JPH0693153B2 - Magnet controller - Google Patents

Magnet controller

Info

Publication number
JPH0693153B2
JPH0693153B2 JP60247709A JP24770985A JPH0693153B2 JP H0693153 B2 JPH0693153 B2 JP H0693153B2 JP 60247709 A JP60247709 A JP 60247709A JP 24770985 A JP24770985 A JP 24770985A JP H0693153 B2 JPH0693153 B2 JP H0693153B2
Authority
JP
Japan
Prior art keywords
magnetic field
magnet
developing
carrier
toner
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
JP60247709A
Other languages
Japanese (ja)
Other versions
JPS62108272A (en
Inventor
泰 掛橋
嘉男 坂田
文仁 毛利
孚史 阪内
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.)
Kaneka Corp
Original Assignee
Kaneka Corp
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 Kaneka Corp filed Critical Kaneka Corp
Priority to JP60247709A priority Critical patent/JPH0693153B2/en
Publication of JPS62108272A publication Critical patent/JPS62108272A/en
Publication of JPH0693153B2 publication Critical patent/JPH0693153B2/en
Anticipated expiration legal-status Critical
Expired - Lifetime legal-status Critical Current

Links

Classifications

    • GPHYSICS
    • G03PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
    • G03GELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
    • G03G15/00Apparatus for electrographic processes using a charge pattern
    • G03G15/06Apparatus for electrographic processes using a charge pattern for developing
    • G03G15/08Apparatus for electrographic processes using a charge pattern for developing using a solid developer, e.g. powder developer
    • G03G15/09Apparatus for electrographic processes using a charge pattern for developing using a solid developer, e.g. powder developer using magnetic brush
    • G03G15/0921Details concerning the magnetic brush roller structure, e.g. magnet configuration

Description

【発明の詳細な説明】 「産業上の利用分野」 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。
The present invention relates to a developing magnet roller for a plain paper copying machine, and more specifically, it provides a good image and, at the same time, drops toner or carrier from the developing device. The present invention relates to a magnet roller that is effective in preventing scattering.

「従来技術と問題点」 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。
"Prior Art and Problems" In developing a plain paper copying machine, a magnet roller is often used for carrying toner and carrier. One of the drawbacks peculiar to such a magnetic developing system is that the magnetic toner generated by the magnetic field generated around the magnet roller and the carrier cannot be sufficiently captured by the carrier, and they fall and scatter around the developing device, resulting in Not only is there a problem of causing stains, but there is also a problem that the toner and carrier attached to the photoconductor lowers the gradation of the image, and the image quality such as white spots and black spots deteriorates.

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。
Heretofore, as a method of preventing the toner and carrier from falling and scattering, attention has been paid to the radial magnetic field component HR at the developing magnetic pole on the sleeve surface of the magnet roller, and by making HR as large as possible, the toner and carrier The method of increasing the capturing power of is generally adopted. For this purpose, a means of using a magnet having a high magnetic property (for example, an anisotropic sintered ferrite magnet) after finishing with high dimensional accuracy is used.
However, this method has a drawback that the cost is high.

「問題点を解決するための手段」 本発明者らはかかる欠点を解消し、中程度の磁気特性を
有する安価な磁石を用いてもトナー、キヤリヤーの落下
・飛散の無いマグネツトローラーについて鋭意研究した
結果、本発明を完成した。
"Means for Solving Problems" The inventors of the present invention have solved the above drawbacks, and have diligently studied a magnet roller that does not drop or scatter toner or carrier even if an inexpensive magnet having a medium magnetic property is used. As a result, the present invention has been completed.

即ち、本発明は支持軸周に複数個のマグネツトを接合配
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を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。
That is, the present invention relates to a magnet roller for a plain paper copying machine, which comprises a magnet group in which a plurality of magnets are joined and arranged around a support shaft and a non-magnetic sleeve covering the outer circumference of the magnet group, in the vicinity of the developing magnetic pole. , There is a combined magnetic field vector of the radial magnetic field component and the tangential magnetic field component that has a radial magnetic field component on the sleeve of the developing magnetic pole larger than the peak value, and its range is 45 from the developing magnetic pole center. The content is a magnet roller characterized by being within °.

従来、現像用マグネツトローラーの磁界強度分布はその
スリーブ表面に於ける放射方向磁界成分にのみ着目され
てきた。本発明者らはトナー、キヤリヤーの捕捉力に関
して検討を重ねてきた結果、トナー、キヤリヤーの捕捉
力はマグネツトローラーのスリーブ上での特定方向磁界
成分によって規定されるのではなく、各方向成分のベク
トル和として得られる合成磁界ベクトルの絶対値によっ
て規定されていることを見出した。即ち、第1図に於い
て、HRは放射方向磁界成分、HTは接線方向磁界成分、HA
は合成磁界ベクトルを表すが、トナー、キヤリヤーの捕
捉力はHRではなくHAによって規定される。そこで本発明
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HRのピーク値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・飛散が事実上生じない
ことを見出した。
Conventionally, the magnetic field strength distribution of the developing magnet roller has been focused only on the radial magnetic field component on the sleeve surface. The inventors of the present invention have conducted extensive studies on the trapping force of toner and carrier, and as a result, the trapping force of toner and carrier is not regulated by the magnetic field component in a specific direction on the sleeve of the magnet roller, but by It was found that it is defined by the absolute value of the composite magnetic field vector obtained as the vector sum. That is, in FIG. 1, HR is a radial magnetic field component, HT is a tangential magnetic field component, and HA.
Represents the composite magnetic field vector, but the trapping force of toner and carrier is defined by HA instead of HR. Therefore, the present inventors examined various magnetic field distributions of HA in addition to the magnetic field distribution of HR on the surface of the sleeve of the magnet roller, and found that HA near the developing magnetic pole was larger than the peak value PG of HR. When there are two magnetic field vectors with the absolute value of, the range of HA ≧ PG is within 45 ° from the center of the developing magnetic pole, the peak value of HR is relatively small. It has been found that even a roller has a high toner and carrier trapping force, and these particles do not fall or scatter.

ここでいう磁極中心とは、1つの磁性のHR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第2図に示した。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。
The magnetic pole center referred to here is the distribution center of two points on the left and right that cut this pattern at the half-height of the PG value in one magnetic HR distribution pattern. An example of the magnetic field distribution on the sleeve surface of the magnet roller, which is effective for preventing the toner and carrier from falling as described above, is shown in FIG. Although it is not clear why such surface magnetic field distribution is effective, regions where HA ≧ PG appear on the left and right sides of the developing magnetic pole, and the HA distribution is a double-headed distribution with two peaks.
It is considered that the toner and carrier existing between the two peaks are stably captured.

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
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。
The area where HA ≧ PG is preferably within 45 ° from the magnetic pole center of the developing magnetic pole, more preferably within 30 ° C., 15
It is more preferable if it is within the range of °. If such a region is too wide, various inconveniences occur. In other words, the amount of toner and carrier held in the area becomes excessive, and the weight effect causes the toner and carrier to drop violently.
The direction of the magnetic field vector at the peak of HA opens too outward,
For example, the trapping action of toner and carrier is reduced. Therefore, it is preferable that the area where HA ≧ PG is within the above-mentioned angle range, but if the angle range is too narrow, the area for trapping toner and carrier becomes small and the effect becomes insufficient. Although it cannot be unconditionally specified because it fluctuates depending on the peak value level, it is preferable that the range be approximately 5 ° or more. Furthermore, it has been described that it is inconvenient if the vector direction at the peak of the magnetic field vector HA is too wide, but it is also possible to define this opening as the angle formed by the vector HA with respect to the radial direction and suppress it within a certain angle. It is valid.

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
も現像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。
Further, in order to adjust the supply amount of toner and carrier to the developing magnetic pole, it is common to provide a blade for measuring toner and carrier scraping in front of the developing magnetic pole, for example, in the vicinity of about 45 to 50 ° from the center of the developing magnetic pole. Is. If the magnetic field HA at the position of this blade is too strong, in addition to the above-mentioned weighing being difficult, there is also the drawback that the magnet roller drive torque will be high, so the range HA ≥ PG is higher than the position of this blade. It is necessary to be on the center side of the developing magnetic pole. Therefore, HA ≧ PG
It is necessary that the position of is within the above range.

尚、現像スリーブや感光体は一定の方向に回転して使用
されるので、この磁界ベクトルHAのピーク位置は、必ず
しもHRのピークの両側にある必要はなく、少なくとも有
効な片側にあれば良い。
Since the developing sleeve and the photoconductor are used by rotating in a fixed direction, the peak position of the magnetic field vector HA does not necessarily have to be on both sides of the peak of HR, but may be on at least one effective side.

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。
As described above, the magnet roller according to the present invention is effective in preventing the toner and the carrier from falling as a result of the strong capturing force even when the value of the magnetic field component in the radial direction is relatively low. By pulling back the toner and carrier attached to the extra portion (white portion in the image) to the magnet roller side, the resolving power is enhanced and the gradation and fine line property are improved. Therefore, it is not necessary to use a magnet having particularly high magnetic characteristics.

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
性の特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。従って、本発
明で用いる各磁極用マグネツトには汎用される一般的な
マグネツト材質が使用できるが、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
磁石が好ましい。
In order to realize such a magnet roller, the orientation and magnetization direction and sectional shape of the magnet to be used and the combination method with the adjacent magnet are adjusted. For example, the width of the permanent magnet corresponding to the developing magnetic pole in the rotation angle direction 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 of the permanent magnet in the rotation direction is Means such as a shape closer to the sleeve surface (double-headed shape),
Alternatively, there is means such as arranging a magnet having the same characteristics as the permanent magnet adjacent to the developing magnetic pole and having the same magnetic field effect to increase the HA at both ends of the developing magnetic pole. Used in combination. Therefore, although a general-purpose magnet material generally used can be used for each magnetic pole magnet used in the present invention, it is desirable that the magnetic material has a degree of freedom in the orientation and magnetization direction and a degree of freedom in the cross-sectional shape. Therefore,
So-called plastics and bonded magnets using rubber as a binder are preferred.

「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。
"Examples" Hereinafter, the present invention will be described with reference to Examples, but the present invention is not limited thereto.

実施例1、比較例1 第3図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のパターン図は第4図の如くであった。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。
Example 1 and Comparative Example 1 As shown in the cross section of the scale diagram in FIG. 3, the maximum energy product of each shape was 1.
5MGOe plastic anisotropic magnet (2) (2 ')
Each of (2 ') and (2') molded and magnetized into the illustrated shape was joined to an iron shaft (1), and the outer diameter of rotation was finished to 27.5 mm for assembly. The pattern diagram of HR and HA at the position 0.5 mm from the sleeve surface was as shown in FIG. HA
The range of ≧ PG was ± 37 °. I did a copy test by incorporating this magnet roller into a plain paper copier.
Almost no drop of toner or carrier was seen.

一方、比較のために第5図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H
R、HAのパターン図を第6図に示したが、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。
On the other hand, for comparison, the magnet roller with the aluminum shaft (1) and the magnets (2) (2 ') (2') (2 ') of maximum energy product 3.5MGOe joined in a scaled shape as shown in FIG. 5 is removed. It was assembled using an aluminum sleeve (3) with a diameter of 31 mm. In the copy test using this magnet roller, toner and carrier were found to have fallen and stains were observed on the paper. H at 0.5 mm from the sleeve surface
A pattern diagram of R and HA is shown in FIG. 6. The above-mentioned inconvenience occurs even though the PG of this magnet roller is larger than that of the magnet roller according to the present invention. This is because there is no region where ≧ PG.

「作用・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・飛散がなく、良好な複写品質
を与えるものである。
[Operation / Effect] As described above, the magnet roller according to the present invention does not drop or scatter toner or carrier, and provides good copy quality.

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

第1図はマグネツトローラーのスリーブ表面磁界ベクト
ル図、第2図は本発明のマグネツトローラーの磁界分布
の概念図、第3図は本発明の実施態様を示す概略断面
図、第4図は第3図のマグネツトローラーの磁界分布
図、第5図は比較のためのマグネツトローラーの概略断
面図、第6図は第5図のマグネツトローラー磁界分布図
である。 1……シヤフト 2……現像磁極磁石 2′……磁石 3……スリーブ
FIG. 1 is a vector diagram of the magnetic field on the sleeve surface of the magnet roller, FIG. 2 is a conceptual diagram of the 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, and FIG. FIG. 3 is a magnetic field distribution diagram of the magnet roller of FIG. 3, FIG. 5 is a schematic sectional view of the magnet roller for comparison, and FIG. 6 is a magnetic roller magnetic field distribution diagram of FIG. 1 ... Shaft 2 ... Development magnetic pole magnet 2 '... Magnet 3 ... Sleeve

フロントページの続き (56)参考文献 特開 昭54−95243(JP,A) 特開 昭57−114164(JP,A) 特開 昭59−57265(JP,A) 実開 昭51−8745(JP,U)Continuation of the front page (56) References JP-A-54-95243 (JP, A) JP-A-57-114164 (JP, A) JP-A-59-57265 (JP, A) Actual development-Sho 51-8745 (JP , U)

Claims (1)

【特許請求の範囲】[Claims] 【請求項1】支持軸周に複数個のマグネツトを接合配列
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を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。
1. A magnet roller for a plain paper copying machine comprising a magnet group in which a plurality of magnets are joined and arranged around a support shaft, and a non-magnetic sleeve covering the outer circumference of the magnet group, in the vicinity of a developing magnetic pole. , There is a combined magnetic field vector of the radial magnetic field component and the tangential magnetic field component that has a radial magnetic field component on the sleeve of the developing magnetic pole larger than the peak value, and its range is 45 from the developing magnetic pole center. A magnet roller characterized by being within °.
JP60247709A 1985-11-05 1985-11-05 Magnet controller Expired - Lifetime JPH0693153B2 (en)

Priority Applications (1)

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

Applications Claiming Priority (1)

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

Related Child Applications (1)

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

Publications (2)

Publication Number Publication Date
JPS62108272A JPS62108272A (en) 1987-05-19
JPH0693153B2 true JPH0693153B2 (en) 1994-11-16

Family

ID=17167494

Family Applications (1)

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

Country Status (1)

Country Link
JP (1) JPH0693153B2 (en)

Families Citing this family (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH0766215B2 (en) * 1987-03-31 1995-07-19 日立金属株式会社 Development device
JPH0219166U (en) * 1988-03-28 1990-02-08
JP2742924B2 (en) * 1996-09-27 1998-04-22 鐘淵化学工業株式会社 Magnet roller

Family Cites Families (4)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS5334921Y2 (en) * 1974-07-05 1978-08-26
JPS5495243A (en) * 1978-01-11 1979-07-27 Ricoh Co Ltd Magnetic brush developing device
JPS57114164A (en) * 1981-01-07 1982-07-15 Ricoh Co Ltd Magnetic brush developing device
JPS5957265A (en) * 1982-09-27 1984-04-02 Konishiroku Photo Ind Co Ltd Electrophotographic recording device

Also Published As

Publication number Publication date
JPS62108272A (en) 1987-05-19

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