[go: up one dir, main page]

WO2008035487A1 - Rotor of motor - Google Patents

Rotor of motor Download PDF

Info

Publication number
WO2008035487A1
WO2008035487A1 PCT/JP2007/060498 JP2007060498W WO2008035487A1 WO 2008035487 A1 WO2008035487 A1 WO 2008035487A1 JP 2007060498 W JP2007060498 W JP 2007060498W WO 2008035487 A1 WO2008035487 A1 WO 2008035487A1
Authority
WO
WIPO (PCT)
Prior art keywords
rotor
magnet
electric motor
magnetic flux
magnets
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Ceased
Application number
PCT/JP2007/060498
Other languages
French (fr)
Japanese (ja)
Inventor
Tsutomu Tanimoto
Masaki Nakano
Masahiro Tsukamoto
Tadayuki Hatsuda
Tetsuya Niikuni
Yasuhiro Yanagihara
Hiroshi Takashima
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Nissan Motor Co Ltd
Original Assignee
Nissan Motor Co Ltd
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Priority claimed from JP2006252688A external-priority patent/JP2007174885A/en
Priority claimed from JP2006253946A external-priority patent/JP2008079393A/en
Application filed by Nissan Motor Co Ltd filed Critical Nissan Motor Co Ltd
Publication of WO2008035487A1 publication Critical patent/WO2008035487A1/en
Anticipated expiration legal-status Critical
Ceased legal-status Critical Current

Links

Classifications

    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02KDYNAMO-ELECTRIC MACHINES
    • H02K1/00Details of the magnetic circuit
    • H02K1/06Details of the magnetic circuit characterised by the shape, form or construction
    • H02K1/22Rotating parts of the magnetic circuit
    • H02K1/27Rotor cores with permanent magnets
    • H02K1/2706Inner rotors
    • H02K1/272Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis
    • H02K1/274Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis the rotor consisting of two or more circumferentially positioned magnets
    • H02K1/2753Inner rotors the magnetisation axis of the magnets being perpendicular to the rotor axis the rotor consisting of two or more circumferentially positioned magnets the rotor consisting of magnets or groups of magnets arranged with alternating polarity
    • H02K1/278Surface mounted magnets; Inset magnets

Definitions

  • the present invention relates to a rotor of an electric motor.
  • the present invention it is possible to independently rotate two rotors by feeding one composite current, which is a composite of currents corresponding to two rotors, to one stator, It is possible to generate two separate output 'torques with one motor body, and the average value of the current applied to the stator for both rotors simply gives the current to the two motors. There is an effect that the loss due to the current lower than the average value is reduced.
  • the electric motor in the above-described invention assumes that the output destination is only a tire (wheel), for example, in the case of a wheel-in motor in which the electric motor is mounted inside the tire in an automobile or the like. Therefore, two output shafts are unnecessary and redundant. There are also problems such as the need for a mechanism that combines two output shafts into a single shaft. When two separate motors are combined and the torque of two motors is mechanically combined, two motors Since there is a housing, it cannot be downsized. In addition, simply increasing the size of a “normal conventional motor” to increase the motor torque has problems such as an increase in the motor housing and an increase in current loss. That is, there is a demand for the development of a rotor for a rotating electric machine that has a smaller current loss and is further miniaturized.
  • the present invention integrates a plurality of rotors (a plurality of magnets included therein) having a different number of pole pairs into a single physique.
  • a motor rotor that is reduced in size and has low current loss.
  • the rotor of the electric motor of the present invention that solves the above-described problems is obtained by adding together a plurality of magnet magnetic fluxes corresponding to a plurality of magnet sets each having a different number of magnetic poles.
  • the place where this is done (referred to as the flux noria part) is characterized in that a low-flux magnet is placed or the magnet is removed so that the amount of magnetic flux is reduced compared to the place where the magnetic flux is not canceled.
  • a magnet magnetized so that the magnetic flux is concentrated in a portion where the magnetic flux is increased by the addition of the magnetic flux of the magnetic flux tl is arranged in the space from which the magnet that solves the above-described problems is removed.
  • the magnetic flux concentration effect may be enhanced while effectively using the space where the magnet is removed.
  • the rotor of the electric motor generates magnetic flux that generates a magnetic flux equivalent to a magnet magnetic flux obtained by adding together the magnetic fluxes of a plurality of magnet sets each having a different number of magnetic poles.
  • the member is a member that generates a magnetic flux corresponding to the combined magnetic flux so as to superimpose and cancel the magnet magnetic flux of the set of the plurality of magnets, and the portion where the magnetic flux is canceled is compared with the portion where the magnetic flux is not canceled.
  • a low-flux magnet is arranged or the magnet is removed to reduce the amount of magnetic flux.
  • the rotor of the electric motor of the second invention has two sets of the plurality of magnets, and the magnetic flux of the number of magnetic pole components of each set (that is, the arrangement of the magnets constituting each set) is predetermined. The phase difference is provided.
  • the predetermined phase difference energizes a stator winding constituting the electric motor (based on a combination of the number of magnetic poles of the plurality of magnet sets).
  • the absolute peak value of the winding current is set to be minimum.
  • the predetermined phase difference energizes a stator winding constituting the electric motor (based on a combination of the number of magnetic poles of the plurality of magnet sets). It is characterized in that the average value of the absolute value of the winding current is set to be minimum.
  • the predetermined phase difference energizes the stator windings constituting the electric motor (based on the combination of the number of magnetic poles of the plurality of magnet sets).
  • the effective value of the winding current is set to be a minimum.
  • the predetermined phase difference is based on the two magnet magnetic fluxes (based on the combination of the number of magnetic poles of the plurality of magnet sets) corresponding to the two sets of magnets. It is characterized in that the peak value of the magnetic flux summing up is set to be the minimum.
  • the predetermined phase difference constitutes the electric motor when the rotor rotates (based on a combination of the number of magnetic poles of the plurality of magnet sets). It is characterized in that it is set so that the peak value of the induced voltage generated in the stator winding is minimized.
  • the magnetic flux generating member (that is, the magnet constituting the set of the plurality of magnets in this member) is at least one set of the set of the plurality of magnets.
  • the corresponding magnet magnetic flux is formed so as to be distributed in a sinusoidal shape in the circumferential direction of the rotor.
  • the surface shape of at least one of the plurality of magnet sets facing the stator constituting the electric motor (that is, when cut by a plane perpendicular to the axis of the electric motor)
  • a magnet set that assumes that the cross-sectional shape is an arc shape whose diameter is smaller than the radius from the rotor axis for each magnetic pole with respect to the circumferential direction of the rotor.
  • the magnetic flux generating member is a permanent magnet
  • the permanent magnet is constituted by a first permanent magnet and a second permanent magnet
  • the second The magnet characteristics with respect to the temperature change of the second permanent magnet are more stable than those of the second permanent magnet (i.e., the magnet characteristic change with respect to the temperature change of the second permanent magnet is more stable than that of the first permanent magnet). Small).
  • the set of the plurality of magnets includes a first magnet set having a low magnetic pole number and a second magnet set having a high magnetic pole number,
  • the magnets constituting the first magnet set (low magnetic pole number) and the second magnet set (high magnetic pole number) are arranged so that the magnetic flux of the first set of magnets (low magnetic pole component) is strengthened when canceling out the magnets constituting the.
  • the set of the plurality of magnets includes a first magnet set having a low magnetic pole number and a second magnet set having a high magnetic pole number,
  • the magnets constituting the first magnet set (low magnetic pole number) and the second magnet set (high magnetic pole number) are arranged so that the magnetic fluxes of the magnets constituting the second set of magnets (high magnetic pole component) are strengthened when the magnets constituting the are canceled.
  • the magnetic flux generating member is composed of a plurality of permanent magnets, and the circumferential length (as viewed from the rotor center) of the plurality of permanent magnets is All the same 1 (the magnet pitch of the permanent magnets is the same for all magnets).
  • the magnetic flux generating member is composed of a plurality of permanent magnets, and the circumferential length (as viewed from the rotor center) of the plurality of permanent magnets is It differs depending on the magnet (the magnet pitch of the permanent magnet is configured with a different length depending on the magnet).
  • the magnetic flux generating member is composed of a plurality of permanent magnets, and the thickness of the plurality of permanent magnets (as viewed from the rotor center) in the radial direction is It is characterized by being different depending on the magnet (that is, the magnet thickness in the radial direction varies depending on the magnet).
  • the rotor of the electric motor according to the eighteenth aspect of the present invention is the rotation of an electric motor in which magnets magnetized so that the magnetic flux is concentrated on the portion where the magnetic flux is increased tl by the addition of the magnetic flux to the portion where the magnet is removed. Characterized by a child.
  • the rotor of the electric motor according to the nineteenth aspect of the invention is characterized in that one or more magnets magnetized so that the magnetic flux is concentrated on the portion where the magnetic flux is increased tl by the sum of the magnetic flux at the portion where the magnet is removed. It features a motor rotor that is arranged so that the magnetic flux is concentrated depending on the magnetic direction.
  • the rotor of the electric motor of the twentieth invention is characterized in that the magnetized magnet is a rotor of the electric motor such that the magnetic flux is concentrated by the installation angle of one or more magnets.
  • the rotor of the electric motor of the twenty-first invention is characterized in that the magnetized magnet is a rotor of the electric motor in which the magnetic flux is concentrated by combining two or more vectors.
  • the rotor of the electric motor of the twenty-second invention is an electric motor rotor in which the magnetized magnet concentrates the magnetic flux by one or more magnets and one or more flux noria.
  • the solving means of the present invention has been described as an apparatus, but the present invention can also be realized as a method substantially corresponding to these, and the scope of the present invention includes these as well. It was understood that
  • FIG. 1 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a first embodiment of the present invention.
  • FIG. 3 is a diagram showing an example of a composite state of two sine waves.
  • FIG. 5 is a cross-sectional view showing a configuration of an electric motor using the rotor according to the first embodiment of the present invention.
  • FIG. 6 is an explanatory diagram of a rotor according to a second embodiment.
  • FIG. 7 is an explanatory diagram of changes in the peak value of the magnetic flux in the second embodiment.
  • FIG. 8 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a third embodiment of the present invention.
  • FIG. 10 is an explanatory diagram of changes in the induced voltage peak value in the third embodiment.
  • FIG. 11 is a cross-sectional view showing a configuration of an electric motor using a rotor (modified example) according to a third embodiment.
  • FIG. 13 A sectional view showing the configuration of an electric motor using a rotor according to a fourth embodiment of the present invention.
  • FIG. 15 A sectional view showing the configuration of an electric motor using a rotor according to a fifth embodiment of the present invention.
  • FIG. 16 is an explanatory diagram of a rotor according to a fifth embodiment.
  • FIG. 17 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a sixth embodiment of the present invention.
  • FIG. 18 is a diagram showing a linear arrangement of a magnet arrangement in which a magnet with a high magnetic pole number (4 poles) (virtual rotor) is combined with a magnet region with a low magnetic pole number (2 poles) and an electrical angle of one cycle.
  • FIG. 19 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a seventh embodiment of the present invention.
  • FIG. 21 is a view showing only the mechanical angle 120 degrees of the rotor of FIG. 17 (an example in which the width is changed).
  • FIG. 22 is a view showing only the mechanical angle 120 degrees of the rotor of FIG. 17 (example in which the thickness is changed).
  • FIG. 23 is a cross sectional explanatory view schematically showing a configuration of a rotor and a stator of an electric motor according to an eighth embodiment of the present invention.
  • FIG. 24 is a cross-sectional explanatory view showing an example of another magnetization direction in the magnet of FIG.
  • FIG. 25 is a cross-sectional explanatory view schematically showing a configuration of a rotor and a stator of a motor having a four-pole pair of rotors in a 12-slot stator.
  • FIG. 26 is an explanatory cross-sectional view schematically showing a configuration of a rotor and a stator of a motor having an 8-pole rotor in a 12-slot stator.
  • FIG. 29 schematically shows a configuration of a rotor and a stator of an electric motor according to a tenth embodiment of the present invention, in which (a) is a cross-sectional explanatory diagram when magnets are arranged on the surface, and (b) is a diagram illustrating magnets.
  • FIG. 6 is a cross-sectional explanatory diagram when embedded.
  • FIG. 30 schematically shows a configuration of a rotor and a stator of an electric motor according to an eleventh embodiment of the present invention.
  • A is a cross-sectional explanatory view when the magnet is arranged on the surface.
  • B is a diagram illustrating the magnet.
  • FIG. 6 is a cross-sectional explanatory diagram when embedded.
  • FIG. 1 is a cross-sectional view showing the configuration of an electric motor using a rotor according to a first embodiment of the present invention.
  • Reference numeral 11 denotes a stator, which is composed of 18 divided cores 12, and each of the 18 divided cores 12 is wound with winding wires 13 in a concentrated manner.
  • 3 pieces arranged every 6 pieces are 1 set (total 6 sets) Connected in series or in parallel, one of which is connected to one of the other phases as a neutral point
  • the other is inside an inverter (not shown), and is connected to the P side / ⁇ side of the power supply line via a switching element.
  • This inverter is configured to control 6 phases. Note that this stator can be applied to the same operating force S even with a core that is not divided by the force described by the divided core, or the present invention can be applied to a slotless motor. Also, the shoreline is applicable not only to concentrated winding but also to distributed ridges.
  • the rotor 14 is a rotor, and in this embodiment, the rotor 14 includes three negative pole magnets N1 to N3 and six negative pole magnets S1 to S6, and these magnets are connected to a three pole pair. It functions as two sets of magnets with two types of pole pairs, six pole pairs.
  • the two sets of magnets in this case are conceptual and have three poles for one current that makes up the combined current supplied to the stator windings that are not clearly separated. Means that there is one set of magnets that behave as a set of pairs of magnets, and one set of magnets that behaves as a set of six pole pairs for the other current that makes up the composite current
  • the magnets S1 to S6 and Nl to 3 function as both sets of magnets at the same time.
  • FIG. 2 is an explanatory diagram of the rotor generation of the first embodiment.
  • (A) in FIG. 2 is a rotor of an electric motor having a two-rotor structure.
  • the rotor has 6 pole pairs of magnets.
  • FIG. 2B shows the magnets arranged in two layers on the surface of the inner rotor. A slight phase adjustment is made at the time of arrangement, and the details will be described later.
  • the rotor 14A has two types of magnets (N pole and S pole) with different magnetization directions in contact with each other at several positions. As is well known, when magnets with different magnetization directions are bonded together, the magnets are equivalent if they have the same magnetic force.
  • Fig. 2 (C) shows the removal of the partial force magnet with magnets with different magnetizations seen in the radial direction.
  • This rotor 14 has N pole magnets N1 to N3, Includes S-pole magnets S1-S6.
  • N1 to N3 includes S-pole magnets S1-S6.
  • the rotor 14 that generates the composite magnetic flux CF of the three-pole pair and the six-pole pair as shown by a curved line is completed.
  • the inner rotor and outer rotor are integrated.
  • the motor functions. That is, the rotor 14A is a rotor having a configuration in which the first rotor of the inner rotor and the second rotor of the outer rotor are integrated together.
  • the present invention is further directed to the configuration of FIG. 2 (C) in which an unnecessary magnet is removed, which is an improvement to such a configuration, and the torque is improved by reducing the inertia of the deleted magnet. This has the effect of reducing the weight of the motor and reducing the cost of the deleted magnet.
  • the area from which unnecessary magnets are removed is a space, and air occupies the area.
  • the area occupied by air does not pass magnetic flux and functions. Really. That is, it is necessary to place a member other than a material that can easily pass magnetic flux such as iron in this area from which the magnet has been removed, but space (air) is usually sufficient.
  • space air
  • phase difference is used for the purpose of relaxing the magnetic saturation of the magnetic field of the rotor, it is conceivable to apply the above configuration with the phase difference of 0 to the rotor magnet. .
  • phase difference there is an optimum phase difference depending on the purpose as described above, and each is set.
  • a 6-phase inverter is connected to the stator, and it is sufficient if current is applied so as to generate a composite sinusoidal magnetic flux corresponding to the rotor magnetic field of 3 pole pairs and 6 pole pairs. ,.
  • the current command is rotated according to the position of the rotor in the same way as a normal motor.
  • this motor generates a composite magnetic flux corresponding to both pole pairs.
  • a sine wave of 3 cycles is generated. Therefore, the inverter is considered as 6 phases, and the current value at each position obtained by dividing 1 cycle of the sine wave into 6 is calculated as the command value of each phase.
  • a 6-pole pair of magnets generates a 6-cycle sine wave, so the current command value at the position where the 1-cycle sine wave is divided into 3 parts is obtained.
  • the command values for the second and fifth phases and the third and sixth phases are used. After this, the command values of the 3-pole pair and 6-pole pair are added together to perform current control as the command value of the 6-phase inverter. This causes the rotor to generate torque and rotate.
  • Torque is generated by the above operation. Torque is generated by the interaction of field magnetic flux (magnetic flux generated by the rotor) and current magnetic flux (rotating magnetic flux generated by the stator). It is generated according to the fundamental wave component (in this example, 3 pole pair and 6 pole pair). In this example, since the magnetic flux obtained by combining sine waves with amplitude 1 is generated, the fundamental wave component is naturally amplitude 1, so that for an electric motor that is rotated alone with amplitude 1 It is theoretically possible to generate almost twice the torque with a single motor.
  • the fundamental wave component in this example, 3 pole pair and 6 pole pair
  • FIG. 5 is a cross-sectional view showing the configuration of an electric motor using a rotor according to the second embodiment of the present invention.
  • a 12-slot 6-phase stator 21 is combined with a 2-pole / 4-pole pair rotor.
  • the stator 21 has 12 cores 22 and 12 windings 23.
  • the rotor 24 ⁇ in FIG. 6 is equivalent to the rotor 24 in FIG.
  • the magnets provided in the rotor 24 are two negative magnets N21 and N22, and two negative S magnets S21 and S22.
  • Fig. 7 shows the peak values of the magnetic flux of the magnet when the two-pole pair and the four-pole pair of magnetic flux with amplitude 1 are combined and the phase of both is changed as in the first embodiment.
  • FIGS. 8 to 12 are diagrams related to the third embodiment, in which a 2-pole / 6-pole pair rotor is combined with an 18-slot 9-phase stator.
  • FIG. 8 is a cross-sectional view showing the configuration of an electric motor using a rotor according to a third embodiment of the present invention.
  • the stator 31 has 18 cores 32 and 18 windings 33.
  • the rotor 34A in FIG. 9 is equivalent to the rotor 34 in FIG.
  • the magnets provided on the rotor 34 are four N-pole magnets N31 to N34 and four S-pole magnets S21 to S34. Fig.
  • FIG. 10 shows the peak value of the induced voltage when the magnetic flux of amplitude 1 of 2 pole pairs and 6 pole pairs is combined and the phase of both is changed as in the first embodiment. From Fig. 10, the peak value of the induced voltage is maximized when the phase difference between the two is 0 ° (60 °), and the peak value of the induced voltage is minimized when it is 30 ° (90 °). Maximizing the peak value of the induced voltage makes it possible to increase the torque of the motor, and conversely, minimizing the peak value of the induced voltage enables high rotation speed of the motor. For this reason, in FIG.
  • the end of the magnet (the contact portion of the magnets with different magnetic poles), that is, the phase zero point is set to overlap with each other, and the phase difference is set to 0 °.
  • the rotor structure shown in Fig. 8 is obtained through the same process.
  • the end of the magnet is overlapped so that it is 30 °, and the rotor structure of Fig. 11 is obtained.
  • the stator 41 has 18 cores 42 and 18 windings 43.
  • the rotor 44A in FIG. 12 is equivalent to the rotor 44 in FIG.
  • the magnets provided on the rotor 44 are two N-pole magnets N41 N42, S magnets with two S poles, S41 and S42.
  • FIG. 13 and 14 are diagrams related to the fourth embodiment, and the basic configuration is the same as that of FIG. 5 of the second embodiment.
  • FIG. 13 is a cross-sectional view showing the configuration of an electric motor using a rotor according to a fourth embodiment of the present invention.
  • the stator 51 has 12 cores 52 and 12 windings 53.
  • the rotor 54A in FIG. 14 is equivalent to the rotor 54 in FIG.
  • the magnets provided on the rotor 54 are four N-pole magnets N51 to N54 and four S-pole magnets S51 to S54.
  • the difference from the second embodiment is the magnet surface shape.
  • the magnet surface in the second embodiment has a circular arc shape that is concentric with the rotor shaft center.
  • the surface of the 4-pole pair magnet is larger than the radius of the rotor shaft center force as shown in FIG. It has an arc shape with a small diameter.
  • the rotor structure shown in FIG. 13 can be obtained by adding the two-pole / four-pole pairs shown in FIG. 14 through the same process as in Example 1.
  • the magnetic flux corresponding to the 4-pole pair of magnets has a substantially sinusoidal shape, so that unnecessary cogging torque with less harmonic magnetic flux can be reduced.
  • only one of the two magnetic poles can have a sinusoidal shape. Both magnetic poles can have a sinusoidal shape.
  • FIG. 15 and 16 are diagrams relating to the fifth embodiment, and the basic configuration is the same as that of FIG. 5 of the second embodiment.
  • FIG. 15 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a fifth embodiment of the present invention.
  • the stator 61 has twelve cores 62 and twelve winding wires 63.
  • the rotor 64A in FIG. 16 is equivalent to the rotor 64 in FIG.
  • the magnets provided in the rotor 64 are two N-pole magnets N61 and N62, and two S-pole magnets S61 and S62.
  • the difference from the second embodiment is that there is a gap between adjacent magnets.
  • the magnet according to the second embodiment is arranged with no gap between adjacent magnets.
  • the magnet according to the second embodiment has an interval of 22.5 degrees between adjacent magnets as shown in FIG.
  • an iron core member such as a laminated steel plate is arranged.
  • FIG. 17 is a cross-sectional view showing a configuration of an electric motor using a rotor according to the sixth embodiment of the present invention.
  • the stator 71 is composed of 18 cores 72 and 18 windings 73, and the windings 73 are wound around the 18 divided cores 72 in a concentrated manner.
  • Three of the windings are arranged in every 6 pieces, and one set (total 6 sets) is connected in series or in parallel, and one of them is connected to one of the other phases as a neutral point
  • the other is connected to the P side and ⁇ side of the power supply line via a switching element inside an inverter (not shown).
  • this inverter is configured to control six phases.
  • this stator is described with a divided core, it is well known that the same operation can be performed with a core that is not divided.
  • the shoreline is applicable not only to concentrated winding but also to distributed ridges.
  • the rotor 74 has two types of pole pairs: a three-pole pair and a six-pole pair.
  • the force by which the permanent magnet is disposed on the surface of the rotor 74 will be described with reference to some permanent magnets 75a to 75d as an example.
  • Permanent magnets 75a and 75b are magnets that have the same magnetization direction and are magnetized so as to generate magnetic flux as indicated by arrows AR1 and AR2 by urging outwardly the center CTR force of rotor 74.
  • the permanent magnets 75c and 75d are magnets that have the same magnetization direction and are magnetized so as to generate magnetic flux as indicated by arrows AR3 and AR4 from the outside toward the center CTR of the rotor 74.
  • the length of the arrow AR1-4 line mimics the magnitude of the magnetic flux. Therefore, normally, if the magnetization directions of the former and the latter are reversed, magnetic fluxes in the opposite direction are generated in the former and the latter.
  • the permanent magnets 75a and 75c and the permanent magnets 75b and 75d are composed of the same magnet, and the magnetic flux strength of the permanent magnets 75a and 75c is larger.
  • Figure 17 shows the shape of a surface magnet, but the same applies to an embedded magnet-shaped rotor.
  • the permanent magnets 75a and 75c are composed of rare earth magnets having both excellent coercive force and residual magnetic flux density, and the permanent magnets 75b and 75d have either one of coercive force and residual magnetic flux density than the permanent magnets 75a and 75c. Or both are composed of inferior magnets.
  • neodymium magnets can be considered for the permanent magnets 75a and 75b, and neodymium magnets, ferrite magnets, alnico magnets, etc., which are inferior to the permanent magnets 75a and 75b, can be applied to the permanent magnets 75b and 75d. . Therefore, the cost of an expensive neodymium magnet can be reduced as compared with a conventional rotor. Then like this The reason for the magnet arrangement will be described in detail with reference to FIG.
  • FIG. 18 shows a magnet considered in the present invention when a magnet (virtual rotor) having a high magnetic pole number (4 poles) is combined with a magnet region having a low magnetic pole number (2 poles) and an electrical angle of 1 period. It is the figure which represented arrangement
  • Figure 18 (a) shows a virtual rotor with a low number of magnetic poles (two poles) before combination.
  • Figure 18 (b) shows a virtual rotor with a high number of magnetic poles (4 poles) before combination.
  • the number in the permanent magnet indicates the magnitude of the magnetic flux of the magnet, and the figure indicates the polarity of the magnet (that is, the magnetic flux indicates whether the central force also goes to the outside or to the center).
  • the magnetic flux on the 2 pole side is set large, so when combined, the permanent magnets 75a and 75b and the permanent magnets 75c and 75d are arranged next to each other, and the magnetic flux waveform has components on the 2 pole side. The configuration is easily emphasized.
  • FIG. 19 is a cross-sectional view showing a configuration of an electric motor using a rotor according to the seventh embodiment of the present invention.
  • the stator 81 is composed of 18 cores 82 and 18 windings 83, and the windings 83 are concentrated around the 18 divided cores 82.
  • the rotor 84 has two types of pole pairs: a 3-pole pair and a 6-pole pair. Permanent magnets are arranged on the surface of the rotor 84, and the configuration will be described with some permanent magnets 85a to 85d as an example.
  • the difference between the seventh embodiment and the sixth embodiment is that in the seventh embodiment, the magnetic flux on the high magnetic pole number side is easily emphasized, and the permanent magnets 85a, 85d, 85b, 85c
  • the adjacent magnetic force arrows AR5, AR8, AR6, and AR7 are configured to alternately switch the direction of magnetic flux.
  • Fig. 20 shows a combination of magnet sets in which the direction of magnetic flux generation alternates for each magnet.
  • Fig. 20 shows a magnet considered in the present invention when a magnet (virtual rotor) having a high magnetic pole number (4 poles) is combined with a magnet region having a low magnetic pole number (2 poles) and an electrical angle of 1 period. It is the figure which represented arrangement
  • the two-pole and four-pole magnet phases used in the combination are one type of force, and various magnets can be obtained using the same concept even when these magnets have an arbitrary phase difference.
  • Arrangement Can be considered.
  • the combination of the number of poles according to force which explains the combination of two and four poles, can be considered similarly.
  • the permanent magnets 75a to 75d and 85a to 85d need not have the same magnet width.
  • Fig. 21 shows a diagram in which only the mechanical angle of 120 degrees of the rotor in Fig. 17 is taken out (example in which the width is changed).
  • the permanent magnets 75a and 75c and the permanent magnets 75b and 75d are the same type of magnet, the permanent magnets 75a and 75c have the maximum magnet width Wa, and the permanent magnets 75b and 75d have the maximum magnet width Wb.
  • the magnetic flux level (strength) of the number of magnetic poles constituting them can be changed. “Width ⁇ Width ⁇ !” Increases the magnetic flux on the 2-pole side, and “width Wa and width Wb” increases the magnetic flux on the 4-pole side.
  • FIG. 22 shows a diagram in which only the mechanical angle of 120 degrees of the rotor of FIG. 17 is taken out (example in which the thickness is changed).
  • the permanent magnets 75a and 75c and the permanent magnets 75b and 75d are the same type of magnet.
  • the maximum magnet thickness of the permanent magnets 75a and 75c is Ta, and the maximum magnet thickness of the permanent magnets 75b and 75d is Tb.
  • Magnets such as Alnico have low holding power, so if the magnet thickness is too thin, it will be easy to demagnetize, and it is necessary to set the magnet thickness according to the respective magnet characteristics.
  • the magnetic flux can be increased by increasing the magnet thickness to some extent, the magnetic flux levels of the 2-pole and 4-pole can be changed.
  • the magnet thickness is increased too much, the magnetic flux density is gradually saturated and the magnetic resistance increases, so that no effect is obtained.
  • a 6-phase inverter is connected to the stator as described above, and it is sufficient to apply current to generate a composite sinusoidal magnetic flux corresponding to the rotor magnetic field of 3 pole pairs and 6 pole pairs. ,.
  • the current command is rotated according to the position of the rotor in the same way as a normal motor.
  • this motor generates a composite magnetic flux corresponding to both pole pairs. Therefore, the inverter is considered to have 6 phases, and the current value at each position obtained by dividing one cycle of the sine wave into 6 is calculated as the command value for each phase.
  • a 6-pole pair a 6-cycle sine wave is generated, so it is obtained as a current command value at a position where one sine wave cycle is divided into 3 parts, and the 6-phase inverter first, fourth, The command values for Phases 2 and 5 and Phases 3 and 6 are used. After this, the command values of the 3 pole pair and 6 pole pair are added together to control the current as the command value of the 6-phase inverter. This As a result, the rotor generates torque and rotates.
  • Torque is generated by the above operation, but torque is the force generated by the interaction of field magnetic flux (magnetic flux generated by the rotor) and current magnetic flux (rotational magnetic flux generated by the stator). It is generated according to wave components (in this example, 3 pole pairs and 6 pole pairs). In Example 1 of this time, torque that is the sum of torques of 3 poles and 6 poles is generated.
  • all the magnets in one rotor use magnets having the same characteristics, but in the present invention, the magnet characteristics are low! Can be generated.
  • the loss generated by the current flowing at that time is smaller than the sum of the absolute value average and the square average of the combined current as described above, and the single average value, the loss is clearly small. From the above, it is possible to obtain the effect of generating a torque equivalent to two motors with one electric motor and having a smaller loss than that of two electric motors.
  • FIGS. 23 to 27 are cross-sectional explanatory views schematically showing the configurations of the rotor and the stator of the electric motor according to the eighth embodiment of the present invention.
  • FIG. 24 is an explanatory cross-sectional view showing another example of the magnetization direction in the magnet of FIG.
  • the arrow in a figure has shown the magnetization direction of the magnet, and it is the same also in another figure.
  • the magnet 112 arranged in the flux noria part is magnetized so that the magnetization direction is one direction or more in multiple directions so that the magnetic flux is concentrated in the direction of the magnetic flux increasing part by the sum of the magnetic fluxes. ing.
  • the magnetization direction of the magnet 112 is not a single angle, but a single direction may be formed by a set of multidirectional magnetic fluxes having a plurality of different tilt angles (see arrows in the figure). good.
  • the simple arrangement of the magnet 112 can improve the torque without newly securing a magnet installation space, or can generate an equivalent torque with a small amount of magnetism.
  • the electric motor 10 as the composite magnetic flux motor has a configuration in which a 4-pole rotor and an 8-pole rotor are overlapped.
  • FIG. 25 is an explanatory cross-sectional view schematically showing a configuration of a rotor and a stator of an electric motor having a 4-pole pair of rotors in a 12-slot stator.
  • FIG. 26 is a cross-sectional explanatory view schematically showing a configuration of a rotor and a stator of an electric motor having an 8-pole pair of rotors in a 12-slot stator.
  • FIG. 27 is an explanatory cross-sectional view schematically showing a configuration of a rotor and a stator of an electric motor in which a 4-pole rotor and an 8-pole rotor are superimposed.
  • the electric motor 10 is a low magnetic pole number electric motor having a stator 91 having 12 slots 91a and a rotor 104 in which four pole pairs of magnets 115 are arranged.
  • the electric motor 10 is a high magnetic pole number electric motor having a stator 91 having twelve slots 91a and a rotor 114 in which eight pole pairs of magnets 115 are arranged.
  • the electric motor 10 having a configuration in which the four-pole rotor 104 of the electric motor 10 (see FIG. 25) and the eight-pole rotor 114 of the electric motor 10 (see FIG. 26) are overlapped.
  • the portion where the different poles overlap is regarded as the flux noria portion 120a. This is because the portion where the different polarities overlap in the rotor radial direction is canceled by the opposite magnetization directions.
  • a flux NOROR portion which is a magnetic flux reduction portion by the combined magnetic flux of the rotor 94 is provided.
  • a magnet 11 2 (see 023, 24) composed of magnets 112a and 112b magnetized so that the magnetic flux is concentrated in the direction of the magnetic flux increasing part by the sum of the magnet magnetic flux adjacent to this part Has been.
  • the electric motor 10 that generates the magnetic flux obtained by combining the sine waves generates the magnetic flux corresponding to the different number of magnetic poles on the surface.
  • a rotor 94 having a generating member and a stator 91 to which a current is applied so that a plurality of current magnetic fields corresponding to the number of magnetic poles can be combined and rotated.
  • a stator 91 to which a current is applied so that a plurality of current magnetic fields corresponding to the number of magnetic poles can be combined and rotated.
  • the torque can be improved without newly securing a magnet installation space, or the equivalent torque can be generated with a small magnet amount.
  • the auxiliary magnetic pole is arranged in the region (the magnetic flux blank region necessary for producing the composite magnetic flux) without arranging the magnet in the first place, the space efficiency due to the arrangement of the auxiliary magnetic pole is poor.
  • the combination of the composite magnetic flux rotor and the auxiliary magnetic pole motor must be secured for the auxiliary magnetic pole motor, and a magnet installation space inevitably exists, which is disadvantageous for the auxiliary magnetic pole motor. Since it does not occur, it is more effective.
  • FIG. 28 schematically shows a configuration of a rotor and a stator of an electric motor according to a ninth embodiment of the present invention.
  • (A) is a cross-sectional explanatory view when the magnet is arranged on the surface
  • (b) is a diagram of the magnet.
  • FIG. 5 is a cross-sectional explanatory diagram when embedded.
  • the electric motor 10 has a magnetic flux in the direction of the magnetic flux increasing portion due to the sum of the magnetic fluxes in the flux noria portion 120a (see FIG. 27) that is the magnetic flux decreasing portion due to the sum of the magnetic fluxes of the rotor 134.
  • the magnet 127 with one or more installation angles is arranged so that can be concentrated. Other configurations and operations are the same as those of the motor 10.
  • the torque can be improved at low cost without newly securing a magnet installation space, or the equivalent torque can be reduced with a small amount of magnet. Can be generated.
  • FIG. 29 schematically shows the configuration of the rotor and stator of the electric motor according to the tenth embodiment of the present invention. It is shown schematically, (a) is a cross-sectional explanatory diagram when magnets are arranged on the surface, and (b) is a cross-sectional explanatory diagram when magnets are embedded and arranged.
  • the electric motor 10 has a magnetic flux concentrated in the direction of the magnetic flux increasing portion 120a (see FIG. 27), which is the magnetic flux decreasing portion due to the sum of the magnetic fluxes of the rotor 144.
  • Two or more magnets 132 are arranged so that a composite vector can be formed.
  • a plurality of magnets 132a, 132b, 132c that form a composite magnetic flux vector that concentrates the magnetic flux on the magnet can be replaced.
  • FIG. 30 schematically shows a configuration of a rotor and a stator of an electric motor according to an eleventh embodiment of the present invention
  • (a) is a cross-sectional explanatory diagram when magnets are arranged on the surface
  • (b) is a magnet FIG.
  • the magnetic flux is concentrated in the direction of the magnetic flux increasing portion due to the sum of the magnetic fluxes in the flux noria portion (see FIG. 27), which is the magnetic flux decreasing portion due to the sum of the magnetic fluxes of the rotor 154.
  • One or more magnets 137 and one or more flux barrier portions 138 are arranged.
  • At least a part of the portion of the rotor 154, which is regarded as a flattened barrier portion, which is a magnetic flux decreasing portion due to the sum of the magnetic fluxes of the rotor, are replaced by magnets 137a and 137b in which magnetic flux is concentrated, and a flux noor part 138 located on the outer peripheral side of both magnets 137a and 137b.
  • the electric motor according to the present invention includes a rotor having a magnetic flux generating member for generating a magnetic flux corresponding to a plurality of different magnetic poles on its surface, and the plurality of magnets. At least one of the stators to which a current can be applied so that a plurality of current magnetic fields corresponding to the number of poles can be rotated and rotated is provided, and the magnetic flux is reduced at the portion where the magnetic flux is reduced by adding the magnetic flux.
  • the magnets are magnetized so that the magnetic flux concentrates on the part where the magnetic flux is increased by adding together!].
  • the magnetic flux of the magnet disposed in at least a part of the portion where the magnetic flux is reduced due to the sum of the magnetic fluxes is concentrated on the portion where the magnetic flux is increased due to the sum of the magnetic flux depending on the installation angle of one or more magnets. ing.
  • the torque can be improved at a low cost without newly securing a magnet installation space, or an equivalent torque can be generated with a small amount of magnet.
  • the magnetic flux of the magnet arranged at least in a portion where the magnetic flux is reduced due to the sum of the magnetic fluxes is concentrated on the portion where the magnetic flux is increased due to the sum of the magnetic fluxes by vector synthesis of two or more magnetic fluxes.
  • the magnetic flux of the magnet disposed in at least a part of the portion where the magnetic flux is reduced due to the sum of the magnetic fluxes is combined with one or more magnets and one or more flux cores ⁇ It concentrates on the part that increased.
  • the rotor magnet is shown as N pole and S pole.-There is an example described. Note that it is similar. Furthermore, the N-pole and S-pole magnets are oriented in the direction of the magnetic field force. Magnets whose magnetization directions are in the radial direction (in the opposite direction) so that they are in the radial direction of the rotor center. (Slave side), S pole is arranged outside (stator side). Further, in some embodiments, the magnet is a force using the magnetizing direction arranged in the radial direction. The arrangement is not limited to this arrangement, and if the magnetic field lines are almost in the radial direction, there is no problem. Even a magnet arrangement.
  • a part of the plurality of magnet magnetic fluxes are generated so as to cancel each other, and the portion where the magnetic flux is canceled is arranged with a small amount of the magnetic flux generating member, or the magnet is deleted. , The amount of expensive permanent magnets used can be reduced.
  • this configuration uses a magnetic flux generating member that generates a plurality of magnet magnetic fluxes corresponding to a plurality of magnet sets each having a different number of magnetic poles. Of course, it is possible to reduce the loss due to the loss compared to the case where the two rotors are rotated independently.
  • the weight of the rotor itself is reduced by reducing the number of magnets at the magnetic flux canceling position, and it is further effective in improving the torque by reducing the inertia of the deleted magnet and reducing the weight of the motor. Even when an electromagnet is used, similar effects such as cost reduction, torque improvement, and motor weight reduction can be obtained.
  • the peak of the winding current is obtained by providing a predetermined phase difference in the magnetic flux of each magnetic pole number component (that is, between each set of magnets generating each magnetic flux). Any one of the value, magnetic flux peak value, and induced voltage peak value can be set to a desired value.
  • the absolute peak value of the winding current flowing through the stator winding of the motor is minimized, which is advantageous in reducing the switching element capacity of the inverter.
  • the average value of the absolute value of the winding current flowing through the stator winding of the motor is minimized, it is possible to reduce the loss of the IGBT or the diode that causes a constant voltage drop. It will be advantageous.
  • the effective value of the winding current flowing through the stator winding of the motor is minimized, which is advantageous in reducing the copper loss generated in the winding.
  • the peak value of the magnetic flux obtained by adding the two magnet magnetic fluxes is minimized, which is advantageous in suppressing the occurrence of magnetic saturation.
  • the motor can be rotated at high speed.
  • the peak value of the induced voltage generated in the stator winding of the motor is maximized, so that the torque of the motor can be increased.
  • the magnetic flux generating member (that is, the magnet constituting the set of the plurality of magnets in the member) corresponds to at least one set of the plurality of magnet sets.
  • the magnetic flux generating member corresponds to at least one set of the plurality of magnet sets.
  • the cogging torque can be reduced.
  • At least one of the plurality of magnet sets constitutes the electric motor.
  • the surface shape facing the stator that is, the cross-sectional shape when cut by a plane perpendicular to the axis of the motor
  • the surface shape facing the stator is separated from the rotor axis for each magnetic pole in the circumferential direction of the rotor.
  • At least one of the plurality of magnetic poles is arranged so that a difference occurs between the d-axis inductance and the q-axis inductance, so that the reluctance torque can be obtained.
  • the torque can be increased without increasing the number of magnetic flux generating members.
  • a rotor that can easily generate composite magnetic flux (it is not a mere gap, and can control passing magnetic flux), and can generate composite magnetic flux at low cost. It becomes possible to do.
  • a magnetic flux waveform can be distorted to generate a plurality of order component magnetic fluxes.
  • the magnetic flux waveform can be distorted to generate a plurality of order component magnetic fluxes, and demagnetization is not caused even when the rotor becomes hot.
  • a rotating electrical machine can be realized.
  • a rotating electrical machine in which the magnetic flux of the order component on the high magnetic pole number side is emphasized can be realized.
  • the eleventh to fourteenth inventions can be realized and magnets having the same volume may be prepared.
  • the content ratio of the fundamental wave and the harmonic component of the magnetic flux can be changed by changing the magnet pitch (the circumferential length of each magnet).
  • the eleventh to fourteenth inventions can be realized and magnets having the same volume may be prepared.
  • the magnetized magnet placed in the portion from which the magnet has been removed concentrates the magnetic flux in the portion where the magnetic flux has been increased by the addition of the magnetic flux of the magnet. The torque can be improved without securing a new value, and further downsizing can be realized.

Landscapes

  • Engineering & Computer Science (AREA)
  • Power Engineering (AREA)
  • Permanent Field Magnets Of Synchronous Machinery (AREA)

Abstract

A rotor (14) of a motor for a vehicle having a flux generation member generating by adding up a plurality of magnet fluxes corresponding to a plurality of sets of magnet each having a different number of poles, characterized in that the flux is generated to be offset partially between respective magnet fluxes corresponding to the plurality of sets (N, S) of magnet, low flux magnets (N1-N3, S1-S6) are arranged such that the quantity of flux becomes smaller at the position where the flux is offset than at the position where the flux is not offset, or a flux generation member from which the magnet is removed is provided. An auxiliary magnet for reinforcing and concentrating flux convergence may be arranged in a space from where the magnet is removed.

Description

明 細 書  Specification

電動機の回転子  Electric motor rotor

技術分野  Technical field

[0001] 本発明は電動機の回転子に関する。  [0001] The present invention relates to a rotor of an electric motor.

背景技術  Background art

[0002] 近年自動車にも多数用いられて 、る電動機では、自動車と!/、う用途上、小型化と効 率に対して厳しい要求がある。現在、電動モータを走行用に搭載した自動車の多く は、エンジンの出力と電動機の出力を組み合わせて走行するハイブリッド自動車であ り、発電機用途と電動機用途の 2つの電動機を搭載したものが多ぐこのようなハイブ リツド自動車用電動機の小型化 ·高効率化を実現する手段として、本出願人は複合 電流方式の 2ロータ電動機 (特許文献 1を参照された!ヽ。 )を開発した。  [0002] In recent years, electric motors that are widely used in automobiles have severe demands for miniaturization and efficiency for automobiles and applications. Currently, many automobiles equipped with electric motors for running are hybrid cars that run by combining engine output and motor output, and many have two electric motors for generators and motors. As a means for realizing the miniaturization and high efficiency of such a hybrid automobile motor, the present applicant has developed a composite current type two-rotor motor (refer to Patent Document 1!).

[0003] この発明によれば、 2つの回転子に対応した電流を複合した 1つの複合電流を 1つ の固定子に給電することで 2つの回転子を独立に回転させることが可能であり、 1つ の電動機体格で別個の 2つの出力'トルクを発生させることが可能であるとともに、両 回転子に合わせて固定子に与えられる電流の平均値は、単純に 2つの電動機に電 流を与えた場合の平均値より低ぐ電流による損失が低減するという効果がある。  [0003] According to the present invention, it is possible to independently rotate two rotors by feeding one composite current, which is a composite of currents corresponding to two rotors, to one stator, It is possible to generate two separate output 'torques with one motor body, and the average value of the current applied to the stator for both rotors simply gives the current to the two motors. There is an effect that the loss due to the current lower than the average value is reduced.

[0004] 一方、磁石トルクを高めるために、補助磁極を設置することが考えられる (特許文献 2)が、この場合、補助磁極を設置するための場所、即ち、磁石スペースを新たに確 保する必要があった。  [0004] On the other hand, it is conceivable to install an auxiliary magnetic pole in order to increase the magnet torque (Patent Document 2). In this case, however, a place for installing the auxiliary magnetic pole, that is, a magnet space is newly secured. There was a need.

特許文献 1 :特許第 3480301号 (段落 0010,0011、図 1)  Patent Document 1: Japanese Patent No. 3480301 (paragraphs 0010,0011, Fig. 1)

特許文献 2 :特開 2003— 347121号公報  Patent Document 2: Japanese Patent Laid-Open No. 2003-347121

発明の開示  Disclosure of the invention

[0005] し力しながら、上述の発明における電動機は、例えば、自動車などで電動機をタイ ャの内側に搭載するホイールインモータのような場合、出力先はタイヤ (ホイール)の みを想定しているため、出力軸が 2つは必要無ぐ冗長となる。また、 2つの出力軸を 結合して 1軸にする機構が必要となるなどの問題もある。また、別個の 2つの電動機を 組み合わせて電動機 2つ分のトルクを機械的に結合した場合には、 2つ分の電動機 筐体があるため小型化できない。さらに、電動機トルクを上げるために、単に「通常の 従来電動機 1台」を大型化しただけでは、電動機筐体も大きくなり、電流損失も大きく なるなどの問題があった。即ち、さらに電流損失が少なくさらに小型化された回転電 動機の回転子の開発が求められている。 However, the electric motor in the above-described invention assumes that the output destination is only a tire (wheel), for example, in the case of a wheel-in motor in which the electric motor is mounted inside the tire in an automobile or the like. Therefore, two output shafts are unnecessary and redundant. There are also problems such as the need for a mechanism that combines two output shafts into a single shaft. When two separate motors are combined and the torque of two motors is mechanically combined, two motors Since there is a housing, it cannot be downsized. In addition, simply increasing the size of a “normal conventional motor” to increase the motor torque has problems such as an increase in the motor housing and an increase in current loss. That is, there is a demand for the development of a rotor for a rotating electric machine that has a smaller current loss and is further miniaturized.

[0006] 本発明は、上記の問題点に鑑み、複数に分かれている、異なる極対数の複数の回 転子 (そこに含まれる複数の磁石)を一体に統合し、 1つの電動機の体格に小型化し 、電流の低損失ィ匕を図った電動機の回転子を提供する。  [0006] In view of the above problems, the present invention integrates a plurality of rotors (a plurality of magnets included therein) having a different number of pole pairs into a single physique. Provided is a motor rotor that is reduced in size and has low current loss.

[0007] 即ち、上述した諸課題を解決すベぐ本発明の電動機の回転子は、それぞれの組 が異なる磁極数で構成される複数の磁石の組に相当する複数の磁石磁束を合算し て発生させる一つの回転子に配置される磁束発生部材であって、前記複数の磁石 の組に相当する前記磁石磁束の各々の間で、磁束の一部を相殺するように発生させ 、磁束が相殺される箇所 (これをフラックスノリア部という)は、磁束が相殺されない箇 所に比べて磁束量を少なくするように、低磁束磁石を配置するか、もしくは磁石を除 去したことを特徴とする。  That is, the rotor of the electric motor of the present invention that solves the above-described problems is obtained by adding together a plurality of magnet magnetic fluxes corresponding to a plurality of magnet sets each having a different number of magnetic poles. A magnetic flux generating member disposed in one rotor to be generated, wherein the magnetic flux is generated so as to cancel a part of the magnetic flux between each of the magnet magnetic fluxes corresponding to the set of the plurality of magnets. The place where this is done (referred to as the flux noria part) is characterized in that a low-flux magnet is placed or the magnet is removed so that the amount of magnetic flux is reduced compared to the place where the magnetic flux is not canceled.

[0008] さらに、上述した諸課題を解決すベぐ磁石を除去した空間に、磁石磁束の合算に より磁束の増力 tlした部分に磁束が集中するように着磁した磁石を配置して、磁束^^ 中させ磁石を除去した空間を有効に利用しつつ磁束の集中効果を高めてもよい。  [0008] Further, a magnet magnetized so that the magnetic flux is concentrated in a portion where the magnetic flux is increased by the addition of the magnetic flux of the magnetic flux tl is arranged in the space from which the magnet that solves the above-described problems is removed. ^^ The magnetic flux concentration effect may be enhanced while effectively using the space where the magnet is removed.

[0009] 即ち、第 1の発明の電動機の回転子は、それぞれの組が異なる磁極数で構成され る複数の磁石の組の磁石磁束を合算した磁石磁束に相当する磁束を発生させる磁 束発生部材であって、前記複数の磁石の組の前記磁石磁束を重畳及び相殺するよ うに合算磁束に相当する磁束を発生させ、磁束が相殺される箇所は、磁束が相殺さ れない箇所に比べて磁束量を少なくするように、低磁束磁石を配置するか、もしくは 磁石を除去したことを特徴とする。  That is, the rotor of the electric motor according to the first aspect of the invention generates magnetic flux that generates a magnetic flux equivalent to a magnet magnetic flux obtained by adding together the magnetic fluxes of a plurality of magnet sets each having a different number of magnetic poles. The member is a member that generates a magnetic flux corresponding to the combined magnetic flux so as to superimpose and cancel the magnet magnetic flux of the set of the plurality of magnets, and the portion where the magnetic flux is canceled is compared with the portion where the magnetic flux is not canceled. A low-flux magnet is arranged or the magnet is removed to reduce the amount of magnetic flux.

[0010] また、第 2の発明の電動機の回転子は、前記複数の磁石の組が 2組あり、これら各 組の磁極数成分の磁束 (即ち、各組を構成する磁石の配置)に所定の位相差を設け ることを特徴とする。  [0010] In addition, the rotor of the electric motor of the second invention has two sets of the plurality of magnets, and the magnetic flux of the number of magnetic pole components of each set (that is, the arrangement of the magnets constituting each set) is predetermined. The phase difference is provided.

[0011] また、第 3の発明の電動機の回転子は、前記所定の位相差が、(前記複数の磁石 の組の磁極数の組み合わせに基づき)前記電動機を構成する固定子卷線に通電す る卷線電流の絶対値のピーク値が最小になるように設定されることを特徴とする。 [0011] Further, in the rotor of the electric motor according to the third aspect of the invention, the predetermined phase difference energizes a stator winding constituting the electric motor (based on a combination of the number of magnetic poles of the plurality of magnet sets). The absolute peak value of the winding current is set to be minimum.

[0012] また、第 4の発明の電動機の回転子は、前記所定の位相差が、(前記複数の磁石 の組の磁極数の組み合わせに基づき)前記電動機を構成する固定子卷線に通電す る卷線電流の絶対値の平均値が最小になるように設定されることを特徴とする。  [0012] Further, in the rotor of the electric motor according to the fourth aspect of the invention, the predetermined phase difference energizes a stator winding constituting the electric motor (based on a combination of the number of magnetic poles of the plurality of magnet sets). It is characterized in that the average value of the absolute value of the winding current is set to be minimum.

[0013] また、第 5の発明の電動機の回転子は、前記所定の位相差が、(前記複数の磁石 の組の磁極数の組み合わせに基づき)前記電動機を構成する固定子卷線に通電す る卷線電流の実効値が最小になるように設定されることを特徴とする。  [0013] Further, in the rotor of the electric motor according to the fifth aspect of the invention, the predetermined phase difference energizes the stator windings constituting the electric motor (based on the combination of the number of magnetic poles of the plurality of magnet sets). The effective value of the winding current is set to be a minimum.

[0014] また、第 6の発明の電動機の回転子は、前記所定の位相差が、(前記複数の磁石 の組の磁極数の組み合わせに基づき)前記 2組の磁石に相当する 2つの磁石磁束を 合算した磁束のピーク値が最小になるように設定されることを特徴とする。  [0014] Further, in the rotor of the electric motor of the sixth invention, the predetermined phase difference is based on the two magnet magnetic fluxes (based on the combination of the number of magnetic poles of the plurality of magnet sets) corresponding to the two sets of magnets. It is characterized in that the peak value of the magnetic flux summing up is set to be the minimum.

[0015] また、第 7の発明の電動機の回転子は、前記所定の位相差が、(前記複数の磁石 の組の磁極数の組み合わせに基づき)前記回転子の回転時に前記電動機を構成す る固定子卷線に発生する誘起電圧のピーク値が最小になるように設定されることを特 徴とする。  [0015] Further, in the rotor of the electric motor according to the seventh aspect of the invention, the predetermined phase difference constitutes the electric motor when the rotor rotates (based on a combination of the number of magnetic poles of the plurality of magnet sets). It is characterized in that it is set so that the peak value of the induced voltage generated in the stator winding is minimized.

[0016] また、第 8の発明の電動機の回転子は、前記所定の位相差が、(前記複数の磁石 の組の磁極数の組み合わせに基づき)前記回転子の回転時に前記電動機を構成す る固定子卷線に発生する誘起電圧のピーク値が最大になるように設定されることを特 徴とする。  [0016] In addition, the rotor of the electric motor of the eighth invention configures the electric motor so that the predetermined phase difference is based on a combination of the number of magnetic poles of the plurality of magnet sets when the rotor rotates. It is characterized in that it is set so that the peak value of the induced voltage generated in the stator winding is maximized.

[0017] また、第 9の発明の電動機の回転子は、前記磁束発生部材 (即ちこの部材における 前記複数の磁石の組を構成する磁石)は、前記複数の磁石の組の少なくとも 1つの 組に相当する磁石磁束が、回転子円周方向に正弦波状に分布するように形成される ことを特徴とする。  [0017] Further, in the rotor of the electric motor according to the ninth aspect of the invention, the magnetic flux generating member (that is, the magnet constituting the set of the plurality of magnets in this member) is at least one set of the set of the plurality of magnets. The corresponding magnet magnetic flux is formed so as to be distributed in a sinusoidal shape in the circumferential direction of the rotor.

[0018] 例えば、前記複数の磁石の組のうちの少なくとも 1つの組の磁石の、前記電動機を 構成する固定子に対向する表面形状 (即ち、電動機の軸心に垂直な平面で切ったと きの断面形状)を、回転子円周方向に対して、磁極ごとに、回転子軸心からの半径よ り小さい径の円弧形状とすることを想定した磁石の組を、他の通常の表面形状の磁 石の組と、合体させた表面形状 (この形状自体が曲線となる)にすることによって、簡 易かつ簡便に、磁束を回転子円周方向に正弦波状に分布させることが可能となる。 [0019] また、第 10の発明の電動機の回転子は、前記磁束発生部材における前記複数の 磁石の組のうち少なくとも 1つの組における磁極力 d軸インダクタンスと q軸インダクタ ンスとの間に差が生じるように配置されて 、ることを特徴とする。 [0018] For example, the surface shape of at least one of the plurality of magnet sets facing the stator constituting the electric motor (that is, when cut by a plane perpendicular to the axis of the electric motor) A magnet set that assumes that the cross-sectional shape is an arc shape whose diameter is smaller than the radius from the rotor axis for each magnetic pole with respect to the circumferential direction of the rotor. By combining the surface of the magnet and the combined surface shape (this shape itself becomes a curve), the magnetic flux can be distributed in a sinusoidal shape in the circumferential direction of the rotor easily and simply. [0019] Also, in the rotor of the electric motor of the tenth invention, there is a difference between the magnetic pole force d-axis inductance and the q-axis inductance in at least one of the plurality of sets of magnets in the magnetic flux generating member. It is arranged so that it occurs.

[0020] また、第 11の発明の電動機の回転子は、前記磁束発生部材が永久磁石であり、前 記永久磁石が、第 1の永久磁石と第 2の永久磁石によって構成され、前記第 1の永久 磁石の残留磁束密度および Zまたは保磁力が、前記第 2の永久磁石のそれよりも大 きい (即ち、高残留磁束密度、かつ、高保磁力である第 1の永久磁石と、第 1の永久 磁石よりも残留磁束密度および保磁力が小さい第 2の永久磁石によって構成される) ことを特徴とする。  [0020] Further, in the rotor of the electric motor according to an eleventh aspect of the invention, the magnetic flux generating member is a permanent magnet, and the permanent magnet is constituted by a first permanent magnet and a second permanent magnet. The permanent magnet has a residual magnetic flux density and a Z or coercive force larger than that of the second permanent magnet (that is, the first permanent magnet having a high residual magnetic flux density and a high coercive force, and the first permanent magnet). It is characterized by a second permanent magnet having a smaller residual magnetic flux density and coercive force than the permanent magnet).

[0021] また、第 12の発明の電動機の回転子は、前記磁束発生部材が永久磁石であり、前 記永久磁石が、第 1の永久磁石と第 2の永久磁石によって構成され、前記第 2の永久 磁石の温度変化に対する磁石特性が、前記第 2の永久磁石のそれよりも安定である (即ち、第 2の永久磁石の温度変化に対する磁石特性変化が、第 1の永久磁石のそ れより小さ 、)ことを特徴とする。  [0021] Further, in the rotor of the electric motor according to a twelfth aspect of the invention, the magnetic flux generating member is a permanent magnet, and the permanent magnet is constituted by a first permanent magnet and a second permanent magnet, and the second The magnet characteristics with respect to the temperature change of the second permanent magnet are more stable than those of the second permanent magnet (i.e., the magnet characteristic change with respect to the temperature change of the second permanent magnet is more stable than that of the first permanent magnet). Small).

[0022] また、第 13の発明の電動機の回転子は、前記複数の磁石の組が、低磁極数の第 1 の磁石の組と高磁極数の第 2の磁石の組とからなり、前記第 1および第 2の磁石の組 を構成する磁石をそれぞれ配置するにあたり、前記第 1の磁石の組 (低磁極数)を構 成する磁石と、前記第 2の磁石の組 (高磁極数)を構成する磁石を相殺する際に、前 記第 1の磁石の組 (低磁極成分)の磁束が強まるように磁石を配置することを特徴と する。  [0022] Further, in the rotor of the electric motor according to a thirteenth aspect of the present invention, the set of the plurality of magnets includes a first magnet set having a low magnetic pole number and a second magnet set having a high magnetic pole number, When arranging the magnets constituting the first and second magnet sets, the magnets constituting the first magnet set (low magnetic pole number) and the second magnet set (high magnetic pole number) The magnets are arranged so that the magnetic flux of the first set of magnets (low magnetic pole component) is strengthened when canceling out the magnets constituting the.

[0023] また、第 14の発明の電動機の回転子は、前記複数の磁石の組が、低磁極数の第 1 の磁石の組と高磁極数の第 2の磁石の組とからなり、前記第 1および第 2の磁石の組 を構成する磁石をそれぞれ配置するにあたり、前記第 1の磁石の組 (低磁極数)を構 成する磁石と、前記第 2の磁石の組 (高磁極数)を構成する磁石を相殺する際に、前 記第 2の磁石の組 (高磁極成分)を構成する磁石の磁束が強まるように磁石を配置す ることを特徴とする。  [0023] Further, in the rotor of the electric motor according to the fourteenth aspect of the invention, the set of the plurality of magnets includes a first magnet set having a low magnetic pole number and a second magnet set having a high magnetic pole number, When arranging the magnets constituting the first and second magnet sets, the magnets constituting the first magnet set (low magnetic pole number) and the second magnet set (high magnetic pole number) The magnets are arranged so that the magnetic fluxes of the magnets constituting the second set of magnets (high magnetic pole component) are strengthened when the magnets constituting the are canceled.

[0024] また、第 15の発明の電動機の回転子は、前記磁束発生部材が複数の永久磁石に より構成され、前記複数の永久磁石の(回転子中心から見て)周方向の長さが全て同 一である(前記永久磁石の磁石ピッチが、すべての磁石において同一の長さで構成 する)ことを特徴とする。 [0024] Further, in the rotor of the electric motor of the fifteenth aspect of the invention, the magnetic flux generating member is composed of a plurality of permanent magnets, and the circumferential length (as viewed from the rotor center) of the plurality of permanent magnets is All the same 1 (the magnet pitch of the permanent magnets is the same for all magnets).

[0025] また、第 16の発明の電動機の回転子は、前記磁束発生部材が複数の永久磁石に より構成され、前記複数の永久磁石の(回転子中心から見て)周方向の長さが磁石に よって異なる(前記永久磁石の磁石ピッチを磁石によって異なる長さで構成する)こと を特徴とする。  [0025] Further, in the rotor of the electric motor according to the sixteenth aspect of the invention, the magnetic flux generating member is composed of a plurality of permanent magnets, and the circumferential length (as viewed from the rotor center) of the plurality of permanent magnets is It differs depending on the magnet (the magnet pitch of the permanent magnet is configured with a different length depending on the magnet).

[0026] また、第 17の発明の電動機の回転子は、前記磁束発生部材が複数の永久磁石に より構成され、前記複数の永久磁石の(回転子中心から見て)半径方向の厚さが、磁 石によって異なる(即ち、半径方向の磁石厚を磁石によって異ならせる)ことを特徴と する。  [0026] Further, in the rotor of the electric motor according to the seventeenth aspect of the invention, the magnetic flux generating member is composed of a plurality of permanent magnets, and the thickness of the plurality of permanent magnets (as viewed from the rotor center) in the radial direction is It is characterized by being different depending on the magnet (that is, the magnet thickness in the radial direction varies depending on the magnet).

[0027] また、第 18の発明の電動機の回転子は、磁石を除去した部分に磁石磁束の合算 により磁束の増力 tlした部分に磁束が集中するように着磁した磁石を配置した電動機 の回転子を特徴とする。  [0027] Further, the rotor of the electric motor according to the eighteenth aspect of the present invention is the rotation of an electric motor in which magnets magnetized so that the magnetic flux is concentrated on the portion where the magnetic flux is increased tl by the addition of the magnetic flux to the portion where the magnet is removed. Characterized by a child.

[0028] また、第 19の発明の電動機の回転子は、磁石を除去した部分に磁石磁束の合算 により磁束の増力 tlした部分に磁束が集中するように着磁した磁石を一つ以上の着磁 方向により磁束が集中するように配置した電動機の回転子を特徴とする。 [0028] Further, the rotor of the electric motor according to the nineteenth aspect of the invention is characterized in that one or more magnets magnetized so that the magnetic flux is concentrated on the portion where the magnetic flux is increased tl by the sum of the magnetic flux at the portion where the magnet is removed. It features a motor rotor that is arranged so that the magnetic flux is concentrated depending on the magnetic direction.

[0029] また、第 20の発明の電動機の回転子は、着磁した磁石が一つ以上の磁石の設置 角度により磁束が集中するようにした電動機の回転子であることを特徴とする。 [0029] Further, the rotor of the electric motor of the twentieth invention is characterized in that the magnetized magnet is a rotor of the electric motor such that the magnetic flux is concentrated by the installation angle of one or more magnets.

[0030] また、第 21の発明の電動機の回転子は、着磁した磁石がその 2以上のベクトル合 成によって磁束が集中するようにした電動機の回転子であることを特徴とする。 [0030] Further, the rotor of the electric motor of the twenty-first invention is characterized in that the magnetized magnet is a rotor of the electric motor in which the magnetic flux is concentrated by combining two or more vectors.

[0031] また、第 22の発明の電動機の回転子は、着磁した磁石が一つ以上の磁石と一つ 以上のフラックスノリアにより磁束が集中するようにした電動機の回転子であることを 特徴とする。 [0031] Further, the rotor of the electric motor of the twenty-second invention is an electric motor rotor in which the magnetized magnet concentrates the magnetic flux by one or more magnets and one or more flux noria. And

[0032] 上述したように本発明の解決手段を装置として説明してきたが、本発明はこれらに 実質的に相当する方法としても実現し得るものであり、本発明の範囲にはこれらも包 含されるものと理解された 、。  As described above, the solving means of the present invention has been described as an apparatus, but the present invention can also be realized as a method substantially corresponding to these, and the scope of the present invention includes these as well. It was understood that

図面の簡単な説明  Brief Description of Drawings

[0033] [図 1]本発明の第 1の実施例による回転子を用いた電動機の構成を示す断面図であ る。 FIG. 1 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a first embodiment of the present invention. The

圆 2]第 1の実施例の回転子生成説明図である。 [2] It is a rotor generation explanatory diagram of the first embodiment.

[図 3]2つの正弦波の複合状態の 1例を示す図である。  FIG. 3 is a diagram showing an example of a composite state of two sine waves.

圆 4]2つの正弦波複合によるピーク'平均値等の変化説明図である。 圆 4] It is an explanatory diagram of changes in the peak 'average value etc. due to two sine wave composites.

圆 5]本発明の第 1の実施例による回転子を用いた電動機の構成を示す断面図であ る。 [5] FIG. 5 is a cross-sectional view showing a configuration of an electric motor using the rotor according to the first embodiment of the present invention.

[図 6]第 2の実施例の回転子の説明図である。  FIG. 6 is an explanatory diagram of a rotor according to a second embodiment.

圆 7]第 2の実施例における磁石磁束のピーク値の変化説明図である。 [7] FIG. 7 is an explanatory diagram of changes in the peak value of the magnetic flux in the second embodiment.

圆 8]本発明の第 3の実施例による回転子を用いた電動機の構成を示す断面図であ る。 [8] FIG. 8 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a third embodiment of the present invention.

[図 9]第 3の実施例の回転子の説明図である。  FIG. 9 is an explanatory diagram of a rotor according to a third embodiment.

圆 10]第 3の実施例における誘起電圧ピーク値の変化説明図である。 [10] FIG. 10 is an explanatory diagram of changes in the induced voltage peak value in the third embodiment.

圆 11]第 3の実施例による回転子 (変形例)を用いた電動機の構成を示す断面図で ある。 [11] FIG. 11 is a cross-sectional view showing a configuration of an electric motor using a rotor (modified example) according to a third embodiment.

圆 12]第 3の実施例の回転子 (変形例)の説明図である。 圆 12] It is explanatory drawing of the rotor (modification) of 3rd Example.

圆 13]本発明の第 4の実施例による回転子を用いた電動機の構成を示す断面図で ある。 13] A sectional view showing the configuration of an electric motor using a rotor according to a fourth embodiment of the present invention.

[図 14]第 4の実施例の回転子の説明図である。  FIG. 14 is an explanatory diagram of a rotor according to a fourth embodiment.

圆 15]本発明の第 5の実施例による回転子を用いた電動機の構成を示す断面図で ある。 FIG. 15] A sectional view showing the configuration of an electric motor using a rotor according to a fifth embodiment of the present invention.

[図 16]第 5の実施例の回転子の説明図である。  FIG. 16 is an explanatory diagram of a rotor according to a fifth embodiment.

圆 17]本発明の第 6の実施例による回転子を用いた電動機の構成を示す断面図で ある。 FIG. 17 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a sixth embodiment of the present invention.

[図 18]低磁極数 (2極)の電気角 1周期の磁石領域に対して高磁極数 (4極)の磁石 ( 仮想ロータ)を組み合わせた磁石配置をリニアモデルで表した図である。  FIG. 18 is a diagram showing a linear arrangement of a magnet arrangement in which a magnet with a high magnetic pole number (4 poles) (virtual rotor) is combined with a magnet region with a low magnetic pole number (2 poles) and an electrical angle of one cycle.

圆 19]本発明の第 7の実施例による回転子を用いた電動機の構成を示す断面図で ある。 [19] FIG. 19 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a seventh embodiment of the present invention.

[図 20]低磁極数 (2極)の電気角 1周期の磁石領域に対して高磁極数 (4極)の磁石 ( 仮想ロータ)を組み合わせた磁石配置をリニアモデルで表した図である。 [Figure 20] Magnet with low magnetic pole number (2 poles) and electrical angle of 1 period, magnet with high magnetic pole number (4 poles) It is the figure which represented the magnet arrangement | positioning which combined the virtual rotor) with the linear model.

[図 21]図 17の回転子の機械角 120度のみ取り出した図である(幅を変えた例)。  FIG. 21 is a view showing only the mechanical angle 120 degrees of the rotor of FIG. 17 (an example in which the width is changed).

[図 22]図 17の回転子の機械角 120度のみ取り出した図である (厚さを変えた例)。  FIG. 22 is a view showing only the mechanical angle 120 degrees of the rotor of FIG. 17 (example in which the thickness is changed).

[図 23]この発明の第 8実施の形態に係る電動機の回転子と固定子の構成を概略的 に示す断面説明図である。  FIG. 23 is a cross sectional explanatory view schematically showing a configuration of a rotor and a stator of an electric motor according to an eighth embodiment of the present invention.

[図 24]図 23の磁石における他の着磁方向の例を示す断面説明図である。  24 is a cross-sectional explanatory view showing an example of another magnetization direction in the magnet of FIG.

[図 25] 12スロットの固定子に 4極対の回転子を有するモータの回転子と固定子の構 成を概略的に示す断面説明図である。  FIG. 25 is a cross-sectional explanatory view schematically showing a configuration of a rotor and a stator of a motor having a four-pole pair of rotors in a 12-slot stator.

[図 26] 12スロットの固定子に 8極対の回転子を有するモータの回転子と固定子の構 成を概略的に示す断面説明図である。  FIG. 26 is an explanatory cross-sectional view schematically showing a configuration of a rotor and a stator of a motor having an 8-pole rotor in a 12-slot stator.

[図 27]4極対の回転子と 8極対の回転子を重ね合わせたモータの回転子と固定子の 構成を概略的に示す断面説明図である。  FIG. 27 is a cross-sectional explanatory view schematically showing a configuration of a rotor and a stator of a motor in which a 4-pole rotor and an 8-pole rotor are superimposed.

[図 28]この発明の第 9実施の形態に係る電動機の回転子と固定子の構成を概略的 に示し、(a)は磁石を表面配置した場合の断面説明図、(b)は磁石を埋め込み配置 した場合の断面説明図である。  FIG. 28 schematically shows a configuration of a rotor and a stator of an electric motor according to a ninth embodiment of the present invention. (A) is a cross-sectional explanatory view when the magnet is arranged on the surface. (B) is a diagram illustrating the magnet. FIG. 6 is a cross-sectional explanatory diagram when embedded.

[図 29]この発明の第 10実施の形態に係る電動機の回転子と固定子の構成を概略的 に示し、(a)は磁石を表面配置した場合の断面説明図、(b)は磁石を埋め込み配置 した場合の断面説明図である。  FIG. 29 schematically shows a configuration of a rotor and a stator of an electric motor according to a tenth embodiment of the present invention, in which (a) is a cross-sectional explanatory diagram when magnets are arranged on the surface, and (b) is a diagram illustrating magnets. FIG. 6 is a cross-sectional explanatory diagram when embedded.

[図 30]この発明の第 11実施の形態に係る電動機の回転子と固定子の構成を概略的 に示し、(a)は磁石を表面配置した場合の断面説明図、(b)は磁石を埋め込み配置 した場合の断面説明図である。  FIG. 30 schematically shows a configuration of a rotor and a stator of an electric motor according to an eleventh embodiment of the present invention. (A) is a cross-sectional explanatory view when the magnet is arranged on the surface. (B) is a diagram illustrating the magnet. FIG. 6 is a cross-sectional explanatory diagram when embedded.

発明を実施するための最良の形態  BEST MODE FOR CARRYING OUT THE INVENTION

[0034] 以降、諸図面を参照しつつ、本発明の実施態様を詳細に説明する。  Hereinafter, embodiments of the present invention will be described in detail with reference to the drawings.

[0035] 第 1の実施例  [0035] First Example

図 1は、本発明の第 1の実施例による回転子を用いた電動機の構成を示す断面図 である。まず構成を説明する。 11は固定子であり、 18個の分割されたコア 12から構 成され、 18個の分割されたコア 12には、それぞれ卷線 13が集中的に巻かれている 。この卷線は、 6個おきに配置されている 3個が 1セット(トータル 6セット)となっており 、直列、あるいは並列に接続され、その一方が中性点として他の相の一方と接続されFIG. 1 is a cross-sectional view showing the configuration of an electric motor using a rotor according to a first embodiment of the present invention. First, the configuration will be described. Reference numeral 11 denotes a stator, which is composed of 18 divided cores 12, and each of the 18 divided cores 12 is wound with winding wires 13 in a concentrated manner. In this shoreline, 3 pieces arranged every 6 pieces are 1 set (total 6 sets) Connected in series or in parallel, one of which is connected to one of the other phases as a neutral point

、他方は図示しないインバータの内部で、電源ラインの P側 ·Ν側にスイッチング素子 を介して接続されている。このインバータは 6相を制御する構成となっている。なお、 この固定子は分割されたコアで記述されている力 分割されないコアでも同様の動作 力 Sできること、或いはスロットレス型電動機でも本発明を適用することが可能である。ま た、卷線は集中巻に限らず分布卷でも適用可能である。 The other is inside an inverter (not shown), and is connected to the P side / Ν side of the power supply line via a switching element. This inverter is configured to control 6 phases. Note that this stator can be applied to the same operating force S even with a core that is not divided by the force described by the divided core, or the present invention can be applied to a slotless motor. Also, the shoreline is applicable not only to concentrated winding but also to distributed ridges.

[0036] 14は回転子であり、この実施例では、回転子 14は、 Ν極の 3つ磁石 N1〜N3、 S極 の 6つの磁石 S1〜S6を含み、これらの磁石は 3極対と 6極対の 2種類の極対数を備 える 2組の磁石として機能する。この場合の 2組の磁石は、概念的なものであり、部材 が明確に分離されているものではなぐ固定子の卷線に供給される複合電流を構成 する 1つの電流に対して、 3極対の磁石のセットとして振る舞う磁石の組が 1つあり、複 合電流を構成するもう 1つの電流に対して、 6極対の磁石のセットとして振る舞う磁石 の組が 1つあることを意味するものであり、各磁石 S1〜S6、 Nl〜3が同時に双方の 組の磁石として機能するものである。この詳細については図 2を参照して説明する。 以降、作図や説明の便宜上、回転子の磁石を N極、 S極として図示 *説明するが、 N S極の構成 ·配置を逆に置き換えても発明の作用 ·効果は同様であることに留意さ れたい。 [0036] 14 is a rotor, and in this embodiment, the rotor 14 includes three negative pole magnets N1 to N3 and six negative pole magnets S1 to S6, and these magnets are connected to a three pole pair. It functions as two sets of magnets with two types of pole pairs, six pole pairs. The two sets of magnets in this case are conceptual and have three poles for one current that makes up the combined current supplied to the stator windings that are not clearly separated. Means that there is one set of magnets that behave as a set of pairs of magnets, and one set of magnets that behaves as a set of six pole pairs for the other current that makes up the composite current The magnets S1 to S6 and Nl to 3 function as both sets of magnets at the same time. This will be described in detail with reference to FIG. In the following, for convenience of drawing and explanation, the rotor magnets are shown as N poles and S poles. * The explanation will be made, but it should be noted that the operation and effect of the invention are the same even if the configuration and arrangement of NS poles are reversed. I want to be.

[0037] 図 2は、第 1の実施例の回転子生成説明図であり、図 2の (A)は、 2回転子構造の 電動機の回転子であり、内側回転子が 3極対、外側回転子が 6極対の磁石を備える 。この磁石を内側の回転子の表層に 2層に配置したのが図 2の(B)である。配置の際 に、若干の位相調整をしているがその詳細は後述する。図 2 (B)を見ると、回転子 14 Aは着磁方向の異なる 2種類の磁石(N極、 S極)が幾つかの位置で互いに接してい る。周知のように着磁方向の異なる磁石を張り合わせた場合、双方の磁力が同じであ れば磁石が無 、物と等価である。  [0037] FIG. 2 is an explanatory diagram of the rotor generation of the first embodiment. (A) in FIG. 2 is a rotor of an electric motor having a two-rotor structure. The rotor has 6 pole pairs of magnets. FIG. 2B shows the magnets arranged in two layers on the surface of the inner rotor. A slight phase adjustment is made at the time of arrangement, and the details will be described later. As shown in Fig. 2 (B), the rotor 14A has two types of magnets (N pole and S pole) with different magnetization directions in contact with each other at several positions. As is well known, when magnets with different magnetization directions are bonded together, the magnets are equivalent if they have the same magnetic force.

[0038] そこで、径方向に見て異なる着磁の磁石が張り合わせてある部分力 磁石を排除し たのが図 2 (C)であり、この回転子 14には N極の磁石 N1〜N3, S極の磁石 S1〜S6 が含まれる。この結果、周囲に曲線で示したような、 3極対と 6極対の複合磁束 CFを 発生する回転子 14が完成する。なお、内側回転子と外側回転子とを一体にした構成 である図 2 (B)の構成でも電動機は機能する。つまり、回転子 14Aは、インナーロー タの第 1の回転子とアウターロータの第 2の回転子とを一体ィ匕した構成の回転子であ る。本発明は、さらに、このような構成に改良を加えた、不要な磁石を除去した図 2 (C )の構成を対象とするものであり、削除した磁石分の慣性の低減によるトルクの向上、 電動機の軽量化、削除した磁石の分の経費節減などの効果がある。 [0038] Fig. 2 (C) shows the removal of the partial force magnet with magnets with different magnetizations seen in the radial direction. This rotor 14 has N pole magnets N1 to N3, Includes S-pole magnets S1-S6. As a result, the rotor 14 that generates the composite magnetic flux CF of the three-pole pair and the six-pole pair as shown by a curved line is completed. Note that the inner rotor and outer rotor are integrated. Even in the configuration of Fig. 2 (B), the motor functions. That is, the rotor 14A is a rotor having a configuration in which the first rotor of the inner rotor and the second rotor of the outer rotor are integrated together. The present invention is further directed to the configuration of FIG. 2 (C) in which an unnecessary magnet is removed, which is an improvement to such a configuration, and the torque is improved by reducing the inertia of the deleted magnet. This has the effect of reducing the weight of the motor and reducing the cost of the deleted magnet.

[0039] なお、図 2 (C)では、不要な磁石を除去した領域は空間となっており、空気がその 領域を占めて 、るが、この空気が占める領域は磁束を通さな 、機能を果たして 、る。 即ち、磁石を除去したこの領域には、鉄などの磁束を通し易い素材以外の部材を置 く必要があるが、通常は空間(空気)でこと足りる。もちろん、当該領域には空気以外 の磁束を通しにく ヽ部材が設置されて ヽても力まわな 、。  In FIG. 2 (C), the area from which unnecessary magnets are removed is a space, and air occupies the area. However, the area occupied by air does not pass magnetic flux and functions. Really. That is, it is necessary to place a member other than a material that can easily pass magnetic flux such as iron in this area from which the magnet has been removed, but space (air) is usually sufficient. Of course, there is a saddle member that can pass magnetic fluxes other than air in that area.

[0040] 図 3は、 3極対と 6極対の回転子を駆動させるための正弦波(振幅 1)の各電流、お よびこれらを複合させた複合電流の一例としての各波形を示す。この両者を複合させ る場合、双方の位相によって波形が変化することは容易に想像でき、位相を変化さ せた場合の絶対値のピーク、絶対値の平均値、二乗平均値を示したのが図 4の (A) 、(B)、 (C)である。この正弦波の複合を回転磁束を発生させる電流に適用した場合 には、絶対値のピークはインバータのスイッチング素子容量に関与し、絶対値の平均 値は一定電圧降下を発生する、電力変換器の構成部材であるパワー素子 (IGBTな ど) ·ダイオードなどの損失に関与し、二乗平均値は卷線など一定抵抗での損失に関 与する。  [0040] FIG. 3 shows each current of a sine wave (amplitude 1) for driving a rotor having 3 pole pairs and 6 pole pairs, and each waveform as an example of a composite current obtained by combining these currents. When both are combined, it is easy to imagine that the waveform changes depending on the phase of both, and the peak of the absolute value, the average value of the absolute value, and the mean square value are shown when the phase is changed. These are (A), (B), and (C) in Figure 4. When this sine wave composite is applied to a current that generates rotating magnetic flux, the peak of the absolute value is related to the switching element capacity of the inverter, and the average value of the absolute value is a constant voltage drop. Power element (IGBT, etc.) that is a component • It is related to the loss of the diode, etc., and the mean square value is related to the loss with a constant resistance such as a winding.

[0041] この図を見ると、双方の位相差が 0 (または 30° )の場合に絶対値ピークと絶対値 の平均値とが最小になり、二乗平均値は位相に関係なく一定となることが分る。また 各図には 3極対と 6極対の、それぞれで求めた値の和が別の線で示されており、いず れも複合させた場合の方が小さくなつていることがわかる。したがって、電流を位相差 力 SOとなるように制御すれば、スイッチング素子の容量 · IGBTなどの損失 ·抵抗の損 失、すべてに優位な条件といえる。電流をこの条件とするためには、回転子で発生す る磁束は、 3極対と 6極対それぞれに対して 1Z4周期ずれていることが必要であり、 3 極対については 30° 、6極対については 15° となるので、差し引き 15° ずれていれ ば良い。このことから図 2 (B)では両者の磁石の端が 15° となるように重ね合わせて 、最も損失が少ないような構成にしてある。 [0041] Looking at this figure, when the phase difference between the two is 0 (or 30 °), the absolute value peak and the average value of the absolute value are minimized, and the mean square value is constant regardless of the phase. I understand. In each figure, the sum of the values obtained for the 3-pole pair and the 6-pole pair is shown by separate lines, and it can be seen that both are smaller when combined. Therefore, if the current is controlled so as to have the phase difference SO, it can be said that the switching element capacity, the loss of the IGBT, etc., the loss of the resistance are all favorable conditions. In order for the current to be in this condition, the magnetic flux generated by the rotor must be shifted by 1Z4 period for each of the 3-pole and 6-pole pairs. The pole pair is 15 °, so it is sufficient to deviate by 15 °. Therefore, in Fig. 2 (B), the two magnets are overlapped so that their ends are 15 °. The structure is such that the loss is the least.

[0042] なお、この位相差にっ 、ては、回転子の磁界の磁気飽和を緩和する目的で用いる ならば、上記の位相差 0での構成を回転子の磁石に適用することが考えられる。位相 差に関してはこのように目的によって最適の位相差があり、それぞれ設定されるもの とする。  [0042] If this phase difference is used for the purpose of relaxing the magnetic saturation of the magnetic field of the rotor, it is conceivable to apply the above configuration with the phase difference of 0 to the rotor magnet. . As for the phase difference, there is an optimum phase difference depending on the purpose as described above, and each is set.

[0043] 次に動作を説明する。固定子には前述のように 6相のインバータが接続されており 、これによつて 3極対と 6極対の回転子磁界に対応した複合正弦波磁束を発生するよ うに電流を与えれば良 、。回転子の位置に応じて電流指令を回転させるのは通常の 電動機と同じであるが、この電動機では両極対に対応する複合磁束を発生させるた め、まず 3極対の磁石の組 (セット)に対しては、 3周期の正弦波を発生させるので、ィ ンバータを 6相と考え、正弦波 1周期を 6分割した各位置での電流値を各相の指令値 として計算する。一方、 6極対の磁石の組に対しては、 6周期の正弦波を発生させる ので、正弦波 1周期を 3分割した位置での電流指令値として求め、 6相インバータ第 1 と第 4相、第 2と第 5相、第 3と第 6相の指令値とする。この後、 3極対と 6極対の指令値 それぞれを足し合わせ、 6相インバータの指令値として電流制御を行う。このことで回 転子がトルクを発生し回転する。  Next, the operation will be described. As described above, a 6-phase inverter is connected to the stator, and it is sufficient if current is applied so as to generate a composite sinusoidal magnetic flux corresponding to the rotor magnetic field of 3 pole pairs and 6 pole pairs. ,. The current command is rotated according to the position of the rotor in the same way as a normal motor. However, this motor generates a composite magnetic flux corresponding to both pole pairs. For, a sine wave of 3 cycles is generated. Therefore, the inverter is considered as 6 phases, and the current value at each position obtained by dividing 1 cycle of the sine wave into 6 is calculated as the command value of each phase. On the other hand, a 6-pole pair of magnets generates a 6-cycle sine wave, so the current command value at the position where the 1-cycle sine wave is divided into 3 parts is obtained. The command values for the second and fifth phases and the third and sixth phases are used. After this, the command values of the 3-pole pair and 6-pole pair are added together to perform current control as the command value of the 6-phase inverter. This causes the rotor to generate torque and rotate.

[0044] 次に効果を説明する。上記の動作によりトルクを発生するが、トルクは界磁磁束 (回 転子で発生する磁束)と電流磁束 (固定子で発生する回転磁束)の相互作用によって 発生するが、これは各々の磁束の基本波成分 (この実施例の場合には、 3極対と 6極 対)に応じて発生する。今回の実施例では各々振幅 1の正弦波を複合して得られた 磁束を発生しているので、基本波成分は当然のごとく振幅 1であり、従って振幅 1で 単独で回される電動機に対してほぼ 2倍のトルクを 1つの電動機で発生させることが 理論上可能となる。  Next, the effect will be described. Torque is generated by the above operation. Torque is generated by the interaction of field magnetic flux (magnetic flux generated by the rotor) and current magnetic flux (rotating magnetic flux generated by the stator). It is generated according to the fundamental wave component (in this example, 3 pole pair and 6 pole pair). In this example, since the magnetic flux obtained by combining sine waves with amplitude 1 is generated, the fundamental wave component is naturally amplitude 1, so that for an electric motor that is rotated alone with amplitude 1 It is theoretically possible to generate almost twice the torque with a single motor.

[0045] さらに、その時に流れる電流で発生する損失は、前記のように複合された電流の絶 対値平均'二乗平均、ともに単独の平均値の和より減少しているため、損失は明らか に小さい。以上より、 1つ分の体格の電動機でほぼ 2つ分のトルクを発生しつつ、電 流による損失は電動機 2つ分より小さ 、と 、う効果が得られる。  [0045] Further, since the loss generated by the current flowing at that time is smaller than the sum of the average value of the combined current as described above, the square average, and the single average value, the loss is clear. small. From the above, it is possible to obtain the effect that a motor of one physique generates approximately two torques while the loss due to current is smaller than that of two motors.

[0046] 第 2の実施例 図 5は、本発明の第 2の実施例による回転子を用いた電動機の構成を示す断面図 である。この実施例は、 2極対 ·4極対の回転子に 12スロット 6相の固定子 21を組み 合わせたものである。固定子 21は、 12個のコア 22、 12個の卷線 23を有する。図 6の 回転子 24Αは、図 5の回転子 24と等価のものである。回転子 24に設けてある磁石は Ν極の 2つの磁石 N21、 N22、 S極の 2つの磁石 S21, S22である。 2極対と 4極対の 振幅 1の磁束を複合させ、第 1の実施例のように両者の位相を変化させた時の磁石 磁束のピーク値を図 7に示す。図 7より、双方の位相差が 0° (45° 、90° )の場合に 磁石磁束のピーク値が最小となる。磁石磁束のピークを最小化することで磁気飽和 の発生しにくい電動機を実現できる。このことから図 6では磁石の端が 0° となるよう に重ね合わせており、以降、実施例 1と同様の過程 (不要な磁石を除去)を経て、最 終的には図 5のような回転子構造が得られる。 [0046] Second Example FIG. 5 is a cross-sectional view showing the configuration of an electric motor using a rotor according to the second embodiment of the present invention. In this embodiment, a 12-slot 6-phase stator 21 is combined with a 2-pole / 4-pole pair rotor. The stator 21 has 12 cores 22 and 12 windings 23. The rotor 24Α in FIG. 6 is equivalent to the rotor 24 in FIG. The magnets provided in the rotor 24 are two negative magnets N21 and N22, and two negative S magnets S21 and S22. Fig. 7 shows the peak values of the magnetic flux of the magnet when the two-pole pair and the four-pole pair of magnetic flux with amplitude 1 are combined and the phase of both is changed as in the first embodiment. From Fig. 7, when the phase difference between the two is 0 ° (45 °, 90 °), the peak value of the magnetic flux is minimum. By minimizing the magnetic flux peak, an electric motor that is less likely to cause magnetic saturation can be realized. For this reason, in Fig. 6, the end of the magnet is overlapped so as to be 0 °, and after that, the same process as in Example 1 (removing unnecessary magnets) is performed, and finally, as shown in Fig. 5. A rotor structure is obtained.

第 3の実施例 Third embodiment

図 8から図 12は、第 3の実施例に関する図であり、 2極対 · 6極対の回転子に 18スロ ット 9相の固定子を組み合わせたものである。図 8は、本発明の第 3の実施例による回 転子を用いた電動機の構成を示す断面図である。固定子 31は、 18個のコア 32、 18 個の卷線 33を有する。図 9の回転子 34Aは、図 5の回転子 34と等価のものである。 回転子 34に設けてある磁石は N極の 4つの磁石 N31〜N34、 S極の 4つの磁石 S21 〜S34である。 2極対と 6極対の振幅 1の磁束を複合させ、第 1の実施例のように両者 の位相を変化させた時の誘起電圧のピーク値を図 10に示す。図 10より、双方の位相 差が 0° (60° )の場合に誘起電圧のピーク値が最大となり、 30° (90° )の場合に 誘起電圧のピーク値が最小となる。誘起電圧のピーク値を最大化することで電動機 の高トルク化が可能となり、逆に、誘起電圧のピーク値を最小化することで電動機の 高回転ィ匕が可能となる。このこと力ゝら、図 9では、磁石の端 (磁極の異なる磁石の接触 部)、即ち、位相ゼロ点同士を重ね合うようにして位相差 0° に設定しており、以降、 実施例 1と同様の過程を経て図 8のような回転子構造が得られる。また、図 12では磁 石の端が 30° となるように重ね合わせており、図 11の回転子構造が得られる。固定 子 41は、 18個のコア 42、 18個の卷線 43を有する。図 12の回転子 44Aは、図 11の 回転子 44と等価のものである。回転子 44に設けてある磁石は N極の 2つの磁石 N41 、 N42、 S極の 2つの磁石 S41、 S42である。 FIGS. 8 to 12 are diagrams related to the third embodiment, in which a 2-pole / 6-pole pair rotor is combined with an 18-slot 9-phase stator. FIG. 8 is a cross-sectional view showing the configuration of an electric motor using a rotor according to a third embodiment of the present invention. The stator 31 has 18 cores 32 and 18 windings 33. The rotor 34A in FIG. 9 is equivalent to the rotor 34 in FIG. The magnets provided on the rotor 34 are four N-pole magnets N31 to N34 and four S-pole magnets S21 to S34. Fig. 10 shows the peak value of the induced voltage when the magnetic flux of amplitude 1 of 2 pole pairs and 6 pole pairs is combined and the phase of both is changed as in the first embodiment. From Fig. 10, the peak value of the induced voltage is maximized when the phase difference between the two is 0 ° (60 °), and the peak value of the induced voltage is minimized when it is 30 ° (90 °). Maximizing the peak value of the induced voltage makes it possible to increase the torque of the motor, and conversely, minimizing the peak value of the induced voltage enables high rotation speed of the motor. For this reason, in FIG. 9, the end of the magnet (the contact portion of the magnets with different magnetic poles), that is, the phase zero point is set to overlap with each other, and the phase difference is set to 0 °. The rotor structure shown in Fig. 8 is obtained through the same process. In addition, in Fig. 12, the end of the magnet is overlapped so that it is 30 °, and the rotor structure of Fig. 11 is obtained. The stator 41 has 18 cores 42 and 18 windings 43. The rotor 44A in FIG. 12 is equivalent to the rotor 44 in FIG. The magnets provided on the rotor 44 are two N-pole magnets N41 N42, S magnets with two S poles, S41 and S42.

[0048] 第 4の実施例  [0048] Fourth embodiment

図 13と図 14は第 4の実施例に関する図であり、基本構成は第 2の実施例の図 5と 同様である。図 13は、本発明の第 4の実施例による回転子を用いた電動機の構成を 示す断面図である。固定子 51は、 12個のコア 52、 12個の卷線 53を有する。図 14の 回転子 54Aは、図 13の回転子 54と等価のものである。回転子 54に設けてある磁石 は N極の 4つの磁石 N51〜N54、 S極の 4つの磁石 S51〜S54である。第 2の実施 例との違いは磁石表面形状である。第 2の実施例における磁石表面は、回転子軸心 と同心の円弧形状をしている力 本実施例においては、図 14のように 4極対の磁石 表面が回転子軸心力もの半径より小さい径の円弧形状をなしている。図 14の 2極対 · 4極対の磁石を実施例 1と同様の過程を経て合算して図 13のような回転子構造が得 られる。この回転子構造では、 4極対の磁石の組に相当する磁束は略正弦波形状を なしているため、高調波磁束が少なぐ不要なコギングトルクを低減することが可能と なる。なお、本実施例では 2つの磁極のうち一方のみ正弦波形状とした力 両方の磁 極を正弦波形状とすることも可能である。  13 and 14 are diagrams related to the fourth embodiment, and the basic configuration is the same as that of FIG. 5 of the second embodiment. FIG. 13 is a cross-sectional view showing the configuration of an electric motor using a rotor according to a fourth embodiment of the present invention. The stator 51 has 12 cores 52 and 12 windings 53. The rotor 54A in FIG. 14 is equivalent to the rotor 54 in FIG. The magnets provided on the rotor 54 are four N-pole magnets N51 to N54 and four S-pole magnets S51 to S54. The difference from the second embodiment is the magnet surface shape. The magnet surface in the second embodiment has a circular arc shape that is concentric with the rotor shaft center. In this embodiment, the surface of the 4-pole pair magnet is larger than the radius of the rotor shaft center force as shown in FIG. It has an arc shape with a small diameter. The rotor structure shown in FIG. 13 can be obtained by adding the two-pole / four-pole pairs shown in FIG. 14 through the same process as in Example 1. In this rotor structure, the magnetic flux corresponding to the 4-pole pair of magnets has a substantially sinusoidal shape, so that unnecessary cogging torque with less harmonic magnetic flux can be reduced. In this embodiment, only one of the two magnetic poles can have a sinusoidal shape. Both magnetic poles can have a sinusoidal shape.

[0049] 第 5の実施例  [0049] Fifth embodiment

図 15と図 16は第 5の実施例に関する図であり、基本構成は第 2の実施例の図 5と 同様である。図 15は、本発明の第 5の実施例による回転子を用いた電動機の構成を 示す断面図である。固定子 61は、 12個のコア 62、 12個の卷線 63を有する。図 16の 回転子 64Aは、図 15の回転子 64と等価のものである。回転子 64に設けてある磁石 は N極の 2つの磁石 N61、 N62、 S極の 2つの磁石 S61, S62である。第 2の実施例 との違いは隣り合う磁石の間に間隔を空けている点である。第 2の実施例における磁 石は隣り合う磁石との間に間隔を空けることなく配置している力 本実施例の磁石は 図 16のように隣り合う磁石との間に 22. 5度の間隔を空けており、その間は積層鋼板 のような鉄心部材を配置して 、る。これを合算し実施例 1と同様の過程を経て図 15の 回転子構造が得られる。この配置においては、各磁極の d軸インダクタンスと q軸イン ダクタンスに差が生じるので、磁石トルクにカロえてリラクタンストルクが得られる。  15 and 16 are diagrams relating to the fifth embodiment, and the basic configuration is the same as that of FIG. 5 of the second embodiment. FIG. 15 is a cross-sectional view showing a configuration of an electric motor using a rotor according to a fifth embodiment of the present invention. The stator 61 has twelve cores 62 and twelve winding wires 63. The rotor 64A in FIG. 16 is equivalent to the rotor 64 in FIG. The magnets provided in the rotor 64 are two N-pole magnets N61 and N62, and two S-pole magnets S61 and S62. The difference from the second embodiment is that there is a gap between adjacent magnets. The magnet according to the second embodiment is arranged with no gap between adjacent magnets. The magnet according to the second embodiment has an interval of 22.5 degrees between adjacent magnets as shown in FIG. In the meantime, an iron core member such as a laminated steel plate is arranged. These are added together and the rotor structure shown in FIG. 15 is obtained through the same process as in the first embodiment. In this arrangement, there is a difference between the d-axis inductance and q-axis inductance of each magnetic pole, so reluctance torque can be obtained in addition to the magnet torque.

[0050] 第 6の実施例 (低磁極数側の磁束を強調する構成) 図 17および図 18は第 6の実施例に関する図である。図 17は、本発明の第 6の実施 例による回転子を用いた電動機の構成を示す断面図である。固定子 71は、 18個の コア 72、 18個の卷線 73から構成され、 18個の分割されたコア 72には、それぞれ卷 線 73が集中的に巻かれている。この卷線は、 6個おきに配置されている 3個が 1セット (トータル 6セット)となっており、直列、あるいは並列に接続され、その一方が中性点 として他の相の一方と接続され、他方は図示しないインバータの内部で、電源ライン の P側 ·Ν側にスイッチング素子を介して接続されて 、る。このインバータは前述した ように 6相を制御する構成となっている。なお、この固定子は分割されたコアで記述さ れているが、分割されないコアでも同様の動作ができることは周知のとおりである。ま た卷線は集中巻に限らず分布卷でも適用可能である。 [0050] Sixth embodiment (configuration in which the magnetic flux on the low magnetic pole number side is emphasized) 17 and 18 are diagrams related to the sixth embodiment. FIG. 17 is a cross-sectional view showing a configuration of an electric motor using a rotor according to the sixth embodiment of the present invention. The stator 71 is composed of 18 cores 72 and 18 windings 73, and the windings 73 are wound around the 18 divided cores 72 in a concentrated manner. Three of the windings are arranged in every 6 pieces, and one set (total 6 sets) is connected in series or in parallel, and one of them is connected to one of the other phases as a neutral point The other is connected to the P side and Ν side of the power supply line via a switching element inside an inverter (not shown). As described above, this inverter is configured to control six phases. Although this stator is described with a divided core, it is well known that the same operation can be performed with a core that is not divided. The shoreline is applicable not only to concentrated winding but also to distributed ridges.

[0051] 回転子 74は、この実施例では 3極対と 6極対の 2種類の極対数を備える。回転子 74 の表面には永久磁石が配置される力 その一部の永久磁石 75a〜75dを例に構成 を説明する。永久磁石 75a、 75bは、それぞれ同じ着磁方向であり、回転子 74の中 心 CTR力 外側に向力つて矢印 AR1、AR2のように磁束を発生するように着磁され た磁石である。一方、永久磁石 75c、 75dは、それぞれ同じ着磁方向であり、外側か ら回転子 74の中心 CTRに向力つて矢印 AR3、AR4のように磁束を発生するように 着磁された磁石である。矢印 AR1— 4の線分の長さは、磁束の大きさを模したもので ある。従って、通常は、前者と後者の着磁方向を反対にすれば、前者と後者とで反対 方向の磁束が発生する。  [0051] In this embodiment, the rotor 74 has two types of pole pairs: a three-pole pair and a six-pole pair. The force by which the permanent magnet is disposed on the surface of the rotor 74 will be described with reference to some permanent magnets 75a to 75d as an example. Permanent magnets 75a and 75b are magnets that have the same magnetization direction and are magnetized so as to generate magnetic flux as indicated by arrows AR1 and AR2 by urging outwardly the center CTR force of rotor 74. On the other hand, the permanent magnets 75c and 75d are magnets that have the same magnetization direction and are magnetized so as to generate magnetic flux as indicated by arrows AR3 and AR4 from the outside toward the center CTR of the rotor 74. . The length of the arrow AR1-4 line mimics the magnitude of the magnetic flux. Therefore, normally, if the magnetization directions of the former and the latter are reversed, magnetic fluxes in the opposite direction are generated in the former and the latter.

[0052] 永久磁石 75a、 75cおよび永久磁石 75b、 75dはそれぞれ同じ磁石で構成されて おり、磁石の磁束強さは永久磁石 75a、 75cの方が大きい。また,図 17は表面磁石 形状であるが、埋め込み式磁石形状の回転子でも同様である。ところで、永久磁石 7 5a、 75cは保磁力 ·残留磁束密度が共に優れている希土類磁石で構成され、永久磁 石 75b、 75dは永久磁石 75a、 75cよりも保持力 ·残留磁束密度がどちらか一方もしく は両方劣っている磁石により構成される。例として、永久磁石 75a、 75bはネオジム磁 石が考えられ、永久磁石 75b、 75dには永久磁石 75a、 75bよりも磁石特性の劣るネ オジム磁石やフェライト磁石、アルニコ磁石などが適用できると考えられる。よって、従 来の回転子と比較して高価なネオジム系磁石のコストが低減できる。次にこのような 磁石配置にする理由を図 18で詳細に説明する。 [0052] The permanent magnets 75a and 75c and the permanent magnets 75b and 75d are composed of the same magnet, and the magnetic flux strength of the permanent magnets 75a and 75c is larger. Figure 17 shows the shape of a surface magnet, but the same applies to an embedded magnet-shaped rotor. By the way, the permanent magnets 75a and 75c are composed of rare earth magnets having both excellent coercive force and residual magnetic flux density, and the permanent magnets 75b and 75d have either one of coercive force and residual magnetic flux density than the permanent magnets 75a and 75c. Or both are composed of inferior magnets. As an example, neodymium magnets can be considered for the permanent magnets 75a and 75b, and neodymium magnets, ferrite magnets, alnico magnets, etc., which are inferior to the permanent magnets 75a and 75b, can be applied to the permanent magnets 75b and 75d. . Therefore, the cost of an expensive neodymium magnet can be reduced as compared with a conventional rotor. Then like this The reason for the magnet arrangement will be described in detail with reference to FIG.

[0053] 図 18は、低磁極数(2極)の電気角 1周期の磁石領域に対して高磁極数 (4極)の磁 石 (仮想ロータ)を組み合わせた場合に本発明で考えられる磁石配置をリニアモデル で表した図であり、ロータの円周に沿った展開図である。図 18 (a)は、組み合わせる 前の低磁極数(2極)の仮想ロータを示すものである。図 18 (b)は、組み合わせる前 の高磁極数 (4極)の仮想ロータを示すものである。また、永久磁石内の数字は磁石 磁束の大きさを表し、士は磁石の極性 (即ち、磁束が中心力も外へ向かうか、中心に 向力うかを示す)を表す。図 18では 2極側の磁束を大きく設定している為、組み合わ せた際には永久磁石 75a、 75bおよび永久磁石 75c、 75dはそれぞれ隣合わせの配 置となり、磁束波形は 2極側の成分が強調され易い構成となる。  FIG. 18 shows a magnet considered in the present invention when a magnet (virtual rotor) having a high magnetic pole number (4 poles) is combined with a magnet region having a low magnetic pole number (2 poles) and an electrical angle of 1 period. It is the figure which represented arrangement | positioning with the linear model, and is a development view along the circumference of a rotor. Figure 18 (a) shows a virtual rotor with a low number of magnetic poles (two poles) before combination. Figure 18 (b) shows a virtual rotor with a high number of magnetic poles (4 poles) before combination. The number in the permanent magnet indicates the magnitude of the magnetic flux of the magnet, and the figure indicates the polarity of the magnet (that is, the magnetic flux indicates whether the central force also goes to the outside or to the center). In Fig. 18, the magnetic flux on the 2 pole side is set large, so when combined, the permanent magnets 75a and 75b and the permanent magnets 75c and 75d are arranged next to each other, and the magnetic flux waveform has components on the 2 pole side. The configuration is easily emphasized.

[0054] 第 7の実施例(高磁極数側の磁束を強調する構成)  [0054] Seventh embodiment (configuration in which the magnetic flux on the high magnetic pole number side is emphasized)

図 19は、本発明の第 7の実施例による回転子を用いた電動機の構成を示す断面 図である。固定子 81は、 18個のコア 82、 18個の卷線 83から構成され、 18個の分割 されたコア 82には、それぞれ卷線 83が集中的に巻かれている。回転子 84は、この実 施例では 3極対と 6極対の 2種類の極対数を備える。回転子 84の表面には永久磁石 が配置されるが、その一部の永久磁石 85a〜85dを例に構成を説明する。第 7の実 施例と第 6の実施例との差異は、第 7の実施例では、高磁極数側の磁束が強調され 易い構成になっており、永久磁石 85a、 85d、 85b、 85cのような隣接する磁石力 矢 印 AR5、 AR8、 AR6、 AR7のように交互に磁束の方向がスィッチする構成になって いる。このように磁束発生方向が磁石毎に交互になるような磁石の組の組み合わせ を図 20に示す。  FIG. 19 is a cross-sectional view showing a configuration of an electric motor using a rotor according to the seventh embodiment of the present invention. The stator 81 is composed of 18 cores 82 and 18 windings 83, and the windings 83 are concentrated around the 18 divided cores 82. In this embodiment, the rotor 84 has two types of pole pairs: a 3-pole pair and a 6-pole pair. Permanent magnets are arranged on the surface of the rotor 84, and the configuration will be described with some permanent magnets 85a to 85d as an example. The difference between the seventh embodiment and the sixth embodiment is that in the seventh embodiment, the magnetic flux on the high magnetic pole number side is easily emphasized, and the permanent magnets 85a, 85d, 85b, 85c The adjacent magnetic force arrows AR5, AR8, AR6, and AR7 are configured to alternately switch the direction of magnetic flux. Fig. 20 shows a combination of magnet sets in which the direction of magnetic flux generation alternates for each magnet.

[0055] 図 20は、低磁極数(2極)の電気角 1周期の磁石領域に対して高磁極数 (4極)の磁 石 (仮想ロータ)を組み合わせた場合に本発明で考えられる磁石配置をリニアモデル で表した図であり、ロータの円周に沿った展開図である。 4極側の磁束を大きく設定し ている為、組み合わせた際には永久磁石 85a、 85dおよび永久磁石 85c、 85bがそ れぞれ隣合わせの配置となり、磁束波形は 4極側の成分が強調され易い構成となる。  [0055] Fig. 20 shows a magnet considered in the present invention when a magnet (virtual rotor) having a high magnetic pole number (4 poles) is combined with a magnet region having a low magnetic pole number (2 poles) and an electrical angle of 1 period. It is the figure which represented arrangement | positioning with the linear model, and is a development view along the circumference of a rotor. Since the magnetic flux on the 4-pole side is set large, when combined, the permanent magnets 85a and 85d and the permanent magnets 85c and 85b are arranged next to each other, and the magnetic flux waveform emphasizes the 4-pole side component. Easy configuration.

[0056] なお、図 18、図 20では組み合わせに使用した 2極と 4極の磁石位相は 1種類である 力、これらの磁石に任意の位相差を持たせた場合も同じ考え方により様々な磁石配 置が考えられる。また、この例では 2極と 4極の組み合わせを説明した力 別の極数の 組み合わせでも同様に考えられる。 [0056] In FIGS. 18 and 20, the two-pole and four-pole magnet phases used in the combination are one type of force, and various magnets can be obtained using the same concept even when these magnets have an arbitrary phase difference. Arrangement Can be considered. In this example, the combination of the number of poles according to force, which explains the combination of two and four poles, can be considered similarly.

[0057] 永久磁石 75a〜75d、 85a〜85dの磁石の磁石幅は同じにする必要はない。図 21 に、図 17の回転子の機械角 120度のみ取り出した図を示す (幅を変えた例)。永久磁 石 75a、 75cと永久磁石 75b、 75dはそれぞれ同じ種類の磁石であり、永久磁石 75a 、 75cの磁石最大幅が Wa、永久磁石 75b、 75dの磁石最大幅が Wbである。幅 Wa、 幅 Wbの長さを変えることによって、これらを構成する磁極数の磁束レベル (強度)を 変えることができる。「幅 ^^^ 幅^^!)」とすると 2極側の磁束が大きくなり、「幅 Waく幅 Wb」とすると 4極側の磁束が大きくなる構成となる。  [0057] The permanent magnets 75a to 75d and 85a to 85d need not have the same magnet width. Fig. 21 shows a diagram in which only the mechanical angle of 120 degrees of the rotor in Fig. 17 is taken out (example in which the width is changed). The permanent magnets 75a and 75c and the permanent magnets 75b and 75d are the same type of magnet, the permanent magnets 75a and 75c have the maximum magnet width Wa, and the permanent magnets 75b and 75d have the maximum magnet width Wb. By changing the length of the width Wa and the width Wb, the magnetic flux level (strength) of the number of magnetic poles constituting them can be changed. “Width ^^^ Width ^^!)” Increases the magnetic flux on the 2-pole side, and “width Wa and width Wb” increases the magnetic flux on the 4-pole side.

[0058] 永久磁石 75a〜75dの磁石厚についても同様に同じにする必要はない。図 22に図 17の回転子の機械角 120度のみ取り出した図を示す (厚さを変えた例)。永久磁石 7 5a、 75cと永久磁石 75b、 75dはそれぞれ同じ種類の磁石であり、永久磁石 75a、 75 cの磁石最大厚さが Ta、永久磁石 75b、 75dの磁石最大厚さが Tbである。アルニコ などの磁石は保持力が低いため磁石厚が薄すぎる場合は減磁し易くなり、それぞれ の磁石特性に合わせた磁石厚を設定する必要がある。また磁石厚をある程度まで上 げることによって磁石磁束を増加させることができるため、 2極と 4極の磁束レベルを変 えることができる。ただし、磁石厚を厚くし過ぎても磁石磁束密度はしだいに飽和し、 磁気抵抗が増加するため効果が得られないのは周知である。  Similarly, the magnet thicknesses of the permanent magnets 75a to 75d need not be the same. FIG. 22 shows a diagram in which only the mechanical angle of 120 degrees of the rotor of FIG. 17 is taken out (example in which the thickness is changed). The permanent magnets 75a and 75c and the permanent magnets 75b and 75d are the same type of magnet. The maximum magnet thickness of the permanent magnets 75a and 75c is Ta, and the maximum magnet thickness of the permanent magnets 75b and 75d is Tb. Magnets such as Alnico have low holding power, so if the magnet thickness is too thin, it will be easy to demagnetize, and it is necessary to set the magnet thickness according to the respective magnet characteristics. Moreover, since the magnetic flux can be increased by increasing the magnet thickness to some extent, the magnetic flux levels of the 2-pole and 4-pole can be changed. However, it is well known that even if the magnet thickness is increased too much, the magnetic flux density is gradually saturated and the magnetic resistance increases, so that no effect is obtained.

[0059] 次に、第 6および第 7の実施例による電動機の動作を説明する。固定子には先述の ように 6相のインバータが接続されており、これによつて 3極対と 6極対の回転子磁界 に対応した複合正弦波磁束を発生するように電流を与えれば良 、。回転子の位置に 応じて電流指令を回転させるのは通常の電動機と同じであるが、この電動機では両 極対に対応する複合磁束を発生させるため、まず 3極対に対しては、 3周期の正弦波 を発生させるので、インバータを 6相と考え、正弦波 1周期を 6分割した各位置での電 流値を各相の指令値として計算する。一方、 6極対に対しては、 6周期の正弦波を発 生させるので、正弦波 1周期を 3分割した位置での電流指令値として求め、 6相イン バータ第 1と第 4相、第 2と第 5相、第 3と第 6相の指令値とする。この後 3極対と 6極対 の指令値それぞれを足し合わせ、 6相インバータの指令値として電流制御を行う。こ のことで回転子がトルクを発生し回転する。 Next, the operation of the electric motor according to the sixth and seventh embodiments will be described. A 6-phase inverter is connected to the stator as described above, and it is sufficient to apply current to generate a composite sinusoidal magnetic flux corresponding to the rotor magnetic field of 3 pole pairs and 6 pole pairs. ,. The current command is rotated according to the position of the rotor in the same way as a normal motor. However, this motor generates a composite magnetic flux corresponding to both pole pairs. Therefore, the inverter is considered to have 6 phases, and the current value at each position obtained by dividing one cycle of the sine wave into 6 is calculated as the command value for each phase. On the other hand, for a 6-pole pair, a 6-cycle sine wave is generated, so it is obtained as a current command value at a position where one sine wave cycle is divided into 3 parts, and the 6-phase inverter first, fourth, The command values for Phases 2 and 5 and Phases 3 and 6 are used. After this, the command values of the 3 pole pair and 6 pole pair are added together to control the current as the command value of the 6-phase inverter. This As a result, the rotor generates torque and rotates.

[0060] 次に、第 6および第 7の実施例による電動機の効果を説明する。上記の動作によりト ルクを発生するが、トルクは界磁磁束 (回転子で発生する磁束)と電流磁束 (固定子で 発生する回転磁束)の相互作用によって発生する力 これは各々の磁束の基本波成 分 (この実施例の場合には、 3極対と 6極対)に応じて発生する。今回の実施例 1では 3極と 6極のトルクが合算されたトルクが生じる。従来の回転子は 1つの回転子内の磁 石はすべて同じ特性の磁石を使用するが、本発明では磁石特性が低!、磁石を入れ ることにより低コストィ匕を図り尚且つ従来通りのトルクを発生することができる。さらにそ の時に流れる電流で発生する損失は、前記のように複合された電流の絶対値平均 · 二乗平均、ともに単独の平均値の和より減少しているため、損失は明らかに小さい。 以上より、 1つ分の体格の電動機で 2つ分のトルクを発生しつつ、電流による損失は 電動機 2つ分より小さ 、と 、う効果が得られる。  Next, effects of the electric motors according to the sixth and seventh embodiments will be described. Torque is generated by the above operation, but torque is the force generated by the interaction of field magnetic flux (magnetic flux generated by the rotor) and current magnetic flux (rotational magnetic flux generated by the stator). It is generated according to wave components (in this example, 3 pole pairs and 6 pole pairs). In Example 1 of this time, torque that is the sum of torques of 3 poles and 6 poles is generated. In the conventional rotor, all the magnets in one rotor use magnets having the same characteristics, but in the present invention, the magnet characteristics are low! Can be generated. Furthermore, since the loss generated by the current flowing at that time is smaller than the sum of the absolute value average and the square average of the combined current as described above, and the single average value, the loss is clearly small. From the above, it is possible to obtain the effect of generating a torque equivalent to two motors with one electric motor and having a smaller loss than that of two electric motors.

[0061] (第 8実施の形態)  [0061] (Eighth embodiment)

図 23乃至図 27は、この発明の第 8実施の形態に係る電動機の回転子と固定子の 構成を概略的に示す断面説明図である。図 24は、図 23の磁石における他の着磁方 向の例を示す断面説明図である。なお、図中の矢印は磁石の着磁方向を示しており 、他の図においても同様である。  FIGS. 23 to 27 are cross-sectional explanatory views schematically showing the configurations of the rotor and the stator of the electric motor according to the eighth embodiment of the present invention. FIG. 24 is an explanatory cross-sectional view showing another example of the magnetization direction in the magnet of FIG. In addition, the arrow in a figure has shown the magnetization direction of the magnet, and it is the same also in another figure.

[0062] 図 23に示すように、電動機 10は、異なる複数の磁極数に相当する磁石磁束を合 算して発生させる回転子 94を有する複合磁束電動機であり、磁石磁束の合算による 磁束の減少部であるフラックスノリア部に、着磁方向を持つ磁石 112a, 112bからな る磁石 112を配置して!/、る。  [0062] As shown in Fig. 23, the electric motor 10 is a composite magnetic flux motor having a rotor 94 that generates a magnetic flux corresponding to a plurality of different magnetic pole numbers, and reduces the magnetic flux by adding the magnetic flux. A magnet 112 made up of magnets 112a and 112b having a magnetization direction is arranged in the flux noria part which is a part!

[0063] フラックスノリア部に配置された磁石 112は、磁石磁束の合算による磁束の増加部 方向に磁束が集中するように、着磁方向が一方向以上の多方向となるように着磁さ れている。この磁石 112の着磁方向は、図 24に示すように、単一角度ではなく複数 の異なった傾き角度を有する多方向磁束の集合(図中、矢印参照)により一方向を形 成しても良い。これにより、簡易な磁石 112の配置によって、磁石設置スペースを新 たに確保することなくトルクを向上させることができ、或いは同等のトルクを少ない磁 石量で発生させることができる。 [0064] この複合磁束電動機である電動機 10は、 4極対のロータと 8極対のロータを重ね合 わせた構成を有している。 [0063] The magnet 112 arranged in the flux noria part is magnetized so that the magnetization direction is one direction or more in multiple directions so that the magnetic flux is concentrated in the direction of the magnetic flux increasing part by the sum of the magnetic fluxes. ing. As shown in FIG. 24, the magnetization direction of the magnet 112 is not a single angle, but a single direction may be formed by a set of multidirectional magnetic fluxes having a plurality of different tilt angles (see arrows in the figure). good. As a result, the simple arrangement of the magnet 112 can improve the torque without newly securing a magnet installation space, or can generate an equivalent torque with a small amount of magnetism. [0064] The electric motor 10 as the composite magnetic flux motor has a configuration in which a 4-pole rotor and an 8-pole rotor are overlapped.

[0065] 図 25は、 12スロットの固定子に 4極対の回転子を有する電動機の回転子と固定子 の構成を概略的に示す断面説明図である。図 26は、 12スロットの固定子に 8極対の 回転子を有する電動機の回転子と固定子の構成を概略的に示す断面説明図である 。図 27は、 4極対の回転子と 8極対の回転子を重ね合わせた電動機の回転子と固定 子の構成を概略的に示す断面説明図である。  FIG. 25 is an explanatory cross-sectional view schematically showing a configuration of a rotor and a stator of an electric motor having a 4-pole pair of rotors in a 12-slot stator. FIG. 26 is a cross-sectional explanatory view schematically showing a configuration of a rotor and a stator of an electric motor having an 8-pole pair of rotors in a 12-slot stator. FIG. 27 is an explanatory cross-sectional view schematically showing a configuration of a rotor and a stator of an electric motor in which a 4-pole rotor and an 8-pole rotor are superimposed.

[0066] 図 25に示すように、電動機 10は、スロット 91aの数が 12の固定子 91、及び 4極対 の磁石 115が配置されたロータ 104を有する低磁極数電動機であり、図 26に示すよ うに、電動機 10は、スロット 91aの数が 12の固定子 91、及び 8極対の磁石 115が配 置されたロータ 114を有する高磁極数電動機である。そして、図 27に示すように、電 動機 10の 4極対のロータ 104 (図 25参照)と、電動機 10の 8極対のロータ 114 (図 26 参照)を重ね合わせた構成を有する電動機 10は、ロータ 124のロータ径方向におい て異極同士重なる部分がフラックスノリア部 120aと見なされる。これは、ロータ径方 向において異極同士が重なる部分は、着磁方向が相反することにより相殺されるた めである。  [0066] As shown in FIG. 25, the electric motor 10 is a low magnetic pole number electric motor having a stator 91 having 12 slots 91a and a rotor 104 in which four pole pairs of magnets 115 are arranged. As shown, the electric motor 10 is a high magnetic pole number electric motor having a stator 91 having twelve slots 91a and a rotor 114 in which eight pole pairs of magnets 115 are arranged. As shown in FIG. 27, the electric motor 10 having a configuration in which the four-pole rotor 104 of the electric motor 10 (see FIG. 25) and the eight-pole rotor 114 of the electric motor 10 (see FIG. 26) are overlapped. In the rotor radial direction of the rotor 124, the portion where the different poles overlap is regarded as the flux noria portion 120a. This is because the portion where the different polarities overlap in the rotor radial direction is canceled by the opposite magnetization directions.

[0067] つまり、 4極対のロータと 8極対のロータを重ね合わせた構成を有する複合磁束電 動機である電動機 10には、ロータ 94の磁石磁束合算による磁束減少部であるフラッ クスノ リア部と見なされる部分に、この部分に隣接する磁石磁束合算による磁束増加 部の方向に磁束が集中するように着磁した磁石 112a, 112bから構成される磁石 11 2 (023, 24参照)が、配置されている。  That is, in the electric motor 10 which is a composite magnetic flux motor having a configuration in which a 4-pole pair rotor and an 8-pole pair rotor are superposed, a flux NOROR portion which is a magnetic flux reduction portion by the combined magnetic flux of the rotor 94 is provided. A magnet 11 2 (see 023, 24) composed of magnets 112a and 112b magnetized so that the magnetic flux is concentrated in the direction of the magnetic flux increasing part by the sum of the magnet magnetic flux adjacent to this part Has been.

[0068] このように、正弦波を複合して得られた磁束を発生して!/、る電動機 10は、異なる複 数の磁極数に相当する磁石磁束をその表面に合算して発生させる磁束発生部材を 持つ回転子 94と、この複数の磁極数に対応した複数の電流磁界を合算し、且つ、回 転させることができるように電流を与えられる固定子 91の、何れか一方、或いは両方 を備え、回転子 94の磁石磁束の合算により磁束の減少した部分であるフラックスバリ ァ部に、磁石磁束の合算により磁束の増力!]した部分に磁束が集中するように、ー以 上の方向に着磁した磁石 12を配置して 、る。 [0069] 即ち、磁石磁束の合算による磁束の減少部であるフラックスバリア部と見なされる部 分の少なくとも一部を、この部分に隣接する磁石磁束の合算による磁束の増加部方 向に磁束を集中させた磁石に置き換えることで、磁石設置スペースを新たに確保す ることなくトルクを向上させることができ、或いは同等のトルクを少ない磁石量で発生さ せることができる。 [0068] In this way, the electric motor 10 that generates the magnetic flux obtained by combining the sine waves generates the magnetic flux corresponding to the different number of magnetic poles on the surface. One or both of a rotor 94 having a generating member and a stator 91 to which a current is applied so that a plurality of current magnetic fields corresponding to the number of magnetic poles can be combined and rotated. In order to concentrate the magnetic flux on the flux barrier part where the magnetic flux decreased due to the sum of the magnet magnetic flux of the rotor 94, and on the part where the magnetic flux increased due to the sum of the magnetic flux! Place magnet 12 magnetized on [0069] That is, at least a part of the part regarded as a flux barrier part, which is a magnetic flux decreasing part due to the sum of the magnet magnetic fluxes, is concentrated in the direction of the magnetic flux increasing part due to the sum of the magnet magnetic fluxes adjacent to this part. By replacing the magnet with the magnet, the torque can be improved without newly securing a magnet installation space, or the equivalent torque can be generated with a small magnet amount.

[0070] このように、そもそも磁石を配置しな 、領域 (複合磁束を作るためには必要な磁束 空白領域)に補助磁極を配置しているので、補助磁極の配置によるスペース効率が 悪ィ匕することはない。つまり、複合磁束ロータと補助磁極電動機の組み合わせは、補 助磁極電動機にぉ 、て確保しなければならな 、磁石設置スペースが必然的に存在 するので、補助磁極電動機にとって不利となる点が構成上発生しないので、より効果 的である。  [0070] As described above, since the auxiliary magnetic pole is arranged in the region (the magnetic flux blank region necessary for producing the composite magnetic flux) without arranging the magnet in the first place, the space efficiency due to the arrangement of the auxiliary magnetic pole is poor. Never do. In other words, the combination of the composite magnetic flux rotor and the auxiliary magnetic pole motor must be secured for the auxiliary magnetic pole motor, and a magnet installation space inevitably exists, which is disadvantageous for the auxiliary magnetic pole motor. Since it does not occur, it is more effective.

[0071] (第 9実施の形態)  [0071] (Ninth embodiment)

図 28は、この発明の第 9実施の形態に係る電動機の回転子と固定子の構成を概略 的に示し、(a)は磁石を表面配置した場合の断面説明図、(b)は磁石を埋め込み配 置した場合の断面説明図である。図 28に示すように、電動機 10は、ロータ 134の磁 石磁束の合算による磁束の減少部であるフラックスノリア部 120a (図 27参照)に、磁 石磁束の合算による磁束の増加部方向に磁束が集中するように、 1つ以上の設置角 度を設けた磁石 127を配置している。その他の構成及び作用は、電動機 10と同様で ある。  FIG. 28 schematically shows a configuration of a rotor and a stator of an electric motor according to a ninth embodiment of the present invention. (A) is a cross-sectional explanatory view when the magnet is arranged on the surface, and (b) is a diagram of the magnet. FIG. 5 is a cross-sectional explanatory diagram when embedded. As shown in FIG. 28, the electric motor 10 has a magnetic flux in the direction of the magnetic flux increasing portion due to the sum of the magnetic fluxes in the flux noria portion 120a (see FIG. 27) that is the magnetic flux decreasing portion due to the sum of the magnetic fluxes of the rotor 134. The magnet 127 with one or more installation angles is arranged so that can be concentrated. Other configurations and operations are the same as those of the motor 10.

[0072] つまり、電動機 10には、ロータ 134の磁石磁束合算による磁束減少部であるフラッ タスバリア部 126aと見なされる部分の少なくとも一部を、この部分に隣接する磁石磁 束合算による磁束増加部の方向に磁束が集中する角度に設置した磁石 127a, 127 b (図 28参照)力も構成される磁石 27に、置き換えて 、る。  That is, in the electric motor 10, at least a part of the portion regarded as the flats barrier portion 126a, which is a magnetic flux reduction portion by the magnetic flux summation of the rotor 134, is added to the magnetic flux increase portion by the magnetic flux summation adjacent to this portion. The magnets 127a and 127b (see FIG. 28) installed at angles at which magnetic flux concentrates in the direction are replaced with magnets 27 that are also configured.

[0073] これにより、磁石 127に一般的な形状の磁石を用いれば、磁石設置スペースを新た に確保することなく低コストでトルクを向上させることができ、或いは同等のトルクを少 な 、磁石量で発生させることができる。  [0073] Thus, if a magnet with a general shape is used as the magnet 127, the torque can be improved at low cost without newly securing a magnet installation space, or the equivalent torque can be reduced with a small amount of magnet. Can be generated.

[0074] (第 10実施の形態)  [0074] (Tenth embodiment)

図 29は、この発明の第 10実施の形態に係る電動機の回転子と固定子の構成を概 略的に示し、(a)は磁石を表面配置した場合の断面説明図、(b)は磁石を埋め込み 配置した場合の断面説明図である。図 29に示すように、電動機 10は、ロータ 144の 磁石磁束の合算による磁束の減少部であるフラックスノリア部 120a (図 27参照)を、 磁石磁束の合算による磁束の増加部方向に磁束が集中するような合成ベクトルが形 成できるように、 2つ以上の磁石 132を配置している。 FIG. 29 schematically shows the configuration of the rotor and stator of the electric motor according to the tenth embodiment of the present invention. It is shown schematically, (a) is a cross-sectional explanatory diagram when magnets are arranged on the surface, and (b) is a cross-sectional explanatory diagram when magnets are embedded and arranged. As shown in FIG. 29, the electric motor 10 has a magnetic flux concentrated in the direction of the magnetic flux increasing portion 120a (see FIG. 27), which is the magnetic flux decreasing portion due to the sum of the magnetic fluxes of the rotor 144. Two or more magnets 132 are arranged so that a composite vector can be formed.

[0075] つまり、電動機 10には、ロータ 144の磁石磁束合算による磁束減少部であるフラッ クスノリア部と見なされる部分の少なくとも一部を、この部分に隣接する磁石磁束合 算による磁束増加部の方向に磁束を集中させる合成磁束ベクトルを形成する複数( この f列で ίま、 3偶)の磁石 132a, 132b, 132c【こ、置き換えて ヽる。  That is, in the electric motor 10, at least a part of the portion of the rotor 144 that is considered to be a flux noria part, which is a magnetic flux reduction part by the sum of magnet magnetic fluxes, is directed to the direction of the magnetic flux increase part by the sum of the magnet magnetic fluxes adjacent to this part. A plurality of magnets 132a, 132b, 132c that form a composite magnetic flux vector that concentrates the magnetic flux on the magnet (this f row is ί, 3 even) can be replaced.

[0076] これにより、磁石の表面積を稼げることから、磁石設置スペースを新たに確保するこ となくより一層、トルクを向上させることができ、或いは同等のトルクを少ない磁石量で 発生させることができる。  [0076] Thereby, since the surface area of the magnet can be increased, the torque can be further improved without newly securing a magnet installation space, or the equivalent torque can be generated with a small magnet amount. .

[0077] (第 11実施の形態)  [0077] (Eleventh embodiment)

図 30は、この発明の第 11の実施の形態に係る電動機の回転子と固定子の構成を 概略的に示し、(a)は磁石を表面配置した場合の断面説明図、(b)は磁石を埋め込 み配置した場合の断面説明図である。図 30に示すように、電動機 10は、ロータ 154 の磁石磁束の合算による磁束の減少部であるフラックスノリア部(図 27参照)に、磁 石磁束の合算による磁束の増加部方向に磁束が集中するように、 1つ以上の磁石 13 7と 1つ以上のフラックスバリア部 138を配置している。  FIG. 30 schematically shows a configuration of a rotor and a stator of an electric motor according to an eleventh embodiment of the present invention, (a) is a cross-sectional explanatory diagram when magnets are arranged on the surface, and (b) is a magnet FIG. As shown in FIG. 30, in the electric motor 10, the magnetic flux is concentrated in the direction of the magnetic flux increasing portion due to the sum of the magnetic fluxes in the flux noria portion (see FIG. 27), which is the magnetic flux decreasing portion due to the sum of the magnetic fluxes of the rotor 154. One or more magnets 137 and one or more flux barrier portions 138 are arranged.

[0078] つまり、電動機 10には、ロータ 154の磁石磁束合算による磁束減少部であるフラッ タスバリア部と見なされる部分の少なくとも一部を、この部分に隣接する磁石磁束の 合算による磁束の増加部方向に磁束を集中させた磁石 137a, 137bと、両磁石 137 a, 137bの外周側に位置するフラックスノ リア部 138に、置き換えている。  That is, in the electric motor 10, at least a part of the portion of the rotor 154, which is regarded as a flattened barrier portion, which is a magnetic flux decreasing portion due to the sum of the magnetic fluxes of the rotor, Are replaced by magnets 137a and 137b in which magnetic flux is concentrated, and a flux noor part 138 located on the outer peripheral side of both magnets 137a and 137b.

[0079] これにより、磁石の容易な配置で、且つ、一般的な形状の磁石を用いれば低コスト で、磁石設置スペースを新たに確保することなくトルクを向上させることができ、或い は同等のトルクを少ない磁石量で発生させることができる。  [0079] This makes it possible to improve the torque with a simple arrangement of magnets and at a low cost if a magnet having a general shape is used, and without securing a new magnet installation space, or equivalently. Torque can be generated with a small amount of magnet.

[0080] 上述したように、この発明に係る電動機は、異なる複数の磁極数に相当する磁石磁 束を、その表面に合算して発生させる磁束発生部材を持つ回転子と、この複数の磁 極数に対応した複数の電流磁界を合算し、且つ、回転させることができるように電流 を与えられる固定子の、少なくとも一方を備え、磁石磁束の合算により磁束の減少し た部分に、磁石磁束の合算により磁束の増力!]した部分に磁束が集中するように着磁 した磁石を配置している。 [0080] As described above, the electric motor according to the present invention includes a rotor having a magnetic flux generating member for generating a magnetic flux corresponding to a plurality of different magnetic poles on its surface, and the plurality of magnets. At least one of the stators to which a current can be applied so that a plurality of current magnetic fields corresponding to the number of poles can be rotated and rotated is provided, and the magnetic flux is reduced at the portion where the magnetic flux is reduced by adding the magnetic flux. The magnets are magnetized so that the magnetic flux concentrates on the part where the magnetic flux is increased by adding together!].

[0081] つまり、磁石磁束の合算による磁束の減少部であるフラックスノリア部の一部又は 全部を磁石に置き換え、磁石磁束の合算による磁束の増加部方向に磁束を集中さ せることで、磁石設置スペースを新たに確保することなくトルクの向上が可能であり、 更に小型化を実現することができる。  [0081] That is, by replacing part or all of the flux noria part, which is a magnetic flux decrease part due to the sum of magnet magnetic fluxes, with a magnet, and concentrating the magnetic flux in the direction of the magnetic flux increase part due to the sum of magnet magnetic fluxes, The torque can be improved without securing a new space, and further downsizing can be realized.

[0082] また、磁石磁束の合算により磁束の減少した部分の少なくとも一部に配置する磁石 の磁束を、一以上の着磁方向によって、磁石磁束の合算により磁束の増力!]した部分 に集中させている。つまり、磁石磁束の合算による磁束の減少部であるフラックスバリ ァ部の一部又は全部を、磁石磁束の合算による磁束の増加部方向に磁束が集中す るよう着磁した磁石に置き換えることで、簡易な磁石配置で、磁石設置スペースを新 たに確保することなくトルクを向上させることができ、或いは同等のトルクを少ない磁 石量で発生させることができる。  [0082] Further, the magnetic flux of the magnet disposed in at least a part of the portion where the magnetic flux is reduced due to the sum of the magnetic fluxes is concentrated on the portion where the magnetic flux is increased due to the sum of the magnet magnetic fluxes according to one or more magnetization directions. ing. In other words, by replacing a part or all of the flux barrier part, which is the magnetic flux decrease part due to the sum of the magnet magnetic fluxes, with a magnet magnetized so that the magnetic flux concentrates in the direction of the magnetic flux increase part due to the sum of the magnet magnetic fluxes, With a simple magnet arrangement, torque can be improved without newly securing a magnet installation space, or equivalent torque can be generated with a small amount of magnet.

[0083] また、磁石磁束の合算により磁束の減少した部分の少なくとも一部に配置する磁石 の磁束を、 1以上の磁石の設置角度によって、磁石磁束の合算により磁束の増加し た部分に集中させている。つまり、磁石磁束の合算による磁束の減少部であるフラッ クスノリア部の一部又は全部を、磁石磁束の合算による磁束の増加部方向に磁束が 集中するよう設置角度を設けた磁石に置き換えることで、一般的な形状の磁石を用 いれば低コストで、磁石設置スペースを新たに確保することなくトルクを向上させるこ とができ、或いは同等のトルクを少ない磁石量で発生させることができる。  [0083] In addition, the magnetic flux of the magnet disposed in at least a part of the portion where the magnetic flux is reduced due to the sum of the magnetic fluxes is concentrated on the portion where the magnetic flux is increased due to the sum of the magnetic flux depending on the installation angle of one or more magnets. ing. In other words, by replacing a part or all of the flux noria part, which is a magnetic flux decrease part due to the sum of magnet magnetic fluxes, with a magnet having an installation angle so that the magnetic flux concentrates in the direction of the magnetic flux increase part due to the sum of magnet magnetic fluxes, If a magnet having a general shape is used, the torque can be improved at a low cost without newly securing a magnet installation space, or an equivalent torque can be generated with a small amount of magnet.

[0084] また、磁石磁束の合算により磁束の減少した部分の少なくとも一部に配置する磁石 の磁束を、 2以上の磁束のベクトル合成によって、磁石磁束の合算により磁束の増加 した部分に集中させている。つまり、磁石磁束の合算による磁束の減少部であるフラ ックスバリア部の一部又は全部を、磁石磁束の合算による磁束の増加部方向に磁束 を集中させる合成磁束ベクトルを作る複数の磁石に置き換えることで、磁石の表面積 を稼げるため、磁石設置スペースを新たに確保することなぐより一層トルクを向上さ せることができ、或いは同等のトルクを少ない磁石量で発生させることができる。 [0084] In addition, the magnetic flux of the magnet arranged at least in a portion where the magnetic flux is reduced due to the sum of the magnetic fluxes is concentrated on the portion where the magnetic flux is increased due to the sum of the magnetic fluxes by vector synthesis of two or more magnetic fluxes. Yes. In other words, by replacing some or all of the flux barrier part, which is the magnetic flux decrease part due to the sum of the magnet magnetic fluxes, with a plurality of magnets that create a composite magnetic flux vector that concentrates the magnetic flux in the direction of the magnetic flux increase part due to the sum of the magnet magnetic fluxes. In order to increase the surface area of the magnet, the torque is further improved without securing a new magnet installation space. Or an equivalent torque can be generated with a small amount of magnets.

[0085] また、磁石磁束の合算により磁束の減少した部分の少なくとも一部に配置する磁石 の磁束を、 1以上の磁石と 1以上のフラックスノ《リアによって、前記磁石磁束の合算に より磁束の増カロした部分に集中させている。つまり、磁石磁束の合算による磁束の減 少部であるフラックスノリア部の一部又は全部を、磁石磁束の合算による磁束の増加 部方向に磁束が集中するように磁石とフラックスノリアに置き換えることにより、簡易な 配置で、且つ、一般的な形状の磁石を用いれば低コストで、磁石設置スペースを新 たに確保することなくトルクを向上させることができ、或いは同等のトルクを少ない磁 石量で発生させることができる。  [0085] In addition, the magnetic flux of the magnet disposed in at least a part of the portion where the magnetic flux is reduced due to the sum of the magnetic fluxes is combined with one or more magnets and one or more flux cores << It concentrates on the part that increased. In other words, by replacing part or all of the flux noria part, which is the magnetic flux decrease part due to the sum of the magnet magnetic fluxes, with the magnet and flux noria so that the magnetic flux concentrates in the direction of the magnetic flux increase part due to the sum of the magnet magnetic fluxes, With a simple arrangement and the use of a magnet with a general shape, the cost can be reduced and the torque can be improved without securing a new magnet installation space, or equivalent torque can be generated with a small amount of magnetism. Can be made.

[0086] 本発明を諸図面や実施例に基づき説明してきたが、当業者であれば本開示に基 づき種々の変形や修正を行うことが容易であることに注意されたい。従って、これらの 変形や修正は本発明の範囲に含まれることに留意されたい。例えば、各部材、各手 段、各ステップなどに含まれる機能などは論理的に矛盾しな 、ように再配置可能であ り、複数の部材、手段、ステップなどを 1つに組み合わせたり或いは分割したりするこ とが可能である。なお、実施例では、回転子に永久磁石を設ける形態で説明したが、 電磁石でも本発明の実現することが可能である。また、実施例では、磁石の組は 2組 のものを説明したが、本発明は 3組以上の組の磁石でも同様の作用'効果を達成で きるものである。また、作図や説明の便宜上、回転子の磁石を N極、 S極として図示- 説明してある実施例がある力 N— S極の構成 ·配置を逆に置き換えても発明の作用 •効果は同様であることに留意されたい。さらに、 N極、 S極の磁石は、磁力線の向き 力 ロータ中心の半径方向となるように、着磁方向をそれぞれ半径方向(反対向きで )にした磁石を、例えば、 N極を外側(固定子側)、 S極を外側(固定子側)に配置した ものである。また、幾つかの実施例では磁石は着磁方向を半径方向に配置したもの を用いてある力 この配置には限定されず、磁力線がほぼ半径方向に向いていれば 問題なぐ例えば V字型の磁石配置であってもよ 、。  [0086] Although the present invention has been described based on the drawings and examples, it should be noted that those skilled in the art can easily make various variations and modifications based on the present disclosure. Therefore, it should be noted that these variations and modifications are included in the scope of the present invention. For example, the functions included in each member, each method, each step, etc. can be rearranged so that there is no logical contradiction, and multiple members, means, steps, etc. can be combined or divided into one It is possible to do. In addition, although the embodiment has been described in the form in which the rotor is provided with the permanent magnet, the present invention can also be realized with an electromagnet. In the embodiments, two sets of magnets have been described. However, the present invention can achieve the same effect even with three or more sets of magnets. In addition, for convenience of drawing and explanation, the rotor magnet is shown as N pole and S pole.-There is an example described. Note that it is similar. Furthermore, the N-pole and S-pole magnets are oriented in the direction of the magnetic field force. Magnets whose magnetization directions are in the radial direction (in the opposite direction) so that they are in the radial direction of the rotor center. (Slave side), S pole is arranged outside (stator side). Further, in some embodiments, the magnet is a force using the magnetizing direction arranged in the radial direction. The arrangement is not limited to this arrangement, and if the magnetic field lines are almost in the radial direction, there is no problem. Even a magnet arrangement.

産業上の利用可能性  Industrial applicability

[0087] 第 1の発明によれば、複数の磁石磁束の一部を相殺するように発生させ、磁束が相 殺されている箇所は磁束発生部材の量を少なく配置、もしくは磁石を削除するので、 高価な永久磁石の使用量を抑えることができる。また、本構成では、それぞれの組が 異なる磁極数で構成される複数の磁石の組に相当する複数の磁石磁束を合算して 発生させる磁束発生部材を用いているため、電動機の小型化、電流による損失を 2 つの回転子を独立に回転させる場合よりも低減する効果ももちろん得られる。さらに また、磁束相殺箇所の磁石削減によって回転子自体の重量が軽量化され、削除した 磁石分の慣性の低減によるトルクの向上、電動機の軽量ィ匕などでさらに効果がある。 なお、電磁石を用いた場合でも、同様のコスト低減、トルク向上、電動機軽量ィ匕など の効果を得られる。 [0087] According to the first invention, a part of the plurality of magnet magnetic fluxes are generated so as to cancel each other, and the portion where the magnetic flux is canceled is arranged with a small amount of the magnetic flux generating member, or the magnet is deleted. , The amount of expensive permanent magnets used can be reduced. In addition, this configuration uses a magnetic flux generating member that generates a plurality of magnet magnetic fluxes corresponding to a plurality of magnet sets each having a different number of magnetic poles. Of course, it is possible to reduce the loss due to the loss compared to the case where the two rotors are rotated independently. Furthermore, the weight of the rotor itself is reduced by reducing the number of magnets at the magnetic flux canceling position, and it is further effective in improving the torque by reducing the inertia of the deleted magnet and reducing the weight of the motor. Even when an electromagnet is used, similar effects such as cost reduction, torque improvement, and motor weight reduction can be obtained.

[0088] また、第 2の発明によれば、各々の磁極数成分の磁束 (即ち、各磁束を出す磁石の 各組の間で)に所定の位相差を設けることで、卷線電流のピーク値、磁束ピーク値、 誘起電圧ピーク値のいずれかを所望の値にできる。また、第 3の発明によれば、電動 機の固定子卷線に通電する卷線電流の絶対値のピーク値が最小となるので、インバ ータのスイッチング素子容量を低減する上で有利となる。また、第 4の発明によれば、 電動機の固定子卷線に通電する卷線電流の絶対値の平均値が最小となるので、一 定電圧降下が生じる IGBTやダイオードの損失を低減する上で有利となる。  [0088] Further, according to the second invention, the peak of the winding current is obtained by providing a predetermined phase difference in the magnetic flux of each magnetic pole number component (that is, between each set of magnets generating each magnetic flux). Any one of the value, magnetic flux peak value, and induced voltage peak value can be set to a desired value. According to the third aspect of the invention, the absolute peak value of the winding current flowing through the stator winding of the motor is minimized, which is advantageous in reducing the switching element capacity of the inverter. . Further, according to the fourth invention, since the average value of the absolute value of the winding current flowing through the stator winding of the motor is minimized, it is possible to reduce the loss of the IGBT or the diode that causes a constant voltage drop. It will be advantageous.

[0089] また、第 5の発明によれば、電動機の固定子卷線に通電する卷線電流の実効値が 最小となるので、卷線に生じる銅損を低減する上で有利となる。また、第 6の発明によ れば、 2つの磁石磁束を合算した磁束のピーク値が最小となるので、磁気飽和の発 生を抑える上で有利となる。また、第 7の発明によれば、電動機の固定子卷線に発生 する誘起電圧のピーク値が最小となるので、電動機の高回転ィ匕が可能となる。また、 第 8の発明によれば、電動機の固定子卷線に発生する誘起電圧のピーク値が最大と なるので、電動機の高トルク化が可能となる。  [0089] According to the fifth aspect of the invention, the effective value of the winding current flowing through the stator winding of the motor is minimized, which is advantageous in reducing the copper loss generated in the winding. In addition, according to the sixth aspect of the invention, the peak value of the magnetic flux obtained by adding the two magnet magnetic fluxes is minimized, which is advantageous in suppressing the occurrence of magnetic saturation. Further, according to the seventh aspect, since the peak value of the induced voltage generated in the stator winding of the motor is minimized, the motor can be rotated at high speed. Further, according to the eighth invention, the peak value of the induced voltage generated in the stator winding of the motor is maximized, so that the torque of the motor can be increased.

[0090] また、第 9発明によれば、前記磁束発生部材 (即ちこの部材における前記複数の磁 石の組を構成する磁石)について、複数の磁石の組の少なくとも 1つの組に相当する 磁石磁束を、回転子円周方向に正弦波状に分布するように形成することにって、回 転子軸心と同心の円弧形状の磁束発生部材を配置する場合に比べて磁束の高調 波成分が低下し、コギングトルクを低減することができる。  [0090] According to the ninth aspect of the present invention, the magnetic flux generating member (that is, the magnet constituting the set of the plurality of magnets in the member) corresponds to at least one set of the plurality of magnet sets. Are distributed in a sine wave pattern in the circumferential direction of the rotor, which reduces the harmonic component of the magnetic flux compared to the case where an arc-shaped magnetic flux generating member concentric with the rotor axis is disposed. In addition, the cogging torque can be reduced.

[0091] 前記複数の磁石の組のうちの少なくとも 1つの組の磁石の、前記電動機を構成する 固定子に対向する表面形状 (即ち、電動機の軸心に対して直角をなす平面で切った ときの断面形状)を、回転子円周方向に対して、磁極ごとに、回転子軸心からの半径 より小さい径の円弧形状とすることを想定した磁石の組を、他の通常の表面形状の磁 石の組と、合体させた断面形状 (この形状自体が曲線となる)にすることによって、簡 易かつ簡便に、磁束を回転子円周方向に正弦波状に分布させることが可能となる。 [0091] At least one of the plurality of magnet sets constitutes the electric motor. The surface shape facing the stator (that is, the cross-sectional shape when cut by a plane perpendicular to the axis of the motor) is separated from the rotor axis for each magnetic pole in the circumferential direction of the rotor. By combining a magnet set that assumes an arc shape with a diameter smaller than the radius with another normal surface-shaped magnet set and a combined cross-sectional shape (this shape itself becomes a curve) It is possible to distribute magnetic flux in a sinusoidal shape in the circumferential direction of the rotor easily and simply.

[0092] また、第 10の発明によれば、複数の磁極のうち少なくとも一つ力 d軸インダクタン スと q軸インダクタンスに差が生じるように配置されて ヽるので、リラクタンストルクを得 ることができ、請求項 1から 10の効果に加え、磁束発生部材を増やすことなくトルクを 増カロさせることができる。  [0092] Further, according to the tenth invention, at least one of the plurality of magnetic poles is arranged so that a difference occurs between the d-axis inductance and the q-axis inductance, so that the reluctance torque can be obtained. In addition to the effects of claims 1 to 10, the torque can be increased without increasing the number of magnetic flux generating members.

[0093] また、第 11〜18の発明によれば、複合磁束の生成が容易であって (単なる空隙で はないため、通過磁束がコントロールできる)、安価に複合磁束を生成できる回転子 を提供することが可能となる。  [0093] Further, according to the eleventh to eighteenth inventions, there is provided a rotor that can easily generate composite magnetic flux (it is not a mere gap, and can control passing magnetic flux), and can generate composite magnetic flux at low cost. It becomes possible to do.

[0094] また、第 11の発明によれば、磁束波形を歪ませ複数の次数成分の磁束を発生させ ることができる。また、第 12の発明によれば、磁束波形を歪ませ複数の次数成分の磁 束を発生させることができ、尚且つ、回転子が高温になった場合においても減磁をす ることがない回転電機を実現できる。また、第 13の発明によれば、低磁極数側の次 数成分の磁束を強調した回転電機を実現できる。また、第 14の発明によれば、高磁 極数側の次数成分の磁束を強調した回転電機を実現できる。また、第 15の発明によ れば、第 11〜14の発明が実現できるとともに同一体積の磁石を用意すればよい。ま た、第 16の発明によれば、磁石ピッチ (個々の磁石の周方向の長さ)を変えることに より磁束の基本波と高調波成分の含有比率を変えることができる。また、第 17の発明 によれば、第 11〜14の発明が実現できるとともに同一体積の磁石を用意すればよい 。また、第 18〜22の発明によれば、磁石を削除した部分に配置された着磁された磁 石により、磁石磁束の合算により磁束の増力 tlした部分に磁束が集中するため、磁石 設置スペースを新たに確保することなくトルクの向上が可能であり、更に、小型化を実 現することができる。  [0094] Further, according to the eleventh invention, a magnetic flux waveform can be distorted to generate a plurality of order component magnetic fluxes. According to the twelfth aspect of the invention, the magnetic flux waveform can be distorted to generate a plurality of order component magnetic fluxes, and demagnetization is not caused even when the rotor becomes hot. A rotating electrical machine can be realized. Further, according to the thirteenth invention, it is possible to realize a rotating electrical machine that emphasizes the magnetic flux of the order component on the low magnetic pole number side. Further, according to the fourteenth aspect, a rotating electrical machine in which the magnetic flux of the order component on the high magnetic pole number side is emphasized can be realized. According to the fifteenth invention, the eleventh to fourteenth inventions can be realized and magnets having the same volume may be prepared. In addition, according to the sixteenth invention, the content ratio of the fundamental wave and the harmonic component of the magnetic flux can be changed by changing the magnet pitch (the circumferential length of each magnet). According to the seventeenth invention, the eleventh to fourteenth inventions can be realized and magnets having the same volume may be prepared. Further, according to the eighteenth to twenty-second inventions, the magnetized magnet placed in the portion from which the magnet has been removed concentrates the magnetic flux in the portion where the magnetic flux has been increased by the addition of the magnetic flux of the magnet. The torque can be improved without securing a new value, and further downsizing can be realized.

Claims

請求の範囲  The scope of the claims [1] 複数の回転子のそれぞれの回転子まわりに配置される磁極数が互いに異なる複数 の磁石の組の磁石磁束を合算した磁石磁束に相当する磁束を発生させる一つの回 転子用の磁束発生部材であって、前記複数の磁石の組の前記磁石磁束を重畳及び 相殺する合算した磁束に相当する磁束を発生させ、磁束が相殺される箇所は、磁束 が相殺されな 、箇所に比べて磁束量を少なくするように、低磁束磁石を配置するか、 もしくは磁石を除去したことを特徴とする電動機の回転子。  [1] Magnetic flux for a single rotor that generates a magnetic flux equivalent to a magnetic flux obtained by adding together the magnetic fluxes of a plurality of magnet sets with different numbers of magnetic poles arranged around each rotor of a plurality of rotors Compared to a location where a magnetic flux corresponding to a combined magnetic flux generated by superimposing and canceling the magnet magnetic flux of the set of the plurality of magnets is generated and the magnetic flux is canceled is not canceled. A rotor for an electric motor, wherein a low-flux magnet is arranged or a magnet is removed so as to reduce the amount of magnetic flux. [2] 請求項 1に記載の電動機の回転子において、  [2] In the rotor of the electric motor according to claim 1, 前記複数の磁石の組が 2組あり、これら各組の磁極数成分の磁束に所定の位相差 を設けることを特徴とする電動機の回転子。  There are two sets of the plurality of magnets, and a predetermined phase difference is provided in the magnetic flux of the magnetic pole number component of each set. [3] 請求項 2に記載の電動機の回転子において、 [3] In the rotor of the electric motor according to claim 2, 前記所定の位相差が、前記電動機を構成する固定子卷線に通電する卷線電流の 絶対値のピーク値が最小になるように設定されることを特徴とする電動機の回転子。  The motor rotor according to claim 1, wherein the predetermined phase difference is set so that a peak value of an absolute value of a winding current flowing through a stator winding constituting the motor is minimized. [4] 請求項 2に記載の電動機の回転子において、 [4] In the rotor of the electric motor according to claim 2, 前記所定の位相差が、前記電動機を構成する固定子卷線に通電する卷線電流の 絶対値の平均値が最小になるように設定されることを特徴とする電動機の回転子。  The electric motor rotor according to claim 1, wherein the predetermined phase difference is set such that an average value of absolute values of a winding current flowing through a stator winding constituting the electric motor is minimized. [5] 請求項 2に記載の電動機の回転子において、 [5] In the rotor of the electric motor according to claim 2, 前記所定の位相差が、前記電動機を構成する固定子卷線に通電する卷線電流の 実効値が最小になるように設定されることを特徴とする電動機の回転子。  The electric motor rotor according to claim 1, wherein the predetermined phase difference is set so that an effective value of a winding current flowing through a stator winding constituting the motor is minimized. [6] 請求項 2に記載の電動機の回転子において、 [6] In the rotor of the electric motor according to claim 2, 前記所定の位相差が、前記 2組の磁石に相当する 2つの磁石磁束を合算した磁束 のピーク値が最小になるように設定されることを特徴とする電動機の回転子。  The electric motor rotor according to claim 1, wherein the predetermined phase difference is set such that a peak value of a magnetic flux obtained by adding two magnetic fluxes corresponding to the two sets of magnets is minimized. [7] 請求項 2に記載の電動機の回転子において、 [7] In the rotor of the electric motor according to claim 2, 前記所定の位相差が、前記回転子の回転時に前記電動機を構成する固定子卷線 に発生する誘起電圧のピーク値が最小になるように設定されることを特徴とする電動 機の回転子。  The electric motor rotor, wherein the predetermined phase difference is set so that a peak value of an induced voltage generated in a stator winding constituting the electric motor when the rotor rotates is minimized. [8] 請求項 2に記載の電動機の回転子において、  [8] In the rotor of the electric motor according to claim 2, 前記所定の位相差が、前記回転子の回転時に前記電動機を構成する固定子卷線 に発生する誘起電圧のピーク値が最大になるように設定されることを特徴とする電動 機の回転子。 The predetermined phase difference is a stator winding that constitutes the electric motor when the rotor rotates. The rotor of the electric motor is characterized in that the peak value of the induced voltage generated in the motor is set to a maximum. 請求項 1〜8のいずれか 1項に記載の電動機の回転子において、  In the rotor of the electric motor according to any one of claims 1 to 8, 前記磁束発生部材は、前記複数の磁石の組の少なくとも 1つの組に相当する磁石 磁束が、回転子円周方向に正弦波状に分布するように形成されることを特徴とする 電動機の回転子。  The rotor of an electric motor, wherein the magnetic flux generating member is formed such that a magnet magnetic flux corresponding to at least one of the plurality of magnets is distributed in a sine wave shape in a circumferential direction of the rotor. 請求項 1〜8のいずれか 1項に記載の電動機の回転子において、  In the rotor of the electric motor according to any one of claims 1 to 8, 前記磁束発生部材における前記複数の磁石の組のうち少なくとも 1つの組における 磁極が、 d軸インダクタンスと q軸インダクタンスとの間に差が生じるように配置されて いることを特徴とする電動機の回転子。  The rotor of the electric motor, wherein the magnetic poles in at least one of the plurality of magnets in the magnetic flux generating member are arranged so that a difference occurs between the d-axis inductance and the q-axis inductance. . 請求項 1に記載の電動機の回転子において、  In the rotor of the electric motor according to claim 1, 前記磁束発生部材が永久磁石であり、前記永久磁石が、第 1の永久磁石と第 2の 永久磁石によって構成され、前記第 1の永久磁石の残留磁束密度および Zまたは保 磁力が、前記第 2の永久磁石のそれよりも大きいことを特徴とする電動機の回転子。 請求項 1に記載の電動機の回転子において、  The magnetic flux generating member is a permanent magnet, and the permanent magnet is constituted by a first permanent magnet and a second permanent magnet, and the residual magnetic flux density and Z or coercive force of the first permanent magnet are the second permanent magnet. An electric motor rotor characterized by being larger than that of a permanent magnet. In the rotor of the electric motor according to claim 1, 前記磁束発生部材が永久磁石であり、前記永久磁石が、第 1の永久磁石と第 2の 永久磁石によって構成され、前記第 2の永久磁石の温度変化に対する磁石特性が、 前記第 2の永久磁石のそれよりも安定であることを特徴とする電動機の回転子。 請求項 1に記載の電動機の回転子において、  The magnetic flux generating member is a permanent magnet, the permanent magnet is composed of a first permanent magnet and a second permanent magnet, and the second permanent magnet has a magnet characteristic with respect to a temperature change of the second permanent magnet. An electric motor rotor characterized by being more stable than that of the motor. In the rotor of the electric motor according to claim 1, 前記複数の磁石の組が、低磁極数の第 1の磁石の組と高磁極数の第 2の磁石の組 とからなり、前記第 1および第 2の磁石の組を構成する磁石をそれぞれ配置するにあ たり、前記第 1の磁石の組を構成する磁石と、前記第 2の磁石の組を構成する磁石を 相殺する際に、前記第 1の磁石の組の磁束が強まるように磁石を配置することを特徴 とする電動機の回転子。  The plurality of magnet sets are composed of a first magnet set having a low number of magnetic poles and a second magnet set having a high number of magnetic poles, and the magnets constituting the first and second magnet sets are arranged respectively. In doing so, when canceling out the magnets constituting the first magnet set and the magnets constituting the second magnet set, the magnets are arranged so that the magnetic flux of the first magnet set is strengthened. An electric motor rotor characterized by being arranged. 請求項 1に記載の電動機の回転子において、  In the rotor of the electric motor according to claim 1, 前記複数の磁石の組が、低磁極数の第 1の磁石の組と高磁極数の第 2の磁石の組 とからなり、前記第 1および第 2の磁石の組を構成する磁石をそれぞれ配置するにあ たり、前記第 1の磁石の組を構成する磁石と、前記第 2の磁石の組を構成する磁石を 相殺する際に、前記第 2の磁石の組を構成する磁石の磁束が強まるように磁石を配 置することを特徴とする電動機の回転子。 The plurality of magnet sets are composed of a first magnet set having a low number of magnetic poles and a second magnet set having a high number of magnetic poles, and the magnets constituting the first and second magnet sets are arranged respectively. In doing so, a magnet constituting the first magnet set and a magnet constituting the second magnet set are provided. A rotor for an electric motor, wherein magnets are arranged so that magnetic fluxes of magnets constituting the second magnet set are strengthened when canceling. [15] 請求項 1に記載の電動機の回転子において、 [15] In the rotor of the electric motor according to claim 1, 前記磁束発生部材が複数の永久磁石により構成され、前記複数の永久磁石の周 方向の長さが全て同一であることを特徴とする電動機の回転子。  The rotor of an electric motor, wherein the magnetic flux generating member is composed of a plurality of permanent magnets, and the circumferential lengths of the plurality of permanent magnets are all the same. [16] 請求項 1に記載の電動機の回転子において、 [16] In the rotor of the electric motor according to claim 1, 前記磁束発生部材が複数の永久磁石により構成され、前記複数の永久磁石の周 方向の長さが磁石によって異なることを特徴とする電動機の回転子。  The rotor of an electric motor, wherein the magnetic flux generating member is composed of a plurality of permanent magnets, and the circumferential lengths of the plurality of permanent magnets differ depending on the magnets. [17] 請求項 1に記載の電動機の回転子において、 [17] In the rotor of the electric motor according to claim 1, 前記磁束発生部材が複数の永久磁石により構成され、前記複数の永久磁石の半 径方向の厚さが、磁石によって異なることを特徴とする電動機の回転子。  The rotor of an electric motor, wherein the magnetic flux generating member is composed of a plurality of permanent magnets, and the thicknesses of the plurality of permanent magnets in the radial direction differ depending on the magnets. [18] 請求項 1ないし 8のいずれかに記載の電動機の回転子において、前記磁石を除去 した部分に磁石磁束の合算により磁束の増力!]した部分に磁束が集中するように着磁 した磁石を配置した電動機の回転子。  [18] The rotor of the electric motor according to any one of claims 1 to 8, wherein the magnet is magnetized so that the magnetic flux is concentrated at a portion where the magnetic flux is increased by adding the magnetic flux to the portion where the magnet is removed! An electric motor rotor. [19] 請求項 18に記載の電動機の回転子において、前記着磁した磁石は、一つ以上の 着磁方向により磁束が集中するようにした電動機の回転子。 [19] The rotor of the electric motor according to claim 18, wherein the magnetized magnet is configured such that magnetic flux concentrates in one or more magnetization directions. [20] 請求項 18に記載の電動機の回転子において、前記着磁した磁石は、一つ以上の 磁石の設置角度により磁束が集中するようにした電動機の回転子。 [20] The rotor of the electric motor according to claim 18, wherein the magnetized magnet concentrates magnetic flux depending on an installation angle of one or more magnets. [21] 請求項 18に記載の電動機の回転子において、前記着磁した磁石は、その 2以上 のベクトル合成によって磁束が集中するようにした電動機の回転子。 21. The electric motor rotor according to claim 18, wherein the magnetized magnet is configured such that magnetic flux is concentrated by combining two or more vectors thereof. [22] 請求項 18に記載の電動機の回転子において、前記着磁した磁石は、一つ以上の 磁石と一つ以上のフラックスノ《リアにより磁束が集中するようにした電動機の回転子。 22. The rotor of an electric motor according to claim 18, wherein the magnetized magnet is configured such that magnetic flux is concentrated by one or more magnets and one or more fluxno << rears.
PCT/JP2007/060498 2006-09-19 2007-05-23 Rotor of motor Ceased WO2008035487A1 (en)

Applications Claiming Priority (4)

Application Number Priority Date Filing Date Title
JP2006252688A JP2007174885A (en) 2005-11-24 2006-09-19 Synchronous motor rotor
JP2006-252688 2006-09-19
JP2006253946A JP2008079393A (en) 2006-09-20 2006-09-20 Electric motor
JP2006-253946 2006-09-20

Publications (1)

Publication Number Publication Date
WO2008035487A1 true WO2008035487A1 (en) 2008-03-27

Family

ID=39200317

Family Applications (1)

Application Number Title Priority Date Filing Date
PCT/JP2007/060498 Ceased WO2008035487A1 (en) 2006-09-19 2007-05-23 Rotor of motor

Country Status (1)

Country Link
WO (1) WO2008035487A1 (en)

Cited By (6)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010259242A (en) * 2009-04-27 2010-11-11 Nissan Motor Co Ltd Electric motor
JP2011036060A (en) * 2009-08-04 2011-02-17 Nissan Motor Co Ltd Motor
CN111670529A (en) * 2018-01-31 2020-09-15 Lg伊诺特有限公司 Rotors and motors including rotors
EP3874585A4 (en) * 2018-10-31 2022-11-30 Optiphase Drive Systems, Inc. Electric machine with permanent magnet rotor
JP2023535378A (en) * 2020-07-17 2023-08-17 エルジー イノテック カンパニー リミテッド motor
CN119651956A (en) * 2025-02-11 2025-03-18 华侨大学 A rotor slotting device and a bilateral permanent magnet motor thereof

Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH11225464A (en) * 1998-02-06 1999-08-17 Matsushita Electric Ind Co Ltd Electric motor, power generator, vacuum cleaner, electric fan and electric car
JP2000134891A (en) * 1998-10-28 2000-05-12 Okuma Corp Synchronous motor and its control device
JP2004336968A (en) * 2003-05-12 2004-11-25 Rikogaku Shinkokai Bearing-less motor, and its rotor position control circuit and rotor position control method

Patent Citations (3)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JPH11225464A (en) * 1998-02-06 1999-08-17 Matsushita Electric Ind Co Ltd Electric motor, power generator, vacuum cleaner, electric fan and electric car
JP2000134891A (en) * 1998-10-28 2000-05-12 Okuma Corp Synchronous motor and its control device
JP2004336968A (en) * 2003-05-12 2004-11-25 Rikogaku Shinkokai Bearing-less motor, and its rotor position control circuit and rotor position control method

Cited By (9)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
JP2010259242A (en) * 2009-04-27 2010-11-11 Nissan Motor Co Ltd Electric motor
JP2011036060A (en) * 2009-08-04 2011-02-17 Nissan Motor Co Ltd Motor
CN111670529A (en) * 2018-01-31 2020-09-15 Lg伊诺特有限公司 Rotors and motors including rotors
EP3748818A4 (en) * 2018-01-31 2021-03-31 LG Innotek Co., Ltd. ROTOR AND MOTOR INCLUDING IT
US11888355B2 (en) 2018-01-31 2024-01-30 Lg Innotek Co., Ltd. Rotor and motor including same
EP3874585A4 (en) * 2018-10-31 2022-11-30 Optiphase Drive Systems, Inc. Electric machine with permanent magnet rotor
US11646618B2 (en) 2018-10-31 2023-05-09 Optiphase Drive Systems, Inc. Electric machine with permanent magnet rotor
JP2023535378A (en) * 2020-07-17 2023-08-17 エルジー イノテック カンパニー リミテッド motor
CN119651956A (en) * 2025-02-11 2025-03-18 华侨大学 A rotor slotting device and a bilateral permanent magnet motor thereof

Similar Documents

Publication Publication Date Title
JP6874675B2 (en) Rotating machine
JP4670871B2 (en) motor
US9071118B2 (en) Axial motor
JP5751794B2 (en) Traction motor for electric vehicles
US7291945B2 (en) AC motor and control device therefor
CN101114777B (en) Claw-teeth-type rotating electrical machine
EP1253701B1 (en) Motor
WO2019064801A1 (en) Permanent magnet rotating electric machine
Takano et al. Design and analysis of a switched reluctance motor for next generation hybrid vehicle without PM materials
WO2007072707A1 (en) Electric motor and its rotor, and magnetic core for the rotor
CN103038986A (en) Electric motor
KR20220044429A (en) Electric motor having stacked different rotor segments and method for designing the same
WO2008035487A1 (en) Rotor of motor
CN102422510A (en) Synchronous machine
JP5538984B2 (en) Permanent magnet motor
WO2007123057A1 (en) Motor
JP2003088078A (en) Brushless dc motor
JP2002153033A (en) Ipm motor
JP2007174885A (en) Synchronous motor rotor
JP5261871B2 (en) Synchronous motor
JP2006174651A (en) Core, armature, manufacturing method thereof, and electric motor
JP2008079393A (en) Electric motor
JP5440670B2 (en) Electric motor
JP2008263681A (en) Ac motor
JP4748058B2 (en) Permanent magnet motor, refrigerant compressor and blower

Legal Events

Date Code Title Description
121 Ep: the epo has been informed by wipo that ep was designated in this application

Ref document number: 07743932

Country of ref document: EP

Kind code of ref document: A1

NENP Non-entry into the national phase

Ref country code: DE

122 Ep: pct application non-entry in european phase

Ref document number: 07743932

Country of ref document: EP

Kind code of ref document: A1