PRINT HEAD FOR ELECTROSTATIC PRINTING

Abstract: Print head for electrostatic printing of documents in accordance with the so called aperture matrix technique (DFC = Digital Control Filter) comprising means (14, 16, 17) for charging toner particles (2) with a certain polarity, a toner depositing matrix (3), which is provided with a number of toner depositing apertures (6), through which toner particles (2) are able to pass, means (5, 8) for controlling the deposit of toner particles to certain predetermined deposit positions, and means for feeding a document (7) to be printed below the toner deposit matrix (3). The means for charging the toner particles (2) with a certain polarity comprise two co-operating brushes, viz. a feeding brush (14) and a flipping brush (16) to bring the toner particles (2) to be charged by the fibres rubbing against the toner particles, and a flipper blade (17) is situated adjacent to the exit for the flipping brush (16), which blade flips toner particles (2) from the brush fibres (16a) so that there is created a cloud of charged toner particles (2), which are attracted against the aperture matrix (3, 4) and by electric attraction are controlled by an individual blocking field (4, 5, 10) for every aperture (6) in the aperture matrix (3), which blocking field is arranged to open and close, respectively, the toner deposit apertures (6) individually in an electric manner.

Description: PRINT HEAD FOR ELECTROSTATIC PRINTING Field of the invention This invention relates to a print head for electrostatic printing of documents in accordance with the so called aperture matrix technique, which usually is called DCF- technique being an abbreviation of Digital Control Filter technique, which print head includes means for charging of tuner particles with a certain polarity, a tuner depositing matrix which is provided with a plurality of apertures, trough which the toner particles can pass, means for controlling the deposit of tuner particles to certain specific depositing positions, and means for feeding a document, which in to be printed under the aperture matrix. Prior Art During approximately the last 10 to 15 years work has proceeded to simplify the so-called laser printer technique. Characteristic of his technique is that a digitalized pic- ture is applied on a rotating, light sensitive drum by means of digitalized light. Then different electrical levels on the drum surface will represent the picture, subsequently the picture is developed by electrically charged powder, and finally the picture is moved to the document by pressure transfer. Pressure and heat between a pair of rollers fix the digitalized picture now existing on the document . The characterising feature of this printing technique is that a pulverised dry ink is used, which generally is called a toner and is fixed to the documents by a fuse- pressure process, whereby the document is provided with an excellent durability for a long time and resistance to external influence by mechanical wear and moisture etc. The present simplifying proceedings is to eliminate the previous intermediate step of storing the picture on a drum, where it is developed and later moved to the docu- ment . This involves unnecessary costs due to additional components and an increased risk for distorting the digital information on its way from the computer to the state, in which is fixed on a document . The most recently developed laser printers provide a picture quality of 600 DPI (dots per inch) or better. To cover an A4 page with all possible dot positions 34 million positions are required at a resolution of 600 x 600 DPI. The problem is to find a technique by which it is possible to apply a powder dot in the shape of a small dot on the correct location on the document, when there are 34 million possibilities . The most successful technique during the last few years is to use a so-called "Digital Controlled Filter" (DCF) , henceforth called a matrix or an aperture matrix, comprising a row of small apertures in a thin foil. The apertures are opened or closed by application of an electrical volt- age, which generates a field that attracts the electrically charged powder to pass or not to pass through the apertures. On one side of the foil the document is situated, upon which the particles land, and on the other side of the foil the charged powder is situated on a conveyor. In most applications this conveyor consists of a roller with a thin layer of electrically charged powder. This technique was described for the first time in the US patent No. 3,689,935 to 'Pressman and Casanova in September 5, 1972. Several later patents disclose various improvements of the Pressman/Casanova patent, e.g. US patent No. 4,491,855 (Fuji/Ando - Canon from 1985), US patent No. 4,912,489 (Schmidlin - Xerox from 1990) and Swedish patent No. 8704883-1 (Ove Larsson - Array Printers from 1989) . The various improvement methods disclosed in these patents relate to how the electrical field around each aperture is appplied to obtain a more efficient transfer of the powder through the apertures down to the document . Problem 5 An aperture matrix may comprise a row of apertures covering the width of an A4 sheet, i.e. 210 mm or a row of 4960 apertures to create a 600 DPI print-out. The advantage with this type of aperture matrix is that printing can be done with continuous paper feed and with continuous fixing, and w in other words a continuous printing process is obtained. There are many problems connected with an aperture matrix being as wide as said 210 mm. is 1. If every aperture is connected with a drive circuit for the application of a voltage on a round electrode, which is arranged around the aperture, this involves several thousands ring electrodes, connection lines and drive circuits, and with increasing number of apertures in the aperture 0 matrix the probability increases for breakdown in any of these apertures, rings, connection lines or drive circuits. 2. If the control field for opening and closing the apertures in the aperture matrix is applied between ring elec- 5 trode and powder feed surface there is an additional problem, for the distance between the aperture matrix and the powder feed must have the magnitude of 0.1 to 0.15 mm, since available drive circuits can stand a maximum of 300 to 350 volt. Therefore this distance is not allowed to vary 0 more than 0.02-0.04 mm since the variation of the distance has an influence on the 'electrical filed, which in turn has an influence on the blackness of the printout . Since the aperture matrix is a thin foil it is very difficult to maintain a distance of 0.1 to 0.15 mm within the said tol- 5 erance between the aperture matrix an the powder feed surface over the entire width of an A4 sheet . 3. According to paragraph 2 drive circuits are required, which can stand at least 300 volts and preferably more, and such drive circuits in the form of integrated circuits are still too expensive, which creates a cost problem. The solution of the cost problem is to use lower voltage or fewer circuits. 4. A further problem is that there exists a certain percentage of powder, which not will be charged or charged to the opposite potential. This powder can not be controlled by electric control fields but will fly around without control or deposit on undesirable surfaces. Common types of printing powder will be electrically charged with negative potential, when the powder particles rub against some other suitable material. This rubbing is usually created in two ways, either with a rotating magnetic field in case the powder is provided with magnetite and a rotating magnetic brush is created, which rub the particles against a roller. In case the powder lacks magnetite a rotating brush or a foam rubber roller, which rotates against a steel roller, rubs the powder particles against this steel roller. In booth cases the correct amount of powder is dosed on the rotating steel roller by means of a flexible rubber blade. This dosing, called doctoring, has a grinding influence on the powder, and the disintegration of powder particles causes creation of particles, which are booth incorrectly charged and uncharged. The four main problems mentioned above are the reason for the fact that the technique mentioned above not yet has been any great commercial success, though it offers direct transfer of digital information from a computer to a document . The invention Our proposal is to use an aperture matrix comprising en isolating foil with a completely covering, electrically conducting surface on one side of the foil (called the base side) . On the other side of the foil there are a greater number of electrically conducting rings (called ring side) , each of which is formed around an aperture through the aperture matrix. Each ring is connected to a voltage source through a separate line to a control transistor. The base side of the foil has a common potential, since it has a completely covering, electrically conducting surface. According to the invention it is proposed that the electrically charged powder now is applied above the base side on the aperture matrix as a cloud of charged particles, which constantly are moving. This cloud is created in such a way, that toner which is situated in a toner container, is fed forwards by a feeding brush, which rotates clockwise (in the case shown in fig 2) with a low number of revolutions to correspond with the consumption of tuner in the printing process . Tangential to the feeding brush is a flipping brush, which rotates anticlockwise with a higher number of revolutions than the feeding brush. In the tangential point between these brushes stirring of the particles occur due to the difference in number of rotations between the brushes. The mission of the feeding brush is to control, dependent on its number of revolutions, that the amount of tuner in the flipping brush is on the right level in order to guarantee that the toner concentration in the toner cloud not varies due to variations of the amount of tuner in the flipping brush. To provide a negative charge of tuners, the fibres of either the flipping brush or in booth the feeding brush and the flipping brush consist of a material, which is tribo- electrically positive with respect to the toner. When the particles collide with the brush fibres in the moment of stirring, the fibres become positively charged and the Λ τ> ■ 4H 1 O 0 Φ !H to β 4H • H φ φ », -H 4-1 Di TJ Φ 1 β fd 0 4-1 A Φ rH JH β CO Λ 1 Φ φ β β β C o -H JH Λ >H 4-1 A A Φ Φ -rl CO CO ft 1 0 > TJ CO • H 4-1 4-1 β r © 0] Λ 4-1 ft β td 4-1 -rl o ft 4-1 fd φ β -H 0 CO -rl φ fd ft -H > -H 4-1 Φ o 0 • H • H φ ft β Φ CO β ft 0 4-1 u rH 4-1 rH 4-1 4-1 A ft Λ β β o ft Φ > H Φ rH X 0 UH β CO fd β β 0 A 4H πJ CO u -H 4-1 CO DI Φ 4H β W .β rd A "4H td Φ 0 0 0 4-1 -rl ft -rl φ Φ rH fd β td 0 4-1 t _ -. ε rd 4-1 4-> 4 A A TJ 4-1 ft cα Φ T> fd ft 01 Φ β X! CO β A 4H Λ ε td f3 αj φ rH CO 4-> φ Φ -rl .β rH ε β A O Φ β 4-1 4-1 A CQ 4-1 4H J υ cα 0 4-J ε β r-i 4-1 Φ CO TJ 4 :-J 01 ■ H 4J 0 ■ H JH 0 Φ 4-1 β o 4-1 4- ) id Φ -H φ T> • fd 4-1 Λ fd 0 o β ft CO Λ 1 u β A Φ 0 φ β 4 Φ 4-> a Λ • s 3 X 2 β 4J Φ TJ A 4-1 -rH ft 0 r-i £ -rl Φ 4-1 β X! A 0 4-1 J 01 _ 0 ■ s id 0 -rl 4-1 Φ CO .β β co 4-1 -rl 4J fd ε CO Φ 0 4J 4-1 ε β u μ 0 CO r-i rl • rt O 4-1 2 H fd Φ β H Φ -rl S 4H ■ H φ fd β Λ • H 4-1 τ_ s cα υ 4-1 cα fd 0 |χj o -rH 4H ΛJ TJ D O 4-1 0 4-1 0 TJ 0 t cα 4-1 0 β tτj Φ td Φ A Φ • A -H β SH U β β A Φ O 4-1 JH r-i Φ ε β CO 4 β id JH H n ε cα A 4-> β Φ CO JH fd ft Φ fd fd -H CO CO Λ CO Φ β 0 Φ A td 0 4-1 u φ -rl 4-1 Φ β β 4-> 4-1 . A Λ CO -H β φ -H 4-1 4-1 Λ rH OJ - cα -H β Φ 0 cn 0 fd TJ Φ 4J - β JH TJ JH • H Φ td φ 4 rH β - cα 4-1 o Λ ,β CO o N A ε O β A Φ TJ O A A r-i Λ TJ ΛJ ε ε CO A σ -rl β cα T> φ ri 4-1 β CO CD ε & 0 4-i 0 > Φ ! 03 Φ -H Ό fd • H fd 4-1 β > •H Φ JH A td 4-1 3 3 - o Φ 01 φ ε r-i 4J 0 Di β D -r| 4H A fd cα X -H 4-1 rH fd 4-1 ft CO n H O X ,β β IH -rl U β ε Λ JH β 4H U Λ 0 A ft cα β U S -H φ A JH -H s • H β -H X fd CO Λ -H Φ β Φ JH CO Λ ft Φ 0 • H Λ! *» A ft -β CO 4-1 ft 4 4-1 rl υ CO X! β ft td A 0) A ft β J •H rH u 4-> O φ φ 4-1 fd 01 4-1 4-1 rd ft 0 Φ TJ <d φ o Di ft 4J φ 4-1 ft JH TJ 1 r-i o H fd τ> β β fd Φ -H φ β Φ Λ u Λ β -H O Φ β fd Λ Φ 4- 4H ■ H rH (TJ JQ (TJ 0 β Φ -H O ε Φ ft rH ft CO 0 CO -H rH 4-1 TJ > 0 4H U U> 4-1 rH ft rH 4-1 A ft TJ XI fd 4H fd -rl 4-1 β Φ 0 rH Di ft 4H CO β fd 4-1 O 4-1 Φ β C Φ •rl CO A 4-1 ft β φ o 4H Φ β ft -H td A td Λ TJ T 1 Λ πJ s S φ • •H Φ M r-i φ Φ φ φ Φ 4-> β > ■ H -H Φ X TJ φ A 4-1 Φ J E-« ft Φ <d φ A TJ O rH 4-1 ti r-i A A A u A 0 β r- • H ft rH ,β Φ X r-i φ A 4-1 >H f Λ β JH Λ 4-> Φ n MH X, -H 4-1 4-1 4-1 β 4-1 β O fd 4J ft 4H 4-1 • H r-i D) 0 ■ • M CO 0 4-> 4-1 ε μ Φ 3Ϊ fd Λ O -H • H α> . .JH . td 4-1 0 4-1 J TJ 0 ) 3 4-) CO J*. fd Φ φ 4-1 4H 4H β Φ •rl ω r-i Φ 4H 4J A fd CQ CQ CQ 0 ) α 4H A 0 ? A A ft - 0 0 0 O -H β 0 4H Λ 0 Φ td CO Λ β CQ β Di 0 A A Φ 0 Φ 4H 0 4-1 U fd TJ -rl fd rH 0 ft 4-1 A ε U ε % β T V-l 4J 4 A 4J -H φ A Di -rl 4-J φ Φ CO 4-1 A Φ ε 4-1 r φ TJ rH rl Φ 4-1 4-1 TJ Φ A fd TJ 4-1 A (d 4-1 CO Λ 4-1 4H Φ rH >-. Φ ϋ β Λ Φ β £ D> • H CO td ■ ϊ A JH TJ φ • H O -H υ υ O -H 4J . fd fd >. Φ rH O 4-1 Φ o Λ ■ H CO TJ > Ό _ 0 • H X! CO -H CD ■ H -H Φ TJ A A Φ •rl Φ JH 0 Φ Λ 4 4-) ft τ> T) φ TJ in 4-1 *. 4-1 £ ft .β β A β r-i A 4H φ 4-1 CO σi 4-1 4H > 0 4H 4 J ft <D β •. β (d Φ β • H Φ En Φ S (d Φ υ 0 01 td -rl 4H rH TJ -H rH φ φ 4-1 O S 4-1 β -rl CO Φ CO TJ Λ ■ H 4-1 rH 4-1 φ CQ 4J Di OJ β rH rH A A A rH β β -rl -H H φ td • .. u 4H Λ Φ fd U fd rH D β φ ε ft -H fd 0 C > ITJ 4H • H 4-1 Di U > td rH φ -rl ft A ε >H CO Φ 0 ^ tJl A fd 0 td A Di β -H β JH • H 4-1 Λ •rl 0 4-1 β Λ 4-1 ε Φ φ ε TJ o 4H 4-1 t> 4-1 φ • rl ft β 4H t 4-1 (U Φ o CO td TJ Φ 0 u β φ φ β r-i CO >. φ β Φ β β ft 4-1 fd Di Λ CO • rl CO to φ 0 l N -H Φ Λ A to 0 U β Λ Φ Φ Φ A 5 JH -rl 4J 4 cn E-< £ Λ rd 4-1 β φ Q< J Λ 4-1 4-1 • 4-1 -H Φ rd cα φ r-i A U > 4-1 0 φ β r- 4H β fd tτj ? ft to 0 > ε β Φ 5 Φ o 4-1 Λ Φ β A Φ 4-1 ■ H ^ A 4-1 4H 0 O β Λ 4-1 Q • H Φ A β 4H 4-1 4-1 ε ^ 4-1 > Φ 4J 4H 4J Φ - -* o CO 4-> - CO Φ ε u - 4-1 φ 0 TJ O (d • H A • H 0 A -H 0 . Φ 4-1 s Di O φ Ss ε fd O 4-1 TJ φ φ Φ ft Φ co 4 4-1 4-1 to A CQ Λ β β ω Φ fd • α td 0 CO -rl φ l 3 rl s φ φ (H A 01 TJ -H O φ CO 4-1 CQ 4-1 β • rl •5 β > . Φ f u TJ Φ ε Φ 0 Φ 4-1 TJ u φ β CO Φ TJ ft TJ β 4H 0 ε • o 0 -H 4-) A rH 4 Φ β r- 4-1 fd ft r-i > Φ ■ rl X 0 A fd • rl rd 0 β β ■ H !H -H A CQ 4-) 4-) CO 4-1 Λ cα A fd υ H CO fd U 0 A CO Φ o EH ε 0 ε 0 O ft £ ft Q fd td CQ A rH H td fd υ •O o ι • ^ o O Ό o •o »N <N <» p_ the front edge of the brush housing surrounding the flipping brush, is preferably connected to the same positive voltage as the centre shaft of the flipping brush, so that tuner, which not manages to return to the brush, will get stuck there and successively is fed back into the brush. As an alternative proposal the centre shaft of the flipping brush is connected to en alternating voltage being 180° out of phase in relation to the printing process. When the apertures are open practically no toner is returned to the brush. When the apertures are closed, however, maximal amount of tuner is returned to the brush. This function is controlled by the computer card of the print unit, so that these fields are synchronised (see fig 3) . These toner particles will now follow the flipping brush back to the tangential point between the brushes, where the particles are mixed with new particles and recharged. Booth brushes are surrounded by a housing, which tightly fits around the periphery of the brushes. The reason for this is that toner, being fed forwards by the brushes, shall advance and that no tuner shall spatter out from the brushes due to centrifugal force when the brushes rotate. Thereby control is secured that all charged tuner will arrive in the proper place . The housings around the brushes also provide a possibility of changing the brushes when the toner container is changed. Thereby a new set of brushes will be provided every time the toner container is changed, and the risk of worn out and damaged brushes is reduced. On the ring side of the aperture matrix the document is situated, and under the document there is a back electrode, which is connected to a positive potential of 1000-2000 volts. Between this back electrode an the base side of the aperture matrix, which has the level of zero volt, there is formed an electric field, called the main field, through the apertures in the aperture matrix, and around the aper- ture edge on the base side of the aperture matrix an edge field will be formed. This edge field is directed in such a manner, that toner particles moving down through the aperture when the ring around the aperture on the aperture side is at zero volts. If the ring around the aperture is at minus 100-200 volts, the edge field gets the opposite direction, whereby a barrier field is created. The toner particles in the toner cloud are not able to move downwards through the apertures . The toner particles, which are located in or closely below the aperture, will now move upwards through the hole back into the toner cloud, and the aperture will be blocked for tuner in the cloud. If the ring is at zero volts, the main field will accordingly drive tuner from the cloud down through the aperture to the document, but if the ring has a negative potential of 100-200 volts the blocking field will block transport of tuner, and no tuner will pass through the aperture . The patent US-A-5 , 404 , 159 discloses an arrangement, by means of which printing is provided by a toner cloud. This prior art arrangement, however, is different from the present invention mainly through the way a stable tuner cloud is created: - in the present arrangement there is firstly used a feeding brush, the task of which is to feed a controlled amount of tuner to a flipping brush, so that the flipping brush receives the correct toner concentration to cerate a prerequisite for the correct toner concentration in the toner cloud; - the flipping brush is contacting the feeding brush to create a charge between the brush fibres of the flipping brush and the toner, so that toner shall stick to the brush fibres by electrical force; 4H J φ 0 TJ CO I X Φ Φ TJ © 0 4-1 Di 4-1 Φ id Φ rH CQ rH TJ β • H ε s τ> X! rH Φ -rH Φ Φ td • TJ D) Φ X! • H rH JH U 1 1 JH β 1 id β 4-> β β CQ ? JH 4-> H β Φ TJ 0 TJ • H DI -H td 0 0 M 4-J -H XJ JH CO © 0 0 Φ CQ β β β -H XJ Φ JH XI Φ 4H β TJ £ S TJ ft Φ CQ id rd cn CO β rH β X! rH Φ Φ TJ 4-1 4-1 πi TJ 4-1 4-1 φ 0 rH β ft Φ -H ε ε β CO υ φ r © © U 0 CQ β JH φ a JH > β CN U U JH Φ CQ Φ TJ 5 φ Φ td X! 0 td X! W TJ JH X β β fd Φ TJ 0 . Φ Φ φ XJ • H 4-1 ■ ri rH o XJ > 4-1 CQ Φ Φ JH ft φ 4-J • jβ JH β LO O rd υ 4-1 Di U ft fd rH CQ cn β rH XJ 4-1 X! 4H Φ TJ 4-1 ■ ri X • H XJ J XJ XJ 4 H Φ id 0. • H JH • H fd U Φ β Φ EH EH CQ • H 4-1 • H CO XJ 4-1 4-1 4J CN 4-1 β u TJ O O X! Φ CO Φ φ rH X 0 TJ TJ φ 4H φ 0 id JH X EH 0 ft. S in cn Φ XJ 4-1 ft φ X Φ XJ JH U -H u X • β • β DI > 4-1 DI 4-1 U β 0 β CQ T) 0 β JH 4-1 id TJ 4-1 XJ 4-1 Φ ■ JH υ CO fd so φ TJ Φ 0 Φ fd 0 • -H 4-J 3 Φ β CQ ft CO ■ H β • H fd 4-1 TJ 4-1 4-1 td 4-1 4-1 Φ DI ε β β ε r-i CQ 0 r-i td ■ H n JH 4-1 > Φ φ Φ CQ JH fd rH XI rH 00 φ X TJ s A Φ O β TJ Ό 4 φ β JH φ X! XI > Φ rd 0 fd ε rH 0 JH φ β Φ ε 0 td φ r-i rH 0 • H O X! • H rH Φ Φ > 4-1 0 > XJ ft ft fd rd > φ β td Φ TJ X! A υ ■ ri Φ 4-1 cn ■ 4-1 JH rH ft β rd JH 0 φ ε TJ 4-1 TJ CQ X! CQ 4-1 υ • H TJ ■U > JH Φ td rd o XJ β r-i ft XI CQ Φ JH JH CQ O 0 r-i T) -rl 4-J JH β ■ ri 4-1 rH td 0 id X JH β β TJ • H A ε td -H X! Φ β 0 -H o JH φ Φ β J Φ •H XI A JH Φ rH ε ft -H β -H Φ » r-i td -H X! 4-1 TJ 4-1 β o 4-J ft ■ ri id EH φ J td DI 5 id -H Φ JH 4-1 Φ <* r-i φ td O JH rH JH Φ CN O td 4H X 4-1 4-J β ft 4H β JH 4-1 JH J CN > fd XI ε Φ 0 4H 0 Φ CO JH 1 Φ - • td JH XI 0 •. td Φ td Φ 4-1 Φ O 4H 4-J TJ . 0 ft ft -H Φ o rH X β O ε β 0 JH o JH DI β υ TJ β β Φ φ β o td XJ o φ • H -H ε ft O Φ J TJ 4H X! H Φ β -H S id 4 Φ XI •H β td 0 JH JH CN 0 β TJ X 4-1 o JH id Φ φ TJ in 4-J β -H Q 0 Φ r-i CO fd u -H β ft rH rH φ o φ Φ -H H X 4-1 ε TJ JH β T) TJ β X β Φ ft JH Φ ' O JH 4-1 4-1 u JH • H Di X! 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JH 4-1 JH υ Φ υ β 4J Φ Φ 4-1 r 0 4-1 0 β 4-J • CO Φ XJ JH • H > Φ φ 0 Φ 4-1 4-1 JH φ β 4-J 0 ζj id 4-1 TJ • m 4-1 β 4-J 4-1 fd • ε β 4-1 4-1 4H 4-1 0 ft φ s -H id td ft TJ fd rH 0 XJ •rl • s ID β Φ JH rH β =L φ β td 0 fd ε td XJ td 4-1 fd 4H 0 ε ft fd β Φ XI TJ 4-1 CO 0 •rH Di TJ > VD Φ 0 0 CO β ε ε D 4-1 Φ 4-1 0 JH 0 ft φ β Φ Φ ft CQ -H U1 td 4H 0 φ φ H Φ CQ XI • ** β Φ JH X υ U Φ 4-1 4-1 ft JH VO • H 4 Di JH CQ td -H 4-J H XI Φ φ β XJ JH β • H ft X! Φ ■ H 1 XJ CQ U ft 0 β JH JH ft Φ td 1 Di 4H XJ JH TJ 4-J Φ • H TJ Φ rd β 4-1 TJ JH 4-1 CO 4-1 β id 0 β 4-1 Φ C fd JH Φ rH in Φ β 4-1 Dl .— - β TJ rd φ TJ ε 15 4-1 β ■ H -H 4H JH H Di t X! 0 β X! r-i 0 XJ -H CN Φ SN 0 4H β 4-1 4-1 • H O TJ 0 td Φ TJ rd CO ■ s Φ β β υ 4-1 4-J 4-1 rH CQ >s 4-1 TJ 0 TJ rH r-i O O β td cα Φ ϋ a ε JH Φ φ Di Φ td 0 ft 4-1 -H r JH td -H rH Φ CQ 4-1 rH υ • H φ XJ φ β JH JH H td XJ x! β td 4 Φ Φ 4H υ Φ β Φ Φ β JH td • rd JH Φ 4-> JH 0 Φ Φ β Φ r-i 4-1 Φ u X! Φ ft 0 -H JH 4-1 0 4H rH -H Φ JH co ε U CO β XJ XJ O XJ td V£> so TJ X ft β 4-1 TJ id JH id id υ 4-1 Φ φ Φ 4-1 td TJ 4-1 fd 4-1 4-1 4-> υ β • H td TJ r Φ 4-1 rH ε cn U -H cn 4-1 β J TJ rH X! CQ XI Φ JH Φ Φ A Φ id JH β 4-i 0 XJ TJ U -H -H Φ 4-1 Φ Φ • ϊ • H 0 o • H rH Φ J 4-J J • XJ rH .. JH JH 4-J β u H o Di ■ H Φ ε X X ft J X XI Di 0 CQ > -H Φ rH ft Φ u D f- 4-1 td so β TJ β -. fd rd o td β β CO r-i • H 0 -H & fd • H ft J TJ XJ td td 4-1 (d β ■ H 4-1 Φ 4-1 TJ JH H 0 ε 1 t -* Di Φ CO JH JH β ft JH fd Φ 0 β 4-1 φ JH CO H rH JH 4-1 4 ■ 5 4-1 JH β ft 4-1 4-1 Φ Φ CQ H s rH 4-1 u fd JH O 4-1 Φ Φ Φ 4-1 JH β Φ β JH Φ β Φ Φ Φ Φ β r © 4-1 • XJ -H Φ JH ft td β 4H fd 4H J J td Φ - -H β CQ XJ JH 4-1 X! Φ J Φ β ft rd ft • H XJ > Φ o td H 4-1 JH XI 0 td ε fd 0 ε 0 H 4-J A N 00 4H 0 -H 4-1 υ td 4 ε -5 4-1 4-1 td O id 4H 4-1 0 JH o l o •o <N between the ring 5 and the base side 4. Between the base side 4 and the back electrode 8 there is then created a field trough the aperture 6, called the main field 9. This field is strong enough to move the negatively charged pow- der particles from the powder cloud 1 down to the document 7. Figure 2 shows an embodiment of a mechanical powder feeder, charger and cloud creator. The arrangement comprises a feeding brush 14, which is mounted adjacent to the orifice of a powder container 15 and rotates clockwise while slowly feeding new toner powder 2 with the same rate as the toner powder is consumed by the print process. The feeding brush is enclosed in a housing 15a in order to feed toner emitted from the toner container 15. A flipping brush 16 in mounted so that it is contacting the feeding brush 14 , but it rotates with a much higher periph- eral speed than the feeding brush 14 and in anticlockwise direction. At the contact between the feeding brush 14 and the flipping brush 16 the powder particles 2 will rub against the brush fibres 16a of the flipping brush 16. These brush fibres 16a must be made of a material which tribo-electrically gives the fibres a positive charge and the toner a negative charge. Then the negatively charged particles 2 will stick on the positively charged straws 16a of the flipping brush 16. The brush arrangement also comprises a flipper blade 17. When the straws 16a of the flipping brush 16 with the powder particles 2 arrive to the flipper blade 17, the straws are bent backwards, and when the straw tip passes the flipper blade 17, the straw flips and throws the negatively charged powder particles 2 down towards the surface of the aperture matrix. It is essential that the flipping brush 16 is arranged in the centre of the aperture zone 6 and that the distance between the brush 16 and the upper side of the aperture matrix 3 does not exceed 0,5 mm. The flipping brush 16 is enclosed in a housing 15b to secure that all toner in the flipping brush 16 is fed to the flipper blade 17 to secure that the concentration of tuner is maintained stable in the powder cloud 1. In that way there is created a cloud 1 of powder above the aperture matrix 3, which cloud is floating above the aperture zone 6 of the aperture matrix 3. Owing to the positioning of the flipping brush 16 in rela- tion to the aperture zone 6, and owing to the fact that both the feeding brush 14 and the flipping brush 16 are enclosed in housings 15a and 15b, respectively, it is ensured that the tuner concentration in the toner cloud is uniform over the entire aperture zone 6. To ensure a stable toner concentration in the powder cloud 1 the central shaft of the brush and the front edge 15c of the brush housing 15b are connected to an electrically positive voltage level 18. Due to the fact that an electrical field is created between the flipping brush 16 and the upper side 4 of the aperture matrix 3, which field has such direction that toner, which not has been fed down through the matrix apertures 6, will be returned to the flipping brush 16 and also to the front edge 15c of the brush housing 15b, where the straws 16 can capture the toner and bring it back to the contact point between the feeding brush 14 and the flipping brush 16 for recharging the particles. In figure 3 there is shown an alternative arrangement for voltage excitation of the flipping brush 16. The voltage unit 19 provides an alternating voltage to the flipping brush 16, so that the field, which lifts tuner back to the flipping brush 16, has a maximum value when all of the apertures in the aperture matrix 3 are closed and has a minimum value during the period, in which the apertures shall be open. This is controlled by means of data in a computer card 20. In other words, the return field is alternating synchronously with the print cycle but is 180° out of phase with respect to the print cycle. In this manner the toner concentration may be maximum during the period when the apertures are open. In order not to overfill the powder cloud, the return feed takes place during that time when the apertures are closed between two openings of the apertures . Designation numerals 1 powder cloud 15 powder container 2 powder particles 15a housing for feeding 3 aperture matrix brush 4 base side 15b housing for flipping 5 current conducting ring brush 6 matrix aperture 15c front edge of the brush 7 document housing 8 back electrode 16 flipping brush 9 main field 16a brush straws 10 blocking field 17 flipper blade 11 brush housing 18 positive connection 12 funnel shaped portion 19 brush voltage unit 14 feeding brush 20 computer card

Claims: MS o o W CΛ H υ o- • tf H CD fi -rl rd H υ •* +> β φ •W o id 0 ft ιo o Q Ό O " f - I I are arranged to open the toner deposit aperture (6) individually at neutral voltage and close the aperture (6) at negative voltage excitation and create a blocking field (10) for the aperture (6) between the ring (5) on the bot- torn side of the matrix (3) and the base layer (4) on the upper side of the matrix (3), which field prevents depositing toner particles (2) through the toner deposit aperture (6) . 4. Print head according to claim 1, 2 or 3 , characterized in, that the feeding brush (14) is enclosed in a housing (15a) for feeding downwards a defined amount of tuner to the flipping brush (16) , which also is enclosed in a housing (15b) for feeding downwards a defined amount of tuner to the powder cloud (1) . 5. Print head according to claim 4, characterized in, that the feeding brush (14) with a portion of the brush periphery is in contact with the flipping brush (16) , the brush fibres (16a) of which are made of such a material that they tribo-electrically charge the toner particles negatively, whereas the brush fibres become positively charged. 6. Print head according to any of the preceding claims, characterized in, that the flipping brush (16) is centrally located over the toner deposit apertures (6) to provide a uniform distribution of the toner cloud over the aperture zone. 7. Print head according to claim 6, characterized in, that the distance between the : flipping brush (16) and the toner deposit apertures (6) in the toner matrix (3) is 0,5 mm or less. 8. Print head according to any of the preceding claims, characterized in, that the brush straws of the flipping brush are semi-resistive, and that the central shaft of the brush is connected to a positive voltage. 9. Print head according to any of the preceding claims, characterized in, that the front edge (15c) of the housing (15b) of the flipping brush (16) is connected to a positive voltage, so that an electrical field is created between the edge of the brush housing (15c) and the base side (4) of the aperture matrix. 10. Print head according to claim 9, characterized in, that the electrical field between the edge (15c) of the brush housing and the base side (4) of the aperture matrix has a size of such order of magnitude, that it influences the toner particles (2) with the same force as the flip force from the flipping brush (16) . 11. Print head according to any of the preceding claims, characterized in, that a voltage power unit (19) is arranged to provide the flipping brush (16) with such alternating voltage, that the field, which lifts the toner back to the flipping brush (16, has a maximum value when all apertures in the aperture matrix (3) are closed and a minimum vlue during that period when the apertures in the aperture matrix (3) shall be open. 12. Print head according to claim 11, characterized in, that the voltage excitation of the flipping brush is controlled by a computer card (20) in such manner, that the return field for the toner is alternating synchronously with the print cycle and is 180° out of phase with respect to the print cycle . 13. Print head according to any of the preceding claims, characterized in, that below the document (7) to be printed there is a back electrode (8) , which creates a main field (9) producing a pull downwards of charged toner particles (2) towards the upper side of the document (7) . 14. Print head according to any of the preceding claims, characterized in, that the cloud (1) of tuner particles (2) is created by means of one or two powder feeding brushes (14, 16) , which are arranged to charge toner particles (2) and thereby cause that the particles are pulled down towards the aperture matrix (3) , and a flipper blade (17) , is arranged adjacent to one flipping brush (16) , against which blade (17) the straws (16) flip loose the downwards fed toner particles (2) . 15. Print head according to claim 14, characterized in, that a brush in the arrangement is constituted by a powder feeding brush (14) feeding powder particles (2) forwards from a powder container, and that a second brush, which co— operates with the first one, is a flipping brush (16) which takes over the feeding of powder particles (2) down towards the aperture matrix (3) . 16. Print head according to claim 14, characterized in, that the flipping brush (16) is rotating in a direction opposite to the rotation direction of the powder feeding brush (14) . 17. Print head according to claim 14 or 15, characterized in, that the flipping brush (16) rotates with higher speed than the powder feeding brush (14) .

Inventors: SUNDSTROEM PER, SUNDSTROEM, PER
Applicants: DIGITAL FILTER PRINTING AB, SUNDSTROEM PER, SUNDSTROEM, PER
Application year: 2000
Main classification: B41J2
IPC codes: B41J2, G03G15