JPH02267576A - Developing device - Google Patents

Developing device

Info

Publication number
JPH02267576A
JPH02267576A JP1087873A JP8787389A JPH02267576A JP H02267576 A JPH02267576 A JP H02267576A JP 1087873 A JP1087873 A JP 1087873A JP 8787389 A JP8787389 A JP 8787389A JP H02267576 A JPH02267576 A JP H02267576A
Authority
JP
Japan
Prior art keywords
coils
armature
cylinder
coil
developing device
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.)
Pending
Application number
JP1087873A
Other languages
Japanese (ja)
Inventor
Masao Karibe
苅部 征夫
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
Canon Precision Inc
Original Assignee
Canon Inc
Canon Precision 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, Canon Precision Inc filed Critical Canon Inc
Priority to JP1087873A priority Critical patent/JPH02267576A/en
Publication of JPH02267576A publication Critical patent/JPH02267576A/en
Pending legal-status Critical Current

Links

Abstract

PURPOSE:To obtain an alternation rotating magnetic field and to quiet a rotational noise by a simple constitution by bringing an AC current of plural phases to electric conduction to plural sets of armature coils. CONSTITUTION:Along the inside circumference of a cylinder 11 of a developing sleeve 10, a single coil (b) of an armature coil 13 is provided between single coils (a) of an armature coil 12, and provided by shifting electrical angles of the adjacent single coils (a), (b) by 90 deg. each. In this state, an AC current of two phases being 90 deg. out of phase is brought to electric conduction to the coils 12, 13, respectively, and on the outside periphery of the cylinder 11, an alternation rotating magnetic field is generated. In such a way, while a magnetic developer is being attracted onto the outside circumferential surface of the cylinder 11, the developer moves on the outside circumferential surface of the cylinder in accordance with a rotating speed of the rotating magnetic field. Accordingly, the developer moves to an image carrying body 1 from a prescribed position in a developing device 3, and attracted to its electrostatic latent image.

Description

【発明の詳細な説明】 (産業上の利用分野) 本発明は電子写真法等を採用する画像形成装置の現像装
置に関する。
DETAILED DESCRIPTION OF THE INVENTION (Field of Industrial Application) The present invention relates to a developing device of an image forming apparatus that employs electrophotography or the like.

(従来の技術) 例えば、電子写真法を採用した複写機等においては、像
担持体である感光ドラム上に形成された静電潜像を現像
装置により現像し、これを現像像として顕像化する必要
かある。ここで静電潜像の現像にあたって現像装置を介
して該現像装置中の現像剤(トナー)を静電潜像の方へ
供給する必要かあるか、この働きをするのが現像装置中
の現像スリーブである。該現像スリーブは一般に非磁性
材料からなる円筒部材内に多極着磁された永久磁石を回
転させ、該永久磁石からの漏洩磁界が永久磁石の回転と
共に移動することを利用して1円筒部材の外周面に沿っ
て磁性トナーを近接する感光ドラムの方へ供給するもの
が多く用いられている。
(Prior art) For example, in a copying machine that uses electrophotography, an electrostatic latent image formed on a photosensitive drum, which is an image carrier, is developed by a developing device, and this is visualized as a developed image. Is there a need to do that? When developing an electrostatic latent image, do you need to supply the developer (toner) in the developing device to the electrostatic latent image through the developing device? It's a sleeve. The developing sleeve generally rotates a multi-pole magnetized permanent magnet within a cylindrical member made of a non-magnetic material, and utilizes the fact that the leakage magnetic field from the permanent magnet moves with the rotation of the permanent magnet. Many devices are used that supply magnetic toner along the outer peripheral surface toward an adjacent photosensitive drum.

かかる現像スリーブを有する現像装置100を第12図
により説明すれば、図中110は感光ドラム120に近
接して配設される現像スリーブであって、該現像スリー
ブ110はトナー(磁性材を含有する磁性トナー)に接
する非磁性の薄肉円筒部材illと、該円筒部材Ill
内に回転自在に配設される環状で多極着磁の永久磁石1
12等とから構成されている。そして前記円筒部材11
1の外周部には内部の永久磁石112からの漏洩磁界に
より1図中斜線で示す如くトナーTか吸着されている。
A developing device 100 having such a developing sleeve will be described with reference to FIG. a non-magnetic thin-walled cylindrical member ill in contact with the magnetic toner), and the cylindrical member Ill
An annular, multi-pole magnetized permanent magnet 1 rotatably disposed inside
It is composed of 12 mag. and the cylindrical member 11
Toner T is attracted to the outer periphery of the magnet 1 as shown by diagonal lines in FIG. 1 due to a leakage magnetic field from an internal permanent magnet 112.

ここて、永久磁石112が図中矢印の如く反時計方向に
回転すれば、その漏洩磁界も回転移動するため1円筒部
材111上の吸着トナーTも永久磁石112の回転とは
逆方向、即ち図示の如く時計方向に回転して移動するこ
ととなる。従って円筒部材111上の吸着トナーTを永
久磁石112の回転により感光ドラム120との対向部
に順次移動させ、このトナーを感光ドラム120上の静
電潜像に吸着させて、該静電潜像をトナー像に変えるこ
とかできることとなる。
Here, if the permanent magnet 112 rotates counterclockwise as shown by the arrow in the figure, its leakage magnetic field also rotates, so that the attracted toner T on the first cylindrical member 111 also moves in the opposite direction to the rotation of the permanent magnet 112, that is, as shown in the figure. It will rotate and move clockwise as shown. Therefore, the attracted toner T on the cylindrical member 111 is sequentially moved to a portion facing the photosensitive drum 120 by the rotation of the permanent magnet 112, and this toner is attracted to the electrostatic latent image on the photosensitive drum 120, so that the toner T is attracted to the electrostatic latent image on the photosensitive drum 120. This means that it is possible to convert the image into a toner image.

(発明が解決しようとする課題) しかしながら上記従来技術における現像装置100では
永久磁石112を回転させることを基本原理としている
ため、該永久磁石112を回転支持するための軸受装置
や、永久磁石112を回転させるためのモータやベルト
又は減速ギヤ等を必要とし構造的に複雑となっていた。
(Problem to be Solved by the Invention) However, since the basic principle of the developing device 100 according to the above-mentioned prior art is to rotate the permanent magnet 112, a bearing device for rotatably supporting the permanent magnet 112, a bearing device for rotationally supporting the permanent magnet 112, etc. It requires a motor, belt, reduction gear, etc. for rotation, making it structurally complex.

また永久磁石112が回転するので回転騒音が発生し、
このため静かなオフィス等で使用される複写機やプリン
タ等に騒音を発生させるといった不都合があった。
Also, since the permanent magnet 112 rotates, rotation noise is generated.
This has caused the inconvenience of generating noise in copying machines, printers, etc. used in quiet offices and the like.

本発明は上記問題に鑑みてなされたもので、その目的と
する処は、*担持体上の静電潜像に現像剤を供給するに
際し、機械的な回転部分が不要で構成か簡単、且つ騒音
のない現像装置を提供するにある。
The present invention has been made in view of the above problems, and its objectives are: *When supplying developer to an electrostatic latent image on a carrier, there is no need for mechanical rotating parts, and the structure is simple; The purpose is to provide a noise-free developing device.

(課題を解決するための手段) 上記目的を達成すべく本発明は、磁力により現像剤を移
動させて像担持体上の静電潜像を現像する現像装置にお
いて、像担持体に近接して配設される非磁性材よりなる
薄肉円筒の内部にP個の単コイルからなる第1の電機子
コイルと同じくP個の単コイルからなる第2の電機子コ
イルとをこの円筒の周方向に互いに電気角を90度ずつ
ずらせて交互に配設し、該第1.第2の電機子コイルに
それぞれ90度位相の異なる2相の交流電流を通電して
前記円筒外周上に交番回転磁界を発生させ、該回転磁界
により円筒外周面に沿って磁性現像剤を像担持体の方へ
移動させることを特徴とする。
(Means for Solving the Problems) In order to achieve the above object, the present invention provides a developing device that develops an electrostatic latent image on an image carrier by moving a developer using magnetic force. A first armature coil made of P single coils and a second armature coil made of P single coils are placed inside a thin cylinder made of a non-magnetic material in the circumferential direction of this cylinder. The first. An alternating rotating magnetic field is generated on the outer periphery of the cylinder by applying two-phase alternating currents having a phase difference of 90 degrees to the second armature coil, and the rotating magnetic field carries an image of the magnetic developer along the outer periphery of the cylinder. It is characterized by moving towards the body.

また本発明は、磁力により現像剤を移動させて像担持体
上の静電潜像を現像する現像装置において、像担持体に
近接して配設される非磁性材よりなる薄肉円筒の内部に
それぞれ2P個ずつの単コイルからなる第1.第2.第
3の電機子コイルをこの円筒の周方向にその互いの単コ
イルか交互に配設されると共に隣り合う単コイルの電気
角か120度ずつずらされた状態で配設し、この第1.
第2、第3の電機子コイルにそれぞれ120度位相の異
なる3相の交流電流を通電して前記円筒外周上に交番回
転磁界を発生させ、該回転磁界により円筒外周面に沿っ
て磁性現像剤を像担持体の方へ移動させることを特徴と
する。
The present invention also provides a developing device that develops an electrostatic latent image on an image carrier by moving a developer using magnetic force, in which a thin cylinder made of a non-magnetic material is disposed close to the image carrier. The first coil consists of 2P single coils each. Second. The third armature coils are arranged in the circumferential direction of the cylinder such that the single coils alternate with each other and are shifted by 120 degrees in electrical angle from adjacent single coils.
A three-phase alternating current with a phase difference of 120 degrees is applied to the second and third armature coils to generate an alternating rotating magnetic field on the outer periphery of the cylinder, and the rotating magnetic field causes the magnetic developer to move along the outer periphery of the cylinder. is characterized in that it moves toward the image carrier.

(作用) 円筒の内周に沿って、第1の電機子コイルの単コイル間
に第2の電機子コイルの単コイルを配設すると共に、隣
り合う第1の電機子コイルの単コイルと第2の電機子コ
イルの単コイルとの電気角を90度ずつずらせて配設し
、且つ第1.第2の電機子コイルにそれぞれ90度位相
の異なる2相の交通電流を通電したため1円筒外周上に
交番回転磁界を発生させることができる。
(Function) A single coil of the second armature coil is arranged between the single coils of the first armature coil along the inner circumference of the cylinder, and a single coil of the adjacent first armature coil and the single coil of the first armature coil The second armature coil is arranged with an electrical angle shifted from the single coil by 90 degrees, and the first. Since the second armature coils are energized with two-phase traffic currents each having a phase difference of 90 degrees, an alternating rotating magnetic field can be generated on the outer periphery of one cylinder.

これは円筒内で永久磁石を回転させるのと同様な効果を
もたらすため1円筒の外周面上に磁性現像剤が吸漏され
つつ回転磁界の回転速度に従ってこの現像剤が円筒外周
面上を移動する。従って現像剤は現像装置内の所定位置
から像担持体の方へ移動し、その静電潜像に吸着される
This produces an effect similar to that of rotating a permanent magnet within a cylinder, so the magnetic developer is absorbed and leaked onto the outer circumferential surface of the cylinder, and the developer moves on the outer circumferential surface of the cylinder according to the rotational speed of the rotating magnetic field. . Therefore, the developer moves from a predetermined position in the developing device toward the image carrier and is attracted to the electrostatic latent image.

尚、3相交流を使用する3組の第1.第25w43の電
機子コイルを使用する場合も考え方は全く同一であるの
て、その作用の説明は省略する。
In addition, the first of three sets using three-phase alternating current. Since the concept is exactly the same when using the 25th w43rd armature coil, the explanation of its operation will be omitted.

(実施例) 以下に本発明の1実施例を電子写真法を採用する複写機
を例にとり添付図面に基づいて説明する。
(Embodiment) An embodiment of the present invention will be described below with reference to the accompanying drawings, taking a copying machine that employs electrophotography as an example.

先ず、第1図により複写機による画像形成の概要を説明
すれば、図中1は像担持体である感光ドラムであり、該
感光ドラムlの回りには一次帯電器2.現像装f3.転
写帯電器4.クリーニング器5が配設されている。即ち
一次帯電器2により一様帯電された感光ドラムl上に不
図示の原稿からの画像光りが露光されると、該画像光り
に徒って感光ドラム1上には静電潜像が形成される。該
静電潜像は感光ドラムlの回転とともに現像装置3の方
へ移動し、該現像装置3中の現像剤(磁性材を含有する
磁性トナーのことであり、以降トナーと称す)を介し現
像され、顕像化されてトナー像に変えられる。そしてこ
のトナー像は不図示の給紙系から搬送されてあくる転写
紙R上に転写帯電器4を介して転写される1次にトナー
像を相持する転写紙Rは不図示の定着器の方へ送られ、
このトナー像が転写紙R上に永久像として定着されると
共に、転写の終了した感光トラム1はクリーニング器5
によりその残留トナーがクリーニングされ、以降同様な
作業かくつかえあされて順次転写紙R上に画像が形成さ
れる。
First, an outline of image formation by a copying machine will be explained with reference to FIG. 1. In the figure, 1 is a photosensitive drum which is an image bearing member, and around the photosensitive drum 1 are primary chargers 2. Developing device f3. Transfer charger4. A cleaning device 5 is provided. That is, when image light from a document (not shown) is exposed onto the photosensitive drum l uniformly charged by the primary charger 2, an electrostatic latent image is formed on the photosensitive drum 1 due to the image light. Ru. The electrostatic latent image moves toward the developing device 3 as the photosensitive drum l rotates, and is developed through the developer (magnetic toner containing a magnetic material, hereinafter referred to as toner) in the developing device 3. The image is visualized and turned into a toner image. This toner image is transferred from a paper feed system (not shown) onto a transfer paper R via a transfer charger 4. The transfer paper R carrying the primary toner image is transferred to a fixing device (not shown). sent to
This toner image is fixed as a permanent image on the transfer paper R, and the photosensitive tram 1 after the transfer is transferred to a cleaning device 5.
The residual toner is cleaned, and images are sequentially formed on the transfer paper R by performing similar operations.

ここで前記現像装置3は内部にトナーを有する現像器本
体3aと、該現像器本体3a内に収容され、当該現像器
本体3a内のトナーを感光トラムlの方へ供給して該感
光トラムl上の静電潜像をトナー像に変える現像スリー
ブlO等とから構成されている。該現像スリーブlOは
現像器本体3aから外方へ露出する部分が感光ドラム近
接して配設されており、現像器本体3a内のトナーをこ
の感光トラムlとの近接部10aまで移動させて該感光
ドラムの静電潜像に吸着させるものである。
Here, the developing device 3 includes a developing device main body 3a having toner therein, and is housed within the developing device main body 3a, and supplies the toner in the developing device main body 3a toward the photosensitive tram l. It is composed of a developing sleeve 10, etc., which converts the electrostatic latent image on the top into a toner image. The developing sleeve lO has a portion exposed outwardly from the developing device main body 3a disposed close to the photosensitive drum, and moves the toner in the developing device main body 3a to the proximal portion 10a to the photosensitive tram l. It is made to adhere to the electrostatic latent image on the photosensitive drum.

さて1次に第2図乃至第6図に基づき、現像スリーブl
Oによるトナーの搬送機構について説明する。
First, based on Figures 2 to 6, the developing sleeve l
The toner transport mechanism using O will be explained.

t14P図は現像スリーブlOの断面を概念的に示した
図であり、非磁性材よりなる薄肉円筒部材11の内面に
は外側に第1電機子コイル12が内側に第2電機子コイ
ル13が配設されている。第1、第2電機子コイル12
.13はそれぞれ所定のコアに巻線された22個(Pは
正の整数であり1本実施例の場合P−9である)、即ち
18個の単コイルa又はbが円筒部材11の周方向に等
間隔に配設されたものであり、各車コイルa(又はb)
は交互に逆極性の磁界を発生させるべく電気的に接続さ
れている。
Figure t14P is a diagram conceptually showing a cross section of the developing sleeve IO, in which a first armature coil 12 is arranged on the outside and a second armature coil 13 is arranged on the inside of the thin cylindrical member 11 made of a non-magnetic material. It is set up. First and second armature coils 12
.. 13 are 22 single coils (P is a positive integer and is P-9 in the case of this embodiment) each wound around a predetermined core, that is, 18 single coils a or b are wound in the circumferential direction of the cylindrical member 11. The coils a (or b) of each car are arranged at equal intervals.
are electrically connected to alternately generate magnetic fields of opposite polarity.

即ち2つの磁極なN、Sで示すと1例えば第1電機子コ
イル12の奇数番の単コイルal+83+・”allが
円筒部材11の半径方向外方部側にNの磁極を発生させ
た場合、偶数番の単コイルa、、a、、・・mal@は
円筒部材11の半径方向外方部側にSの磁極を発生させ
、同様に第2電機子コイルの奇数番の単コイルb、、b
3.・・・b17が円筒部材11の半径方向外方部側に
Nの磁極を発生させた場合、偶数番の単コイルba、b
4.・・・b18は円筒部材11の半径方向外方部側に
Sの磁極を発生させることとなる。
That is, if two magnetic poles, N and S, are represented by 1, for example, the odd-numbered single coil al+83+・"all of the first armature coil 12 generates N magnetic poles on the radially outer side of the cylindrical member 11, The even-numbered single coils a,,a,...mal@ generate magnetic poles S on the radially outer side of the cylindrical member 11, and similarly the odd-numbered single coils b,... b
3. ...If b17 generates N magnetic poles on the radially outer side of the cylindrical member 11, even numbered single coils ba, b
4. ...b18 generates a magnetic pole of S on the radially outer side of the cylindrical member 11.

また第1電機子コイル12と第2電機子コイル13とは
互いに単コイルa(又はb)の半ピッチ分たけ、即ち電
気角で90度分だけずらして配設されている。
Further, the first armature coil 12 and the second armature coil 13 are arranged to be shifted from each other by half the pitch of the single coil a (or b), that is, by 90 degrees in electrical angle.

ここで第1電機子コイル12の各単コイル3間の電気的
接続方法を第3図により説明すれば、単コイルa14の
右側から流入し、その左側から流出した電流は単コイル
aSSの左側に流入し、その右側から流出する如く単コ
イルa13と単コイルa14は電気的に接続されている
。以降能の単コイルa1.・・・も同様に接続され、最
終的に単コイルa4の右端から電流が流出するようにな
っており、単コイルa 14+ a 11の各右端が電
源の入力端子Paとなっている。従って該入力端子Pa
に交流電流を通電すれば隣接する各単コイルaの磁界は
互いに逆極性となる。尚、pbは第2電機子コイル13
の電源の入力端子であり、この第2電機子コイル13の
各単コイル5間の電気的な接続も前記・第1tJm子コ
イルのものと同様になつているものとする。
Here, to explain the electrical connection method between each single coil 3 of the first armature coil 12 with reference to FIG. 3, the current flows in from the right side of the single coil a14 and flows out from the left side of the single coil aSS. The single coil a13 and the single coil a14 are electrically connected so that the current flows in and flows out from the right side. Single coil a1. ... are connected in the same way, so that the current finally flows out from the right end of the single coil a4, and the right ends of each of the single coils a14+a11 serve as input terminals Pa of the power supply. Therefore, the input terminal Pa
When an alternating current is applied to the coils, the magnetic fields of the adjacent single coils a have opposite polarities. In addition, pb is the second armature coil 13
It is assumed that the electrical connection between each single coil 5 of this second armature coil 13 is the same as that of the first tJm child coil.

尚、以上の説明では第1、第2電機子コイル12.13
の各単コイルa、bが互いに直列に接続されている場合
について説明したが、これに限る必要はなく、各単コイ
ルa又はbを並列に接続してもよく、また何個かの単コ
イルa又はbを直列に接続し、これ等を並列に接続する
等、種々の接続方法が可能であり、これ等は使用電源電
圧とコイルのインダクタンスとのバランスにより選定さ
れる。
In addition, in the above explanation, the first and second armature coils 12, 13
Although the case where the single coils a and b are connected in series has been described, it is not limited to this, and each single coil a or b may be connected in parallel, or several single coils may be connected in parallel. Various connection methods are possible, such as connecting a or b in series and connecting them in parallel, and these are selected depending on the balance between the power supply voltage used and the inductance of the coil.

また第1、第2電機子コイル12.13には第5図で示
される如く、それぞれ位相が90度ずれた周波数fの交
流電流、即ちIcos2πft。
Further, as shown in FIG. 5, the first and second armature coils 12 and 13 are supplied with alternating currents having a frequency f whose phases are shifted by 90 degrees, that is, Icos2πft.

l5in2πftを供給する必要があるが、これは第4
図で示される如く電源20と第1、第2電機子コイル1
2.13の電源の入力端子Pa。
It is necessary to supply l5in2πft, which is the fourth
As shown in the figure, a power supply 20 and first and second armature coils 1
2.13 power supply input terminal Pa.

pb間に駆動回路21を接続することにより実現される
This is realized by connecting the drive circuit 21 between pb and pb.

第6図はこの駆動回路21の一例を示すもので、21A
は周知のCR発信回路でCI+ Ct *r 11 r
 2は発信周波数を決めるコンデンサ及び電気抵抗であ
り、それぞれの容量及び抵抗を(: 1 * Cw +
 r I+ r 2とすれば1発信周波数fは、 で表わされる。尚、V ccは電源の電圧であり、A1
はオペアンプである。また21BはCR発信回路21A
で発生した周波Ifの交流電流から90度位相のずれた
2相の交流電流をつくり出す回路であり、コンデンサC
3により90度位相のずれた交流電流を発生させている
。尚、A2はバッファアンプ用のオペアンプであり、2
1a。
FIG. 6 shows an example of this drive circuit 21.
is a well-known CR oscillation circuit, CI+ Ct *r 11 r
2 is a capacitor and electric resistance that determine the oscillation frequency, and their respective capacitance and resistance are (: 1 * Cw +
If r I+ r 2, one oscillation frequency f is expressed as follows. Note that Vcc is the voltage of the power supply, and A1
is an operational amplifier. Also, 21B is the CR transmitting circuit 21A
This is a circuit that creates two-phase alternating current with a phase shift of 90 degrees from the alternating current of frequency If generated by capacitor C.
3 generates alternating currents with a phase shift of 90 degrees. In addition, A2 is an operational amplifier for a buffer amplifier, and 2
1a.

21bは第1.第2電機子コイル12.13の電源の入
力端子P−,Pbに接続される出力端子である。
21b is the first. This is an output terminal connected to the input terminals P- and Pb of the power source of the second armature coil 12.13.

次に第1.第2電機子コイル12.13の作用について
説明する。
Next, the first. The action of the second armature coil 12.13 will be explained.

第1.第2電機子コイル12.13にそれぞれ゛位相が
90度ずれた周波数fの交流電流が通電されると、第1
、第2電機子コイル12.13の回りに回転磁界か発生
すれが、以下このことを式て説明する。
1st. When an alternating current with a frequency f whose phase is shifted by 90 degrees is applied to the second armature coils 12 and 13, the first
, a rotating magnetic field is generated around the second armature coil 12, 13. This will be explained below using a formula.

まず第1電機子コイル12に単位電流を流した場合1円
筒部材11の半径方向に生じる磁界Haは単コイルaの
数を2P、所定位置からの円筒部材11の外周面に沿つ
た周方向角度をθ(第2図参照)、定数をHvとすれば
First, when a unit current is passed through the first armature coil 12, the magnetic field Ha generated in the radial direction of the cylindrical member 11 is determined by the number of single coils a being 2P, and the circumferential angle along the outer peripheral surface of the cylindrical member 11 from a predetermined position. Let θ (see Figure 2) and the constant be Hv.

HaxHv−sinPθ で示される。また第2電機子コイル13に単位電流を流
した場合、円筒部材11の半径方向に生じる磁界Hbも
、上記と同様に HbwHv−cosPθ で示される。
It is expressed as HaxHv-sinPθ. Further, when a unit current is passed through the second armature coil 13, the magnetic field Hb generated in the radial direction of the cylindrical member 11 is also expressed as HbwHv-cosPθ as described above.

次に以上の第1、第2電機子コイル12.13にIco
s2wft、Isin2wftの90度位相の異なる2
相の交流電流をそれぞれ通電すると、第1.第2電機子
コイル12.13による合成磁界Hは。
Next, Ico is applied to the above first and second armature coils 12 and 13.
s2wft, Isin2wft with 90 degree phase difference
When the alternating current of each phase is applied, the first. The composite magnetic field H due to the second armature coil 12.13 is:

HwHalcos2wft +)lb−1sin 2πft mHv 争 1 −5in(Pθ+2πft)となり1
合成磁界Hは2個の正弦波が周波数fでθの方向に進行
する交番回転磁界となる。尚Iは交流電流の振幅である
HwHalcos2wft +) lb-1sin 2πft mHv 1 -5in(Pθ+2πft) becomes 1
The composite magnetic field H is an alternating rotating magnetic field in which two sine waves advance in the direction of θ at a frequency f. Note that I is the amplitude of the alternating current.

従って本現像スリーブlOにおいても円筒部材11の外
周面上に回転磁界を発生させることができるため、第1
2図の従来技術で示される如く。
Therefore, in the present developing sleeve 1O as well, it is possible to generate a rotating magnetic field on the outer peripheral surface of the cylindrical member 11.
As shown in the prior art of FIG.

この円筒部材11の周方向にトナーを移動させて、該ト
ナーにより感光トラムlの上静電潜像の現像ができるこ
ととなる。
By moving the toner in the circumferential direction of the cylindrical member 11, the electrostatic latent image on the photosensitive tram l can be developed with the toner.

以上の如く、第1.第2電機子コイル12゜13に90
度位相のずれた交流電流を流すことにより円筒部材11
の外周面上に回転磁界を発生させることができるため、
従来の如く円筒部材11内で永久磁石を機械的に回転さ
せる必要がなく、永久磁石に対する軸受装置や、永久磁
石回転用のモータやベルト又は減速機が不要となり、構
造が単純化すると共に、従来の如く永久磁石等に起因・
する回転騒音は全く生じなくなる。
As mentioned above, the first. 2nd armature coil 12° 13 to 90
The cylindrical member 11 is
A rotating magnetic field can be generated on the outer circumferential surface of the
There is no need to mechanically rotate the permanent magnet within the cylindrical member 11 as in the past, and there is no need for a bearing device for the permanent magnet, a motor, a belt, or a speed reducer for rotating the permanent magnet. Due to permanent magnets etc.
No rotational noise occurs at all.

次に第1、第2電機子コイル12.13の具体的構成を
第7図乃至第9図により説明する。
Next, the specific structure of the first and second armature coils 12, 13 will be explained with reference to FIGS. 7 to 9.

第7図は集中巻タイプの第1、第2電機子コイル12.
13を示しており、30は積層鉄心よりなるコアであり
2該コア30の外周部にはその周方向に等間隔に4P個
(この場合P=5であるから4P−20となる)の突極
30−1.・・・か形成されている。該突極30−1.
・・・にはコイル31、・・・が各々集中巻されて単コ
イルa、bが形成されているが、図示の如く1つおきの
単コイル”I e at 1 fa211116によっ
て第11141子コイル12が構成され、これらの単コ
イルal + a2 +a、・・・は互いに隣りあう単
コイル(例えばa、に対してa8)が逆極性の磁界を発
生するよう、即ち電気角で180度ずれるように電気的
に接続されている。また第1電機子コイル12の単コイ
ルal t at l aツ・・・間には第2電橡子コ
イル13の単コイルb+ 、b* 、b3・・・が配設
され、該単コイルbも互いに隣り合う拳コイル(例えば
blに対してbiが逆極性の磁界を発生するよう、即ち
電気角で180度ずれるよう電気的に接続されている。
FIG. 7 shows the concentrated winding type first and second armature coils 12.
13, 30 is a core made of a laminated iron core, and 2 The outer periphery of the core 30 has 4P protrusions (in this case, P=5, so 4P-20) at equal intervals in the circumferential direction. pole 30-1. ...is formed. The salient pole 30-1.
, coils 31, . are constructed, and these single coils al + a2 + a, ... are arranged so that the adjacent single coils (for example, a8 for a) generate magnetic fields of opposite polarity, that is, they are shifted by 180 degrees in electrical angle. The single coils b+, b*, b3, etc. of the second armature coil 13 are electrically connected between them. The single coils b are also electrically connected so that the adjacent fist coils (for example, bi generate a magnetic field of opposite polarity to bl, that is, are shifted by 180 degrees in electrical angle).

更に隣り合う単コイルa、bは電気角で90度ずれるよ
うに電気的に位置決めされている。
Further, adjacent single coils a and b are electrically positioned so as to be shifted by 90 degrees in electrical angle.

即ち2つの磁極なN、Sで示せば、各単コイルa、bの
外端部側には図示の如く、例えば単コイル&、かう時計
回りにN 、I Nh I Ss * Sb +N、、
Nb 、・・・の磁極が発生しているが、隣り合う第1
電機子コイル12の単コイルaと第2電機子コイル13
の単コイルbとは電気角で90度だけずれた状態て配設
されているため、前記NaとNb、NbとSa、Saと
s b 、 −・・とにはそれぞれ電気角で90度の差
があることとなる。従ってかがるW41、第2電機子コ
イル12.13に90度位相の異なる交流電流を通電す
れば、第1、第2電機子コイル12.13により回転磁
界を発生させることがてきることとなる。
That is, if the two magnetic poles are N and S, then on the outer end side of each single coil a and b, for example, as shown in the figure, there is a single coil &, clockwise like this, N, I Nh I Ss * Sb + N, etc.
Nb,... magnetic poles are generated, but the adjacent first
Single coil a of armature coil 12 and second armature coil 13
Since the single coil b is arranged to be deviated from the single coil b by 90 degrees in electrical angle, Na and Nb, Nb and Sa, Sa and s b, -... are each separated by 90 degrees in electrical angle. There will be a difference. Therefore, if alternating currents with a phase difference of 90 degrees are applied to the second armature coil 12.13, a rotating magnetic field can be generated by the first and second armature coils 12.13. Become.

第8図は分布巻きタイプの第1、第2電機子コイル12
.13を示しており、コア30は第7ry1のものと同
様に20個の突極30−1.・・・を有しているが、コ
イル31.・・・は隣り合う突極3〇−1、−・・にま
たがって巻回されている。即ち例えば第1電機子コイル
12の単コイルa□は突極30−1と30−2とにわた
ってコイル31が巻回され、単コイルa、は突極30−
2と30−3とにわたってコイル31が巻回される如く
配設されており、また第2電機子コイル13の単コイル
b1は突極30−2と30−3にわたってコイル31が
巻回され、単コイルb2は突極30−4と30−5とに
わたってコイル31が巻回される如く配設されている。
Figure 8 shows the first and second armature coils 12 of the distributed winding type.
.. 13, and the core 30 has 20 salient poles 30-1. ..., but the coil 31. ... is wound across adjacent salient poles 30-1, -.... That is, for example, in the single coil a□ of the first armature coil 12, the coil 31 is wound around the salient poles 30-1 and 30-2, and the single coil a is wound around the salient poles 30-1 and 30-2.
The coil 31 is wound around the salient poles 30-2 and 30-3, and the single coil b1 of the second armature coil 13 has the coil 31 wound around the salient poles 30-2 and 30-3. The single coil b2 is arranged so that the coil 31 is wound across the salient poles 30-4 and 30-5.

即ち例えば単コイルa、とす、とは突極30−2を共有
しており、第1.第2電機子コイル12.13はいわゆ
る分布巻の電機子を構成していることとなる。かかる場
合においても、第1電機子コイル12の隣り合う各単コ
イルal。
That is, for example, the single coils a and A share the salient pole 30-2, and the first. The second armature coils 12 and 13 constitute a so-called distributed winding armature. Even in such a case, each adjacent single coil al of the first armature coil 12.

@ * 、 6mmを電気角で180度ずれるようおの
おの電気的に接続し、同様に第2電機子コイル13の隣
り合う各単コイルb+ * b* * ””も電気角で
180度ずれるように電気的に接続することにより、第
7図で示した集中巻の第1、第2電機子コイル12.1
3と同様な機能を発揮させることができる。
@ * , 6 mm are electrically connected to each other so that they are shifted by 180 degrees in electrical angle, and similarly, each adjacent single coil b+ * b * * "" of the second armature coil 13 is also electrically connected so that they are shifted by 180 degrees in electrical angle. By connecting the concentrated winding first and second armature coils 12.1 shown in FIG.
It can perform the same function as 3.

また第9図は波巻きタイプの第1、第2電機子コイル1
2.13を示しており、かかるものにおいても、集中巻
5分布巻のものと全く同様の機能を有している。
Fig. 9 shows the wave-wound type first and second armature coils 1.
2.13, and this type also has exactly the same function as the one with 5 concentrated windings and distributed winding.

さて1以上の説明では2相の交流電流を供給する場合の
電機子コイルについて説明したが、交番回転磁界を発生
させるには2相に限定されるわけではなく、3相、4相
と種々な構成が可能である。但し相数が多くなるに従っ
て駆動回路21の構成が複雑となり2円筒部材11回り
の磁極ピッチが大きくなって、同一円周上で得られる進
行波の波の数が少なくなるという欠点があるが、それだ
け良質の交番回転磁界が得られる。
Now, in the above explanation, we have explained the armature coil when supplying two-phase alternating current, but generating an alternating rotating magnetic field is not limited to two-phase, but various types such as three-phase and four-phase. Configurable. However, as the number of phases increases, the structure of the drive circuit 21 becomes more complex, and the pitch of the magnetic poles around the two cylindrical members 11 increases, resulting in a decrease in the number of traveling waves that can be obtained on the same circumference. The higher the quality of the alternating rotating magnetic field, the higher the quality of the alternating rotating magnetic field.

第10図は3相交流に対する集中巻の電機子コイルの具
体的構成を示しており、コア30中の3つおきの突極3
0−1・・・毎の単コイルa8、’a I + ””及
びす、、b、、−・・及びCI t Ct + ””を
それぞれ電気的に接続して第1、第2、第3電機子コイ
ル12,13.14を形成し、隣り合う単コイルa、b
、c間の電気角が120度となるようにしておけば、こ
の第1.第2.第3電機子コイル12,13.14に位
相が120度ずつ異なる3相交流を通電することにより
、第1゜第2.第3電機子コイル12,13.14回り
に交番回転磁界を発生させることができる。
FIG. 10 shows a specific configuration of a concentrated winding armature coil for three-phase alternating current, with every third salient pole 3 in the core 30
The single coils a8, 'a I + ``'' and s, b, -... and CI t Ct + ``'' of each 0-1... are electrically connected to the first, second, and Forming three armature coils 12, 13 and 14, adjacent single coils a and b
, c is set to 120 degrees, then this first . Second. By energizing the third armature coils 12, 13, and 14 with three-phase alternating current whose phases differ by 120 degrees, the first, second, and third armature coils are energized. An alternating rotating magnetic field can be generated around the third armature coils 12, 13, and 14.

また第11図は3相交流に対する分布巻の電機子コイル
の具体的構成を示すものであり、コア30中の3つの突
極30−1−・・に対してコイル31を巻回することに
より1つの単コイルa、又はb+又はclを形成するも
のであり、その他は2相交流の場合と同様であるので説
明は省略する。
FIG. 11 shows a specific configuration of a distributed winding armature coil for three-phase alternating current. By winding the coil 31 around the three salient poles 30-1 in the core 30, One single coil a, b+, or cl is formed, and the rest is the same as in the case of two-phase alternating current, so the explanation will be omitted.

尚以上の説明は電気写真法を採用する複写機を対象とし
て行なったが、本発明に係る現像装置は電子写真法に限
らず、単に静電潜像を磁性現像剤で現像するものであれ
ばどのようなものにでも適用できるのは勿論である。
Although the above explanation has been made with reference to a copying machine that uses electrophotography, the developing device according to the present invention is not limited to electrophotography, and can be used as long as it simply develops an electrostatic latent image with a magnetic developer. Of course, it can be applied to anything.

(発明の効果) 以上の説明で明らかな如く本発明によれば、2組又は3
組の電機子コイルに2相又は3相の交流電流を通電する
ことにより、多極着磁した永久磁石を等速回転させる場
合と同じ交番回転磁界を得ることができ、従来よりも簡
単な構成で2且つ低コストで回転騒音のない静かな現像
装置を提供できる。
(Effect of the invention) As is clear from the above explanation, according to the present invention, two or three sets of
By applying two-phase or three-phase alternating current to a set of armature coils, it is possible to obtain the same alternating rotating magnetic field as when rotating a multi-pole magnetized permanent magnet at a constant speed, and the configuration is simpler than the conventional one. 2, it is possible to provide a quiet developing device with no rotational noise at low cost.

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

第1図は複写機による画像形成を説明するための図、第
2図は現像スリーブの概念的断面図、第3図は電機子コ
イルの配線状態を示す図、第4図は電機子コイルへの電
源供給を説明する図、第5図は90度位相の異なる2つ
の交流電流の説明図、第6図は所定周波数て90度位相
の異なる交流電流を発生させる回路図、第7図は2組集
中巻の場合の第1.第2電機子コイルの説明図、第8図
は2組分布巻の場合の第1.第2電機子コイルの説明図
、第9図は2相波巻の場合の第1.第2電機子コイルの
説明図、第1θ図は3組集中巻の場合の第1.第2、第
3電機子コイルの説明図、1ul1図は3相分布巻の場
合の第1.第2.第3電機子コイルの説明図、第12図
は従来技術の説明図である。 l・・・感光ドラム(像担持体)、3−・・現像装置1
1・・・円筒部材(円筒)、12−・・第1電機子コイ
ル(第1の電機子コイル)、13・・・第2電機子コイ
ル(第2の電機子コイル)、14−・・第3電機子コイ
ル(第3の電機子コイル)、a、b、c・・・単コイル
。 特許出願人  キャノン株式会社 キャノン精機株式会社 代理人 弁理士    山  下  亮第4図 、10 第5図 第8図 第9図 j 第12図 第10図
Fig. 1 is a diagram for explaining image formation by a copying machine, Fig. 2 is a conceptual cross-sectional view of the developing sleeve, Fig. 3 is a diagram showing the wiring state of the armature coil, and Fig. 4 is a diagram showing the wiring state of the armature coil. Figure 5 is a diagram explaining two alternating currents with a phase difference of 90 degrees, Figure 6 is a circuit diagram for generating alternating currents with a phase difference of 90 degrees at a predetermined frequency, and Figure 7 is a diagram explaining the power supply of two AC currents with a phase difference of 90 degrees. First, in the case of group concentrated winding. An explanatory diagram of the second armature coil, FIG. 8 shows the first armature coil in the case of two sets of distributed winding. An explanatory diagram of the second armature coil, FIG. 9 shows the first armature coil in the case of two-phase wave winding. An explanatory diagram of the second armature coil, Fig. 1θ shows the first armature coil in the case of three sets of concentrated winding. An explanatory diagram of the second and third armature coils, Figure 1ul1 shows the first and third armature coils in the case of three-phase distributed winding. Second. An explanatory diagram of the third armature coil, FIG. 12 is an explanatory diagram of the prior art. l...Photosensitive drum (image carrier), 3-...Developing device 1
1... Cylindrical member (cylinder), 12-... First armature coil (first armature coil), 13... Second armature coil (second armature coil), 14-... Third armature coil (third armature coil), a, b, c... single coil. Patent Applicant Canon Co., Ltd. Canon Seiki Co., Ltd. Representative Patent Attorney Ryo Yamashita Figure 4, 10 Figure 5 Figure 8 Figure 9j Figure 12 Figure 10

Claims (4)

【特許請求の範囲】[Claims] (1)磁力により現像剤を移動させて像担持体上の静電
潜像を現像する現像装置において、像担持体に近接して
配設される非磁性材よりなる薄肉円筒の内部にP個の単
コイルからなる第1の電機子コイルと同じくP個の単コ
イルからなる第2の電機子コイルとをこの円筒の周方向
に互いに電気角を90度ずつずらせて交互に配設し、該
第1、第2の電機子コイルにそれぞれ90度位相の異な
る2相の交流電流を通電して前記円筒外周上に交番回転
磁界を発生させ、該回転磁界により円筒外周面に沿って
磁性現像剤を像担持体の方へ移動させることを特徴とす
る現像装置。
(1) In a developing device that develops an electrostatic latent image on an image carrier by moving a developer using magnetic force, a thin cylinder made of a non-magnetic material is disposed close to the image carrier. A first armature coil consisting of P single coils and a second armature coil similarly consisting of P single coils are arranged alternately in the circumferential direction of this cylinder with electrical angles shifted by 90 degrees from each other. A two-phase alternating current having a phase different by 90 degrees is applied to the first and second armature coils to generate an alternating rotating magnetic field on the outer periphery of the cylinder, and the rotating magnetic field causes the magnetic developer to move along the outer periphery of the cylinder. A developing device characterized in that it moves toward an image carrier.
(2)前記第1、第2の電機子コイルを、2P個の積層
突極磁心にそれぞれ集中巻されたP個ずつの単コイルか
らなる2組の電機子コイルから構成したことを特徴とす
る請求項1記載の現像装置。
(2) The first and second armature coils are comprised of two sets of armature coils each consisting of P single coils each concentratedly wound around 2P laminated salient pole magnetic cores. The developing device according to claim 1.
(3)前記第1、第2の電機子コイルを、4P個の積層
突極磁心の互いに隣り合う2つの突極にまたがって巻回
された分布巻の2P個ずつの単コイルからなる2組の電
機子コイルから構成したことを特徴とする請求項1記載
の現像装置。
(3) The first and second armature coils are two sets each consisting of 2P single coils with distributed winding wound across two adjacent salient poles of 4P laminated salient pole magnetic cores. 2. The developing device according to claim 1, comprising an armature coil.
(4)磁力により現像剤を移動させて像担持体上の静電
潜像を現像する現像装置において、像担持体に近接して
配設される非磁性材よりなる薄肉円筒の内部にそれぞれ
2P個ずつの単コイルからなる第1、第2、第3の電機
子コイルをこの円筒の周方向にその互いの単コイルが交
互に配設されると共に隣り合う単コイルの電気角が12
0度ずつずらされた状態で配設し、この第1、第2、第
3の電機子コイルにそれぞれ120度位相の異なる3相
の交流電流を通電して前記円筒外周上に交番回転磁界を
発生させ、該回転磁界により円筒外周面に沿って磁性現
像剤を像担持体の方へ移動されることを特徴とする現像
装置。
(4) In a developing device that develops an electrostatic latent image on an image carrier by moving a developer using magnetic force, each of the two pins is placed inside a thin cylinder made of a non-magnetic material disposed close to the image carrier. The first, second, and third armature coils each consisting of a single coil are arranged alternately in the circumferential direction of this cylinder, and the electrical angle between adjacent single coils is 12.
The first, second, and third armature coils are arranged so that they are shifted by 0 degrees, and three-phase alternating currents having a phase difference of 120 degrees are applied to the first, second, and third armature coils to create an alternating rotating magnetic field on the outer periphery of the cylinder. What is claimed is: 1. A developing device that generates a rotating magnetic field and moves a magnetic developer toward an image bearing member along an outer circumferential surface of a cylinder.
JP1087873A 1989-04-10 1989-04-10 Developing device Pending JPH02267576A (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
JP1087873A JPH02267576A (en) 1989-04-10 1989-04-10 Developing device

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
JP1087873A JPH02267576A (en) 1989-04-10 1989-04-10 Developing device

Publications (1)

Publication Number Publication Date
JPH02267576A true JPH02267576A (en) 1990-11-01

Family

ID=13926987

Family Applications (1)

Application Number Title Priority Date Filing Date
JP1087873A Pending JPH02267576A (en) 1989-04-10 1989-04-10 Developing device

Country Status (1)

Country Link
JP (1) JPH02267576A (en)

Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63202648U (en) * 1987-06-19 1988-12-27

Patent Citations (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPS63202648U (en) * 1987-06-19 1988-12-27

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