JP2013005510A - Electromagnetic rotary electric machine - Google Patents

Abstract

PROBLEM TO BE SOLVED: To provide an electromagnetic rotary electric machine that allows many harmonic components included in a rotating magnetic field to be interlinked with rotor windings so as to increase induced current generated in the rotor windings.SOLUTION: A stator 12 includes a plurality of stator windings 20u, 20v, and 20w wound around teeth 18. A rotor 14 includes: a rotor core 24; a plurality of rotor windings 28n and 28s wound around a plurality of main salient poles 26 of the rotor 14; and diodes, as magnetic property adjusting sections, that circumferentially vary magnetic properties developed in the main salient poles 26 by induced electromotive force generated in the rotor windings 28n and 28s. The rotor 14 has auxiliary salient poles 44, with polarities, that project from respective circumferential side surfaces of the main salient poles 26.

Description

  The present invention relates to an electromagnet type rotating electrical machine in which a stator and a rotor are arranged to face each other.

  Conventionally, as described in Patent Document 1, an electromagnetic rotating electrical machine in which a stator and a rotor are arranged to face each other, and salient poles provided at a plurality of locations in the circumferential direction of the rotor, and wound around each salient pole. 2. Description of the Related Art There is known an electromagnet type rotating electrical machine that includes mounted rotor windings and includes a rotor winding that is divided from each other and a diode that is connected to each rotor winding. Each diode rectifies the current flowing in each rotor winding so that the magnetization direction is reversed between salient poles adjacent in the circumferential direction of the rotor. The stator includes teeth provided at a plurality of locations in the circumferential direction of the stator core. A plurality of stator windings are wound around the stator teeth in a concentrated manner. A rotating magnetic field that rotates in the circumferential direction is generated in the stator by passing a plurality of phases of alternating current through the stator windings of the plurality of phases. Then, an induction current is generated in the rotor winding by spatial harmonics that are harmonic components generated in the magnetomotive force distribution generated in the stator, and N and S poles are alternately formed in the salient poles in the circumferential direction of the rotor, Torque is generated in the rotor. At this time, a current rectified by each diode flows through each rotor winding, whereby each salient pole is magnetized to generate a magnet with a fixed magnetic pole.

  In such an electromagnet type rotating electrical machine, the salient pole interacts with the rotating magnetic field of the stator, and torque acts on the rotor. Further, the torque acting on the rotor can be efficiently increased by utilizing the harmonic component of the magnetic field formed by the stator.

JP 2009-112091 A

  In such a rotating electrical machine, there is room for improvement in terms of increasing the induced current generated in the rotor winding for forming the electromagnet in the rotor.

  An object of the present invention is to increase an induced current generated in a rotor winding by interlinking a lot of harmonic components contained in a rotating magnetic field with the rotor winding in an electromagnet type rotating electrical machine.

  The electromagnet type rotating electrical machine according to the present invention employs the following means in order to achieve the above object.

  An electromagnet type rotating electrical machine according to the present invention is an electromagnet type rotating electrical machine in which a stator and a rotor are arranged to face each other, and the stator includes a stator core, teeth disposed at a plurality of locations in the circumferential direction of the stator core, and at least the above A plurality of stator windings wound around the stator core or the teeth to generate a rotating magnetic field, and the rotor includes a rotor core, main salient poles arranged at a plurality of locations in the circumferential direction of the rotor core, and the main coils. A plurality of rotor windings at least partially wound around salient poles, and a magnetic characteristic that alternately causes magnetic characteristics generated in the plurality of main salient poles by induced electromotive force generated in each rotor winding in the circumferential direction An electromagnet-type rotating electric machine, wherein the rotor further includes an auxiliary salient pole having magnetism protruding from a circumferential side surface of each main salient pole. It is.

  According to the electromagnet type rotating electrical machine according to the present invention, the rotor protrudes from the circumferential side surface of each main salient pole and includes magnetic auxiliary salient poles. Therefore, the rotor is included in the rotating magnetic field generated by the stator, and the rotor winding It is possible to increase the harmonic components interlinked with each other. For this reason, the change of the magnetic flux density of the magnetic flux linked to the rotor winding can be increased, and the induced current induced in the rotor winding can be increased.

  In the electromagnet-type rotating electrical machine according to the present invention, preferably, each of the rotor windings is connected to a rectifying element that is the magnetic characteristic adjusting unit, and the rectifying element is connected to the rotor winding by generating an induced electromotive force. By rectifying the current flowing through the rotor winding, the phases of the current flowing through the rotor windings adjacent in the circumferential direction are alternately changed between the A phase and the B phase.

  In the electromagnet-type rotating electrical machine according to the present invention, preferably, the tip of the auxiliary salient pole is positioned on the outer side in the radial direction of the rotor than the root of the auxiliary salient pole.

  According to the above configuration, according to the tip position of the auxiliary salient pole, a necessary magnetic flux component of spatial harmonics is efficiently induced from the auxiliary salient pole to the main salient pole, and a large amount of magnetic flux is efficiently chained to the rotor winding. The induced current induced in the rotor winding can be increased.

  In the electromagnet-type rotating electrical machine according to the present invention, preferably, the auxiliary salient poles are provided on both side surfaces in the circumferential direction of the main salient poles so as to protrude in the circumferential direction or in a direction inclined with respect to the circumferential direction, respectively. It has been.

  In the electromagnet-type rotating electrical machine according to the present invention, preferably, two auxiliary salient poles are circumferential side surfaces of two main salient poles adjacent to each other in the circumferential direction and are coupled to circumferential side surfaces facing each other. Are not connected to each other.

  According to the above configuration, it is possible to suppress the flow of magnetic flux that does not contribute to the torque to the main salient pole, improve the torque, and easily arrange the rotor winding inside the auxiliary salient pole in the radial direction of the rotor.

  In the electromagnet-type rotating electrical machine according to the present invention, preferably, the auxiliary salient pole is inclined with respect to the circumferential direction so as to be radially outward of the rotor toward the tip on the circumferential side surface of the main salient pole. Protrudes in the direction.

  According to the above configuration, without excessively increasing the length of the auxiliary salient pole, a necessary magnetic flux component of space harmonics is efficiently induced from the auxiliary salient pole to the main salient pole, and the rotor winding is efficiently increased. Thus, the induced current induced in the rotor winding can be increased.

  In the electromagnet-type rotating electrical machine according to the present invention, preferably, the auxiliary salient pole is coupled so as to project in the circumferential direction from the circumferential side surface of the main salient pole, and is directed radially outward at the intermediate portion. It is bent.

  According to the said structure, it becomes easy to arrange | position many rotor windings outside an auxiliary salient pole regarding the radial direction of a rotor.

  In the electromagnet type rotating electrical machine according to the present invention, preferably, the auxiliary salient pole has a tip portion whose width in the circumferential direction increases toward the radially outer side of the rotor.

  According to the above configuration, the magnetic flux component of the spatial harmonics is efficiently guided from the auxiliary salient pole or main salient pole to the main salient pole or auxiliary salient pole without excessively reducing the rotor winding arrangement space. As a result, a large amount of magnetic flux can be efficiently linked to the rotor winding, and the induced current induced in the rotor winding can be increased.

  In the electromagnet-type rotating electrical machine according to the present invention, preferably, the width of each rotor winding in the circumferential direction of the rotor is shorter than a width corresponding to 180 ° in electrical angle.

  In the electromagnet-type rotating electrical machine according to the present invention, preferably, the width of each rotor winding in the circumferential direction of the rotor is equal to a width corresponding to an electrical angle of 90 °.

  According to the electromagnet type rotating electrical machine of the present invention, it is possible to increase the induced current generated in the rotor winding by interlinking the spatial harmonics included in the rotating magnetic field with the rotor winding.

In the electromagnet-type rotary electric machine of embodiment of this invention, it is a schematic sectional drawing which shows a circumferential direction part of a rotor and a stator. It is the A section enlarged view of FIG. In embodiment of this invention, it is a schematic diagram which shows a mode that the magnetic flux produced | generated by the induced current which flows into a rotor coil | winding flows in a rotor. FIG. 4 is a diagram corresponding to FIG. 3, showing a diode connected to a rotor winding. In an embodiment of the invention, it is a figure showing an equivalent circuit of a connection circuit of two rotor windings wound around a main salient pole adjacent in the circumferential direction of a rotor. It is a figure corresponding to Drawing 5A which shows another example which reduced the number of diodes connected to a rotor winding. It is a figure which shows schematic structure of the rotary electric machine drive system which drives the electromagnet-type rotary electric machine of FIG. In the electromagnet-type rotary electric machine of FIG. 1, it is a figure which shows the result of having calculated the amplitude of the linkage flux to a rotor winding, changing the width | variety (theta) of the rotor winding regarding the circumferential direction. It is a figure which shows the magnetic flux line which induces a rotor electric current in the simulation result in the electromagnet-type rotary electric machine of a comparative example. It is a figure which shows the magnetic flux line which induces a rotor electric current in the simulation result in the electromagnet-type rotary electric machine of embodiment of this invention. In the electromagnet-type rotary electric machine of another embodiment of this invention, it is a figure corresponding to FIG. 2 which shows the 1st example of another example of an auxiliary salient pole. In the electromagnet-type rotary electric machine of another embodiment of this invention, it is the B section enlarged correspondence view of FIG. 2 which shows the 2nd example of another example of an auxiliary salient pole. In the electromagnet-type rotary electric machine of another embodiment of this invention, it is the B section enlarged correspondence view of FIG. 2 which shows the 3rd example of another example of an auxiliary salient pole. In the electromagnet-type rotary electric machine of another embodiment of this invention, it is the B section enlarged correspondence view of FIG. 2 which shows the 4th example of another example of an auxiliary salient pole. In the electromagnet-type rotary electric machine of another embodiment of this invention, it is a schematic sectional drawing which shows a circumferential direction part of a rotor and a stator. FIG. 15 is a schematic diagram showing how the magnetic flux generated by the induced current flowing in the rotor winding flows in the rotor in the electromagnet-type rotating electrical machine of FIG. 14. In the electromagnet-type rotary electric machine of another embodiment of this invention, it is a schematic diagram which shows a mode that the magnetic flux produced | generated by the induced current which flows into a rotor coil | winding flows in a rotor.

  Hereinafter, embodiments of the present invention will be described with reference to the drawings. 1-7 is a figure which shows embodiment of this invention. FIG. 1 is a schematic cross-sectional view showing a part of the rotor and the stator in the circumferential direction in the electromagnet-type rotating electrical machine of the present embodiment. FIG. 2 is an enlarged view of part A in FIG. FIG. 3 is a schematic diagram showing how the magnetic flux generated by the induced current flowing in the rotor winding flows in the rotor in the present embodiment. FIG. 4 is a diagram corresponding to FIG. 3 and showing a diode connected to the rotor winding. As shown in FIG. 1, an electromagnet-type rotating electrical machine (hereinafter simply referred to as “rotating electrical machine”) 10 that functions as an electric motor or a generator includes a stator 12 fixed to a casing (not shown), a predetermined gap with the stator 12. And a rotor 14 that is opposed to the inner side in the radial direction and is rotatable with respect to the stator 12 (note that the “radial direction” simply refers to a radial direction perpendicular to the rotation center axis of the rotor). The same is true throughout and in the claims.)

  Further, the stator 12 includes a stator core 16 that is a stator yoke, teeth 18 that are disposed in the circumferential direction of the stator core 16, and a plurality of phases wound around each of the teeth 18, that is, more specifically, u. Stator windings 20u, 20v, and 20w of three phases (phase, v phase, and w phase). That is, a plurality of teeth 18 projecting radially inward (toward the rotor 14) are arranged on the inner peripheral surface of the stator core 16 at intervals from each other along the circumferential direction of the stator 12. A status lot 22 is formed between them. The stator core 16 and the plurality of teeth 18 are integrally provided with a magnetic material.

  The stator windings 20u, 20v, and 20w of each phase are wound around the teeth 18 through the status lot 22 in a concentrated manner with short nodes. As described above, the stator windings 20u, 20v, and 20w are wound around the teeth 18 to form a magnetic pole. Then, by passing a plurality of phases of alternating current through the plurality of stator windings 20u, 20v, and 20w, a plurality of teeth 18 arranged in the circumferential direction are magnetized, and a rotating magnetic field that rotates in the circumferential direction is generated in the stator 12. . That is, the stator windings 20u, 20v, and 20w having a plurality of phases generate a rotating magnetic field in the stator 12. Note that the stator winding is not limited to the configuration in which the stator winding is wound around the teeth 18 of the stator 12 as described above. It is also possible to generate a rotating magnetic field in the stator 12 by using a toroidal winding.

  The rotating magnetic field formed on the teeth 18 acts on the rotor 14 from the tip surface. In the example shown in FIG. 1, one pole pair is configured by three teeth 18 around which three-phase (u-phase, v-phase, and w-phase) stator windings 20u, 20v, and 20w are wound.

  On the other hand, the rotor 14 is a protrusion that is disposed to protrude radially outward (toward the stator 12) at a plurality of circumferentially equidistant locations on the outer surface of the rotor core 24 that is a cylindrical rotor yoke. A main salient pole 26 and a plurality of rotor windings 28n and 28s (referred to simply as “circumferential direction”, a direction along a circle drawn around the rotation center axis of the rotor). The same throughout the specification and claims). The rotor core 24 and the plurality of main salient poles 26 are integrally provided by a magnetic material such as a laminate in which a plurality of magnetic steel plates are laminated. More specifically, with respect to the circumferential direction of the rotor 14, every other main salient pole 26 is wound with a plurality of first rotor windings 28n by concentrated winding, and the first rotor winding 28n is wound around the main salient pole 26. A plurality of second rotor windings 28s are wound around the other main salient poles 26 adjacent to each other in the circumferential direction every other main salient pole 26 by concentrated winding.

  Further, as shown in FIGS. 2 to 4, each first rotor winding 28 n has a first induction winding 30 wound on the tip side (the upper end side in FIGS. 2 to 4) of the main salient pole 26, And a first common winding 32 connected to the first induction winding 30. The first common winding 32 is wound on the base side (the lower end side in FIGS. 2 to 4) of the main salient pole 26 around which the first induction winding 30 is wound. Each of the second rotor windings 28s has a second induction winding wound around the tip of another main salient pole 26 adjacent to the main salient pole 26 around which the first rotor winding 28n is wound in the circumferential direction. 34 and a second common winding 36 connected to the second induction winding 34. The second common winding 36 is wound on the base side of the main salient pole 26 around which the second induction winding 34 is wound.

  As shown in FIG. 4, two main salient poles 26 adjacent in the circumferential direction of the rotor 14 are taken as one set, and one end of a first induction winding 30 wound around one main salient pole 26 in each set, Then, one end of a second induction winding 34 wound around another main salient pole 26 is connected via two first diodes 38 and a second diode 40 which are two magnetic characteristic adjusting units and rectifiers. Yes. That is, FIG. 5A shows an equivalent circuit of a connection circuit of two rotor windings 28n and 28s wound around the main salient poles 26 adjacent to each other in the circumferential direction of the rotor 14 (FIG. 4) in the present embodiment. FIG. As shown in FIG. 5A, one end of the first induction winding 30 and the second induction winding 34 is connected at a connection point R via a first diode 38 and a second diode 40 whose forward directions are opposite to each other. ing.

  Also, as shown in FIGS. 4 and 5A, one end of the first common winding 32 wound around one main salient pole 26 in each group has a second common winding wound around another main salient pole 26. Connected to one end of line 36. The first common winding 32 and the second common winding 36 are connected in series to form a common winding set 42. Further, the other end of the first common winding 32 is connected to the connection point R, and the other end of the second common winding 36 is opposite to the connection point R of the first induction winding 30 and the second induction winding 34. Is connected to the other end. Further, the winding central axes of the induction windings 30 and 34 and the common windings 32 and 36 of the rotor windings 28n and 28s coincide with the radial direction of the rotor 14 (FIG. 1). The induction windings 30 and 34 and the common windings 32 and 36 are wound around the corresponding main salient poles 26 via an insulating insulator (not shown) made of resin or the like. You can also.

  In such a configuration, as will be described later, the rectified current flows through the first induction winding 30, the second induction winding 34, the first common winding 32, and the second common winding 36, thereby causing the main salient pole. 26 is magnetized and functions as a magnetic pole part. Returning to FIG. 1, the stator 12 generates a rotating magnetic field by passing an alternating current through the stator windings 20u, 20v, and 20w. This rotating magnetic field is not only a fundamental wave component but also a fundamental wave. It contains a higher order harmonic component magnetic field.

  More specifically, the distribution of the magnetomotive force that generates the rotating magnetic field in the stator 12 is caused by the arrangement of the stator windings 20u, 20v, 20w of each phase and the shape of the stator core 16 by the teeth 18 and the status lot 22 ( It does not have a sinusoidal distribution (of the fundamental wave only) and includes harmonic components. In particular, in the concentrated winding, the stator windings 20u, 20v, 20w of the respective phases do not overlap each other, so that the amplitude level of the harmonic component generated in the magnetomotive force distribution of the stator 12 increases. For example, when the stator windings 20u, 20v, and 20w are three-phase concentrated windings, the harmonic component is a temporal third-order component of the input electrical frequency, and the amplitude level of the spatial second-order component increases. The harmonic components generated in the magnetomotive force due to the arrangement of the stator windings 20u, 20v, 20w and the shape of the stator core 16 are called spatial harmonics.

  When a rotating magnetic field including this space-emphasized wave component acts on the rotor 14 from the stator 12, the fluctuation of the leakage magnetic flux leaking into the space between the main salient poles 26 of the rotor 14 is generated due to the fluctuation of the spatial harmonic magnetic flux. Thus, an induced electromotive force is generated in at least one of the induction windings 30 and 34 shown in FIG. In addition, the induction windings 30 and 34 near the stator 12 on the tip side of the main salient pole 26 have a function of mainly generating an induced current, and the common windings 32 and 36 far from the stator 12 mainly have the main projection. A function of magnetizing the pole 26 can be provided. Further, as understood from the equivalent circuit of FIG. 5A, the total current flowing through the induction windings 30 and 34 wound around the adjacent main salient poles 26 (FIGS. 3 and 4) is the common windings 32 and 36. The currents that flow through Further, since the adjacent common windings 32 and 36 are connected in series, the same effect can be obtained as when the number of turns is increased in both, and the magnetic flux flowing through each main salient pole 26 remains the same. The current flowing through each common winding 32, 36 can be reduced.

  When an induced electromotive force is generated in each induction winding 30, 34, diodes 38, 40 are connected to the first induction winding 30, the second induction winding 34, the first common winding 32, and the second common winding 36. A direct current corresponding to the commutation direction flows, and the main salient pole 26 around which the rotor windings 28n and 28s are wound is magnetized, so that the main salient pole 26 functions as a magnetic pole portion that is a magnet with a fixed magnetic pole. . As shown in FIG. 4, the winding directions of the first rotor winding 28n and the second rotor winding 28s adjacent to each other in the circumferential direction are reversed, and the magnetization directions are reversed between the main salient poles 26 adjacent to each other in the circumferential direction. Become. In the illustrated example, an N pole is generated at the tip of the main salient pole 26 around which the first rotor winding 28n is wound, and an S pole is at the tip of the main salient pole 26 around which the second rotor winding 28s is wound. It is generated. For this reason, the N pole and the S pole are alternately arranged in the circumferential direction of the rotor 14. Each diode 38, 40 (FIG. 4) has a magnetic characteristic generated in the plurality of main salient poles 26 by the induced electromotive force generated in the plurality of rotor windings 28n, 28s wound around each main salient pole 26. The direction is changed alternately.

  The diodes 38 and 40 are connected to the corresponding induction windings 30 and 34, and the induction coils 30 and 34 are generated by the induction electromotive force generated by the rotating magnetic field including the spatial harmonics generated by the stator 12. By rectifying the current flowing through the rotor 14, the phases of the current flowing through the induction windings 30 and 34 adjacent to each other in the circumferential direction of the rotor 14 are alternately changed between the A phase and the B phase. The A phase generates an N pole on the tip side of the corresponding main salient pole 26, and the B phase generates an S pole on the tip side of the corresponding main salient pole 26.

  Further, as shown in FIG. 1, the width θ of each induction winding 30, 34 and each common winding 32, 36 in the circumferential direction of the rotor 14 is shorter than the width corresponding to 180 ° in terms of the electrical angle of the rotor 14. The induction windings 30 and 34 and the common windings 32 and 36 are wound around the main salient pole 26 with a short-pitch winding. More preferably, the width θ of each induction winding 30, 34 and each common winding 32, 36 in the circumferential direction of the rotor 14 is equal to or substantially equal to a width corresponding to 90 ° in electrical angle of the rotor 14. Yes. The width θ of each induction winding 30, 34 and each common winding 32, 36 here is determined in consideration of the cross-sectional area of each induction winding 30, 34 and each common winding 32, 36. It can be represented by the center width of the cross section of the lines 30 and 34 and the common windings 32 and 36. That is, the widths of the induction windings 30 and 34 and the common windings 32 and 36 are average values of the widths of the inner and outer peripheral surfaces of the induction windings 30 and 34 and the common windings 32 and 36. θ can be expressed. The electrical angle of the rotor 14 is represented by a value obtained by multiplying the mechanical angle of the rotor 14 by the number of pole pairs p of the rotor 14 (electrical angle = mechanical angle × p). Therefore, the width θ of each induction winding 30, 34 and each common winding 32, 36 in the circumferential direction is from the rotation center axis of the rotor 14 to each induction winding 30, 34 and each common winding 32, 36. When the distance is r, the following expression (1) is satisfied.

θ <π × r / p (1)
The reason why the width θ is regulated in this way will be described in detail later.

  In particular, in the present embodiment, the rotor 14 includes auxiliary salient poles 44 on both sides in the circumferential direction of the main salient poles 26 arranged at a plurality of locations in the circumferential direction. The auxiliary salient pole 44 protrudes in a direction inclined with respect to the circumferential direction from both side surfaces of the main salient pole 26 over almost the entire length of the main salient pole 26 in the axial direction (front and back directions in FIGS. 1 and 2). It is a magnetic material. For this reason, the auxiliary salient pole 44 projects from both side surfaces of the main salient pole 26. For example, in the example shown in the figure, the auxiliary salient poles 44 are located radially outward of the rotor 14 toward the tip in the radial direction (vertical direction in FIG. 2) intermediate side surfaces of the respective main salient poles 26. It protrudes in a direction inclined with respect to the circumferential direction. For this reason, the tip of each auxiliary salient pole 44 is located on the radially outer side of the rotor 14 with respect to the base of the auxiliary salient pole 44. Further, the width of each auxiliary salient pole 44 is made substantially the same, being larger at the root portion and smaller than the width of the root portion from the intermediate portion to the tip portion.

  Such auxiliary salient poles 44 are formed between the main salient poles 26 of the rotor 14 as shown in FIG. 3, and are arranged in a plurality of rotor slots 46 in which the rotor windings 28n and 28s are arranged inside. The adjacent main salient poles 26 protrude from the circumferential side surfaces facing each other. Further, the two auxiliary salient poles 44 disposed in the same rotor slot 46 are not directly coupled to each other, and the tip portions are separated from each other. Such an auxiliary salient pole 44 can be formed of the same magnetic material as the rotor core 24 and the main salient pole 26. For example, the rotor core 24, the main salient poles 26, and the auxiliary salient poles 44 can be integrally formed by a laminate configured by laminating a plurality of magnetic steel plates in the axial direction.

  Of the rotor windings 28 n and 28 s wound around the main salient poles 26, the induction windings 30 and 34 and the common windings 32 and 36 are partitioned by the auxiliary salient poles 44 in the corresponding rotor slots 46. Have been separated. The induction windings 30 and 34 and the common windings 32 and 36 wound around the same main salient pole 26 are auxiliary salient poles such as one or both coil end sides (not shown) provided outside the axial end surface of the rotor core 24. They are connected to each other at a portion away from 44. The induction windings 30 and 34 and the common windings 32 and 36 can be formed of different materials. For example, each of the common windings 32 and 36 is formed of a conductive material such as copper wire, and each of the induction windings 30 and 34 is lighter than the conductive material constituting the common winding such as aluminum or aluminum alloy. It can also be formed of another conductive material. Further, as shown in FIG. 2, a flange portion 48 projecting on both sides in the circumferential direction is formed at the tip of each main salient pole 26 to prevent the induction windings 30 and 34 (34 see FIG. 3 etc.) from coming off. You can also plan.

  Such a rotating electrical machine 10 is driven by the rotating electrical machine drive system 50 of FIG. FIG. 6 is a diagram showing a schematic configuration of a rotating electrical machine drive system 50 that drives the rotating electrical machine 10 of FIG. The rotating electrical machine drive system 50 includes the rotating electrical machine 10, an inverter 52 that is a drive unit that drives the rotating electrical machine 10, a control device 54 that controls the inverter 52, and a power storage device 56 that is a power supply unit. Drive.

  The power storage device 56 is provided as a direct current power source and is chargeable / dischargeable, and is constituted by, for example, a secondary battery. The inverter 52 includes U-phase, V-phase, and W-phase three-phase arms Au, Av, and Aw, and each phase arm Au, Av, and Aw has two switching elements Sw connected in series. The switching element Sw is a transistor, an IGBT, or the like. A diode Di is connected in antiparallel to each switching element Sw. The midpoint of each arm Au, Av, Aw is connected to one end side of the corresponding phase stator windings 20u, 20v, 20w constituting the rotating electrical machine 10. In the stator windings 20u, 20v, and 20w, stator windings of the same phase are connected in series with each other, and stator windings 20u, 20v, and 20w of different phases are connected at a neutral point.

  Further, the positive electrode side and the negative electrode side of the power storage device 56 are respectively connected to the positive electrode side and the negative electrode side of the inverter 52, and a capacitor 58 is connected in parallel to the inverter 52 between the power storage device 56 and the inverter 52. Has been. The control device 54 calculates a torque target of the rotating electrical machine 10 according to an acceleration command signal input from, for example, an accelerator pedal sensor (not shown) of the vehicle, for example, and each according to a current command value according to the torque target or the like. The switching operation of the switching element Sw is controlled. The control device 54 includes a signal representing a current value detected by a current sensor 60 provided on the stator winding (for example, 20u, 20v) side of at least two phases of the three phases, and a rotation angle detection unit such as a resolver. A signal indicating the rotation angle of the rotor 14 (FIG. 1) of the rotating electrical machine 10 detected by (not shown) is input. The control device 54 includes a microcomputer having a CPU, a memory, and the like, and controls the torque of the rotating electrical machine 10 by controlling the switching of the switching element Sw of the inverter 52. The control device 54 can also be configured by a plurality of control devices divided for each function.

  Such a control device 54 converts the DC power from the power storage device 56 into three-phase AC power of u-phase, v-phase, and w-phase by the switching operation of each switching element Sw constituting the inverter 52, and It is possible to supply electric power of a phase corresponding to each phase of the windings 20u, 20v, and 20w. The rotating electrical machine drive system 50 is used, for example, as a vehicular travel power generator mounted on a hybrid vehicle, a fuel cell vehicle, an electric vehicle or the like that includes an engine and a travel motor as drive sources. Note that a DC / DC converter that is a voltage conversion unit may be connected between the power storage device 56 and the inverter 52 so that the voltage of the power storage device 56 can be boosted and supplied to the inverter 52.

  In the rotating electrical machine 10 described above, a rotating magnetic field (fundamental wave component) formed in the teeth 18 is applied to the rotor 14 by passing a three-phase alternating current through the three-phase stator windings 20u, 20v, and 20w. Accordingly, the main salient pole 26 is attracted to the rotating magnetic field of the teeth 18 so that the magnetic resistance of the rotor 14 is reduced. As a result, torque (reluctance torque) acts on the rotor 14.

  Further, when the rotating magnetic field including the spatial harmonic component formed in the teeth 18 is linked to the induction windings 30 and 34 of the rotor windings 28n and 28s of the rotor 14, the induction windings 30 and 34 have a space. An induced electromotive force is generated in each of the rotor windings 28n and 28s due to a magnetic flux fluctuation having a frequency different from the rotation frequency of the rotor 14 (fundamental wave component of the rotating magnetic field) caused by the harmonic component. The current flowing through each of the rotor windings 28n and 28s along with the generation of the induced electromotive force is rectified by the respective diodes 38 and 40 to be unidirectional (direct current). The main salient poles 26 are magnetized in accordance with the direct current rectified by the diodes 38 and 40 flowing into the rotor windings 28n and 28s, so that the main salient poles 26 have magnetic poles (N poles). It functions as a fixed magnet).

  For example, as shown in FIG. 3, the teeth 18 wound with the stator windings 20u, 20v, 20w of the respective phases of the stator 12 are opposed to the main salient poles 26 wound with the rotor windings 28n, 28s in the radial direction. However, let us consider a case where one tooth 18 faces the center position between two main salient poles 26 adjacent to each other in the circumferential direction of the rotor 14. Further, in this state, as indicated by a broken line arrow in FIG. 3, a case where a q-axis magnetic flux, which is a magnetic flux of a spatial second-order spatial harmonic, flows from the stator 12 to the rotor 14 as the magnetomotive force of the stator 12 is considered. . In this case, the presence of the auxiliary salient poles 44 induces a large amount of spatial harmonics from the teeth 18 (in the W phase in FIG. 3) of the stator 12 to the main salient poles 26 via the auxiliary salient poles 44. Can be induced to another tooth 18 (U-phase and V-phase in FIG. 3), and a large amount of magnetic flux can be linked to the induction windings 30 and 34. FIG. 3 shows a state corresponding to the phase angle at which the maximum q-axis magnetic flux flows from one tooth 18, and the direction and magnitude of the q-axis magnetic flux change in one electrical cycle. In FIG. 3, the broken line arrow α indicates the magnetic flux interlinking with the induction winding 30, and the broken arrow β indicates the magnetic flux interlinking with the induction winding 34. In this case, the second diode 40 (FIG. 4) is connected to the second induction winding 34 wound around the main salient pole 26 that is the S pole, and the second diode 40 sets the corresponding main salient pole 26 as the S pole. Current in the direction of For this reason, the magnetic flux tends to flow in the direction where the S pole becomes the N pole due to the q-axis magnetic flux on the main salient pole 26 on the S pole side, and the induced current tends to flow in the second induction winding 34 in a direction that prevents this. The flow is not hindered by the second diode 40. As a result, as shown by the solid line arrows in FIG. In some cases, the q-axis magnetic flux tends to flow from the teeth 18 of the stator 12 to the auxiliary salient poles 44 through the N-pole main salient poles 26. Is about to flow, an induced current tends to flow through the first induction winding 30 wound around the N-pole main salient pole 26 in a direction that prevents this. In this case, the first diode 38 (FIG. 4) connected to the first induction winding 30 causes a current to flow in the direction in which the corresponding main salient pole 26 is the N pole. In this case also, as indicated by the solid line arrow in FIG. For this reason, each main salient pole 26 is magnetized to N pole or S pole. As described above, since the auxiliary salient poles 44 protrude from both side surfaces of each main salient pole 26, there is no auxiliary salient pole 44, that is, a space between the main salient poles 26 adjacent in the circumferential direction in each slot 46. Compared with the case where there is only one, the maximum value of the amplitude of the magnetic flux interlinking with each induction winding 30 and 34 can be increased, so that the change of the interlinkage magnetic flux can be increased.

  Then, the magnetic field of each main salient pole 26 (magnet with a fixed magnetic pole) interacts with the rotating magnetic field (fundamental wave component) generated by the stator 12, thereby causing attraction and repulsion. Torque (torque corresponding to magnet torque) is also applied to the rotor 14 by electromagnetic interaction (attraction and repulsion) between the rotating magnetic field (fundamental wave component) generated by the stator 12 and the magnetic field of the main salient pole 26 (magnet). The rotor 14 is driven to rotate in synchronization with the rotating magnetic field (fundamental wave component) generated by the stator 12. As described above, the rotating electrical machine 10 can function as an electric motor that generates power (mechanical power) in the rotor 14 by using power supplied to the stator windings 20u, 20v, and 20w.

  Further, since the phases of the induced current flowing through the first induction winding 30 and the induced current flowing through the second induction winding 34 are out of phase, the phases of the first induction winding 30 and the second induction winding 34 are out of phase. Half-wave rectification is generated. On the other hand, the first common winding 32 and the second common winding 36 have a current having the magnitude of the sum of the currents flowing through the first induction winding 30 and the second induction winding 34. For example, a large direct current flows continuously. For this reason, it becomes easy to form a magnetic pole in each main salient pole 26, and the torque of the rotor 14 can be increased.

  In addition, according to the rotating electrical machine 10 of the present embodiment, the rotor 14 protrudes from the circumferential side surface of each main salient pole 26 and includes the auxiliary salient pole 44 having magnetism. The auxiliary harmonics 44 can effectively increase the spatial harmonics that are included and interlink with the rotor windings 28n and 28s, for example, the spatial secondary harmonic components that are time-thirds. . For example, many magnetic fluxes of harmonic components of the magnetomotive force distribution generated in the stator 12 are guided from the teeth 18 of the stator 12 to the main salient poles 26 via the auxiliary salient poles 44, and are transferred to the rotor windings 28n and 28s. Many magnetic fluxes can be linked. It is also possible to induce a large amount of magnetic flux of harmonic components from the tooth 18 to the auxiliary salient pole 44 via the main salient pole 26, and to link a lot of magnetic flux to the rotor windings 28n and 28s. Therefore, the change in the magnetic flux density of the magnetic flux interlinking with the rotor windings 28n and 28s can be increased, the induced current induced in the rotor windings 28n and 28s can be increased, and the electromagnet formed on the main salient pole 26. The magnetic force of the magnetic pole can be increased. For this reason, the torque of the rotating electrical machine 10 can be improved without increasing the rotor magnetic force and increasing the size of the rotating electrical machine 10. Further, since a desired torque can be obtained even if the stator current passed through the stator windings 20u, 20v, and 20w is reduced, copper loss can be reduced and efficiency can be improved. As a result, the torque and efficiency of the rotating electrical machine 10 can be improved. In this way, the auxiliary salient pole 44 made of a magnetic material is projected directly on the side surface in the circumferential direction of the main salient pole 26, and the main salient pole 26 and the auxiliary salient pole 44 are directly magnetically coupled, so that the magnetic path is Since it is formed, the flux linkage to the rotor windings 28n and 28s can be increased, and the torque and efficiency of the rotating electrical machine 10 can be improved.

  On the other hand, unlike the present invention, when the auxiliary salient pole 44 is not formed on the circumferential side surface of the main salient pole 26, the number of interlinkage magnetic fluxes for generating an induced current in the rotor windings 28n and 28s is small. Thus, the induced current generated in the rotor windings 28n and 28s is reduced. For this reason, the magnetic force of the electromagnet formed by the induced current flowing through the rotor windings 28n and 28s becomes weak, and there is room for improvement in terms of improving the torque of the rotating electrical machine 10. Further, in order to obtain a desired torque with this configuration, it is necessary to flow a large stator current through the stator windings 20u, 20v, and 20w, and the copper loss of the stator windings 20u, 20v, and 20w increases, and the efficiency decreases. It is also a cause. According to the present invention, it is possible to improve the torque and efficiency of the rotating electrical machine 10 without any such inconvenience.

  In addition, since the tips of the auxiliary salient poles 44 are located on the radially outer side of the rotor 14 with respect to the roots of the auxiliary salient poles 44, magnetic fluxes that require spatial harmonics according to the tip positions of the auxiliary salient poles 44. The components can be efficiently guided from the auxiliary salient poles 44 to the main salient poles 26 so that a large amount of magnetic flux can be efficiently linked to the rotor windings 28n and 28s, and the torque and efficiency can be improved more effectively.

  Further, the two auxiliary salient poles 44 that are coupled to the circumferential side surfaces of the two main salient poles 26 adjacent to each other in the circumferential direction and are opposed to each other in the circumferential direction are not coupled to each other. The magnetic flux that does not contribute to the torque can be suppressed from flowing to the pole 26, the torque can be improved, and the common windings 32, 36 of the rotor windings 28n, 28s can be provided inside the auxiliary salient pole 44 in the radial direction of the rotor 14. Easy to place.

  On the other hand, unlike the present embodiment, the two auxiliary salient poles 44 coupled to the circumferential side surfaces facing each other can be connected to each other in the rotor slot 46. In this case, for example, Of the rotor 14, the main salient pole 26 that becomes the N pole, the auxiliary salient pole 44 that is coupled to the main salient pole 26, and another salient pole 44 that is coupled to the auxiliary salient pole 44 from the rotor core 24 that is off the main salient pole 26. There is a possibility that the auxiliary salient pole 44, the main salient pole 26, which is the S pole to which this other auxiliary salient pole 44 is coupled, and the magnetic circuit in which the magnetic flux flows in sequence in the rotor core 24 and loops. In this case, this looping magnetic circuit does not contribute to torque. Further, since the magnetic flux flows through the looped magnetic circuit, it flows to the tip of the main salient pole 26, and the magnetic flux contributing to the torque tends to decrease. For this reason, as in the present embodiment, the two auxiliary salient poles 44 coupled to the circumferential side surfaces facing each other are not connected to each other in the rotor slot 46 to improve torque. From the standpoint of this, it is preferable.

  Further, when the tip ends of the two auxiliary salient poles 44 coupled to the circumferential side surfaces of the main salient poles 26 facing each other in the circumferential direction of the rotor 14 are connected to each other in the rotor slot 46, the diameter of the rotor 14 is increased. Although it becomes difficult to dispose the rotor windings 28n and 28s inside the auxiliary salient pole 44 with respect to the direction, this embodiment can eliminate such inconvenience.

  Further, each auxiliary salient pole 44 protrudes in a direction inclined with respect to the circumferential direction so as to be radially outward of the rotor 14 toward the tip side on the circumferential side surface of each main salient pole 26. For this reason, without excessively increasing the length of each auxiliary salient pole 44, a magnetic flux component required for spatial harmonics, for example, a spatial second harmonic component having a high magnetic flux density is transferred from the auxiliary salient pole 44 to the main salient pole 26. Thus, a large amount of magnetic flux can be efficiently linked to the rotor windings 28n and 28s, and the torque and efficiency can be improved more effectively.

  Further, in the present embodiment, the width θ in the circumferential direction of the rotor 14 is regulated in each rotor winding 28n, 28s as described in the above equation (1). For this reason, the induced electromotive force due to the spatial harmonics of the rotating magnetic field generated in the rotor windings 28n and 28s can be increased. That is, the amplitude (variation width) of the interlinkage magnetic flux to the rotor windings 28n and 28s due to the spatial harmonics is affected by the width θ of the rotor windings 28n and 28s in the circumferential direction. Here, FIG. 7 shows a result of calculating the amplitude (variation width) of the interlinkage magnetic flux to the rotor windings 28n and 28s while changing the width θ of the rotor windings 28n and 28s in the circumferential direction. In FIG. 7, the coil width θ is shown in terms of electrical angle. As shown in FIG. 7, the fluctuation width of the linkage flux to the rotor windings 28n and 28s increases as the coil width θ decreases from 180 °, so the coil width θ is made smaller than 180 °. By setting the rotor windings 28n and 28s to short-pitch windings, it is possible to increase the amplitude of the interlinkage magnetic flux due to spatial harmonics compared to full-pitch windings.

  Therefore, in the rotating electrical machine 10 (FIG. 1), the width of each main salient pole 26 in the circumferential direction is made smaller than the width corresponding to 180 ° in electrical angle, and the rotor windings 28 n and 28 s are shorted to each main salient pole 26. By winding with the node winding, the induced electromotive force due to the spatial harmonics generated in the rotor windings 28n and 28s can be efficiently increased. As a result, the torque acting on the rotor 14 can be increased efficiently.

  Furthermore, as shown in FIG. 7, when the coil width θ is 90 °, the amplitude of the interlinkage magnetic flux due to the spatial harmonics is maximized. Therefore, in order to further increase the amplitude of the interlinkage magnetic flux to the rotor windings 28n and 28s due to the spatial harmonics, the width θ of each rotor winding 28n and 28s in the circumferential direction is 90 ° in terms of the electrical angle of the rotor 14. It is preferably equal (or nearly equal) to the corresponding width. Therefore, when the number of pole pairs of the rotor 14 is p and the distance from the rotation center axis of the rotor 14 to the rotor windings 28n, 28s is r, the width θ of each rotor winding 28n, 28s in the circumferential direction is It is preferable that the following expression (2) is satisfied (or substantially satisfied).

  θ = π × r / (2 × p) (2)

  By doing so, the induced electromotive force due to the spatial harmonics generated in the rotor windings 28n and 28s can be maximized, and the magnetic flux generated in each main salient pole 26 by the induced current can be increased most efficiently. Can do. As a result, the torque acting on the rotor 14 can be increased more efficiently. That is, when the width θ greatly exceeds the width corresponding to 90 °, the magnetomotive forces in the direction of canceling each other easily interlink with the rotor windings 28n and 28s, but smaller than the width corresponding to 90 °. Therefore, the possibility becomes low. However, when the width θ is greatly reduced from a width corresponding to 90 °, the magnitude of the magnetomotive force linked to the rotor windings 28n and 28s is greatly reduced. For this reason, such inconvenience can be prevented by setting the width θ to a width corresponding to about 90 °. For this reason, it is preferable that the width θ of each rotor winding 28n, 28s in the circumferential direction is substantially equal to a width corresponding to 90 ° in electrical angle.

  In the rotating electrical machine 10, the torque of the rotor 14 can also be controlled by controlling the current advance angle with respect to the rotor position, which is the phase of the alternating current that flows through the stator windings 20u, 20v, and 20w. Furthermore, the torque of the rotor 14 can also be controlled by controlling the amplitude of the alternating current flowing through the stator windings 20u, 20v, 20w. Further, since the torque of the rotor 14 changes even when the rotation speed of the rotor 14 is changed, the torque of the rotor 14 can be controlled by controlling the rotation speed of the rotor 14.

  Next, simulation results of magnetic flux lines of space harmonics of the rotating electrical machine will be described in the comparative example and the present embodiment with reference to FIGS. 8 and 9. 8 and 9 are schematic diagrams showing magnetic flux lines of spatial harmonics, respectively. FIG. 8 shows the case of the comparative example, and FIG. 9 shows the case of the embodiment shown in FIGS. Each is shown. In the comparative example shown in FIG. 8, the auxiliary salient poles 44 are omitted in the rotating electrical machine 10 of the embodiment shown in FIGS. 8 and 9, the phase relationship between the rotor 14 and the stator 12 is the same. In this case, a part in the circumferential direction of the teeth 18 of the stator 12 and a part in the circumferential direction of the main salient pole 26 of the rotor 14 are opposed to each other in the radial direction.

  As is clear from this simulation result, in the present embodiment shown in FIG. 9 where the auxiliary salient poles 44 are provided, the magnetic flux lines of spatial harmonics are supplemented compared to the comparative example of FIG. It can be seen that there are many interlinkages with the induction windings 30 and 34 while passing through the salient poles 44.

  In the configuration shown in FIG. 4 and FIG. 5A described above, the two main salient poles 26 adjacent in the circumferential direction of the rotor 14 are regarded as one set, and each set is wound around one main salient pole 26. One end of one induction winding 30 and one end of a second induction winding 34 wound around another main salient pole 26 are connected via a first diode 38 and a second diode 40 which are two rectifier elements. Explained when to do. However, in this embodiment, it can also be configured as shown in FIG. 5B. FIG. 5B is a diagram corresponding to FIG. 5A, showing another example in which the number of diodes connected to the rotor winding is reduced. In another example shown in FIG. 5B, in the present embodiment, a plurality of first induction windings 30 wound around the distal end side of every other main salient pole 26 (see FIG. 3) in the circumferential direction that becomes the north pole of the rotor. Are connected in series to form a first induction winding set 86, and a plurality of second induction windings 34 wound around the tip end of every other main salient pole 26 in the circumferential direction that becomes the S pole of the rotor. Are connected in series to form a second induction winding set 88. One end of the first induction winding set 86 and the second induction winding set 88 is connected at the connection point R via the first diode 38 and the second diode 40 whose forward directions are opposite to each other.

  Further, as shown in FIG. 5B, when the two main salient poles 26 (see FIG. 3) of the N pole and the S pole adjacent to each other in the circumferential direction of the rotor are set as one set, the first common winding 32 in each set. The second common windings 36 are connected in series to form a common winding set 42, and all the common winding sets 42 related to all the main salient poles 26 are connected in series. Furthermore, among the plurality of common winding sets 42 connected in series, one end of the first common winding 32 of one common winding set 42 serving as one end is connected to the connection point R, and another common winding serving as the other end is connected. One end of the second common winding 36 of the wire set 42 is connected to the other end opposite to the connection point R of the first induction winding set 86 and the second induction winding set 88. In such a configuration, unlike the configurations shown in FIGS. 4 and 5A described above, the total number of diodes provided in the rotor can be reduced to two, that is, the first diode 38 and the second diode 40. Even in this case, auxiliary salient poles 44 (see FIG. 3) are formed on the side surfaces of the respective main salient poles 26, and the induction windings 30, 34 are respectively provided in the radially outer and radially inner spaces partitioned by the auxiliary salient poles 44. And common windings 32 and 36 can be arranged.

  In the embodiment shown in FIGS. 1 to 7 described above, the case where the induction windings 30 and 34 of the rotor windings 28n and 28s and the common windings 32 and 36 are entirely wound around the main salient pole 26 is described. did. However, the rotor has an annular core made of a magnetic material, a main salient pole made of magnetic material provided at a plurality of locations in the circumferential direction of the annular core, and an auxiliary salient pole having magnetism protruding from the circumferential side surface of the main salient pole. In addition, in the configuration in which the rotor induction winding is wound radially outward from the auxiliary salient pole of each main salient pole, the configuration is a toroidal winding in which the rotor common winding is wound around the annular core that is out of the main salient pole. Can also be adopted.

  Next, FIG. 10 is a view corresponding to FIG. 2 and showing a first example of another example of the auxiliary salient pole 44 in the rotating electrical machine according to another embodiment of the present invention. In the configuration shown in FIG. 10, the auxiliary salient poles 44 are coupled so as to project in the circumferential direction from both circumferential side surfaces of the main salient poles 26, and are substantially perpendicular so as to go radially outward at the middle portion in the length direction. It is bent. That is, in the auxiliary salient pole 44, the distal end side plate portion 76 in the radial direction is coupled to the root side plate portion 74 in the circumferential direction. For this reason, the tip side portion of each auxiliary salient pole 44 extends in the substantially radial direction of the rotor 14. Further, the tip side portion of each auxiliary salient pole 44 and the main salient pole 26 are arranged in parallel. In addition, the front end side portion of each main salient pole 26 can be coupled to the root side portion at an obtuse angle. For example, the tip side portion of each main salient pole 26 may be provided in the radial direction facing the center of the rotor 14.

  In the configuration shown in FIG. 10, unlike the configuration shown in FIG. 2, the total cross-sectional area of the induction winding 30 (34) arranged on the radially outer side of the auxiliary salient pole 44 can be increased. For this reason, it becomes easy to arrange many rotor windings 28n (28s) outside the auxiliary salient poles 44 in the radial direction of the rotor 14. Other configurations and operations are the same as those of the embodiment shown in FIGS.

  Next, FIG. 11 is an enlarged view corresponding to part B of FIG. 2, showing a second example of another example of the auxiliary salient pole 44 in a rotating electrical machine according to another embodiment of the present invention. In the configuration shown in FIG. 11, in the embodiment shown in FIGS. 1 to 7, the wide tip portion 62 whose width in the circumferential direction increases toward the tip at the tip of each auxiliary salient pole 44 is provided. . That is, each auxiliary salient pole 44 has a wide tip portion 62, and the width of the wide tip portion 62 in the circumferential direction increases toward the outer side in the radial direction of the rotor 14. The front end surface P of the wide front end 62 facing the stator 12 is a curved surface along the circumferential direction of the annular gap space 64 between the stator 12 and the rotor 14 or a flat surface in contact with the curved surface. According to such a configuration, a magnetic flux component necessary for spatial harmonics from the stator 12, for example, a spatial secondary harmonic component, without increasing the width in the circumferential direction of each auxiliary salient pole 44 as a whole. Can be efficiently guided from the auxiliary salient pole 44 to the main salient pole 26. For this reason, the magnetic flux component necessary for the spatial harmonics from the stator 12 is passed through the auxiliary salient pole 44 or the main salient pole 26 without excessively reducing the arrangement space of the rotor windings 28n (28s). A large amount of magnetic flux can be efficiently linked to the rotor winding 28n (28s) by efficiently inducing the pole 44. As a result, the torque and efficiency of the rotating electrical machine 10 can be effectively improved. Other configurations and operations are the same as those of the embodiment shown in FIGS.

  FIG. 12 is an enlarged view corresponding to part B of FIG. 2, showing a third example of another example of the auxiliary salient pole 44 in the rotating electrical machine according to another embodiment of the present invention. In the configuration shown in FIG. 12, not only the tip portion of the auxiliary salient pole 44 but also the intermediate portion has a larger width in the circumferential direction. That is, the width of the auxiliary salient pole 44 in the circumferential direction is gradually increased from the root portion toward the tip. Further, a wide tip portion 66 is provided at the tip portion of the auxiliary salient pole 44 so that the width in the circumferential direction increases toward the radially outer side of the rotor 14. In the case of such a configuration, similarly to the configuration shown in FIG. 11 described above, a necessary magnetic flux component of spatial harmonics is generated from the stator 12 without excessively reducing the arrangement space of the rotor windings 28n (28s). The torque and efficiency of the rotating electrical machine 10 can be effectively improved by efficiently guiding the main salient pole 26 or the auxiliary salient pole 44 through the auxiliary salient pole 44 or the main salient pole 26. Other configurations and operations are the same as those of the embodiment shown in FIGS. 1 to 7 or the configuration shown in FIG.

  FIG. 13 is an enlarged view corresponding to part B of FIG. 2 showing a fourth example of another example of the auxiliary salient pole 44 in the rotating electrical machine according to another embodiment of the present invention. As in the configuration shown in FIG. 13, the auxiliary salient pole 44 has the tip end surface P between the stator 12 and the rotor 14 even when the circumferential width of the tip portion is the same in the entire length direction. It is also possible to use a curved surface along the circumferential direction of the gap space 64 or a flat surface in contact with the curved surface. Other configurations and operations are the same as those of the embodiment shown in FIGS.

  FIG. 14 is a schematic cross-sectional view showing part of the rotor 14 and the stator 12 in the circumferential direction in a rotating electrical machine according to another embodiment of the present invention. FIG. 15 is a schematic diagram showing how the magnetic flux generated by the induced current flowing in the rotor windings 68n and 68s flows in the rotor 14 in the electromagnet-type rotating electrical machine of FIG. In the embodiment shown in FIGS. 1 to 7 described above, the case where the induction windings 30 and 34 and the common windings 32 and 36 are wound around the main salient poles 26 has been described. However, as shown in FIGS. 14 and 15, the rotor windings 68 n and 68 s wound around each main salient pole 26 are replaced with another rotor winding 68 s wound around another adjacent main salient pole 26. , 68n can be divided. That is, the rotor 14 has a plurality of first rotor windings 68n wound around each other main salient pole 26 in the circumferential direction by concentrated winding, and the main salient pole 26 wound with the first rotor winding 68n. A plurality of second rotor windings 68s are wound in concentrated winding on every other main salient pole 26 in the circumferential direction, which are adjacent main salient poles 26.

  A second rotor winding circuit in which one first diode 38 is connected to a first rotor winding circuit 70 in which a plurality of first rotor windings 68n are connected in series, and a plurality of second rotor windings 68s are connected in series. One second diode 40 is connected to 72. That is, a plurality of first rotor windings 68n arranged every other in the circumferential direction of the rotor 14 are electrically connected in series and connected endlessly, and a first diode is partly disposed therebetween. 38 is connected in series with each first rotor winding 68n to constitute a first rotor winding circuit 70. Each first rotor winding 68n is wound around a main salient pole 26 that functions as the same magnetic pole (N pole).

  The plurality of second rotor windings 68s are electrically connected in series and are connected in an endless manner, and a second diode 40 is connected in series with each of the second rotor windings 68s in part between them. Thus, a second rotor winding circuit 72 is configured. Each second rotor winding 68s is wound around the main salient pole 26 that functions as the same magnetic pole (S pole). Further, the rotor windings 68n and 68s wound around the main salient poles 26 adjacent to each other in the circumferential direction (where magnets having different magnetic poles are formed) are electrically separated from each other.

  Also, the current rectification directions of the rotor windings 68n and 68s by the diodes 38 and 40 are reversed so that the main salient poles 26 adjacent to each other in the circumferential direction of the rotor 14 have different magnetic poles. Yes. That is, the direction of current flowing in the first rotor winding 68n and the second rotor winding 68s arranged adjacent to each other in the circumferential direction (rectification direction by the diodes 38 and 40), that is, the forward direction is opposite to each other. The diodes 38 and 40 are connected to the rotor windings 68n and 68s. The diodes 38 and 40 are connected to the rotor windings 68n and 68s in opposite directions.

  Further, the winding central axis of each rotor winding 68n, 68s coincides with the radial direction. The diodes 38 and 40 rectify the current flowing through the corresponding rotor windings 68n and 68s by the generation of the induced electromotive force due to the rotating magnetic field including the spatial harmonics generated by the stator 12, so that the circumference of the rotor 14 is increased. The phases of the currents flowing through the rotor windings 68n and 68s adjacent in the direction are alternately changed between the A phase and the B phase. The diodes 38 and 40 independently rectify the current flowing through the corresponding rotor windings 68n and 68s by the generation of the induced electromotive force, and generate a plurality of circumferential directions generated by the current flowing through the rotor windings 68n and 68s. The magnetic characteristics of the main salient poles 26 are alternately changed in the circumferential direction. In this configuration, the number of diodes 38 and 40 can be reduced to two as a whole, and the winding structure of the rotor 14 can be simplified.

  Further, the auxiliary salient poles 44 are protruded on both side surfaces of the main salient poles 26 in the circumferential direction, and the rotor windings 68n and 68s wound around the main salient poles 26 by the auxiliary salient poles 44 are divided into the tip side and the root side. However, the tip ends and the root sides of the rotor windings 68n and 68s are connected in series. In the example shown in the figure, the auxiliary salient pole 44 is formed so as to protrude from the circumferential side surface of the main salient pole 26 in a direction inclined with respect to the circumferential direction. However, as in the configuration shown in FIG. The salient poles 44 may be formed so as to protrude in the circumferential direction on both sides in the circumferential direction and bend in the radial direction at the intermediate portion. Further, as in the configuration shown in FIGS. 11 and 12, the circumferential width of the tip of the auxiliary salient pole 44 can be increased. In the case of the configuration shown in FIGS. 14 and 15 as well, the spatial harmonics contained in the rotating magnetic field generated by the stator 12 are interlinked with the rotor windings 68n and 68s so as to improve the torque and efficiency of the rotating electrical machine 10. can do. Other configurations and operations are the same as those shown in FIGS.

  Further, as shown in FIG. 16, the first diode 38 or the second diode 40 can be short-circuited for each of the rotor windings 68n and 68s wound around the main salient poles 26, respectively. . Other configurations and operations are the same as the configurations shown in FIGS. 1 to 7 or the configurations shown in FIGS.

  Although illustration is omitted, in the rotating electrical machine drive system 50 shown in FIG. 6 described above, the pulse current is periodically superimposed on the q-axis current or the d-axis current of the rotating electrical machine 10 to further increase the speed of the rotating electrical machine 10. Torque can also be increased. When superimposing the pulse current on the q-axis current, it is preferable to superimpose a decreasing pulse current that increases after decreasing in a pulse shape from the viewpoint of miniaturization of the inverter 52 and the like. When superimposing a pulse current on a d-axis current, it is preferable from the aspect of torque increase to superimpose an increasing pulse current that increases after increasing in a pulse shape. The increasing pulse current can be superimposed on the d-axis current, and at the same time the decreasing pulse current can be superimposed on the q-axis current. The d-axis refers to the magnetic pole direction that is the winding central axis direction of the rotor windings 28n, 28s (or 68n, 68s) with respect to the circumferential direction of the rotating electrical machine 10, and the q-axis is an electrical angle with respect to the d-axis. The direction advanced 90 degrees. For example, when the rotation direction of the rotor 14 is defined as shown in FIGS. 1 and 14, the d-axis direction and the q-axis direction are defined by the relationships shown by arrows in FIGS. The

  As mentioned above, although the form for implementing this invention was demonstrated, this invention is not limited to such embodiment at all, and it can implement with a various form in the range which does not deviate from the summary of this invention. Of course. For example, in the above description, the case where the rotor is disposed opposite to the inner side in the radial direction of the stator has been described. However, the present invention can be implemented even in a configuration in which the rotor is disposed opposite to the outer side in the radial direction of the stator. In addition, the case where the stator winding is wound on the stator by concentrated winding has been described, but for example, if the stator can generate a rotating magnetic field including spatial harmonics, the stator winding may be wound on the stator by distributed winding. The present invention can be implemented. In each of the above embodiments, the case where the magnetic characteristic adjusting unit is a diode has been described. However, the function of varying the magnetic characteristics generated in the plurality of main salient poles in the circumferential direction by the induced electromotive force generated in the rotor windings. Any other configuration can be adopted as long as it has the following. In the present invention, for example, a configuration such as an axial gap type rotating electrical machine can be employed.

  DESCRIPTION OF SYMBOLS 10 Electromagnet-type rotary electric machine, 12 Stator, 14 Rotor, 16 Stator core, 18 Teeth, 20u, 20v, 20w Stator winding, 22 Status lot, 24 Rotor core, 26 Main salient pole, 28n 1st rotor winding, 28s 2nd rotor Winding, 30 First induction winding, 32 First common winding, 34 Second induction winding, 36 Second common winding, 38 First diode, 40 Second diode, 42 Common winding set, 44 Auxiliary bump Pole, 46 rotor slot, 48 collar, 50 rotating electrical machine drive system, 52 inverter, 54 control device, 56 power storage device, 58 capacitor, 60 current sensor, 62 wide tip, 64 gap space, 66 wide tip, 68n, 68s rotor winding, 70 first rotor winding circuit, 72 second rotor winding circuit, 74 root side plate Part, 76 tip side plate part, 86 1st induction winding group, 88 2nd induction winding group.

Claims (9)

An electromagnet type rotating electrical machine in which a stator and a rotor are arranged to face each other,
The stator includes a stator core, teeth disposed at a plurality of positions in the circumferential direction of the stator core, and at least a plurality of stator windings wound around the stator core or the teeth to generate a rotating magnetic field,
The rotor is generated in a rotor core, main salient poles arranged at a plurality of locations in the circumferential direction of the rotor core, a plurality of rotor windings wound at least partially on the main salient poles, and the rotor windings. A magnetic property adjusting unit that alternately changes the magnetic properties generated in the plurality of main salient poles by the induced electromotive force in the circumferential direction,
Further, the rotor includes an auxiliary salient pole that protrudes from a circumferential side surface of each main salient pole and has magnetism.   Each of the rotor windings is connected to a rectifying element that is the magnetic characteristic adjusting unit, and the rectifying element is adjacent to the circumferential direction by rectifying a current flowing through the rotor winding by generating an induced electromotive force. An electromagnet-type rotating electrical machine characterized in that the phase of the current flowing through the rotor winding is alternately changed between the A phase and the B phase. In the electromagnet-type rotating electrical machine according to claim 1 or 2,
The electromagnet-type rotating electrical machine characterized in that the tip of the auxiliary salient pole is located on the radially outer side of the rotor with respect to the base of the auxiliary salient pole. The electromagnet-type rotating electrical machine according to any one of claims 1 to 3,
The auxiliary salient pole is provided on each side surface in the circumferential direction of each main salient pole so as to protrude in the circumferential direction or in a direction inclined with respect to the circumferential direction, respectively. In the electromagnet type rotating electrical machine according to claim 4,
An electromagnet rotation characterized in that two auxiliary salient poles connected to circumferential side surfaces of two main salient poles adjacent to each other in the circumferential direction are not coupled to each other. Electric. The electromagnet-type rotating electrical machine according to claim 5,
The electromagnet-type rotating electrical machine characterized in that the auxiliary salient pole protrudes on the circumferential side surface of the main salient pole in a direction inclined with respect to the circumferential direction so as to be radially outward of the rotor toward the tip. The electromagnet-type rotating electrical machine according to claim 5,
The auxiliary salient pole is coupled so as to project from the circumferential side surface of the main salient pole in the circumferential direction, and is bent so as to be radially outward at an intermediate portion. In the electromagnet type rotating electrical machine according to claim 6 or 7,
The electromagnet-type rotating electrical machine, wherein the auxiliary salient pole has a tip portion whose width in the circumferential direction increases toward the radially outer side of the rotor. The electromagnet-type rotating electrical machine according to any one of claims 1 to 8,
The width of each rotor winding in the circumferential direction of the rotor is shorter than a width corresponding to 180 ° in electrical angle.

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