JP2742924B2 - Magnet roller - Google Patents

Magnet roller

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Publication number
JP2742924B2
JP2742924B2 JP8277338A JP27733896A JP2742924B2 JP 2742924 B2 JP2742924 B2 JP 2742924B2 JP 8277338 A JP8277338 A JP 8277338A JP 27733896 A JP27733896 A JP 27733896A JP 2742924 B2 JP2742924 B2 JP 2742924B2
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JP
Japan
Prior art keywords
magnetic field
magnet
developing
magnetic pole
magnet roller
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
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JP8277338A
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Japanese (ja)
Other versions
JPH09179410A (en
Inventor
泰 掛橋
嘉男 坂田
文仁 毛利
孚史 阪内
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Kaneka Corp
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Kaneka Corp
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Publication date
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Description

【発明の詳細な説明】 【0001】 【発明の属する技術分野】本発明は普通紙複写機の現像
用マグネツトローラーに関し、更に詳しくは、良好な画
像を与えるとともに、現像装置よりのトナーやキヤリヤ
ーの落下・飛散防止に有効なマグネツトローラーに関す
るものである。 【0002】 【従来の技術】普通紙複写機の現像にはトナー、キヤリ
ヤーの搬送用にマグネツトローラーが多用されている。
かかる磁気式現像方式特有の欠点の1つに、マグネツト
ローラーの周辺に生起される磁界による磁性体トナー、
キヤリヤーの捕捉力が不足して現像装置周辺にこれらが
落下・飛散して複写機の汚れを招くという問題があるば
かりでなく、感光体上に付着したトナーやキヤリヤーが
画像の階調性を低下させたり、白抜けや黒点等画質を悪
くするという問題がある。 【0003】従来、かかる、トナー、キヤリヤーの落下
・飛散防止の方法としては、マグネツトローラーのスリ
ーブ表面に於ける現像磁極での放射方向磁界成分HRに
着目し、HRを極力大とすることによりトナー、キヤリ
ヤーの捕捉力を高める方法が一般に採用されている。こ
のためには磁気特性の高い磁石(例えば異方性焼結フエ
ライト磁石)を高寸法精度に仕上げ加工して用いる等の
手段がとられる。しかしながら、この方法では原価が高
くなるという憾みがある。 【0004】実開昭51−8745号公報の第3図には
円筒状磁石を用い現像磁極21の巾を充分にし、且つこ
れと分離して近接した位置に狭い巾の搬送用磁極22、
23を設けることにより、従来の断面矩形型磁石を用い
た場合の問題、即ち垂直方向の磁束密度A’が大きく現
像極の搬送に寄与する接線方向の磁束密度B’が小さく
なり搬送能力が小さいという問題を解決したことが開示
されている。同図には垂直方向の磁束密度A’と接線方
向の磁束密度B’が図示されているが、該磁束密度A’
の分布は2山(ピーク)であり、現像剤の所謂「穂立
ち」に乱れが生じ、コピー時のテーリング(尾引き)や
紙へのキヤリヤー付着、トナー付着が生じ易く良好な画
質が得られにくいという問題がある。また磁石材料につ
いては明示されてはいないが、出願時期からみて焼結磁
石であると判断されるが、焼結磁石は成形性、配向着磁
方向の自由度、断面形状の自由度に制約があり、従っ
て、マグネツトローラーの設計も自ら制約されることに
なる。 【0005】 【発明が解決しようとする課題】本発明は上記の如き従
来技術の欠点を解消し、中程度の磁気特性を有する安価
な磁石を用いても捕捉力が強くなり、その結果、トナ
ー、キヤリヤーの落下・飛散が効果的に防止されるとと
もに、解像力が高められ、階調性や細線性が向上したマ
グネツトローラーを提供するものである。 【0006】 【課題を解決するための手段】即ち、本発明は支持軸周
に複数個のボンド磁石を接合配列したマグネツト群と上
記マグネツト群の外周をカバーする非磁性スリーブとか
らなる普通紙複写機用マグネツトローラーに於いて、現
像磁極の近傍に、該現像磁極のスリーブ上での放射方向
磁界成分が単一ピークを有し、且つ該ピーク値よりも大
きい、該放射方向磁界成分と接線方向磁界成分との合成
磁界ベクトルが存在し、且つその範囲がトナー、キヤリ
ヤーすり切り計量用刃の位置よりも現像磁極中心側であ
って該現像磁極中心から45゜以内であることを特徴と
するマグネツトローラーを内容とする。 【0007】 【発明の実施の形態】現像用マグネツトローラーの磁界
強度の評価は、その測定の容易さから、スリーブ表面に
於ける放射方向磁界成分HRのみを測ることによって行
なわれるのが一般的である。しかし、磁界はベクトル量
であるから、接線方向磁界成分HTも必然的に存在して
おり、当然、それも現像機構に寄与するものと考えられ
る。そこで、本発明者らは放射方向磁界成分と接線方向
磁界成分とを合成した「合成磁界HA」に着目して研究
した結果、トナー、キヤリアーの捕捉力は、通常測定さ
れるところの放射方向磁界成分値とよりも、合成磁界の
絶対値とより強く関連づけられることを見い出した。 【0008】さらに、本発明者らはマグネツトローラー
のスリーブ表面に於けるHRの磁界分布に加えて、HA
の磁界分布を種々変えて検討したところ、 現像磁極の近傍に単一ピークからなるHRを有し、且
つ該ピーク値PGよりも大なるHAの絶対値を有する磁
界ベクトルが存在すること、 HA≧PGとなる範囲がトナー、キヤリヤーすり切り
計量用刃の位置よりも現像磁極中心側であって該現像磁
極中心から45゜以内にあること、の2条件が満足され
た場合、HRのピーク値が相対的に小さなマグネツトロ
ーラーであってもトナー、キヤリヤーの捕捉力が高く、
これらの落下・飛散が事実上生じず、且つ良好な複写品
質が得られることを見出した。 【0009】ここでいう磁極中心とは、1つの磁性のH
Rの分布パターンに於いて、PG値の半値高さでこのパ
ターンを切る左右の2点の振分け中心をいう。上記の如
きトナー、キヤリヤーの落下防止に有効なマグネツトロ
ーラーのスリーブ表面磁界分布の例を図2に示した。何
故かかる表面磁界分布が有効であるかは明確ではない
が、HA≧PGとなる領域が現像磁極の左右にそれぞれ
あらわれ、且つ、HAの分布は2つのピークを有する双
頭型分布となり、この2つのピーク間に存在するトナ
ー、キヤリヤーが安定に捕捉されている故と考えられ
る。尚、本発明において、HRは単一ピークであること
が必要である。HRが複数個のピークとなるとHA分布
も複数個(2を越える値)のピークを持つものになり、
現像剤の所謂「穂立ち」に乱れが生じ、テーリングやキ
ヤリヤー付着が生じ易く、良好な画質が得られない。 【0010】HA≧PGとなる領域は該現像磁極の磁極
中心から45゜以内にあるのが好ましく、30℃以内な
らばより好ましく、15゜以内ならば更に好ましい。か
かる領域が余りに広すぎると種々の不都合が生じる。即
ち、該領域に保持されるトナー、キヤリヤー量が過大と
なってその重量効果にてトナー、キヤリヤーの落下が激
しくなる、磁界ベクトルHAのピークにおける磁界ベク
トル方向が外に開きすぎ、トナー、キヤリヤーの捕捉作
用が低下する等である。従って、HA≧PGとなる領域
は前記角度範囲内にあるのが良いが、過度に狭い角度範
囲となってしまうとトナー、キヤリヤーを捕捉する領域
が小さくなり効果が不十分となるから、HRのピーク値
の水準により変動するため一概には規定はできないもの
の、概ね5゜以上の範囲にわたることが良い。更に、磁
界ベクトルHAのピークにおけるベクトル方向が開きす
ぎると不都合であることは前記したが、この開きを放射
方向に対してベクトルHAがなす角度と規定して、一定
の角度以内に抑制することも有効である。 【0011】更に、現像磁極へのトナー、キヤリヤーの
供給量を調節する目的で、現像磁極の手前、例えば現像
磁極中心より概ね45〜50゜の近傍にトナー、キヤリ
ヤーすり切り計量用の刃を設けることが一般的である。
この刃の位置における磁界HAが強すぎると、上記計量
が困難となるに加えて、マグネツトローラー駆動トルク
が高くなるという欠点も出てくるのでHA≧PGとなる
範囲はこの刃の位置よりも現象磁極中心側にあることを
要する。従って、HA≧PGとなる位置は前記範囲にあ
ることが必要である。 【0012】尚、本発明における「スリーブ上での磁界
成分」について説明すると、マグネツトローラーが担う
ところの磁気ブラシ現像は「スリーブ面上」において出
現するので、業界においては、マグネツトローラーの磁
界測定位置は「スリーブ面上」とか「スリーブ上」とさ
れるのが通例である。しかし、実際には測定に用いる
「ホールプローブ」の構造上の事情により、スリーブ面
に接触する位置からやや離れた位置で磁界測定が行なわ
れてきた。即ち、磁界を測るセンサーであるホール素子
はプローブの表面からある深さdだけ離れた位置に埋設
されている。この素子をプロープ表面に露出させること
は可能ではあるが、被測定物に接触することによって摩
耗する上に温度変動の影響をうけて動作が安定しないこ
とがよく知られている。従って、前記したようにホール
素子は埋設された状態で市販されているのが普通であ
る。かくして、「スリーブ面上で測定する」といっても
厳密にはスリーブ面に接触する位置からdだけ離れた位
置で測定していることになるが、そのようにして測った
磁界を「スリーブ面上での磁界」と呼ぶことは業界の慣
行である。例えば特公昭60−37607号公報では、
「このときのスリーブ20表面上における磁束分布を測
定した。(第4欄12〜14行)」と記載され、また実
公昭57−9798号公報では、「ロール表面磁束密度
は1000Gまで高めることができた。(第2欄19〜
21行)」と記載され、測定位置については記載されて
いない。 【0013】後記実施例において、測定位置としては、
用いたホールプローブの値であるd=0.5mmが記載さ
れている。そもそも、磁界パタンの特徴(極大あるいは
極小)はマグネツトに近くなるほど明瞭になるので、d
=0.5mmにおいて成り立つことは、字義通りの「スリ
ーブ上」に於いても成り立つ。従って、実施例をd=
0.5mmの位置で行なったとしても本発明の主旨と相違
する結果が出るわけではない。 【0014】以上述べた様に、本発明によるマグネツト
ローラーは放射方向磁界成分(HR)の値が相対的に低
くても捕捉力が強くなった結果、トナー、キヤリヤーの
落下防止に有効であり、且つ、感光体上の余分な部分
(画像で白の部分)に付着したトナー、キヤリヤーをマ
グネツトローラー側へ引き戻すことにより、解像力が高
められ、階調性や細線性が向上する。それ故、磁気特性
が特段に高い磁石を用いる必要がない。 【0015】かかるマグネツトローラーを実現するに
は、使用するマグネツトの配向着磁方向や断面形状及び
隣接するマグネツトとの組合せ方法を調節して行う。例
えば現像磁極に相当する永久磁石の回転角度方向の巾を
広くする、同永久磁石の回転方向の両端部を中央部より
も強く着磁する、同永久磁石の回転方向の断面形状を両
端部がスリーブ面により近くなる形状(双頭形状)とな
る等の手段、或いは現像磁極に相当する永久磁石に隣接
するこれと同性の磁性を有する磁石を配置し、その合成
磁場効果を利用して現像磁極の両端部でのHAを大きく
する等の手段があり、これらは組み合わせて用いられ
る。 【0016】従って、本発明で用いる各磁極用マグネツ
トには、配向着磁方向の自由度、断面形状の自由度があ
ることが望ましい。それ故、いわゆるプラスチツク、ゴ
ムをバインダーとするボンド磁石が用いられる。尚、本
発明において、接合配列とは複数個のボンド磁石が支持
軸上において互いの周方向の端面を接合して配列するこ
とを指す。 【0017】 【実施例】以下、本発明を実施例によって説明するが、
本発明はこれらにより何ら制約されるものではない。 【0018】実施例1、比較例1 図3に示した縮尺図の断面の如く、外径31mmのアル
ミニウムスリーブ(3)内に各形状の最大エネルギー積
1.5MGOeのプラスチツク異方性磁石(2)
(2’)(2’)(2’)を図示した各形状に成形・着
磁したものを鉄製シヤフト(1)に接合し、回転外径を
27.5mmに仕上げて組み立てた。スリーブ表面から
0.5mmの位置におけるHR、HAのパターン図は図
4の如くであった。HA≧PGとなる範囲は±37゜で
あった。このマグネツトローラーを普通紙複写機に組み
こみ複写テストを行ったが、トナー、キヤリヤーの落下
は殆ど見られなかった。 【0019】一方、比較のために図5の如き縮尺形状に
アルミニウムシヤフト(1)及び最大エネルギー積3.
5MGOeの磁石(2)(2’)(2’)(2’)を接
合したマグネツトローラーを外径31mmのアルミニウ
ムスリーブ(3)を用いて組立てた。このマグネツトロ
ーラーを用いた複写テストではトナー、キヤリヤーの落
下がみられ、紙に汚れが観察された。スリーブ表面から
0.5mmの位置におけるHR、HAのパターン図を図
6に示したが、このマグネツトローラーのPGは上記本
発明によるマグネツトローラーよりも大であるにもかか
わらず、上記の不都合が生じており、これはHA≧PG
となる領域が存在しないことに因るものである。 【0020】 【発明の効果】以上述べた様に、本発明によるマグネツ
トローラーは、トナー、キヤリヤーの落下・飛散を効果
的に防止できるとともに、良好な複写品質を与えるもの
である。本発明によれば、高品質のマグネツトローラー
を効率よく設計することができる。
Description: BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a magnet roller for development of a plain paper copying machine, and more particularly, to a method for providing a good image and providing toner and a carrier from a development device. The present invention relates to a magnet roller which is effective for preventing falling and scattering of the magnet. 2. Description of the Related Art Magnet rollers are frequently used in developing plain paper copiers to transport toner and carriers.
One of the disadvantages unique to such a magnetic developing method is that a magnetic toner caused by a magnetic field generated around a magnet roller,
In addition to the problem that the carrier catching power is insufficient and these fall and scatter around the developing device and cause the copier to become dirty, the toner and the carrier adhered to the photoreceptor reduce the gradation of the image. There is a problem that the image quality deteriorates such as white spots and black spots. Conventionally, as a method for preventing the toner and the carrier from falling and scattering, a method is employed in which the HR is maximized by focusing on the magnetic field component HR in the developing magnetic pole on the sleeve surface of the magnet roller. In general, a method of increasing the capturing power of toner and carrier is adopted. For this purpose, a method is used in which a magnet having high magnetic properties (for example, an anisotropic sintered ferrite magnet) is finished with high dimensional accuracy and used. However, there is a regret that this method increases the cost. FIG. 3 of Japanese Utility Model Laid-Open Publication No. 51-8745 shows that the width of the developing magnetic pole 21 is made sufficient by using a cylindrical magnet and is separated from the developing magnetic pole 21 so as to be close to the conveying magnetic pole 22 having a narrow width.
By providing the magnet 23, the problem in the case of using a conventional magnet having a rectangular cross section, that is, the magnetic flux density A 'in the vertical direction is large, the magnetic flux density B' in the tangential direction contributing to the transport of the developing pole is small, and the transport capacity is small. It is disclosed that this problem has been solved. FIG. 3 shows the magnetic flux density A ′ in the vertical direction and the magnetic flux density B ′ in the tangential direction.
Distribution is two peaks, so that the so-called “spike” of the developer is disturbed, and tailing (tailing) at copying, carrier adhesion to paper and toner adhesion are likely to occur, and good image quality is obtained. There is a problem that it is difficult. Although the magnet material is not specified, it is determined from the filing date that it is a sintered magnet.However, the sintered magnet has restrictions on the formability, the degree of freedom in the orientation and magnetization direction, and the degree of freedom in the cross-sectional shape. Yes, and therefore the design of the magnet roller is also constrained. SUMMARY OF THE INVENTION The present invention solves the above-mentioned drawbacks of the prior art, and the use of an inexpensive magnet having moderate magnetic properties results in a strong catching force. It is an object of the present invention to provide a magnet roller in which the carrier is effectively prevented from dropping and scattering, the resolution is enhanced, and the gradation and fine line properties are improved. That is, the present invention provides a plain paper copy comprising a magnet group in which a plurality of bond magnets are joined and arranged around a support shaft and a non-magnetic sleeve covering the outer circumference of the magnet group. In the machine magnet roller, a magnetic field component in the radial direction on the sleeve of the developing magnetic pole has a single peak near the developing magnetic pole and is larger than the peak value and is tangential to the magnetic field component in the radial direction. A magnetic field vector having a combined magnetic field vector with the directional magnetic field component, and a range of the composite magnetic field vector being closer to the center of the developing magnetic pole than the position of the toner and the carrier measuring blade and within 45 ° from the center of the developing magnetic pole. Includes net rollers. DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS The magnetic field strength of a developing magnet roller is generally evaluated by measuring only the radial magnetic field component HR at the sleeve surface, because of its ease of measurement. It is. However, since the magnetic field is a vector quantity, a tangential magnetic field component HT is inevitably present, and it is considered that this naturally contributes to the developing mechanism. The inventors of the present invention focused on a “synthetic magnetic field HA” that combines a radial magnetic field component and a tangential magnetic field component, and as a result, the trapping force of toner and a carrier is generally measured in the radial magnetic field. It has been found that it is more strongly associated with the absolute value of the resultant magnetic field than with the component value. Further, the present inventors, in addition to the HR magnetic field distribution on the surface of the sleeve of the magnet roller,
When the magnetic field distribution was varied and examined, it was found that a magnetic field vector having an HR consisting of a single peak near the developing magnetic pole and having an absolute value of HA larger than the peak value PG, HA ≧ When the two conditions that the PG range is on the center of the developing magnetic pole from the position of the toner and the carrier and the blade for metering and is within 45 ° from the center of the developing magnetic pole are satisfied, the peak value of HR becomes relative. Even a small magnet roller has a high toner and carrier capture power,
It has been found that these drops and scatters do not substantially occur and that good copy quality can be obtained. The magnetic pole center referred to here is one magnetic H
In the distribution pattern of R, it refers to the distribution center of two points on the left and right that cut this pattern at the half value height of the PG value. FIG. 2 shows an example of the magnetic field distribution on the surface of the sleeve of the magnet roller which is effective in preventing the toner and the carrier from dropping as described above. It is not clear why such a surface magnetic field distribution is effective, but regions where HA ≧ PG appear on the left and right sides of the developing magnetic pole, respectively, and the distribution of HA becomes a double-headed distribution having two peaks. It is considered that the toner and carrier present between the peaks are stably captured. In the present invention, HR needs to be a single peak. When the HR has a plurality of peaks, the HA distribution also has a plurality of (values exceeding 2) peaks,
Disorder occurs in the so-called "spring" of the developer, so that tailing and carrier adhesion are likely to occur, and good image quality cannot be obtained. The area where HA ≧ PG is preferably within 45 ° from the center of the magnetic pole of the developing magnetic pole, more preferably within 30 ° C., even more preferably within 15 °. If the area is too large, various disadvantages occur. That is, the amount of the toner and the carrier held in the area becomes excessive and the weight effect causes the toner and the carrier to drop sharply. The direction of the magnetic field vector at the peak of the magnetic field vector HA is excessively opened outward, and the toner and the carrier are removed. For example, the capturing effect is reduced. Therefore, the region where HA ≧ PG is preferably within the above-mentioned angle range, but if the angle range is too narrow, the region for capturing toner and carrier becomes small and the effect becomes insufficient. Since it varies depending on the level of the peak value, it cannot be unconditionally specified, but it is preferable that the range covers a range of about 5 ° or more. Further, as described above, it is inconvenient if the vector direction at the peak of the magnetic field vector HA is too open, but it is also possible to restrict this opening to an angle formed by the vector HA with respect to the radiation direction and suppress the opening within a certain angle. It is valid. Further, in order to adjust the amount of toner and carrier supplied to the developing magnetic pole, a blade for measuring the amount of toner and carrier cut off is provided before the developing magnetic pole, for example, in the vicinity of about 45 to 50 ° from the center of the developing magnetic pole. Is common.
If the magnetic field HA at the position of this blade is too strong, in addition to the difficulty of the above-mentioned measurement, there is also a drawback that the driving torque of the magnet roller increases, so that the range of HA ≧ PG is smaller than the position of this blade. Must be on the center side of the magnetic pole. Therefore, the position where HA ≧ PG needs to be within the above range. In the present invention, the "magnetic field component on the sleeve" will be described. Since the magnetic brush development performed by the magnet roller appears on the "sleeve surface", the magnetic field of the magnet roller has been developed in the industry. The measurement position is usually “on the sleeve surface” or “on the sleeve”. However, actually, due to the structure of the “hole probe” used for measurement, the magnetic field measurement has been performed at a position slightly away from the position in contact with the sleeve surface. That is, the Hall element, which is a sensor for measuring the magnetic field, is embedded at a position separated by a certain depth d from the surface of the probe. Although it is possible to expose this element to the probe surface, it is well known that the element is worn by contact with the object to be measured and its operation is not stable due to the influence of temperature fluctuation. Therefore, as described above, the Hall element is usually commercially available in an embedded state. Thus, strictly speaking, "measurement on the sleeve surface" means that the measurement is performed at a position distant from the position in contact with the sleeve surface by d. Calling "magnetic field above" is an industry practice. For example, in Japanese Patent Publication No. 60-37607,
In this case, it is described that "the magnetic flux distribution on the surface of the sleeve 20 was measured. (Col. 4, lines 12 to 14)." According to Japanese Utility Model Publication No. 57-9798, "the roll surface magnetic flux density can be increased to 1000G. (Second column 19-
21)), and the measurement position is not described. In the embodiment described later, the measurement position is
The value of the used hole probe, d = 0.5 mm, is described. In the first place, the characteristics (maximum or minimum) of the magnetic field pattern become clearer as they are closer to the magnet.
= 0.5 mm also holds true on the literal “on the sleeve”. Therefore, the embodiment is represented by d =
Even if it is performed at the position of 0.5 mm, a result different from the gist of the present invention is not obtained. As described above, the magnet roller according to the present invention is effective in preventing the toner and the carrier from dropping because the trapping force is increased even if the value of the radial magnetic field component (HR) is relatively low. In addition, the toner and the carrier adhered to an extra portion (white portion in the image) on the photoreceptor are pulled back to the magnet roller, so that the resolving power is enhanced, and the gradation and fine line are improved. Therefore, it is not necessary to use a magnet having a particularly high magnetic property. In order to realize such a magnet roller, the magnet is used by adjusting the orientation and magnetizing direction and sectional shape of the magnet to be used and the method of combining the magnet with an adjacent magnet. For example, the width in the rotation angle direction of the permanent magnet corresponding to the developing magnetic pole is widened, both ends in the rotation direction of the permanent magnet are magnetized more strongly than the center part, and the cross-sectional shape in the rotation direction of the permanent magnet is both ends. Means such as a shape closer to the sleeve surface (double-headed shape), or a magnet having the same magnetism as the permanent magnet corresponding to the developing magnetic pole is arranged, and the developing magnetic pole There are means such as increasing the HA at both ends, and these are used in combination. Therefore, it is desirable that each magnetic pole for use in the present invention has a degree of freedom in the orientation and magnetization direction and a degree of freedom in the cross-sectional shape. Therefore, a bonded magnet using a so-called plastic or rubber as a binder is used. In the present invention, the term “joining arrangement” means that a plurality of bonded magnets are arranged by joining their circumferential end faces on a support shaft. Hereinafter, the present invention will be described with reference to examples.
The present invention is not limited by these. Example 1 and Comparative Example 1 As shown in the cross-sectional view of the scale shown in FIG. 3, a plastic anisotropic magnet (2) having a maximum energy product of 1.5 MGOe of each shape was placed in an aluminum sleeve (3) having an outer diameter of 31 mm. )
(2 ') (2') (2 ') molded and magnetized into the respective shapes shown in the figure were joined to an iron shaft (1), and the outer diameter of rotation was finished to 27.5 mm and assembled. FIG. 4 shows a pattern diagram of HR and HA at a position of 0.5 mm from the surface of the sleeve. The range where HA ≧ PG was ± 37 °. This magnet roller was assembled in a plain paper copying machine and a copying test was carried out. As a result, toner and carrier were hardly dropped. On the other hand, for comparison, the aluminum shaft (1) and the maximum energy product 3.
A magnet roller to which 5MGOe magnets (2), (2 ′), (2 ′), and (2 ′) were joined was assembled using an aluminum sleeve (3) having an outer diameter of 31 mm. In a copy test using this magnet roller, toner and carrier dropped, and stains were observed on the paper. FIG. 6 shows a pattern diagram of HR and HA at a position of 0.5 mm from the surface of the sleeve. However, although the PG of the magnet roller is larger than the magnet roller according to the present invention, the disadvantages described above are obtained. And HA ≧ PG
Is not present. As described above, the magnet roller according to the present invention can effectively prevent the toner and the carrier from dropping and scattering, and provide good copy quality. According to the present invention, a high quality magnet roller can be efficiently designed.

【図面の簡単な説明】 【図1】マグネツトローラーのスリーブ表面磁界ベクト
ル図である。 【図2】本発明のマグネツトローラーの磁界分布の概念
図である。 【図3】本発明の実施態様を示す概略断面図である。 【図4】図3のマグネツトローラーの磁界分布図であ
る。 【図5】比較のためのマグネツトローラーの概略断面図
である。 【図6】図5のマグネツトローラー磁界分布図である。 【符号の説明】 1 シヤフト 2 現像磁極磁石 2’ 磁石 3 スリーブ
BRIEF DESCRIPTION OF THE DRAWINGS FIG. 1 is a magnetic field vector diagram of a sleeve surface of a magnet roller. FIG. 2 is a conceptual diagram of a magnetic field distribution of the magnet roller of the present invention. FIG. 3 is a schematic sectional view showing an embodiment of the present invention. FIG. 4 is a magnetic field distribution diagram of the magnet roller of FIG. 3; FIG. 5 is a schematic sectional view of a magnet roller for comparison. 6 is a magnetic roller magnetic field distribution diagram of FIG. [Description of Signs] 1 shaft 2 developing magnetic pole magnet 2 'magnet 3 sleeve

Claims (1)

(57)【特許請求の範囲】 1.支持軸周に複数個のボンド磁石を接合配列したマグ
ネツト群と上記マグネツト群の外周をカバーする非磁性
スリーブとからなる普通紙複写機用マグネツトローラー
に於いて、現像磁極の近傍に、該現像磁極のスリーブ上
での放射方向磁界成分が単一ピークを有し、且つ該ピー
ク値よりも大きい、該放射方向磁界成分と接線方向磁界
成分との合成磁界ベクトルが存在し、且つその範囲がト
ナー、キヤリヤーすり切り計量用刃の位置よりも現像磁
極中心側であって該現像磁極中心から45゜以内である
ことを特徴とするマグネツトローラー。
(57) [Claims] In a magnet roller for a plain paper copying machine comprising a magnet group in which a plurality of bond magnets are joined and arranged around the support shaft and a non-magnetic sleeve covering the outer circumference of the magnet group, the developing roller is disposed near the developing magnetic pole. There is a combined magnetic field vector of the radial magnetic field component and the tangential magnetic field component whose radial magnetic field component on the sleeve of the magnetic pole has a single peak and is larger than the peak value, and the range is the toner. A magnet roller which is closer to the center of the developing magnetic pole than the position of the carrier wear measuring blade and is within 45 ° from the center of the developing magnetic pole.
JP8277338A 1996-09-27 1996-09-27 Magnet roller Expired - Lifetime JP2742924B2 (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP8277338A JP2742924B2 (en) 1996-09-27 1996-09-27 Magnet roller

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP8277338A JP2742924B2 (en) 1996-09-27 1996-09-27 Magnet roller

Related Parent Applications (1)

Application Number Title Priority Date Filing Date
JP60247709A Division JPH0693153B2 (en) 1985-11-05 1985-11-05 Magnet controller

Publications (2)

Publication Number Publication Date
JPH09179410A JPH09179410A (en) 1997-07-11
JP2742924B2 true JP2742924B2 (en) 1998-04-22

Family

ID=17582141

Family Applications (1)

Application Number Title Priority Date Filing Date
JP8277338A Expired - Lifetime JP2742924B2 (en) 1996-09-27 1996-09-27 Magnet roller

Country Status (1)

Country Link
JP (1) JP2742924B2 (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62108272A (en) * 1985-11-05 1987-05-19 Kanegafuchi Chem Ind Co Ltd Magnet roller

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS62108272A (en) * 1985-11-05 1987-05-19 Kanegafuchi Chem Ind Co Ltd Magnet roller

Also Published As

Publication number Publication date
JPH09179410A (en) 1997-07-11

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