JPH10271900A - Power conversion device - Google Patents

Abstract

PROBLEM TO BE SOLVED: To inhibit a torque ripple by a theoretically introduced compensating method, or to suppress the torque ripple surely even when a control object and an operation state are changed. SOLUTION: A converter 2 converts an AC into a DC and outputs the DC. An inverter 4 converts the DC output from the converter 2 into an AC having arbitrary frequency to drive and control an induction motor 6. The inverter 4 has a vector controller 18 adjusting the voltage vector of the AC output from the inverter 4 so that a torque-component current is kept constant as a flux-component current is pulsated on a rotational coordinate system consisting of an axis of magnetic flux and a torque axis crossing at right angles with the axis of magnetic flux in response to the variation of the DC output from the converter 2.

Description

DETAILED DESCRIPTION OF THE INVENTION

[0001]

BACKGROUND OF THE INVENTION 1. Field of the Invention The present invention relates to a power converter for driving an induction motor comprising a converter and an inverter which receives a DC output voltage from the converter and converts the DC output voltage into a variable voltage / variable frequency alternating current.

[0002]

2. Description of the Related Art In a system for obtaining a direct current from an AC power source by a converter, a harmonic is superimposed on a current flowing from the converter to a capacitor connected to the output side of the converter, so that a DC link voltage (voltage between capacitor terminals) pulsates. . The pulsation frequency is 6 fso which is six times the power supply frequency fso when the power supply is three-phase, and when the power supply is single-phase,
The frequency is 2fso, which is twice the power supply frequency fso. When a three-phase AC is generated from a DC voltage by an inverter, fluctuations in the DC link voltage cause a problem in that a beat phenomenon of a phase current and a ripple in torque occur. The phase current beat phenomenon is a phenomenon in which the phase current oscillates at the frequency of the difference between the fluctuation frequency of the DC link voltage and the inverter frequency fi. Ripple occurs in the torque at the frequency of the fluctuation of the DC link voltage. In particular, when the power supply is a single phase, the fluctuation frequency of the DC link voltage is low, which causes a problem. When the power supply frequency is 50 Hz or 60 Hz, the fluctuation frequency of the DC link voltage is 100 Hz or 120 Hz. Tokuhei 7-46
Japanese Patent Publication No. 918 discloses a control method for removing the imbalance, assuming that the cause of the beat phenomenon of the phase current is a positive / negative imbalance voltage superimposed on the phase voltage.

The above-mentioned publication points out that the torque ripple can be suppressed by finely adjusting the correction coefficient and the phase when adjusting the inverter frequency with respect to the current beat.

[0004]

However, in the above-mentioned publication, regarding the point that the torque ripple can be suppressed by finely adjusting the correction coefficient and the phase, only the effect is pointed out from the result of the simulation, and the grounds are as follows. Nothing is said. Further, although it is pointed out that adjustment according to the inverter frequency is necessary, there is a problem that the adjustment method is unclear because there is no theoretical support, and actual adjustment is difficult.

Accordingly, the present invention has been made to solve the above-mentioned problems, and it is intended to suppress the torque ripple by a compensation method which is theoretically derived, or to surely reduce the torque ripple even if the controlled object or the operating condition changes. It is an object of the present invention to provide a power converter that suppresses power.

[0006]

SUMMARY OF THE INVENTION In order to solve the above-mentioned problems, an invention according to claim 1 is a converter that converts an alternating current into a direct current and outputs the converted direct current, and converts the direct current output by the converter to an arbitrary frequency. An inverter that converts and outputs the alternating current, an induction motor that is driven by the alternating current output by the inverter, and a magnetic flux axis and a torque axis that is orthogonal to the magnetic flux axis according to the fluctuation of the direct current output by the converter. And a vector control means for adjusting an AC voltage vector output by the inverter so that the torque component current becomes constant while the magnetic flux component current pulsates on the rotating coordinate system.

According to a second aspect of the present invention, there is provided a converter for converting an alternating current into a direct current and outputting the same, an inverter for converting the direct current output from the converter into an alternating current having an arbitrary frequency and outputting the same, and an output from the inverter. An induction motor driven by an alternating current and, in response to a change in the direct current output by the converter, on a rotating coordinate system including a magnetic flux axis and a torque axis orthogonal to the magnetic flux axis, while the magnetic flux component current pulsates,
Vector control means for adjusting a phase angle from the magnetic flux axis to an AC voltage vector output by the inverter so that the torque component current is constant.

According to a third aspect of the present invention, in the second aspect, the vector control means adjusts a phase angle from the magnetic flux axis to an AC voltage vector output from the inverter. The output frequency of the inverter is adjusted.

According to a fourth aspect of the present invention, in the first aspect of the present invention, the vector control means generates a magnetic flux component current in accordance with a change in DC output from the converter. Instead of controlling the torque component current to be constant while pulsating, the torque of the induction motor is controlled to be constant.

According to a fifth aspect of the present invention, in the first aspect of the present invention, the vector control means generates a magnetic flux component current in accordance with a change in DC output from the converter. Instead of controlling the torque component current to be constant while pulsating, the power consumption of the inverter is controlled to be constant.

According to a sixth aspect of the present invention, in the first aspect of the present invention, the vector control means generates a magnetic flux component current in accordance with a change in DC output from the converter. Instead of controlling the torque component current to be constant while pulsating, the current flowing into the inverter is controlled to be constant.

According to a seventh aspect of the present invention, in the first aspect of the present invention, the vector control means generates a magnetic flux component current in accordance with a change in DC output from the converter. Instead of controlling the torque component current to be constant while pulsating, control is performed so that the magnitude of the output current of the inverter on the rotating coordinate system is constant.

According to the present invention, a converter for converting an alternating current into a direct current and outputting the same, an inverter for converting the direct current output from the converter into an alternating current of an arbitrary frequency and outputting the same, and an output from the inverter In accordance with the induction motor driven by the alternating current and the fluctuation of the direct current output by the converter, the torque component current is made constant on a rotating coordinate system including a magnetic flux axis and a torque axis orthogonal to the magnetic flux axis. Vector control means for adjusting the magnetic flux component voltage and the torque component voltage.

According to a ninth aspect of the present invention, there is provided a converter for converting an alternating current into a direct current and outputting the same, an inverter for converting the direct current output from the converter into an alternating current having an arbitrary frequency and outputting the same, An induction motor driven by the converter, and in response to a change in DC output from the converter, a magnetic flux component current pulsates on a rotating coordinate system including a magnetic flux axis and a torque axis orthogonal to the magnetic flux axis.
Vector control means for adjusting the magnetic flux component current.

According to a tenth aspect of the present invention, in the invention according to any one of the first to ninth aspects, the adjustment by the vector control means is such that the number of pulses included in a half cycle of the output voltage of the inverter is adjusted. 1 is performed in the control mode.

According to an eleventh aspect of the present invention, in the power conversion device according to any one of the first to ninth aspects, the adjustment by the vector control means includes a pulse included in a half cycle of the output voltage of the inverter. It is characterized in that it is not performed according to the number.

[0017]

Embodiments of the present invention will be described below in detail with reference to the drawings. FIG. 1 is a configuration diagram of a power converter showing a first embodiment of the present invention.
The single-phase converter 2 converts the single-phase alternating current of the power supply 1 to direct current,
Further, the inverter 4 converts a direct current into an alternating current to convert the direct current into an alternating current.
Drive. The power supply 1 assumes a single phase. In this case, since the current flowing from the single-phase converter 2 to the DC capacitor 3 includes a harmonic having a frequency twice as high as the power supply frequency of the power supply 1, the DC link voltage pulsates at twice the power supply frequency. In the present embodiment, it is assumed that the control system for operating the inverter 4 and driving the induction motor 6 is a so-called vector control system. Vector control is a method of controlling current, voltage, and magnetic flux as vector quantities, and performs control on a rotating coordinate system defined as dq axes. The d axis is called the magnetic flux axis, and the q axis is called the torque axis. Vector control is a technique known from various documents such as “Electrical Equipment Engineering II” published by the Institute of Electrical Engineers of Japan, and there are many methods. In the present embodiment, for example, by controlling the slip angle frequency appropriately, the secondary magnetic flux of the induction motor 6 is controlled by the slip frequency type vector control that matches the d-axis, and has no current minor loop.

The configuration of the vector control device 18 will be specifically described. The slip angle frequency calculator 10 calculates a slip angle frequency reference ωs ^* by inputting a secondary magnetic flux command value φ2d ^* and a torque command value Tm ^* to be described later, and the adder 101 detects the slip angle frequency reference ωs ^* . Motor speed ωr and slip angle frequency reference ωs ^*
To calculate the inverter angular frequency ωi. The inverter angular frequency ωi is integrated by the integrator 11 and becomes an inverter output voltage phase reference value θi ^* . d
Axis current command calculator 12 calculates the first order d-axis current command value id ^* Enter the secondary magnetic flux command value .phi.2d ^*. The q-axis current command calculator 13 calculates the secondary magnetic flux command value φ2d ^* and the torque command value Tm.
^{With *} as an input, a primary q-axis current command value iq ^* is calculated. And a d-axis voltage command calculator 14 and a q-axis voltage command calculator
Reference numeral 15 inputs the primary d-axis current command value id ^* and the primary q-axis current command value iq ^* , and calculates the d and q-axis voltage command values Vd ^* and Vq ^* necessary for flowing those currents. I do. In the coordinate system converter 16, the voltage command value Vd on the dq axis rotation coordinate system
^*, The magnitude of the voltage command value Vq ^* | V | and voltage vector (Vd ^*, Vq ^*) for the d-axis to calculate the phase angle reference value .theta.v ^* (see FIG. 2). The phase angle reference value θv ^* of this voltage command is added to a correction amount Δθv described later by an adder 102 to become a phase angle θv of the output voltage on the dq axis rotary coordinate system. The output voltage phase angle θi is added to the value θi ^* . The gate controller 17 generates a gate signal for driving the inverter 4 according to the output voltage phase angle θi.

Further, the vector control device 18 includes the inverter 4
Constitute a vector control system in the case of operating with one pulse. The vector control for one pulse is known from literatures ("Vector control in fixed voltage mode", H7 IEEJ Industrial Application Division National Convention, No. 196). The magnetic flux command corrector 9 compares the magnitude | V | of the output voltage command value on the dq axis rotation coordinate system with the magnitude of a DC link voltage described later, and corrects the secondary flux reference φd ^ref so that they match. To output the secondary magnetic flux command value φ2d ^* .

The voltage detector 8 detects the DC link voltage Vdc, and the fluctuation calculator 19 calculates a fluctuation sine wave ΔVdc which is a fluctuation of the DC link voltage Vdc. The compensation amount calculator 20 calculates the fluctuation amount ΔVdc of the DC link voltage and the DC link voltage V
Enter dc. The compensation amount calculator 20 is configured, for example, as shown in FIG. Compensation gain calculator 21, compensation phase calculator 22
Are the output angular frequency ωi of the inverter, the angular frequency ωr of the motor, the secondary magnetic flux command value φ2d ^* , the primary q-axis current command value iq
^* , The phase angle θv of the output voltage on the dq axis rotating coordinate system, the power supply frequency ωso or the fluctuation frequency of the DC link voltage Vdc and the parameters of the motor, and the compensation gain K,
The compensation phase γ is calculated.

These operations are described later, for example (2.
It is also possible to calculate from the formulas 9) and (30), or to have a table for each input parameter and read from the table. The sine wave gain phase adjuster 23 compensates the amplitude of the fluctuating sine wave ΔVdc of the DC link voltage, which is the output of the fluctuating amount calculator 19, by the compensation gain K as shown in FIG. The phase is compensated by γ. The output of the sine wave gain phase adjuster 23 is also a sine wave. This output sine wave is divided by the DC link voltage Vdc, and becomes a correction amount Δθv to the output voltage phase angle on the dq axes of the inverter. This correction amount Δθv is calculated based on the coordinate system converter
The adder 102 adds the dq-axis output voltage phase angle reference value θv ^* , which is the 16 output, to an output voltage phase angle θv on the dq-axis rotating coordinate system. The output voltage phase angle θv is added by an adder 103 to an output voltage phase angle reference value θi ^* , which is a reference for the phase of the d-axis of the rotating coordinate system with respect to the fixed coordinate a-axis, and becomes an output voltage phase angle θi of the inverter. FIG. 2 shows the state of the output voltage vector on the dq-axis rotating coordinate system, and shows the output voltage vector reference V ^* (the vector symbol → is omitted, the same applies hereinafter) and the corrected output power vector V. I have. The phase angle from the d-axis to the output voltage vector reference V ^* is θv ^* , the phase angle correction amount superimposed on the reference is Δθv, and the phase angle from the d-axis to the output voltage vector V obtained by adding the two is θv.

The gate controller 17 generates a gate signal based on the output voltage phase angle θi of the inverter. The principle by which torque ripple can be suppressed by the above configuration will be described below.

First, the principle of suppressing the torque ripple generated in the induction motor 6 under the condition that the DC link voltage Vdc fluctuates will be briefly described, and then, the control method for suppressing the ripple will be described based on theoretical considerations.

In this embodiment, a dq-axis rotating coordinate system in which the secondary magnetic flux axis and the d-axis are matched is introduced. The dq axis rotation coordinate system rotates on the stationary coordinate system in accordance with the rotation frequency of the secondary magnetic flux. The d-axis is called the magnetic flux axis, and the q-axis is called the torque axis. In a steady state where there is no change in the DC link voltage Vdc, each state quantity on the dq axis rotation coordinate system is a DC quantity. This consideration on the dq axis rotation coordinate system is based on the same concept as so-called vector control. Strictly speaking, the torque generated in the induction motor 6 is a value obtained by multiplying the outer product by a coefficient, but is a product of the secondary magnetic flux and a torque current (q-axis current) Iq which is a primary current component orthogonal to the secondary magnetic flux. The area is as shown in FIG.

Assuming that the DC link voltage Vdc is constant as shown in FIG. 5B, the output voltage vector V of the inverter 4 stops on the dq axis rotation coordinates. Since the output voltage vector V stops, the current vector I1 also stops. Therefore, since no ripple exists in the q-axis current, that is, the torque current Iq, no torque ripple occurs.

However, when the DC link voltage Vdc fluctuates as shown in FIG. 5C, the magnitude of the output voltage vector V also fluctuates. In particular, in an operation mode called a one-pulse mode, it is impossible to arbitrarily control the magnitude of the output voltage, so that the fluctuation of the DC link voltage Vdc directly affects the output voltage. Since the current of the inverter 4 flows according to the output voltage, the current vector I1 also fluctuates. For this reason, the torque current Iq fluctuates, and torque ripple occurs.

In all the operation modes including the one-pulse mode, the phase angle θv of the output voltage vector can be controlled from the d-axis. Thus, the torque angle Iv is controlled to be constant by manipulating the phase angle θv as shown in FIG. This is d
This is a result of changing the trajectory of the fluctuation of the output voltage vector V on the q-axis coordinate system. In the one-pulse mode, the magnitude of the output voltage vector V is uniquely determined by the DC link voltage Vdc. Therefore, when the DC link voltage Vdc fluctuates, the magnitude of the output voltage vector V also fluctuates, and this fluctuation is suppressed. It is impossible. In this method, the DC link voltage V
The influence of the fluctuation of dc is all reflected on the ripple of the excitation (d-axis) current Id, and the torque (q-axis) current is controlled to be constant.
The follow-up characteristic of the secondary magnetic flux is slow with respect to the fluctuation of the exciting current Id, and the secondary magnetic flux is almost constant. Since there is no change in both the torque current and the secondary magnetic flux, it is possible to suppress the change in torque.

The principle of suppressing torque ripple has been briefly described above. Hereinafter, from a theoretical consideration, it is shown that the torque ripple can be suppressed by adopting the configuration of FIG. In general, the characteristics of the induction motor 6 are described below on a dq axis rotation coordinate system. The generated torque is expressed by equation (3).

[0029]

(Equation 1)

Where Vd: primary voltage of d-axis Vq: primary voltage of q-axis id: primary current of d-axis iq: primary current of q-axis φ2d: secondary magnetic flux of d-axis φ2q: secondary magnetic flux of q-axis ωr: motor the rotational angular frequency .omega.s: slip angular frequency .omega.i: inverter output angular frequency R1: 1 primary resistance R2: 2 primary resistance L1: 1 primary self-inductance L2: 2 primary self-inductance M: mutual inductance ^{R12: R1 + R2 · M 2} / L2 ² σ: 1−M ² / (L 1 · L ² ) S: Laplace operator Tm: Motor torque If the d-axis is selected so as to coincide with the secondary magnetic flux axis, the q-axis secondary magnetic flux φ2q becomes zero and the rotation of the coordinates The inverter output frequency ωi, which is the speed, matches the secondary magnetic flux angular frequency ωφ.
Therefore, the equations (1) to (3) can be converted into the following equations.

[0031]

(Equation 2)

Where ωφ is the secondary magnetic flux angular frequency, and the average value is ￣ for each state quantity on the dq axis rotation coordinate system.
And fluctuating components are indicated with Δ. Here, it is assumed that the fluctuating component is a fluctuating frequency of the DC link voltage Vdc. In the case of the single-phase power supply shown in FIG.
Hz is a fluctuation component of 100 Hz, and if the power supply is 60 Hz, it is a fluctuation component of 120 Hz.

[0033]

(Equation 3) The state equation regarding the amount of fluctuation is as follows.

[0034]

(Equation 4)

Equation (8) is solved for the fluctuation amount Δφ2d of the d-axis secondary magnetic flux and the fluctuation amount Δiq of the torque current, and the torque fluctuation amount ΔTm is converted into the dq-axis output voltage fluctuation amount ΔVd, It can be represented by ΔVq.

[0036]

(Equation 5) Let the torque fluctuation in equation (10) be zero. Under these conditions, the relationship between the fluctuation amounts ΔVq, ΔVq of the dq-axis output voltage is calculated.

[0037]

(Equation 6)

Therefore, the torque ripple can be reduced by the relationship between the variation ΔVd of the d-axis output voltage and the variation ΔVq of the q-axis output voltage as expressed by the following equation (14). Assuming that the power supply angular frequency is ωso, the frequency twice as high
The problem is torque ripple at ωso. Therefore, if the variation ΔVd of the d-axis output voltage is given by the equation (16), the torque ripple can be suppressed when the variation ΔVq of the q-axis output voltage is given by the equation (17).

[0039]

ΔVd = ΔVsin (2ωsot + ψ) (16) ΔVq = K · ΔVsin (2ωsot + ψ + γ) (17) K = | H1 (2jωso) | (18) γ = arg ｛H1 (2jωso)｝ (19) where ωso : Power supply angular frequency j: Complex number FIGS. 7 and 8 depict the trajectory of the fluctuation of the dq-axis output voltage vector from the simulation results. The horizontal axis represents the fluctuation amount ΔVd of the d-axis output voltage, and the vertical axis represents the fluctuation amount ΔVq of the q-axis output voltage. FIG. 7 shows a fluctuation trajectory of the dq-axis output voltage when the torque ripple remains, and FIG. 8 shows a dq axis when the torque ripple is suppressed.
This is the fluctuation trajectory of the export voltage. 7A and 8A, FIG. 7A shows that the detected d-axis output voltage variation ΔVd is (1)
6)-Variation ΔVq of q-axis output voltage obtained by equations (19)
(B) illustrates the detected variation ΔVq of the q-axis output voltage with respect to the detected variation ΔVd of the d-axis output voltage. (C) is a superposition of (a) and (b). In FIG. 7 where the torque ripple remains, the trajectories (a) and (b) do not match. This means that equation (14) is not satisfied, while in the case of FIG. 8 in which torque ripple is suppressed, the trajectories (a) and (b) match, and equation (14) is satisfied. Can be confirmed. This indicates that the above analysis results are valid.

Next, the fluctuation amounts ΔVq, Δ of the dq-axis output voltage
The relationship between Vq and dq-axis output voltage vector V is derived. FIG.
Indicates an output voltage vector V of the inverter on the dq-axis rotating coordinate system. The d axis, that is, the secondary magnetic flux axis is the real axis,
Assuming that the q axis is an imaginary axis, the voltage vector V can be represented by the following equation.

[0041]

(Equation 8)

Vdc is the DC link voltage, and θv is the phase angle from the d axis, ie, the secondary magnetic flux axis to the output voltage vector axis. The DC link voltage Vdc and the phase angle θv are separated into an average value and a fluctuation amount. The subscript ￣ indicates the average value, and the subscript Δ indicates the amount of fluctuation.

[0043]

(Equation 9) From the dq-axis output voltage vector V shown in the equation (20), the following equation holds for the vector variation ΔV.

[0044]

[Equation 10] Then, the vector variation ΔV of the voltage vector represented by the equation (22) is divided into a real part and an imaginary part, and is expressed by the variation amounts ΔVd and ΔVq of the dq-axis output voltage, and the equation (23) is obtained.

[0045]

[Equation 11]

Equation (23) indicates that the d-axis voltage and the q-axis voltage are affected by the fluctuation ΔVdc of the DC link voltage Vdc. It also shows that the d-axis voltage and the q-axis voltage can be controlled by manipulating the phase angle θv of the output voltage.

Accordingly, when the fluctuation amounts ΔVd and ΔVq of the dq-axis output voltage expressed by the expression (23) satisfy the conditional expression expressed by the expression (14), the torque ripple can be suppressed. Therefore, substituting equation (23) into equation (14), the variation Δ of phase angle θv
Especially about θv.

[0048]

(Equation 12)

Here, assuming that the variation ΔVdc of the DC link voltage is given by the following equation (27), the correction amount Δθv to the phase angle of the output voltage vector on the dq axis rotating coordinate system is (24) to (26)
This can be expressed by equation (28).

[0050]

(Equation 13) Then, the compensation amount Δθv calculated by the equation (28) is added to the output voltage phase angle reference value θv ^* of the inverter 4 to obtain the output voltage phase angle θv.

[0051]

[Expression 14] θv = θv ^* + Δθv (31) As described above, the inverter 4 is calculated based on the expressions (27) to (30).
It can be understood that the torque can be controlled to be constant by manipulating the output voltage phase θv in the dq-axis rotating coordinate system.

As can be confirmed from the equations (12), (25) to (30), in order to suppress the torque ripple under the condition that the DC link voltage Vdc fluctuates, the output angular frequency ωi ( Secondary magnetic flux angular frequency ωφ), motor rotational angular frequency ωr, output voltage vector phase angle θv on dq axis rotary coordinate system, torque current iq, secondary magnetic flux φ2d, motor parameters, power supply frequency ωso or DC link voltage A fluctuating frequency is required. Therefore, it can be seen that in order to strictly suppress the torque ripple, it is necessary to appropriately adjust the correction amount Δθv according to the change in the state amount described above. For example, in train control, not only the speed but also the state such as a notch command and powering / regeneration must be grasped and appropriate compensation performed.

FIGS. 9 to 11 show simulation results. In this simulation, the system shown in FIG.
The power frequency ωso is set to 60 Hz. Therefore, the DC link voltage Vdc pulsates at 120 Hz. FIG. 9 shows a response when the beatless control is not performed. Inverter 4
It can be confirmed that the U-phase current Iu, which is the output of the above, makes a large beat. Overcurrent is apt to occur for this beat. As for the torque Tm, a torque ripple of 120 Hz is generated. Vibration and noise caused by this cause a problem. The torque current Iq and the excitation current Id are both 1
Pulsating at 20 Hz.

FIG. 10 shows the result of the conventional beatless control method. When the inverter frequency ωi is 120 Hz, the torque ripple increases when the inverter frequency ωi departs from 120 Hz in order to adjust so as to suppress the beat phenomenon. This is because the effect of the beatless control is degraded due to an operation state different from the operation condition at the time of adjustment, and is not limited to a change in the frequency ωi of the inverter. Therefore, it is necessary to change the compensation method according to the operating state in order to suppress the torque ripple in any operating state. FIG. 11 shows the results when the compensation parameters are changed according to the driving conditions, as shown in the equations (27) to (30). It can be seen that torque ripple is controlled in all inverter frequency bands.
At this time, the beat of the U-phase current Iu is also suppressed at the same time. In this control method, the torque current Iq is controlled to be constant, and can be confirmed from simulation results. At this time, since the exciting current Id is not particularly controlled, a pulsation of 120 Hz is generated. This means that the torque current Iq is kept constant by reflecting all the effects of the fluctuation of the DC link voltage Vdc on the exciting current Id. No pulsation occurs in the secondary magnetic flux φ2 regardless of the pulsation of the exciting current Id. This is because the response of the secondary magnetic flux φ2 is slow,
This indicates that it cannot respond to the 120 Hz ripple of the exciting current Id. The torque Tm is represented by the product of the secondary magnetic flux φ2 and the q-axis current, that is, the torque current Iq. Secondary magnetic flux φ
In addition, since there is no ripple in the torque current Iq, the torque ripple is suppressed.

Therefore, by adopting the above-described configuration, it is possible to suppress the fluctuation of the torque caused by the pulsation of the DC link voltage Vdc. In consideration of the operating condition, the output angular frequency ωi of the inverter, the rotational angular frequency ωr of the motor, the output voltage vector phase angle θv on the dq axis coordinate system, the torque current iq,
Compensation value Δθv according to secondary magnetic flux φ2d, motor parameter, power supply frequency ωso, or fluctuation frequency of DC link voltage
Therefore, the effect can be expected under any driving conditions. The compensation method is sought analytically, and can be easily adjusted in an actual machine.

FIG. 12 is a block diagram showing a second embodiment of the present invention. This embodiment differs from the first embodiment only in the calculation unit (that is, the addition unit 102 in FIG. 1) of the output voltage phase angle θv on the dq axis rotation coordinate system, and therefore only this part will be described. .

For example, when considering a train drive system,
As the PWM method, for example, asynchronous, synchronous 9 pulses determined by the number of pulses included in a half cycle of the output voltage, synchronous 5
There are various pulse modes such as pulse, synchronous 3 pulse, and synchronous 1 pulse. Which pulse mode is used in which speed band depends on the control target and the switching element. FIG. 12 shows that the phase angle correction to the output voltage on the dq axis coordinate system is not performed in the pulse mode. For example, in a certain pulse mode, the changeover switch 102a adds 0 to the output voltage phase angle reference θv ^* and the adder 102b instead of the phase angle Δθv to the output voltage on the dq axis coordinates, and Obtain the output voltage phase angle θv.

With such a configuration, it is possible to perform appropriate beatless control for each pulse mode. Therefore, in the low-speed range where torque ripple as a beat phenomenon does not occur, or in the pulse mode in which the magnitude of the output voltage vector can be controlled freely and at high speed, unnecessary beatless control is cut off, unnecessary interference is suppressed, and torque Deterioration of characteristics can be suppressed.

FIG. 13 is a block diagram showing a third embodiment of the present invention. The present embodiment is different from the first embodiment in that a fluctuation calculator for calculating the fluctuation of the DC link voltage is provided.
Since only 19 is different, only this part will be described.

For example, in a train operating over both power supply bands of 50 Hz / 60 Hz, the frequency of the fluctuation of the DC link voltage also changes to 100 Hz / 120 Hz according to the power supply. In such a case, as shown in FIG. 13, a 100-Hz band-pass filter 24 and a 120-Hz band-pass filter 25 are provided, and the output of the band-pass filter is switched according to the power supply frequency detected by the power supply frequency detector 26. Indicates a device to be switched. For example, when it is detected that the power supply frequency is 50 Hz, the output of the 100 Hz band-pass filter is used as the variation ΔVdc of the DC link voltage.
And

By adopting the above configuration, even when the power supply frequency is switched between 50 Hz and 60 Hz, the characteristic of the band-pass filter is changed and the frequency component of the change is extracted, so that gain and phase are added at the detection stage. And the effect of beatless control can be maintained. The bandpass filter extracts only a specific frequency component. 120 for 100Hz detection
The Hz signal results in reduced gain and phase rotation. Therefore, in a beatless compensator assuming a power supply frequency of 50 Hz, the effect of suppressing torque ripple is greatly deteriorated in a section of a power supply frequency of 60 Hz.

Here, the power supply frequency is shown as the signal used for switching, but the same effect can be obtained by detecting the fluctuating frequency of the DC link voltage and using this as the switching signal. FIG. 4 is a block diagram showing a fourth embodiment of the present invention. This embodiment is different from the first embodiment in that
Only the variation calculator 19 for calculating the variation of the DC link voltage is different, and only this portion will be described. In FIG. 14, FIG.
Even when the power supply frequency is slightly changed, including the case where the power supply frequency is switched to 50 Hz / 60 Hz as shown in the above, the frequency of the change is detected and the frequency characteristics of the band-pass filter are controlled. Is shown. Fig. 14
Shows a configuration realized by software.
For example, the transfer function of the band-pass filter 29 is represented by Expression (32). Then, the frequency obtained by doubling the angular frequency [rad / s] detected by the power supply frequency detector 26 by the multiplier 28 is set as the characteristic frequency F [rad / s]. F obtains a similar effect even when the fluctuation frequency of the DC link voltage is set.

[0063]

(Equation 15) Also, as in FIG. 13, a plurality of band-pass filters may be provided for stepwise frequencies, and appropriate switching may be performed according to the frequencies.

With the above configuration, even when the power supply frequency is switched to 50 Hz / 60 Hz, even if the power supply frequency is slightly changed, the characteristics do not change with respect to the fluctuation frequency. Can be maintained. If the Q-factor of the band-pass filter is high without changing the characteristics of the band-pass filter with respect to the fluctuation of the power supply frequency, the signal gain deterioration and phase rotation are large,
As a result, highly accurate torque characteristics cannot be obtained. By making the characteristic frequency of the band-pass filter correspond to the instantaneous power supply frequency, the effect can always be obtained.

Here, the power supply frequency is shown as the signal used for switching, but a similar effect can be obtained by detecting the fluctuating frequency of the DC link voltage and using this as the switching signal. FIG. 15 is a configuration diagram of a power conversion device according to a fifth embodiment of the present invention. This embodiment is different from the first embodiment only in the calculation unit of the correction amount Δθv to the output voltage phase angle on the dq axis rotation coordinate system, and therefore, only this part will be described.

The phase current of the motor detected by the current detector 5 is converted by the coordinate system converter 30 into a current amount on dq axis coordinates. The q-axis current Iq is subtracted from a q-axis current command value Iq ^* used in the vector controller 18 by a subtractor 104.
Deducted by This q-axis current deviation is input to the q-axis current suppressor 31. The q-axis current suppressor 31 performs, for example, PI control using the q-axis current deviation as an input. This control method is not limited to PI control. The output of the q-axis current suppressor 31 is the correction amount Δθv to the output voltage phase angle on the dq-axis coordinate system.

With the above configuration, the output voltage phase angle is manipulated according to the deviation of the q-axis current, so that the q-axis current, that is, the torque current can be controlled to be constant. As described above, since the secondary magnetic flux is maintained substantially constant, torque ripple can be suppressed. Also,
Since the feedback control is used, the effect can be expected even when there is a disturbance or a modeling error.

FIG. 16 is a configuration diagram of a power converter according to a sixth embodiment of the present invention. This embodiment is different from the first embodiment only in that the calculation unit of the correction amount Δθv to the output voltage phase angle on the dq axis rotation coordinate system is different.
Only this part will be described.

A torque detector 32 is installed on the induction motor 6,
The generated torque detected by the torque detector 32 is input to the torque pulsation detector 33. Where the torque detector
A similar effect can be obtained by using a torque estimator for estimating the generated torque instead of 32. The torque pulsation detector 33 calculates and detects the torque pulsation ΔT, and inputs it to the torque pulsation suppressor. The torque pulsation suppressor 34 performs, for example, PI control using the torque pulsation amount ΔT as an input. This control method is not limited to PI control. The output of the torque pulsation controller 34 is a correction amount Δθv to the output voltage phase angle on the dq axis coordinate system.

With the above configuration, the phase angle of the output voltage is controlled according to the torque pulsation, so that the torque pulsation can be suppressed. Because of feedback control, even when there is disturbance or modeling error,
The effect can be expected.

FIG. 17 is a configuration diagram of a power converter showing a seventh embodiment of the present invention. This embodiment is different from the first embodiment only in that the calculation unit of the correction amount Δθv to the output voltage phase angle on the dq axis rotation coordinate system is different.
Only this part will be described.

The voltage detector 8 detects the DC link voltage Vdc, and the current detector 35 detects the current flowing from the DC capacitor 3 to the inverter 4. The power calculator 36 calculates the power consumed by the inverter 4. For example, the power P of the inverter 4 is obtained by multiplying the DC link voltage by the current flowing from the DC capacitor 3 to the inverter 4. The power P calculated by the power calculator 36 is input to the power fluctuation calculator 37, and the power fluctuation ΔP is calculated.

The calculated power fluctuation ΔP is input to the power fluctuation suppressor 38. The power fluctuation suppressor 38 performs, for example, PI control using the power fluctuation ΔP as an input. This control method is not limited to PI control. The output of the power fluctuation suppressor 38 is the correction amount Δθv to the output voltage phase angle on the dq axis coordinate system.

With the above configuration, it is possible to control the phase angle of the output voltage according to the power fluctuation of the inverter, and to suppress the fluctuation of the power consumed by the inverter. Most of the power consumed by the inverter is the output of the motor. Therefore, by controlling the power consumed by the inverter to be constant, fluctuations in the motor output can be suppressed. Since the torque ripple affects the motor output, it is possible to suppress the torque ripple by suppressing the fluctuation of the motor output.

FIG. 18 is a configuration diagram of a power converter showing an eighth embodiment of the present invention. This embodiment is different from the first embodiment only in that the calculation unit of the correction amount Δθv to the output voltage phase angle on the dq axis rotation coordinate system is different.
Only this part will be described.

The current Iinv flowing from the DC capacitor 3 to the inverter 4 detected by the current detector 35 is input to the current pulsation calculator 39. The current pulsation calculator 39 calculates a pulsation ΔIinv of the input amount Iinv. The calculated inverter current fluctuation amount ΔIinv is input to current pulsation suppressor 40. The current pulsation suppressor 40 performs, for example, PI control with the amount of change ΔIinv of the current to the inverter as an input. This control method is not limited to PI control.
The output of the current pulsation suppressor 40 is a correction amount Δθv to the output voltage phase angle on the dq axis coordinate system.

With the above configuration, d is determined according to the current ripple flowing from DC capacitor 3 to inverter 4.
By manipulating the output voltage phase angle on the q-axis, it is possible to suppress current ripple flowing from the DC capacitor 3 to the inverter 4. Since the power consumed by the inverter fluctuates simultaneously with the occurrence of the torque ripple, the current flowing into the inverter also pulsates. By suppressing the pulsation of the inverter current, the power fluctuation of the motor is suppressed. Therefore, torque ripple can be suppressed.

FIG. 19 is a configuration diagram of a power converter showing a ninth embodiment of the present invention. This embodiment is different from the first embodiment only in that the calculation unit of the correction amount Δθv to the output voltage phase angle on the dq axis rotation coordinate system is different.
Only this part will be described.

The motor phase current detected by the current detector 5 is converted by the coordinate converter 30 into currents Id and Iq on the dq axis rotating coordinate system. The current vector length calculator 41 calculates the magnitude I of the current vector on the dq axis rotating coordinate system from the square root of the sum of squares of the currents Id and Iq. The calculated current vector length I is input to the current pulsation calculator 42, and the pulsation amount ΔI is calculated. Current pulsation ΔI
Is input to the current pulsation suppressor 43. Current pulsation suppressor 43
Then, for example, PI control is performed. This control method is called PI
It is not limited to control. The output of the current pulsation suppressor 43 is the correction amount Δθ to the output voltage phase angle on the dq axis coordinate system.
v.

With the above configuration, it is possible to suppress the fluctuation of the magnitude of the current vector on the dq axis rotation coordinate system. As described above, the torque ripple can be suppressed by suppressing the torque current ripple. At this time, even if the torque current is constant, the exciting current, that is, the d-axis current is not constant. However, when the torque current is constant, the exciting current ripple is small, and the variation of the magnitude of the current vector is relatively small. Therefore, by controlling the magnitude of the current vector on the dq-axis coordinate system to be constant, torque current, that is, torque pulsation can be suppressed.

FIG. 20 is a configuration diagram of a power converter according to a tenth embodiment of the present invention. This embodiment is different from the first embodiment only in that the calculation unit of the correction amount Δθv to the output voltage phase angle on the dq axis rotation coordinate system is different.
Only this part will be described.

The DC link voltage Vdc detected by the voltage detector 8 is input to a fluctuation calculator 19, and a sine wave ΔVdc, which is the fluctuation, is calculated. This fluctuating sine wave is input to the sine wave gain phase compensator 23. The gain phase compensator 23 compensates the gain and phase of the input sine wave as shown in FIG. In this example, the gain is K
1. γ1 is compensated as the phase. The output of the sine wave gain phase compensator 23 is the compensation amount ΔVd for the d-axis output voltage. The correction amount ΔVd for the d-axis output voltage is calculated based on the d-axis voltage reference V
Addition of d ^* and the adder 104 results in a d-axis output voltage Vd. Similarly, the sine wave gain phase compensator 23 receives the fluctuation sine wave ΔVdc of the DC link voltage Vdc as input, calculates a correction amount ΔVq for the q-axis output voltage, and adds the q-axis voltage reference Vq ^* to the adder 105. Then, it becomes the q-axis output voltage Vq.

With the above configuration, the correction amount is superimposed on the d-axis output voltage and the q-axis output voltage in accordance with the fluctuation of the DC link voltage, so that the d-axis output voltage and the q-axis output voltage are independent of each other. Can be pulsated. In this case, d
The correction amount to the axis output voltage and the correction amount to the q-axis output voltage are sine waves having mutually independent amplitudes and phases. The above (16)
According to Equations (19), for a change in the DC link voltage,
It is shown that torque ripple can be suppressed by appropriately changing the dq-axis voltage. Therefore, by superimposing independent compensation signals on the d-axis output voltage and the q-axis output voltage, torque ripple can be suppressed.

FIG. 21 is a configuration diagram of a power converter showing an eleventh embodiment of the present invention. This embodiment is different from the first embodiment in the calculation of the d-axis current command value.
Only this part will be described.

In the vector controller 18, the secondary magnetic flux command value φ2d ^* is input, and the d-axis current command calculator 12
A shaft current command value id ^* is generated. The DC link voltage is detected by the voltage detector 8 and input to the fluctuation calculator 19. In the variation calculator 19, the sine wave ΔV
dc is calculated. This fluctuating sine wave ΔVdc is input to the sine wave gain phase compensator 23. Sine wave gain phase compensator
At 23, the gain and phase are compensated for the input sine wave ΔVdc as shown in FIG. In this example, the gain is K,
Γ is compensated as the phase. Sine wave gain phase compensator
The output of 23 is the correction amount ΔId ^* to the d-axis current command id ^* . The correction amount ΔId ^* is obtained by adding the d-axis current command Id ^* and the adder
The value is added at 106 and becomes an input to the d-axis voltage command calculator 14 and the q-axis voltage command calculator 15.

With the above configuration, it is possible to pulsate the d-axis current by superimposing the correction amount on the d-axis current command according to the fluctuation of the DC link voltage. As described above, when the DC link voltage fluctuates and the torque current ripple is suppressed, the exciting current does not become constant and pulsates at the same frequency as the DC link voltage. Therefore, the sine wave ΔVdc the variation of the DC link voltage, the gain and a sine wave ΔId which is compensated by the phase ^* superimposed on the d-axis current command, by pulsing the d-axis current deliberately, the ripple of the torque current It becomes possible to suppress. Since the secondary magnetic flux follows the d-axis current slowly and is kept almost constant, torque ripple suppression can be expected.

FIG. 22 is a configuration diagram of a power converter showing a twelfth embodiment of the present invention. This embodiment differs from the first embodiment in the dimension of the correction amount, and therefore only this portion will be described.

FIG. 22 shows that the q-axis current controller 30 generates a correction amount Δθv for the output voltage phase angle on the dq axes in the fifth embodiment shown in FIG. The correction amount Δωi to the output frequency is created. Then, the adder 107 adds the correction amount Δωi to the output ωi ^* of the adder 101 to generate an inverter angular frequency ωi.

With the above configuration, the frequency of the inverter is adjusted according to the fluctuation of the DC link voltage.
This corresponds to pulsating the rotation frequency of the dq-axis rotation coordinate system when considered as vector control. From the theoretical analysis described above, to suppress the torque ripple, dq
Manipulating the output voltage phase on the axis rotation coordinate system was essential. Here, the d-axis means a secondary magnetic flux axis. Therefore, in order to suppress the torque ripple, it can be paraphrased that it is essential to adjust the phase angle from the secondary magnetic flux axis to the output voltage axis. By pulsating the rotation frequency of the dq axis rotation coordinate system as in the present embodiment,
The d axis and the secondary magnetic flux axis do not coincide. Therefore, since the vector control is not in the ideal state, the characteristics may be degraded due to unnecessary interference. However, if the control speed of the vector control is slow and the control does not interfere with the pulsation of the rotation frequency of the dq-axis rotary coordinate system, the output voltage phase angle on the dq-axis coordinate system is constant. In this case, the rotation frequency of the dq-axis coordinate system pulsates, the output voltage phase angle on the dq-axis coordinate system is constant, and the rotation frequency of the secondary magnetic flux is constant as described above. Will pulsate. Therefore, torque ripple can be suppressed.

Although the present embodiment is based on the fifth embodiment, the output voltage phase angle on the dq-axis rotating coordinate system can also be based on the sixth to eleventh embodiments. By adjusting the inverter frequency instead of adjusting
A similar effect is obtained.

As described above, when the output voltage on the dq axis is manipulated and the q-axis current is controlled to be constant while the DC link voltage fluctuates, even if the d-axis current pulsates, the d-axis current is reduced. Since the secondary magnetic flux does not follow the pulsation, there is no pulsation in the secondary magnetic flux. Therefore, since the secondary magnetic flux and the q-axis current are constant, torque ripple can be suppressed.

Further, the following other effects can be obtained. (1) When the phase angle of the output voltage on the dq axis is controlled in a state where the DC link voltage fluctuates and the q axis current is controlled to be constant, even if the d axis current pulsates, the pulsation of the d axis current becomes 2
Since the secondary magnetic flux does not follow, there is no pulsation in the secondary magnetic flux. Therefore, since the secondary magnetic flux and the q-axis current are constant, torque ripple can be suppressed.

(2) With the DC link voltage fluctuating,
To reflect the fluctuation of the torque on the dq-axis output voltage, directly detect the torque, and adjust the output voltage or the phase angle of the output voltage so as to suppress the fluctuation, thus suppressing the fluctuation of the torque more effectively. Becomes possible.

(3) With the DC link voltage fluctuating,
If the fluctuation of the power consumed by the inverter is reflected on the dq-axis output voltage and the pulsation of the power is suppressed, the power consumed by the inverter is various losses and the mechanical output. Since the output is large and the mechanical output is a product of the speed and the torque, and the speed does not change at a high speed, it is possible to suppress the fluctuation of the torque.

(4) The pulsation of the current flowing from the DC capacitor into the inverter is strongly affected by the fluctuation of the power consumed by the inverter. It is possible to suppress the pulsation of the power consumed by the device. As described above, fluctuations in power consumed by the inverter greatly affect torque ripple. Therefore, torque ripple can be suppressed by suppressing pulsation of current flowing from the DC capacitor to the inverter.

(5) When suppressing torque ripple in a state where the DC link voltage fluctuates, it is essential to reduce the torque current ripple. In a state in which the torque current ripple is suppressed, even if the operation mode of the inverter is the one-pulse mode and the magnitude of the output voltage cannot be arbitrarily suppressed, the excitation current slightly pulsates,
The amount of pulsation decreases. For this reason, by suppressing the fluctuation of the current value on the d-q axis, it is possible to suppress the ripple of the q-axis current together with the d-axis current. Therefore, torque ripple can be suppressed.

(6) With the DC link voltage fluctuating,
By independently controlling the fluctuation of the d-axis voltage and the fluctuation of the q-axis voltage according to the DC link voltage, the ripple of the q-axis current can be suppressed. As described above, since the secondary magnetic flux is constant, torque ripple can be suppressed.

(7) Under the condition that the DC link voltage fluctuates and the output voltage of the inverter cannot be controlled freely and at high speed, it is impossible to control the dq-axis current value to a constant value. Is intentionally pulsated and the q-axis current is controlled to be constant, so that the secondary magnetic flux is constant as described above, so that torque ripple can be suppressed.

(8) With the DC link voltage fluctuating,
When the operating conditions change, if the torque ripple compensation method or compensation gain is changed,
It is possible to effectively suppress torque ripple.

(9) With the DC link voltage fluctuating,
When the torque command changes, the compensation method or compensation gain of the torque ripple is changed. It is possible to effectively suppress torque ripple regardless of the torque command.

(10) With the DC link voltage fluctuating,
When the parameters of the induction motor, which is the load, change,
By changing the compensation method or compensation gain of the torque ripple, it is possible to effectively suppress the torque ripple irrespective of the variation of the parameter of the induction motor.

(11) With the DC link voltage fluctuating,
By changing the torque ripple compensation method or the compensation gain between the powering operation and the regenerative operation, it is possible to effectively suppress the torque ripple irrespective of the powering operation and the regenerative operation.

(12) With the DC link voltage fluctuating,
When the phase angle of the output voltage vector on the dq-axis coordinate system changes and the compensation method or compensation gain of the torque ripple is changed, the effective method is independent of the phase angle of the output voltage vector on the dq-axis coordinate system. Therefore, it is possible to suppress torque ripple.

(13) With the DC link voltage fluctuating,
If the method of compensating for torque ripple or the compensation gain is changed when the output frequency of the inverter changes, torque ripple can be effectively suppressed regardless of the output frequency of the inverter.

(14) With the DC link voltage fluctuating,
If the torque ripple compensation method or compensation gain is changed when the rotation frequency of the motor changes, it is possible to effectively suppress the ripple regardless of the rotation frequency of the motor.

(15) With the DC link voltage fluctuating,
If the fluctuation method of the torque ripple or the compensation gain is changed when the fluctuation frequency of the power supply frequency or the DC link voltage changes, the torque ripple can be effectively suppressed regardless of the fluctuation frequency of the power supply frequency or the DC link voltage. It is possible.

(16) With the DC link voltage fluctuating,
When the power supply frequency changes to 50 Hz / 60 Hz, it is determined whether the power supply frequency is 50 Hz or 60 Hz, and when the frequency component of the pulsation to be detected is changed, the power supply frequency becomes 50H.
Even at z or 60 Hz, torque ripple can be effectively suppressed.

(17) With the DC link voltage fluctuating,
When the power supply frequency fluctuates, if the frequency component of the pulsation to be detected is changed according to the power supply frequency, it is possible to effectively suppress the torque ripple even when the power supply frequency fluctuates.

(18) With the DC link voltage fluctuating,
Even when the PWM operation mode is the one-pulse mode, the torque ripple can be suppressed by adjusting the phase angle of the dq-axis output voltage, changing the dq-axis voltage, and controlling the q-axis current to be constant.

(19) With the DC link voltage fluctuating,
When suppressing torque ripple by vector control, torque ripple can be suppressed by adjusting the output frequency of the inverter.

(20) The cause of torque ripple is that the magnitude of the output voltage of the inverter cannot be controlled freely and at high speed, and this may be possible depending on the operation mode of PWM. By not performing torque ripple suppression, unnecessary interference can be suppressed, and deterioration of torque characteristics can be prevented.

[0112]

As described above, according to the present invention, for example, when the power supply is a single-phase power supply, it is possible to suppress the torque ripple when the inverter output frequency is close to twice the frequency of the power supply. As a result, noise can be reduced, and the failure rate of the mechanical and electrical systems can be reduced. In addition, when applied to a train, an effect of improving riding comfort can be obtained.

Further, according to the present invention, since the compensation is performed successively based on the theoretically obtained compensation amount, the torque ripple can be suppressed even in any operating condition or a controlled object having different parameter values. And labor can be greatly reduced.

[Brief description of the drawings]

FIG. 1 is a configuration diagram of a power conversion device according to a first embodiment of the present invention.

FIG. 2 is a relationship diagram between a dq-axis output voltage phase angle and an output voltage vector.

FIG. 3 is a configuration diagram of a compensation amount calculator.

FIG. 4 is a relationship diagram between a compensation gain and a compensation phase.

5A is a diagram showing a generated torque of a motor on a dq axis rotation coordinate system, FIG. 5B is a vector diagram when there is no change in DC link voltage, and FIG. 5C is a diagram showing a change in DC link voltage It is a vector diagram in the case where there is.

FIG. 6 is a vector diagram in a case where a DC link voltage fluctuates on a dq-axis rotating coordinate system and torque ripple is suppressed.

FIG. 7 is a trajectory diagram of a fluctuation amount of a dq-axis output voltage when there is a torque ripple.

FIG. 8 is a trajectory diagram of the fluctuation amount of the dq-axis output voltage when there is no torque ripple.

FIG. 9 is a simulation result when beatless control is not performed.

FIG. 10 is a simulation result when a beatless control method according to a conventional method is applied.

FIG. 11 is a simulation result in the case of performing compensation shown in Expressions (17) to (20).

FIG. 12 is a configuration diagram illustrating a second embodiment of the present invention.

FIG. 13 is a configuration diagram illustrating a third embodiment of the present invention.

FIG. 14 is a configuration diagram illustrating a fourth embodiment of the present invention.

FIG. 15 is a configuration diagram illustrating a fifth embodiment of the present invention.

FIG. 16 is a configuration diagram illustrating a sixth embodiment of the present invention.

FIG. 17 is a configuration diagram illustrating a seventh embodiment of the present invention.

FIG. 18 is a configuration diagram illustrating an eighth embodiment of the present invention.

FIG. 19 is a configuration diagram illustrating a ninth embodiment of the present invention.

FIG. 20 is a configuration diagram illustrating a tenth embodiment of the present invention.

FIG. 21 is a configuration diagram illustrating an eleventh embodiment of the present invention.

FIG. 22 is a configuration diagram illustrating a twelfth embodiment of the present invention.

[Explanation of symbols]

 DESCRIPTION OF SYMBOLS 1 ... Power supply 2 ... Single phase converter 3 ... DC capacitor 4 ... Inverter 5 ... Current detector 6 ... Induction motor 7 ... Speed detector 8 ... Voltage detector 9 ... Magnetic flux command corrector 10 ... Slip angle frequency calculator 11 ... Integration Unit 12 ... d-axis current command calculator 13 ... q-axis current command calculator 14 ... d-axis voltage command calculator 15 ... q-axis voltage command calculator 16 ... coordinate system converter 17 ... gate controller 18 ... vector controller 19 … Fluctuation amount calculator 20… compensation amount calculator 21… compensation gain calculator 22… compensation phase calculator 23… sine wave gain phase adjuster 24… 100 Hz bandpass filter 25… 120 Hz bandpass filter 26… power supply frequency detector 27 ... Changeover switch 28 ... Multiplier 29 ... Band pass filter 30 ... Coordinate system converter 31 ... q-axis current suppressor 32 ... Torque detector 33 ... Torque pulsation detector 34 ... Torque pulsation suppressor 35 ... Detector 36 ... Power calculation Table 37 ... Power fluctuation performance Calculator 38 Power fluctuation controller 39 Current pulsation calculator 40 Current pulsation suppressor 41 Current vector length calculator 42 Current pulsation calculator 43 Current pulsation suppressors 101 to 107 Adders

Claims (11)

[Claims] 1. A converter that converts an alternating current into a direct current and outputs the same, an inverter that converts the direct current output by the converter into an alternating current of an arbitrary frequency and outputs the same, and an induction motor driven by the alternating current output by the inverter. In accordance with a change in the DC output from the converter, the torque component current is kept constant while the magnetic flux component current is pulsating on a rotating coordinate system including a magnetic flux axis and a torque axis orthogonal to the magnetic flux axis. And a vector control means for adjusting an AC voltage vector output from the inverter. 2. A converter that converts an alternating current into a direct current and outputs the same, an inverter that converts the direct current output by the converter into an alternating current of an arbitrary frequency and outputs the same, and an induction motor driven by the alternating current output by the inverter. In accordance with a change in the DC output from the converter, the torque component current is kept constant while the magnetic flux component current is pulsating on a rotating coordinate system including a magnetic flux axis and a torque axis orthogonal to the magnetic flux axis. And a vector control means for adjusting a phase angle from the magnetic flux axis to an AC voltage vector output from the inverter. 3. The power converter according to claim 2, wherein the vector control means adjusts a phase angle from the magnetic flux axis to an AC voltage vector output by the inverter, instead of adjusting an output frequency of the inverter. A power converter characterized by adjusting the following. 4. The power conversion device according to claim 1, wherein the vector control means controls the torque while keeping the magnetic flux component current pulsating in response to a change in the DC output from the converter. A power converter, wherein the torque of the induction motor is controlled to be constant, instead of controlling the component current to be constant. 5. The power conversion device according to claim 1, wherein the vector control unit controls the torque while keeping the magnetic flux component current pulsating in accordance with a change in the DC output from the converter. A power converter, wherein the power consumption of the inverter is controlled to be constant, instead of controlling the component current to be constant. 6. The power conversion device according to claim 1, wherein the vector control unit controls the torque while keeping the magnetic flux component current pulsating in response to a change in the DC output from the converter. A power converter, wherein the current flowing into the inverter is controlled to be constant, instead of controlling the component current to be constant. 7. The power conversion device according to claim 1, wherein the vector control means controls the torque while keeping the magnetic flux component current pulsating in response to a change in the DC output from the converter. Instead of controlling the component current to be constant, control is performed so that the magnitude of the output current of the inverter on the rotating coordinate system is constant. 8. A converter that converts an alternating current into a direct current and outputs the same, an inverter that converts the direct current output by the converter into an alternating current of an arbitrary frequency and outputs the same, and an induction motor driven by the alternating current output by the inverter. And a magnetic flux component voltage and a torque component voltage such that a torque component current is constant on a rotating coordinate system including a magnetic flux axis and a torque axis orthogonal to the magnetic flux axis in accordance with a change in DC output from the converter. And a vector control unit that adjusts the power. 9. A converter for converting an alternating current to a direct current and outputting the same, an inverter for converting the direct current output from the converter to an alternating current having an arbitrary frequency and outputting the same, and an induction motor driven by the alternating current output from the inverter. And adjusting the magnetic flux component current so that the magnetic flux component current pulsates on a rotating coordinate system including a magnetic flux axis and a torque axis orthogonal to the magnetic flux axis in accordance with the fluctuation of the DC output from the converter. A power converter having vector control means. 10. The power converter according to claim 1, wherein the adjustment by the vector control unit is performed in a control mode in which the number of pulses included in a half cycle of the output voltage of the inverter is one. A power conversion device characterized by performing the above. 11. The power conversion device according to claim 1, wherein the adjustment by the vector control unit is not performed according to the number of pulses included in a half cycle of the output voltage of the inverter. A power converter characterized by the above-mentioned.