The present invention claims priority under 35 U.S.C. § 119 to Japanese Application No. 2019-043944 filed Mar. 11, 2019, is incorporated herein by reference in its entirety.
The present disclosure relates to a motor control device, a method of estimating an initial position of a magnetic pole of a rotor, and an image forming apparatus, and is used for controlling an alternating-current (AC) motor such as a sensorless-type brushless direct-current (DC) motor (also referred to as a permanent magnet synchronous motor).
A sensorless-type brushless DC motor does not include a sensor for detecting a magnetic pole position of a permanent magnet of a rotor with respect to each phase coil of a stator. Thus, in general, before starting the motor, a stator is energized at a prescribed electrical angle so as to pull the magnetic pole of the rotor to a position in accordance with the energized electrical angle (hereinafter also referred to as an energization angle), and subsequently start the rotation of the motor.
When the rotor is to be pulled, however, the rotor is pulled while being displaced by up to ±180°. Thus, the rotor may vibrate greatly. In such a case, it is necessary to wait until the vibrations are reduced to the level at which the motor can be started.
Furthermore, in the application that does not allow the rotor to move before starting the motor, a method of pulling the rotor cannot be employed. For example, when a brushless DC motor is adopted as a motor for paper feeding for conveyance of paper in an electrophotographic-type image forming apparatus, a method of pulling a rotor cannot be employed for estimating the initial position of the magnetic pole, which is due to the following reason. Specifically, when the rotor is moved before starting the motor, a sheet of paper is fed accordingly, which leads to jamming.
Thus, an inductive sensing method (for example, see Japanese Patent No. 2547778) is known as a method of estimating a magnetic pole position of a rotor in the rest state without pulling the rotor. The method of estimating an initial position utilizes the property of an effective inductance that slightly changes in accordance with the positional relation between the magnetic pole position of the rotor and the current magnetic field by the stator winding when the stator winding is applied with a voltage at a level not causing rotation of the rotor at a plurality of electrical angles. Specifically, according to Japanese Patent No. 2547778, the position of the magnetic pole of the rotor is indicated by the energization angle showing the highest current value at the time when the stator winding is applied with a voltage at each electrical angle for a prescribed energization time period.
The method of estimating the initial position by inductive sensing utilizes a magnetic saturation phenomenon, for example. When a stator current is caused to flow in a d-axis direction corresponding to the direction of the magnetic pole of the rotor, a magnetic flux by a permanent magnet of the rotor and a magnetic flux by the current are added. Thereby, a magnetic saturation occurs to reduce the inductance. Such reduction of the inductance can be detected by a change of the stator current. Furthermore, in the case of an interior permanent magnet (IPM) motor, saliency occurs by which the inductance in the q-axis direction becomes larger than the inductance in the d-axis direction. Thus, in this case, an effective inductance decreases in the case of a d-axis current even if no magnetic saturation occurs.
One of the problems of the above-mentioned initial position estimation method is a significant dependence on the structure and the characteristics of the motor, which is due to the following reasons. Specifically, depending on the structure of the motor, the effective inductance only slightly changes, with the result that: the stator current scarcely changes in accordance with the energization angle; or the energization angle at which the peak value of the stator current is detected does not indicate the magnetic pole position of the rotor (which will be specifically described in embodiments).
Specifically, when a magnetic saturation phenomenon is utilized, the voltage to be applied and the voltage application time period need to be set to the levels at which magnetic saturation occurs when at least a d-axis current flows. This is because, on the levels at which magnetic saturation scarcely occurs, the energization angle at which the highest current value is achieved may be displaced from the magnetic pole position, and a sufficient signal-to-noise (SN) ratio may not be obtained. However, the motor efficiency has been recently improved to thereby increase motors that are less likely to cause magnetic saturation, so that accurate initial position estimation has been becoming difficult.
On the other hand, if the voltage to be applied and the voltage application time period are excessively increased for significantly reducing the inductance, there occurs a problem that the rotor moves. As a result, detection errors may occur or start-up may fail.
Particularly an inner rotor-type motor causes a problem in the above-described point (but the present disclosure is not limited to an inner rotor-type motor). Since the inner rotor-type motor has small inertia, which is advantageous in the case where the motor is repeatedly started and stopped at frequent intervals. However, when the inertia is small as in the inner rotor-type motor in the case where the initial position is estimated in an inductive sensing scheme, there occurs a problem that a rotor is moved readily by the current flowing through the stator winding during the initial position estimation.
The present disclosure has been made in consideration of the above-described problems occurring in an inductive sensing scheme. An object of the present disclosure is to allow accurate estimation of the initial position of the magnetic pole of the rotor even at a relatively small applied voltage and even in a relatively short voltage application time period when the initial position of the magnetic pole is estimated by an inductive sensing scheme in a sensorless-type motor driven with voltages in a plurality of phases. Other objects and features of the present disclosure will be clearly described in the embodiments.
To achieve at least one of the above-mentioned objects, according to an aspect of the present invention, a motor control device that controls a motor of a sensorless type reflecting one aspect of the present invention comprises: a drive circuit that applies a voltage to each of a plurality of phases of a stator winding of the motor; and a control circuit that controls the drive circuit. When the control circuit estimates an initial magnetic pole position of a rotor of the motor in an inductive sensing scheme, the control circuit performs the following (i) to (v). (i) The control circuit causes the drive circuit to continuously or intermittently apply a voltage to the stator winding at each of a plurality of energization angles while sequentially changing the energization angles, and at a voltage value and for an energization time period, the voltage value and the energization time period being set such that the rotor does not rotate. (ii) The control circuit converts peak values of currents flowing through the phases of the stator winding into a first current component having an electrical angle that is equal to a corresponding one of the energization angles and a second current component that is different in electrical angle by 90 degrees from the first current component, each of the peak values being obtained at a corresponding one of the energization angles. (iii) The control circuit determines a cosine value of each of a plurality of first correction angles that correspond to the respective energization angles, multiplies a value of the first current component corresponding to each of the peak values of the currents flowing through the stator winding by the cosine value of a corresponding one of the first correction angles at each of the energization angles, obtains a total sum of multiplication results obtained at the energization angles, and thereby calculates a first integrated value. (iv) The control circuit determines a sine value of each of a plurality of second correction angles corresponding to the respective energization angles, multiplies a value of the first current component corresponding to each of the peak values of the currents flowing through the stator winding by the sine value of a corresponding one of the second correction angles at each of the energization angles, obtains a total sum of multiplication results obtained at the energization angles, and thereby calculates a second integrated value. (v) The control circuit calculates an estimated initial position of a magnetic pole of the rotor based on a ratio between the first integrated value and the second integrated value.
The advantages and features provided by one or more embodiments of the invention will become more fully understood from the detailed description given hereinbelow and the appended drawings which are given by way of illustration only, and thus are not intended as a definition of the limits of the present invention.
Hereinafter, one or more embodiments of the present invention will be described with reference to the drawings. However, the scope of the invention is not limited to the disclosed embodiments.
While a brushless DC motor will be hereinafter described by way of example, the present disclosure is applicable to a sensorless-type AC motor driven by voltages in a plurality of phases (a brushless DC motor is also a type of an AC motor). The same or corresponding components will be denoted by the same reference characters, and description thereof will not be repeated.
[Entire Configuration of Motor Control Device]
Drive circuit 40 is an inverter circuit in a pulse width modulation (PWM) control system. Drive circuit 40 converts a direct-current (DC) drive voltage DV into a three-phase AC voltage, and outputs the converted three-phase AC voltage. Specifically, based on inverter drive signals U+, U−, V+, V−, W+, and W− as PWM signals received from sensorless vector control circuit 50, drive circuit 40 supplies a U-phase voltage UM, a V-phase voltage VM, and a W-phase voltage WM to brushless DC motor 30. Drive circuit 40 includes an inverter circuit 41, a U-phase current detection circuit 43U, a V-phase current detection circuit 43V, and a pre-drive circuit 44.
Inverter circuit 41 includes a U-phase arm circuit 42U, a V-phase arm circuit 42V, and a W-phase arm circuit 42W. These arm circuits 42U, 42V, and 42W are connected in parallel with one another between the node receiving a DC drive voltage DV and the node receiving a ground voltage GND. For simplifying the following description, the node receiving DC drive voltage DV may be referred to as a drive voltage node DV while the node receiving ground voltage GND may be referred to as a ground node GND.
U-phase arm circuit 42U includes a U-phase transistor FU+ on the high potential side and a U-phase transistor FU− on the low potential side that are connected in series to each other. A connection node Nu between U-phase transistors FU+ and FU− is connected to one end of a U-phase winding 31U of brushless DC motor 30. The other end of U-phase winding 31U is connected to a neutral point 32.
As shown in
Similarly, V-phase arm circuit 42V includes a V-phase transistor FV+ on the high potential side and a V-phase transistor FV− on the low potential side that are connected in series to each other. A connection node Nv between V-phase transistors FV+ and FV− is connected to one end of V-phase winding 31V of brushless DC motor 30. The other end of V-phase winding 31V is connected to neutral point 32.
Similarly, W-phase arm circuit 42W includes a W-phase transistor FW+ on the high potential side and a W-phase transistor FW− on the low potential side that are connected in series to each other. A connection node Nw between W-phase transistors FW+ and FW− is connected to one end of W-phase winding 31W of brushless DC motor 30. The other end of W-phase winding 31W is connected to neutral point 32.
U-phase current detection circuit 43U and V-phase current detection circuit 43V serve as circuits for detecting a motor current with a two-shunt method. Specifically, U-phase current detection circuit 43U is connected between U-phase transistor FU− on the low potential side and ground node GND. V-phase current detection circuit 43V is connected between V-phase transistor FV− on the low potential side and ground node GND.
U-phase current detection circuit 43U and V-phase current detection circuit 43V each include a shunt resistance. The resistance value of the shunt resistance is as small as the order of 1/10Ω. Thus, the signal showing a U-phase current Iu detected by U-phase current detection circuit 43U and the signal showing a V-phase current Iv detected by V-phase current detection circuit 43V are amplified by an amplifier (not shown). Then, the signal showing U-phase current Iu and the signal showing V-phase current Iv are analog-to-digital (AD)-converted by an AD converter (not shown) and thereafter fed into sensorless vector control circuit 50.
A W-phase current Iw does not need to be detected since it can be calculated according to Kirchhoff's current rule based on U-phase current Iu and V-phase current Iv, that is, in accordance with Iw=−Iu−Iv. More generally, among U-phase current Iu, V-phase current Iv, and W-phase current Iw, currents of two phases only have to be detected, and the current value of one remaining phase can be calculated from the values of the detected currents of these two phases.
Pre-drive circuit 44 amplifies inverter drive signals U+, U−, V+, V−, W+, and W− that are PWM signals received from sensorless vector control circuit 50 so as to be output to the gates of transistors FU+, FU−, FV+, FV−, FW+, and FW−, respectively.
The types of transistors FU+, FU−, FV+, FV−, FW+, and FW− are not particularly limited, and, for example, may be a metal oxide semiconductor field effect transistor (MOSFET), may be a bipolar transistor, or may be an insulated gate bipolar transistor (IGBT).
Sensorless vector control circuit 50, which serves as a circuit for vector-controlling brushless DC motor 30, generates inverter drive signals U+, U−, V+, V−, W+, and W−, and supplies the generated signals to drive circuit 40. Furthermore, when brushless DC motor 30 is started, sensorless vector control circuit 50 estimates the initial position of the magnetic pole of the rotor in the rest state by an inductive sensing scheme.
Sensorless vector control circuit 50 may be configured as a dedicated circuit such as an application specific integrated circuit (ASIC), or may be configured to implement its function utilizing a field programmable gate array (FPGA) and/or a microcomputer.
High-order control circuit 60 is configured based on a computer including a central processing unit (CPU), memory, and the like. High-order control circuit 60 outputs a start command, a stop command, a rotation angle speed command value, and the like to sensorless vector control circuit 50.
Unlike the above-described configuration, sensorless vector control circuit 50 and high-order control circuit 60 may be configured as one control circuit by an ASIC, an FPGA or the like.
[Overview of Motor Operation]
Referring to
Before the motor is restarted from a time point t40, the initial position of the magnetic pole of the rotor is estimated in a time period from time point t30 to time point t40. In order to apply a torque in the rotation direction to the rotor, a three-phase AC current needs to be supplied to stator winding 31 at an appropriate electrical angle in accordance with the initial position of the magnetic pole of the rotor. Thereby, the initial position of the magnetic pole of the rotor is estimated. In the present disclosure, an inductive sensing scheme is used as a method of estimating an initial position of a magnetic pole of a rotor.
When rotation of the rotor is started at time point t40, the brushless DC motor is subsequently controlled by a sensorless vector control scheme. The steady operation at a fixed rotation speed is started from a time point t50.
[Coordinate Axes in Sensorless Vector Control Scheme]
Referring to
In the case of a sensorless vector control scheme as a control scheme not utilizing a position sensor for detecting the rotation angle of the rotor, the position information showing the rotation angle of the rotor needs to be estimated by a certain method. The estimated magnetic pole direction is defined as a γ-axis while the direction in which the phase advances at an electrical angle of 90° from the γ-axis is defined as a δ-axis. The angle of the γ-axis from the U-phase coordinate axis is defined as θM. The delay of θM with respect to θ is defined as Δθ.
The coordinate axis in
[Configuration of Sensorless Vector Control Circuit]
Referring to
In the following, the operation of sensorless vector control circuit 50 during the motor operation will be first simply described with reference to
Coordinate transformation unit 55 receives a signal showing U-phase current Iu detected in U-phase current detection circuit 43U of drive circuit 40 and a signal showing V-phase current Iv detected in V-phase current detection circuit 43V of drive circuit 40. Coordinate transformation unit 55 calculates W-phase current Iw from U-phase current Iu and V-phase current Iv. Then, coordinate transformation unit 55 performs coordinate transformation of U-phase current Iu, V-phase current Iv, and W-phase current Iw to thereby generate a γ-axis current Iγ and a δ-axis current Iδ. This is performed specifically according to the following procedure.
First, according to the following equation (1), coordinate transformation unit 55 transforms the currents of three phases including a U-phase, a V-phase, and a W-phase into two-phase currents of an α-axis current Iα and a β-axis current Iβ. This transformation is referred to as Clarke transformation.
Then, according to the following equation (2), coordinate transformation unit 55 transforms α-axis current Iα and β-axis current Iβ into a γ-axis current Iγ and a δ-axis current Iδ as a rotating system of coordinates. This transformation is referred to as Park transformation. In the following equation (2), θM is an electrical angle of the magnetic pole direction estimated by magnetic pole position estimation unit 56, that is, an angle of the γ-axis from the U-phase coordinate axis. Coordinate transformation unit 55 receives the information about estimated magnetic pole position θM from magnetic pole position estimation unit 56 through connection changeover switch 59.
Rotation speed controller 51 receives a start command, a stop command and a target rotation angle speed ω* from high-order control circuit 60. Rotation speed controller 51 determines a γ-axis current command value Iγ* and a δ-axis current command value Iδ* to brushless DC motor 30 based on target rotation angle speed ω* and a rotation angle speed ωM of rotor 35 that is estimated by magnetic pole position estimation unit 56, for example, by proportional-integral (PI) control, proportional-integral-differential (PID) control or the like.
Current controller 52 determines a γ-axis voltage command value Vγ* and a δ-axis voltage command value Vδ*, for example, by PI control, PID control or the like based on γ-axis current command value Iγ* and δ-axis current command value Iδ* that are supplied from rotation speed controller 51, and γ-axis current Iγ and δ-axis current Iδ at present that are supplied from coordinate transformation unit 55.
Coordinate transformation unit 53 receives γ-axis voltage command value Vγ* and δ-axis voltage command value Vδ from current controller 52. Coordinate transformation unit 53 and current controller 52 are connected to each other through connection changeover switch 58. Coordinate transformation unit 53 performs coordinate transformation of γ-axis voltage command value Vγ* and δ-axis voltage command value Vδ*, to thereby generate a U-phase voltage command value Vu*, a V-phase voltage command value Vv*, and a W-phase voltage command value Vw*. This is performed specifically according to the following procedure.
First, according to the following equation (3), coordinate transformation unit 53 transforms γ-axis voltage command value Vγ* and δ-axis voltage command value Vδ into an α-axis voltage command value Vα* and a n-axis voltage command value Vβ*. This transformation is referred to as reverse Park transformation. In the following equation (3), θM is an electrical angle in the magnetic pole direction estimated by magnetic pole position estimation unit 56, that is, an angle of the γ-axis from the U-phase coordinate axis.
Then, according to the following equation (4), coordinate transformation unit 53 transforms α-axis voltage command value Vα* and n-axis voltage command value Vβ* into U-phase voltage command value Vu*, V-phase voltage command value Vv*, and W-phase voltage command value Vw* of three phases. This transformation is referred to as reverse Clarke transformation. In addition, transformation of two phases of α and β into three phases of a U-phase, a V-phase, and a W-phase may be performed using space vector transformation in place of reverse Clarke transformation.
Based on U-phase voltage command value Vu*, V-phase voltage command value Vv* and W-phase voltage command value Vw*, PWM conversion unit 54 generates inverter drive signals U+, U−, V+, V−, W+, and W− as PWM signals for driving the gates of transistors FU+, FU−, FV+, FV−, FW+, and FW−, respectively.
Magnetic pole position estimation unit 56 estimates rotation angle speed ωM of rotor 35 at present and an electrical angle θM showing the magnetic pole position of rotor 35 at present based on γ-axis current Iγ and δ-axis current Iδ, and also on γ-axis voltage command value Vγ* and δ-axis voltage command value Vδ*. Specifically, magnetic pole position estimation unit 56 calculates rotation angle speed ωM at which the γ-axis induced voltage becomes zero, and estimates electrical angle θM showing the magnetic pole position based on rotation angle speed ωM. Magnetic pole position estimation unit 56 outputs the estimated rotation angle speed ωM to high-order control circuit 60 and also to rotation speed controller 51. Furthermore, magnetic pole position estimation unit 56 outputs the information about electrical angle θM showing the estimated magnetic pole position to coordinate transformation units 53 and 55.
[Estimation of Initial Position of Magnetic Pole of Rotor in Rest State]
The following is a detailed explanation about the procedure of estimating the initial position of the magnetic pole of the rotor in the rest state with reference to
Since magnetic pole position estimation unit 56 in
In this case, in the inductive sensing scheme, a constant voltage is applied continuously or intermittently by PWM to stator winding 31 while sequentially changing a plurality of energization angles, so as to detect a change in the current flowing through stator winding 31 at each energization angle. In this case, the time period of energization to stator winding 31 and the magnitude of the voltage applied to stator winding 31 are set at levels at which rotor 35 does not rotate. When the energization time period is extremely short or the magnitude of the voltage applied is extremely small, the initial position of the magnetic pole cannot be detected, so that attention is required.
As described above, the method of estimating the initial position by inductive sensing utilizes the property of an effective inductance that slightly changes in accordance with the positional relation between the magnetic pole position of the rotor and the current magnetic field by the stator winding when the stator winding is applied with a voltage at a level not causing rotation of the rotor at a plurality of electrical angles. This change in inductance is based on the magnetic saturation phenomenon that remarkably occurs in the case of a d-axis current. Furthermore, in the case of an interior permanent magnet (IPM) motor having saliency by which the inductance in the q-axis direction becomes larger than the inductance in the d-axis direction, any change in inductance may be able to be detected even if no magnetic saturation occurs.
Specifically, the method often used for detecting the direction of the magnetic pole of the rotor is to set the command values for the energization time period and the applied voltage at each energization angle (specifically, the command value of the γ-axis voltage) to be constant, and detect a peak value of the γ-axis current within the energization time period to thereby determine that the energization angle at which the peak value attains a maximum value (that is, the energization angle at which an effective inductance attains a minimum value) corresponds to the magnetic pole direction.
However, as described above, when the energization time period and the magnitude of the applied voltage are limited to the levels at which the motor does not rotate, or depending on the structure and the characteristics of the motor, the energization angle at which the peak value of the γ-axis current attains a maximum value may not correspond to the direction of the magnetic pole, or there may be a plurality of energization angles at which the peak value attains a maximum value. The present disclosure provides a method that allows accurate detection of the initial position of the magnetic pole of the rotor even in the above-described case, which will be specifically described later with reference to
Referring to
(1. Setting of γ-Axis Voltage Command Value, Energization Angle and Energization Time Period by Initial Position Estimation Unit)
Initial position estimation unit 57 sets the magnitude of γ-axis voltage command value Vγ*, electrical angle θM referred to as energization angle θM) of each phase voltage to be applied to stator winding 31, and the energization time period. Initial position estimation unit 57 sets δ-axis voltage command value Vδ at zero.
The magnitude of γ-axis voltage command value Vγ* and the length of the energization time period are set such that γ-axis current Iγ with a sufficient SN ratio is obtained in the range not causing rotation of rotor 35. Electrical angle θM is set at a plurality of angles in the range from 0 degree to 360 degrees. For example, initial position estimation unit 57 changes electrical angle θM in a range from 0 degree to 330 degrees by 30 degrees.
(2. Coordinate Transformation Unit 53)
Coordinate transformation unit 53 performs coordinate transformation of γ-axis voltage command value Vγ* and δ-axis voltage command value Vδ (=0), to thereby generate U-phase voltage command value Vu*, V-phase voltage command value Vv*, and W-phase voltage command value Vw*. This coordinate transformation is performed, for example, using reverse Park transformation represented by the above-mentioned equation (3) and reverse Clarke transformation represented by the above-mentioned equation (4).
Specifically, U-phase voltage command value Vu*, V-phase voltage command value Vv*, and W-phase voltage command value Vw* are represented by the following equation (5). In the following equation (5), the amplitude of the voltage command value is defined as V0.
Referring to
(3. PWM Conversion Unit 54)
Again referring to
According to the generated inverter drive signals U+, U−, V+, V−, W+, and W−, drive circuit 40 supplies U-phase voltage UM, V-phase voltage VM, and W-phase voltage WM to U-phase winding 31U, V-phase winding 31V, and W-phase winding 31W, respectively, of brushless DC motor 30. The total number of pulses of the inverter drive signals corresponds to the energization time period that has been set. U-phase current detection circuit 43U and V-phase current detection circuit 43V that are provided in drive circuit 40 detect U-phase current Iu and V-phase current Iv, respectively. The signals showing the detected U-phase current Iu and V-phase current Iv are input into coordinate transformation unit 55.
(4. Coordinate Transformation Unit 55)
Coordinate transformation unit 55 calculates W-phase current Iw based on U-phase current Iu and V-phase current Iv. Then, coordinate transformation unit 55 performs coordinate transformation of U-phase current Iu, V-phase current Iv, and W-phase current Iw, to thereby generate γ-axis current Iγ and δ-axis current Iδ. This coordinate transformation is performed using Clarke transformation in the above-mentioned equation (1) and Park transformation in the above-mentioned equation (2).
In this case, γ-axis current Iγ corresponds to the current component having the same electrical angle as that of the energization angle. Also, δ-axis current Iδ corresponds to the current component that is different in electrical angle by 90 degrees from the energization angle. In the present specification, γ-axis current Iγ is also referred to as the first current component while δ-axis current Iδ is also referred to as the second current component.
In addition, if there is no difference in electrical property and magnetic property among the U-phase, the V-phase and the W-phase, and also if there is no influence of the permanent magnet of rotor 35, the ratio among U-phase current Iu, V-phase current Iv, and W-phase current Iw should be equal to the ratio among voltage command values Vu*, Vv*, and Vw*. Accordingly, in this virtual case, δ-axis current Iδ is zero irrespective of the energization angle while γ-axis current Iγ is a fixed value irrespective of the energization angle. In fact, however, the magnitude of γ-axis current Iγ changes in accordance with the position of the permanent magnet of the rotor. Also, the electrical property and the magnetic property vary among the phases depending on the structures of the stator and the rotor, so that the magnitude of y-axis current Iγ changes.
Referring to
Then, in a time period from time point t3 to a time point t4, initial position estimation unit 57 sets energization angle θM at 30 degrees and also sets γ-axis voltage command value Vγ* at the same set value as the previous value. As a result, γ-axis current Iγ gradually increases from 0 A in a time period from time point t3 to time point t4, and reaches a peak value Iγp2 at time point t4. At and after time point t4, voltage application to stator winding 31 is stopped, so that γ-axis current Iγ gradually decreases.
Subsequently, in a similar manner, the set angle of energization angle θM is changed. Then, at the changed energization angle θM, a pulse-width-modulated constant voltage is applied to stator winding 31. In this case, γ-axis voltage command value Vγ* is the same at each energization angle while the energization time period is also the same at each energization angle. Then, the peak value of γ-axis current Iγ at the end of voltage application is detected.
(5. Estimation of Magnetic Pole Position of Rotor by Initial Position Estimation Unit)
Again referring to
Ideally, energization angle θM at which the peak value of γ-axis current Iγ attains a maximum value is approximately equivalent to an initial magnetic pole position θ of rotor 35. In practice, however, position θ of the magnetic pole of rotor 35 is often not equivalent to energization angle θM at which the peak value of γ-axis current Iγ attains a maximum value.
In the case of
Then, referring to
As shown in
[Specific Example of Problem About Inductive Sensing Scheme]
As described above, when the length of the energization time period and the magnitude of the applied voltage each are limited to the level at which the motor does not rotate, or depending on the structure and the characteristics of the motor, the energization angle at which the peak value of the γ-axis current attains a maximum value may not be equivalent to the direction of the magnetic pole. In the following, a specific example in such a case will be described.
Furthermore,
In the case shown in
Also in the case as described above, initial position estimation unit 57 in the present embodiment can accurately estimate magnetic pole position θ of the rotor. In the following, a specific initial position estimation method in initial position estimation unit 57 will be described.
[Details of Operation of Initial Position Estimation Unit]
(1. Functional Block Diagram)
Cosine computing unit 72 and sine computing unit 73 each receive energization angle θM that is set. For example, an energization angle θM[i] is set at (i−1)×30° in accordance with number i (i is an integer equal to or greater than 1 and equal to or less than 12). For example, energization angle θM=0° on the condition that i=0, and energization angle θM=330° on the condition that i=12.
Cosine computing unit 72 calculates a cosine function value cos (θM[i]) of the received energization angle θM. Sine computing unit 73 calculates a sine function value sin (θM[i]) of the received energization angle θM. In place of actually calculating a trigonometric function value, the calculation result of the trigonometric function value may be stored in the form of a table in advance in memory, from which the cosine function value and the sine function value corresponding to energization angle θM may be read.
Again referring to
Similarly, at each energization angle θM[i], multiplier 75 multiplies peak value Iγp[i] of γ-axis current Iγ corresponding to energization angle θM[i] by sine function value sin (θM[i]) corresponding to energization angle θM[i]. This computation is performed each time number i is updated. Integrator 77 integrates the results of computation by multiplier 75 that are obtained at each energization angle θM[i]. The integrated value (that is, a total sum) of the results of computation by multiplier 75 for all energization angles θM[i] is defined as an integrated value S2.
Based on integrated value S1 calculated by integrator 76 and integrated value S2 calculated by integrator 77, specifically based on the ratio between integrated values S1 and S2, initial position computing unit 78 calculates a phase angle ϕ1 of the approximate curve by a trigonometric function, as will be described below in detail. Phase angle ϕ1 corresponds to the phase of the trigonometric function on the condition that energization angle θM=0, that is, corresponds to a so-called initial phase. It should be noted that phase angle ϕ1 also includes the case where the sign of the initial phase is reversed. Based on this phase angle ϕ1, initial position computing unit 78 calculates the estimate value of the initial position of the magnetic pole of the rotor. More specifically, when the approximate curve by a trigonometric function is assumed to be A0+A1• cos (θM−ϕ1), the estimate value of the initial position of the magnetic pole of the rotor becomes equal to phase angle ϕ1. Furthermore, phase angle ϕ1 can be calculated by the inverse tangent of the ratio between integrated value S1 and integrated value S2, that is, by tan−1(S2/S1).
(2. Theory of Estimate Calculation)
The following is an explanation about the theory based on which the initial position of the magnetic pole of the rotor can be estimated through the above-mentioned procedure.
Peak values Iγp of the γ-axis current that are obtained in accordance with energization angles θM are arranged sequentially in order of energization angles θM so as to plot a graph. The waveform of the obtained peak values Iγp of the γ-axis current is assumed to be approximated by a trigonometric function curve. Specifically, as shown in the following equation (6), it is assumed that peak value Iγp of the γ-axis current as a function of θM is expanded in a series of a plurality of cosine functions having different cycles.
Iγp(θM)=A0+A1 cos(θM−ϕ1)+A2 cos(2θM−ϕ2)+A3 cos(3θM−ϕ3)+ (6)
In the above-mentioned equation (6), A0, A1, A2, . . . each show a coefficient, and ϕ1, ϕ2, ϕ3, . . . each show a phase. The first term on the right side of the above-mentioned equation (6) shows a prescribed component irrespective of θM; the second term on the right side shows the first-order component having a cycle of 360°; and the third term on the right side shows the second-order component having a cycle of 180°. The fourth and subsequent terms show higher order components.
Then, the above-mentioned equation (6) is multiplied by cos (θM), and θM is subjected to an integration computation in an integration section from −π to π. By this computation, the first term on the right side of the above-mentioned equation (6) results in zero, and also, the third and subsequent terms on the right side of the equation (6) also results in zero. Thus, only the computation result in the second term on the right side remains, so that the following equation (7) is eventually obtained. Since the above-mentioned integration calculation corresponds to the above-mentioned calculation of integrated value S1 the integrated value is denoted as S1.
Similarly, the above-mentioned equation (6) is multiplied by sin (θM), and θM is subjected to integration computation in an integration section from −π to π. By this computation, the first term on the right side of the above-mentioned equation (6) results in zero, and also, the third and subsequent terms on the right side of the equation (6) results in zero. Thus, only the computation result in the second term on the right side remains, so that the following equation (8) is eventually obtained. Since the above-mentioned integration calculation corresponds to the above-mentioned calculation of integrated value S2, the integrated value is denoted as S2.
By calculating an inverse tangent using the ratio between integrated value S1 in the above-mentioned equation (7) and integrated value S2 in the above-mentioned equation (8), phase angle ϕ1 can be calculated as shown in the following equation (9).
The above-mentioned calculation can be considered as approximating the change of peak value Iγp of the γ-axis current with respect to energization angle θM by the trigonometric function having a cycle of 360° (that is, one cycle of the electrical angle). In other words, the change of peak value Iγp of the γ-axis current with respect to energization angle θM is approximated by A0+A1• cos (θM−ϕ1). This approximation equation has a maximum value A0+A1 on the condition that θM=ϕ1. Accordingly, ϕ1 that is an electrical angle at which the approximation equation has a maximum value can be estimated as a magnetic pole position of the rotor.
It should be noted that the approximation equation of the trigonometric function curve is not limited to the above-mentioned equations. For example, the following is an explanation about the case where the change of peak value Iγp of the γ-axis current with respect to energization angle θM is approximated by A0+A1• sin (θM+ϕ1). In this case, by calculating integrated values S1 and S2 in the same manner as described above, phase angle ϕ1 can be calculated by tan−1(S1/S2). It should be noted that the ratio between integrated value S1 and integrated value S2 is reversed from the equation (9). This approximation equation has a maximum value A0+ A1 on the condition that θM=90°−ϕ1. Accordingly, 90°−ϕ1 that is an electrical angle θM at which the approximation equation has a maximum value can be estimated as a magnetic pole position of the rotor.
The above description has been made with reference to an integration calculation assuming that energization angle θM continuously changes. When energization angle θM is discrete, integration calculation is changed to total sum calculation as shown in the following equation (10), but the calculation manner is basically the same. The following equation (10) represents the case where there are 12 energization angles θM at each 30°, which is equivalent to the calculation in the above-described case in
(3. One Example of Result of Initial Position Estimation)
The above-mentioned
(4. Flowchart)
In step S100 in
The parameter at which the number of energization times is counted is defined as i. Parameter i is initialized to an initial value 0. Also, the parameter showing the energization time period is defined as j. Parameter j is counted up from 0 to m. Furthermore, integrated values S1 and S2 are initialized to zero.
In this case, energization angle θM[i] corresponding to number of energization times i is stored in the form of a table in memory in advance, for example.
As shown in
Again referring to
In the next step S111, from the table, coordinate transformation unit 53 reads energization angle θM[i] corresponding to parameter i, and cosine value A1[i] and sine value A2[i] at this energization angle θM[i]. Coordinate transformation unit 53 calculates U-phase voltage command value Vu*, V-phase voltage command value Vv*, and W-phase voltage command value Vw* based on cosine value A1 [i] and sine value A2[i] that have been read and γ-axis voltage command value Vγ* that has been set in advance. Furthermore, based on the above-mentioned voltage command values Vu*, Vv*, and Vw*, PWM conversion unit 54 generates inverter drive signals U+, U−, V+, V−, W+, and W−, each of which is a PWM signal.
In the next step S112, based on inverter drive signals U+, U−, V+, V−, W+, and W−, drive circuit 40 starts application of the pulse-width-modulated U-phase voltage UM, V-phase voltage VM, and W-phase voltage M to each phase of stator winding 31 of brushless DC motor 30 (energization ON).
The time period of energization to stator winding 31 is controlled by parameter j. Specifically, while incrementing parameter j showing the pulse number of the PWM pulse (step S113), PWM conversion unit 54 continues to output inverter drive signals U+, U−, V+, V−, W+, and W—until parameter j reaches m that is an upper limit value.
When parameter j reaches m that is an upper limit value (that is, YES in step S114), then in the next step S115, U-phase current detection circuit 43U and V-phase current detection circuit 43V in
Furthermore, initial position estimation unit 57 sets γ-axis voltage command value Vγ* at zero, thereby setting each of U-phase voltage UM, V-phase voltage VM, and W-phase voltage WM that are output from drive circuit 40 at zero (energization OFF). As described above, U-phase current Iu and V-phase current Iv that are measured simultaneously with or immediately before turning-off of energization correspond to the peak values in the energization time period.
Then, in the next step S116, coordinate transformation unit 55 calculates W-phase current Iw based on U-phase current Iu and V-phase current Iv according to Iw=−Iu−Iv. This W-phase current Iw corresponds to the peak value in the energization time period. Based on energization angle θM[i] and cosine value A1[i] and sine value A2 [i] corresponding to this energization angle θM[i], each of which is selected in step S111, coordinate transformation unit 55 calculates γ-axis current Iγ and δ-axis current Iδ from phase currents Iu, Iv, and Iw. These γ-axis current Iγ and δ-axis current Iδ correspond to the peak values (Iγp, Iδp) in the energization time period.
In the next step S117, initial position estimation unit 57 multiplies the peak value of γ-axis current Iγ by a cosine function value A1 [i] of the present energization angle θM[i], and adds the multiplication result to integrated value S1. Furthermore, initial position estimation unit 57 multiplies the peak value of γ-axis current Iγ by a sine function value A2[i] of energization angle θM[i], and adds the multiplication result to integrated value S2.
Up to this point, detection of the peak value of γ-axis current Iγ corresponding to the present parameter i (and accordingly, corresponding to the present energization angle θM[i]) and updates of integrated values S1 and S2 based on the detection result are completed. When parameter i has not reached the number of energization times n (NO in step S118), the process is returned to step S110 and the process in the above-mentioned steps S110 to S117 is repeated.
When parameter i has reached the number of energization times n, that is, when detection of the peak value of γ-axis current Iγ and updates of integrated values S1 and S2 based on the detection result are completed for all of energization angles θM[i] (YES in step S118), initial position estimation unit 57 calculates the inverse tangent of the ratio between integrated values S1 and S2 according to the above-mentioned equation (9), thereby calculating phase angle ϕ1 (step S120). Then in the next step S140, initial position estimation unit 57 sets ϕ1 as the estimated initial position of the magnetic pole of the rotor. Up to this point, the process of estimating the initial position ends.
According to the motor control device in the first embodiment as described above, when the initial position of the magnetic pole of the rotor is estimated by an inductive sensing scheme, the peak value of the γ-axis current is detected at each energization angle. Then, the phase angle of the trigonometric function curve is calculated assuming that the change of the peak value of the γ-axis current with respect to the energization angle is approximated by the trigonometric function curve having the same cycle as one cycle of the electrical angle of the motor. The initial magnetic pole position of the rotor is estimated based on the value of this phase angle. The initial magnetic pole position of the rotor corresponds to the electrical angle at which the approximate curve has a maximum value.
The specific method of calculating the above-described phase angle is as follows. First, the product of the peak value of the γ-axis current and the cosine value of the energization angle is calculated at each energization angle, and then, the total sum of the values of the products obtained at respective energization angles is calculated as a first integrated value. Then, the product of the peak value of the γ-axis current and the integrated value of the energization angle is calculated at each energization angle, and then, the total sum of the values of the products obtained at respective energization angles is calculated as a second integrated value. The inverse tangent of the ratio between the first integrated value and the second integrated value corresponds to the above-mentioned phase angle.
According to the above-mentioned method of estimating the initial position of the magnetic pole of the rotor, the initial position of the magnetic pole of the rotor can be accurately estimated even if the magnitude of the voltage to be applied and the length of the voltage application time period at each energization angle are limited so as to prevent the rotor from rotating. Furthermore, since the voltage application time period at each energization angle can be shortened, the time period required for estimating the initial position can be shortened.
[Modification]
Although the three-phase brushless DC motor has been described by way of example in the above, any AC motor that is driven with the voltages in two or more phases allows estimation of the initial position of the magnetic pole of the rotor in a similar procedure. Specifically, the peak values of the currents in a plurality of phases are subjected to variable transformation at energization angles, and thereby divided into: the first current component (corresponding to the above-mentioned γ-axis current) having the same electrical angle as that of the energization angle; and the second current component (corresponding to the above-mentioned δ-axis current component) that is different in electrical angle by 90 degrees from the energization angle. By using the obtained first current component, the initial position of the magnetic pole of the rotor can be estimated in the same procedure as described above.
Also, according to the above description, one cycle of the electrical angle of the motor is divided equally by 30°. Then, using the peak value of the γ-axis current obtained at each of 12 energization angles, the initial position of the magnetic pole of the rotor is estimated. Theoretically, once the direction of the torque applied to the rotor is determined, the motor can be at least started up. Accordingly, the motor can be started if there is information about the peak value of the γ-axis current obtained at at least two different energization angles of one cycle of the electrical angle of the motor.
The following is an explanation describing by which degree the energization angle should be set in one cycle of the electrical angle, from the viewpoint of an estimation error of the initial magnetic pole position caused by a folding distortion.
When one cycle of the electrical angle of the brushless DC motor is divided equally into L segments and sampled L times (that is, in the case of L energization angles), the component having the wave number larger than L/2 is folded and overlapped with the component having the wave number smaller than L/2 according to the sampling theorem. Thus, the first-order component used for estimating the magnetic pole position of the rotor (that is, the component having a cycle of) 360° is overlapped with the (L-1)-order component having a cycle of 360°/(L-1). Thus, in order to prevent the waveform of the first-order component from being influenced by the folding distortion, it is necessary to limit a ratio R of the amplitude of the (L-1)-order folding component with respect to the amplitude of the first-order component.
As shown in
(i) First, the relation between the energization angle and the peak value of the γ-axis current is experimentally obtained in advance. In this case, the sampling number in one cycle of the electrical angle is increased as much as possible. Then, the Fourier series component of each order is calculated based on the experiment result. (ii) Then, a maximum allowable amount OA [degree] of the error is determined based on the folding distortion included in the estimated initial position. (iii) Then, based on the Fourier series component of each order obtained in the above (i), L is determined such that the ratio [%] of the amplitude of the (L-1)-order component with respect to the amplitude of the first-order component becomes equal to or less than a value that is 1.67 times as large as θA.
The second embodiment will be described with regard to a method of reducing an error of the estimate value of the initial position of the magnetic pole of the rotor according to the first embodiment. Specifically, in place of the method shown in
[Operation of Initial Position Estimation Unit]
(1. Functional Block Diagram)
Cosine computing unit 72 calculates a cosine value of correction angle θf[i] calculated by correction angle computing unit 82. Multiplier 74 multiplies peak value Iγp[i] of γ-axis current Iy corresponding to energization angle θM[i] by cosine function value cos (θf[i]) at each energization angle θM[i].
Similarly, sine computing unit 73 calculates a sine value of correction angle θg[i] calculated by correction angle computing unit 83. Multiplier 74 multiplies peak value Iγp[i] of γ-axis current Iγ corresponding to energization angle θM[i] by sine function value sin (θg[i]) at each energization angle θM[i].
Since other features in
In
(2. Specific Configuration Example of Correction Angle Computing Unit)
Referring to
The reason why the correction amount is cyclically changed as described above is because the error of the estimated initial position of the magnetic pole of the rotor cyclically changes with respect to the electrical angle of the motor. Coefficient βf, phase angle αf, and amplitude Af are selected so as to cancel out this error. Usually, the error of the estimated initial position of the magnetic pole of the rotor changes in the same cycle as one cycle of the electrical angle of the motor. Thus, coefficient βf is set at 1 in many cases. Phase angle αf and amplitude Af can be experimentally set so as to reduce the error of the estimated initial position.
(3. Flowchart)
Specifically, in step S117A, initial position estimation unit 57 calculates correction angle θf[i] corresponding to the present energization angle θM[i] using phase angle αf and amplitude Af that are determined in advance so as to reduce the error of the estimated initial position, according to the following equation.
θf[i]=θM[i]+Af• sin(θM[i]+αf) (11)
Initial position estimation unit 57 multiplies the peak value of γ-axis current Iγ by the cosine function value of correction angle θf[i], and then, adds the multiplication result to integrated value S1. Furthermore, initial position estimation unit 57 multiplies the peak value of γ-axis current Iγ by the sine function value of correction angle θf[i], and then, adds the multiplication result to integrated value S2.
Since other steps in
(4. First Modification)
Specifically, correction table 82A is a table showing the correspondence relation between energization angle θM[i] and correction angle θf[i]. Correction angle θf[i] of correction table 82A shows the computation result by correction angle computing unit 82 in
Similarly, correction table 83A is a table showing the correspondence relation between energization angle θM[i] and correction angle θg[i]. Correction angle θg[i] of correction table 83A shows the computation result by correction angle computing unit 83 in
In
Since other features in
Referring to
(5. Second Modification)
Specifically, cosine function table 87 is a table showing the correspondence relation between energization angle θM[i] and a cosine value of correction angle θf[i]. In cosine function table 87, the cosine value of correction angle θf[i] is obtained by applying a cosine function to the computation result obtained by correction angle computing unit 82 in
Similarly, sine function table 88 is a table showing the correspondence relation between energization angle θM[i] and a sine value of correction angle θg[i]. In correction table 83A, the sine value of correction angle θg[i] is obtained by applying a sine function to the computation result by correction angle computing unit 83 in
Since other features in
In the following, the effect in the second embodiment will be described with reference to a specific example.
The numerical values in the table shown in
As shown in
On the other hand, it turns out that the error of the estimated initial position in the second embodiment is significantly smaller than the error of the estimated initial position in the first embodiment. This consequently proved the following effect. Specifically, in place of the method of estimating the initial position of the magnetic pole of the rotor using the cosine value and the sine value of energization angle θM[i] as in the first embodiment, the cosine value and the sine value of correction angle θf[i] are used to estimate the initial position of the magnetic pole of the rotor, so that the error of the estimate value of the initial position of the magnetic pole of the rotor can be reduced.
As shown in
The third embodiment will be described with regard to an example in which a calibration is performed for further reducing this remaining error of the estimated initial position. Specifically, as in the case where the data shown in
The following is an explanation about the case where the approximate curve by a trigonometric function showing the relation between the energization angle and the γ current peak value corresponding thereto is set at A0+A1• cos (θM−ϕ1). In this case, since the trigonometric function curve exhibits a maximum value on the condition that θM=phase angle can be defined as an estimated magnetic pole position without any change. As described above, it should be noted that, when the approximate curve by a trigonometric function is applied in another function form, the trigonometric function curve does not necessarily attain a maximum value on the condition that θM=ϕ1.
[Method of Estimating Initial Position of Magnetic Pole of Rotor]
Referring to
Then, in the procedure shown in steps S100 to S118 in
Then, as in step S120 in
In the next step S130, initial position estimation unit 57 calculates an error θe corresponding to estimate value ϕ1 of the magnetic pole position by interpolation using the calibration data as show in
In the next step S140, initial position estimation unit 57 sets the corrected estimate value ϕ1)i as an initial position of the magnetic pole of the rotor.
Referring to
In this case, when the rotor is to be pulled, a set value p2 of γ-axis voltage command value Vγ* is set to be smaller than a set value p in
The parameter at which the number of energization times is counted is defined as k. Parameter k is initialized to an initial value 0. The parameter showing the energization time period is defined as j. Parameter j is counted up from 0 to m2.
In this case, an energization angle θM[k] corresponding to the number of energization times k and the cosine value and the sine value each corresponding to energization angle θM[k] are stored, for example, in the form of a table as shown in
In the next step S210, initial position estimation unit 57 increments parameter k showing the number of energization times by one. Furthermore, initial position estimation unit 57 sets parameter j showing the energization time period at an initial value 0.
In the next step 5211, from the table, coordinate transformation unit 53 reads energization angle θM[k] corresponding to parameter k, and the cosine value and the sine value at this energization angle θM[k]. Based on the cosine value and the sine value that have been read and γ-axis voltage command value Vγ* that has been set in advance, coordinate transformation unit 53 calculates U-phase voltage command value Vu*, V-phase voltage command value Vv*, and W-phase voltage command value Vw*. Furthermore, based on the above-mentioned voltage command values Vu*, Vv*, and Vw*, PWM conversion unit 54 generates inverter drive signals U+, U−, V+, V−, W+, and W−, each of which is a PWM signal.
In the next step S212, based on inverter drive signals U+, U−, V+, V−, W+, and W−, drive circuit 40 starts application of the pulse-width modulated U-phase voltage UM, V-phase voltage VM, and W-phase voltage WM to each phase of stator winding 31 of brushless DC motor 30 (energization ON).
The energization time period for stator winding 31 is controlled by parameter j. Specifically, while incrementing parameter j showing the pulse number of the PWM pulse (step S213), PWM conversion unit 54 continues to output inverter drive signals U+, U−, V+, V−, W+, and W—until parameter j reaches m2 as an upper limit value.
When parameter j reaches m2 as an upper limit value (that is, YES in step S214), then in the next step S215, initial position estimation unit 57 sets γ-axis voltage command value Vγ* at zero, thereby setting U-phase voltage UM, V-phase voltage VM, and W-phase voltage WM that are output from drive circuit 40 at zero (energization OFF). Thus, magnetic pole position θ of the rotor becomes equal to energization angle θM.
In the next step S216, initial position estimation unit 57 obtains phase angle ϕ1 as an estimate value of the magnetic pole position of the rotor in the same procedure as that in steps S100 to S120 in
In the next step S217, initial position estimation unit 57 calculates an error θe[k] of estimated magnetic pole position ϕ1 with respect to a true magnetic pole position θ. Since magnetic pole position θ is equal to energization angle θM[k], error θe[k] can be calculated by ϕ1−θM[k].
As above, calculation of error θe[k] at magnetic pole position θ of the rotor corresponding to the present parameter k (equal to energization angle θM[k]) is completed. When parameter k does not reach the number of energization times n2 (NO in step S218), the process returns to step S210, and then, the process in the above-mentioned steps S210 to S217 is repeated.
When parameter k reaches the number of energization times n, that is, when calculation of error θe[k] of the estimate value for each energization angle θM[k] is completed (YES in step S218), initial position estimation unit 57 stores, in memory, the calibration data showing the relation between estimate value ϕ1 of the magnetic pole position of the rotor and its error θe. As above, the process of creating calibration data ends.
According to the motor control device in the third embodiment, the error of the estimate value of the magnetic pole position (that is, the deviation between true magnetic pole position θ and estimated magnetic pole position ϕ1) is detected in advance for each motor. Then, the initial position of the magnetic pole estimated according to the procedure shown in the second embodiment is corrected using the error of the estimate value of the initial magnetic pole position obtained in advance, with the result that the estimation accuracy can be further improved.
[Modification]
In the above description, calibration data is created in the form of a table, to specify error θe corresponding to estimate value ϕ1 of the magnetic pole position obtained by interpolation. In contrast, the polynomial approximation equation showing the relation between estimate value ϕ1 of the magnetic pole position corresponding to already-known magnetic pole position θ and error θe thereof may be derived in advance, or the polynomial approximation equation showing the relation between estimate value ϕ1 of the magnetic pole position corresponding to already-known magnetic pole position θ and the corrected value thereof may be derived in advance. In this case, for estimate value ϕ1 of the magnetic pole position obtained with respect to unknown magnetic pole position θ, corresponding error θe or corrected estimate value ϕ1 may be determined using the derived polynomial approximation equation.
The fourth embodiment will be described with regard to an example in which the motor control device described in each of the first to third embodiments is used for controlling each of motors for driving a paper feed roller, a timing roller, a conveyance roller and the like in an image forming apparatus, which will be hereinafter described with reference to the accompanying drawings.
[Configuration Example of Image Forming Apparatus]
Referring to
Imaging unit 181 includes four photoreceptor cartridges 191, 192, 193, 194, a primary transfer roller 131, a transfer belt 132, a toner bottle 123, a secondary transfer roller 133, and a fixing device 105.
Photoreceptor cartridges 191, 192, 193, 194 form toner images of four colors including yellow (Y), magenta (M), cyan (C), and black (K), respectively. Each of photoreceptor cartridges 191, 192, 193, 194 includes a cylindrical photoreceptor 110, a charging unit 111, an image exposure device 112 including a light source, and a developing device 102 including a developing roller 121.
Charging unit 111 uniformly charges the surface of photoreceptor 110 at a prescribed potential. Image exposure device 112 causes the image corresponding to a document image to be exposed to the charged region of photoreceptor 110. Thereby, an electrostatic latent image is formed on photoreceptor 110. Using developing roller 121 to which developing bias is applied, developing device 102 causes toner to adhere to the electrostatic latent image, thereby forming a visible toner image.
Also, four toner bottles 123 are provided corresponding to their respective photoreceptor cartridges 191, 192, 193, and 194. Toner is supplied from toner bottles 123 to their respective photoreceptor cartridges. A stirring fin 124 for stirring toner is provided inside each of toner bottles 123.
Four primary transfer rollers 131 are provided so as to face their respective four photoreceptors 110. Each of photoreceptors 110 and a corresponding one of primary transfer rollers 131 are pressed against each other with transfer belt 132 interposed therebetween. Furthermore, a bias for attracting toner is applied to each primary transfer roller 131. Thereby, the visible toner image on the surface of photoreceptor 110 after development is transferred onto transfer belt 132.
The visible toner image transferred onto transfer belt 132 is conveyed to the position of secondary transfer roller 133. A transfer voltage is also applied to secondary transfer roller 133 in the same manner as with the primary transfer roller. Thereby, the visible toner image conveyed by transfer belt 132 is transferred onto a sheet of paper as a recording medium 183 at a nip portion between secondary transfer roller 133 and transfer belt 132.
The visible toner image transferred onto recording medium 183 is conveyed to fixing device 105. Fixing device 105 has a fixing roller 150 and uses this fixing roller 150 to heat and pressurize recording medium 183, thereby fixing the visible toner image on recording medium 183. Recording medium 183 after fixation is discharged by a paper discharge roller 151 onto a paper discharge tray 152.
Paper feed mechanism 182 takes in a sheet of paper as recording medium 183 from paper feed cassettes 140 and 142, and then conveys the sheet of paper to secondary transfer roller 133. Paper feed mechanism 182 includes paper feed cassettes 140, 142, paper feed rollers 141, 143, a conveyance roller 144, and a timing roller 145.
Recording media 183 housed in paper feed cassette 140 in the first stage are taken out one by one by paper feed roller 141 and conveyed to timing roller 145. Recording media 183 housed in paper feed cassette 142 in the second stage are taken out one by one by paper feed roller 143 and conveyed through conveyance roller 144 to timing roller 145.
Timing roller 145 stops the supplied recording medium 183, thereby adjusting: the timing at which the visible toner image transferred onto transfer belt 132 is conveyed to secondary transfer roller 133; and the timing at which recording medium 183 is supplied to secondary transfer roller 133.
Document reading device 160 reads the document image on a document sheet 161, to thereby generate image data. In the example shown in
Document sheets 161 placed on document platen 162 are taken in one by one by paper feed roller 170. Document sheet 161 is conveyed by document conveyance rollers 163 and 171, and thereby, reaches a document reading position.
At the document reading position, light source 164 applies light upon the document image on document sheet 161. The light reflected on the surface of document sheet 161 is reflected by mirror 165, and thereafter, condensed by lens 166 so as to be incident upon image sensor 167. As a result, the document image on document sheet 161 is formed as an image on the sensor surface of image sensor 167, and the image data of the document image is produced by image sensor 167.
Document sheet 161 having passed through the document reading position is discharged by document discharge roller 172 onto paper discharge tray 173.
[Application of Brushless DC Motor to Driving Source of Roller]
In image forming apparatus 180 configured as described above, various types of rollers have been driven conventionally using stepping motors in many cases, but brushless DC motors are currently used in many cases. This is because there are problems that a stepping motor is larger in noise, greater in power consumption and lower in efficiency than a brushless DC motor.
However, for closed loop control, a normal brushless DC motor is provided with a Hall element or an encoder for detecting the rotation position of the rotor. Extra costs required for providing such a sensor also cause a new problem that the normal brushless DC motor is higher in cost than the stepping motor that allows open loop control. It is strongly desired to use a sensorless-type brushless DC motor in order to solve the above-described problems.
In this case, the sensorless-type brushless DC motor requires estimation of the initial position of the magnetic pole of the rotor when the motor in the stopped state is started. As a method of estimating the initial position, generally, the stator is energized at a prescribed energization angle, and the magnetic pole of the rotor is attracted to the position corresponding to the energization angle, and thereafter, rotation of the motor is started.
However, in the case of image forming apparatus 180, the above-described method of pulling the rotor cannot be used particularly for the motors for driving paper feed rollers 141, 143 and 170 and timing roller 145, for the following reason. Specifically, in the case of paper feed rollers 141, 143, and 170, a sheet of paper is held by a roller nip. In the case of timing roller 145, the tip of a sheet of paper comes into contact with the inlet of the roller nip. Thus, by pulling the rotor, the roller is rotated to thereby cause a sheet of paper as recording medium 183 to be also moved together, which may cause a paper jam in the case of paper feed rollers 141, 143 and 170, and also, which may lead to difficulty in achieving accurate timing control in the case of timing roller 145.
For the reasons as described above, the initial position of the magnetic pole of the rotor is estimated by an inductive sensing scheme in which the stator winding is applied with a voltage enough to prevent the rotor from rotating, as already described above. In this initial position estimation, the motor control device and the motor controlling method described in the first to third embodiments are applicable in order to estimate the initial position with accuracy and in a short time period.
[Details of Method of Controlling Roller]
In this case, it is desirable that sensorless vector control circuit 50A for controlling brushless DC motor 30A for driving one of paper feed rollers 141, 143, 170 and timing roller 145 serves to correct phase angle ϕ1 as an estimate value of the initial position of the magnetic pole of the rotor by using the calibration data, as described in the third embodiment. Thereby, the initial position of the magnetic pole of the rotor can be more accurately estimated.
For brushless DC motors 30B and 30C for driving the conveyance rollers, it is not necessary to create calibration data and correct phase angle ϕ1 as an estimated magnetic pole position based on the calibration data. However, depending on the configurations of the roller and the motor, some of the conveyance rollers may be desirably calibrated for suppressing errors.
Specifically, focusing attention on a diameter D of the conveyance roller, a speed reduction ratio G from the motor to the conveyance roller, and the number of pole pairs P of the motor, it may be determined based on comparison between at least one of these values and a reference value whether calibration should be performed or not. As diameter D of the conveyance roller becomes larger, errors become more significant. Thus, it is desirable to perform a calibration. As speed reduction ratio G from the motor to the conveyance roller becomes smaller, errors become more significant. Thus, it is desirable to perform a calibration. As the number of pole pairs P of the motor becomes smaller, errors become more significant. Thus, it is desirable to perform a calibration.
Alternatively, when a determination value D/(G•P) is calculated based on the above-mentioned parameters D, P, and G and this determination value is equal to or greater than the reference value (that is, in the case of brushless DC motor 30B in
Referring to
Referring to
Then, sensorless vector control circuit 50 receives a print command from high-order control circuit 60 (S402 and starts the brushless DC motor for conveying the sheets of paper (S403). When printing ends (S404) and a prescribed waiting time has elapsed, high-order control circuit 60 turns off the elements other than a standby power supply to shift to a standby mode (S406). Immediately before shifting to a standby mode, sensorless vector control circuit 50 creates calibration data (S405). This leads to an advantage that a brushless DC motor can be immediately started without having to create calibration data when the standby mode is canceled in response to a print command from high-order control circuit 60.
Although embodiments of the present invention have been described and illustrated in detail, the disclosed embodiments are made for purposes of illustration and example only and not limitation. The scope of the present invention should be interpreted by terms of the appended claims.
Number | Date | Country | Kind |
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JP2019-043944 | Mar 2019 | JP | national |
Number | Name | Date | Kind |
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4876491 | Squires et al. | Oct 1989 | A |
20130049656 | Yasui | Feb 2013 | A1 |
Number | Date | Country |
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2547778 | Aug 1996 | JP |
Number | Date | Country | |
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20200295689 A1 | Sep 2020 | US |