EP0000789B1 - Verfahren und Vorrichtung zur Erzeugung geladener Teilchen - Google Patents
Verfahren und Vorrichtung zur Erzeugung geladener Teilchen Download PDFInfo
- Publication number
- EP0000789B1 EP0000789B1 EP78100651A EP78100651A EP0000789B1 EP 0000789 B1 EP0000789 B1 EP 0000789B1 EP 78100651 A EP78100651 A EP 78100651A EP 78100651 A EP78100651 A EP 78100651A EP 0000789 B1 EP0000789 B1 EP 0000789B1
- Authority
- EP
- European Patent Office
- Prior art keywords
- electrode
- ions
- electrodes
- extracted
- dielectric member
- 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
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Classifications
-
- H—ELECTRICITY
- H01—ELECTRIC ELEMENTS
- H01T—SPARK GAPS; OVERVOLTAGE ARRESTERS USING SPARK GAPS; SPARKING PLUGS; CORONA DEVICES; GENERATING IONS TO BE INTRODUCED INTO NON-ENCLOSED GASES
- H01T19/00—Devices providing for corona discharge
-
- B—PERFORMING OPERATIONS; TRANSPORTING
- B41—PRINTING; LINING MACHINES; TYPEWRITERS; STAMPS
- B41J—TYPEWRITERS; SELECTIVE PRINTING MECHANISMS, i.e. MECHANISMS PRINTING OTHERWISE THAN FROM A FORME; CORRECTION OF TYPOGRAPHICAL ERRORS
- B41J2/00—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed
- B41J2/385—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective supply of electric current or selective application of magnetism to a printing or impression-transfer material
- B41J2/41—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective supply of electric current or selective application of magnetism to a printing or impression-transfer material for electrostatic printing
- B41J2/415—Typewriters or selective printing mechanisms characterised by the printing or marking process for which they are designed characterised by selective supply of electric current or selective application of magnetism to a printing or impression-transfer material for electrostatic printing by passing charged particles through a hole or a slit
-
- 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
- G03G15/22—Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20
- G03G15/32—Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20 in which the charge pattern is formed dotwise, e.g. by a thermal head
- G03G15/321—Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20 in which the charge pattern is formed dotwise, e.g. by a thermal head by charge transfer onto the recording material in accordance with the image
- G03G15/323—Apparatus for electrographic processes using a charge pattern involving the combination of more than one step according to groups G03G13/02 - G03G13/20 in which the charge pattern is formed dotwise, e.g. by a thermal head by charge transfer onto the recording material in accordance with the image by modulating charged particles through holes or a slit
Definitions
- This invention relates to the generation of charged particles, and more particularly, to the generation of ions with high current densities.
- Ions can be generated in a wide variety of ways. Common techniques include the use of air gap breakdown, corona discharges and spark discharges. Other techniques employ tribo-electricity, radiation (Alpha, Beta, and Gamma, as well as x-rays and ultra-violet light) and microwave breakdown.
- Air gap breakdown i.e., discharges occurring in small gaps between a stylus or wire and the surface of a dielectric material, are widely employed in the formation of electrostatic images.
- Representative U.S. patents are G. R. Mott 3.208.076; E. W. Marshall 3.631.509; A. D. Brown, Jr. 3.662.396; A. E. Bliss et al. 3.792.495; R. F. Borelli 3.958.251; and R. T. Lamb 3.725.950.
- the gap spacing be maintained between about 0.005 and 0.02 mm in order to be able to operate with applied potentials at reasonable levels and maintain charge image integrity. Even then, the latent charge image is not uniform, so that the resultant electrostatically toned image lacks good definition and dot fill.
- corona discharge from a small diameter wire or a point source is the corona discharge from a small diameter wire or a point source.
- Illustrative U.S. Patents are P. Lee 3.358.289; Lee F. Frank 3.611.414; A. E. Jvirblis 3.623.123; H. Bresnik 3.765.027; P. J. Magill et al. 3.715.762; and R. A. Fotland 3.961.574.
- Corona discharges are widely employed in electrostatic precipitation, and are used almost exclusively in electrostatic copiers to charge photoconductive surface prior to exposure. Corona discharges are also extensively employed in electrostatic separators and in electrostatic coating and spraying equipment.
- corona discharges provide limited currents.
- the maximum discharge current density heretofore obtained has been on the order of 10 microamperes per square centimeter. This can impose a severe printing speed limitation.
- coronas can create significant maintenance problems. Corona wires are small and fragile and easily broken. Because of their high operating potentials, they collect dirt and dust and must be frequently cleaned or replaced.
- An alternative technique for forming high density corona discharges is to use high velocity air streams. For example, if high pressure air is employed with a small orifice at the corona discharge point, current densities as high as 1 000 microamperes per square centimeter are reportedly obtainable (Proceedings of the Conference on Static Electrification, London 1967, Page 139 of The Institute of Physics and Physical Society, London SW1). This technique is awkward, however, and requires both a pressurized air source and critical geometry in order to prevent premature electrical breakdown.
- Another method of forming ions which is particularly useful in electrostatic applications, uses an electrical spark discharge.
- Representative U.S. patents are B. E. Byrd 3.321.768; H. Epstein 3.335.322; C. D. Hendricks Jr. 3.545.374; and W. P. Foster 3.362.325.
- a low energy spark discharge technique is described by Krekow and Schram in IEEE transactions on Electronic Devices, E. D.-21 # 3, Page 189, March 1974.
- the electrical spark discharge is objectionable, however, where uniform ion currents are desired or required. This is particularly true where the discharge occurs over the surface of a dielectric.
- NL 7700013 discloses a corona device for charging and discharging dielectric surfaces, of a type including a conductive wire coated with a thick dielectric material, and a flat "shield" electrode contacting or closely spaced from the thick dielectric material.
- the geometry of the device is not suited to electrostatic imaging, in that the generated ions are not organized in a coherent electrostatic pattern.
- electrostatic imaging involves the use of a matrix of transversely oriented electrodes.
- One such device is disclosed in UA-Patent 3 971 465. Such devices have the advantage of providing a multiplexable ion source.
- FR-2 121 299 discloses a spark plug ion generator, of the type including two electrodes to which an impulse voltage is applied and which electrodes are separated by an air gap.
- the air gap loses its dielectric characteristics during air gap breakdown, which results in several functional disadvantages.
- the discharge energy depends on external circuit elements, rather than inherent characteristics of the device.
- the air gap discharges are not tempered by the "self-quenching" property of a solid dielectric between two electrodes, thus providing less reliable ion generation.
- Another object is to provide a reliable and stable source of ions.
- a related object is to provide an ion generating system which does not require critical periodic maintenance.
- Another related object is to simplify maintenance and eliminate the objectionable characteristics of corona wires, including the fragility and tendency to collect dirt and dust.
- a further object of the invention is to provide an easily controlled source of ions.
- a related object is to provide a multiplexable source of ions using different voltage sources to supply an alternating breakdown field and an ion extraction field.
- Yet another object of the invention is to generate ion currents for use in producing electrostatic images in which charge image integrity is maintained.
- a related object is to achieve comparatively uniform charge images which can be toned with good definition and dot fill.
- the invention refers to method and apparatus of generating ions in air which comprises applying alternating potential between first and second electrodes separated by a solid dielectric member.
- the invention is characterized in that the second electrode has an edge surface disposed opposite an intermediate portion of the first electrode and remote from the edge of the dielectric member to define an air region at the junction of the edge surface and the solid dielectric member so that the alternating potential between the first and second electrode induces ion producing electrical discharges in the air region.
- Ions thus produced can be extracted from the air region by an ion extraction potential which is applied between the second and a third electrode.
- the ions can be used for purposes of electrostatic imaging or in other cases where ions are suitable.
- the extracted ions may be applied to a further member.
- This further member can be a dielectric surface with a conductive backing.
- the further member can also be a particulate matter.
- the extraction is accomplished using a direct voltage.
- an electrostatic pattern is formed with said extracted ions.
- the method can be performed in a way that the ions are extracted by a direct voltage applied to the second electrode, with a gap patterned in accordance with the configuration of a character or symbol for which a charge image is desired.
- the first electrode from an open mesh woven metal screen.
- first and second electrodes each comprise a multiplicity of electrodes forming cross points in a matrix array, configured such that the second electrodes on one side of the solid dielectric member contain apertures at matrix electrode crossover regions.
- a further way of performing the method is that the ions are extracted from selected matrix apertures by simultaneously providing both an electrical discharge in said aperture and an external ion extraction field.
- the method may further comprise the step of collecting the charged particulate matter on a conductive surface.
- the method may further comprise the step of collecting the charged particulate matter onto plain paper to form a visible image.
- the apparatus for generating ions in air comprises a solid dielectric member, first and second electrodes being separated by the solid dielectric member and means for applying an alternating potential between the first and second electrode.
- This apparatus is characterized in that an edge surface of the second . electrode is disposed opposite an intermediate portion of the first electrode and remote from the edge of the dielectric member to define an air region at the junction of the edge surface and the solid dielectric member.
- the apparatus may be provided with a third electrode to extract ions from the air region.
- the second electrode preferably comprises a mask electrode, the aperture in said second electrode being patterned in the configuration of a character or symbol for which a charge image is desired.
- the apparatus may be provided in a way that said first and second electrodes comprise a multiplicity of electrodes contacting a dielectric sheet and forming cross points in a matrix array, configured such that the first electrodes on one side of the dielectric sheet comprise selector bars, and the second electrodes on the other side of said dielectric sheet comprise air breakdown electrodes transversely oriented with respect to the selector bars, with apertures at matrix crossover regions.
- an ion generator 10 in accordance with the invention is used in producing an air gap breakdown between a solid dielectric 11 and respective conducting electrodes 12-1 and 12-2 using a source 13 of alternating potential.
- an electric fringing fields E A and Eg in the air gaps 14-a and 14-b exceed the breakdown field of air, an electric discharge occurs which results in the charging of the dielectric 11 in regions 11-a and 11-b adjacent electrode edges.
- the generator 10 of Figure 1 therefore, produces an air gap breakdown twice per cycle of applied alternating potentials from the source 13 and thus generates an alternating polarity supply of ions.
- the extraction of ions produced in accordance with the generator 10 of Figure 1 is illustrated by the generator-extractor 20 of Figure 2.
- the generator 20A includes a dielectric 21 between conducting electrodes 22-1 and 22-2.
- the electrode 22-1 is encapsulated or surrounded by an insulating material 23. Alternating potential is applied between the conducting electrodes 22-1 and 22-2 by a source 24A.
- the second electrode 22-2 has a hole 21-h where the desired air gap breakdown occurs relative to a region 21-r of the dielectric 21 to provide a source of ions.
- the ions in the gap 21-h may be extracted by a direct current potential applied from a source 24-B to provide an external electric field between the electrode 22-2 and a grounded auxiliary electrode 22-3.
- An illustrative insulating surface to be charged by the ion source in Figure 2 is a dielectric (electrographic) paper 25 consisting of a conducting base 25-P coated with a thin dielectric layer 25-d.
- the electrode 22-2 When a switch 26 is switched to position X and is grounded as shown, the electrode 22-2 is also at ground potential and no external field is present in the region between the ion generator 20A and the dielectric paper 25. However, when the switch 26 is switched to position y, the potential of the source 24, is applied to the electrode 22-2. This provides an electric field between the ion reservoir 21-r and the backing of dielectric paper 25. The ions extracted from the air gap breakdown region then charge the surface of the dielectric layer 25-d.
- the generator and ion extractor 20 of Figure 2 is readily employed, for example, in the formation of characters on dielectric paper in high speed electrographic printing. Illustrative sources for the electrographic printing of characters in accordance with the invention are shown in Figures 3 and 4.
- a character generator 30 is formed by a dielectric member.31 which is sandwiched between an etched conducting sheet 32-1 and a set of counter-electrodes 32-2, 32-3 and 32-4.
- the etched or mask electrode 32-1 illustratively is shown with etched characters A, B and C.
- the fringing fields at the edges of the etched characters provide a high density source of ions when an air gap breakdown according to the invention is produced by alternating potential applied between the etched electrode 32-1 and the counterelectrodes.
- a source of high frequency alternating voltage (not shown) is applied between the etched electrode 32-1 and the associated counter-electrode 32-3. This provides a high density supply of ions in the region of the dielectric 31 at the edges of the etched character B in the mask 32-1.
- the ions are then extracted and transferred to a suitable dielectric surface, for example the dielectric coated paper 25 of Figure 2, by the application of a direct voltage between the paper backing and the mask 32-1, resulting in the formation of the electrographic latent image B on the dielectric surface of the paper 25.
- a suitable dielectric surface for example the dielectric coated paper 25 of Figure 2
- the matrix ion generator 40 Figure 4 may be employed.
- the generator 40 makes use of a dielectric sheet 41 with a set of apertured air gap breakdown electrodes 42-1 through 42-4 on one side and a set of selector bars 43-1 through 43-4 on the other side, with a separate selector being provided for each different aperture 45 in each different finger electrode 42-1 to 42-4.
- Matrix location 45 23 is printed by simultaneously applying a high frequency potential between selector bar 43-3 and ground and a direct current potential between finger electrode 42-2 and a dielectric receptor member's counterelectrode. Unselected fingers as well as the dielectric members counter-electrode are maintained at ground potential.
- the number of required voltage electrodes is significantly reduced. If, for example, it is desired to print a dot matrix array across a 20 mm wide area at a dot matrix resolution of 200 dots per 25 mm, 1600 separate electrodes would be required if multiplexing were not employed. By utilizing the array of Figure 4 with, for example, 20 alternating frequency selector bars, only 80 finger electrodes would be required and the total number of electrodes is reduced from 1600 to 100.
- the invention may be employed to form a rectangular area of charge using geometry of the module 50 shown in Figure 5.
- Charging electrodes 52-1 and 52-2 are separated from the electrode 52-3 by a dielectric member 51, with the electrode 52-3 potted in an insulator 55.
- the region between the electrode 52-1 and 52-2 provides a slot in which an air gap-discharge is formed when a high frequency alternating potential is applied between electrodes 52-1 and 52-2 and electrode 52-3.
- the charging array of Figure 5 may be employed in a plain paper copier to replace the coronas normally found in such a copier.
- FIG. 6 illustrates schematically a plain paper copier employing charging arrays of the kind shown in Figure 5.
- a copier drum 61 is charged using a charging element 62-1, having the configuration shown in Figure 5. If the drum is selenium or a selenium alloy and it is desired to charge the surface, for example, to a positive potential of 600 volts, then the slotted electrode 62-1 is maintained at 600 volts. After charging, the drum 61 is discharged with an optical image provided by a scanner at station 63. The resulting latent electrostatic image is toned at station 66 and the toner is transferred to a plain paper sheet 68, using a transfer ion generator 62-2 according to Figure 5, with the slotted electrode again maintained at a positive potential.
- the latent residual electrostatic image in the surface of the drum and any uncharged toner may be electrically discharged by employing a discharge unit 62-3, also according to Figure 5.
- a discharge unit 62-3 also according to Figure 5.
- the slotted electrode is maintained at ground potential and any residual charge on the surface of the drum and toner causes ions to be extracted from the air gap breakdown in the slot, thus effectively discharging the surface.
- a cleaning brush 64 is employed to remove residual toner remaining on the surface and the drum is then ready to be recharged.
- a dot matrix charging head 65 which may be configured according to Figure 4. This permits a plain paper copier to be employed as a printer. In that event the drum 61 is discharged at station 63 and recharged by the dot matrix printing head 65, permitting the machine 60 to function both as a copier and a printer. In addition, the apparatus 60 may function simultaneously as a copier and printer where overlays are desired.
- Strips of 25 microns stainless steel foil are laminated on both sides of Corning (registered trademark) code 8871 capacitor ribbon glass.
- the stainless foil is coated with resist and photo etched with a pattern similar to that shown in Figure 4, with holes or apertures in the fingers approximately 0,15 mm in diameter. This provides a charging head which can be employed to generate latent electrostatic dot matrix character images on dielectric paper according to Figure 2.
- Charging occurs only when there is simultaneously a potential of negative 400 volts on the fingers containing the holes and an alternating potential of 2 kilovolts peak at a frequency of 500 kilohertz supplied between the finger and the counter electrode.
- a spacing of 0,02 mm is maintained between the print head assembly and the dielectric surface of the electrophotographic sheet.
- the duration of the print pulse is 20 microseconds. Under these conditions, it is found that a latent electrostatic image of approximately 300 volts is produced on the dielectric sheet. This image is subsequently toned and fused to provide a dense dot matrix character image.
- the ion current extracted from this charging head, as collected by an electrode spaced 0,2 mm away from the head, is found to be 1 milliampere per square centimeter.
- Example I is repeated employing a polyimide dielectric rather than capacitor glass. As before, a 25 microns stainless steel foil is laminated on both sides to 25 microns thick Kapton (registered trademark) polyimide film. Results equivalent to those of Example I are obtained at an applied high frequency potential of 1,5 kilovolts peak.
- Kapton registered trademark
- An electrostatic charging head of the type shown in Figure 3 is fabricated employing 25 microns stainless steel foil laminated to both sides of 25 microns polyimide film. Results equivalent to those of Example I are obtained at
- An electrostatic charging head of the type shown in Figure 3 is fabricated employing 25 microns stainless steel foil laminated to both sides of 25 microns polyimide sheet.
- 2,54 mm high characters are etched in the foil on one side of the foil as indicated in Figure 3.
- bridges 25 to 50 microns in thickness are left unetched.
- the character stroke width is etched to 150 microns. Printing is carried out by applying the potentials of Example II with a pulse width of 40 microseconds. The toned images exhibit sharp edges and high optical density.
- the character stroke width in the image is 0,3 mm.
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- Physics & Mathematics (AREA)
- General Physics & Mathematics (AREA)
- Engineering & Computer Science (AREA)
- Plasma & Fusion (AREA)
- Printers Or Recording Devices Using Electromagnetic And Radiation Means (AREA)
- Electrophotography Using Other Than Carlson'S Method (AREA)
- Elimination Of Static Electricity (AREA)
Claims (22)
Applications Claiming Priority (2)
Application Number | Priority Date | Filing Date | Title |
---|---|---|---|
US05/824,252 US4155093A (en) | 1977-08-12 | 1977-08-12 | Method and apparatus for generating charged particles |
US824252 | 1992-01-22 |
Publications (3)
Publication Number | Publication Date |
---|---|
EP0000789A2 EP0000789A2 (de) | 1979-02-21 |
EP0000789A3 EP0000789A3 (en) | 1979-03-07 |
EP0000789B1 true EP0000789B1 (de) | 1984-08-15 |
Family
ID=25240954
Family Applications (1)
Application Number | Title | Priority Date | Filing Date |
---|---|---|---|
EP78100651A Expired EP0000789B1 (de) | 1977-08-12 | 1978-08-11 | Verfahren und Vorrichtung zur Erzeugung geladener Teilchen |
Country Status (9)
Country | Link |
---|---|
US (1) | US4155093A (de) |
EP (1) | EP0000789B1 (de) |
JP (1) | JPS5453537A (de) |
AU (1) | AU522601B2 (de) |
BR (1) | BR7805182A (de) |
CA (1) | CA1108685A (de) |
DE (1) | DE2862435D1 (de) |
ES (1) | ES472517A1 (de) |
MX (1) | MX145196A (de) |
Families Citing this family (76)
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-
1977
- 1977-08-12 US US05/824,252 patent/US4155093A/en not_active Expired - Lifetime
-
1978
- 1978-08-09 CA CA308,964A patent/CA1108685A/en not_active Expired
- 1978-08-11 ES ES472517A patent/ES472517A1/es not_active Expired
- 1978-08-11 EP EP78100651A patent/EP0000789B1/de not_active Expired
- 1978-08-11 MX MX174512A patent/MX145196A/es unknown
- 1978-08-11 DE DE7878100651T patent/DE2862435D1/de not_active Expired
- 1978-08-11 AU AU38836/78A patent/AU522601B2/en not_active Expired
- 1978-08-11 BR BR7805182A patent/BR7805182A/pt unknown
- 1978-08-12 JP JP9861078A patent/JPS5453537A/ja active Granted
Also Published As
Publication number | Publication date |
---|---|
JPH024904B2 (de) | 1990-01-30 |
MX145196A (es) | 1982-01-13 |
US4155093A (en) | 1979-05-15 |
ES472517A1 (es) | 1979-03-16 |
EP0000789A3 (en) | 1979-03-07 |
BR7805182A (pt) | 1979-04-24 |
JPS5453537A (en) | 1979-04-26 |
DE2862435D1 (en) | 1984-09-20 |
CA1108685A (en) | 1981-09-08 |
AU3883678A (en) | 1980-02-14 |
EP0000789A2 (de) | 1979-02-21 |
AU522601B2 (en) | 1982-06-17 |
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