JPS6260713B2 - - Google Patents

Info

Publication number
JPS6260713B2
JPS6260713B2 JP53029569A JP2956978A JPS6260713B2 JP S6260713 B2 JPS6260713 B2 JP S6260713B2 JP 53029569 A JP53029569 A JP 53029569A JP 2956978 A JP2956978 A JP 2956978A JP S6260713 B2 JPS6260713 B2 JP S6260713B2
Authority
JP
Japan
Prior art keywords
magnetic
magnetic pole
magnet
sleeve element
attraction force
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
Application number
JP53029569A
Other languages
Japanese (ja)
Other versions
JPS54122131A (en
Inventor
Manabu Mochizuki
Masahide Harada
Mitsuo Tanaka
Hiroharu Suzuki
Kazuaki Tagawa
Kazuo Kobayashi
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.)
Ricoh Co Ltd
Original Assignee
Ricoh Co Ltd
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 Ricoh Co Ltd filed Critical Ricoh Co Ltd
Priority to JP2956978A priority Critical patent/JPS54122131A/en
Priority to CA000319418A priority patent/CA1135046A/en
Priority to EP19790100081 priority patent/EP0003134B1/en
Priority to EP80107642A priority patent/EP0031503B1/en
Priority to DE8080107642T priority patent/DE2967496D1/en
Priority to DE7979100081T priority patent/DE2960948D1/en
Publication of JPS54122131A publication Critical patent/JPS54122131A/en
Publication of JPS6260713B2 publication Critical patent/JPS6260713B2/ja
Granted legal-status Critical Current

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  • Magnetic Brush Developing In Electrophotography (AREA)

Description

【発明の詳細な説明】 本発明は電子複写機等に用いる磁気ブラシ式の
乾式現像装置に係る。
DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a magnetic brush type dry developing device used in electronic copying machines and the like.

乾式現像装置の一つとして知られている磁気ブ
ラシ式現像装置は、非磁性のスリーブ要素と、前
記スリーブ要素内に配置され前記スリーブ要素の
外周表面に所定の磁極の磁場を与える磁石とを含
んでおり、かかる現像装置においては、磁性粉末
を含む現像剤が前記磁石の磁気作用により前記ス
リーブ要素の外周表面にブラシ状の穂になつて保
持され、それが前記スリーブ要素の回転に伴い感
光体(静電潜像担持体)の表面に向けて順次搬送
されて直接前記感光体の光導電層に接触すること
により現像作用が営まれる。かかる型の現像プロ
セスに於ける現像力は、下式により示される。
A magnetic brush type developing device, which is known as a type of dry developing device, includes a non-magnetic sleeve element and a magnet that is disposed within the sleeve element and applies a magnetic field of a predetermined magnetic pole to the outer peripheral surface of the sleeve element. In such a developing device, a developer containing magnetic powder is held in the form of brush-like ears on the outer peripheral surface of the sleeve element by the magnetic action of the magnet, and as the sleeve element rotates, the developer is applied to the photoreceptor. A developing action is carried out by being sequentially conveyed toward the surface of the electrostatic latent image carrier and directly contacting the photoconductive layer of the photoreceptor. The developing power in this type of developing process is expressed by the following equation.

F=FC−FM ただし、Fは現像力、FCは感光体の静電作用
による現像剤の電気的吸引力、FMは磁気ブラシ
式現像装置の磁気作用による現像剤の磁気的吸引
力である。
F = F C - F M , where F is the developing force, F C is the electric attraction force of the developer due to the electrostatic action of the photoreceptor, and F M is the magnetic attraction of the developer due to the magnetic action of the magnetic brush developing device. It is power.

上式から磁気ブラシ式現像装置による磁気的吸
引力FMは現像力Fに対して負のバイアス的役割
を持つていることが理解されよう。そこで、前記
磁気的吸引力FMをパラメーターとして現像特性
を表わすと、第1図に示すようになる。第1図の
グラフは縦軸にトナー付着量Mを、横軸に感光体
上の表面電荷Qを示している。実線は前記磁気的
吸引力FMが比較的小さい時の現像特性を、また
破線は前記磁気的吸引力FMが比較的大きい時の
現像特性を各々示している。なお、磁気的吸引力
Mが比較的大きい時も小さい時も現像時間は互
いに同一とした。第1図に示すグラフからも明ら
かな如く、磁気的吸引力FMを小さくすると、ト
ナー付着量Mが電荷量Qの比較的少ない所から飽
和し、従つて現像むらが発生しにくくなる。ま
た、磁気的吸引力FMが小さいと、同一現像時間
に於けるトナー付着量Mが前記磁気的吸引力FM
を大きくした時に比べて多く、従つて同一トナー
付着量Mの場合、磁気的吸引力FMが大きい時に
比べて現像時間の短縮が可能である。しかし、前
記磁気的吸引力FMを小さくすると、地肌汚れが
多くなり、また画像のシヤープ性が劣り、画像品
質的にはあまり良い結果を生じない。
From the above equation, it will be understood that the magnetic attraction force F M by the magnetic brush type developing device has a negative biasing role with respect to the developing force F. Therefore, when the development characteristics are expressed using the magnetic attraction force F M as a parameter, it becomes as shown in FIG. In the graph of FIG. 1, the vertical axis shows the toner adhesion amount M, and the horizontal axis shows the surface charge Q on the photoreceptor. The solid line shows the development characteristics when the magnetic attraction force F M is relatively small, and the broken line shows the development characteristics when the magnetic attraction force F M is relatively large. Incidentally, the development time was set to be the same when the magnetic attraction force F M was relatively large and small. As is clear from the graph shown in FIG. 1, when the magnetic attraction force F M is reduced, the toner adhesion amount M becomes saturated from a point where the charge amount Q is relatively small, and uneven development becomes less likely to occur. Furthermore, if the magnetic attraction force F M is small, the toner adhesion amount M at the same development time will be reduced by the magnetic attraction force F M
Therefore, for the same toner adhesion amount M, the developing time can be shortened compared to when the magnetic attraction force F M is large. However, when the magnetic attraction force F M is reduced, background stains increase, the sharpness of the image is poor, and the image quality is not very good.

これに対して従来、磁気ブラシ式の現像装置を
感光体の移動方向に沿つて二つ隔置して設け、こ
のうち感光体の移動方向の上流側に位置する現像
装置の磁気的吸引力を比較的小さく設定し、また
感光体の移動方向の下流側にある現像装置の磁気
的吸引力を比較的大きく設定し、感光体の移動方
向の上流側に位置する現像装置によつて現像剤を
均一に感光体に付着させ、感光体の移動方向の下
流側にある現像装置によつて地汚れ等をなくすべ
く画像を整像させるように構成されたものが知ら
れている。かかる現像装置は一応所期の目的を達
成するが、しかし、構造が複雑になり、重量、ス
ペースの面で問題を生じ、また高コストなものに
なる。
In contrast, conventionally, two magnetic brush type developing devices are provided spaced apart along the direction of movement of the photoreceptor, and the magnetic attraction force of the developing device located upstream in the direction of movement of the photoreceptor is The magnetic attraction force of the developing device located downstream in the direction of movement of the photoreceptor is set relatively small, and the magnetic attraction force of the developing device located upstream in the direction of movement of the photoreceptor is set to be relatively large. There is known a structure in which the toner is uniformly adhered to the photoreceptor and the image is adjusted to eliminate background smudges and the like by a developing device located downstream in the direction of movement of the photoreceptor. Although such a developing device achieves its intended purpose, it has a complicated structure, poses problems in terms of weight and space, and is also expensive.

本発明は構造を簡単にして上述した如きダブル
スリーブ形の現像装置と同等の効果を得ることが
できる、新しい型の磁気ブラシ式現像装置を提供
せんとするものである。
The present invention aims to provide a new type of magnetic brush type developing device which has a simple structure and can obtain the same effects as the above-mentioned double sleeve type developing device.

ところで、本願出願人と同一の出願人は特開昭
54−95243号に於いて、磁石の磁極部形状を工夫
することにより一つの磁石が現像作用位置のスリ
ーブ表面上に於いて複数のピークを持つた磁気的
吸引力分布を発生することを見出し、そのことを
有効に利用した磁気ブラシ式現像装置を提案され
ている。
By the way, the same applicant as the applicant of the present application is
In No. 54-95243, it was discovered that by devising the shape of the magnetic pole part of the magnet, one magnet could generate a magnetic attraction force distribution with multiple peaks on the sleeve surface at the development action position, A magnetic brush type developing device that effectively utilizes this fact has been proposed.

本発明は磁石の磁極部形状を工夫することによ
り一つの磁石が現像作用位置に於いて複数のピー
クを持つた磁気的吸引力分布を発生することをさ
らに有効に利用して前述の目的を達成せんとする
ものである。
The present invention achieves the above-mentioned object by making more effective use of the fact that one magnet generates a magnetic attraction force distribution having multiple peaks at the development action position by devising the shape of the magnetic pole part of the magnet. This is what I am trying to do.

かかる目的は、本発明によれば回転する非磁性
のスリーブ要素と、前記現像作用位置に対向して
前記スリーブ要素内に固定配置され前記スリーブ
要素の外周表面に磁場を生じる磁石とを有する磁
気ブラシ現像装置に於いて、前記磁石は前記スリ
ーブ外周表面上の現像作用位置にて複数個のピー
クを持つた磁気的吸引力分布を発生し得る磁極面
形状をもつ一つの磁極部を有し且つ前記磁気的吸
引力分布のピークのうち静電潜像担持体の移動方
向の下流側のものが上流側のものより強くなるよ
う構成されている如き磁気ブラシ現像装置によつ
て達成される。
According to the invention, such an object is achieved by providing a magnetic brush having a rotating non-magnetic sleeve element and a magnet fixedly disposed within the sleeve element opposite to the developing position and generating a magnetic field on the outer circumferential surface of the sleeve element. In the developing device, the magnet has one magnetic pole portion having a magnetic pole surface shape capable of generating a magnetic attractive force distribution having a plurality of peaks at a developing action position on the outer circumferential surface of the sleeve; This is achieved by a magnetic brush developing device configured such that among the peaks of the magnetic attractive force distribution, those on the downstream side in the moving direction of the electrostatic latent image carrier are stronger than those on the upstream side.

以下に添付の図を用いて本発明を実施例につい
て詳細に説明する。
DESCRIPTION OF THE PREFERRED EMBODIMENTS The present invention will be described in detail below with reference to the accompanying drawings.

第2図は本発明による乾式現像装置の一つの実
施例を示す概略構成図である。第2図に示されて
いる乾式現像装置は、それ自身の中心軸線を回転
中心として第2図でみて反時計方向に回転駆動さ
れる非磁性のスリーブ要素1を含んでおり、この
スリーブ要素1の内部に磁石2を有している。前
記スリーブ要素1はその一部にてドラム状の静電
潜像担持体、いわゆる感光体ドラム3の周面に所
定の間隔を置いて対向しており、また前記磁石2
はその対向領域、すなわち現像作用位置にて前記
スリーブ要素1を隔てて前記感光体ドラム3の周
面に対向する一つの磁極部を、例えばN磁極を有
しており、前記現像作用位置にて前記スリーブ要
素1の外周表面に磁場を生じている。この磁石
は、上記位置に固定して配置されている。なお、
図示していないが現像剤搬送用の磁石がスリーブ
要素1内に内蔵されている。前記磁極部は、第3
図に拡大して示されている如く、その磁極部磁極
面の感光体ドラム移動方向の下流側に偏倚した位
置に凹溝4を有し、その凹溝4より感光体ドラム
移動方向の上流側に幅広の第一の磁極部5を、前
記感光体ドラム移動方向下流側に幅狭の第二の磁
極部6を構成している。
FIG. 2 is a schematic diagram showing one embodiment of the dry developing device according to the present invention. The dry developing device shown in FIG. 2 includes a non-magnetic sleeve element 1 which is rotationally driven in a counterclockwise direction as viewed in FIG. 2 about its own central axis. It has a magnet 2 inside. A portion of the sleeve element 1 faces the peripheral surface of a drum-shaped electrostatic latent image carrier, so-called photosensitive drum 3, with a predetermined distance therebetween, and the magnet 2
has one magnetic pole portion, for example, an N magnetic pole, which faces the circumferential surface of the photoreceptor drum 3 across the sleeve element 1 at its opposing region, that is, at the development action position, and at the development action position. A magnetic field is generated on the outer peripheral surface of the sleeve element 1. This magnet is fixedly arranged at the above position. In addition,
Although not shown, a magnet for transporting the developer is built into the sleeve element 1. The magnetic pole part is a third
As shown in the enlarged view, the magnetic pole part has a concave groove 4 at a position offset to the downstream side in the photoconductor drum movement direction on the magnetic pole surface, and the concave groove 4 is on the upstream side in the photoconductor drum movement direction. A wide first magnetic pole portion 5 is formed on the downstream side in the direction of movement of the photoreceptor drum, and a narrow second magnetic pole portion 6 is formed on the downstream side in the direction of movement of the photosensitive drum.

各磁極部5,6は、単一磁石の一方の磁極部の
磁極面に凹溝4を切削加工することにより形成さ
れてもよく、あるいは個別の着磁された磁石片を
磁極面上に間隔を置いて接着等により一体化して
形成されたものであつてもよい。そして第5図と
第7図にも示すように、スリーブ要素1に対向し
ている磁石の一端の磁極部磁極面は凹凸に形成さ
れているので、一見複数の磁極が存在するように
見えるが、各磁極部は、同一極性(図示の場合N
極)であるから、実質的に一つの磁極部からなつ
ている。ということができる。
Each magnetic pole part 5, 6 may be formed by cutting a groove 4 into the magnetic pole face of one of the magnetic pole parts of a single magnet, or by cutting individual magnetized magnet pieces at intervals on the magnetic pole face. It may also be formed by placing two parts and integrating them by adhesion or the like. As shown in FIGS. 5 and 7, the magnetic pole surface of the magnetic pole part at one end of the magnet facing the sleeve element 1 is formed in an uneven manner, so at first glance it appears that there are multiple magnetic poles. , each magnetic pole part has the same polarity (N in the case shown)
Since it is a magnetic pole (pole), it essentially consists of one magnetic pole part. It can be said that.

さて、このように、一方の磁極部の磁極面に凹
凸部を有する磁石では、両端の磁極間(N―S極
間)の距離が凹部と凸部とで異なり、このため、
磁石の内部に発生する反磁場(demagneti zing
field)の強さが、凹部と凸部とでは異なる強さ
となる。
Now, in this way, in a magnet that has an uneven part on the magnetic pole surface of one magnetic pole part, the distance between the magnetic poles at both ends (between N and S poles) is different between the concave part and the convex part, and therefore,
The demagnetizing field generated inside the magnet
field) is different between concave portions and convex portions.

今少し詳しく説明すると、磁石内部に発生する
反磁場は、磁石の寸法や形状によつて変化し、一
般的には磁石の磁極面の大きさに対して磁極間
(N―S極間)の距離が長いほど小さくなる。こ
のため、一様に磁化された磁石であつても、磁極
部の磁極面に凹凸部を形成し、部分的に磁極間距
離を変えることによつて、凹部と凸部に作用する
反磁場の強さを変えることができる。
To explain in more detail, the demagnetizing field generated inside a magnet changes depending on the size and shape of the magnet, and generally speaking, the demagnetizing field generated inside a magnet changes depending on the size and shape of the magnet. The longer the distance, the smaller it becomes. Therefore, even if the magnet is uniformly magnetized, by forming uneven parts on the magnetic pole face of the magnetic pole part and partially changing the distance between the magnetic poles, the demagnetizing field acting on the concave and convex parts can be reduced. You can change the strength.

すなわち、磁石の磁極面に凹部を形成すると、
凹部部分には強い反磁場が作用し、このため凹部
部分が磁石外に発生する磁場の強さは磁極の他の
部分が発生する磁場の強さより弱くなる。逆に、
磁極面に凸部を形成した場合には、凸部部分の磁
場の強ささが他の部分より強くなる。
In other words, when a recess is formed on the magnetic pole face of the magnet,
A strong demagnetizing field acts on the recessed portion, so that the strength of the magnetic field generated outside the magnet by the recessed portion is weaker than that generated by other portions of the magnetic pole. vice versa,
When a convex portion is formed on the magnetic pole surface, the strength of the magnetic field at the convex portion is stronger than at other portions.

従つて、第3図に示す如く、磁石2の磁極部
(図ではN極)磁極面に凹溝4が一つ設けられた
場合には、その凹溝4を有する磁極部に於いて二
つのピークを有する磁気的吸引力分布の磁場が得
られ、前記スリーブ要素1の外周表面に於いて第
4図に示す如き磁気的吸引力分布の磁場が発生す
る。
Therefore, as shown in FIG. 3, when one concave groove 4 is provided on the magnetic pole face of the magnet 2 (the N pole in the figure), two grooves are formed in the magnetic pole part having the concave groove 4. A magnetic field with a magnetic attraction force distribution having a peak is obtained, and a magnetic field with a magnetic attraction force distribution as shown in FIG. 4 is generated on the outer peripheral surface of the sleeve element 1.

次に、複数のピークを有する磁気的吸引力分布
生成の詳細を第9図に基づいて説明する。磁石に
最も近い位置においては同図aに示すように、鋭
角部な4つのヒピークが形成されているのである
が、磁石から離れるに連れて同図bに示すように
そのピークは鈍化しその数も3つになる。そし
て、磁石から更に離れた位置(スリーブ外周表面
の位置)においては、同図cに示すように、ピー
クは更に鈍化してその数も2になつてしまう。第
9図cに示すピークの数と形状が第4図に示すも
のである。すなわち、第一の磁極部5と第二の磁
極部6とを比較すると、凹溝4がスリーブ1の移
動方向において下流側に偏倚して形成されている
ため、両磁極部に作用する反磁場の強さが異な
り、第二の磁極部6の方の磁界が強くなる。その
ために、第二の磁極部6から発生する磁束密度は
第一の磁極部5のそれよりも高くなつているの
で、第一の磁極部5の磁気的吸引力よりも第二の
磁極部6の磁気的吸引力の方が強くなつている。
Next, details of generating a magnetic attraction force distribution having a plurality of peaks will be explained based on FIG. 9. At the position closest to the magnet, four acute-angled hip peaks are formed, as shown in Figure a, but as you move away from the magnet, the peaks become blunter and their number decreases, as shown in Figure b. There will also be three. Then, at a position further away from the magnet (the position of the outer circumferential surface of the sleeve), the peak becomes even more blunt, and the number of peaks decreases to 2, as shown in Figure c. The number and shape of the peaks shown in FIG. 9c are those shown in FIG. That is, when comparing the first magnetic pole part 5 and the second magnetic pole part 6, since the groove 4 is formed to be biased toward the downstream side in the moving direction of the sleeve 1, the demagnetizing field acting on both magnetic pole parts is The strength of the magnetic field is different, and the magnetic field of the second magnetic pole part 6 is stronger. Therefore, the magnetic flux density generated from the second magnetic pole part 6 is higher than that of the first magnetic pole part 5, so the magnetic attraction force of the second magnetic pole part 6 is higher than that of the first magnetic pole part 5. The magnetic attraction of is becoming stronger.

従つて、現像に際しては、感光体ドラム3の移
動方向の上流側にある第一の磁極部5による比較
的弱い磁気的吸引力によつて感光体ドラム3の静
電潜像に対して良好な均一な現像剤の付着が行な
われ、その後、感光体ドラムの移動方向の下流側
にある第二の磁極部6による比較的強い磁気的吸
引力によつて前記感光体ドラム3上の画像の整像
が行なわれる。これにより濃度のむらがなく、地
汚れもない品質の良い画像が得られるようにな
る。
Therefore, during development, the electrostatic latent image on the photoreceptor drum 3 is effectively attracted by the relatively weak magnetic attraction force of the first magnetic pole portion 5 located on the upstream side in the moving direction of the photoreceptor drum 3. The developer is uniformly attached, and then the image on the photoreceptor drum 3 is aligned by a relatively strong magnetic attraction force by the second magnetic pole part 6 located downstream in the direction of movement of the photoreceptor drum. The statue is performed. This makes it possible to obtain high-quality images without uneven density and background smudges.

第5図は本発明による乾式現像装置の他の一つ
の実施例の要部を拡大して示す縦断面図である。
かかる実施例の場合、磁石2の磁極部は、スリー
ブ要素1の外周表面に対して所定の第一の間隔を
有する第一の磁極部7と、前記スリーブ要素1の
外周表面に対して前記第一の間隔より小さい第二
の間隔を有する第二の磁極部8とを有し、段付き
端部になつている。この場合、前記第一の磁極部
7は前記第二の磁極部8より感光体ドラム3の移
動方向遅れ側に設けられている。
FIG. 5 is a longitudinal sectional view showing an enlarged main part of another embodiment of the dry developing device according to the present invention.
In the case of such an embodiment, the magnetic pole portions of the magnet 2 include a first magnetic pole portion 7 having a predetermined first spacing with respect to the outer circumferential surface of the sleeve element 1 and a first magnetic pole portion 7 having a predetermined first spacing with respect to the outer circumferential surface of the sleeve element 1. and a second magnetic pole portion 8 having a second spacing smaller than the first spacing, resulting in a stepped end. In this case, the first magnetic pole part 7 is provided on the lag side of the second magnetic pole part 8 in the moving direction of the photosensitive drum 3.

かかる実施例に於いては、前記スリーブ要素1
の外周表面には第6図に示す如き磁気的吸引力分
布の磁場が生じ、上述した実施例と同様の作用が
得られる。なお、第6図に示す磁気的吸引力の分
布は、スリーブ1の外周表面のものであつて、磁
石に近い部分における分布は第9図で説明したも
のから容易に理解されよう。
In such an embodiment, the sleeve element 1
A magnetic field having a magnetic attractive force distribution as shown in FIG. 6 is generated on the outer circumferential surface of the magnet, and the same effect as in the embodiment described above is obtained. The distribution of the magnetic attraction force shown in FIG. 6 is that of the outer circumferential surface of the sleeve 1, and the distribution in the portion near the magnet will be easily understood from what was explained in FIG. 9.

第7図は本発明による現像装置のさらに他の一
つの実施例を示す要部の縦断面図である。かかる
実施例の場合、磁石2の磁極部は、二の凹溝9,
10を互いに隔置して有しており、その各凹溝に
よつて区切られた第一、第二、第三の磁極部1
1,12,13を有している。前記三つの磁極部
のうち感光体ドラムの移動方向の上流側の二つは
スリーブ要素1の外周表面に対して互いに等しい
間隔を有しているが、最も感光体ドラムの移動方
向の下流側にある第三の磁極部13は他のものよ
り前記スリーブ要素1の外周表面により接近して
いる。かかる実施例の場合は、第8図に示す如く
三つのピークを有する磁気的吸引力分布の磁場が
得られ、またそのピークのうち最も感光体ドラム
3の移動方向の下流側にあるものが強い磁気的吸
引力を有している。なお、第8図に示す磁気的吸
引力の分布は、スリーブ1の外周表面のものであ
つて、磁石に近い部分における分布は第9図で説
明したものから容易に理解されよう。かかる実施
例の場合は、第一及び第二の磁極部11,12に
よる比較的弱い磁気的吸引力の条件によつて感光
体ドラム3の静電潜像に対して良好で均一な現像
剤の付着が行なわれ、第三の磁極部13による比
較的強い磁気的吸引力の条件で前記感光体ドラム
3上の画像の整像が行なわれる。なお、本発明に
使用される磁性現像剤としては、非磁性トナーを
磁性キヤリヤとから成る二成分現像剤又は磁性ト
ナーのみから成る一成分現像剤がある。
FIG. 7 is a longitudinal cross-sectional view of the essential parts of yet another embodiment of the developing device according to the present invention. In the case of such an embodiment, the magnetic pole part of the magnet 2 has two grooves 9,
10 spaced apart from each other, first, second, and third magnetic pole parts 1 separated by respective grooves.
1, 12, and 13. Of the three magnetic pole parts, the two on the upstream side in the direction of movement of the photoreceptor drum have equal spacing from each other with respect to the outer circumferential surface of the sleeve element 1, but the two on the upstream side in the direction of movement of the photoreceptor drum are the most downstream in the direction of movement of the photoreceptor drum. Some third pole sections 13 are closer to the outer circumferential surface of said sleeve element 1 than others. In the case of such an embodiment, as shown in FIG. 8, a magnetic field with a magnetic attractive force distribution having three peaks is obtained, and among the peaks, the one located on the downstream side in the direction of movement of the photoreceptor drum 3 is the strongest. It has magnetic attraction. The distribution of the magnetic attraction force shown in FIG. 8 is that of the outer circumferential surface of the sleeve 1, and the distribution in the portion near the magnet will be easily understood from what was explained in FIG. 9. In the case of this embodiment, a good and uniform developer is applied to the electrostatic latent image on the photoreceptor drum 3 under the condition of relatively weak magnetic attraction force by the first and second magnetic pole parts 11 and 12. The adhesion is performed, and the image on the photoreceptor drum 3 is imaged under the condition of a relatively strong magnetic attraction force by the third magnetic pole portion 13. The magnetic developer used in the present invention may be a two-component developer consisting of a non-magnetic toner and a magnetic carrier, or a one-component developer consisting only of magnetic toner.

以上の如く本発明によれば、実質的に一つの磁
石によつて現像作用位置に比較的弱い磁気的吸引
力の条件と比較的強い磁気的吸引力の条件が与え
られるので、構造を複雑にすることなく、濃度む
らがなく且つ地汚れもない品質のよい複写画像が
得られる。
As described above, according to the present invention, a relatively weak magnetic attraction condition and a relatively strong magnetic attraction condition are provided to the developing position by substantially one magnet, so that the structure is not complicated. A high-quality copy image with no density unevenness and background smudge can be obtained.

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

第1図は現像装置の磁気的吸引力をパラメータ
ーとして現像特性を示したグラフ、第2図は本発
明による磁気ブラシ現像装置の一実施例示す概略
縦断面図、第3図はそれの要部を拡大して示す縦
断面図、第4図は第2図に示した磁石を用いた場
合のスリーブ要素の外周表面に於ける磁気的吸引
力分布を示すグラフ、第5図は本発明による現像
装置の他の一つの実施例の要部を示す縦断面図、
第6図は第5図に示した磁石を用いた場合のスリ
ーブ要素の外周表面に於ける磁気的吸引力分布を
示すグラフ、第7図は本発明による現像装置のさ
らに他の一つの実施例の要部を示す縦断面図、第
8図は第7図に示した磁石を用いた場合のスリー
ブ要素の外周表面に於ける磁気的吸引力分布を示
すグラフ、第9図は磁石から離れるに連れて変動
する磁気的吸引力のの変化を説明するための説明
図である。 1……スリーブ要素、2……磁石、3……感光
体ドラム、4……凹溝、5……第一の磁極部、6
……第二の磁極部、7……第一の磁極部、8……
第二の磁極部、9,10……凹溝、11……第一
の磁極部、12……第二の磁極部、13……第三
の磁極部。
Fig. 1 is a graph showing the development characteristics using the magnetic attraction force of the developing device as a parameter, Fig. 2 is a schematic vertical sectional view showing an embodiment of the magnetic brush developing device according to the present invention, and Fig. 3 is the main part thereof. FIG. 4 is a graph showing the magnetic attraction force distribution on the outer peripheral surface of the sleeve element when the magnet shown in FIG. 2 is used. FIG. A vertical cross-sectional view showing the main parts of another embodiment of the device,
FIG. 6 is a graph showing the magnetic attraction force distribution on the outer peripheral surface of the sleeve element when the magnet shown in FIG. 5 is used, and FIG. 7 is a graph showing still another embodiment of the developing device according to the present invention. FIG. 8 is a graph showing the magnetic attraction force distribution on the outer peripheral surface of the sleeve element when the magnet shown in FIG. 7 is used, and FIG. FIG. 3 is an explanatory diagram for explaining a change in magnetic attraction force that changes with the change in magnetic attraction force. DESCRIPTION OF SYMBOLS 1... Sleeve element, 2... Magnet, 3... Photosensitive drum, 4... Concave groove, 5... First magnetic pole part, 6
...Second magnetic pole part, 7...First magnetic pole part, 8...
Second magnetic pole part, 9, 10... Concave groove, 11... First magnetic pole part, 12... Second magnetic pole part, 13... Third magnetic pole part.

Claims (1)

【特許請求の範囲】 1 静電潜像担持体の現像作用位置に近接して配
置されていて、回転する非磁性のスリーブ要素
と、前記現像作用位置に対向して前記スリーブ要
素内に固定配置され前記スリーブ要素の外周表面
に磁場を生じる磁石とを有する磁気ブラシ現像装
置に於いて、 前記磁石は前記スリーブ外周表面上の現像作用
位置にて複数個のピークを持つた磁気的吸引力分
布を発生する磁極面形状を持つた磁極部を有し且
つ前記磁気的吸引力分布のピークのうち静電潜像
担持体の移動方向の下流側のものが上流側のもの
より強くなるように構成されていることを特徴と
する磁気ブラシ現像装置。
[Scope of Claims] 1. A rotating non-magnetic sleeve element that is disposed close to a developing position of the electrostatic latent image carrier, and a rotating non-magnetic sleeve element that is fixedly disposed within the sleeve element opposite to the developing position. and a magnet that generates a magnetic field on the outer circumferential surface of the sleeve element, wherein the magnet generates a magnetic attraction force distribution having a plurality of peaks at a developing action position on the outer circumferential surface of the sleeve. It has a magnetic pole part having a magnetic pole surface shape, and is configured such that among the peaks of the magnetic attractive force distribution, the peaks on the downstream side in the moving direction of the electrostatic latent image carrier are stronger than the peaks on the upstream side. A magnetic brush developing device characterized by:
JP2956978A 1978-01-11 1978-03-15 Magnetic brush developing device Granted JPS54122131A (en)

Priority Applications (6)

Application Number Priority Date Filing Date Title
JP2956978A JPS54122131A (en) 1978-03-15 1978-03-15 Magnetic brush developing device
CA000319418A CA1135046A (en) 1978-01-11 1979-01-10 Magnetic brush development apparatus
EP19790100081 EP0003134B1 (en) 1978-01-11 1979-01-11 Magnetic brush development apparatus
EP80107642A EP0031503B1 (en) 1978-01-11 1979-01-11 Magnetic brush development apparatus
DE8080107642T DE2967496D1 (en) 1978-01-11 1979-01-11 Magnetic brush development apparatus
DE7979100081T DE2960948D1 (en) 1978-01-11 1979-01-11 Magnetic brush development apparatus

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP2956978A JPS54122131A (en) 1978-03-15 1978-03-15 Magnetic brush developing device

Publications (2)

Publication Number Publication Date
JPS54122131A JPS54122131A (en) 1979-09-21
JPS6260713B2 true JPS6260713B2 (en) 1987-12-17

Family

ID=12279746

Family Applications (1)

Application Number Title Priority Date Filing Date
JP2956978A Granted JPS54122131A (en) 1978-01-11 1978-03-15 Magnetic brush developing device

Country Status (1)

Country Link
JP (1) JPS54122131A (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2540348Y2 (en) * 1993-08-06 1997-07-02 有馬 孝榮 Learning clock

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5146133A (en) * 1974-10-18 1976-04-20 Ricoh Kk Jikigenzosochi
JPS5152843A (en) * 1974-11-05 1976-05-10 Hitachi Metals Ltd
JPS5263344A (en) * 1975-11-19 1977-05-25 Ricoh Co Ltd Toner density control by magnetic brush

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5146133A (en) * 1974-10-18 1976-04-20 Ricoh Kk Jikigenzosochi
JPS5152843A (en) * 1974-11-05 1976-05-10 Hitachi Metals Ltd
JPS5263344A (en) * 1975-11-19 1977-05-25 Ricoh Co Ltd Toner density control by magnetic brush

Also Published As

Publication number Publication date
JPS54122131A (en) 1979-09-21

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