The present invention relates to an optical scanning apparatus that scans a scanning target surface with a laser light flux emitted from a light source and deflected by a deflection unit, and an image forming apparatus including this optical scanning apparatus, such as a laser beam printer (hereinafter referred to as an LBP), a digital copying machine, and a digital fax machine (FAX).
An optical scanning apparatus for use with an image forming apparatus based on the electrophotographic method optically writes an image onto a photosensitive drum or the like with use of a laser beam as discussed in Japanese Patent Application Laid-Open No. 2016-109780. The optical scanning apparatus discussed in Japanese Patent Application Laid-Open No. 2016-109780 writes the image onto the photosensitive drum in the following manner. The optical scanning apparatus emits a laser light flux from a semiconductor laser unit. The emitted laser light flux passes through a lens and is imaged as a linear image on a reflection surface of a polygon mirror. Then, the laser light flux is deflected due to a rotation of the polygon mirror, and is imaged and caused to scan on a photosensitive surface (the scanning target surface) that is a surface of the photosensitive drum via an fθ lens, by which an electrostatic latent image is formed on the scanning target surface. When the polygon mirror is located in a predetermined rotational phase, the reflected laser light flux is incident on a beam detector (BD) sensor as a signal output unit that outputs a BD signal.
However, according to the technique discussed in Japanese Patent Application Laid-Open No. 2016-109780, the semiconductor laser unit, the BD sensor, and the fθ lens are arranged on a same plane, and the laser light flux is deflected and caused to scan on the same plane. Therefore, to dispose the BD sensor, an angle of the laser light flux from the semiconductor laser unit with respect to a center of the photosensitive surface in a scanning direction (a laser incident angle) is undesirably increased to approximately a right angle.
The increase in the laser incident angle leads to an increase in a width of the linear image on the reflection surface of the polygon mirror, raising a necessity of increasing a width of the reflection surface of the polygon mirror in a longitudinal direction of the linear image (hereinafter referred to as a width in a main scanning direction). The increase in the width of the reflection surface of the polygon mirror in the main scanning direction may result in increase in processing cost and material cost of the polygon mirror.
Therefore, according to an aspect of the present invention, a representative configuration of an optical scanning apparatus includes a light source configured to emit a laser light flux, a deflection unit configured to deflect the laser light flux emitted from the light source, and a light reception member configured in such a manner that the laser light flux reflected by the deflection unit is incident thereon. The light source emits the laser light flux tilted by a predetermined angle with respect to a horizontal direction toward the deflection unit. The light reception member is disposed above or below the light source, and the laser light flux reflected by the deflection unit and tilted by the predetermined angle with respect to the horizontal direction is incident on the light reception member.
Further features of the present invention will become apparent from the following description of exemplary embodiments with reference to the attached drawings.
In the following description, an exemplary embodiment of the present invention will be described in detail with reference to the drawings by way of example. However, dimensions, materials, shapes, a relative layout, and the like of components that will be described in the following exemplary embodiment shall be changed as appropriate according to a configuration of an apparatus to which the present invention is applied and various kinds of conditions. Therefore, they are not intended to limit the scope of the present invention only thereto unless otherwise specifically indicated.
In the following description, a first exemplary embodiment will be described. First, an image forming apparatus D1 will be described with reference to
The image forming apparatus D1 includes the optical scanning apparatus 101, and scans a photosensitive drum as an image bearing member by the optical scanning apparatus 101 to form an image on a recording material P such as recording paper based on an image drawn by this scanning. As illustrated in
Next, the optical scanning apparatus 101 according to the present exemplary embodiment will be described with reference to
(Optical Scanning Apparatus)
As illustrated in
The semiconductor laser unit 1, the compound anamorphic collimator lens 11, the scanning motor 5, and the scanning lens 7, which is an imaging unit, are fixed in the optical box 9 by press-fitting, adhesion, fastening with a screw, or the like.
The semiconductor laser unit 1 emits the laser light flux L, and forms a linear image on the reflection surface 12 of the polygon mirror 4 by the anamorphic collimator lens 2. The polygon mirror (a deflection unit) 4 is rotationally driven by the scanning motor 5, and deflects the laser light flux L emitted from the semiconductor laser unit 1. Then, the laser light flux L deflected by the polygon mirror 4 is imaged and scans on a scanning target surface (the surface of the photosensitive drum 8) by passing through the scanning lens 7.
In the present disclosure, a scanning direction in which the laser light flux L deflected by the polygon mirror 4 is caused to scan the scanning target surface (the surface of the photosensitive drum 8) is defined to be a main scanning direction X, and a direction perpendicular to this scanning direction is defined to be a sub scanning direction Y.
The semiconductor laser unit 1 and the BD sensor 6 are arranged on a same line in the direction (the sub scanning direction Y) perpendicular to the scanning direction (the main scanning direction X) as illustrated in
Further, in the optical scanning apparatus 101, the semiconductor laser unit 1 and the BD sensor 6 are disposed respectively on one side and the other side of the polygon mirror 4 in the direction (the sub scanning direction Y) perpendicular to the scanning direction (the main scanning direction X) deflected by the above-described polygon mirror 4.
More specifically, as illustrated in
The laser light flux L tilted upward is emitted from the semiconductor laser unit 1 toward the polygon mirror 4, and the BD sensor 6 is disposed above the semiconductor laser unit 1 in a direction along a rotational shaft of the polygon mirror 4 (the sub scanning direction Y). More specifically, the BD sensor 6 is disposed in such a manner that the above-described incident point 6a is located at a higher position than the emission point 1a of the semiconductor laser unit 1. This layout allows the semiconductor laser unit 1 and the scanning lens 7 to be located close to each other in the scanning direction as illustrated in
Further, a distance h between the semiconductor laser unit 1 and the BD sensor 6 mounted on the same substrate 20 can be set within a range of 6 mm to 20 mm in the direction along the rotational shaft of the polygon mirror 4 (the sub scanning direction Y) as illustrated in
Further, the BD sensor 6 is disposed on the same surface as a surface (one surface) of the substrate 20 where the semiconductor laser unit 1 is mounted as illustrated in
In
Time periods (a) to (d) illustrated in
In the present exemplary embodiment, the laser light flux L can be incident on the BD sensor 6 at the time period (b) when the reflection surface 12b faces the laser light flux L straight, and a time period other than the time period (b) can be used as an image formation time period (c) during which the laser light flux L is caused to scan on the photosensitive drum 8. Therefore, a large proportion of a laser light emission possible time period (T) can be used as the image formation time period (c). In other words, the present exemplary embodiment can shorten the laser light emission possible time period (T) while securing a certain time period as the image formation time period (c).
The laser light emission possible time period (T) is proportional to a width W of the reflection surface 12 of the polygon mirror 4 in the main scanning direction illustrated in
In rotational phases of the polygon mirror 4 illustrated in
S=A/sin(90−θ/2) (1)
The narrow width of the linear image S allows a large portion to be allocated to the rotational phase of the polygon mirror 4 within a range where the laser light flux L is prevented from hitting the corners 13a and 13b of the polygon mirror 4, thereby allowing the reflection surface 12 of the polygon mirror 4 to have a narrower width in the main scanning direction.
As illustrated in
The reduction in the width W of the reflection surface 12 of the polygon mirror 4 in the main scanning direction leads to a reduction in a distance A from a center of the rotational shaft 14 of the polygon mirror 4 to each of the corners 13a and 13b illustrated in
Further, the airflow W1 is a turbulent flow and causes fluid noise, so that the reduction in the width W of the reflection surface 12 in the main scanning direction also leads to a reduction in the turbulent flow indicated by W1 and thus a reduction in the fluid noise. The reflection surface 12b has been described here, but the same also applies to the other three reflection surfaces.
Next, the scanning motor 5 in the optical scanning apparatus 101 will be described with reference to
In
The scanning motor 5 is fixed to the optical box 19 via the iron substrate 18 with use of screws 16a and 16b. Further, the polygon mirror 4, the rotational shaft (a fixed shaft) 14, and the rotor frame 15 are rotationally driven as an integrated rotational body.
Now, a correction of balance of the rotational body will be described. The rotational body is subject to an offset of a center of gravity of the rotational body from a rotational center due to, for example, variations in a connected state of each of parts and a dimension of a part (initial unbalance). In other words, mass unbalance occurs in the rotational body, and dynamic disequilibrium occurs when the rotational body is rotationally driven. The occurrence of the dynamic disequilibrium may cause a vibration and/or noise due to a wobbling rotation of the rotational body, thereby resulting in deterioration of an image quality of the image forming apparatus D1 and/or an increase in the noise. Therefore, the present exemplary embodiment attempts to adjust the balance and reduce the mass unbalance of the rotational body by applying the balance weight 17 on a top surface of the rotor frame 15 forming the rotational body.
The balance weight 17 is formed by mixing metallic particles, glass beads, or the like in a photo-curable adhesive such as an ultraviolet curable adhesive, and is placed at an appropriate position of the rotor frame 15 by an appropriate amount and cured to be attached to the rotor frame 15 by being irradiated with light such as ultraviolet light. Further, if the balance weight 17 has low specific gravity, this leads to an increase in an application amount thereof, thereby causing a variation in the application amount, a shift of the application position, and/or an increase in a time period taken to cure the balance weight 17. If the balance weight 17 has high specific gravity, this leads to an increase in the variation in the application amount per application. Therefore, generally, a balance weight having specific gravity of approximately 1 to 3 is used.
The number of times that the balance is corrected depends on an initial unbalance amount of the rotational body. If the initial unbalance amount is large, the balance weight 17 should be applied by a large amount, which causes the variation in the application amount and/or the shift of the application position. Therefore, the balance may be unable to be corrected to a predetermined or smaller unbalance amount by being corrected once, and the balance may be corrected twice.
The initial unbalance amount of the rotational body can be expressed as a product of the mass of the rotational body and a distance from the rotational center of the rotational body to the center of gravity of the rotational body. Reducing the width W of the reflection surface 12 of the polygon mirror 4 in the main scanning direction leads to a reduction in the mass of the polygon mirror 4 and thus a reduction in the initial unbalance amount of the rotational body. As a result, the present exemplary embodiment can reduce the application amount of the balance weight 17 when the balance is corrected, thereby improving accuracy of the application amount of the balance weight 17. In other words, the present exemplary embodiment allows the balance to be accurately corrected, thereby allowing the balance weight 17 to be placed at one portion in the same correction surface. Therefore, the present exemplary embodiment can reduce the fluid noise of an unpleasant frequency that occurs at the balance weight portion due to the rotation of the rotational body. Further, the present exemplary embodiment reduces a weight of the rotational body by reducing the mass of the polygon mirror 4, thereby reducing an inertial moment of the rotational body and thus succeeding in shortening a time period taken until the rotational body reaches a rated number of rotations (a rise time period). In other words, the present exemplary embodiment can shorten a time period taken since the optical scanning apparatus 101 rises until the optical scanning apparatus 101 becomes ready for the exposure, thus shortening a time period taken for the image forming apparatus D1 to print the first page.
Next, how a shift of an irradiation position is improved when the size of the reflection surface 12 of the polygon mirror 4 in the main scanning direction is reduced will be described with reference to
Reducing the width W of the reflection surface 12 of the polygon mirror 4 in the main scanning direction leads to a reduction in the positional shift amount Sa of the deflection point when the polygon mirror 4 is rotated. The reduction in the positional shift amount Sa leads to a reduction in a shift amount of the exposure point in the sub scanning direction due to the optical face tilt, thereby improving the above-described banding.
In the present exemplary embodiment, the laser light flux L tilted upward is emitted from the semiconductor laser unit 1 toward the polygon mirror 4, and the BD sensor 6 is disposed above the semiconductor laser unit 1. This layout can reduce the laser incident angle, and reduce the width W of the reflection surface 12 of the polygon mirror 4 in the main scanning direction.
According to the present exemplary embodiment, processing cost and material cost of the polygon mirror are reduced due to the reduction in the width of the reflection surface of the polygon mirror in the main scanning direction. Further, the present exemplary embodiment makes it difficult to contaminate the end of the reflection surface because of the reduction in the rotational speed at the end of the reflection surface of the polygon mirror. Further, the present exemplary embodiment reduces the noise when the polygon mirror is rotated at a high speed. Further, the present exemplary embodiment shortens the time period taken until the polygon mirror reaches the rated number of rotations, thereby allowing the first page to be printed in a shorter time period. Lastly, the reduction in the size of the reflection surface of the polygon mirror leads to the reduction in the positional shift of the deflection point when the laser light flux is caused to scan on the photosensitive surface drum, thereby improving the banding.
In the above-described exemplary embodiment, the optical scanning apparatus 101 has been described referring to the configuration in which the BD sensor 6 is disposed above the semiconductor laser unit 1 in the direction along the rotational shaft 14 of the polygon mirror 4 by way of example, but is not limited thereto. The optical scanning apparatus 101 may be configured in such a manner that the BD sensor 6 is disposed below the semiconductor laser unit 1 in the direction along the rotational shaft 14 of the polygon mirror 4. More specifically, the optical scanning apparatus 101 may be configured in such a manner that the BD sensor 6 is disposed so as to allow the above-described incident point 6a to be located at a lower position than the emission point 1a of the semiconductor laser unit 1. In other words, the semiconductor laser unit 1 emits the laser light flux L tilted downward by the predetermined angle a degrees with respect to the horizontal direction toward the reflection surface 12 of the polygon mirror 4. The BD sensor 6 is disposed below the semiconductor laser unit 1, and the laser light flux L reflected by the polygon mirror 4 and tilted downward by the above-described predetermined angle α degrees with respect to the horizontal direction is incident on the BD sensor 6. A similar effect to the above-described exemplary embodiment can also be acquired by employing such a configuration.
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. 2017-047260, filed Mar. 13, 2017, No. 2017-248612, filed Dec. 26, 2017, which are hereby incorporated by reference herein in their entirety.
Number | Date | Country | Kind |
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2017-047260 | Mar 2017 | JP | national |
2017-248612 | Dec 2017 | JP | national |
Number | Name | Date | Kind |
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5805323 | Ichikawa | Sep 1998 | A |
6512623 | Ishihara | Jan 2003 | B1 |
9581929 | Nagatoshi | Feb 2017 | B2 |
Number | Date | Country |
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2016-109780 | Jun 2016 | JP |
Number | Date | Country | |
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20180259876 A1 | Sep 2018 | US |