JP2011120333A - Rotor for permanent magnet embedded motor, blower, and compressor - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a rotor for a permanent magnet embedded motor, which reduce torque ripples by a slit, without giving a skew. <P>SOLUTION: This rotor 100 for the permanent magnet embedded motor includes: a rotor core 101; a plurality of permanent magnet insertion holes 102, which are created in the rotor core 101; cavities 104 at the ends of the permanent magnets; a plurality of permanent magnets 103, which are inserted into the permanent magnet insertion holes 102; and slits, which are created at the cores outside the permanent magnet insertion holes 102. The slits are created severally roughly symmetrical about the center line of each magnetic pole, and they are constituted so that at least one point of intersection of the extensions of the center lines of the slits exists, on the center lines of each magnetic pole, and at least one magnetic pole, where the interval between the point of intersection of the extensions of the center lines of the slits and the permanent magnet is different from those of other magnetic poles, exists among a plurality of magnetic poles that are constituted of a plurality of permanent magnets. <P>COPYRIGHT: (C)2011,JPO&INPIT

Description

  The present invention relates to a rotor of a permanent magnet embedded motor, and more particularly to a slit shape disposed in an outer peripheral core portion of a permanent magnet insertion hole. The present invention also relates to a blower and a compressor that use a permanent magnet embedded motor on which a rotor of the permanent magnet embedded motor is mounted. Hereinafter, the permanent magnet embedded motor may be simply referred to as an electric motor.

  Conventionally, there has been proposed a technique for reducing torque ripple of an electric motor by dividing a rotor into a plurality of rotor cores and shifting each of them in a circumferential direction by a predetermined angle.

  However, the technology for reducing the torque ripple of these electric motors has a problem that the harmonic components of the vibrations of a plurality of orders cannot be reduced at the same time because the axial deviation angle of each of the rotor cores is one. .

  Therefore, the following rotors have been proposed for the purpose of supplying a rotor that can simultaneously reduce the harmonic components of a plurality of orders of vibration. That is, the rotor includes a first rotor core, a second rotor core, and a third rotor core that are connected to each other in the rotation axis Z direction. The first rotor core, the second rotor core, and the third rotor core have the same configuration. The first rotor core includes a side surface parallel to the rotation axis Z and a field magnet that forms a plurality of magnetic pole faces different from each other in the number of pole pairs on the side surface, and is uniform in the direction of the rotation axis Z. It is a configuration. The first rotor core and the second rotor core form a skew angle θ1 degree in the circumferential direction of the rotation axis Z, and the second rotor core and the third rotor core have a skew angle θ2 degrees. Forming. By determining the skew angle θ by 360 / (2pn) (p: the number of pole pairs, an integer larger than n: 1), the harmonic component of the vibration having the order of n can be reduced. Therefore, in this case, harmonic components of vibrations of two orders can be reduced (see, for example, Patent Document 1).

JP 2008-131783 A

  The rotor of a conventional permanent magnet embedded motor has been designed to reduce noise by providing a slit or skew to reduce torque ripple. However, applying the skew is difficult to manufacture because the phase of the rotor is changed. For this reason, there is a problem in that the cost at the time of manufacture increases and the efficiency decreases due to a decrease in the torque of the electric motor.

  The present invention has been made to solve the above-described problems, and provides a rotor of a permanent magnet embedded motor in which torque ripple can be reduced by a slit without applying a skew.

  Also provided are a blower and a compressor equipped with an embedded permanent magnet motor using the rotor of the embedded permanent magnet motor.

The rotor of the permanent magnet embedded motor according to the present invention includes a rotor core formed by laminating a predetermined number of electromagnetic steel sheets punched into a predetermined shape,
A plurality of permanent magnet insertion holes formed along the outer periphery of the rotor core;
Permanent magnet end gaps provided at both ends of the permanent magnet insertion hole;
A plurality of permanent magnets inserted into the permanent magnet insertion holes;
A plurality of slits formed in the iron core portion outside the permanent magnet insertion hole, and
The plurality of slits are formed so as to be substantially symmetrical with respect to the magnetic pole center line, and are configured such that at least one intersection of the extension lines of the slit center line exists on the magnetic pole center line,
Among the plurality of magnetic poles composed of a plurality of permanent magnets, at least one magnetic pole having a distance between the intersection of the extension line of the center line of the slit and the permanent magnet is different from that of the other magnetic poles.

  In the rotor of the interior permanent magnet motor according to the present invention, the plurality of slits are formed substantially symmetrically with respect to the magnetic pole center line, and the intersection of the extension lines of the slit center lines is at least one point on the magnetic pole center line. Among the plurality of magnetic poles configured to exist and composed of a plurality of permanent magnets, at least one magnetic pole having a distance between the intersection of the extension line of the center line of the slit and the permanent magnet is different from that of the other magnetic poles. Therefore, the torque ripple can be reduced due to the effect of shifting the torque phase of the magnetic poles.

It is a figure shown for a comparison and is a cross-sectional view of a rotor 300 of a general permanent magnet embedded motor. It is a figure shown for a comparison and is a cross-sectional view of the rotor core 301 of the rotor 300 of a general permanent magnet embedded motor. It is a figure shown for a comparison and is the elements on larger scale of the rotor 300 of a general permanent magnet embedded motor. It is a figure shown for a comparison and is the elements on larger scale of the rotor core 301 of the rotor 300 of a general permanent magnet embedded motor. In the figure shown for comparison, in the rotor 300 of a general embedded permanent magnet motor, the distance L between the intersection A of the extension lines of the center lines of the slits 305 having one magnetic pole and the permanent magnet 303 is changed. The figure which compared the torque at the time. FIG. 3 shows the first embodiment, and is a cross-sectional view of a rotor 100 of a permanent magnet embedded motor. FIG. 3 shows the first embodiment, and is a transverse cross-sectional view of a rotor core 101 of a rotor 100 of a permanent magnet embedded motor. FIG. 5 shows the first embodiment and is an enlarged view of the vicinity of the magnetic pole a of the rotor 100. FIG. 5 shows the first embodiment, and is an enlarged view near the magnetic pole a of the rotor core 101. FIG. 5 shows the first embodiment and is an enlarged view in the vicinity of the magnetic pole b of the rotor 100. FIG. 5 shows the first embodiment, and is an enlarged view near the magnetic pole b of the rotor core 101. FIG. 5 shows the first embodiment and is an enlarged view in the vicinity of the magnetic pole c of the rotor 100. FIG. 5 shows the first embodiment, and is an enlarged view near the magnetic pole c of the rotor core 101. FIG. 5 shows the first embodiment, and is an enlarged view of the vicinity of the magnetic pole d of the rotor 100. FIG. FIG. 5 shows the first embodiment, and is an enlarged view near the magnetic pole d of the rotor core 101. FIG. The figure which shows Embodiment 1, and is a figure which shows a torque waveform when La = Lc = L1 and Lb = Ld = L2. In the figure which shows Embodiment 1, each torque waveform of La = Lb = Lc = L1 and Ld = L2, La = Lc = L1, Lb = Ld = L2, La = L1 and Lb = Lc = Ld = L2 is shown. FIG. FIG. 5 shows the first embodiment, and is a cross-sectional view of a rotor 200 of a permanent magnet embedded motor according to a modification. FIG. 5 shows the first embodiment, and is a cross-sectional view of a rotor core 201 of a rotor 200 of a permanent magnet embedded motor according to a modification. FIG. 5 shows the first embodiment and is an enlarged view in the vicinity of the magnetic pole a of the rotor 200. FIG. 5 shows the first embodiment, and is an enlarged view near the magnetic pole a of the rotor core 201. FIG. 5 shows the first embodiment and is an enlarged view of the vicinity of the magnetic pole b of the rotor 200. FIG. 5 shows the first embodiment, and is an enlarged view near the magnetic pole b of the rotor core 201. FIG. 5 shows the first embodiment and is an enlarged view in the vicinity of a magnetic pole c of a rotor 200. FIG. 5 shows the first embodiment, and is an enlarged view of the vicinity of a magnetic pole c of a rotor core 201. FIG. 5 shows the first embodiment and is an enlarged view in the vicinity of the magnetic pole d of the rotor 200. FIG. 5 shows the first embodiment, and is an enlarged view near the magnetic pole d of the rotor core 201. FIG.

Embodiment 1 FIG.
FIGS. 1 to 5 are views for comparison, FIG. 1 is a cross-sectional view of a rotor 300 of a general permanent magnet embedded motor, and FIG. 2 is a rotor of a general permanent magnet embedded motor. FIG. 3 is a partially enlarged cross-sectional view of a rotor 300 of a general permanent magnet embedded motor, and FIG. 4 is a rotor 300 of a general permanent magnet embedded motor. 5 is a partially enlarged cross-sectional view of the rotor core 301 of FIG. 5, and FIG. 5 shows the distance between the intersection A of the extension lines of the center lines of the plurality of slits 305 and the permanent magnet 303 in the rotor 300 of a general embedded permanent magnet motor. It is the figure which compared the torque when changing L.

  First, a general permanent magnet embedded motor rotor 300 will be described. A rotor 300 of the permanent magnet embedded motor shown in FIG. 1 includes at least a rotor core 301 and a permanent magnet 303.

  Note that the rotor 300 of the permanent magnet embedded motor is simply referred to as the rotor 300. Further, the rotor 300 or the like may be simply referred to as a rotor.

  The rotor core 301 has a substantially circular cross-sectional shape as a whole, a thin electromagnetic steel plate (for example, a thickness of about 0.1 to 1.0 mm, and a non-oriented electrical steel plate (biased in a specific direction of the steel plate). The crystal axis direction of each crystal is arranged as randomly as possible so as not to exhibit magnetic properties))) is punched with a mold into a predetermined shape, and a predetermined number (multiple) is laminated.

  The rotor core 301 is formed with four permanent magnet insertion holes 302 having a rectangular cross section so as to form a quadrangle in the circumferential direction (see FIG. 2).

  A four-pole rotor 300 is formed by inserting four flat-plate-shaped permanent magnets 303 magnetized so that N poles and S poles are alternately arranged inside the permanent magnet insertion hole 302. .

  For the permanent magnet 303, for example, rare earth mainly containing neodymium, iron, or boron is used.

  At both ends of the permanent magnet insertion hole 302, permanent magnet end gaps 304 that are connected to the permanent magnet insertion hole 302 are formed.

  The permanent magnet end portion gap 304 suppresses the leakage magnetic flux of the permanent magnet 303 between the poles.

  A plurality of slits 305 are formed in the peripheral direction of the permanent magnet insertion hole 302 at predetermined intervals in the circumferential direction. In the rotor 300 of FIG. 1, five slits 305 are formed in one magnetic pole.

  The five slits 305 are arranged symmetrically with respect to the magnetic pole center, and an intersection A of the extension line of the center line of each slit 305 exists on the magnetic pole center line.

  In the rotor 300 shown in FIG. 1, the magnetic flux generated from the permanent magnet 303 is concentrated on the magnetic pole center by tilting the slit 305 toward the magnetic pole center side, so that the magnetic flux density at the outer peripheral portion of the rotor 300 is sinusoidal. Thereby, the harmonics of the induced voltage are reduced and the cogging torque is reduced. As a result, torque ripple was reduced.

  Hereinafter, the effect of the slit 305 will be described. Magnetic flux generated from the permanent magnet 303 of the rotor 300 flows into the stator (not shown) through the outer peripheral core portion of the permanent magnet 303.

  At that time, the magnetic path of the magnetic flux generated from the permanent magnet 303 is restricted by the iron core portion between the adjacent slits 305.

  When the slit 305 is not present, the magnetic flux generated from the permanent magnet 303 can move freely in the outer peripheral core portion of the permanent magnet 303, so that the magnetic flux easily flows, and torque ripple is caused by the influence. Was getting worse.

  That is, the slit 305 restricts the magnetic flux generated from the permanent magnet 303 from freely moving around the outer peripheral core portion of the permanent magnet 303.

  Therefore, by changing the shape of the slit 305, the magnetic flux at the outer peripheral portion of the rotor 300 can be freely changed.

  However, the rotor 300 shown in FIG. 1 rotates with torque generated by the magnetic force generated from the permanent magnet 303 in the rotor 300 and the magnetic force generated from the stator (not shown). However, with only the slit 305, it is difficult to sufficiently reduce the torque ripple, and there is a problem that noise increases.

  Next, the torque when the distance L between the intersection A of the extension lines of the center lines of the plurality of slits 305 of each magnetic pole shown in FIG. 1 and the permanent magnet 303 is changed will be described.

  FIG. 5 shows respective torque waveforms when the distance L between the intersection A of the extension line of the center line of the plurality of slits 305 of each magnetic pole and the permanent magnet 303 is changed to L1 and L2.

  The torque waveform shown in FIG. 5 is a torque waveform of an embedded permanent magnet motor (hereinafter sometimes simply referred to as a motor) in which the number of slots is 6, and a rotor 300 is combined with a concentrated winding stator.

  A 4-pole 6-slot motor generates torque ripple due to the effects of cogging torque and harmonics of the induced voltage, and generally has a slit-free shape. The fundamental component of torque ripple is the number of poles (4) And the 12th order (12f) of the least common multiple of the number of slots (6). One period of the fundamental wave component 12f is 30 degrees in mechanical angle.

  Since the rotor 300 in FIG. 1 has a slit 305 and brings the surface magnetic flux of the rotor 300 close to a sinusoidal shape, it is possible to reduce the harmonic components of the cogging torque and the induced voltage. As a result, the torque ripple can be reduced by reducing 12f, which is the fundamental wave component of the torque ripple, to 24f, 36f, 48f.

  The torque waveform shown in FIG. 5 is an example of four poles and six stator slots, and has a periodicity at a mechanical angle of 30 deg, and therefore shows a waveform up to a mechanical angle of 30 deg.

  L1 and L2 have a relationship of L1> L2. That is, when the distance L between the intersection point A of the extension lines of the center lines of the plurality of slits 305 of each magnetic pole and the permanent magnet 303 is increased, the torque ripple waveform shifts to the right as shown in FIG. The mechanical angle in FIG. 5 indicates the position of the rotor 300 with respect to the stator (not shown), and an arbitrary position is set to 0 °. When the distance L is changed, for example, the peak position (mechanical angle) of the torque ripple waveform changes.

  It can be seen that by changing the distance L between the intersection point A of the extension lines of the center lines of the plurality of slits 305 of each magnetic pole and the permanent magnet 303, the magnetic flux on the outer periphery of the rotor changes, and as a result, the torque waveform also changes. .

  However, although the torque waveform changes by changing the distance L, only changing the distance L has little torque ripple reduction effect.

  In the present embodiment, as described above, by changing the distance L between the intersection point A of the extension line of the center line of the plurality of slits 305 of each magnetic pole and the permanent magnet 303, the peak position of the torque ripple waveform (machine Note that if the torque ripple waveforms with different angles and different peak positions (mechanical angles) are synthesized, the peak of the synthesized torque ripple waveform decreases.

  In other words, the distance L between the intersections of the extension lines of the center lines of the slits of one magnetic pole and the permanent magnet is not the same in all (even) magnetic poles of the rotor, and the magnetic poles are combined differently. As a result, the torque ripple waveform peak is expected to be reduced by synthesizing torque from magnetic poles having different distances L.

  6 to 27 show the first embodiment, FIG. 6 is a cross-sectional view of the rotor 100 of the permanent magnet embedded motor, and FIG. 7 is the rotor core of the rotor 100 of the permanent magnet embedded motor. 8 is an enlarged view of the vicinity of the magnetic pole a of the rotor 100, FIG. 9 is an enlarged view of the vicinity of the magnetic pole a of the rotor core 101, and FIG. 10 is an enlarged view of the vicinity of the magnetic pole b of the rotor 100. 11 is an enlarged view of the rotor core 101 near the magnetic pole b, FIG. 12 is an enlarged view of the rotor 100 near the magnetic pole c, FIG. 13 is an enlarged view of the rotor core 101 near the magnetic pole c, and FIG. FIG. 15 is an enlarged view of the vicinity of the magnetic pole d of the rotor core 101. FIG. 16 is a diagram showing torque waveforms when La = Lc = L1 and Lb = Ld = L2. FIG. Lb = Lc = L1, Ld = L2, La = Lc = L1, Lb = Ld = L2, L = L1 and Lb = Lc = Ld = L2 are diagrams showing torque waveforms, FIG. 18 is a cross-sectional view of a rotor 200 of a permanent magnet embedded motor according to a modification, and FIG. 19 is a permanent magnet embedded according to a modification. FIG. 20 is an enlarged view of the vicinity of the magnetic pole a of the rotor 200, FIG. 21 is an enlarged view of the vicinity of the magnetic pole a of the rotor core 201, and FIG. FIG. 23 is an enlarged view of the vicinity of the magnetic pole b of the rotor core 201, FIG. 24 is an enlarged view of the vicinity of the magnetic pole c of the rotor 200, and FIG. 25 is an enlarged view of the vicinity of the magnetic pole c of the rotor core 201. FIG. 26 is an enlarged view of the rotor 200 near the magnetic pole d, and FIG. 27 is an enlarged view of the rotor core 201 near the magnetic pole d.

  The rotor 100 (hereinafter simply referred to as the rotor 100) of the permanent magnet embedded motor according to the present embodiment will be described with reference to FIGS.

  A rotor 100 of the permanent magnet embedded motor shown in FIG. 6 includes at least a rotor core 101 and a permanent magnet 103.

  The rotor 100 of the permanent magnet embedded motor is simply referred to as the rotor 100. Further, the rotor 100 or the like may be simply referred to as a rotor.

  The rotor core 101 has a substantially circular cross-sectional shape as a whole, a thin electromagnetic steel plate (for example, a thickness of about 0.1 to 1.0 mm, and a non-oriented electrical steel plate (biased in a specific direction of the steel plate). The crystal axis direction of each crystal is arranged as randomly as possible so as not to exhibit magnetic properties))) is punched with a mold into a predetermined shape, and a predetermined number (multiple) is laminated.

  The rotor core 101 is formed with four permanent magnet insertion holes 102 having a rectangular cross section so as to form a quadrangle in the circumferential direction (see FIG. 7).

  A four-pole rotor 100 is formed by inserting four plate-shaped permanent magnets 103 magnetized so that N poles and S poles are alternately arranged inside the permanent magnet insertion hole 102. .

  For the permanent magnet 103, for example, a rare earth mainly containing neodymium, iron, or boron is used.

  At both ends of the permanent magnet insertion hole 102, permanent magnet end gaps 104 connected to the permanent magnet insertion hole 102 are formed.

  The permanent magnet end gap 104 suppresses the leakage magnetic flux of the permanent magnet 103 between the poles.

  A plurality of slits are formed at predetermined intervals in the circumferential direction in the outer peripheral iron core portion of the permanent magnet insertion hole 102. In the rotor 100 of FIG. 6, five slits are formed in one magnetic pole.

  The five slits are arranged symmetrically with respect to the magnetic pole center, and an intersection A of the extension line of the center line of each slit exists on the magnetic pole center line.

  The present embodiment is characterized in that the configuration of the slit of each magnetic pole is different.

  In FIG. 6, names are given to the respective magnetic poles located at four positions. In FIG. 6, the upper magnetic pole is a magnetic pole a, the right magnetic pole is a magnetic pole b, the lower magnetic pole is a magnetic pole c, and the left magnetic pole is a magnetic pole d.

  The slit of the magnetic pole a is the slit 105a, the slit of the magnetic pole b is the slit 105b, the slit of the magnetic pole c is the slit 105c, and the slit of the magnetic pole d is the slit 105d.

  In the magnetic poles a to d, the number of slits constituting the slits 105a to 105d is the same, and the intersection point of the extension lines of the center lines of the slits is the same as that on the magnetic pole center line.

  In the magnetic poles a to d, the distance between the intersection of the extension lines of the center lines of the slits 105a to 105d and the permanent magnet 103 is different.

  8 and 9, the configuration of the magnetic pole a will be described mainly with the slit 105a. As shown in FIGS. 8 and 9, the slit 105 a includes five slits 105 a-1, a slit 105 a-2, a slit 105 a-3, a slit 105 a-4, and a slit 105 a-5.

  The center line of the slit 105a-3 substantially coincides with the magnetic pole center line. The slits 105a-2 and 105a-4 on both sides of the slit 105a-3 are inclined at a predetermined angle toward the magnetic pole center line. The extension lines of the center lines of the slits 105a-2 and 105a-4 intersect at the intersection A on the magnetic pole center line outside the rotor 100.

  The slits 105a-1 and 105a-5 located on the outermost side in the circumferential direction are also inclined at a predetermined angle toward the magnetic pole center line. The inclination angles of the slits 105a-1 and 105a-5 are larger than the inclination angles of the slits 105a-2 and 105a-4. The extension lines of the center lines of the slits 105 a-1 and the slits 105 a-5 also intersect at the intersection A on the magnetic pole center line outside the rotor 100.

  In the magnetic pole a, the distance between the intersection A and the permanent magnet 103 is La.

  10 and 11, the configuration of the magnetic pole b will be described mainly with the slit 105b. As shown in FIGS. 10 and 11, the slit 105b includes five slits 105b-1, a slit 105b-2, a slit 105b-3, a slit 105b-4, and a slit 105b-5.

  The center line of the slit 105b-3 substantially coincides with the magnetic pole center line. The slits 105b-2 and 105b-4 on both sides of the slit 105b-3 are inclined at a predetermined angle toward the magnetic pole center line. Then, at the intersection B on the magnetic pole center line outside the rotor 100, the extension lines of the respective center lines of the slit 105b-2 and the slit 105b-4 intersect.

  The slit 105b-1 and the slit 105b-5 located on the outermost side in the circumferential direction are also inclined at a predetermined angle toward the magnetic pole center line. The inclination angles of the slit 105b-1 and the slit 105b-5 are larger than the inclination angles of the slit 105b-2 and the slit 105b-4. The extension lines of the center lines of the slits 105 b-1 and 105 b-5 also intersect at the intersection B on the magnetic pole center line outside the rotor 100.

  In the magnetic pole b, the distance between the intersection B and the permanent magnet 103 is Lb.

  The configuration of the magnetic pole c will be described mainly with the slit 105c with reference to FIGS. As illustrated in FIGS. 12 and 13, the slit 105 c includes five slits 105 c-1, a slit 105 c-2, a slit 105 c-3, a slit 105 c-4, and a slit 105 c-5.

  The center line of the slit 105c-3 substantially coincides with the magnetic pole center line. The slits 105c-2 and 105c-4 on both sides of the slit 105c-3 are inclined at a predetermined angle toward the magnetic pole center line. Then, at the intersection C on the magnetic pole center line outside the rotor 100, the extension lines of the respective center lines of the slit 105c-2 and the slit 105c-4 intersect.

  The slit 105c-1 and the slit 105c-5 located on the outermost side in the circumferential direction are also inclined at a predetermined angle toward the magnetic pole center line. The inclination angles of the slit 105c-1 and the slit 105c-5 are larger than the inclination angles of the slit 105c-2 and the slit 105c-4. The extension lines of the center lines of the slits 105 c-1 and 105 c-5 also intersect at the intersection C on the magnetic pole center line outside the rotor 100.

  In the magnetic pole c, the distance between the intersection C and the permanent magnet 103 is Lc.

  14 and 15, the configuration of the magnetic pole d will be described mainly with the slit 105d. As shown in FIGS. 14 and 15, the slit 105d includes five slits 105d-1, a slit 105d-2, a slit 105d-3, a slit 105d-4, and a slit 105d-5.

  The center line of the slit 105d-3 substantially coincides with the magnetic pole center line. The slits 105d-2 and 105d-4 on both sides of the slit 105d-3 are inclined at a predetermined angle toward the magnetic pole center line. Then, at the intersection D on the magnetic pole center line outside the rotor 100, the extension lines of the respective center lines of the slit 105d-2 and the slit 105d-4 intersect.

  The slits 105d-1 and 105d-5 located on the outermost side in the circumferential direction are also inclined at a predetermined angle toward the magnetic pole center line. The inclination angles of the slit 105d-1 and the slit 105d-5 are larger than the inclination angles of the slit 105d-2 and the slit 105d-4. The extension lines of the center lines of the slits 105d-1 and 105d-5 also intersect at the intersection D on the magnetic pole center line outside the rotor 100.

  In the magnetic pole d, the distance between the intersection D and the permanent magnet 103 is Ld.

  As described above, the rotor 100 according to the first embodiment is characterized in that the distances La to Ld between the intersections A to D in the magnetic poles a to d and the permanent magnet 103 are different for each magnetic pole.

  However, FIGS. 6 to 15 show an example of La = Lc = L1> Lb = Ld = L2, which is the most preferable mode. In the case of La = Lc = L1> Lb = Ld = L2, the magnetic pole pair constituted by the magnetic pole a and the magnetic pole b and the magnetic pole pair constituted by the magnetic pole c and the magnetic pole d have the same configuration. This is a preferred embodiment.

  However, FIGS. 6 to 15 are examples, and the distance between the intersection A and the permanent magnet 103 in at least one of the magnetic poles a to d may be different from the other magnetic poles.

  As shown in FIG. 5, by changing the distance L between the intersection point A on the extension line of the slit and the permanent magnet, the torque waveform changes, so that La, Lb, Lc, and Ld have different dimensions, One rotor 100 generates four different waveform torques.

  That is, the torque generated in the rotor 100 is a torque obtained by synthesizing torques having different waveforms generated in the magnetic poles a to d. The synthesized torque has a small torque ripple and can form the rotor 100 with low noise.

  FIG. 16 shows torque waveforms when La = Lc = L1 and Lb = Ld = L2 (L1> L2). In FIG. 16, the torque waveform of L = L1 shows the torque waveform when La to Ld are all L1. Moreover, the torque waveform of L = L2 shows a torque waveform when La to Ld are all L2.

  In FIG. 16, the torque waveform of La = Lc = L1 and Lb = Ld = L2 is the most preferable aspect, and torque when La = Lc = L1> Lb = Ld = L2 (rotor 100 shown in FIG. 6). Waveform is shown.

  The torque waveform of La = Lc = L1 and Lb = Ld = L2 is a combination of the torque waveform of L = L1 and the torque waveform of L = L2.

  Thereby, it can be seen that the torque ripple in the torque waveform of La = Lc = L1 and Lb = Ld = L2 is reduced as compared to when La to Ld are all L1 or when La to Ld are all L2. .

  Thus, by setting the distances La to Ld between the magnetic pole a to the magnetic pole d to be La = Lc = L1 and Lb = Ld = L2 (L1> L2), the torque ripple is reduced, and the low-noise rotor 100 is obtained. can get.

  FIG. 17 shows torque waveforms when La = Lb = Lc = L1 and Ld = L2 (L1> L2), La = L1 and Lb = Lc = Ld = L2 (L1> L2). For comparison, torque waveforms of La = Lc = L1 and Lb = Ld = L2 (L1> L2) shown in FIG. 16 are also shown. Further, a torque waveform when La = Lb = Lc = Ld = L1 is also shown.

  La = Lc = L1 and Lb = Ld = L2 (L1> L2), La = Lb = Lc = L1 and Ld = L2 (L1> L2), La = L1 and Lb = Lc = Ld = L2 (L1> L2) In either case, the torque ripple is smaller than when La = Lb = Lc = Ld = L1.

  That is, in at least one of the magnetic poles a to d, the distance between the intersection A and the permanent magnet 103 is made different from that of the other magnetic poles, so that the intersections A to D of the magnetic poles a to d are permanent. Compared to the case where the distance to the magnet 103 is the same, the torque ripple is reduced.

  In particular, it can be seen that the torque ripple is the smallest when La = Lc = L1 and Lb = Ld = L2 (L1> L2).

  By setting La = Lc = L1 and Lb = Ld = L2 (L1> L2), the torque waveforms of the magnetic pole portions of La and Lc and the magnetic pole portions of Lb and Ld change, and the combined value is the torque. Occurs as. As a result, torque pulsation is reduced and torque ripple is reduced.

  The most preferred embodiment of the rotor 100 of FIG. 6 has four poles. When one magnetic pole pair is constituted by the magnetic pole a and the magnetic pole b, the other one magnetic pole pair constituted by the magnetic pole c and the magnetic pole d has the same slit configuration. When this is generalized, if the configuration of each magnetic pole pair is the configuration of the magnetic pole pair of the rotor 100 of FIG. 6 which is the most preferable mode, torque pulsation can be reduced and torque ripple can be reduced.

  A modified rotor 200 will be described with reference to FIGS. In the rotor 200 of the modified example, in each magnetic pole, the intersection of the extension line of the center line of the slit disposed on the outside and the intersection of the extension lines of the slit center lines on both sides of the slit on the magnetic pole center line are Characterized by points located at different points on the center line. The intersection of the extension lines of the center lines of the slits arranged on the outside is farther from the permanent magnet than the intersection of the extension lines of the slit center lines on both sides of the slit on the magnetic pole center line.

  In the rotor 200 according to the modification, four or more slits are formed in one magnetic pole, and two or more intersections of extension lines of the center line of the slit exist at different points on the magnetic pole center line.

  The configuration of the rotor 200 of the modified example is the same as that of the rotor 100 except for the above differences. The configuration of the magnetic poles a to d will be described mainly with the slits 205a to 205d.

  The permanent magnet insertion hole 202, the permanent magnet 203, and the permanent magnet end gap 204 of the rotor core 201 of the rotor 200 of the modified example are the permanent magnet insertion hole 102, the permanent magnet 103, and the permanent magnet end gap 204 of the rotor core 100 of the rotor 100. This is the same as the magnet end gap 104.

  20 and 21, the configuration of the magnetic pole a will be described mainly with the slit 205a. As shown in FIG. 20 and FIG. 21, the slit 205a includes five slits 205a-1, a slit 205a-2, a slit 205a-3, a slit 205a-4, and a slit 205a-5.

  The center line of the slit 205a-3 substantially coincides with the magnetic pole center line. The slits 205a-2 and 205a-4 on both sides of the slit 205a-3 are inclined at a predetermined angle toward the magnetic pole center line. Then, at the intersection A1 on the magnetic pole center line outside the rotor 200, the extension lines of the respective center lines of the slit 205a-2 and the slit 205a-4 intersect.

  The slits 205a-1 and 205a-5 located on the outermost side in the circumferential direction are also inclined at a predetermined angle toward the magnetic pole center line. The inclination angles of the slits 205a-1 and 205a-5 are larger than the inclination angles of the slits 205a-2 and 205a-4. The extension lines of the center lines of the slits 205 a-1 and the slit 205 a-5 intersect at an intersection A 2 on the magnetic pole center line outside the rotor 200.

  In the magnetic pole a, the distance between the intersection A1 and the permanent magnet 203 is La1. The distance between the intersection A2 and the permanent magnet 203 is La2. The distance La1 and the distance La2 have a relationship of La2> La1.

  22 and 23, the configuration of the magnetic pole b will be described mainly with the slit 205b. As shown in FIGS. 22 and 23, the slit 205b includes five slits 205b-1, a slit 205b-2, a slit 205b-3, a slit 205b-4, and a slit 205b-5.

  The center line of the slit 205b-3 substantially coincides with the magnetic pole center line. The slits 205b-2 and 205b-4 on both sides of the slit 205b-3 are inclined at a predetermined angle toward the magnetic pole center line. Then, at the intersection B1 on the magnetic pole center line outside the rotor 200, the extension lines of the respective center lines of the slit 205b-2 and the slit 205b-4 intersect.

  The slit 205b-1 and the slit 205b-5 located on the outermost side in the circumferential direction are also inclined at a predetermined angle toward the magnetic pole center line. The inclination angles of the slits 205b-1 and 205b-5 are larger than the inclination angles of the slits 205b-2 and 205b-4. The extension lines of the center lines of the slits 205b-1 and the slits 105b-5 intersect at an intersection B2 on the magnetic pole center line outside the rotor 200.

  In the magnetic pole b, the distance between the intersection B1 and the permanent magnet 203 is Lb1. Further, the distance between the intersection B2 and the permanent magnet 203 is Lb2. The distance Lb1 and the distance Lb2 have a relationship of Lb2> Lb1.

  24 and 25, the configuration of the magnetic pole c will be described mainly with the slit 205c. As shown in FIGS. 24 and 25, the slit 205c includes five slits 205c-1, a slit 205c-2, a slit 205c-3, a slit 205c-4, and a slit 205c-5.

  The center line of the slit 205c-3 substantially coincides with the magnetic pole center line. The slits 205c-2 and 205c-4 on both sides of the slit 205c-3 are inclined at a predetermined angle toward the magnetic pole center line. Then, at the intersection C1 on the magnetic pole center line outside the rotor 200, the extension lines of the respective center lines of the slit 205c-2 and the slit 205c-4 intersect.

  The slit 205c-1 and the slit 205c-5 located on the outermost side in the circumferential direction are also inclined at a predetermined angle toward the magnetic pole center line. The inclination angles of the slit 205c-1 and the slit 205c-5 are larger than the inclination angles of the slit 205c-2 and the slit 205c-4. The extension lines of the center lines of the slit 205c-1 and the slit 205c-5 intersect at an intersection C2 on the magnetic pole center line outside the rotor 200.

  In the magnetic pole c, the distance between the intersection C1 and the permanent magnet 203 is Lc1. Further, the distance between the intersection C2 and the permanent magnet 203 is Lc2. The distance Lc1 and the distance Lc2 have a relationship of Lc2> Lc1.

  26 and 27, the configuration of the magnetic pole d will be described mainly with the slit 205d. As shown in FIGS. 26 and 27, the slit 205dc includes five slits 205d-1, a slit 205d-2, a slit 205d-3, a slit 205d-4, and a slit 205d-5.

  The center line of the slit 205d-3 substantially coincides with the magnetic pole center line. The slits 205d-2 and 205d-4 on both sides of the slit 205d-3 are inclined at a predetermined angle toward the magnetic pole center line. Then, at the intersection D1 on the magnetic pole center line outside the rotor 200, the extension lines of the respective center lines of the slit 205d-2 and the slit 205d-4 intersect.

  The slit 205d-1 and the slit 205d-5 located on the outermost side in the circumferential direction are also inclined at a predetermined angle toward the magnetic pole center line. The inclination angles of the slits 205d-1 and 205d-5 are larger than the inclination angles of the slits 205d-2 and 205d-4. The extension lines of the center lines of the slits 205d-1 and 205d-5 intersect at an intersection D2 on the magnetic pole center line outside the rotor 200.

  In the magnetic pole d, the distance between the intersection D1 and the permanent magnet 203 is Ld1. The distance between the intersection D2 and the permanent magnet 203 is Ld2. The distance Ld1 and the distance Ld2 have a relationship of Ld2> Ld1.

  For example, in the magnetic pole a of the rotor 200, the intersection A1 corresponds to the intersection A of the magnetic pole a of the rotor 100. The intersection A2 is farther from the permanent magnet 203 than the intersection A.

  However, the relationship is not limited to the above, and it is only necessary that the intersection A1 and the intersection A2 are on the magnetic pole center line and the positions thereof are different.

  As a result of verifying the torque of the rotor 200 of the modified example, a result substantially equivalent to that of the rotor 100 was obtained. That is, in a certain magnetic pole, the intersection of the extension lines of the center line of each slit may be anywhere as long as it is on the magnetic pole center line.

  Further, for example, in the magnetic pole a, when the intersection A2 is located farther from the permanent magnet 203 than the intersection A1 (FIGS. 20 and 21), the inclination angles of the outer slit 205a-1 and slit 205a-2 are rotated. It becomes smaller than the inclination angle of the slits 105a-1 and 105a-2 outside the magnetic pole a of the child 100. Thereby, the circumferential direction dimension of the iron core between the slit 205a-1 and the slit 205a-2 or between the slit 205a-5 and the slit 205a-4 is the same as the slit 105a-1 of the magnetic pole a of the rotor 100. It becomes larger than the circumferential direction dimension of the iron core between the slit 105a-2 or between the slit 105a-5 and the slit 105a-4. As a result, there is an effect that the iron core portion between the slit 205a-1 and the slit 205a-2 or between the slit 205a-5 and the slit 205a-4 is hardly saturated.

  In order to make the magnetic flux generated from the rotor 200 sinusoidal, it is effective to concentrate the magnetic flux at the center of the magnetic pole. By satisfying the relationships La1 <La2, Lb1 <Lb2, Lc1 <Lc2, and Ld1 <Ld2, the slits closer to the magnetic pole center (for example, the slit 205a-2 and the slit 205a-4) are inclined toward the magnetic pole center. This makes it possible to concentrate the magnetic flux more on the magnetic pole center, which is effective in reducing noise.

  The effect of this embodiment can be obtained if there is at least one intersection of the extension line of the center line of the slit with respect to one magnetic pole.

  Even when there are a plurality of intersections of the extension lines of the center line of the slit for one magnetic pole, the effect can be obtained by applying this embodiment to one of the intersections.

  Further, as an effect of the present embodiment, the harmonic component of the induced voltage can be reduced by the slit and the harmonic iron loss can be reduced, so that a highly efficient rotor can be obtained.

  Further, since the rotor with low vibration can be obtained by reducing the torque ripple, the life of the rotor can be extended.

  Moreover, although the rotor demonstrated above was a rotor with 4 poles, even if it is a rotor other than 4 poles, torque ripple can be reduced by applying the shape of this Embodiment. And a rotor with high efficiency and low noise can be obtained.

  Further, the rotor described above has five slits for one magnetic pole. However, the rotor of the present embodiment has a shape in which two or more slits exist for one magnetic pole. There is an effect.

  Further, the winding of the stator (not shown) may be either distributed winding or concentrated winding.

  In addition, when sintered rare earth magnets are used for the permanent magnets 103 and 203, the sintered rare earth magnet has a high magnetic force, so the magnetic flux density of the rotor is higher than when other magnets are used, and the influence of the slits is increased. . Therefore, when a sintered rare earth magnet is used for the rotor, the effect can be further improved.

  Further, by mounting the electric motor (for example, a permanent magnet embedded motor) using the rotors 100 and 200 of the first embodiment on a compressor such as a refrigeration cycle apparatus and a blower such as an air conditioner, high efficiency is achieved. A low-cost, long-life compressor and blower can be obtained.

  DESCRIPTION OF SYMBOLS 100 Rotor, 101 Rotor core, 102 Permanent magnet insertion hole, 103 Permanent magnet, 104 Permanent magnet end space, 105a slit, 105a-1 slit, 105a-2 slit, 105a-3 slit, 105a-4 slit, 105a -5 slit, 105b slit, 105b-1 slit, 105b-2 slit, 105b-3 slit, 105b-4 slit, 105b-5 slit, 105c slit, 105c-1 slit, 105c-2 slit, 105c-3 slit, 105c-4 slit, 105c-5 slit, 105d slit, 105d-1 slit, 105d-2 slit, 105d-3 slit, 105d-4 slit, 105d-5 slit, 200 rotator, 201 Rotor core, 202 permanent magnet insertion hole, 203 permanent magnet, 204 permanent magnet end gap, 205a slit, 205a-1 slit, 205a-2 slit, 205a-3 slit, 205a-4 slit, 205a-5 slit, 205b Slit, 205b-1 slit, 205b-2 slit, 205b-3 slit, 205b-4 slit, 205b-5 slit, 205c slit, 205c-1 slit, 205c-2 slit, 205c-3 slit, 205c-4 slit, 205c-5 slit, 205d slit, 205d-1 slit, 205d-2 slit, 205d-3 slit, 205d-4 slit, 205d-5 slit, 300 rotor, 301 rotor core, 302 Permanent magnet insertion hole, 303 Permanent magnet, 304 Permanent magnet end gap, 305 Slit.

Claims (6)

A rotor core formed by laminating a predetermined number of electromagnetic steel sheets punched into a predetermined shape;
A plurality of permanent magnet insertion holes formed along the outer periphery of the rotor core;
Permanent magnet end gaps provided at both ends of the permanent magnet insertion hole;
A plurality of permanent magnets inserted into the permanent magnet insertion holes;
A plurality of slits formed in the iron core portion outside the permanent magnet insertion hole,
The plurality of slits are formed substantially symmetrically with respect to the magnetic pole center line, and are configured such that at least one intersection of the extension lines of the center line of the slit exists on the magnetic pole center line,
Among the plurality of magnetic poles composed of the plurality of permanent magnets, there is at least one magnetic pole whose distance between the intersection of the extension line of the center line of the slit and the permanent magnet is different from other magnetic poles. A rotor of a permanent magnet embedded motor characterized by the above.   2. The slits are formed in one magnetic pole, and there are two or more intersections of extension lines of the center line of the slits at different points on the magnetic pole center line. Of permanent magnet embedded motor.   The distance between the intersection of the extension line of the center line of the slit far from the magnetic pole center and the permanent magnet and the distance between the intersection of the extension line of the center line of the slit near the magnetic pole center and the permanent magnet are 3. The rotor of an embedded permanent magnet motor according to claim 1, wherein the rotor is small.   The rotor of a permanent magnet embedded motor according to any one of claims 1 to 3, wherein a rare earth magnet is used as the permanent magnet.   A blower comprising the rotor of a permanent magnet embedded motor according to any one of claims 1 to 4.   A compressor comprising the rotor of a permanent magnet embedded motor according to any one of claims 1 to 4.

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