1. Field of the Invention
The present invention relates to an image forming apparatus.
2. Description of the Related Art
One problem of an image forming apparatus is that the surface potential of a photosensitive drum (photoreceptor) changes due to various factors, which results in a drop in image quality. For example, if the quantity of laser light emitted from a scanner unit drops, the surface potential of the photosensitive drum may become lower than a desired potential, whereby image quality deteriorates. Here a technique to detect the drop in quantity of laser light based on a transfer current amount is known (Japanese Patent Application Laid-Open No. 2012-155075).
Various factors may cause a drop in the quantity of the laser light. For example, if the image forming apparatus is continuously used in air in which such micro-foreign matter as dust and chemical substances are floating, the foreign matter enters the apparatus main body and adheres to the laser light source and other optical components inside the scanner unit. The deposition of dust on the surface of such optical components as a reflection mirror and an imaging lens of the scanner unit causes a gradual drop in reflectance and transmittance, whereby the quantity of laser light emitted from the scanner unit drops. On the other hand, if foreign matter adheres to an emission point of a laser element, such as a laser diode, the quantity of laser light drops dramatically. Therefore a technique to accurately determine a factor that causes a drop in the quantity of laser light is demanded.
With the foregoing in view, it is an object of the present invention to accurately determine a factor that causes a drop in the quantity of laser light.
To achieve the above object, an image forming apparatus according to the present invention has:
a light emitting member that includes a first emission portion to which drive current is supplied and from which first laser light is emitted;
a photoreceptor to which the first laser light is emitted;
a detection portion that detects a value on a surface potential of the photoreceptor; and
a determination portion that determines an abnormality of the light emitting member, wherein
the detection portion detects, a plurality of times, a value on the surface potential of a portion of the photoreceptor to which the first laser light is emitted, and the determination portion determines whether the light emitting member is in an abnormal state, based on a change amount of the value on the surface potential detected by the detection portion.
To achieve the above object, an image forming apparatus according to the present invention has:
a first light emitting member that includes a first emission portion emitting first laser light and a second emission portion emitting second laser light, and that emits the first laser light and the second laser light by supply of a common first drive current;
a second light emitting member that includes a third emission portion emitting third laser light and a fourth emission portion emitting fourth laser light, and that emits the third laser light and the fourth laser light by supply of a common second drive current;
a photoreceptor to which the first laser light and the third laser light are emitted;
a light receiving portion that receives the second laser light and the fourth laser light;
a light quantity control portion that controls a light quantity of the first laser light, which is emitted to the photoreceptor, based on the light quantity of the second laser light received by the light receiving portion, and controls a light quantity of the third laser light, which is emitted to the photoreceptor, based on the light quantity of the fourth laser light received by the light receiving portion;
a detection portion that detects a value on a first surface potential of a portion of the photoreceptor to which the first laser light is emitted, and a value on a second surface potential of a portion of the photoreceptor to which the third laser light is emitted; and
a determination portion that determines an abnormality of the light emitting member, wherein
the determination portion determines that the light emitting member is in an abnormal state when only one of the value on the first surface potential and the value on the second surface potential, detected by the detection portion, is a first predetermined value or more, and also determines that the light emitting member is in an abnormal state when only one of the value on the first surface potential and the value on the second surface potential, detected by the detection portion, is a second predetermined value or less.
Further features of the present invention will become apparent from the following description of exemplary embodiments (with reference to the attached drawings).
Embodiments of the present invention will now be described in detail based on examples with reference to the drawings. The dimensions, materials, shapes and relative dispositions or the like of the components described in the embodiments may need to be appropriately changed depending on the configuration and various conditions of the apparatus to which the present invention is applied. In other words, the scope of the invention is not limited to the following embodiments.
With reference to
The image forming apparatus 100 includes a paper feeding cassette 101 where recording sheets are set, a pick up roller 102 that picks up paper, a paper feeding roller 103 that feeds and transports paper, a fixing apparatus 104 that fixes a toner image on paper, and a paper ejecting roller 105 that ejects paper. The image forming apparatus 100 also includes an image forming process portion 106 that performs charging, exposure, development, transfer or the like.
Paper that is set in the paper feeding cassette 101 is picked up by the pick up roller 102, and is fed and transported by the paper feeding roller 103. Then the toner image is transferred to the paper in the image forming process portion 106, and the toner image is fixed on the paper by the fixing apparatus 104. Then [the paper] is ejected from the image forming apparatus 100 by the paper ejecting roller 105.
Now, details on the image forming process portion 106 will be described with reference to
A transfer bias generated by the transfer circuit 206 (voltage applying portion) is applied to the transfer roller 204. The transfer circuit 206 can change the output bias value and polarity to positive/negative by the control portion 107 that controls the operation sequence of the image forming apparatus. The current detection circuit 210 can detect current A that flows from the transfer circuit 206 to the transfer roller 204, the photosensitive drum 201, and a drum earth 209.
In the non-image area, the control portion 107 detects information acquired by the current detection circuit 210 when DC voltage is applied to the transfer roller 204. The control portion 107 determines the discharge start voltage between the photosensitive drum 201 and the transfer roller 204 based on each of the detected current values, and calculates the surface potential VL on the photosensitive drum 201 (hereafter called “drum potential VL”) using the determination result. The image forming process, including the charging of the photosensitive drum 201, exposure to light by the scanner unit 207 or the like using the above procedure, is controlled by the control portion 107 that controls the image forming apparatus constituted by a CPU, ASIC or the like.
<Scanner Unit>
Now the scanner unit of this example will be described with reference to
As shown in
The imaging lens 404 is designed to scan the photosensitive drum 201 at a constant speed, and the laser light reflected by the reflection mirror 405 forms a spot on the photosensitive drum 201 and scans in the arrow A direction. By the photosensitive drum 201 rotating in the arrow R direction, an electrostatic latent image is formed on the photosensitive drum 201.
If the image forming apparatus 100 is continuously used in air where micro dust and chemical substances are floating, the dust and chemical substances enter the main body of the image forming apparatus 100. Although the scanner unit 207 is located inside the image forming apparatus 100, the micro dust and chemical substances adhere to the optical components or the like inside the scanner unit 207 via an air duct that cools inside the image forming apparatus 100 or the like. If dust is deposited on the surfaces of the reflection mirror 405 and the imaging lens 404, for example, reflectance and transmittance gradually drop.
Example 1 of the present invention will now be described. A package of the laser light source according to Example 1 will be described with reference to
In the can package, the laser diode 304 is mounted on a stem (not illustrated), and is sealed by a metal can 502 on which a glass 501 is adhered. Some can packages are open packages which are not sealed and are without glass 501. In this case, the laser diode 304 is exposed to air.
In this example, a laser light quantity abnormality determination, in the case of using the laser light source 300 in a can package without the glass 501, will be described as an example. The laser diode 304 is created by cleaving end faces on both ends of the resonator, and includes a reflection mirror that transmits a part of the laser light. First laser light that is emitted, passing through the front side reflection mirror of the laser light source 300 (hereafter called “front light”), exposes the photosensitive drum 201 to light. Second laser light that is emitted, passing through the rear side reflection mirror (hereafter called “rear light”), is directed to the PD sensor 305 disposed on the opposite surface. The front light and the rear light are laser light which is emitted by a common drive current supply.
In the laser diode 304 used for the laser light source 300, the laser light is emitted from micro emission points (emission portions). Normally in a laser diode 304 used for the image forming apparatus 100, a size of the emission point is several μm2. Therefore if even one several micro meter sized foreign matter adheres to the front side emission point 304a (first emission portion) of the laser diode 304, the front light is dramatically interrupted, and a desired light quantity may not be acquired on the photosensitive drum 201, or the spot shape may deform. As a result, image quality drops.
If foreign matter adheres to the rear side emission point 304b (second emission portion) of the laser diode 304, the light quantity of the rear light emitted to the PD sensor 305 drops. As mentioned above, the light quantity is controlled to be constant so that the quantity of the light received by the PD sensor 305 becomes constant, hence in this case, the front light quantity becomes higher than the desired light quantity.
The laser light emitted from the emission point of the laser diode 304 spreads, and the spot diameter on an optical component in the scanner unit 207 is larger than the size of the emission point. Further, the polygon mirror 403, the imaging lens 404, the reflection mirror 405 and the like are sequentially scanned, hence if dust adheres to these optical components, light quantity gently drops in accordance with the amount of the adhering dust.
On the other hand, as mentioned above, even one foreign matter adhering to the laser diode 304 dramatically changes the light quantity, since the size of the emission point is small. According to the present invention, the light quantity abnormality (abnormal state) of the laser light source 300 is determined by utilizing the difference of the sensitivity to foreign matter between the laser light source 300 (laser diode 304) and other optical components.
<Drum Potential Measurement>
The measurement of the drum potential will be described in more detail with reference to
Therefore the discharge current that flows between the photosensitive drum 201 and the transfer roller 204 can be calculated using a Δ value generated by subtracting the straight light (1) from the curve (1). Then the voltage when this Δ value reaches a desired current value (e.g. 3 [μA] or −3 [μA]) is determined as the voltage where discharge started. Regarding the discharge characteristics of the photosensitive drum 201, the potential difference required for discharge differs depending on the difference of the environment and the film thickness of the photosensitive drum.
If the surface property of the transfer roller 204 is equivalent to that of the photosensitive drum 201, then as shown in
[Math. 1]
VL=(VDh+VD1)/2 Expression 1
The drum potential after emitting the laser light can also be determined in the same manner. Bias around the estimated drum potential after emitting the laser light is applied, and the discharge start voltage VL1 on the negative side of the estimated drum potential after emitting the laser light and the discharge start voltage VLh on the positive side of the estimated drum potential after emitting the laser light, are determined. Then ½ of the total of the determined VL1 and VLh is determined as the drum potential VL. In other words, the drum potential VL after emitting the laser light can be given by the following Expression 2.
[Math. 2]
VL=(VLh−VL1)/2 Expression 2
<Laser Light Quantity Abnormality Determination Method>
Now a laser light quantity abnormality determination method according to this example will be described with reference to
The abscissa in
Here the plot of the white circles in
As the plot of the white circles in
When laser failure occurs, the absolute value of the change amount of the drum potential in a predetermined period (between X1 and X2 and between X3 and X4 in
A control of determining an abnormality of the laser light quantity by the control portion 107 will be further described with reference to
First when the laser light quantity abnormality determination sequence is started, the photosensitive drum 201 is rotated (S901), and the photosensitive drum 201 is charged with a charging bias (e.g. −350 V) used for printing (S902). Then the laser light is emitted at a predetermined light quantity (S903), and when the electrostatic latent image formed on the photosensitive drum 201 reaches the transfer roller 204 by the rotation of the photosensitive drum 201, a predetermined transfer positive bias is applied (S904).
With gradually increasing the transfer positive bias, the discharge start voltage VLh on the positive side is determined from the current A that flows from the transfer roller 204 to the ground of the photosensitive drum 201 (S905). In the same manner, a predetermined transfer negative bias is applied (S906), and with gradually decreasing the transfer negative bias, the discharge start voltage VL1 on the negative side is determined from the current A (S907). Using the above mentioned Expression 2 with VLh and VL1 determined in S905 and S907, the drum potential VLa after emitting the laser light is calculated (S908). Then the drum potential VLb after emitting the laser light in the previous measurement, which was stored in the storage portion (not illustrated) of the control portion 107, is read (S909), and VLa of the current measurement result is stored in the storage portion (S910).
Then it is checked whether the absolute value of the current measurement result VLa has dropped from the previous measurement result VLb by a predetermined voltage VLs or more, that is, whether the light quantity emitted to the photosensitive drum 201 has increased by a predetermined value or more (S911). If the absolute value has dropped by VLs or more (YES in S911), the control portion 107 determines that the rear side emission point 304b (second emission portion) has an abnormality, and stores the laser light quantity abnormality flag, which indicates a drop in the rear light quantity, in the storage portion (S912). The control portion 107 determines that the rear side emission point 304b has an abnormality in the following cases. One is a case when a predetermined quantity of the laser light cannot be emitted from the rear side emission point 304b even if a predetermined drive current is supplied, because of occurrence of a failure or end of life of the rear side emission point 304b itself. The other is a case when the PD sensor 305 cannot receive a predetermined quantity of the laser light from the rear side emission point 304b even if a predetermined drive current is supplied, because of foreign matter adhering to the rear side emission point 304b.
If the change amount is smaller than VLs (NO in S911), then it is checked whether the absolute value of the current measurement result VLa has increased from the previous measurement result VLb by a predetermined voltage VLs or more. In other words, it is checked whether the light quantity emitted to the photosensitive drum 201 surface is a predetermined value or less (S913). If the absolute value has increased by VLs or more in the result (YES in S913), the control portion 107 determines that the front side emission point 304a (first emission portion) has an abnormality, and stores the laser light quantity abnormality flag, which indicates the drop in front light quantity, in the storage portion (S914). For VLs, potential is determined based on the exposure drop rate when foreign matter adheres to the emission point and is stored in the storage portion in advance. The control portion 107 determines that the front side emission point 304a has an abnormality in the following cases. One is a case when a predetermined quantity of the laser light cannot be emitted from the front side emission point 304a even if a predetermined drive current is supplied, because of a failure or life of the front side emission point 304a itself. The other case is a case when the photosensitive drum 201 cannot be exposed to light at a predetermined light quantity even if a predetermined drive current is supplied, because of foreign matter adhering to the front side emission point 304a.
Then it is determined whether the current measurement result VLa is a value within a first predetermined range (VLt1 or more and VLth or less in
If the absolute value of VLa is higher than VLt1 (NO in S915), it is determined whether the absolute value of the current measurement result VLa is the predetermined voltage VLth or more (S918). If VLa is lower than VLth, the sequence ends (NO in S918), and if VLa is VLth or more (YES in S918), then it is determined that the absolute value of the drum potential is high, which is a VL abnormality (S916), and the charging operation is checked next (S917). For VLth, potential is determined based on the exposure amount at which the printed image quality drops significantly because the front light quantity is low, and this potential value is stored in the storage portion in advance.
Now a process of diagnosis to discern from the factors other than the laser light quantity abnormality related to the abnormalities of exposure amount will be described. First in a state where the laser is not emitted, the photosensitive drum 201 is charged with a charging bias (e.g. −350V) (S917). Then, same controls as those are implemented in S904 to S908 are implemented, and the drum potential is calculated using the above mentioned Expression 1. If the drum potential is a value in a second predetermined range (e.g. −400V or more, −300V or less), it is determined that the charging circuit is operating without problems as the voltage applying portion (NO in S919), and the transfer operation is checked (S920). If the drum potential is a value outside the second predetermined range (YES in S919), on the other hand, the notification portion notifies the high voltage power supply failure (S921).
In the transfer operation check (S920), the photosensitive drum 201 is charged at charging bias 0 V, to check whether the transfer circuit 206 is operating correctly as the voltage applying portion. By sequentially applying a predetermined transfer positive bias and transfer negative bias, it is checked whether the assumed current A, that flows from the transfer roller 204 to the ground of the photosensitive drum 201, is detected respectively. If the detected current is outside a predetermined current range (that is, if the drum potential is outside the second predetermined range) (YES in S922), the notification portion notifies the high voltage power supply failure (S921). If the detected current is within the predetermined range (that is, if the drum potential is within the second predetermined range) (NO in S922), it is determined that the transfer circuit 206 is operating normally and a failure occurred to the scanner unit 207.
Then it is checked whether the laser light quantity abnormality flag is stored in the storage portion (S923), and if stored (YES in S923), the notification portion notifies the user of the laser light quantity abnormality (S924). If the laser light quantity abnormality flag is not stored (NO in S923), on the other hand, the notification portion notifies the user of a failure of an optical component other than the laser diode 304 (S925).
In this example, the previous measurement result is used for VLb, but the same effect can be implemented even if an average value of the measurement results, up to the last measurement time, is used. If the values of VLth and VLt1 are not one value, but change depending on the operating environment and durability of the image forming apparatus 100, the laser light quantity abnormality can be determined with even more accuracy. Here a method of calculating the drum potential, from the discharge start voltage based on the current A flowing from the transfer roller 204 to the ground of the photosensitive drum 201, was described. However, the detection portion may calculate the drum potential based on the current flowing from the charging roller 202 or the developing sleeve 203 to the ground of the photosensitive drum 201.
As described above, in this example, the laser light quantity emitted from the scanner unit 207 is indirectly measured by detecting the drum potential, and the laser light quantity abnormality is detected by checking the change amount of the value related to the drum potential. In other words, in this example it is determined whether the laser diode 304 is abnormal or not based on the change amount of a value related to the surface potential of the photosensitive drum 201. Thereby the laser light quantity abnormality can be detected. Further, the cause of the laser light abnormality can be detected in detail by discerning whether the abnormality is of the front light quantity or the rear light quantity. If service personnel or the like collect the causes of an abnormality and feed it back to design and development, quality of the image forming apparatus can be improved.
If the laser light source 300 generates an abnormal quantity of light that deviates from the desired light quantity, the quality of the print image drops. Moreover, if the front light quantity increases, the photosensitive drum 201 may be damaged. The above mentioned control is an example of determining only a failure, but an abnormality may be determined before a failure occurs if a plurality of thresholds are set for the drum potential. Since the abnormality can be notified to the user before the laser light source 300 completely fails, the downtime of the image forming apparatus 100 due to failure can be reduced.
In this example, a can package without glass 501, where the laser diode 304 is exposed to air, was described as an example, but a can package sealed with glass 501 may be used. In the case of the can package in which the laser diode 304 is sealed by the glass 501, the laser spot diameter on the glass 501 is about 100 μm, for example. In this case, the portion on the glass 501 where the laser light passes through corresponds to the first emission portion of the present invention. In the case of this configuration, the front light quantity suddenly drops when a foreign matter of about 100 μm or larger, adheres to the laser spot on the glass 501.
Example 2 will now be described with reference to
<Configuration of Twin-beam Laser>
The twin-beam laser used in Example 2 will be described first.
The laser light from the front side emission point 304a1 and the rear side emission point 304b1 is emitted by a supply of a common first drive current. The laser light from the front side emission point 304a2 and the rear side emission point 304b2 is emitted by a common second drive current supply.
In a standard twin-beam laser used for the image forming apparatus 100, the interval between resonators, that is the emission points, is about 90 μm. Therefore, even if about a several tens μm sized foreign matter adheres to the end face of the reflection mirror of the laser diode 304, it is rare that the foreign matter covers two emission points. Therefore the laser light quantity abnormality is determined using the phenomena in which the light quantity of only one of the two emission points drops when a foreign matter adheres to the other emission point.
<Laser Light Quantity Abnormality Determination Method>
Now a control to determine the laser light quantity abnormality performed by the control portion 107 according to Example 2 will be described with reference to
A laser is emitted from the laser diode A (LDA) as the first light emitting member on one side of the twin-beam at a predetermined light quantity (S1101). Then the drum potential VL1, after emitting the LDA laser, is calculated (S1102). Then it is checked whether VL2 has been detected by the laser diode B (LDB) as the second light emitting member (S1103), and if not, processing returns to S1101, and a laser is emitted from the LDB on the other side of the twin-beam. Then VL2 is calculated in the same manner for the LDB laser as well (S1102).
When calculation of the drum potentials VL1 and VL2 ends, it is checked whether only one of the measurement result VL1 when the LDA laser was emitted, and the measurement result VL2 when the LDB laser was emitted, is VLhe (first predetermined value) or more (S1104). For VLhe, the potential is determined based on the exposure reduction rate when a foreign matter adheres to one of the front side emission points, and this potential value is stored in advance. If only one of VL1 and VL2 is VLhe or more, it is determined that the front side emission point (first emission portion or third emission portion) is abnormal, and a laser light quantity abnormality flag, due to a drop in front light quantity, is stored (S1105).
If not, it is checked whether only one of the drum potentials VL1 and VL2 is VLle (second predetermined value) or less (S1106). If only one of VL1 and VL2 is VLle or less, it is determined that the rear side emission point (second emission portion or fourth emission portion) is abnormal. Then the laser light quantity abnormality flag, due to a drop in rear light quantity, is stored (S1107). Here for VLle, potential is determined based on the exposure increase rate when a foreign matter adheres to one of the rear side emission points, and this potential value is stored in advance.
Then it is checked whether both of the drum potentials VL1 and VL2 are VLhe or more, or VLle or less (S1108). If the result is YES, it is determined that the abnormality is caused by a factor other than the laser light quantity abnormality due to the adhesion of foreign matter on the laser diode 304.
Just like Example 1, if the laser light quantity abnormality flag is stored (if it is determined that one of the first to fourth emission portions is abnormal), the operation of the charging circuit and the transfer circuit is checked to determine whether the abnormality is due to a factor related to an exposure amount abnormality, and not a laser light quantity abnormality. The method for the operation check is the same as Example 1. If it is determined that the charging circuit and the transfer circuit 206 are operating normally (NO in S919 and NO in S922), the notification portion notifies the user of the laser light quantity abnormality (S1109).
Here if the value of VLhe or VLle is not one value but one that changes depending on the operating environment and durability of the image forming apparatus 100, then the laser light quantity abnormality can be determined with even more accuracy. By performing control in this way, laser light quantity abnormality can be accurately determined for the image forming apparatus 100 having a multi-beam laser. Further, the laser light quantity abnormality can be determined with even higher accuracy by combining the control of this example with the control of Example 1. For example, the flow of performing the laser failure notification and optical component failure notification described in S923 to S925 in
In this example, the can package without glass 501 was described. But even in the case of a can package sealed by the glass 501, the beam spot diameter on the glass is about 90 μm, and the interval between spots is about several hundred μm, and it is rare that the adhesion of foreign matter covers all beams of the multi-beam laser. Therefore even in the case of the can package sealed by the glass 501, the laser light quantity abnormality can be determined with even higher accuracy than Example 1.
According to the present invention, a factor that drops the quantity of laser light can be determined with high accuracy.
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 such modifications and equivalent structures and functions.
This application claims the benefit of Japanese Patent Application No. 2014-143577, filed Jul. 11, 2014, which is hereby incorporated by reference herein in its entirety.
Number | Date | Country | Kind |
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2014-143577 | Jul 2014 | JP | national |
Number | Name | Date | Kind |
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6204870 | Nakagawa | Mar 2001 | B1 |
20090087207 | Iida et al. | Apr 2009 | A1 |
20130258032 | Ogasawara | Oct 2013 | A1 |
Number | Date | Country |
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H04-240866 | Aug 1992 | JP |
2002244497 | Aug 2002 | JP |
2006-310876 | Nov 2006 | JP |
2009-042361 | Feb 2009 | JP |
2012-155075 | Aug 2012 | JP |
Entry |
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JP—2002244497—A—T Machine Translation, Japan, Kato et al., Aug. 2002. |
Number | Date | Country | |
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20160011536 A1 | Jan 2016 | US |