JPS5936271A - Conveyance device for solid-state particle - Google Patents
Conveyance device for solid-state particleInfo
- Publication number
- JPS5936271A JPS5936271A JP57147394A JP14739482A JPS5936271A JP S5936271 A JPS5936271 A JP S5936271A JP 57147394 A JP57147394 A JP 57147394A JP 14739482 A JP14739482 A JP 14739482A JP S5936271 A JPS5936271 A JP S5936271A
- Authority
- JP
- Japan
- Prior art keywords
- plate
- solid particles
- particles
- vibrating
- solid
- 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.)
- Granted
Links
Classifications
-
- G—PHYSICS
- G03—PHOTOGRAPHY; CINEMATOGRAPHY; ANALOGOUS TECHNIQUES USING WAVES OTHER THAN OPTICAL WAVES; ELECTROGRAPHY; HOLOGRAPHY
- G03G—ELECTROGRAPHY; ELECTROPHOTOGRAPHY; MAGNETOGRAPHY
- G03G15/00—Apparatus for electrographic processes using a charge pattern
- G03G15/06—Apparatus for electrographic processes using a charge pattern for developing
- G03G15/08—Apparatus for electrographic processes using a charge pattern for developing using a solid developer, e.g. powder developer
- G03G15/0822—Arrangements for preparing, mixing, supplying or dispensing developer
Landscapes
- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Dry Development In Electrophotography (AREA)
- Jigging Conveyors (AREA)
Abstract
Description
【発明の詳細な説明】
本発明は固体粒子を平板、ベルト、ドラム等の板状部材
表面上で搬送する装[K関する。DETAILED DESCRIPTION OF THE INVENTION The present invention relates to a device for conveying solid particles on the surface of a plate-shaped member such as a flat plate, belt, or drum.
固体粒子を板状部材上に乗せて搬送するという装置は、
例えば複写機における現像トナーを搬送する場合等、そ
の用途は広いのであるが、従来用いられていた搬送装置
としては、ベルトコンベアを用いるか、又は磁性体より
なる固体粒子を非磁性体板上に載置し、該非磁性体の下
面に摺接させた永久磁石の移動によって、固体粒子を搬
送するという装置が用いられていた。前記いずれの装置
によっても、搬送される固体粒子が均一の厚さにa置さ
れて搬送されるようにするためには、トリマーによって
可及的に均一にならす他はなく、また、トリマーによる
トリミングによっては、固体粒子の厚さは成る程度以上
厚くならざるを得なかった。A device that transports solid particles by placing them on a plate-like member is
For example, it has a wide range of uses, such as when transporting developed toner in a copying machine. Conventionally, the transport device used was a belt conveyor, or solid particles made of magnetic material were transferred onto a non-magnetic plate. A device has been used in which solid particles are transported by the movement of a permanent magnet placed on the non-magnetic material and brought into sliding contact with the lower surface of the non-magnetic material. In order for the solid particles to be conveyed to be conveyed with a uniform thickness in any of the above-mentioned devices, it is necessary to use a trimmer to make them as uniform as possible. In some cases, the thickness of the solid particles has to be increased to a certain extent.
ところが、例えば電子複写機等におけるトナー搬送装置
においては、搬送したトナーを感光体上の静電潜像に均
一に付着させるためにトナーを帯電させ、しかも板状部
材上に薄く、且つ均一の厚さに載置して搬送するという
装置が要望されるが、上記のとおり従来の搬送装置では
この要望に応えることは困難であった。However, in a toner conveying device such as an electronic copying machine, the toner is electrically charged in order to uniformly adhere the conveyed toner to an electrostatic latent image on a photoreceptor, and moreover, the toner is charged to a thin and uniform thickness on a plate-like member. There is a demand for a device that can place and transport a product, but as mentioned above, it has been difficult to meet this demand with conventional transport devices.
本発明は上記要望に応えるためになされたものであって
、導電体板上に籾電体層を設けて成る振動板を面方向に
振動させると共に、前記導電体板には各振動毎に極性の
異なる電圧を印加し、これに固体粒子を接触させること
によって該固体粒子を帯電させて誘電体層表面上を移動
させるようにした固体粒子の搬送装置を提供することを
目的とする。The present invention has been made in response to the above-mentioned needs, and includes vibrating a diaphragm comprising a rice grain electric layer on a conductive plate in a plane direction, and a polarity of the conductive plate for each vibration. An object of the present invention is to provide a solid particle conveying device in which the solid particles are charged and moved on the surface of a dielectric layer by applying different voltages and bringing the solid particles into contact with the applied voltages.
以下本発明を図面に基づいて詳細に説明する。The present invention will be explained in detail below based on the drawings.
關1図は本発明による固体粒子搬送の原理を説明する概
念図であって、先ず同図(a)に示すよに、導電体板l
土に導電体M2を設けて成る振動板3の誘電体層2の光
面に固体粒子4を乗せ、前記振動板3を矢印への方向に
振動させると、同図(b)に示すように、固体粒子4は
慣性により、元の位置に止まり、振動板3に対し相対的
に同図右方向に位置を移す。それと共に固体粒子4は誘
電体層2との摩擦により帯電するが、この場合鱈電体層
2と固体粒子4との材質の組合わせにより固体粒子4は
正・負いずれかの帯電を選択しうる。Figure 1 is a conceptual diagram explaining the principle of solid particle transport according to the present invention. First, as shown in Figure (a), a conductive plate l is
When solid particles 4 are placed on the optical surface of the dielectric layer 2 of the diaphragm 3, which is made by providing a conductor M2 on soil, and the diaphragm 3 is vibrated in the direction of the arrow, as shown in FIG. , the solid particles 4 remain at their original positions due to inertia, and move to the right in the figure relative to the diaphragm 3. At the same time, the solid particles 4 are charged by friction with the dielectric layer 2, but in this case, depending on the combination of the materials of the cod electric layer 2 and the solid particles 4, the solid particles 4 can be charged positively or negatively. sell.
仮に粒子を正帯電したとすれば次に同図(C)に示すよ
うに、前記振動板3を矢印Bの方向に振動させると共に
、前記導電体板IKはマイナスの電圧を印加すると、前
記によりプラス帯電した固体粒子4は、クーラン引力に
よって導電体板1に吸着されて該導電体板1に道線して
矢印B方向に移動する。次いで同図(d)に示すように
、前記導電体板lにプラスの電圧を印加すると共に再び
振動板3を矢印Aの方向に振動させると、前記固体粒子
4は前記振動板との接触圧が極小になるか又は浮上して
、慣性によりその位置に止まる。Assuming that the particles are positively charged, as shown in FIG. The positively charged solid particles 4 are attracted to the conductor plate 1 by the attractive force of the coolant and move along the conductor plate 1 in the direction of arrow B. Next, as shown in FIG. 4(d), when a positive voltage is applied to the conductor plate l and the diaphragm 3 is again vibrated in the direction of the arrow A, the solid particles 4 are caused by the contact pressure with the diaphragm. becomes minimum or floats up and stays in that position due to inertia.
以上の工程をくり返すことによって、振動板上に載置さ
れた固体粒子4はU電体層2表面上な−1図右方向に搬
送され乙ことになる。By repeating the above steps, the solid particles 4 placed on the diaphragm are transported on the surface of the U electric layer 2 in the -1 right direction in the figure.
前記において、固体粒子が移動するための条件を考察す
ると、
粒子と誘電体層とのJ91擦派数をμとし、粒子の質歓
をmとし、動力加速度をIとし、粒子の帝[1tZとし
、粒子と導電体板間の平均電界強度なEとし、粒子と誘
電体層間のファンデルワース力をωとし、右方向の振動
加速度をαとしたとき、固体粒子が誘電体層の振動に追
従する為の条件は、
μ(穆+zE+ω)>mα
を満たせばよいととにζなる。In the above, considering the conditions for solid particles to move, the J91 friction number between the particle and the dielectric layer is μ, the quality of the particle is m, the power acceleration is I, and the particle impeller [1tZ] , the average electric field strength between the particle and the conductive plate is E, the van der Waals force between the particle and the dielectric layer is ω, and the vibration acceleration in the right direction is α, then the solid particle follows the vibration of the dielectric layer. The conditions for this are ζ, as long as μ(穆+zE+ω)>mα is satisfied.
次に固体粒子がその位置に止まる(第1図dの状態)た
めの条件は、
左方向の振動加速度をlとすれば、
叩−zE +ω≦0
又はμ(叩−ZE+ωくmβ
を満たせばよいことになる。Next, the conditions for the solid particle to stop at that position (the state shown in Figure 1 d) are as follows: If the vibration acceleration in the left direction is l, then if the following equation is satisfied: It will be a good thing.
次に、前記のように振動板3を面方向に振動さ。Next, the diaphragm 3 is vibrated in the plane direction as described above.
せると共に、該振113の導電体板1に11各振動毎に
極性の異なる電圧を印加するための構成の一例を第2図
に示す。即ち、導電体板1上にIWlt体層2を付着し
た振動板3の一端に振動伝達部材5を介して永久磁石6
を取り付け、該永久磁石に)ノずかの間隙を介して電磁
石7を設け、該電磁石7には交流電源を接続する。FIG. 2 shows an example of a configuration for applying voltages of different polarities to the conductor plate 1 of the vibration 113 for each vibration. That is, a permanent magnet 6 is attached to one end of a diaphragm 3 on which an IWlt body layer 2 is attached on a conductor plate 1 via a vibration transmission member 5.
An electromagnet 7 is provided with a small gap between the permanent magnets, and an AC power source is connected to the electromagnets 7.
而して前記交流電源は前記導電体1とアースとにも接続
する。このように構成することによって、前記電磁石7
が永久磁石6を吸着して振動板3を同図左方に振動させ
た時には前記導電体1にはプラス又はマイナスのうち一
方の電圧が、また電磁石の極性が変って振動板3を同図
右方に振動させた時には前記導電体lにはプラス又はマ
イナスのうち前記とは反対の電圧が、交互に印加される
から、第1図で説明した原理によって誘電体層2上に載
置し又は接触させた固体粒子4は、前記誘電体層2の光
面な一方に搬送されることになるのである。The AC power source is also connected to the conductor 1 and ground. With this configuration, the electromagnet 7
When the permanent magnet 6 is attracted and the diaphragm 3 is vibrated to the left in the figure, one of the positive and negative voltages is applied to the conductor 1, and the polarity of the electromagnet is changed, causing the diaphragm 3 to vibrate to the left in the figure. When the conductor l is vibrated to the right, positive or negative voltages opposite to those described above are alternately applied to the conductor l, so it is placed on the dielectric layer 2 according to the principle explained in FIG. Alternatively, the solid particles 4 brought into contact are transported to one of the optical surfaces of the dielectric layer 2.
ここで前記U電体層2及び搬送される固体粒子4の材質
について述べると、−電体層としては例えばナイロンの
ように電気抵抗の高い材質が好都合である。一方搬送さ
れる固体粒子もポリエステル、アクリル、又はこれらの
混合物のよ5な′−電気抵抗高いものがよい。この場合
、同体粒子がプラスに帯電するかマイナス帯電するかは
、固体粒子と誘電体層との材質の組合わせによって定ま
る。Regarding the materials of the U-electroconductor layer 2 and the solid particles 4 to be transported, it is convenient for the -electroconductor layer to be made of a material with high electrical resistance, such as nylon. On the other hand, the solid particles to be conveyed are preferably made of polyester, acrylic, or a mixture thereof, which has a high electrical resistance. In this case, whether the solid particles are positively charged or negatively charged is determined by the combination of materials of the solid particles and the dielectric layer.
ところで、固体粒子の体積抵抗がlOΩ−α以上ある材
質を選んだ場合には、前記誘電体層を除去し導電体1と
兼ねることもできる。By the way, if a material whose solid particles have a volume resistivity of 1OΩ-α or more is selected, the dielectric layer can be removed to serve as the conductor 1.
本発明は上記のよ5に構成し且つ動作するから、振動板
3上に載置し又は接触させた固体粒子を帯電させたうえ
、前記振動板3上を薄く且つ均一の厚さで搬送すること
ができる。しかも搬送方向の変換は前記電磁石を用いる
場合にはその位相を反転させる等の方法によって容易に
行い得る。また振動板を水平でなく、所望の角度だけ傾
げて固体粒子を上り坂方向に搬送することも可能である
。そのための条件について考察すると、振動板を水平面
に対する角度eだけ傾か1させて固体粒子を上り坂方向
に搬送するためには、
μ(M9CO5θ+zE +trr ) > tn (
α十sing)の条件を満たせばよ(、また粒子がその
位置に止まるための条件は、
E/ sinθ〈βであって且つ
m9 CO5θ−zE+ω≦O
又はj! sinθ〈βであって且つ
μ(R9ωSθ−zE+ω)<m(β−5inθ)であ
れば良いことKなる。Since the present invention is configured and operates as described in 5 above, the solid particles placed on or in contact with the diaphragm 3 are charged and then conveyed on the diaphragm 3 with a thin and uniform thickness. be able to. Moreover, when the electromagnet is used, the conveyance direction can be easily changed by reversing its phase. It is also possible to transport the solid particles in an uphill direction by tilting the diaphragm at a desired angle instead of horizontally. Considering the conditions for this, in order to transport solid particles in an uphill direction by tilting the diaphragm by an angle e with respect to the horizontal plane, μ(M9CO5θ+zE +trr) > tn (
(Also, the conditions for the particle to stop at that position are: E/sinθ<β and m9 CO5θ−zE+ω≦O or j!sinθ<β and μ It is good if (R9ωSθ−zE+ω)<m(β−5inθ).
もちろん本発明は前記実施例K P!定される必要はな
いことは云うまでもない。Of course, the present invention is based on the above embodiment K P! Needless to say, there is no need for it to be specified.
例えば振動板の形状は平板に限らずドラム状等の曲面で
あってもよく、用途によってその形状な連木発明は以上
のように、固体粒子に帯電させた上で板状部材上に薄く
、しかも均一の厚さで搬送できるから、電子複写機の現
像用トナーの搬送装置としてはiFK理想的であるだけ
でなく、薬剤、顔料等を正確に所望の割合で混合するた
めの搬送装置等、広い用途が見込まれる。For example, the shape of the diaphragm is not limited to a flat plate, but may also be a curved surface such as a drum shape, depending on the application. Moreover, since it can be conveyed with a uniform thickness, iFK is not only ideal as a conveying device for developing toner in electronic copying machines, but also as a conveying device for mixing chemicals, pigments, etc. in an accurate desired ratio. It is expected to have a wide range of uses.
第1図は本発明による固体粒子搬送の原理説明のための
概念図、諸2図は振動板に′…、圧を印加し且つ振動を
与えるための一例を示す構成図である。
図中、1・・・導電体 2・・・訪電体層3・・
・振動板 4・・・固体粒子6・・・永久磁石
7・・・電磁石8・・・交流電源
出願人 富士ゼロックス株式会社FIG. 1 is a conceptual diagram for explaining the principle of transporting solid particles according to the present invention, and the two figures are configuration diagrams showing an example of applying pressure and vibration to a diaphragm. In the figure, 1... conductor 2... current visitor layer 3...
・Vibration plate 4...Solid particles 6...Permanent magnet
7...Electromagnet 8...AC power supply Applicant: Fuji Xerox Co., Ltd.
Claims (1)
動させると共に、前記導電体板には各振動毎に極性の異
なる電圧を印加することにより、前記糾電体層表面に接
触させる固体粒子を摩擦帯電させて前記綽電体層表面上
を移動させるようにした固体粒子の搬送装置。The surface of the conductive layer is vibrated in the plane direction by vibrating a diaphragm comprising a four-sided electric conductor plate and a voltage having a different polarity is applied to the conductive plate for each vibration. A conveying device for solid particles, wherein the solid particles brought into contact with are frictionally charged and moved on the surface of the electrolyte layer.
Priority Applications (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57147394A JPS5936271A (en) | 1982-08-24 | 1982-08-24 | Conveyance device for solid-state particle |
Applications Claiming Priority (1)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
JP57147394A JPS5936271A (en) | 1982-08-24 | 1982-08-24 | Conveyance device for solid-state particle |
Publications (2)
Publication Number | Publication Date |
---|---|
JPS5936271A true JPS5936271A (en) | 1984-02-28 |
JPH0325783B2 JPH0325783B2 (en) | 1991-04-08 |
Family
ID=15429274
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
JP57147394A Granted JPS5936271A (en) | 1982-08-24 | 1982-08-24 | Conveyance device for solid-state particle |
Country Status (1)
Country | Link |
---|---|
JP (1) | JPS5936271A (en) |
Cited By (1)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2015050138A1 (en) * | 2013-10-01 | 2015-04-09 | 住友理工株式会社 | Transport apparatus |
-
1982
- 1982-08-24 JP JP57147394A patent/JPS5936271A/en active Granted
Cited By (3)
Publication number | Priority date | Publication date | Assignee | Title |
---|---|---|---|---|
WO2015050138A1 (en) * | 2013-10-01 | 2015-04-09 | 住友理工株式会社 | Transport apparatus |
US9409719B2 (en) | 2013-10-01 | 2016-08-09 | Sumitomo Riko Company Limited | Conveying apparatus |
JPWO2015050138A1 (en) * | 2013-10-01 | 2017-03-09 | 住友理工株式会社 | Transport device |
Also Published As
Publication number | Publication date |
---|---|
JPH0325783B2 (en) | 1991-04-08 |
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