the change rate is large and the local maximum value (maximum value) and the local minimum value (minimum value) are clear at a position that is a predetermined distance from the center position to both sides. This is because, as described above, the developing pole of the present embodiment is set so that the absolute value of the density change rate of the horizontal magnetic field component is maximized at a position that is a predetermined distance from the center position of the developing 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5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. 5 shows the state of the developer spikes in which the development area of the apparatus having the development poles whose magnetization is set as described above is enlarged. Both ends N 1 and N 2 of the development area
Since the rate of change of the density of the vertical and horizontal magnetic field components is large, the presence or absence of ears at the end of the development area is clear. As a result, the developer that has risen vertically on the sleeve 2 is arranged neatly in the developing area. As a result, the developer 10 is suction-transferred to the photosensitive drum 1 without being disturbed, and does not cause image disturbance such as “tailing” and “scattering”.

なお、以上説明した本発明装置の磁界発生手段に配設
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て左右対称である
必要はなく、この最大密度点を中央として非対称であっ
てもよい。
The magnet provided in the magnetic field generating means of the device of the present invention described above can be widely applied, such as a ferrite sintered type and a resinous integral molding type. Also, the development pole magnetization need not be symmetrical with respect to the maximum density point of the vertical component as the center, but may be asymmetric with respect to the maximum density point.

[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、静電潜像担持体と回転体の近接領域に現像可能領域
が形成されるように設定した。現像極は、現像領域の略
中央で現像剤担持体の径方向の磁界成分が磁束密度の最
大を成し、現像剤担持体表面の接線方向の磁界成分の変
化率の絶対値の極大点が現像領域内に存在し、現像剤担
持体表の接線方向の磁界成分の変化率の絶対値の極大値
は30ガウス/度以上であることとしたので、現像可能領
域内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。
[Effects of the Invention] As described above, the developing pole of the developing device according to the present invention is set such that a developable area is formed in the area near the electrostatic latent image carrier and the rotating body. At the developing pole, the magnetic field component in the radial direction of the developer carrier forms the maximum of the magnetic flux density at substantially the center of the developing region, and the maximum point of the absolute value of the change rate of the magnetic field component in the tangential direction on the surface of the developer carrier is Since the maximum value of the absolute value of the change rate of the magnetic field component in the tangential direction on the surface of the developer carrier is 30 gauss / degree or more in the development area, the density of the horizontal magnetic field component in the developable area Sharply changes, and the presence or absence of the ears of the developer can be clarified. Therefore, the situation in which development is performed by the inclined developer is eliminated, and image defects such as “tailing” and “splashing” which the conventional device has can be prevented, and the effect of always providing high-quality images can be obtained. Bring. The magnetic field generator can be manufactured by integral molding of a fixed magnet and a resin, and can be significantly reduced in cost and weight as compared with ferrite sintered type magnets, bonded type magnets, and embedded type magnets.

【図面の簡単な説明】[Brief description of the 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3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4図は第3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5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6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……磁界発生手段 10……現像剤 a……現像磁極を形成する磁石
FIG. 1A is a schematic cross-sectional view of an apparatus according to an embodiment of the present invention,
FIG. 1 (B) is an enlarged view of a vertical magnetic field component density distribution in an adjacent area of FIG. 1 (A), and FIG. 2 is a view showing a change rate of a horizontal magnetic field component density and an image failure occurrence state. FIG. 3 is a diagram showing the density distribution of the vertical magnetic field component and the horizontal magnetic field component of the developing pole of the apparatus according to one embodiment of the present invention and the developing pole of the conventional apparatus, and FIG. 4 is FIG. FIG. 5 is a diagram showing the rate of change of the horizontal magnetic field component with respect to the center angle of the rotating body, FIG. 5 is a diagram showing the developing region of the apparatus of the present invention in an enlarged state, and FIG. FIG. 5 is a view showing a state of ears of the developer by enlarging a development region of FIG. DESCRIPTION OF SYMBOLS 1 ... Electrostatic latent image carrier (photosensitive drum) 2 ... Rotator for carrying developer (developing sleeve) 3 ... Magnetic field generating means 10 ... Developer a ... Magnet forming a developing magnetic pole

Claims (1)

(57)【特許請求の範囲】(57) [Claims] 【請求項1】静電潜像担持体と、該静電潜像担持体とで
現像領域を形成し非磁性円筒からなる現像剤担持体と、
該現像剤担持体内に設けられた磁界発生手段とを有する
現像装置において、 上記磁界発生手段は現像領域内に単一の磁極を有し、該
磁極により形成される現像剤担持体上の磁界は、現像領
域の略中央で現像剤担持体の径方向の磁界成分が磁束密
度の最大を成し、現像剤担持体表面の接線方向の磁界成
分の変化率の絶対値の極大点が現像領域内に存在し、現
像剤担持体表面の接線方向の磁界成分の変化率の絶対値
の極大値は30ガウス/度以上であることを特徴とする現
像装置。
An electrostatic latent image carrier, a developer carrier formed of a non-magnetic cylinder and forming a development area with the electrostatic latent image carrier;
A magnetic field generating means provided in the developer carrier, wherein the magnetic field generating means has a single magnetic pole in a developing area, and a magnetic field formed by the magnetic pole on the developer carrier is The magnetic field component in the radial direction of the developer carrying member has a maximum magnetic flux density at substantially the center of the developing region, and the maximum point of the absolute value of the change rate of the magnetic field component in the tangential direction on the surface of the developer carrying member is within the developing region. Wherein the maximum value of the absolute value of the change rate of the magnetic field component in the tangential direction on the surface of the developer carrying member is 30 gauss / degree or more.
JP63228590A 1988-09-14 1988-09-14 Developing device Expired - Lifetime JP2773151B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP63228590A JP2773151B2 (en) 1988-09-14 1988-09-14 Developing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP63228590A JP2773151B2 (en) 1988-09-14 1988-09-14 Developing device

Publications (2)

Publication Number Publication Date
JPH0277772A JPH0277772A (en) 1990-03-16
JP2773151B2 true JP2773151B2 (en) 1998-07-09

Family

ID=16878746

Family Applications (1)

Application Number Title Priority Date Filing Date
JP63228590A Expired - Lifetime JP2773151B2 (en) 1988-09-14 1988-09-14 Developing device

Country Status (1)

Country Link
JP (1) JP2773151B2 (en)

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6671484B2 (en) 2000-09-05 2003-12-30 Ricoh Company, Ltd. Image forming apparatus having developing device with magnet roller with particular magnetic flux density

Families Citing this family (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP5793940B2 (en) * 2011-04-27 2015-10-14 コニカミノルタ株式会社 Developing device and image forming apparatus
JP2017203841A (en) 2016-05-10 2017-11-16 キヤノン株式会社 Developing device and image forming apparatus

Family Cites Families (2)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS61151578A (en) * 1984-12-26 1986-07-10 Casio Comput Co Ltd Developing device
JPH07107618B2 (en) * 1986-05-15 1995-11-15 ミノルタ株式会社 Development device

Cited By (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
US6671484B2 (en) 2000-09-05 2003-12-30 Ricoh Company, Ltd. Image forming apparatus having developing device with magnet roller with particular magnetic flux density

Also Published As

Publication number Publication date
JPH0277772A (en) 1990-03-16

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