A method and system for controlling toner concentration

Abstract: A system (100) controls the concentration of toner in developer in an electrophotographic printer. Toner is applied on a test patch (SD) on a charge-retentive surface in a manner consistent with a desired toner density on a test patch, and the actual toner density on the test patch (SD) is measured. The charge applied to the charge-retentive surface is then adjusted in response to the measured actual toner density to obtain the desired toner density on a subsequent test patch (SD opt ). The change in charge applied to the charge-retentive surface is used to detect a shortage of toner in the developer and feed means (17) is controlled to add toner to the developer.

Description: The present invention relates to a method and system for controlling the concentration of toner within the developer mixture in an electrophotographic printer. An important process parameter for any development system is the ratio of toner particles to carrier within the developer. It is also expectable that, in the course of use of the printer, the toner to carrier (T/C) ratio will change significantly as toner particles are transferred from the developer supply to the photoreceptor and ultimately to print sheets. There have thus been numerous systems devised in the prior art for determining and controlling this TIC ratio in an operating machine. Because carrier particles are generally heavy and magnetic, while toner particles are generally light and non-magnetic, many of these systems involve detecting the behavior of magnetic flux through the developer; placing a quantity of developer between capacitor plates and examining the electrical behavior thereof; or electrically drawing a quantity of toner from the developer and inferring a T/C therefrom. However, very often such systems have proven to be either inaccurate, imprecise, or too expensive for use in inexpensive printers and copiers. From JP-A-4-309 971 a method is known wherein the density of toner patches is measured and the developing field for subsequent copy operations is adjusted. This adjustment is made at a regular timing. An object of the present invention is to provide a method and system of controlling toner concentration without direct physical testing of the developer. According to the present invention, there is provided a method of controlling toner concentration in a quantity of developer material used in an electrophotographic printer wherein toner is applied to an electrostatic latent image on a charge-retentive surface. An initial charge is placed on the charge-retentive surface, and the surface imagewise discharged. Toner is applied on a test patch on the charge-retentive surface in a manner consistent with a desired toner density on a test patch, and the actual toner density on the test patch is measured. The development field is then changed in response to the measured actual toner density to obtain the desired toner density on a subsequent test patch. In response to the magnitude of the development field being changed to exceed a predetermined amount, a quantity of toner is added to the quantity of developer material. The present invention will be described further, by way of examples, with reference to the accompanying drawings, in which:- Figure 1 is a simplified elevational view of the basic elements of an electrophotographic printer; Figure 2 is a graph showing the relative potentials on a portion of a charge-retentive surface in an electrophotographic printer as it passes through a variety of stations; Figure 3 is a systems diagram showing the interrelationship of various functions and potentials within the representative electrophotographic printer of Figure 1; and Figure 4 is a systems diagram, incorporating a flow-chart, illustrating the operation of a system according to the present invention. Figure 1 shows the basic elements of the well-known system by which an electrophotographic printer, such as a copier or a "laser printer," creates a dry-toner image on plain paper. There is provided in the printer a photoreceptor 10, which may be in the form of a belt or drum, and which comprises a charge-retentive surface. The photoreceptor 10 is here entrained on a set of rollers and caused to move through process direction P. Moving from left to right in Figure 1, there is illustrated the basic series of steps by which an electrostatic latent image according to a desired image to be printed is created on the photoreceptor 10, how this latent image is subsequently developed with dry toner, and how the developed image is transferred to a sheet of plain paper. The first step in the electrophotographic process is the general charging of the relevant photoreceptor surface. As seen at the far left of Figure 1, this initial charging is performed by a charge source known as a "scorotron," indicated as 12. The scorotron 12 typically includes an ion-generating structure, such as a hot wire, to impart an electrostatic charge on the surface of the photoreceptor 10 moving past it. The charged portions of the photoreceptor 10 are then selectively discharged in a configuration corresponding to the desired image to be printed, by a raster output scanner or ROS, which generally comprises a laser source 14 and a rotatable mirror 16 which act together, in a manner known in the art, to discharge certain areas of the charged photoreceptor 10. Although the Figure shows a laser source to selectively discharge the charge-retentive surface, other apparatus that can be used for this purpose include an LED bar, or, in a copier, a light-lens system. The laser source 14 is modulated (turned on and off) in accordance with digital image data fed into it, and the rotating mirror 16 causes the modulated beam from laser source 14 to move in a fast-scan direction perpendicular to the process direction P of the photoreceptor 10. The laser source 14 outputs a laser beam having a specific power level, here shown as P L , associated therewith. After certain areas of the photoreceptor 10 are discharged by the laser source 14, the remaining charged areas are developed by a developer unit such as 18 causing a supply of dry toner to contact the surface of photoreceptor 10. The developed image is then advanced, by the motion of photoreceptor 10, to a transfer station including a transfer scorotron such as 20, which causes the toner adhering to the photoreceptor 10 to be electrically transferred to a print sheet, which is typically a sheet of plain paper, to form the image thereon. The sheet of plain paper, with the toner image thereon, is then passed through a fuser 22, which causes the toner to melt, or fuse, into the sheet of paper to create the permanent image. Some of the system elements of the printer shown in Figure 1 are controlled by a control system 100, the operation of which will be described in detail below. Looking now at Figure 2 and with continuing reference to Figure 1, the electrostatic "history" of the representative small area on the photoreceptor 10 as it moves through the various stations in the electrophotographic process is described in detail. Here, the charge on the particular area of photoreceptor 10 is expressed in terms of an electrostatic potential (voltage) on that particular area of the surface. Starting with the initial charging of the surface by scorotron 12, an initial high potential V grid is placed on the given area; in this example V grid is + 240 volts, but this is by way of example and not of limitation. As used in the claims herein, an "initial" charge shall be defined as the charge placed on the photoreceptor or charge-retentive surface prior to the development step, as opposed to any charge incidentally applied to the charge-retentive surface during or as a result of the developing step. Once an initial charge is placed on photoreceptor 10, this charge begins to decay immediately, to the extent that, by the time the representative area reaches the ROS, the potential is slightly decreased to a "dark decay potential," or V ddp , in this example to 230 volts. At the exposure step, if the particular area in question is to be discharged by the action of the laser 14, the potential on that particular area will be markedly reduced, in this example to a value of V exp of 50 volts, which is low enough to ensure that toner will be attracted thereto, particularly relative to highly charged areas thereon. Also associated with a system such as this is a bias voltage, V bias , which is the voltage applied to a relevant portion of the development unit, such as for example the housing thereof or a roll therein. The difference between the dark decay potential V ddp and the bias voltage V bias is known as the "cleaning voltage" V clean , a value which is relevant to the amount of background development in the system. More significantly, development voltage V dev , as shown in the graph of Figure 2, is the difference between the bias voltage V bias and the exposure voltage V exp . V dev thus represents the charge difference which drives the movement of toner to the photoreceptor; as such, V dev is the parameter of most direct relevance to the maintenance of a satisfactory solid area density SD. Another important parameter in an electrophotographic printer is the "saturation" voltage V sat , which is the theoretical maximum possible discharge when the laser source 14 is operating at full power. In the present example, V sat is 30 volts, which is to say that it is generally impossible for a laser of any practical strength to discharge a photoreceptor completely. The value of V sat is generally dependent on the nature of the photoreceptor 10 itself, and the maximum output of the particular laser 14 in the system has a generally asymptotic effect on the value of V sat . In many instances, the value of V sat may be considered a constant, because even a great increase in the power of laser source 14 will not have a substantial effect on the value of V sat . As shown in Figure 1, a densitometer generally indicated as 24 may be used after the developing step to measure the optical density of a solid-density test patch (marked SD) created on the photoreceptor 10 in a manner known in the art. Typically such test patches are created in inter-document zones between image pitches on the photoreceptor, and are placed in known locations where they may be tested by a densitometer in a fixed position after the test patches are developed. In a laser printer, such test patches may be created by specific routines for controlling the laser 14 and rotatable mirror 16, as is known in the art. In the preferred embodiment of the present invention, the system output which is of most interest is the solid area density (SD) test patch, as will be explained in detail below. Figure 3 is a systems diagram showing the basic interactions among the various potentials that are relevant to the electrophotographic process, here organized into a single "black box" indicated as 99, with the relevant inputs and outputs being limited to those outputs which may be readily measured, and those inputs which may be readily controlled. In the diagram it may be seen that certain relationships between relevant potentials are neatly mathematically related, while more subtle or complicated relationships, such as the relationship of V grid to V ddp , are shown as empirical relationships such as f 1 , f 2 , g 1 , g 2 and g 3 . Certain relationships of interest that may be seen in Figure 3 include the fact that V bias is typically of a fixed relationship with V grid and that another relevant potential is the development voltage V dev , which is the difference between V bias and V exp , shown at the box indicated as 90, and which has been shown to have an empirical relationship, through a function f 2 in box 92, to the solid area density SD. (Also shown in Figure 3 is the concept of the "discharge ratio," shown at box 94 which is theorized to have a highly correlative relationship, such as through a function g 3 in box 96, to a halftone density HD, which is not directly relevant to the present discussion. This discharge ratio indicated in box 94 is given as a ratio which takes into account the saturation voltage V sat of the particular photoreceptor, which, incidentally, is also related somewhat to the laser power P L by a relationship g 2 indicated in box 95, although the value of V sat has been found to be substantially constant for a given apparatus.) In the system according to an embodiment of the present invention, the development field V dev required to maintain a solid area density SD is used as the guide to determine when to add toner to the developer to increase the T/C. For systems relying on "discharged-area development," also known as DAD, an example of which is shown in the illustrated embodiments, the photoreceptor surface is charged with an initial charge, and the function of the laser source 14 is to remove this initial charge from areas in which print-black areas of the image are intended. In such a situation, the developer unit 18 is so designed to cause toner particles to adhere to the discharged areas of the photoreceptor, the charge areas of the photoreceptor repelling the toner particles. The magnitude of the development field V dev can be increased by either increasing the discharging power of the laser source 14, which in turn will cause a greater decrease in V exp , or alternately increasing the value of V bias , which is the voltage associated with the developer housing 18 (or a relevant part thereof). Thus, looking at the "black box" configuration of relationships in Figure 3, the two relatively easily controlled physical parameters which can serve as inputs are V bias , the bias of the development unit 18, and P L , the power associated with the laser source 14. Returning to Figure 1, the black box controller 100 accepts as an input the feedback of actual solid-area density SD, and in turn outputs controls for P L to laser source 14, and V bias to development unit 18. It should also be noted that the control system could be modified for electrophotographic systems which rely on "charged-area development," or CAD. In CAD systems, the laser source 14 is used to leave a charge on the areas of the photoreceptor which are intended to be developed with toner, the toner particles in the development unit 18 being so charged as to be attracted to the charged areas on the photoreceptor 10. In the CAD case, the value of V dev can be increased either by raising the photoreceptor charge or reducing the value of V bias on the developer roll 18. However, whether in a DAD or a CAD system, the claimed principle of the present invention, increasing the value of the development field V dev , is the same. As used in the claims herein, the phrase "development field" shall be defined as the difference in voltage between the area of the photoreceptor that is to receive toner and the developer unit (or relevant portion thereof) donating that toner. This definition applies to either the charged-area development or discharged-area development case. In the illustrated embodiment of the system of the present invention, particularly as relating to Figure 2 herein, there is a convention that the arrangement of voltages are all positive. However, it would be apparent to one of skill in the art, that an equivalent system could be designed according to the present invention, wherein negative voltages are applied to the photoreceptor, and in the course of exposure and development the series of voltages in Figure 2 would "rise" toward a zero value. However, for purposes of clarity, only the positive voltage is described and illustrated. Referring again to Figure 1, densitometer 24 is disposed along the path of photoreceptor 10 so as to detect the actual toner density of a test patch shown as SD, which is intended to have the maximum practical solid area density of toner that can be placed on a normally-charged photoreceptor. Systems for measuring the true optical density of a test patch are shown in, for example, US-A-4,989,985 or US-A-5,204,538, both assigned to the assignee hereof and incorporated by reference herein. Densitometer 24, through means known in the art, should detect a density in solid area test patch SD which is consistent with this maximum practical density of toner on the photoreceptor 10; if the densitometer 24 detects less than the maximum practical density of toner, a corrective action by controller 100 will therefore be necessary to increase the toner density in the next or subsequent solid area test patch. As noted above, the most important process parameter for optimizing the density of a solid-area test patch is to adjust (typically, increase) the value of V dev . Controller 100, as shown in Figure 1, is intended to accept as an input the reading of the solid area density SD from densitometer 24, and as an output is adapted to control V dev (by controlling V bias and/or P L ) and also a toner supply 19 for the developer unit 18. In controlling V dev and the behavior of the toner supply 19, the controller exploits short term and long term solutions for maintaining solid area density. V dev can thus be changed relatively easily, and conceivably adjusted either upward or downward for an optimal value of SD. However, it follows that the progressive degradation of solid area density as the toner supply is used up within the developer can be cured only to an extent by increasing V dev . Eventually, the decreasing T/C ratio must be counteracted by directly adding more toner to the developer. In the system of the present invention, the increasing V dev required to maintain the solid area density SD at a desired level is used as a device either to measure by inference the T/C of the developer at a given moment, or more simply as a trigger to detect a condition of insufficient toner in the developer. Figure 4 is a diagram comprising a flow-chart, describing the control behavior of controller 100 in detail. As would be apparent to one skilled in the art, the flow-chart shown within controller 100 could be embodied readily by a microprocessor program, reflecting empirically-collected data about the particular type of apparatus being controlled, or conceivably by means of an analog computer or other control circuit. As can be seen in the flow-chart, the essential function of controller 100 comprises two polling loops. A first loop monitors the solid area density SD from densitometer 24 and compares this reading to a predetermined optimum density SD opt . As can be seen in Figure 4, whenever the measured value of SD is even slightly below the optimum, the controller 100 causes the V dev to be increased by a predetermined amount, the actual value of the predetermined amount being a matter of design choice depending on the desired responsivity of the control system. The second polling loop within controller 100 monitors the actual value of V dev over time. Because of the constraints of the system, it is reasonable to infer that an increase in necessary V dev is the result of a corresponding decrease in T/C, all other parameters being equal. Thus, it is possible to infer a reasonably accurate value of T/C from the necessary value of V dev . For a particular electrophotographic printer, this relationship could be determined empirically. However, it may not be necessary for the actual value of T/C to be calculated in real time. More likely, all that will be necessary is that a condition of too-low T/C will be inferred when V dev exceeds a predetermined "trigger" level. As can be seen in Figure 4, once there is a need, determined by controller 100, to increase the value of V dev in a DAD system, there are two possible physical options: to increase either the value of V bias on the development unit 18, or decrease the value of D exp by increasing the power of the laser device 14, hereshown as P L . Since the object of the controller 100 is to increase the difference between V bias and V exp , it is conceivable that one or the other, or both, of these parameters can be adjusted. In practice, to what extent either of these parameters are adjusted in absolute terms depends on the specific design of a printer. For example, certain laser diodes may not be readily linearly controllable to output a desired laser power, in which case control of V bias to development unit 18 would provide more control. There is shown in Figure 4 an adjustor 50, a circuit which, depending on the specific design of the printer, will control either V bias or P L to various extents in order to obtain a desired value of V dev . Once again, in the illustrated embodiments is shown only a DAD system; it would be apparent to one skilled in the art that in an equivalent CAD system, the value of V dev is increased either by raising the photoreceptor charge (such as by increasing the charging power of an initial V grid , or by decreasing (as opposed to increasing) the value of V bias . In physical terms, the higher the V dev , the more readily toner particles will adhere to the desired areas of photoreceptor 10. However, if there is a paucity of available toner particles within the developer, increases in V dev will have decreasing marginal returns in causing more of these particles to adhere to the photoreceptor in order to maintain a constant SD. At this point, the only solution for maintaining the desired SD is to enrich the developer with a fresh addition of new toner. For the purpose of increasing the toner supply to the developer in unit 18, controller 100 can be adapted to activate a mechanical device such as 17 to cause the admission of more toner such as from hopper 19, into the main developer supply in development unit 18. Numerous schemes for introducing toner as needed into a developer unit 18 are known in the art. Mechanical device 17 could be an openable hatch activated by a solenoid, an auger caused to rotate, or any such mechanical means that are known in the art. The actual toner supply from hopper 19 may, according to the design of the particular machine, comprise pure toner from a bottle, or may comprise some quantity of carrier particles as well. What is important for the present invention is that the introduction of toner or toner-rich developer from hopper 19 substantially increases the T/C of the general developer supply in developer unit 18 from which toner is taken to be applied to the latent image on the photoreceptor. With an enriched developer in the developer unit 18, there will thus be a greater supply of toner particles available within the developer unit 18 to adhere to photoreceptor 10. Because of this greater supply, it will be easier to provide sufficient toner coverage on the photoreceptor to obtain an optimal measured SD at densitometer 24. For this reason, with the newly-enriched developer, a lower value of V dev will be necessary to cause the amount of toner to adhere to the photoreceptor. Thus, after the toner supply is replenished, the value of V dev can return to a relatively low value by the increase in solid density due to the toner dipense, and then subsequently allowed to gradually increase until the next cycle wherein the value of V dev that triggers further introduction of toner into the developer unit 18. In brief, the control system of the present invention employs a"fine tuning" of print quality in the form of short-term variations in the V dev , and a broader, longer-term print quality adjustment in introducing more toner into the developer supply when the value of V grid reaches a predetermined trigger point. A key advantage of this system is that the value of T/C need never be directly measured; rather, the value of T/C is reasonably accurately inferred from the necessary value of V dev required to maintain a desired value of SD. Because the value of T/C need never be directly measured, the necessity for a toner concentration device is obviated. As such devices have been shown by experience to be expensive and/or inaccurate, this relatively easily embodied system can represent a major cost saving in the design of a machine. The basic simplicity of the system of the present invention is particularly advantageous for low-end machines. The fine-tuning aspect of the system, wherein a low detected density is "answered" with an increase in V dev , can be carried out with a very simple circuit; and similarly the "trigger" value of V dev can be used to cause more toner to be introduced into the developer housing, possibly without even the use of a central processor. Further, because the system does not need to measure directly either the T/C ratio or any charge associated with the development step, not only does the system avoid the expense of making such measurements, fewer sources of noise are introduced into the system. The system can thus be incorporated in a copier or printer with very low added cost, particularly in comparison with other prior-art systems. While this invention has been described in conjunction with various embodiments, it is evident that many alternatives, modifications, and variations will be apparent to those skilled in the art. Accordingly, it is intended to embrace all such alternatives, modifications, and variations as fall within the broad scope of the appended claims.

Claims: A method of controlling toner concentration in a quantity of developer material used in an electrophotographic printer including means (17,18) for applying toner to an electrostatic latent image on a charge-retentive surface by creating an electrostatic development field of a preselected magnitude, including: electrostatically applying toner in a manner consistent with a desired toner density on a test patch (SD) on the charge-retentive surface; measuring (24) the actual toner density on the test patch (SD) to indicate a measured toner density; characterised by changing the magnitude of the development field (V dev ) in response to the measured toner density, to obtain the desired toner density on a subsequent test patch; and causing a quantity of toner to be added to the quantity of developer material in response to the development field (V dev ) being changed to exceed a predetermined magnitude. A method as claimed in claim 1, wherein the applying step comprises applying a substantially maximum toner density on the charge-retentive surface. A method as claimed in claim 1 or claim 2, wherein the step of changing the development field (V dev ) does not require directly measuring the magnitude of the development field. A system for controlling toner concentration in a quantity of developer material used in an electrophotographic printer including means for applying toner to an electrostatic latent image on a charge-retentive surface, including: applicator means (12) for applying an initial charge to the charge-retentive surface; means for electrostatically applying toner in a manner consistent with a desired toner density on a test patch (SD) on the charge-retentive surface, said means creating an electrostatic development field (V dev ) of a preselected magnitude; measuring means (24) for measuring the toner density on the test patch (SD) to indicate a measured toner density; characterised by control means (100) for changing the magnitude of the electrostatic development field in response to the measured actual toner density, to obtain the desired toner density on a subsequent test patch; and feed means (17) for causing a quantity of toner to be added to the quantity of developer in response to the magnitude of the electrostatic development field (V dev ) being changed to exceed a predetermined magnitude. A system as claimed in claim 4, wherein the applicator means applies substantially the maximum toner density on the charge-retentive surface. Asystem as claimed in claim 4 or claim 5, wherein the means for changing the development field do not require directly measuring the magnitude of the development field.

Inventors: HENDERSON THOMAS A, HENDERSON, THOMAS A.
Applicants: XEROX CORP, XEROX CORPORATION
Application year: 1995
Main classification: G03G15
IPC codes: G01N21, G03G15