This application is based on and claims priority under 35 USC 119 from Japanese Patent Application No. 2016-059309 filed Mar. 24, 2016.
1. Technical Field
The present invention relates to an discharging light quantity adjusting device and an image forming apparatus.
2. Related Art
In some cases, an image including a residual image of a previously formed image may be formed due to a light exposure history of an image holding member.
According to an aspect of the invention, there is provided an discharging light quantity adjusting device for adjusting a discharging light quantity to be irradiated by an discharging unit in an image forming section that performs a toner image forming process by charging, exposure, and development to an image holding member, the image forming section including: the image holding member on which a toner image is formed while the image holding member rotates and which holds the formed toner image; a charging unit that electrically charges the image holding member; an exposure unit that exposes the image holding member to light so as to form a latent image by a potential distribution on the image holding member; a developing unit that develops the latent image formed on the image holding member by toner so as to form a toner image on the image holding member; a transfer unit that transfers the toner image formed on the image holding member onto a transfer object; the discharging unit that irradiates discharging light onto the image holding member so as to electrically discharge the image holding member; a cleaner that cleans toner remaining on the image holding member after transfer; and an electrometer that measures an electrostatic potential on the image holding member,
wherein the discharging light quantity adjusting device including:
a potential measurement controller that performs:
a first process of causing the image forming section to perform a first toner image forming process to electrically charge the image holding member to a first target potential, and causing the electrometer to measure an electrostatic potential on the image holding member so as to obtain a first measured value,
a second process of causing the image forming section to perform a second toner image forming process to electrically charge the image holding member to a second target potential different from the first target potential and removing, from the image holding member, a toner image formed on the image holding member by the second toner image forming process, and
a third process of causing the image forming section to perform a third toner image forming process to electrically charge the image holding member to a third target potential and causing the electrometer to measure an electrostatic potential on the image holding member so as to obtain a second measured value; and
a light quantity adjusting unit that adjusts a quantity of the discharging light to be irradiated by the discharging unit based on the first and second measured values.
Exemplary embodiments of the present invention will be described in detail based on the following figures, wherein:
Hereinafter, exemplary embodiments of the present invention will be described.
A paper hopper 11 accommodates a paper P in a folded state. The paper P accommodated in the paper hopper 11 is transported in the direction of the arrow A by a front tractor 13 and an upstream tractor 14 via a transfer position facing a photoreceptor 20, and further transported in the direction of the arrow B by a downstream tractor 15 so that the paper P is accommodated in a folded state on a paper stacker 12 via a flash fixing device 16.
The photoreceptor 20 has a drum shape and rotates in the direction of the arrow R. A charging unit 21, an exposure unit 22, and a developing unit 23 are arranged around the photoreceptor 20, and a toner image is formed on the photoreceptor 20 by charging, exposing, and developing processes. The toner image formed on the photoreceptor 20 is transferred onto the paper P by a transfer unit 24.
After the transfer, the photoreceptor 20 is electrically discharged by a discharging unit 25, and cleaned by a cleaner 26 including a cleaning brush 261 and a cleaning blade 262.
The toner image transferred onto the paper P advances into a flash fixing device 16 along with the transport of the paper P, and is irradiated by flash light from the flash fixing device 16 so as to be fixed on the paper P. Scattering toner or fine paper powders generated during the flash light emission by the flash fixing device 16 are sucked by a suction unit 17. Thereafter, the paper P is accommodated on the paper stacker 12.
The book sheeting printer 10 includes a controller 30, and the above-described operations are performed under a control by the controller 30.
Further, the book sheeting printer 10 includes an electrometer 27 that measures a surface potential of the photoreceptor 20. Potential data obtained through the measurement by the electrometer 27 is input to the controller 30. Based on the received potential data, the controller 30 calculates a light quantity of discharging light to be irradiated from the discharging unit 25 to the photoreceptor 20, and controls the discharging unit 25 to irradiate the calculated light quantity of discharging light to the photoreceptor 20. Details will be described later.
Here, prior to describing the exemplary embodiment, a residual image and a cause for the occurrence of the residual image will be described.
In each of the images 50a, 50b, 50c, . . . , “ABCDEFG” characters 52 and a halftone
While rotating, the photoreceptor 20 repeats a cycle that includes electric charge by the charging unit 21, exposure by the exposure unit 22, development by the developing unit 23, transfer of a toner image formed by the development onto paper P through the transfer unit 24, and discharging by the discharging unit 25.
(A) of
(B) of
(C) and (D) of
(E) of
Like (C) of
When the discharging light quantity is deficient, as described above with reference to
Meanwhile, when the discharging light quantity is excessive, as illustrated in (F) of
Although the toner image formed on the photoreceptor 20 is transferred onto the paper P by the operation of the transfer unit 24, the toner forming the toner image partially remain on the photoreceptor 20 rather than being thoroughly (100%) transferred. In this case, when an excessive quantity of discharging light is irradiated, the location on the photoreceptor 20 where the toner of the toner image did not exist prior to the transfer is electrically discharged strongly, but in the location where the toner existed, the discharging light is partially blocked by the remaining toners after the transfer, and the location is not electrically discharged to the same extent as that of the location where the toners did not exist. In this case, the negative residual image may occur as illustrated in (F) of
That is, a residual image may occur in both the case where the discharging light is too strong and the case where the discharging light is too weak. Thus, it is required to irradiate an appropriate quantity of discharging light which is neither overly strong nor overly weak.
In
As illustrated in
A discharging light quantity adjusting mode in the exemplary embodiment will be described based on the above descriptions of the residual image phenomenon and the cause of occurrence of the residual image phenomenon.
This discharging light quantity adjusting mode is executed, for example, when a power is supplied to the book sheeting printer 10 or at a timing designated by an operator.
In the discharging light quantity adjusting mode, the surface potential of the photoreceptor 20 is measured, and the discharging light quantity to be irradiated to the photoreceptor 20 is adjusted by the discharging unit 25 according to the measured surface potential, under the control of the controller 30 illustrated in
In the measurement of the surface potential of the photoreceptor 20, the first process performs a first toner image forming process that electrically charges the photoreceptor 20 with a first target potential and causes the electrometer 27 to measure an electrostatic potential on the photoreceptor 20 so as to obtain a first measured value. Specifically, in the exemplary embodiment, in the first process, an electrostatic latent image P1 having a 0% halftone dot density as a first target potential is formed on the photoreceptor 20 over the length corresponding to the one round of the photoreceptor 20. Since the electrostatic latent image P1 has the 0% halftone dot density, the image is not developed by the developing unit 23, and in other words, become a toner image in blank form.
In the first process, the potential of the 0% halftone dot density is measured by the electrometer 27. This means that the potential after charge as illustrated in (A) of
In addition, the second process is a process of performing a second toner image forming process that charges the photoreceptor 20 with a second target potential different from the first target potential, and remove, from the photoreceptor 20, the toner image formed on the photoreceptor 20 by the second toner image forming process. Specifically, in the exemplary embodiment, an electrostatic latent image P2 having a 100% halftone dot density as the second target potential is formed on the photoreceptor 20. The electrostatic latent image P2 having the 100% halftone dot density is also formed over the length corresponding to the one round of the photoreceptor 20, like the electrostatic latent image P1 of the 0% halftone dot density. In addition, as illustrated in
The electrostatic latent image P2 having the 100% halftone dot density is developed by the developing unit 23, thereby forming a toner image of which the entire face is full of toner. This toner image is transferred onto the paper P, and the remaining toner is removed by the cleaner 26.
In addition, the third process is a process of performing a third toner image forming process that charges the photoreceptor 20 to a third target potential and causes the electrometer 27 to measure the electrostatic potential on the photoreceptor 20 so as to obtain a second measured value. Specifically, in the exemplary embodiment, in the third process, an electrostatic latent image P3 having a 0% halftone dot density as the third target potential is formed over the length corresponding to the one round of the photoreceptor 20, as in the above-described first process. In the third process, the potential of the electrostatic latent image P3 having the 0% halftone dot density is measured by the electrometer 27 over the one round of the photoreceptor 20, and an average potential thereof is calculated.
The potential obtained by the third process corresponds to the potential dropped due to a residual image as illustrated in (E) of
In the discharging light quantity adjusting mode, a differential potential between the potential obtained in the first process and the potential obtained in the third process is calculated. Then, the discharging light quantity is adjusted in the direction of the plus or minus sign of the differential potential by a quantity corresponding to an absolute value of the differential potential.
In this case, the characteristics of the photoreceptor 20 or the discharging unit 25 that is actually used in the book sheeting printer 10 may be measured in advance, or the usage history of, for example, the photoreceptor 20 or the discharging unit 25 may be inspected so that the discharging light quantity may be adjusted to be within the residual image allowable range or to the residual image intensity 0V (see
According to the exemplary embodiment, the discharging light quantity may be adjusted to be within the residual image allowable range, in spite of the change of the characteristic of the photoreceptor 20 (see
In addition, in the exemplary embodiment, while descriptions have been made assuming that each of the first and third target potentials is a potential of an electrostatic latent image having the 0% halftone dot density, each of the first and third target potentials is not required to be a potential of an electrostatic latent image having the 0% halftone dot density. However, a current residual image level can be calculated with higher accuracy in a case where the potential difference of the first and third target potentials from the second target potential is larger. Therefore, it is desirable that each of the first and third target potentials is the potential of the 0% halftone dot density.
In addition, in the exemplary embodiment, while descriptions have been made assuming that the second target potential is a potential of an electrostatic latent image having the 100% halftone dot density, the second target potential is not required to be a potential of an electrostatic latent image having the 100% halftone dot density. However, a current residual image level can be calculated with higher accuracy in a case where the potential difference of the second target potential from the first target potential and the third target potential is larger. Therefore, it is desirable that the second target potential is the potential of the 100% halftone dot density.
In addition, the first and third target potentials are not required to be the same, and even when the first and third target potentials are different from each other, the current residual image level may be calculated after potential measurement. However, the calculation may be facilitated when the first and third target potentials are set in advance. Further, in order to maximize the potential differences between the first and second target potentials and between the second and third target potentials, as described above, both the first and third target potentials are required to be equal to the potential of the 0% halftone dot density.
In addition, in the exemplary embodiment, all the electrostatic latent image P1 of the 0% halftone dot density in the first process, the electrostatic latent image of the 100% halftone dot density in the second process, and the electrostatic latent image of the 0% halftone dot density in the third process are formed to have the length corresponding to the one round of the photoreceptor 20. In the measurement of the average potential over the one round of the photoreceptor 20, it is sufficient if each of the electrostatic latent images P1, P2, and P3 has a length corresponding to the one round of the photoreceptor 20. Formation of a longer electrostatic latent image may cause waste of time or toner.
In addition, even in a case where each of the electrostatic latent images P1, P2, and P3 is shorter than the length corresponding to the rotation cycle of the photoreceptor 20, it is possible to adjust the discharging light quantity by performing a potential measurement for the location when the respective electrostatic latent images P1, P2, and P3 are formed at the same location on the photoreceptor 20. However, when the measurement result for the one round of the photoreceptor 20 is adopted, the discharging light quantity may be favorably adjusted over the entire circumference of the photoreceptor 20.
In addition, in the exemplary embodiment, the book sheeting printer 10 illustrated in
The foregoing description of the exemplary embodiments of the present invention has been provided for the purposes of illustration and description. It is not intended to be exhaustive or to limit the invention to the precise forms disclosed. Obviously, many modifications and variations will be apparent to practitioners skilled in the art. The embodiments were chosen and described in order to best explain the principles of the invention and its practical applications, thereby enabling others skilled in the art to understand the invention for various embodiments and with the various modifications as are suited to the particular use contemplated. It is intended that the scope of the invention be defined by the following claims and their equivalents.
Number | Date | Country | Kind |
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2016-059309 | Mar 2016 | JP | national |
Number | Date | Country |
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57161872 | Oct 1982 | JP |
H05-289458 | Nov 1993 | JP |
2008-191554 | Aug 2008 | JP |
2008-310311 | Dec 2008 | JP |
Number | Date | Country | |
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20170277063 A1 | Sep 2017 | US |