1. Field of the Invention
The present invention relates to image-forming apparatuses and methods for measuring the amount or density of toner of a toner patch formed on a belt-like moving medium suspended on rollers.
2. Description of the Related Art
Known image-forming apparatuses are divided into various types, including electrophotographic apparatuses, heat-transfer apparatuses, and inkjet apparatuses. Among them, electrophotographic apparatuses are superior to other types of image-forming apparatuses in terms of high speed, high image quality, and quiet operation, and thus have increasingly become widespread in recent years. Electrophotographic apparatuses are further divided into various types, including multiple transfer apparatuses and apparatuses having an intermediate transfer member, which are well known types. Other types include multiple development apparatuses, which form color images on a photosensitive member and simultaneously transfer the images to create a single image, and in-line apparatuses, which have image-forming units (process stations) of different colors arranged in line to transfer developed images to a transfer material fed by a transfer belt. Among them, in-line apparatuses are advantageous in terms of high speed, high image quality, and a small number of times of image transfer.
An example of the ETB 1 used in the known art is a resin film having a thickness of about 50 to 200 μm and a volume resistivity of about 109 to 1016 Ωcm and formed of, for example, polyvinylidene fluoride (PVdF), an ethylene-tetrafluoroethylene copolymer (ETFE), a polyimide, polyethylene terephthalate (PET), or a polycarbonate. Another example is a resin film including, for example, a base layer having a thickness of about 0.5 to 2 mm and formed of a rubber, such as an ethylene-propylene-diene monomer (EPDM), and a surface layer formed by dispersing a fluoropolymer, such as polytetrafluoroethylene (PTFE), in a urethane rubber. Such resin films may have, for example, an acrylic coating to increase glossiness.
The image-forming process of the in-line image-forming apparatus will now be described. First, the image-forming process of the process stations 201, 202, 203, and 204 is described below. The description focuses on the image-forming process of the yellow process station 201, although the other process stations 202, 203, and 204 have similar image-forming processes.
Next, the transfer process is described below.
In reversal development, a commonly used development process, a negatively charged toner, for example, is used for development of exposed areas on a negatively charged organic photoconductor (OPC). Hence, bias power supplies 4 apply a positive transfer bias to the transfer rollers 3. The transfer rollers 3 used are typically low-resistance rollers.
In actual printing, the image-forming process, the transfer process, and the feeding of the transfer material P are performed at such timings that toner images of the individual colors are aligned on the transfer material P. These processes are controlled according to the moving speed of the ETB 1 and the distances between the transfer positions of the process stations 201, 202, 203, and 204. A single toner image is created on the transfer material P each time the transfer material P passes through the process stations 201, 202, 203, and 204. After the creation of the toner image, the transfer material P is allowed to pass through a known fusing unit which in turn fuses the toner image on the transfer material P.
Image density varies with the temperature/humidity conditions under which the image-forming apparatus is used and the frequency with which the process stations 201, 202, 203, and 204 are used. Such density variations are corrected by image density control described below.
In
The image density control is intended to maintain a constant maximum density for each color (hereinafter referred to as Dmax control) and to maintain halftone characteristics linear with respect to image signals (hereinafter referred to as Dhalf control). The Dhalf control also has great significance in maintaining a constant color balance and preventing spatters from toner characters of overlapping colors and defective fusion due to excessive amounts of toner deposited.
In the Dmax control, generally, image-forming conditions are controlled by detecting toner patches formed under different image-forming conditions using an optical sensor and determining such conditions that the desired maximum density can be achieved according to the detection results. Halftone toner patches are often formed in the Dmax control. The detection of solid images causes difficulty in providing sufficient detection accuracy because of the narrow range of variations in sensor output relative to variations in the amount of toner. The Dmax control based on the detection of toner patches is not required for systems in which the maximum density for each color depends more largely on the thickness of an OPC and image-forming environments than on image-forming conditions. Such systems are advantageous in terms of usability and toner consumption because the image-forming conditions of the systems can be determined according to environment detection results and CRG tag information.
The Dhalf control cancels out γ characteristics to prevent formation of unnatural images due to deviations of output densities from input image signals and thus enable image processing with linear input/output characteristics. In the Dhalf control, toner patches corresponding to different input image signals are detected using an optical sensor to determine the relationship between input image signals and densities. The controller 31 then converts image signals input from the host computer 20 on the basis of the signal-density relationship to determine the density desired for the input image signals. The Dhalf control is generally performed after the image-forming conditions are determined by the Dmax control.
The toner patches formed on the ETB 1 are electrostatically recovered into the process stations 201, 202, 203, and 204 by a cleaning process. The toner of the toner patches, as well as the toner left after the transfer process, is attracted to the photosensitive members 211 by applying a reverse bias thereto and is scraped off by the cleaning blades 217. The method used for cleaning the ETB 1 is not limited to the electrostatic recovery described above and can also be performed by physical recovery, for example, by bringing a cleaning blade into contact with the ETB 1.
If a density sensor is disposed opposite one of rollers supporting a belt-like rotating medium, foreign matter adhering to the opposite roller, for example, can produce an adverse effect on sensor output despite only small positional variations in glossiness existing on the belt-like rotating medium. This problem is particularly serious for detection of toner patches with lower densities. This problem remains the same for a system with large positional variations in glossiness on a belt-like rotating medium even if sensor outputs measured on toner patches are normalized with respect to those measured on the rotating medium to cancel out variations in the amount of reflected light due to the rotating medium. This problem can be avoided in the normalization method if the circumference of the rotating medium is equal to an integral multiple of that of the opposite roller.
In practice, however, such an integral multiple relationship is often difficult to select because the selection of the circumferences of the rotating medium and the opposite roller is restricted by, for example, the height of the image-forming apparatus. Variations in the amount of light reflected by the rotating medium can be correctly estimated by a modified averaging process if the variations form a sinusoidal curve due to variations in the outer diameter of the opposite roller.
In an example of the averaging process, the amounts of reflected light are detected on the rotating medium or toner patches at regular intervals over a range equivalent to the circumference of the opposite roller. The detection results may be averaged to cancel out misdetection due to the opposite roller. The amount of reflected light can then be correctly estimated by subtracting variations in the amount of reflected light due to the rotating medium. Variations in the amount of reflected light due to foreign matter adhering to the opposite roller, however, are difficult to cancel out by the averaging process because such variations form a periodic but asymmetrical wave.
In light of the above problems, the present invention provides an image-forming apparatus that can accurately measure the density of toner deposited on a belt-like moving medium, such as an ITB or an ETB, with a density sensor even if, for example, foreign matter adheres to a roller disposed opposite the sensor.
An image-forming apparatus according to the present invention includes a plurality of rollers, a belt-like moving medium suspended on the rollers, an image-forming unit that forms a toner image on the belt-like moving medium, an optical sensor that is disposed opposite one of the rollers and produces outputs, a storing unit that stores the outputs produced by the optical sensor in an area where no toner image is formed on the belt-like moving medium, and a determining unit that determines the density of a toner patch image formed by the image-forming unit by correcting an output produced when the optical sensor detects the toner patch image at a position on the roller disposed opposite the sensor on the basis of an output selected from the outputs stored in the storing unit. The selected output is produced at the same position on the roller disposed opposite the sensor as the position where the sensor detects the toner patch image.
The image-forming apparatus according to the present invention can measure the densities of toner patches more accurately by providing an non-toner area with a length that is larger than or equal to the circumference of the roller disposed opposite the optical sensor together with the toner patches and correcting the densities of the toner patches on the basis of sensor outputs produced in the non-toner area.
Further features of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.
Exemplary embodiments of the present invention will now be described with reference to the attached drawings, although the invention is not limited to the embodiments described herein.
A first embodiment of the present invention is described below with reference to
An ETB 1 used in this embodiment is a resin belt including a PVdF film having a circumference of 700 mm and a thickness of 100 μm and an acrylic coating having a thickness of 1 μm. The structure of an optical sensor 13 is schematically illustrated in
In
The properties of reflected light detected when the optical sensor 13 illuminates a toner patch is described in detail below.
As shown in
A density sensor designed to detect specularly reflected light may be used because this type of sensor can measure the amount of black toner on a black ETB. Typical ETBs often have a black or dark gray color because carbon black is dispersed therein for resistance adjustment. A light-receiving element for detecting the amount of diffused reflected light (not shown) may be provided to accurately detect highly chromatic colors.
In this embodiment, the density sensor 13 is disposed opposite a drive roller 6 having a circumference of 74 mm so that the drive roller 6 can support the ETB 1 from backside to stabilize the behavior thereof during rotation. Although the density sensor 13 is disposed opposite the drive roller 6 in this embodiment, the density sensor 13 may be disposed opposite any of rollers supporting the ETB 1, including a roller 7 disposed opposite an attraction roller 5 and tension rollers 8 and 9. In this embodiment, the density sensor 13 is disposed opposite the roller with the largest circumference, namely, the drive roller 6, because the sensor 13 requires higher positional accuracy in the rotational direction as the opposite roller has a smaller circumference.
The ETB 1, as described above, exhibits a stable behavior if the density sensor 13 is disposed opposite any of the rollers supporting the ETB 1. The output of the density sensor 13, however, is susceptible to the state of the opposite roller because the ETB 1 does not have a circumference equal to an integral multiple of that of the opposite roller in this embodiment. That is, foreign matter of unpredictable size can adhere to the opposite roller at unpredictable positions. In the known art, such foreign matter can make it difficult to accurately detect the density of a toner patch. Examples of such foreign matter include dust deposited during manufacturing and ETB shavings left after the use of the image-forming apparatus.
Unlike a substantially sinusoidal sensor output due to variations in the outer diameter of the opposite roller, a sensor output with variations due to foreign matter adhering to the opposite roller forms a periodic but asymmetrical wave (nonsinusoidal wave). Such variations are difficult to remove by an output-averaging process because this process is intended for symmetrical waves. In addition, the averaging process requires an enormous number of sampling points to grasp an output waveform because variations in the amount of reflected light due to the opposite roller vary for individual apparatuses and form a complicated waveform.
A Dhalf control in this embodiment which can cancel out the effect of foreign matter adhering to the opposite roller is described below. In the Dhalf control, the toner density measurement is performed in an area where no toner is deposited on a surface of the ETB 1 without determining and subtracting variations in the amount of reflected light due to the surface of the ETB 1 and the opposite roller, which contribute to misdetection. Hence, the toner density measurement involves misdetection due to, for example, foreign matter adhering to the opposite roller. The misdetection can be revealed from the calculation results of the toner density measurement. The toner densities of toner patches of the individual colors are finally determined by subtracting the misdetection due to the opposite roller from measurements of the toner densities of the toner patches. Ideally, the detection of the non-toner area should result in a toner density of zero; if a certain toner density is detected in the non-toner area, the toner density is fed back to the measurements of the densities of the toner patches as misdetection due to the opposite roller.
In this embodiment, toner deposited on the ETB 1 is electrostatically recovered as in the example of the known art, rather than using a cleaning member for physically scraping off the toner. Toner images formed on the ETB 1 therefore remain during the density control. The toner images remain similarly if a cleaning member that can be separated from the ETB 1 is used.
In this embodiment, a non-toner area (white patch) with a length equivalent to the circumference of the drive roller 6 is provided together with the toner patches of the individual colors. In addition, each of the distances between the leading ends of the toner patches is equal to the circumference of the drive roller 6. Referring to
An exemplary correction process is described below. The control system of the image-forming apparatus in this embodiment is similar to that of the image-forming apparatus of the known art, and the description thereof is omitted.
Referring to
One averaged sensor output is stored in the memory region for each halftone. Relatively large variations in the amount of reflected light due to the ETB 1 used in this embodiment are canceled out by a known method of calibrating (for example, normalizing) sensor outputs measured on toner patches with respect to those measured on a belt. In this embodiment, sensor outputs measured at positions on the ETB 1 where the toner patches are to be formed in the first revolution of the ETB 1 are stored and used to normalize sensor outputs measured on the toner patches formed on the ETB 1 in the second revolution of the ETB 1.
In this embodiment, a reference patch is formed on the ETB 1 to measure and store the time required for one revolution of the ETB 1, thereby aligning the detection positions of the ETB 1 and the toner patches. The time required for one revolution of the ETB 1 may also be determined using, for example, a reference mark or tape provided on the ETB 1 when the ETB 1 is formed.
If a sensor output Ps measured on the toner patches is normalized with respect to a sensor output Pb measured on the ETB 1 as described above, the normalized sensor output Ps/Pb is ideally 1.00 in the non-toner area. That is, the toner density decreases as the normalized sensor output Ps/Pb approaches 1.00 and increases as the normalized sensor output Ps/Pb approaches 0. The actual toner density is determined by converting the normalized sensor output Ps/Pb according to the properties of each color.
If foreign matter adheres to the drive roller 6, the foreign matter forms a bump on the ETB 1, and thus the light-receiving element 302 can fail to detect part of reflected light (
Misdetection due to foreign matter adhering to the drive roller 6 depends largely on the size and shape of the foreign matter and occurs at a substantially constant rate each time the drive roller 6 rotates. Hence, the measured densities of the toner patches can be corrected by measuring misdetection at each phase on the drive roller 6.
An exemplary conversion method is described below with the measurement of yellow toner density as an example. A corrected value of a sensor output measured at the n-th halftone segment of the yellow toner patch by a known method, Y(n)′, is represented by the following equation:
Y(n)′=Y(n)/W(n)
wherein Y(n) is a normalized value of the sensor output measured at the n-th halftone segment; and W(n) is a normalized value of a sensor output measured in the non-toner area at the position corresponding to the n-th halftone segment (at the same phase on the drive roller 6).
In this embodiment, W(n) is measured in the same manner as the measurement of normal toner patches; that is, the non-toner area is detected at eight positions corresponding to eight halftone segments. The measurement results are stored in the memory (Step 3). After the detection of the non-toner area is finished (Step 4), the correction process continues to the detection of the toner patches of the individual colors. Next, Y(n) is measured, corrected, and stored in the memory for each halftone segment (Steps 5 and 6).
The detection is repeated for the toner patches of the other colors. Corrected values of sensor outputs measured on the toner patches can be represented by the following equations:
Bk(n)′=Bk(n)/W(n)
C(n)′=C(n)/W(n)
M(n)′=M(n)/W(n)
After the memory stores the corrected values of the sensor outputs measured on the toner patches of all four colors (Step 7), the corrected values are converted according to the properties of each color to determine the toner densities of the toner patches (Step 8). The toner densities are then subjected to γ correction (Step 9) to complete the halftone correction process (Step 10). As described above, the corrected sensor outputs can be converted according to the properties of each color to determine toner densities with higher accuracy.
The conversion method used is not limited to the example described above, and any method that would enable practice of the present invention is applicable. For example, the conversion may be performed by compensating for the amount of misdetection by addition or subtraction. The method used for determining the density of toner deposited on the ETB 1 on the basis of sensor outputs is not limited to any particular method, and any method that would enable practice of the present invention is applicable. For example, conversion tables or conversion formulas may be used as in this embodiment.
In this embodiment, the non-toner area with a length equivalent to the circumference of the drive roller 6 is provided together with the toner patches so that the total length thereof is not larger than the circumference of the ETB 1, thereby correcting misdetection due to the drive roller 6 more accurately. For systems including an ETB with a significantly stable circumference, misdetection due to a roller disposed opposite a density sensor can be estimated because of the stable relationship between the circumferences of the ETB and the opposite roller even if the total length of toner patches and a non-toner area is larger than the circumference of the ETB.
On the other hand, measurements on toner patches may be corrected as in this embodiment for systems including an ETB that experiences variations in circumference due to the use environment or has dimensional variations in manufacturing. The length of the non-toner area may be larger than or equal to the length of the toner patch of each color (72 mm in this embodiment). In this embodiment, the circumference of the drive roller 6 is close to the length of the toner patch of each color, and the length of the non-toner area is equal to the circumference of the drive roller 6.
The resin used for the ETB 1 in this embodiment, PVdF, has a linear expansion coefficient of about 14×10−5/° C., and thus can experience a change in circumference of 1 to 3 mm, depending on the use environment. As a result, the ETB 1 can cause a deviation in detection position equivalent to the change in circumference.
In this embodiment, as described above, the non-toner area with a length equivalent to the circumference of the drive roller 6 is provided together with the toner patches, and each of the distances Ld between the leading ends of the toner patches is equal to the circumference of the drive roller 6. This embodiment can thus provide a simple method for correcting the densities of the toner patches. In addition, the profile of the non-toner area does not have to be determined in detail over the length equivalent to the circumference of the drive roller 6. The memory capacity used may thus be reduced by storing only sensor outputs measured in the non-toner area at necessary roller phases.
If the ETB 1 is formed of a material that causes no variation in sensor output, such as a polyimide, the sensor outputs measured on the toner patches may be directly used to determine the densities thereof. In this case, for example, a corrected value of a sensor output measured at the n-th halftone segment of the yellow toner patch by a known method, y(n)′, is represented by the following equation:
y(n)′=y(n)/w(n)
wherein y(n) is the sensor output measured at the n-th halftone segment; and w(n) is a sensor output measured in the non-toner area at the position corresponding to the n-th halftone segment (at the same phase on the drive roller 6). The use of such a material for the ETB 1 is advantageous in terms of usability because it can eliminate the need for the normalization described above to reduce the time for density control.
If the sensor outputs measured on the toner patches are normalized with respect to those measured on the ETB 1 as in this embodiment, either the measurement of the sensor outputs on the toner patches or the measurement of the sensor outputs on the ETB 1 may be performed prior to the other measurement. If a cleaning member adjacent to the ETB 1 is not provided, the measurement of the sensor outputs on the ETB 1 may be performed prior to the measurement of the sensor outputs on the toner patches to reduce the time for the Dhalf control and thus enhance usability.
The non-toner area may be positioned upstream or downstream of the toner patches in the process direction or between any two of the toner patches.
Although the image-forming apparatus including the ETB 1 has been described in this embodiment, the embodiment may also be applied to an image-forming apparatus including an ITB suspended on suspension rollers and a density sensor disposed opposite one of the rollers, as mentioned in the description of the known art.
As described above, toner density can be detected with higher accuracy by providing a non-toner area with a length that is larger than or equal to the circumference of the roller disposed opposite the density sensor 13 together with the toner patches, estimating misdetection due to foreign matter adhering to the opposite roller according to sensor outputs measured in the non-toner area, and correcting the results of measurements on the densities of the toner patches.
A second embodiment of the present invention is substantially the same as the first embodiment except that a non-toner area with a length that is at least twice the circumference of the roller disposed opposite the density sensor 13 is provided near the toner patches. The non-toner area allows the estimation of misdetection due to foreign matter adhering to the opposite roller with higher accuracy.
Referring to
The method according to this embodiment allows the estimation of misdetection due to foreign matter adhering to the opposite roller with higher accuracy to suppress the maximum misdetection to 3% or less.
A third embodiment of the present invention is substantially the same as the second embodiment except for the features described below. In the third embodiment, a non-toner area with a length that is at least twice the circumference of the roller disposed opposite the density sensor 13 is provided upstream of the toner patches in the process direction. The results of misdetection are stored for each revolution of the opposite roller and are compared between the revolutions of the opposite roller. The comparison results are used to correct the densities of the toner patches. The non-toner area, for example, has a length that is twice the circumference of the opposite roller (first and second non-toner areas).
If the results for the first and second non-toner areas have similar tendencies, they may be averaged and used as data for density correction, as in the second embodiment. If, on the other hand, the results have significantly different tendencies, the measured densities of the toner patches are corrected on the basis of the outputs measured in the non-toner area immediately before the toner patches.
Referring to the profile graph of
In this embodiment, the data on the second non-toner area is compared with the data on the first non-toner area for each halftone segment after the normalization of the sensor outputs measured on the toner patches. If the comparison reveals a difference of 2.5% or more, the foreign matter is determined to be displaced, and thus the data on the non-toner area immediately before the toner patches is used alone for correction, rather than averaging the results for the two non-toner areas. The method used is not limited to the example described above, and any method that would enable practice of the present invention is applicable. For example, the Dhalf control may be repeated to achieve higher measurement accuracy if the data on the first and second non-toner areas has significantly different tendencies.
The correction method in this embodiment allows the determination whether foreign matter has been displaced or not. Hence, this method not only can achieve high correction accuracy as described in the previous embodiments, but also can reduce the occurrence of rare correction failures such as excessive correction and insufficient correction. The non-toner areas, which are provided upstream of the toner patches in the process direction in this embodiment, may also be provided downstream of the toner patches. In this case, the densities of the toner patches may be corrected using the data on the non-toner area immediately after the toner patches.
While the present invention has been described with reference to exemplary embodiments, it is to be understood that the invention is not limited to the disclosed exemplary embodiments. The scope of the following claims is to be accorded the broadest interpretation so as to encompass all modifications, equivalent structures and functions.
This application claims the benefit of Japanese Application No. 2005-226521 filed Aug. 4, 2005, which is hereby incorporated by reference herein in its entirety.
Number | Date | Country | Kind |
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2005-226521 | Aug 2005 | JP | national |