JP5058661B2 - Image forming apparatus - Google Patents

Description

  The present invention relates to an image forming apparatus capable of relaxing the mounting accuracy between a scanning device and a photosensitive member while maintaining the image quality and reducing the adjustment cost and the like.

  In recent years, further miniaturization and cost reduction have been demanded in the field of image forming apparatuses using electrophotographic technology. In order to realize this miniaturization and cost reduction, a method using a galvano mirror manufactured by a semiconductor manufacturing technique in place of a conventionally used polygon mirror has been proposed (see Patent Document 1). In this method, an image is formed by scanning the laser beam in the main scanning direction by vibrating the mirror at a natural frequency (resonance frequency) generated by the mechanical dimension of the galvanometer mirror. This galvanometer mirror can be made smaller by using a semiconductor manufacturing technique, and a large number of mirrors can be manufactured at one time, so that cost reduction can be expected.

  Further, the nested mirror as in Patent Document 2 has a property that it can be controlled to scan at a substantially equal angular velocity in a scanning area to be used, and a property that a scanning angle can be increased, and the correction optical system can be made small. It can have a simple configuration and is suitable as a scanning device in a small and low-cost image forming apparatus.

  Here, problems have been pointed out regarding the accuracy of the attachment machine between the scanning device and the photosensitive member, and various methods for reducing the attachment accuracy have been proposed (see Patent Document 3 and Patent Document 4).

  In the method of Patent Document 3, the overall magnification and partial magnification of an image to be formed are controlled by controlling the average frequency and the left-right frequency difference of the image clock signal.

In the method of Patent Document 4, the partial magnification of an image to be formed is controlled by inserting or deleting a slight delay at the time of pixel generation.
Both of the above methods use the controller-side function in the image forming apparatus to control the linear velocity on the photoconductor, particularly the drawing time. Advanced LSI technology such as micro delay insertion for data is required.
JP-A-7-175005 JP 2005-208578 A JP 2000-255098 A JP 2000-238342 A

  An object is to maintain the scanning linear velocity on the photosensitive member at a substantially constant speed after relaxing the mounting accuracy between the scanning device and the photosensitive member.

In order to solve the above problems, an image forming apparatus of the present invention is an image forming apparatus that scans a light beam in a main scanning direction of a photosensitive member, and deflects the light beam by resonantly vibrating a deflector. Means, means for driving the deflector by resonance vibration, mounting angle information of the photosensitive member acquired in advance, and drive control means for controlling the deflector driving means in accordance with the mounting angle information. It is characterized by.

  According to the present invention, in a situation where the scanning device and the photosensitive member are mounted at an inclination, the scanning phase speed on the photosensitive member is made substantially constant by controlling the driving phase in the driving means of the nested reciprocating scanning mirror. Can be kept in.

Example 1
Embodiments to which the present invention is applied will be described below with reference to the accompanying drawings.

  FIG. 1 is a diagram illustrating positions and main configurations of a scanning device 10 and a photoconductor 20 in an image forming apparatus according to an embodiment of the present invention.

  In FIG. 1, light emitted from the semiconductor laser 101 is reflected by a nested reciprocating scanning mirror 100 that reciprocally vibrates, passes through an fθ lens 102, and then scans on a photoconductor 20.

  In FIG. 1, the photosensitive member 20 has a semiconductor laser 101 and a virtual photosensitive member surface 200 obtained by reflecting a laser beam when the nested reciprocating scanning mirror 100 in the scanning device 10 has a scanning angle of 0 °. It is assumed that the fθ lens 102, the scanning device 10, and the photoconductor 20 are mounted with an inclination of an angle α depending on the processing accuracy and mounting accuracy of mechanisms and optical components related to the optical path.

  Further, in the scanning device 10, it is assumed that only the range of the angle 30 that is a substantially equal angular speed among the scanning angles of the nested reciprocating scanning mirror 100 is used as the effective scanning region.

  FIG. 2 is a diagram showing the structure of the nested reciprocating scanning mirror 100 in the embodiment of the present invention.

The nested reciprocating scanning mirror 100 has a structure as disclosed in Patent Document 2, and has two torsion springs inside. The torsion spring 1000 and the torsion spring 1001 have a specific angular frequency ω based on their mechanical dimensions. ₁ (resonance frequency F ₁ , ω ₁ = 2πF ₁ ) and vibration mode (vibration mode 1) and vibration at an angular frequency ω ₂ (resonance frequency F ₂ , ω ₂ = 2πF ₂ ) twice the angular frequency ω ₁ Assume that the machine dimensions are designed and processed to have a mode (vibration mode 2). That is, ω ₂ = 2ω ₁ .

  The nested reciprocating scanning mirror 100 is driven by a mirror driving device 103.

  The mirror driving device 103 is a device comprising a coil 105 for passing a current and a magnet 1002 attached to the nested reciprocating scanning mirror 100, and obtains a driving torque of the nested reciprocating scanning mirror by electromagnetic force.

  The drive control device 104 can control the current flowing through the coil 105 according to control parameters.

Here, by controlling the current flowing through the coil by the drive control device 104, the nested reciprocating scanning mirror 100 performs a resonance operation, and performs scanning by the displacement of the scanning angle represented by the following Equation 1.
θ = θ ₁ sin (ω ₁ t + φ ₁ ) + θ ₂ sin (ω ₂ t + φ ₂ )
= Θ ₁ sin (ωt + φ ₁ ) + θ ₂ sin (2ωt + φ ₂ ) Equation 1
θ is a scanning angle at time t when scanned by the nested reciprocating scanning mirror 100, θ ₁ is an amplitude control parameter for vibration mode 1, θ ₂ is an amplitude control parameter for vibration mode 2, and φ ₁ and φ ₂ are vibrations. This is a phase control parameter indicating the relative phase difference between mode 1 and vibration mode 2.

θ ₁ is the maximum displacement angle formed by the nested reciprocating scanning mirror 100 when resonating in vibration mode 1 only, and θ ₂ is the reciprocating reciprocating scanning mirror 100 when resonating in vibration mode 2 only. Is the maximum displacement angle. ω is an angular frequency at which the vibration mode 2 is twice that of the vibration mode 1.

  FIG. 3 is a diagram showing the configuration of the drive control device 104 of the present invention.

The drive control device 104 includes an H-bridge circuit 1040 for current control of the coil 105 and a controller 1041 that controls the H-bridge. The controller 1041 has a PWM (Pulse Width Modulation) type current control circuit, and _The control parameters 1042, 1043, 1044, and 1045 corresponding to ₁ , θ ₂ , φ ₁ , and φ ₂ can be set to control the resonance operation.

  FIG. 4 shows an incident angle when a scanning surface of the photosensitive member 20 is mounted at an attachment angle α and a laser beam scanned at a constant speed through the fθ lens 102 scans the scanning surface of the photosensitive member. FIG. 6 is a diagram showing a relationship of scanning positions on a scanning surface of a photoconductor.

  Here, the x axis coincides with the optical axis of the scanning optical system, and the y axis coincides with the virtual photoconductor surface 200 of FIG. The attachment angle α is a positive value for the direction of rotation from the y-axis to the positive direction of the x-axis, and a negative value for the direction of rotation in the negative direction of the x-axis.

The scanning position y is a scanning position on the virtual photoreceptor surface 200 (y axis), that is, an ideal scanning position when the attachment angle α = 0, and β _y is the laser beam at the scanning position y on the virtual photoreceptor surface 200. The incident angle, y ′ is the scanning position of the laser beam on the photoconductor 20, f _i is the distance from the nested reciprocating scanning mirror 100 to the fθ lens 102, and f _o is from the fθ lens 102 to the virtual photoconductor surface 200. Is the distance.

The incident angle β _y has a positive value in the direction from the x-axis to the positive direction of the y-axis and a negative value in the direction of the y-axis in the negative direction.

Arrow on the photoreceptor 20 of FIG. 4 has a length of 2y _'k across the scan center, and so long.

4, when scanned constant velocity at the virtual photoreceptor surface 200 above, the actual photoreceptor surface 20 scan line length of the scanning start end side of the on y _'- is shorter than y, the scanning of the scan end side The line length y ′ ₊ is longer than y. That is, in order to scan the same length y ′ _{k on} the scanning start end side and the scanning end end side, the scanning angle per unit time, that is, the scanning angular velocity is changed on the scanning start end side and the scanning end end side. It can also be seen that the scanning time must be changed while keeping the scanning angular velocity constant.

For example, when changing the scanning angular velocity, in the example of FIG. 4, the scanning line speed is increased on the scanning start end side, the scanning line speed is decreased on the scanning end end side, or scanning is performed on the scanning start end side. If the time is increased and the scanning time is shortened on the scanning end side, it is possible to scan the same length y ′ _k on the scanning start end side and the scanning end end side.

  In the methods of Patent Document 3 and Patent Document 4 described above, isometric scanning is performed by the latter method of controlling the scanning time. This is because it is very difficult to change the scanning angular velocity in the constant speed scanning by the conventional polygon mirror.

  In the present invention, the nested reciprocating scanning mirror 100 can easily control the scanning angular velocity variably within one scanning period, and using this property, the scanning angular velocity can be controlled between the scanning start end side and the scanning end end side. By controlling, it is possible to scan at the same length on the scanning start end side and the scanning end end side.

In FIG. 4, for example, the fθ lens 102 is designed so that the incident angle β _y of the laser beam on the virtual photoconductor surface 200 is a function of the main scanning direction (y-axis direction) (a fourth or higher order polynomial of y). For example,
cos β _y = A ₄ y ⁴ + A ₃ y ³ + A ₂ y ² + A ₁ y + A _0.
It can be expressed as

  Table 1 shows an example of design parameters related to Formula 6 of the fθ lens 102.

  FIG. 5 is a graph showing Formula 2 using the design parameters of the fθ lens 102 in Table 1.

Here, the following relational expression between the scanning position y ′ on the photoreceptor 20 inclined by the angle α and the scanning position y on the virtual photoreceptor surface 200 by the laser beam incident at the incident angle β _y is as follows. Holds.

Here, the mounting angle of the photosensitive member 20, relationship are four code symbols and the incident angle βy angle α ({α ≧ 0, β y ≧ 0}, {α ≧ 0, β y ≦ 0}, { α ≦ 0, β _y ≧ 0}, {α ≦ 0, β _y ≦ 0},), but both can be expressed by Equation 3. (FIG. 4 shows the case of {α ≧ 0, β _y ≧ 0}, {α ≧ 0, β _y ≦ 0})
When the scanning linear velocity on the photosensitive member surface 20 and v _{y ',} the time required to scan this time is t _y,

It is represented by

Here, the fθ lens 102, since the scanning linear velocity v _y on the photoconductive member surface 200 of the virtual is designed to be constant, is established the following relationship.

  Therefore, Equation 4 can be expressed as follows using Equation 5.

Equation 4 ', when scanning the virtual photoreceptor surface 200 on at a constant scanning line speed v _y, scanning linear velocity v _y on the photoconductor _20' varies according to the mounting angle α and the scanning position y ( It shows that it changes depending on the incident angle β _y ).

FIG. 6 shows the scanning linear velocity v on the photoconductor 20 in the case of α = 0, 0.01, 0.02, 0.05 [degree] using the fθ lens design parameter and the mathematical formula 4 ′ in Table 1. ₆ is a graph in which the value of _{y ′} is normalized with respect to the center of scanning, where the horizontal axis is the scanning position y and the vertical axis is the ratio to the scanning linear velocity v ₀ when y = 0.

As shown in FIG. 6, when α> 0, the scanning linear velocity v _y− below the scanning center (β _y ≦ 0, y <0, scanning start end side) and the scanning center (β _y = 0, y = 0). scanning linear velocity v _{0 in)} above the scanning center _{(β y ≧ 0, y>} 0, the scanning linear velocity v _{y +} at scan end side), it can be seen that the following relationship holds.
v _y− <v ₀ <v _{y +} Expression 6
That is, the scanning linear velocity vy _′ on the photosensitive member 20 is slower on the lower side (y−, scanning start end side) than the scanning center in FIG. 4 and on the upper side (y +, scanning end end side). ) Indicates that it is fast.

When α <0, the direction of the inequality sign in Expression 6 is reversed. That is, the scanning linear velocity vy _′ on the photoconductor 20 is faster on the lower side (scanning start end side) than the scanning center and is slower on the upper side (scanning end end side) than the scanning center.

  Next, the resonance operation and control of the nested reciprocating scanning mirror will be described.

  FIG. 7 shows a case where a laser beam scanned by a nested reciprocating scanning mirror controlled by a composite wave expressed by Formula 1 is mounted on a photoconductor 20 mounted at an mounting angle α = 0 [degrees] through an fθ lens 102. It is the figure which showed the relationship between the scanning position in the case of image formation, and time.

By the fθ lens 102, the resonance operation of the nested reciprocating scanning mirror according to Equation 1 is converted into a constant velocity motion of the image height scanned on the virtual photoreceptor surface 200 on the photoreceptor 20. That is, the following formula 7 holds.
y = fθ = f {θ ₁ sin (ωt + φ ₁ ) + θ ₂ sin (2ωt + φ ₂ ) (9)
y is the image height in the main scanning direction on the virtual photoreceptor surface 200, and f is the focal length of the fθ lens.

Here, the angular velocity θ ′ of the nested reciprocating scanning mirror is θ ′ = ω {θ ₁ cos (ωt + φ ₁ ) + 2θ ₂ (cos (2ωt + φ ₂ ).
It becomes.

Note that φ ₁ and φ ₂ are defined so that a phase difference relationship according to the following equation is established so that θ = 0 at the scanning center (ωt = π, time t = t0 in FIG. 8).

This is because even if φ ₁ and φ ₂ are controlled to change the phase of the drive waveform, the point at which θ = 0 is not changed. If φ ₂ is determined, φ ₁ can be obtained. .

  FIG. 8 and FIG. 9 are graphs showing the relationship between the scanning angle θ expressed by Equation 1 and the angular velocity θ ′ expressed by Equation 10 with respect to time.

8 and 9, θ ₁ = −35 and θ ₂ = −5 are used for the control parameters 1042 (corresponding to θ ₁ of Expression 1) and 1043 (corresponding to θ ₂ of Expression 1).

In FIG. 8, when the value of the control parameter 1044 (corresponding to φ ₁ in Equation 1) is φ ₁ = 0, and the value of the control parameter 1045 (corresponding to φ ₂ in Equation 1) is φ ₂ = 0, the effective scanning range. At 30, the angular velocity at which the laser beam scans on the photoreceptor 20 is substantially constant (substantially constant speed operation) as shown in FIG.

Further, in FIG. 9, the values of the control parameter 1044 (corresponding to φ ₁ in Formula 1) and the control parameter 1045 (corresponding to φ ₂ in Formula 1) are values other than zero (φ ₂ = −10 [degree] in the figure). In the effective scanning range 30, the angular velocity at which the laser beam scans on the photoconductor 20 is substantially proportional to the scanning position as shown in FIG.

That is, by appropriately selecting the values of φ ₁ and φ ₂ , the scanning angular velocity θ ′ of the nested reciprocating scanning mirror is changed within the effective scanning range 30 in proportion to the scanning position y on the virtual photoreceptor surface 200. It shows that it can be made.

'Than in the case of scanning the virtual photoreceptor surface 200 on at a constant scanning line speed v _y, scanning linear velocity v _y on the photoconductor _20' Equation 4 is changed by the mounting angle α and the scanning position y.

From Equation 10, the value of the phase control parameter φ ₂ for controlling the nested reciprocating scanning mirror is appropriately selected so that the scanning angular velocity of the nested reciprocating scanning mirror is controlled to be proportional to the scanning position within the effective scanning range 30. can do.

Scanning angular velocity of the nested reciprocating scanning mirror through the fθ lens 102, to be converted into the scanning linear velocity of the photosensitive member surface 200 of the virtual appropriately the value of the phase control parameter phi ₂ for controlling the nested reciprocating scanning mirror By selecting, on the virtual photoconductor surface 200, the scanning linear velocity can be controlled to be proportional to the scanning position.

Here, if the phase control parameter φ ₂ is selected so as to cancel the change in the scanning linear velocity (equation 4 ′) depending on the mounting angle and the scanning position, the scanning linear velocity on the photoconductor 20 is controlled and the photoconductor 20 is controlled. The scanning line length can be made the same at the scanning start end side and the scanning end end side.

FIG. 10 shows the relationship between the scanning position on the photoconductor 20 and time when scanning is performed using the phase control parameter φ ₂ that cancels out the scanning linear velocity change (Formula 4 ′) depending on the mounting angle and the scanning position. FIG.

  In FIG. 10, it can be seen that the scanning line speed is higher on the scanning start end side, and the scanning line speed is lower on the scanning end end side.

That is, it is only necessary to find the phase control parameter φ ₂ that cancels out the change in the scanning linear velocity expressed by Equation 4 ′.

Incidentally, it is possible to mathematically obtain φ ₂ that cancels the mathematical expression 4 ′ within the effective scanning region, but here, a method for simply obtaining the phase control parameter φ ₂ will be described.

In the present embodiment, a method for obtaining the phase control parameter φ ₂ using the following values will be described.

  In this embodiment, it is assumed that the mounting angle α of the photoconductor is measured at the time of manufacture / shipment and the measurement result α = 0.05 [degrees] is acquired in advance.

  Further, the scanning start end (y = −105 [mm]) and the scanning end end (y = + 105 [mm]) on the virtual photoconductor surface 200 have a scanning angle θ = 21 [degrees] of the nested reciprocating scanning mirror. Shall reach.

From FIG. 6, the ratio of the scanning linear velocity vy _′ when α = 0.05 [degree] and y = −105 [mm] is 0.99971294.
In order to cancel this ratio, the reciprocal of this ratio 1 / 0.99997294 = 1.00028713 may be realized by phase control.

A ratio between the scanning angular velocity θ ′ before changing φ ₂ and the scanning angular velocity θ ′ _φ2 after changing φ ₂ is calculated in advance, and φ ₂ that is the reciprocal value described above may be obtained. .

Here phi ₂ could be obtained with -0.062985 [degrees].

(Example 2)
In the first embodiment, the case where the attachment angle α is measured and acquired in advance has been described.

  In the second embodiment, a method will be described in which scanning timing information is measured and acquired, and a phase control parameter is obtained using this information.

  FIG. 10 shows an example of a method for measuring scanning timing information.

  In FIG. 10, reference numeral 201 denotes a photoconductor for measuring scanning timing information. Light receiving sensors 2010, 2011, and 2012 are provided at y = −105 [mm], y = 0 [mm], and y = + 105 [mm]. It is assumed that each is equipped, has the same shape as the photoconductor 20, and can be easily replaced.

  Of course, only light receiving sensor means that can be simply mounted on the photoconductor 20 may be used.

At the time of manufacturing the image forming apparatus, the scanning timing information measuring photoconductor 201 is attached, the scanning device 10 is operated with the phase control parameter φ ₁ = φ ₂ = 0, and the scanning timing information measuring photoconductor 201 is moved over. Scan with laser light.

  The scanned laser light is received by each of the light receiving sensors 2010, 2011, and 2012, and scanning timing information is measured. At this time, φ2 is obtained from the scanning timing information T1 between the light receiving sensor 2010 and the light receiving sensor 2011, the scanning timing information T2 between the light receiving sensor 2011 and the light receiving sensor 2012, and the scanning timing information T3 between the light receiving sensor 2010 and the light receiving sensor 2012. .

  For example, it is assumed that the scan timing measurement is performed and T1 = 125.02 [us], T2 = 124.98 [us], and T3 = 250.000 [us].

Assuming that the scanning timing when attached at an attachment angle α = 0 [degrees] is T1 = T2 = 125.00 [us],
The scanning timing deviation ratio on the scanning start side is 125.02 / 125.00 = 1.00016.

In the same manner as in Example 1, previously calculating the ratio between _.phi.2 'scanning angular speed θ after changing the and phi _2' scanning angular velocity θ before changing the phi _2, the scanning timing deviation ratio 1.00016 What is necessary is just to obtain | require (phi) ₂ which implement | achieves.
Here, phi ₂ could be obtained with -0.0351 [degrees].

1 is a diagram illustrating a configuration of an image forming apparatus of the present invention. It is a figure which shows the structure of a nested reciprocating scanning mirror. It is a figure which shows the structure of the drive control apparatus of this invention. It is the figure which showed the relationship between the scanning position of a laser beam, and time. FIG. 6 is a diagram illustrating a relationship between design parameters of an fθ lens and Formula 2. It is a figure which shows the ratio of the mounting speed of a photoconductor and the scanning speed in each scanning position. It is the figure which showed the relationship between the scanning position of a laser beam, and time. It is the figure which showed the angle and angular velocity of a nesting type reciprocating scanning mirror in the case of (phi) = 2 = 0 [degrees], and the relationship of time. It is the figure which showed the relationship between the angle and angular velocity of a nesting type reciprocating scanning mirror in case of (phi) 2 = -10 [degree], and time. FIG. 6 is a diagram showing a relationship between a scanning position of laser light and time when φ is controlled according to a mounting angle of a photoconductor. It is a figure which shows the apparatus structure which acquires timing information.

Explanation of symbols

DESCRIPTION OF SYMBOLS 10 Scanning device 20 Photosensitive body 30 Effective scanning area 100 Nested reciprocating scanning mirror 101 Semiconductor laser 102 Constant velocity correction lens 103 Mirror drive device 104 Drive control device 105 Coils 106, 107 Laser light detection device (BD)
200 Virtual photoreceptor surface 1000, 1001 Torsion spring 1002 Magnet 1040 H bridge circuit for current control 1041 Controller 1042 Amplitude control parameter for reference frequency ω 1043 Amplitude control parameter for frequency 2ω 1044 Phase difference parameter for reference frequency ω 1045 Phase difference for frequency 2ω Parameters

Claims (5)

An image forming apparatus that scans a light beam in a main scanning direction of a photoreceptor,
A light beam deflecting means for deflecting the light beam by resonantly vibrating the deflector;
Means for driving the deflector by resonant vibration;
Photosensor mounting angle information acquired in advance,
An image forming apparatus comprising drive control means for controlling the deflector drive means in accordance with the mounting angle information. An image forming apparatus that scans a light beam in a main scanning direction of a photoreceptor,
A light beam deflecting means for deflecting the light beam by resonantly vibrating the deflector;
Means for driving the deflector by resonant vibration;
Scanning timing information acquired in advance;
Drive control means for controlling the deflector drive means in accordance with the scanning timing information;
The light beam deflecting means includes
A plurality of movers and a plurality of torsion springs arranged on the same axis connecting the plurality of movers;
A support portion for supporting a part of the plurality of torsion springs;
Drive means for applying torque to at least one of the movers;
An optical deflector having drive control means for controlling the drive means,
It has a plurality of separated natural vibration modes,
Among the plurality of separated natural vibration modes, there are a reference vibration mode that is a natural vibration mode of a reference frequency and an even multiple vibration mode that is a natural vibration mode of a frequency that is substantially an even multiple of the reference frequency. An image forming apparatus. The light beam deflecting means includes a plurality of movers and a plurality of torsion springs arranged on the same axis connecting the plurality of movers.
A support portion for supporting a part of the plurality of torsion springs;
Drive means for applying torque to at least one of the movers;
An optical deflector having drive control means for controlling the drive means,
It has a plurality of separated natural vibration modes,
Among the plurality of separated natural vibration modes, there are a reference vibration mode that is a natural vibration mode of a reference frequency and an even multiple vibration mode that is a natural vibration mode of a frequency that is substantially an even multiple of the reference frequency. The image forming apparatus according to claim 1 .   The drive control means controls the relative phase of the frequency of the even-fold vibration mode based on the frequency phase of the reference vibration mode of the nested deflector based on the control information generated from the mounting angle information. The image forming apparatus according to claim 1. An image forming apparatus that scans a light beam in a main scanning direction of a photoreceptor,
A light beam deflecting means for deflecting the light beam by resonantly vibrating the deflector;
Means for driving the deflector by resonant vibration;
Scanning timing information acquired in advance;
Drive control means for controlling the deflector drive means according to the scanning timing information,
The drive control means controls the relative phase of the frequency of the even-fold vibration mode with reference to the frequency phase of the reference vibration mode of the nested deflector based on the control information generated from the scanning timing information. be that images forming device.

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