JP5492180B2 - Variable magnetic flux drive system - Google Patents

Description

  The present invention relates to a variable magnetic flux drive system including an inverter that drives a variable magnetic flux motor having a fixed magnet and a variable magnet.

  In recent years, permanent magnet synchronous motors (PM), which are excellent in efficiency and can be expected to be reduced in size and noise, have begun to spread in place of the conventional induction motor IM. For example, permanent magnet synchronous motors are applied as drive motors for railway vehicles and electric vehicles.

  The permanent magnet synchronous motor is a motor that includes a permanent magnet in a rotor and outputs torque using the magnetic flux. Since the induction motor IM generates the magnetic flux itself by the excitation current from the stator, it is disadvantageous to generate a loss due to the excitation current flowing.

  The permanent magnet synchronous motor generates an induced voltage corresponding to the rotational speed because of the permanent magnet. In application fields with a wide rotation range such as railway vehicles and automobiles, it is a condition that the inverter that drives and controls the permanent magnet synchronous motor is not destroyed by an overvoltage due to the induced voltage generated at the maximum rotation speed. That is, the withstand voltage of the inverter is made sufficiently high, or conversely, the magnetic flux of the permanent magnet provided in the motor is limited. The former often affects the power supply, and the latter is often selected.

  If the amount of magnetic flux in that case is compared with the induction motor IM (in the case of IM, the amount of gap magnetic flux created by the exciting current), there are cases where the amount is about 1: 3. In this case, in order to generate the same torque, it is necessary to flow a large (torque) current in a permanent magnet synchronous motor with a small amount of magnetic flux. That is, when the current that outputs the same torque is compared between the induction motor IM and the permanent magnet synchronous motor in the low speed range, the permanent magnet synchronous motor needs to pass a larger current.

  For this reason, the current capacity of the inverter that drives the permanent magnet synchronous motor increases. Furthermore, generally, at low speed, the switching frequency of the switching element in the inverter is high, and the generated loss increases depending on the current value, resulting in large loss and heat generation. A train or the like may be expected to be cooled by running wind, and a large loss at low speeds increases the size of the inverter device because of the need to improve the cooling capacity. Conversely, when the induced voltage is high, field-weakening control is performed. In this case, the efficiency is reduced by superimposing the excitation current.

  Thus, the permanent magnet synchronous motor has advantages and disadvantages due to the inherent magnet. As a motor, the benefits are significant, leading to loss reduction and miniaturization. On the other hand, in the case of variable speed control such as trains and electric cars, operation is less efficient than the conventional induction motor IM. There are also points. In addition, the current capacity of the inverter increases and the loss also increases, so the inverter becomes larger. Since the efficiency of the system itself is dominant on the motor side, the overall efficiency is improved by the application of the permanent magnet synchronous motor. On the other hand, the inverter becomes large, which is not preferable because it is a disadvantage of the system.

  On the other hand, there is a variable magnetic flux motor that can change the magnet magnetic flux by the current from the inverter. Since the amount of magnetic flux of the permanent magnet can be made variable according to the operating conditions, an improvement in efficiency can be expected as compared with a conventional permanent magnet synchronous motor with a fixed magnet. Moreover, when a magnet is unnecessary, it is also possible to suppress an induced voltage as much as possible by reducing the amount of magnetic flux.

Here, when the magnetic flux control is performed by weakening the permanent magnet motor PM, the magnetic flux current is reduced without impairing the torque accuracy, and the inverter and motor loss and the current rating value of the device are reduced (for example, Patent Document 1).
Japanese Patent Laid-Open No. 11-299297

  However, in a variable magnetic flux drive system that drives a variable magnetic flux motor capable of variably controlling the amount of magnet by the magnetizing current from the inverter, it is important how and at what timing the magnetization process for changing the magnetic flux is performed. . The generation of transient torque associated with torque accuracy and magnetization processing, and the timing of magnetization processing to cope with the highest efficiency and a wide speed range are required.

  An object of the present invention is to reduce torque accuracy deterioration due to being a variable magnet, to suppress transient torque accompanying magnetization processing, and further to improve the efficiency of the entire system and to cope with a wide speed range. Is to provide.

A variable magnetic flux drive system according to the present invention includes a variable magnetic flux drive system including an inverter that drives a variable magnetic flux motor having a fixed magnet and a variable magnet, and a torque command generator that generates a torque command of the variable magnetic flux motor; A variable magnetic flux control unit that magnetizes the variable magnet by changing a magnetic flux with a magnetizing current from the inverter, a DQ axis current reference based on a torque command from the torque command generation unit, and a DQ axis from the variable magnetic flux control unit Based on a switch that switches between magnetizing current commands, a magnetization request generator that generates a request to magnetize the variable magnet when a predetermined condition is established for the variable magnetic flux controller, and a torque command from the switch A gate command for controlling the inverter is generated based on a DQ axis current reference or a DQ axis magnetizing current command. And a preparative command generating unit, the magnetization request generation unit, the current increase due to field weakening control of the variable magnet, and wherein the emit the magnetization request before the flux of the variable magnet is changed.

  According to the present invention, it is possible to suppress the deterioration of torque accuracy due to the variable magnet and to suppress the transient torque associated with the magnetization process, further improve the efficiency of the entire system and cope with a wide speed range.

(First embodiment)
FIG. 1 is a block diagram of a variable magnetic flux drive system according to the first embodiment of the present invention. First, the main circuit including the variable magnetic flux motor 4 of the drive system will be described. The inverter 1 converts DC power from a DC power source into AC power and supplies it to the variable magnetic flux motor 4. The currents Iu and Iw supplied to the variable magnetic flux motor 4 are detected by the current detector 2, converted into the D-axis current Id and the Q-axis current Iq by the coordinate conversion unit 7, and input to the voltage command calculation unit 10. The D-axis voltage command Vd * and the Q-axis voltage command Vq * from the voltage command calculation unit 10 are input to the coordinate converter 5 and converted into three-phase voltage commands Vu *, Vv *, and Vw * to the PWM circuit 6. Entered. The PWM circuit 6 performs on / off control of the switching element of the inverter 1 according to the gate command Gst from the gate command generator 15. On the other hand, the rotation angle of the variable magnetic flux motor 4 is detected by the rotation angle sensor 18 and is differentiated by the pseudo-differentiator 8 to obtain the inverter frequency ω 1 and input to the voltage command calculation unit 10 and the magnetic flux command calculation unit 12.

  Here, the variable magnetic flux motor 4 according to the first embodiment of the present invention will be described. FIG. 2 is a simplified model diagram of the variable magnetic flux motor 4 according to the first embodiment of the present invention. The stator side of the variable magnetic flux motor 4 is the same as that of an existing permanent magnet synchronous motor. As the magnet on the rotor side, a fixed magnet 54 having a fixed magnetic flux density and a variable magnet 53 having a variable magnetic flux density. have. In the case of a permanent magnet synchronous motor, only the former fixed magnet is used, and the characteristic of the variable magnetic flux motor is that a variable magnet is provided. Now, assuming that the magnetization direction of the magnet is the D axis, the fixed magnet 54 and the variable magnet 53 are arranged in the D axis direction. In FIG. 2, Ld is a D-axis inductance, and Lq is a Q-axis inductance.

  Next, the fixed magnet 54 and the variable magnet 53 will be described. A fixed magnet (permanent magnet) is a magnet that maintains a magnetized state in a state where no current flows from the outside. Even if it is a fixed magnet, its magnetic flux density does not change strictly under any conditions. Even a permanent magnet synchronous motor is demagnetized by passing an excessive current through the inverter 1 or the like, or is magnetized conversely. That is, it can be considered that the fixed magnet does not change in the amount of magnetic flux but indicates that the magnetic flux density does not substantially change due to the current in a state close to normal rated operation.

  On the other hand, the variable magnet 53 may be considered to indicate a magnet whose magnetic flux density changes depending on the current that can flow through the inverter 1 even under normal rated operating conditions. Such a variable magnet 53 can be designed within a certain range depending on the material and structure of the magnetic material.

  For example, as a fixed magnet (permanent magnet) of a recent permanent magnet synchronous motor, a neodymium (NdFeB) magnet having a high residual magnetic flux density Br is often used. Since the residual magnetic flux density Br (about 1.2 T) is high, it is possible to output a large torque with a small physique, and it is suitable for HEVs and trains that require a high-power and downsized motor. In the case of a conventional permanent magnet synchronous motor, since it is a requirement that it is not demagnetized by a normal current, the neodymium magnet (NdFeB) has a very high coercive force Hc (about 1000 kA / m) (residual magnetic flux density) Therefore, a magnet having a large coercive force is selected for a permanent magnet synchronous motor).

  Here, it can be considered that the variable magnet 53 is a magnetic body such as Alnico AlNiCo (Hc 60 to 120 kA / m) or FeCrCo magnet (Hc about 60 kA / m) having a high residual magnetic flux density and a small coercive force Hc. The magnetic flux density (flux amount) of the neodymium NdFeB magnet is almost constant by the normal amount of current (meaning the amount of current that flows when the conventional permanent magnet synchronous motor is driven by the inverter 1). The magnetic flux density (magnetic flux amount) of the variable magnet can be varied. Strictly speaking, since neodymium is used in the reversible region, the magnetic flux density fluctuates in a very small range, but when the inverter current disappears, it returns to the original value. On the other hand, since the variable magnet 53 is used up to the irreversible region, even if there is no inverter current, the magnet does not change to the initial value and is in a variable state. In FIG. 2, the magnetic flux amount of Alnico, which is the variable magnet 53, may also be considered to be zero in the Q-axis direction (although it is not strictly zero for convenience of design) only by the amount in the D-axis direction changing.

  FIG. 3 is a configuration diagram of the rotor 51 of the variable magnetic flux motor 4. A fixed magnet 54 with high coercive force such as neodymium NdFeB and a variable magnet 53 with low coercive force such as Alnico AlNiCo are combined and arranged in the rotor core 52. The variable magnet 53 is magnetized by the D-axis current without being affected by the Q-axis current because the Q-axis direction and the magnetization direction thereof are orthogonal to each other.

  FIG. 4 is a characteristic diagram of BH characteristics (magnetic flux density-magnetization characteristics) of the fixed magnet 54 and the variable magnet 53. 4, S54 is the BH characteristic of the fixed magnet 54, S53 is the BH characteristic of the variable magnet 53, Br1 is the residual magnetic flux density of the variable magnet 53, and Br2 is the residual magnetic flux density of the fixed magnet 53. H1sat is the saturation value of the variable magnet 53, Hc1 is the holding force of the variable magnet 53, and Hc2 is the holding force of the fixed magnet 53. Further, X is a magnetization region due to the output current of the inverter.

  FIG. 5 is a characteristic diagram showing only the second quadrant (B> 0, H <0) of FIG. 4 in a quantitatively correct relationship. In the case of neodymium NdFeB and Alnico AlNiCo, there is no significant difference in residual magnetic flux density Br1 and Br2, but for coercive force Hc1 and Hc2, 1/115 to 1/8 for Alnico AlNiCo magnet and FeCrCo magnet for neodymium NdFeB magnet It becomes 1/15 at. In the conventional permanent magnet synchronous motor, the magnetization region X due to the output current of the inverter 1 is sufficiently smaller than the coercive force of the neodymium NdFeB magnet and is used in the reversible range of its magnetization characteristics. Since the variable magnet 53 has a small coercive force as described above, it can be used in an irreversible region (even if the current is zero, it does not return to the magnetic flux density B before the current application) in the range of the output current of the inverter 1. The magnetic flux density (magnetic flux amount) can be made variable.

An equivalent simple model of the dynamic characteristics of the variable magnetic flux motor 4 is shown in equation (1). This model is a model on the DQ axis rotation coordinate system in which the D axis is given as the magnet magnetic flux direction and the Q axis is perpendicular to the D axis.

  Where R1: winding resistance, Ld: D-axis inductance, Lq: Q-axis inductance, ΦFIX: fixed magnet (linkage) flux, ΦVAR: variable magnet (linkage) flux, ω1: inverter frequency is there.

  Next, the control block of the variable magnetic flux drive system of the variable magnetic flux motor 4 will be described with reference to FIG. The operation command Run * and the protection signal PROT determined by the protection determination unit 17 are input to the operation command generation unit 16 of the variable magnetic flux drive system. The operation command generation unit 16 generates and outputs an operation state flag Run based on the operation command Run * and the protection signal PROT determined by the protection determination unit 17.

  Basically, when the operation command Run * is entered (Run * = 1), the operation state flag Run is set to the operation state (Run = 1), and when the operation command instructs to stop (Run * = 0) The operation state flag Run is set to the stop state (Run = 0). This is when the protection determination unit 17 determines that the protection is normal rather than protection (PROT = 0), and when the protection determination unit 17 detects protection (PROT = 1), the operation command Run * is “1”. Even so, the operation state is stopped (Run = 0).

  In addition, the operation command generation unit 16 generates a torque permission flag TrqON that permits torque application (TrqON = 1 applies torque, TrqON = 0 does not apply torque). When the operation command Run * is changed from “0” to “1”, the magnetization process is first performed. During this time, the magnetization completion flag FCCmp is “1” during the magnetization process. The torque permission flag TrqON becomes “1” for the first time after this magnetization is completed, that is, when the magnetization completion flag FCCmp is changed from “1” to “0” (the torque is raised after the magnetization is completed). .

  Conversely, when the operation command Run * is “1” to “0”, that is, when operation stop is instructed, first, the torque permission flag TrqON = 0 is set, the torque command Tm * is reduced to zero, and then the operation state Set the flag Run to the stopped state (Run = 0). This relationship will be described later.

  The torque command generator 38 generates a torque command Tm * with a target value of zero when the torque permission flag TrqON = 0, and generates a torque command Tm * such that a desired torque is obtained when TrqON = 1. To do. Regarding the transient state, the rate of change of the torque command may be limited, or it may be made to respond in the primary system, depending on the application. In some cases, it may be changed stepwise.

  The gate command generation unit 15 inputs an operation state flag Run, and generates and outputs a gate command Gst to a switching element included in the inverter 1. When the operation state flag Run changes from stop (= 0) to operation (= 1), the gate command generation unit 15 immediately sets the gate start (Gst = 1) and the operation state flag Run from the operation (= 1). In the case of changing to stop (= 0), the gate is turned off (Gst = 0) after a predetermined time has elapsed. The reason why the gate is turned off after the lapse of the predetermined time is that, as will be described later, the variable magnet 53 is magnetized to a predetermined value to be free run.

  In the magnetic flux command calculation unit 12, since the operation state flag Run and the inverter frequency ω 1, that is, the rotor rotation frequency ω R (in the first embodiment, the control is performed with the rotation angle sensor (resolver) 18, the rotation sensor 18 The rotor rotation frequency obtained by differentiating the angle detected by the pseudo-differentiator 8 is used as an inverter output frequency), and the magnetic flux command Φ * is generated and output as in the following equation, for example.

If (Run == 0)
Φ * = Φmin
Else if (| ω1 | <ωA)
Φ * = Φmax
Else
Φ * = Φmin (2)
Here, Φmin: the minimum amount of magnetic flux that can be taken as a variable magnetic flux motor (> 0), Φmax: the maximum amount of magnetic flux that can be taken as a variable magnetic flux motor, ωA: a predetermined rotational frequency.

  That is, when the operation state flag Run is stopped (Run = 0), the magnetic flux command Φ * is set to the minimum Φmin, and when the operation state (Run = 1) and the rotation frequency ωR is lower than the predetermined value, the magnetic flux The command Φ * is set to the maximum Φmax, and when the speed is higher than a predetermined value, the magnetic flux command Φ * is set to the minimum Φmin. The setting of Φmin and Φmax of the magnetic flux amount will be described later.

  The current reference calculation unit 11 receives the torque command Tm * and the magnetic flux command Φ * as inputs, and calculates the D-axis current reference IdR and the Q-axis current reference IqR as follows.

IdR = 0 (3)
IqR = Tm * / Φ * (4)
Here, the expressions (3) and (4) are arithmetic expressions (the number of motor pole pairs = 1) assuming that the reluctance torque of the variable magnetic flux motor 4 is not used. It may be a salient pole type motor having a difference ΔL between the D axis inductance Ld and the Q axis inductance Lq, or a non-salient pole type motor having no difference.

  However, it is effective to consider the reluctance torque when optimizing the efficiency and considering the maximum output at a predetermined current. In this case, for example, it can be calculated as in the following equation.

IqR = (− Φ * + √ (Φ * 2−4 × (Ld−Lq) × K × Tm *) / {2 × (Ld−Lq) × K} (5)
IdR = K × IqR (6)
Here, K is the ratio of the D-axis current and the Q-axis current, and is a value that varies depending on the application such as the above-described efficiency optimization and maximum output. It is a function for optimization, and its arguments vary such as torque and speed. In general, simple approximations or tables are used.

  The magnetization request generation unit 29 sets the magnetization request flag FCreq to “1” when the magnetic flux command Φ * changes or the operation state flag Run changes, and to “0” otherwise. FIG. 6 is a block diagram of the magnetization request generator 29.

  The previous value of the magnetic flux command Φ * is held by the previous value holding unit 31. The output of the previous value holding unit 31 is the previously stored magnetic flux command Φ *, and is input to the change determination unit 30 together with the current magnetic flux command value Φ *. The change determination unit 30 compares the two inputs and outputs “1” when there is a change in the magnetic flux command value Φ *, and outputs “0” when there is no change. That is, it is set to “1” only when the magnetic flux command Φ * changes. A circuit similar to this is also provided for the operation state flag Run instead of the magnetic flux command Φ *, and the outputs of the two change determination units 30 and 34 are input to the OR circuit 32, and the OR is the magnetization request flag FCreq. Is output as

  That is, the magnetization request flag FCreq is “1” (magnetization request is present) when the magnetic flux command Φ * is changed or the operation state flag Run is changed, and is “0” (no magnetization request) otherwise. . Note that the state in which the operation state flag Run changes may be when the inverter starts, stops, or stops due to protection.

  Next, the variable magnetic flux controller 13 changes the magnetic flux by the magnetization current from the inverter 1 to magnetize the variable magnet. FIG. 7 is a block diagram of the variable magnetic flux control unit 13. The variable magnetic flux control unit 13 inputs the magnetic flux command Φ * that is the output of the magnetic flux command calculation unit 12, and calculates and outputs the D-axis magnetization current command Idm * and the Q-axis magnetization current command Iqm *. The concept of generation is as follows.

  In order to magnetize the variable magnet, a predetermined magnetizing current command Im * may be obtained in accordance with the BH characteristics of the variable magnet shown in FIG. In particular, the magnitude of the magnetization current command Im * is set to be equal to or greater than H1sat in FIG.

  Therefore, since the magnetization current flows to the saturation region of the magnetic substance, the magnetic flux amount Φmin and Φmax to be set by the magnetic flux command calculation unit 12 is a maximum (saturation) value that is positive or negative in the magnetic flux (magnetic flux density) of the variable magnet. And a value obtained by adding a fixed magnet component. That is, if the positive maximum value of the variable magnetic flux amount is ΦVARmax (assuming that the absolute value of the negative maximum value is equal to the positive maximum value) and the magnetic flux amount of the fixed magnet is ΦFIX, it can.

Φmin = ΦFIX −ΦVARmax (7)
Φmax = ΦFIX + ΦVARmax (8)
The magnetizing current command Im * for obtaining the flux command Φ * is output from the magnetizing current table 27 in which the magnetic flux command Φ * is input and the corresponding magnetizing current is stored. Basically, since the magnetization direction of the magnet is the D axis (the D axis is defined as such), the magnetization current command Im * may be given to the magnetization current command Idm * to the D axis. .

  However, the permanent magnet synchronous motor has a considerable difference between the D-axis inductance Ld and the Q-axis inductance Lq, and reluctance torque is generated (torque is generated by flowing the D-axis current). This is particularly remarkable in the case of a PRM motor (permanent magnet reluctance motor) that realizes a wide speed range. For magnetization, a current value equal to or higher than the rated current is required, so that it is assumed that a large reluctance torque is instantaneously generated during the magnetization process. Ideally, even in a motor without saliency, it is naturally assumed that partial magnetic saturation occurs when the above-described excessive magnetization current flows. Thus, by passing a magnetizing current for magnetizing, a transient torque shock occurs, which induces mechanical vibrations and adversely affects riding comfort in the case of an automobile or train, which is not preferable.

  In order to avoid this, not only the D-axis magnetizing current but also the Q-axis magnetizing current (which does not affect the magnetization but contribute to torque reduction) can be used to suppress instantaneous reluctance torque generation. It is. Generally, the permanent magnet synchronous motor torque is expressed by the following equation.

Tm = Φ × Iq + (Ld−Lq) × Id × Iq (9)
Here, when the D-axis magnetization current Idm is passed, a condition that does not generate torque can be obtained by the following equation.

Iq = Tm / (Φ + (Ld−Lq) × Id) (10)
Therefore, if the magnetizing current command is replaced, the following equation is obtained.

Iqm * = Tm / (Φ * + (Ld-Lq) × Idm *) (11)
Here, there is a problem whether the magnetic flux command Φ * should be set before the magnetic flux change, should be set after the magnetic flux change, or should be set in the middle. The magnetization of the variable magnetic flux is complicated and cannot be generally limited. Rather, it is necessary to adjust according to the actual machine, and the magnetic flux command of equation (11) is tabulated based on the actual machine measurement, or the D axis magnetization current command Idm * and the Q axis magnetization current command Iqm * are torque discontinuous. It can be realized by having a function or table obtained by actual machine verification so that the

  In FIG. 7, the Q-axis magnetization current command calculation unit 36 generates and outputs a Q-axis magnetization current command with the magnetization current command Im * (that is, the D-axis magnetization current command Idm *) as an input. The switch 26 outputs a value as the Q-axis magnetization current command Iqm * only during the magnetization completion flag FCCmp = 1 (that is, during the magnetization process), and during the magnetization completion flag FCCmp = 0 (that is, the magnetization process is completed). Gives zero. The Q-axis magnetizing current command calculation unit 36 may have the above formula (11) or a table or function that gives an actually measured Q-axis current command for reducing transient torque based on the actual machine as described above.

  On the other hand, in FIG. 7, the magnetization request flag FCreq is in a switching request state (= 1) at least for a moment when a request to switch the magnetic flux is made. In order to reliably change the magnetic flux, the magnetization request flag FCreq is input to the minimum on-pulse device 28. The magnetization completion flag FCCmp (= 1: during magnetization, = 0: magnetization completion), which is an output, has a function of not being turned off (= 0) for a predetermined time once turned on (= 1). Have. If the magnetization request flag remains on (= 1) for a predetermined time, the magnetization request flag Fcreq is turned off and the magnetization completion flag FCCmp is turned off immediately. Thus, by continuing the magnetization process for a predetermined time, it is possible to perform reliable magnetization.

  When the magnetization completion flag FCCmp is input to the switch 37 of FIG. 1 and magnetization is being performed (magnetization completion flag FCCmp = 1), the magnetization current commands Idm * and Iqm * of the DQ axis that are the outputs of the variable magnetic flux control unit 13 When the magnetization is completed (magnetization completion flag FCCmp = 0), the DQ axis current references IdR and IqR, which are the outputs of the current reference calculation unit 11, are output as DQ axis current commands Id * and Iq *.

  Based on the DQ-axis current commands Id * and Iq * generated as described above, the voltage command calculation unit 10 generates DQ-axis voltage commands Vd * and Vq * so that a current flows so as to match the commands. The coordinate conversion unit 5 converts the signals into three-phase voltage commands Vu *, Vv *, and Vw *, and generates a gate signal through the PWM circuit 6.

  FIG. 8 is a timing chart showing an example of the operation of the variable magnetic flux drive system according to the first embodiment. FIG. 8 shows a situation where the protection signal PROT is not established. When the operation command Rum * is input at time t1, the operation state flag Run rises, and the magnetic flux command Φ * also changes from Φ0 to Φmax. Due to the change in the operation state flag Run and the change in the magnetic flux command Φ *, the magnetization request flag FCreq is turned on, and the magnetization completion flag FCCmp that has been kept on for a predetermined time (between time t1 and time t2) is raised. The D-axis magnetization current command Idm * has a value only during the period of FCCmp = 1 where the magnetization completion flag FCcmp indicates that magnetization is in progress.

  The torque permission flag TrqON becomes “1” at the time t2 when the magnetization completion flag FCcmp changes from “1” to “0”, and the torque command Tm * rises from the time t2. That is, the torque command Tm * does not rise until magnetization is completed immediately after activation (until the magnetization completion flag FCCmp = 0). In this case, the torque command Tm * rises between time t2 and time t3.

  Then, when the magnetic flux command Φ * changes from Φmax to Φmin at time t4, the magnetization request flag FCreq is set, and the magnetization completion flag FCCmp that secures the ON state for a predetermined time (between time t4 and time t5) is set. The D-axis magnetization current command Idm * and the Q-axis magnetization current command I1qm * have values only during the period of FCCmp = 1 in which the magnetization completion flag FCcmp indicates that magnetization is in progress.

  Next, when the operation command Run * is not input at time t6, the torque permission flag TrqON is changed from “1” to “0”, and the torque command Tm * falls between time t6 and time t7. At time t7 when the torque command Tm * becomes zero, the operation state flag Run changes from “1” to “0”, and the magnetic flux command Φ * changes from Φ0 to Φmax. In addition, the magnetization request flag FCreq is set, and the magnetization completion flag FCCmp that has been kept on for a predetermined time (between time 7 and time t8) is set. The D-axis magnetization current command Idm * has a value only during the period of FCCmp = 1 where the magnetization completion flag FCcmp indicates that magnetization is in progress.

  Therefore, from the equation (11), in the magnetization process A (time t1 to time t2) and the magnetization process C (time t7 to time t8), the Q-axis magnetization current command = 0, and the magnetization process B (time t4 to time t4). Only at time t5), the Q-axis magnetizing current command has a value.

  Here, in the variable magnetic flux motor 4, an excessive current flows in the magnetization, so that a transient torque is generated not a little. There is a possibility of inducing mechanical vibration due to this torque shock, and there is a demand for reducing an excessive current in terms of loss and element stress as much as possible. Therefore, in the first embodiment, since the magnetization process is performed under a specific condition, it is possible to suppress the generation of torque shock and loss and the stress of the switching elements constituting the inverter 1 to the minimum necessary. It becomes possible.

  Further, since the magnetization process is performed immediately after starting the inverter 1, the magnetization state of the variable magnet 53 can be determined before starting to apply torque. For example, immediately after the power is turned on, the magnetization state of the variable magnetic flux motor 4 is unknown, and in the free-run state, the magnetization state does not always change due to some factor. For example, when the DC voltage of the inverter 1 decreases and the induced voltage generated by the total magnetic flux exceeds this, current flows from the variable magnet motor 4 to the inverter 1 even when the inverter 1 is stopped. It is also assumed that the magnetization state changes due to the factor. In order to minimize the induced voltage during free run, the amount of magnetic flux that is not used during normal operation may be set before the inverter 1 is stopped. In this case, when starting the inverter 1, it is essential to magnetize to the amount of magnetic flux required for operation.

  That is, since the magnetization state (magnetic flux amount) before starting of the inverter 1 is unclear, in the first embodiment, this is determined and the operation is started. As a result, in the operating state, the total magnet amount is too small and the torque is insufficient, and the actual magnetic flux is not set to a value different from the magnetic flux assumed by the controller, so that the torque accuracy can be reliably ensured.

  In the first embodiment, the torque command is started in a state where the magnetization is completed immediately after the inverter is started. As described above, flowing the Q-axis magnetizing current together with the D-axis magnetizing current has an effect of reducing the transient torque. However, in order to strictly suppress the generation of the transient torque, how many Q-axis magnetizing currents should be passed. It is not possible to determine exactly what is good. On the other hand, only when the torque command Tm * is zero, that is, when the Q-axis magnetization current Iq = 0, the reluctance torque that is the cause of the torque shock is not generated, so that the startup can be performed smoothly. That is, immediately after the start of the inverter 1 and after the magnetization is completed, the torque command is started, so that a smooth start without a torque shock can be performed.

  Further, in the first embodiment, after the operation command is stopped, that is, after it is no longer necessary to apply torque, the magnetization process is performed, and when the magnetization is completed, the gate of the inverter 1 is stopped. Yes.

  While traveling at high speed, such as a train, there is a free-run state in which the inverter 1 is stopped for loss reduction, that is, a coasting state. At this time, if the variable magnetic flux is large, a large induced voltage is also generated. When the induced voltage exceeds the inverter DC voltage, that is, the overhead line voltage, a current flows from the variable magnetic flux motor 4 to the inverter 1 even when the inverter is stopped. This is because the kinetic energy from the variable magnetic flux motor 4 is absorbed, and a braking force is applied to the vehicle, which is not preferable. In addition, when the speed is higher and the amount of magnetic flux is higher, the induced voltage may exceed the withstand voltage on the inverter 1 and the power source side, leading to destruction of the equipment. Therefore, for safety, it is desirable to free run with the total magnetic flux set to zero as much as possible.

  As described above, by reducing the magnetic flux just before the inverter 1 is stopped, it is possible to suppress the occurrence of an induced voltage in free run, and it is possible to avoid the problem of applying a braking force and the possibility of a failure due to an overvoltage of the device. It becomes.

  In particular, among the magnetic fluxes that can be expressed using the variable magnetic flux and the fixed magnetic flux, the magnetic flux whose absolute value is closer to zero is selected and the magnetization process is performed. In the first embodiment, three magnetic flux levels are controlled, and the one having the smallest absolute value is selected. Thereby, generation | occurrence | production suppression of an induced voltage can be made remarkable. The same consideration can be made even when the magnetic flux level is two levels using one variable magnet 53 and the fixed magnet 54, or when the magnetic flux level is four levels or more combining a plurality of variable magnets 53. It is.

  Further, if the variable magnet 53 is not used up to the saturation region, that is, any intermediate value between the positive maximum and the negative maximum of the variable magnet 53 can be used. As a result, it is possible to make the total magnetic flux as zero as possible.

  In addition, for example, by designing the motor structure so that the total magnetic flux of the variable magnet 53 and the total magnetic flux of the fixed magnet 54 are equal, the total magnetic flux can be reduced without changing the use of the variable magnet 53 in the saturation region. It can be zero.

  In the first embodiment, magnetization is performed when the inverter is started and when the inverter is stopped. At this time, the torque command is set to zero. This is because, as described above, an excessive current flows in the magnetization process, so that the generation of transient torque is unavoidable. In a reluctance motor with saliency, since the Q-axis current flows constantly, the generation of transient torque is increased by an excessive magnetizing current to induce mechanical vibration, and the ride comfort is deteriorated in a train or HEV application. Therefore, even in a reluctance motor, since the Q-axis current is zero in a zero torque state, even if an excessive current flows in the D-axis direction due to magnetization, generation of transient torque can be suppressed as much as possible. it can.

  Even in a state where torque is applied, the transient torque can be reduced by the current flowing during the magnetization process. That is, originally, a current in the D-axis direction may be applied to the magnetization process. However, in the salient pole machine, when the Q-axis current flows, the torque varies depending on the D-axis current. Normally, even if it is not a salient pole machine, an excessive current exceeding the rating may flow in the magnetization process, so magnetic saturation occurs instantaneously and there is a possibility of generation of transient torque similar to that of a salient pole machine . In order to suppress this, the Q-axis current is caused to flow as the magnetization current together with the D-axis current. It is clear from equation (11) that the transient torque can be suppressed by the Q-axis current.

  In this way, in order to suppress the transient torque associated with the magnetization process, the transient torque is reduced as much as possible by flowing the Q-axis current together with the D-axis current, and the ride comfort is deteriorated in the induction of mechanical vibrations and in train and HEV applications. Can be suppressed.

  In addition, it is assumed that it is difficult to calculate in advance as in equation (11) because the magnetic flux may change suddenly due to the magnetization process and the equivalent parameter of the motor may fluctuate greatly due to excessive magnetizing current. The Therefore, the Q-axis current should be determined based on the actual machine. That is, it is only necessary to determine the D-axis current necessary for the magnetization process and determine the Q-axis current so that the transient torque can be suppressed. This can be implemented as data stored in a table or the like.

  FIG. 9 is a timing chart showing another example of the operation of the variable magnetic flux drive system according to the first embodiment. FIG. 9 shows a case where the protection signal PROT is established at time ta. That is, it is a timing chart when the inverter is stopped by the protection signal PROT, not when the operation command Run * instructs to stop.

  At the time ta when the protection signal PROT detects the protection operation, the protection signal PROT changes from “0” to “1”. In this state, the operation command Run *, the operation state flag Run, and the torque permission flag TrqON are simultaneously turned off. The gate command Gst is maintained in the on state, and the magnetization process is performed. That is, the magnetization process is performed from the time point ta to the time point tb. As a result, a magnetic flux command Φ * that gives the absolute value of the magnetic flux as close to zero as possible is given.

  As described above, together with the protection detection in which the protection signal PROT changes from “0” to “1”, the inverter 1 is not stopped immediately, but the gate is turned off after the total magnetic flux is reduced. This can reduce the possibility of a secondary failure due to an induced voltage during gate-off in a state in which the protection factor is unknown. For all protection, it is not necessary to notch off after this magnetization process.

(Second Embodiment)
FIG. 10 is a block diagram of a variable magnetic flux drive system according to the second embodiment of the present invention. In the second embodiment, in contrast to the first embodiment shown in FIG. 1, the magnetization request generator 29 replaces the magnetization request flag FCReq output to the variable magnetic flux controller 13 with a torque command generator 38. The pre-magnetization request flag FCReq0 to be output is generated, and the torque command generator 38 inputs the pre-magnetization request flag FCReq0 and the magnetization completion flag FCCmp in addition to the torque permission flag TrqON, and adds the magnetization request flag FCReq to the torque command Tm *. It is made to generate. That is, the torque command generator 38 generates a torque command Tm * for reducing the torque when magnetizing the variable magnet, and outputs the magnetization request flag FCReq to the variable magnetic flux controller 13 after reducing the torque. It is. Thereby, the variable magnetic flux controller 13 operates to magnetize the variable magnet after the torque is reduced. The same elements as those in FIG.

  10, in the first embodiment shown in FIG. 1, the output signal of the magnetization request generation unit 29 is the magnetization request flag FCReq, but in the second embodiment, the previous magnetization request flag FCReq0 is output. . This pre-stage magnetization request flag FCReq0 is input to the torque command generator 38 together with the torque permission signal TrqON and the magnetization completion flag FCCmp.

  FIG. 11 is a block configuration diagram of the torque command generator 38 in the second embodiment. When the previous magnetization request flag FCReq0 is “1”, that is, when there is a request for variable magnetic flux, the RS flip-flop 44 is set. The output of the RS flip-flop 44 is input to the switch 39 via the OR circuit 46. The OR circuit 46 also receives a magnetization completion flag FCCmp.

  The switch 39 switches the output from the torque reference TmR to the predetermined magnetization torque reference TmMag when the output of the OR circuit 46 is “1”. Further, the switching device 40 performs switching by the torque permission flag TrqON. When the torque permission flag TrqON is “1”, the output of the switching device 39 is selected, and when it is “0”, “0” is selected. To do.

  Therefore, if the output of the OR circuit 46 is “1” and the torque permission flag TrqON is in the torque permission state (= 1) while the predetermined torque reference TmMag for magnetization is selected by the switch 39, A magnetizing torque reference TmMag is selected and output from the switch 40. The magnetization torque reference TmMag is limited in its output change slope by the change rate limit 41, and the torque command Tm * gradually changes. The comparator 42 determines whether or not the torque command Tm * is equal to the magnetization torque command TmMag, and outputs “1” if they are equal, and outputs “0” if they are not equal. The output of the comparator 42 and the output of the RS flip-flop 44 are input to the logical product circuit 43, and the logical product is obtained and output as the magnetization request flag FCReq.

  That is, when the change rate limiter 41 causes the gradually changing torque command Tm * to be equal to the magnetization torque command TmMag, the magnetization request flag FCReq becomes the magnetization request (= 1). On the other hand, the magnetization request flag FCReq is input to the delay circuit 45 and output delayed by one control cycle. The output of the delay circuit 45 is input to the reset of the RS flip-flop 44. That is, the magnetization request flag FCReq rises for one cycle in the control cycle (= 1), and is thereafter reset (= 0).

  The magnetization request flag FCReq from the torque command generator 38 is input to the variable magnetic flux controller 13, and the same magnetization process as in the first embodiment is performed. The magnetization completion flag FCCmp from the variable magnetic flux control unit 13 is input to the OR circuit 46 of the torque command generation unit 38 in FIG. 11, and the variable magnetic flux control unit 13 is in the state of magnetization (magnetization completion flag FCCmp = 1). As long as there is, the torque command Tm * is fixed to the magnetization torque command TmMag. As the magnetization is completed (FCCmp = 0), the torque command Tm * gradually increases toward the torque reference TmR by the action of the change rate limiter 41.

  FIG. 12 is a timing chart illustrating an example of the operation of the variable magnetic flux drive system according to the second embodiment. FIG. 12 shows a case where the magnetization torque command TmMag = 0.

  For example, in the operation of the magnetization process B (t4 to t5), the torque command Tm * is narrowed toward zero between time t4 'and time t4 by the previous stage magnetization request flag FCReq0. At the time t4 when it becomes zero, the magnetization request flag FCReq is set and the magnetization process is performed. Until the completion of magnetization (from FCCmp = 1 to 0), the torque command Tm * is maintained at the magnetization torque command = 0.

  As described above, when performing the magnetization process, the torque command Tm * is reduced to the magnetization torque command TmMag so as to be magnetized. Therefore, even in a reluctance motor, the Q-axis current is Since it is zero, even if an excessive current flows in the D-axis direction for magnetization, the generation of transient torque can be suppressed as much as possible.

(Third embodiment)
FIG. 13 is a block diagram of a variable magnetic flux drive system according to the third embodiment of the present invention. In the third embodiment, a modulation factor calculation unit 61 and a field weakening control unit 62 are additionally provided to the first embodiment shown in FIG. 1, and an output signal of the field weakening control unit 62 is generated as a magnetization request. This is output to the unit 29. As a result, the magnetization request generator 29 issues a magnetization request according to the modulation factor of the inverter 1. The same elements as those in FIG.

In FIG. 13, the DC side voltage Vdc of the inverter 1 is detected by the DC voltage detector 60 and input to the modulation factor calculation unit 61. In addition to the DC voltage Vdc, DQ axis voltage commands Vd * and Vq * that are outputs of the voltage command calculation unit 10 are also input to the modulation factor calculation unit 61. The modulation factor calculator 61 calculates the voltage command magnitude V1 * on the DQ axis coordinate system based on the DQ axis voltage commands Vd * and Vq * as shown in the following equation.

Further, the modulation factor calculation unit 61 calculates the maximum DQ axis voltage V1max that can be output from the inverter 1 based on the DC voltage Vdc by the following equation. The maximum output is obtained in the 1 pulse mode.

The modulation rate AL is expressed by the following equation. The modulation factor AL is output from the modulation factor calculator 61. The modulation rate AL is a value between 0 and 1.

The field weakening control unit 62 receives the modulation rate AL from the modulation rate calculation unit 61 and, when the modulation rate AL exceeds a predetermined maximum modulation rate ALmax, corrects and controls the DQ axis current so that AL becomes ALmax. This is field weakening control. The predetermined maximum modulation rate is an arbitrary value, but does not exceed 1. As an example of field weakening control, a correction amount If * for the DQ-axis current is calculated as follows.

  However, s: Laplace operator, Kp: proportional gain, Ki: integral gain, If * is limited to a range of 0 or more. In the above equation, the compensation current command If * for the field weakening is controlled so that the modulation factor AL and the maximum modulation factor ALmax coincide.

  The compensation current command If * for the field weakening finally compensates by applying the current reference IdR and IqR of the DQ axis to the current reference calculation unit 11. In other words, the correction may be made by subtracting the final stage of the calculation formulas (5) and (6) of the current reference calculation unit 11.

  Actually, the compensation current command If * is not simply subtracted and corrected to the D-axis current reference IdR or the Q-axis current reference IqR. is there.

  As described above, field weakening control is possible. By the field weakening control, the compensation current command If * for the field weakening has a value of 0 or more (0 when there is no field weakening, and a positive value in the field weakening) and compensates for the DQ axis current reference. To do.

  This field-weakening compensation current command If * is input to the magnetization request generator 29. The magnetization request generator 29 generates a magnetization request flag FCReq (= 1) in the region where the modulation rate of the inverter is maximized. FIG. 14 is a block diagram showing an example of the magnetization request generator 29 in the third embodiment. A comparison result of the comparator 63 that compares the field-weakening compensation current command If * with a predetermined set value IfMag to the magnetization request generator 29 in the first embodiment shown in FIG. And a change determination unit 64 for determining the change of the above. The same elements as those in FIG. 6 are denoted by the same reference numerals, and redundant description is omitted.

  The field weakening compensation current command If * is compared with a predetermined set value IfMag by the comparator 63. Since the compensation current command If * increases positively in the field weakening region, the set value IfMag is set to positive. When the compensation current command If * increases and becomes larger than the set value IfMag, “1” is output, and when it is smaller, “0” is output. In the change determination unit 64, since the output of the OR circuit 32 that detects the time when the output of the comparator 63 changes and outputs it to the OR circuit 32 is the magnetization request flag FCReq, magnetization processing is performed. That is, in the field weakening region, the magnetization process is performed when the depth of the field weakening becomes large.

  In this magnetization process, for example, if the magnetic flux command calculation unit 12 is set as shown in the above-described equation (2) so as to give a large magnetic flux command Φ * on the low speed side and a small magnetic flux command Φ * on the high speed side. Good. That is, the magnetic flux command Φ * may be switched according to the speed condition.

  FIG. 15 is a characteristic diagram illustrating a response waveform during acceleration of the variable magnetic flux motor 4 according to the third embodiment. FIG. 15 shows a case where the upper limit of the maximum modulation rate ALmax is set to 1. Now, it is assumed that the speed FR of the variable magnetic flux motor 4 has increased from time t0. As the speed FR of the variable magnetic flux motor 4 increases, the modulation rate AL also increases. The field weakening starts at time t1 when the modulation factor AL becomes “1”. That is, the compensation current command If * for the field weakening gradually increases from zero to a positive value. Magnetization process A is performed at time t2 when the compensation current command If * for the field weakening becomes IfMag1, and the magnetic flux decreases from Φ1 to Φ2. At this time, although the magnetic flux decreases, it is still a field weakening region, and the modulation factor is maintained at 1.

  When the compensation current command If * for the field weakening again reaches IfMag2 at time t3, the magnetization process B is performed again, and the magnetic flux decreases from Φ2 to Φ3. In this case, the magnetic flux is greatly reduced, and once the modulation factor AL is less than “1”, it is out of the field weakening region.

  Here, the field weakening is an indispensable function to ensure a wide speed control, but in the case of a permanent magnet synchronous motor, it is necessary to flow a large current for field weakening. A decrease occurs and is not preferable. Therefore, by controlling the magnetic flux according to the magnitude of the compensation current command If * for the field weakening that represents the depth of the field weakening, it is possible to suppress the flow of an excessive current for the field weakening, A reduction in the power factor and efficiency of the motor can be suppressed. As a result, there is an effect that the cooler can be made compact by reducing loss. In addition, a reduction in power factor is reduced, and a switching element having a small current capacity can be used.

  In addition, when the field weakening proceeds due to high speed rotation, it is possible to rotate to a higher speed in order to reduce the magnet magnetic flux, and to operate in a wide speed range.

  Furthermore, in the third embodiment, the upper limit of the maximum modulation rate ALmax is set to “1”, which is a one-pulse mode. The 1-pulse mode outputs the maximum voltage that can be output by the inverter. In addition, one positive / negative pulse is included in one output cycle, and the number of times of switching per cycle is also minimized.

  That is, in the 1-pulse mode, the switching loss of the switching element can be reduced, which contributes to an increase in output voltage and a reduction in the size of the device due to loss reduction. There is no problem as a variable magnetic flux drive system, as in the magnetization process B, where the modulation factor becomes less than “1” after the magnetic flux change. If the switching condition can maintain the one-pulse mode, the burden on the cooler can be reduced without increasing unnecessary switching loss.

  Furthermore, it is desirable to set the compensation current command If * for the field weakening that makes the magnetic flux variable so that the magnetizing process is performed before the magnet is magnetized. When the switching set value IfMag to the compensation current command If * for the field weakening is set to a large value, it is assumed that the magnetization is arbitrarily performed by the current increased by the field weakening control and the magnetic flux is changed. Even in this state, it can be achieved by the third embodiment in which a variable magnet is introduced, such as realizing a wide speed range, but it is desirable to reduce the torque shock accompanying switching when considering mounting on HEVs or trains. When changing the magnetic flux, the magnetic flux fluctuates abruptly, resulting in a torque shock. If the magnet is deliberately changed, the torque shock such as switching to full-tracking current control only during the magnetization process. Can be easily implemented.

  In FIG. 14, only one switching point can be set for the field-weakening compensation current command If *. However, two or more switching points may be provided. FIG. 15 shows a case where there are two switching points (IfMag1, IfMag2).

  FIG. 16 is a characteristic diagram showing a response waveform at the time of deceleration of the variable magnetic flux motor 4 in the third embodiment. As in the case of FIG. 15, for example, the magnetization process A generates a magnetization request at time t13 when the field-weakening compensation current command If * falls below a predetermined value IfMag1. Since the magnetization process B requires the magnetization process outside the field-weakening region, it cannot be realized by the magnetization request based on the compensation current If * for the field-weakening.

  Therefore, the magnetization request generator 29 is configured as shown in FIG. 17 instead of the configuration of FIG. FIG. 17 is a block diagram showing another example of the magnetization request generator 29 in the third embodiment. That is, the magnetization request generator 29 receives the modulation factor AL instead of the field-weakening compensation current command value If *, compares the modulation factor AL with a predetermined set value ALMag by the comparator 63, and compares the result. Is determined by the change determination unit 64 and a magnetization request is issued. Thereby, the magnetization process B is realizable.

  FIG. 18 is a block configuration diagram showing still another example of the magnetization request generation unit 29 in the third embodiment. In this example, the rotor rotational speed ωR of the variable magnetic flux motor 4 is input instead of the modulation rate AL in FIG. The rotor rotation speed ωR is obtained by differentiating the rotation angle detected by the rotation sensor 18.

  The magnetization request generation unit 29 receives the rotor rotational speed ωR of the variable magnetic flux motor 4, compares the rotor rotational speed ωR with a predetermined set value ωRMag by the comparator 63, and changes the comparison result by the change determination unit 64. Determine and issue a magnetization request. That is, as shown in FIG. 18, it is possible to achieve a wide speed range by switching the magnetic flux based on the rotor rotational speed ωR so that the magnetic flux is high at low speed and small at high speed.

The block block diagram of the variable magnetic flux drive system concerning the 1st Embodiment of this invention. The simple model figure of the variable magnetic flux motor in the 1st Embodiment of this invention. The block diagram of the rotor of the variable magnetic flux motor in the 1st Embodiment of this invention. The characteristic view of the BH characteristic (magnetic flux density-magnetization characteristic) of the fixed magnet and variable magnet of a variable magnetic flux motor in a 1st embodiment of the present invention. The characteristic view which shows only the 2nd quadrant (B> 0, H <0) of FIG. 4 in a quantitatively correct relationship. The block block diagram of the magnetization request | requirement production | generation part in the 1st Embodiment of this invention. The block block diagram of the variable magnetic flux control part in the 1st Embodiment of this invention. The timing chart which shows an example of operation | movement of the variable magnetic flux drive system of the 1st Embodiment of this invention. The timing chart which shows another example of operation | movement of the variable magnetic flux drive system of the 1st Embodiment of this invention. The block block diagram of the variable magnetic flux drive system concerning the 2nd Embodiment of this invention. The block block diagram of the torque instruction generation part in the 2nd Embodiment of this invention. The timing chart which shows an example of operation | movement of the variable magnetic flux drive system of the 2nd Embodiment of this invention. The block block diagram of the variable magnetic flux drive system concerning the 3rd Embodiment of this invention. The block block diagram which shows an example of the magnetization request | requirement production | generation part in the 3rd Embodiment of this invention. The characteristic view which shows the response waveform at the time of the acceleration of the variable magnetic flux motor in the 3rd Embodiment of this invention. The characteristic view which shows the response waveform at the time of the deceleration of the variable magnetic flux motor in the 3rd Embodiment of this invention. The block block diagram which shows another example of the magnetization request | requirement production | generation part in the 3rd Embodiment of this invention. The block block diagram which shows another example of the magnetization request | requirement production | generation part in the 3rd Embodiment of this invention.

DESCRIPTION OF SYMBOLS 1 ... Inverter, 2 ... Current detector, 3 ... DC power supply, 4 ... Variable magnetic flux motor, 5 ... Coordinate conversion part, 6 ... PWM circuit, 7 ... Coordinate conversion part, 8 ... Pseudo-differentiator, 10 ... Voltage command calculating part , 11 ... current reference calculation unit, 12 ... magnetic flux command calculation unit, 13 ... variable magnetic flux control unit, 14 ... adder, 15 ... gate command generation unit, 16 ... operation command generation unit, 17 ... protection determination unit, 18 ... rotation Angle sensor, 19 ... subtractor, 20 ... PI controller, 21 ... magnetization current reference calculation unit, 22 ... adder, 23 ... switch, 24 ... magnetization completion determination unit, 25 ... RS flip-flop, 26 ... switch, 27 ... Magnetization current table, 28 ... Minimum on-pulse, 29 ... Magnetic flux variable request generation unit, 30 ... Change determination unit, 31 ... Previous value holding unit, 32 ... Logical sum circuit, 33 ... Previous value holding unit, 34 ... Change Determination unit, 35... Previous value holding unit, 36. Axis magnetization current command calculation unit, 37 ... switch, 38 ... torque command generation unit, 39 ... switch, 40 ... switch, 41 ... change rate limit, 42 ... comparator, 43 ... logical product circuit, 44 ... RS flip-flop 45 ... delay circuit 46 ... OR circuit 51 ... rotor 52 ... rotor core 53 ... variable magnet 54 ... fixed magnet 60 ... DC voltage detector 61 ... modulation factor calculation unit 62 ... Field weakening control unit, 63 ... comparator, 64 ... change determination unit

Claims (2)

In a variable magnetic flux drive system including an inverter that drives a variable magnetic flux motor having a fixed magnet and a variable magnet, a torque command generator that generates a torque command of the variable magnetic flux motor, and a magnetic flux generated by a magnetizing current from the inverter. A variable magnetic flux controller that magnetizes the variable magnet, and a switch that switches between a DQ axis current reference based on a torque command from the torque command generator and a DQ axis magnetizing current command from the variable magnetic flux controller. A magnetization request generation unit that generates a request to magnetize the variable magnet when a predetermined condition is established for the variable magnetic flux control unit, and a DQ axis current reference or a DQ axis magnetization current command based on a torque command from the switch And a gate command generation unit that generates a gate command for controlling the inverter based on The by current increase due to field weakening control of the variable magnet, the variable magnetic flux drive system characterized by emitting a magnetization request before the flux of the variable magnet is changed. The magnetization request generator generates a magnetization request even after the magnetic flux is varied by the field weakening control of the variable magnet and before the magnetic flux of the variable magnet is changed due to the current increase due to the field weakening control. The variable magnetic flux drive system according to claim 1.

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