Method of achieving noise control and noise controlled system

Abstract: Described herein is a method and apparatus for achieving optimum noise control of multiple coronode wires (71, 72) in a copier/printer involves optimizing phase relationships of the voltage on the wires (71, 72) in such a way so as to steer the maximum part of the noise distribution profile in the direction best suited for absorption or dissipation. In a two corotron charging system, the coronode wires (71, 72) are connected to respective power supplies (90, 91) which are controlled by a phase controller (77). The wires (71, 72) are preferably charged such that the phase angle, charge frequency and spacing between wires (71, 72) are optimized.

Description: This invention relates generally to the noise control in a copier or image output terminal (IOT), and more particularly concerns an improved noise control system utilizing an improved method and apparatus for providing optimum noise control in copiers or IOTs by steering the maximum noise into a predetermined location in space. In a typical electrophotographic printing process, a photoconductive member is charged to a substantially uniform potential so as to sensitize the surface thereof. The charged portion of the photoconductive member is exposed to a light image of an original document being reproduced. Exposure of the charged photoconductive member selectively dissipates the charges thereon in the irradiated areas. This records an electrostatic latent image on the photoconductive member corresponding to the informational areas contained within the original document. After the electrostatic latent image is recorded on the photoconductive member, the latent image is developed by bringing a developer material into contact therewith. Generally, the developer material comprises toner particles adhering triboelectrically to carrier granules. The toner particles are attracted from the carrier granules to the latent image forming a toner powder image on the photoconductive member. The toner powder image is then transferred from the photoconductive member to a copy sheet. The toner particles are heated to permanently affix the powder image to the copy sheet. The foregoing generally describes a typical black and white electrophotographic printing machine. With the advent of multicolor electrophotography, it is desirable to use an architecture which comprises a plurality of image forming stations. One example of the plural image forming station architecture is illustrated in US-A-5539501 and utilizes an image-on-image system in which the photoreceptive member is recharged, reimaged and developed for each color separation. This charging, imaging, developing and recharging, reimaging and developing is usually done in a single revolution of the photoreceptor as compared with multipass architectures which allow image on image to be achieved with a single charge, recharge system and imager, etc. This architecture offers a high potential for throughput and image quality. Charging and recharging IOT systems such as disclosed in this specification require at least one charging station and a housing; at least two coronodes mounted in the housing and spaced from each other; and a power supply for energizing each coronode with a phase difference between them. Noise is produced by the or each charging station. Excessive noise from machines, such as, copier/printers in the working environment has been an irritant to others from the advent of such machines until the present day. One of the major contributors has been found to be the charging systems in the machines. Historically, noise from systems comes from the transformer and choke which can be controlled by an enclosure. However, in some systems noise is emitted from the wires of corona devices. JP-A-050197876 refers to this noise emission and describes reducing it by using a half cycle difference in phase between the energisation of adjacent coronodes as is suggested in US-A-5539501. According to one aspect of this invention such a charging system is characterised in that the noise controlled charging system further comprises a phase controller connected to each power supply for controlling phase difference between the energisation of each coronode such that minimum noise is recognized along one direction and maximum noise along another direction; and in that said phase difference is determined as a function of energising frequency and the spacing between the coronodes. In accordance with another aspect of the present invention, there is provided a method of achieving optimum noise control in a charging system of a copier/printer which includes at least two coronodes mounted in a housing and spaced from one another, and power supply means for energising the coronodes at a different phase; characterized in that the method comprises energising the coronodes at a phase difference such that minimum noise is recognized along one direction and maximum noise along another direction; and in that said phase difference is determined as a function of energising frequency and the spacing between the coronodes. In the present invention the noise from wires in charging device is reduced by steering the maximum noise to a predetermined location in space so redistributing the sound field. As a consequence, the unwanted noise can be reflected back to the source and dissipated inside the machine. For additional noise reduction, absorption material is placed underneath the wires. Other features of the present invention will become apparent from the following description given by way of example only, and reference to the accompanying drawings, in which: Figure 1 shows a corona device referred to as a discorotron system in accordance with the present invention employing two corotron wires; Figure 2 shows a corona device referred to as a discorotron system in accordance with this present invention employing three corotron wires; Figure 3 is a diagram showing two coronodes in space separated by some distance 2d; and Figure 4 is a schematic diagram of a four color image output terminal utilizing the discorotron noise reduction apparatus and method of the present invention. This invention relates to a noise reduction scheme for an imaging system of the type which is used to produce an image on image color output in a single revolution or pass of a photoreceptor belt. It will be understood, however, that it is not intended to limit the invention to the embodiment disclosed. On the contrary, it is intended to cover all alternatives, modifications and equivalents as may be included within the invention as defined by the appended claims, including use in a multiple pass image on image color process system, and a single or multiple pass highlight color system. Additionally, this invention relates to corona devices in general. Corona devices are devices that ionize air for purposes of delivering ions to surfaces to be charged. It contains an element called a coronode that stimulates ionization of the air. Examples of corona devices are corotrons, scorotrons, discorotrons and pin corotrons. Examples of a coronode are thin wire, pins, and dielectric coated wire. Turning now to Figure 4, the electrophotographic printing machine of the present invention uses a charge retentive surface in the form of an Active Matrix (AMAT) photoreceptor belt 10 supported for movement in the direction indicated by arrow 12, for advancing sequentially through the various xerographic process stations and controlled by a controller 90. The belt is entrained about a drive roller 14 and two tension rollers 16 and 18 and the roller 14 is operatively connected to a drive motor M for effecting movement of the belt through the xerographic stations. With continued reference to Fig 4, a portion of belt 10 passes through charging station A where a corona generating device, indicated generally by the reference numeral 70, charges the photoconductive surface of belt 10 to a relative high, substantially uniform, preferably negative potential. Next, the charged portion of photoconductive surface is advanced through an imaging station B. At exposure station B, the uniformly charged belt 10 is exposed to a laser based output scanning device 24 which causes the charge retentive surface to be discharged in accordance with the output from the scanning device. Preferably the scanning device is a laser Raster Output Scanner (ROS). Alternatively, the ROS could be replaced by other xerographic exposure devices such as LED arrays. The photoreceptor belt 10, which is initially charged to a voltage V 0 , undergoes dark decay to a level V ddp equal to about -500V. When exposed at the exposure station B it is discharged to V background equal to about -50V. Thus after exposure, the photoreceptor belt 10 contains a monopolar voltage profile of high and low voltages, the former corresponding to charged areas and the latter corresponding to discharged or background areas. At a first development station C, a magnetic brush developer structure, indicated generally by the reference numeral 26 advances insulative magnetic brush (IMB) material 31 into contact with the electrostatic latent image. The development structure 26 comprises a plurality of magnetic brush roller members. These magnetic brush rollers present, for example, charged black toner material to the image areas for development thereof. Appropriate developer biasing is accomplished via power supply 32. A corona recharge device 70 having a high output current vs. control surface voltage (I/V) characteristic slope is employed for raising the voltage level of both the toned and untoned areas on the photoreceptor to a uniform predetermined level. A second exposure or imaging device 38 which may comprise a laser based input and/or output structure is utilized for selectively discharging the photoreceptor belt 10 on toned areas and/or bare areas, pursuant to the image to be developed with a second color developer. At this point, the photoreceptor belt 10 contains toned and untoned areas at relatively high voltage levels and toned and untoned areas at relatively low voltage levels. These low voltage areas represent image areas which are developed using discharged area development (DAD). To this end, a negatively charged, developer material 40 comprising color toner is employed. The toner, which by way of example may be yellow, is contained in a developer housing structure 42 disposed at a second developer station D and is presented to the latent images on the photoreceptor belt 10 by a magnetic brush developer roller. A power supply (not shown) serves to electrically bias the developer structure to a level effective to develop the DAD image areas with negatively charged yellow toner particles 40. The above procedure is repeated for a third imager for a third suitable color toner such as magenta and for a fourth imager and suitable color toner such as cyan. In this manner a full color composite toner image is developed on the photoreceptor belt 10. To the extent to which some toner charge is totally neutralized, or the polarity reversed, thereby causing the composite image developed on the photoreceptor to consist of both positive and negative toner, a negative pretransfer discorotron member 50 is provided to precondition the toner for effective transfer to a substrate using positive corona discharge. Subsequent to pretransfer a sheet of support material 52 is moved into contact with the toner images at transfer station G. The sheet of support material is advanced to transfer station G by conventional sheet feeding apparatus, not shown. Preferably, the sheet feeding apparatus includes a feed roll contacting the uppermost sheet of a stack of copy sheets. The feed roll rotates so as to advance the uppermost sheet from the stack into a chute which directs the advancing sheet of support material into contact with the photoconductive surface of belt 10 in a timed sequence so that the toner powder image developed thereon contacts the advancing sheet of support material at transfer station G. Transfer station G includes a transfer dicorotron 54 which sprays positive ions onto the backside of sheet 52. This attracts the negatively charged toner powder images from the belt 10 to sheet 52. A detack dicorotron 56 is provided for facilitating stripping of the sheets from the belt 10. After transfer, the sheet continues to move, in the direction of arrow 58, onto a conveyor (not shown) which advances the sheet to fusing station H. Fusing station H includes a fuser assembly, indicated generally by the reference numeral 60, which permanently affixes the transferred powder image to sheet 52. Preferably, fuser assembly 60 comprises a heated fuser roller 62 and a backup or pressure roller 64. Sheet 52 passes between fuser roller 62 and backup roller 64 with the toner powder image contacting fuser roller 62. In this manner, the toner powder images are permanently affixed to sheet 52 after it is allowed to cool. After fusing, a chute, not shown, guides the advancing sheets 52 to a catch tray, not shown, for subsequent removal from the printing machine by the operator. After the sheet of support material is separated from the photoconductive surface of belt 10, the residual toner particles carried by the non-image areas on the photoconductive surface are removed therefrom. These particles are removed at cleaning station I using a cleaning brush structure contained in a housing 66. Turning now to FIGS. 1 and 2 inclusive, there is illustrated configurations of discorotrons useful in the printer apparatus of FIG. 4. In FIG. 1, a discorotron system 70 is shown supported by frame member 76 closely adjacent to photoreceptor belt 10. Discorotron is used herein to mean a dielectric coated coronode wire with a charge leveling screen located at a predetermined distance from the corotron wire. The discorotron system 70 comprises two coronode wires 71 and 72 that are enclosed on opposite sides by walls 74 and 75 and a charge leveling screen 78 that are mounted on a bottom support member positioned on frame 76. Acoustic absorption material 79 is included beneath coronodes 71 and 72 while the corotrons are powered by power supplies 90 and 91, respectively and phase controlled by phase controller 77. One way to control noise of discorotron systems is to steer the noise radiated by the discorotron system 70 to a predetermined location. By redistributing the sound field, the unwanted noise can be dissipated inside the machine. For maximum treatment, absorption material 79 can be placed at location(s) where this unwanted noise is directed. Redistribution of noise from discorotron system 70 is accomplished by setting coronodes 71 and 72 at a different phase with phase controller 77, preferably 91° apart for charging frequency set at 4kHz. By doing so, minimum noise will be recognized along one direction and maximum noise recognized along another direction. The desired phase difference is a function of the drive frequency and spacing between the wires. This 91° phase difference is confirmed by the calculations that follow: The sound power of a system (W) is: W = ∫ puds where p is the acoustic pressure, u is the particle velocity, d is half the distance between the two coronodes and s is surface area enclosing the sound source. Here, p=-p(∂ / ∂t)and u= (∂/∂ r ) where  is the velocity potential at a point X due to both coronodes, see Fig 3. The velocity potential at point X can be written as: Let Q 1 = Qe t ( wt+α ) Q 1 = Qe t ( wt-∂ ) where Q is the source strength, α is the phase difference between the two compounds 1 & 2, ω is the angular frequency, k is the wave number and i 2 = -1. Derivation for the above expressions (2), (3) and (4) can be found in M. P. Norton's book entitled "Fundamentals of Noise and Vibration Analysis in Engineering", Cambridge, NY, 1989, pp 125 - 132. Putting (3) and (4) into (2) or =- Qe t ( wt-kr ) 2π r cos( kd cos+ α ) For minimum , cos(kdcos + α) = 0 kdcos + α = π/2 For maximum , cos (kdcos + α) = 1 kdcos + α = 0 Thus, the conditions for minimum and maximum noise is dependent upon the phase difference between the two coronodes 1 and 2, the energising frequency, and the spacing betweenthe two coronodes. To design for minimum  at  = 0 by adjusting α for a system having d = 16 x 10 -3 m, f = 8000Hz, c = 340ms -1 and k = 2πf/c, kd = 2.365 kdcos = α = π/2 α = 45.5° Phase difference = 91° By using a phase difference of 91°, noise of the discorotron has improved from 86dBA to 80 dBA. An improvement of 6dBA corresponds to a 75% improvement. With the sound field located as such, noise emitted by the discorotron will be reflected back into the discorotron housing by the photoreceptor belt 10. Usually this treatment is sufficient to meet the desired purposes, however, under adverse conditions additional attenuation can be achieved by means of noise absorption material 79 placed inside the discorotron housing, as shown in FIG. 1. While it may appear that discorotron noise control may be achieved by charging two corotron wires 180° out of phase with each other, experiment has shown that the current invention is much more effective. The noise level of a discorotron without treatment is 86dBA. The current invention with the corotrons set at about 91° out of phase yields a noise level of 80dBA. The 180° out of phase configuration yields a noise level of 82dBA. With absorption, the current invention yields 76dBA and the 180° out of phase yields 78dBA. Clearly, the result obtained by the present invention is consistently better than that via 180° out of phase. It is 2dB (40%) better. Among all known commercially available corotrons, the charging frequency is less than 800Hz for bare wire systems and 4kHz only for dielectric wires. It was found that the charging frequency of the system can be optimized inside and outside the specifications of these prior devices so that the maximum noise can be steered into a predetermined location for dissipation. For example, as an illustration of the dependence upon frequency, for a coronode system with spacing of d 1.6 x 10 m, the maximum noise can be steered towards the photoreceptor belt 10 of FIG. 1 so that the unwanted noise can be reflected back into the coronode system for dissipation Here, =0,cos  = 1 α = 0, if no phase adjustment is used. d=1.6 x 10 -2 m From equation (7) kd cos  + α = π/2 k = π/2d f = 5313Hz Experiments have confirmed that the optimum frequency for this system is 4800Hz. This frequency is about 90% of prediction. Noise is reduced from 86dBA to 76dBA. This 10dBA improvement corresponds to a 90% improvement. Generally, for corotrons that exist in the market, the spacing (FIG. 4) of the wires is from 10mm to 25mm for bare wire and 30mm only for dielectric wires. With the present invention, it was found that the spacing of the wires can be optimized so that the maximum noise can be steered into a predetermined location for dissipation. For example, in a coronode system with a charging frequency of 4kHz, the maximum noise can be steered towards the photoreceptor 10 of FIG. 1 so that the unwanted noise can be reflected back into the coronode system for dissipation. Here, =0,cos = 1 α = 0, if no phase adjustment is used. k=2nf/c=73.92 From equation (7) kd cos  + α = π/2 73.92 d = π/2 d=2.1 x 10 -2 m, or 4.2 cm apart between the two wires A three wire corona system 80 is shown in FIG. 2 that includes a coronode 73 in addition to coronodes 71 and 72 with screen 78. For a three wire system, noise is controlled by charging the two outside coronodes 71 and 73, at the same voltage and the same phase, with power supplies 90 and 91, respectively. The center coronode 72 is charged twice the voltage and 91° out of phase relative to the outside coronodes by power supply 92. Phase difference between 71/73 and 72 is controlled by a phase controller 77. Absorption with material 79 can be used for additional noise abatement, if desired. In recapitulation, a method and apparatus for achieving optimum noise control for corotron usage is disclosed. The noise improvement over conventional corotron systems is realized by steering and redistributing the sound field in space so that the noise can be reflected back towards the corotron and dissipated within the machine. This can be accomplished by optimizing the phase difference between the wires, the charging frequency and the spacing between the wires.

Claims: A method of achieving optimum noise control in a charging system of a copier/printer which includes at least two coronodes (71, 72; 71, 72, 73) mounted in a housing (74, 75, 76) and spaced from one another, and power supply means (90, 91; 90, 91, 92) for energising the coronodes (71, 72; 71, 72, 73) at a different phase; characterized in that the method comprises energising the coronodes (71,72; 71,72,73) such that at a phase difference minimum noise is recognized along one direction and maximum noise along another direction; and in that said phase difference is determined as a function of energising frequency and the spacing between the coronodes (71,72;71,72,73). A method according to claim 1, wherein the said phase difference is about 91°. A noise controlled charging system comprising: a housing (74, 75, 76); at least two coronodes (71, 72; 71, 72, 73) mounted in the housing (74, 75, 76) and spaced from each other; and a power supply (90, 91; 90, 91, 92) for energizing each coronode (71, 72; 71, 72, 73) with a phase difference between them; characterized in that the noise controlled charging system further comprises a phase controller (77) connected to each power supply (90, 91; 90, 91, 92) for controlling phase difference between the energisation of each coronode (71, 72; 71, 72, 73) such that minimum noise is recognized along one direction and maximum noise along another direction; and in that said phase difference is determined as a function of energising frequency and the spacing between the coronodes (71,72;71,72,73). , A charging system according to claim 3, wherein the said phase difference is about 91°. A charging system according to claims 2 or 3, comprising three coronodes (71, 72, 73) spaced from one another and each connected to a respective power supply (90, 91, 92), the outer coronodes (71, 73) being energised to the same voltage and having the same phase and the central coronode (72) being energised to twice the voltage of the outer coronodes (71, 73). A charging system according to any one of claims 3 to 5, further comprising noise absorption material (79) added to the housing (74, 75, 76). A charging system according to any one of claims 3 to 6, further comprising a conductive screen (78) in cooperation with the housing (74, 75, 76) and positioned closely spaced from the coronodes (71, 72; 71, 72, 73). An electrophotographic printing machine comprising an image carrying medium (10) and at least one charging system according to any one of claims 3 to 7.

Inventors: FOURNIA PETER G, WONG CHEE-CHIU J, FOURNIA, PETER G., WONG, CHEE-CHIU J.
Applicants: XEROX CORP, XEROX CORPORATION
Application year: 1997
Main classification: G03G15
IPC codes: G03G15