The present disclosure relates to a motor, a blower, and an air conditioner.
There is a known rotor of a motor including two types of permanent magnets having different magnetic properties. For example, a rotor described in Patent Reference 1 includes an annular ferrite bonded magnet, and an annular rare-earth bonded magnet provided on the outer periphery of the ferrite bonded magnet.
Patent Reference 1: Japanese Patent Application Publication No. 2005-151757 (see
In the above-described rotor, a magnetic force is enhanced since the ferrite bonded magnet is combined with the rare-earth bonded magnet. However, the rare-earth bonded magnet is more expensive than the ferrite bonded magnet, and thus it is difficult to reduce the manufacturing cost of the rotor with the annular rare-earth bonded magnet.
It is therefore an object of the present disclosure to reduce the manufacturing cost of a motor.
A motor according to the present disclosure includes a rotor having a shaft and a rotor magnet fixed with respect to the shaft, and a stator surrounding the rotor in a radial direction about the shaft. The rotor magnet includes a first magnet magnetized so as to have polar-anisotropic orientation, and second magnets, the number of which is P (P is an even number), provided on an outer circumference of the first magnet, magnetized so as to have polar-anisotropic orientation, and having a stronger magnetic pole than the first magnet. The stator includes a stator core and a coil wound on the stator core. A length Hr of the rotor magnet in an axial direction of the shaft and a length Hs of the stator core in the axial direction satisfy Hr>Hs. The rotor magnet includes, in the axial direction, a stator-facing portion facing the stator core in the radial direction and an overhang portion protruding from the stator core in the axial direction. The first magnet has grooves, the number of which is P, arranged at equal intervals on the outer circumference at the stator-facing portion. The second magnets are respectively disposed in the grooves. A volume ratio of the second magnets to the first magnet is smaller in the overhang portion than in the stator-facing portion.
According to the present disclosure, the volume ratio of the second magnets to the first magnet is smaller in the overhang portion than in the stator-facing portion, and thus the manufacturing cost can be reduced without decrease in output and efficiency of the motor.
As illustrated in
The rotor 1 includes a shaft 10 as a rotating shaft. The center axis of the shaft 10 defining the rotation center of the rotor 1 will be referred to as a center axis Ax. A direction of the center axis Ax will be referred to as an “axial direction.” A direction along a circumference of a circle about the center axis Ax will be referred to as a “circumferential direction,” and a radial direction of the circle about the center axis Ax will be referred to as a “radial direction.”
The stator 6 includes a stator core 61, a coil 62, an insulator 63 (
The stator core 61 includes a yoke 61a which is annular about the center axis Ax, and a plurality of teeth 61b extending inward in the radial direction from the yoke 61a. The teeth 61b are arranged at equal angles in the circumferential direction. Each tooth 61b faces an outer circumference 1c of the rotor 1 via the air gap G. The number of the teeth 61b is 12 in the example illustrated in
The coil 62 is wound on the teeth 61b of the stator core 61. The coil 62 is made of a copper wire or an aluminum wire. The insulator 63 illustrated in
The molding resin part 64 covers the stator core 61, the coil 62, and the insulator 63. The rotor 1 is housed inside the molding resin part 64, and the shaft 10 projects to one side (to the left in the figure) in the axial direction. Of bearings 11 and 12 supporting the shaft 10, the bearing 11 is held by a bracket 13 attached to the one side (left side in the figure) of the molding resin part 64, and the bearing 12 is held on the other side of the molding resin part 64.
The motor 100 is not limited to the structure in which the stator core 61 and the like are covered with the molding resin part 64, and may have a structure in which the stator core 61 is fitted into a cylindrical frame.
In the example illustrated in
Next, a configuration of the rotor 1 will be described.
The rotor 1 includes a shaft 10 and a rotor magnet 50 fixed with respect to the shaft 10. The rotor magnet 50 includes a ferrite bonded magnet 20 and a plurality of rare-earth bonded magnets 30. The number of the rare-earth bonded magnets 30 is equal to the number P of poles of the rotor 1. The ferrite bonded magnet 20 will also be referred to as a first magnet or a first resin magnet. The rare-earth bonded magnet 30 will also be referred to as a second magnet or a second resin magnet.
When the length of the rotor magnet 50 in the axial direction is expressed as Hr and the length of the stator core 61 in the axial direction is expressed as Hs, the length Hr is longer than the length Hs (Hr>Hs).
The rotor magnet 50 projects from the stator core 61 to one side in the axial direction, for example, downward in
The first end surface 50a of the rotor magnet 50 is located at the same position in the axial direction as a first end surface 60a that is one end surface of the stator core 61 in the axial direction. On the other hand, the second end surface 50b of the rotor magnet 50 is located below a second end surface 60b, which is the other end surface of the stator core 61 in the axial direction, in the figure. That is, the second end surface 50b is located on a side with respect to the second end surface 60b away from the first end surface 50a.
Accordingly, the rotor magnet 50 includes a stator-facing portion 51 and an overhang portion 52 in the axial direction. The stator-facing portion 51 faces the stator core 61 via the air gap. The overhang portion 52 protrudes from the stator core 61 in the axial direction.
The inner cylinder portion 41 is cylindrical and fixed to the outer circumference of the shaft 10. The outer cylinder portion 42 is cylindrical and fixed to the inner circumference of the annular ferrite bonded magnet 20. The ribs 43 couple the inner cylinder portion 41 and the outer cylinder portion 42 to each other. The ribs 43 radially extend outward in the radial direction from the outer circumference of the inner cylinder portion 41. In this regard, it is also possible to fix the ferrite bonded magnet 20 directly to the shaft 10 without providing the resin portion 40.
The ferrite bonded magnet 20 includes a ferrite magnet and a resin. The resin included in the ferrite bonded magnet 20 is, for example, at least one of nylon, polyphenylene sulfide (PPS), and an epoxy resin.
A portion of the ferrite bonded magnet 20 included in the stator-facing portion 51 will be referred to as a first portion 21, and a portion of the ferrite bonded magnet 20 included in the overhang portion 52 will be referred to as a second portion 22.
As illustrated in
The ferrite bonded magnet 20 is magnetized so as to have polar-anisotropic orientation. Accordingly, north poles and south poles are alternately formed on the outer circumference 20c of the ferrite bonded magnet 20.
The first portion 21 of the ferrite bonded magnet 20 includes a plurality of grooves 23 on the outer circumference 20c. The grooves 23 are arranged at equal intervals in the circumferential direction. The grooves 23 are located at positions corresponding to north poles and positions corresponding to north poles. The number of the grooves 23 is equal to the number P of poles of the rotor 1. The rare-earth bonded magnets 30 are disposed in the grooves 23.
Each of the grooves 23 has a bottom surface 23a and side surfaces 23b. The bottom surface 23a is a surface of the groove 23 facing outward in the radial direction. The side surfaces 23b extend outward in the radial direction from both ends of the bottom surface 23a in the width direction. The side surface 23b is a boundary between the ferrite bonded magnet 20 and the rare-earth bonded magnet 30.
In the ferrite bonded magnet 20, magnetic fluxes flowing from the grooves 23 of the south poles travel to the adjacent grooves 23 of the north poles, as indicated by broken lines in
In the ferrite bonded magnet 20, a portion between the groove 23 of the north pole and its adjacent groove 23 of the south pole constitutes an inter-pole portion of the rotor 1.
Each of the rare-earth bonded magnets 30 includes a rare-earth magnet and a resin. Examples of the rare earth magnet include a neodymium magnet containing neodymium (Nd), iron (Fe), and boron (B), and a samarium-iron-nitrogen magnet containing samarium (Sm), Fe, and nitrogen (N), and the like. The resin included in the rare-earth bonded magnets 30 is the same as the resin included in the ferrite bonded magnet 20, for example. That is, the resin included in the rare-earth bonded magnets 30 is at least one of nylon, PPS, and an epoxy resin, for example.
The strength of magnetic poles (i.e., magnetic quantity) of the rare-earth bonded magnets 30 is greater than the strength of the magnetic pole of the ferrite bonded magnet 20. In other words, a magnetic force of the rare-earth bonded magnets 30 is greater than a magnetic force of the ferrite bonded magnet 20. That is, the rare-earth bonded magnets 30 are made of a material different from the ferrite bonded magnet 20, and have magnetic properties different from those of the ferrite bonded magnet 20.
The rare-earth bonded magnets 30 are arranged at equal intervals in the circumferential direction. More specifically, the rare-earth bonded magnets 30 are disposed in the grooves 23 of the ferrite bonded magnet 20. In the first embodiment, the rare-earth bonded magnets 30 are bonded to the grooves 23 of the ferrite bonded magnet 20 by integral molding (also referred to as “double molding”) of the ferrite bonded magnet 20 and the rare-earth bonded magnets 30.
The rare-earth bonded magnets 30 are magnetized so as to have polar-anisotropic orientation. Each two of the rare-earth bonded magnets 30 adjacent to each other in the circumferential direction have magnetic poles of different polarities. Outer circumferences 30c of the rare-earth bonded magnets 30 form parts of the outer circumference 1c of the rotor 1 (see
The ferrite bonded magnet 20 and the rare-earth bonded magnets 30 are integrally molded by filling the grooves 23 with a material for the rare-earth bonded magnets 30 in a state where the previously produced ferrite bonded magnet 20 is disposed in a mold. As compared to a manufacturing process in which the ferrite bonded magnet 20 is molded with the previously produced rare-earth bonded magnets 30 disposed in a mold, the work of disposing the rare-earth bonded magnets 30 in the mold one by one can be eliminated, and thus, the manufacturing process of the rotor 1 can be simplified.
Each of the rare-earth bonded magnets 30 has an outer circumferential surface facing outward in the radial direction and an inner circumferential surface facing inward in the radial direction. In the example illustrated in
The outer diameter of the overhang portion 52 of the rotor magnet 50 is equal to the outer diameter of the stator-facing portion 51. Thus, the outer circumference of the second portion 22 of the ferrite bonded magnet 20 is located on the same cylindrical surface as the outer circumference of the first portion 21, and forms a portion of the outer circumference 20c described above.
The ferrite bonded magnet 20 is magnetized as described with reference to
The ferrite bonded magnet 20 has an end surface 20a constituting a portion of the first end surface 50a of the rotor magnet 50. The grooves 23 are open at the end surface 20a. Thus, the rare-earth bonded magnets 30 have end surfaces 30a constituting a portion of the first end surface 50a of the rotor magnet 50.
Next, functions of the first embodiment will be described in comparison with first and second comparative examples.
The rotor 1F of the first comparative example includes a shaft 10 and a rotor magnet 50 fixed with respect to the shaft 10. The rotor magnet 50 includes a ferrite bonded magnet 20 and an annular rare-earth bonded magnet 34 covering the outer circumference of the ferrite bonded magnet 20. A length Hr of the rotor magnet 50 in the axial direction is equal to the length Hs of the stator core 61 (
In the rotor 1F of the first comparative example, the rare-earth bonded magnet 34 is formed in an annular shape to cover the outer circumference of the ferrite bonded magnet 20. Thus, magnetic flux density distribution on the surface of the rotor magnet 50 can be made close to a sine wave.
However, the rare-earth bonded magnet 34 has the annular shape and has a thickness necessary for obtaining sufficient strength in the radial direction, and thus the amount of use of the rare-earth bonded magnets 30 is large. A unit price of a material for the rare-earth bonded magnet 30 is greater than or equal to 10 times a unit price of a material for the ferrite bonded magnet 20. Thus, as the amount of use of the rare-earth bonded magnets 30 increases, the manufacturing cost of the rotor 1F increases.
The rotor 1G of the second comparative example includes a shaft 10 and a rotor magnet 50 fixed with respect to the shaft 10. The rotor magnet 50 includes a ferrite bonded magnet 20 and a plurality of rare-earth bonded magnets 30 arranged on the outer circumference of the ferrite bonded magnet 20. A length Hr of the rotor magnet 50 in the axial direction is equal to a length Hs of the stator core 61 (
In the rotor 1G of the second comparative example, the rare-earth bonded magnets 30 are distributed in the circumferential direction. Accordingly, as compared to the rotor 1F of the first comparative example, the amount of use of the rare-earth bonded magnets 30 can be reduced by, for example, 208, and thus the manufacturing cost of the rotor 1G can be reduced.
Although the magnetic force of the ferrite bonded magnet 20 is smaller than that of the rare-earth bonded magnets 30, the rotor magnet 50 has polar-anisotropic orientation, and the rare-earth bonded magnets 30 are arranged at magnetic pole centers. Thus, it is possible to suppress a decrease of the surface magnetic flux density due to the small amount of use of the rare-earth bonded magnets 30.
However, in the rotor 1G of the second comparative example, since the length Hr of the rotor magnet 50 in the axial direction is equal to the length Hs of the stator core 61 in the axial direction, magnetic fluxes flowing into the stator core 61 are only magnetic fluxes flowing from the ferrite bonded magnet 20 and the rare-earth bonded magnets 30 into the inner circumferential surface of the stator core 61. Thus, it is difficult to increase the magnetic fluxes flowing into the stator core 61. When the length Hr of the rotor magnet 50 in the axial direction is increased, the amount of use of the rare-earth bonded magnets 30 increases accordingly, and the manufacturing cost increases.
On the other hand, in the rotor 1 of the first embodiment, in a manner similar to the rotor 1G of the second comparative example, the rare-earth bonded magnets 30 are distributed in the circumferential direction (see
Further, in the rotor 1 of the first embodiment, since the rotor magnet 50 includes the stator-facing portion 51 and the overhang portion 52 (see
In this example, most part of magnetic fluxes flowing from the overhang portion 52 flows into the end surface of the stator core 61 in the axial direction, but a part of magnetic fluxes becomes leakage fluxes that do not flow into the stator core 61. Thus, the overhang portion 52 is constituted by the ferrite bonded magnet 20 with a low magnetic force, so that magnetic fluxes flowing into the stator core 61 can be increased while reducing the manufacturing cost.
Next, a manufacturing method of the rotor 1 will be described.
In step ST1, the inside of the first mold for molding the ferrite bonded magnet 20 is filled with a material for the ferrite bonded magnet 20. The ferrite bonded magnet 20 is molded by injection molding, for example. The molding method of the ferrite bonded magnet 20 is not limited to injection molding, and may be other molding method such as pressure molding.
In step ST2, the ferrite bonded magnet 20 is molded into a predetermined shape while being oriented. In step ST2, for example, in a state where a magnetic field having a polar anisotropy is generated inside the first mold by using the magnets for orientation, the ferrite bonded magnet 20 is molded so that the material for the ferrite bonded magnet 20 is oriented. In this manner, the ferrite bonded magnet 20 having polar anisotropy is molded.
In step ST3, the molded ferrite bonded magnet 20 is cooled.
In step ST4, the ferrite bonded magnet 20 is taken out from the first mold.
In step ST5, the resulting ferrite bonded magnet 20 is demagnetized.
In step ST6, the ferrite bonded magnet 20 is placed in the second mold for injection molding of the rare-earth bonded magnets 30.
In step ST7, the second mold is filled with the material for the rare-earth bonded magnets 30. The rare-earth bonded magnets 30 are molded by injection molding, for example. The rare-earth bonded magnets 30 may also be molded by other molding methods such as pressure molding as well as injection molding.
As an example, as schematically illustrated in
In step ST8, while the material for the rare-earth bonded magnets 30 is oriented, the rare-earth bonded magnets 30 are shaped into predetermined shapes. In step ST8, in a state where a magnetic field having a polar anisotropy is generated in the second mold by using the magnet for orientation, for example, the rare-earth bonded magnets 30 are molded so that the material for the rare-earth bonded magnets 30 are oriented. In this manner, the rotor magnet 50 in which the ferrite bonded magnet 20 and the plurality of rare-earth bonded magnets 30 are integrally molded is formed.
In step ST9, the rotor magnet 50 formed in step ST8 is cooled.
In step ST10, the cooled rotor magnet 50 is taken out from the second mold.
In step ST11, the rotor magnet 50 taken out in step ST10 is demagnetized.
In step ST12, the rotor magnet 50 is coupled to the shaft 10. As an example, the rotor magnet 50 and the shaft 10 are placed in a third mold, and the third mold is filled with a thermoplastic resin such as PBT, and the resin portion 40 is molded. Accordingly, the rotor magnet 50 is coupled to the shaft 10 through the resin portion 40.
In step ST13, the rotor magnet 50 is magnetized by using a magnetizer, for example. In this manner, the rotor 1 is completed.
In the example described here, the overhang portion 52 does not include the rare-earth bonded magnets 30 and includes only the ferrite bonded magnet 20. However, it is sufficient that a volume ratio of the rare-earth bonded magnets 30 to the ferrite bonded magnet 20 is smaller in the overhang portion 52 than in the stator-facing portion 51.
As an example, the volume ratio of the rare-earth bonded magnets 30 to the ferrite bonded magnet 20 is, for example, 25% in stator-facing portion 51, and is, for example, 0% in the overhang portion 52. An example in which the volume ratio of the rare-earth bonded magnets 30 is larger than 0% in the overhang portion 52 will be described in a third embodiment.
Although description has been made of the configuration in which the overhang portion 52 is provided only on one end of the rotor magnet 50 in the axial direction, the overhang portion 52 may be provided on each end of the rotor magnet 50 in the axial direction. In this regard, the configuration in which the overhang portion 52 is provided only on one end of the rotor magnet 50 in the axial direction is more preferable. This is because the grooves 23 are open at the end surface 20a of the ferrite bonded magnet 20 (see
As described above, in the first embodiment, the rotor magnet 50 of the rotor 1 includes the ferrite bonded magnet 20 as a first magnet and the P rare-earth bonded magnets 30 (P is an integer of two or more) as second magnets. The ferrite bonded magnet 20 is magnetized so as to have polar-anisotropic orientation. The rare-earth bonded magnets 30 are provided on the outer circumference of the ferrite bonded magnet 20, magnetized so as to have polar-anisotropic orientation, and have a stronger magnetic pole than the ferrite bonded magnet 20. The length Hr of the rotor magnet 50 in the axial direction and the length Hs of the stator core 61 in the axial direction satisfy Hr>Hs. The rotor magnet 50 includes, in the axial direction, the stator-facing portion 51 facing the stator core 61 in the radial direction and the overhang portion 52 projecting from the stator core 61 in the axial direction. The volume ratio of the rare-earth bonded magnets 30 to the ferrite bonded magnet 20 is smaller in the overhang portion 52 than in the stator-facing portion 51.
Since the rare-earth bonded magnets 30 are distributed in the circumferential direction as above, the amount of use of the rare-earth bonded magnets 30 can be reduced, and the manufacturing cost of the motor 100 can be reduced. In addition, since the rotor magnet 50 includes the stator-facing portion 51 and the overhang portion 52, effective magnetic fluxes flowing into the stator core 61 can be increased. Further, since the volume ratio of the rare-earth bonded magnets 30 to the ferrite bonded magnet 20 is smaller in the overhang portion 52 than in the stator-facing portion 51, the manufacturing cost can be reduced without decrease in output and efficiency of the motor 100.
In particular, since the overhang portion 52 of the rotor magnet 50 does not include the rare-earth bonded magnets 30 and includes only the ferrite bonded magnet 20, the amount of use of the rare-earth bonded magnets 30 can be further reduced, and the manufacturing cost can be further reduced.
Next, a second embodiment will be described. A motor according to the second embodiment is different from the motor 100 of the first embodiment in the configuration of a rotor 1A.
Similarly to the rotor 1 of the first embodiment, the rotor 1A includes the shaft 10 and the rotor magnet 50. The rotor magnet 50 includes the ferrite bonded magnet 20 as a first magnet and the plurality of rare-earth bonded magnets 30 as second magnets. The rotor magnet 50 includes the stator-facing portion 51 and the overhang portion 52 in the axial direction.
The bottom surface 23a extends in an arc shape projecting inward in the radial direction in
The rare-earth bonded magnet 30 has an outer circumferential surface 31 facing outward in the radial direction, an inner circumferential surface 32 facing inward in the radial direction, and side surfaces 33 at both sides in the circumferential direction. The outer circumferential surface 31 extends in an arc shape about a center axis Ax. The inner circumferential surface 32 extends in an arc shape projecting inward in the radial direction. In this regard, the inner circumferential surface 32 may extend in an arc shape projecting outward in the radial direction or may extend linearly as long as the inner circumferential surface 32 has a shape in conformity with the bottom surface 23a.
In a plane orthogonal to the center axis Ax, a length W2 of the inner circumferential surface 32 of the rare-earth bonded magnet 30 is longer than a length W1 of the outer circumferential surface 31 of the rare-earth bonded magnet 30. Thus, in a plane orthogonal to the center axis Ax, the length of the bottom surface 23a of the groove 23 of the ferrite bonded magnet 20 is longer than the length of an opening of the groove 23 on the outer circumference 20c side.
With this configuration, the rare-earth bonded magnets 30 can be held in the groove 23 of the ferrite bonded magnet 20 so that the rare-earth bonded magnets 30 are not detached outward in the radial direction. Accordingly, detachment of the rare-earth bonded magnets 30 from the ferrite bonded magnet 20 can be prevented, even when separation occurs at an interface between the ferrite bonded magnet 20 and each rare-earth bonded magnet 30 due to a difference in thermal expansion coefficient between the ferrite bonded magnet 20 and the rare-earth bonded magnet 30 or when a centrifugal force caused by rotation of the rotor 1A is exerted thereon.
Except for the aspects described above, the rotor 1A of the second embodiment is configured in a similar manner to the rotor 1 of the first embodiment.
As described above, in the second embodiment, since the length W2 of the inner circumferential surface 32 of the rare-earth bonded magnet 30 is longer than the length W1 of the outer circumferential surface 31 of the rare-earth bonded magnet 30, detachment of the rare-earth bonded magnets 30 from the ferrite bonded magnet 20 can be prevented, and reliability of the motor can be enhanced.
Next, a third embodiment will be described. A motor according to the third embodiment is different from the motor 100 of the first embodiment in a configuration of a rotor 1B.
Similarly to the rotor 1 of the first embodiment, the rotor 1B includes the shaft 10 and the rotor magnet 50. The rotor magnet 50 includes the ferrite bonded magnet 20 as a first magnet and the plurality of rare-earth bonded magnets 30 as second magnets. The rotor magnet 50 includes the stator-facing portion 51 and the overhang portion 52 in the axial direction.
As illustrated in
As illustrated in
The projections 35 of the rare-earth bonded magnets 30 are formed in the process of step ST7 in
In the third embodiment, the overhang portion 52 includes the rare-earth bonded magnets 30 (i.e., projections 35) as well as the ferrite bonded magnet 20. In this regard, a volume ratio of the rare-earth bonded magnets 30 to the ferrite bonded magnet 20 is smaller in the overhang portion 52 than in the stator-facing portion 51.
Since the projections 35 of the rare-earth bonded magnet 30 are engaged with the recesses 25 of the ferrite bonded magnet 20, the rare-earth bonded magnets 30 can be firmly fixed to the ferrite bonded magnet 20. That is, detachment of the rare-earth bonded magnets 30 from the ferrite bonded magnet 20 can be prevented, even when separation occurs at the interface between the ferrite bonded magnet 20 and each rare-earth bonded magnet 30 due to a difference in thermal expansion coefficient between the ferrite bonded magnet 20 and the rare-earth bonded magnet 30 or when a centrifugal force due to rotation of the rotor 1B is exerted thereon.
Except for the aspects described above, the rotor 1B of the third embodiment is configured in a similar manner to the rotor 1 of the first embodiment. As described in the second embodiment, the length W2 of the inner circumferential surface 32 of the rare-earth bonded magnet 30 may be longer than the length W1 of the outer circumferential surface 31 of the rare-earth bonded magnet 30.
As described above, in the third embodiment, since the projections 35 of the rare-earth bonded magnets 30 are engaged with the recesses 25 of the ferrite bonded magnet 20, detachment of the rare-earth bonded magnets 30 from the ferrite bonded magnet 20 is prevented, and reliability of the motor can be enhanced.
The example in which the ferrite bonded magnet 20 includes the recesses 25 and the rare-earth bonded magnets 30 include the projections 35 has been described. However, the ferrite bonded magnet 20 may include projections 27 and the rare-earth bonded magnets 30 may include recesses 37, as shown in a modification of
In this case, in the process of step ST7 in
Next, a fourth embodiment will be described. A motor according to the fourth embodiment is different from the motor 100 of the first embodiment in a configuration of a rotor 1C.
Similarly to the rotor 1 of the first embodiment, the rotor 1C includes the shaft 10 and the rotor magnet 50. The rotor magnet 50 includes the ferrite bonded magnet 20 as a first magnet and the plurality of rare-earth bonded magnets 30 as second magnets. The rotor magnet 50 includes the stator-facing portion 51 and the overhang portion 52 in the axial direction.
As illustrated in
The protrusions 36 of the rare-earth bonded magnets 30 are formed in the process of step ST7 in
Since the protrusions 36 of the rare-earth bonded magnet 30 are engaged with the receiving portions 26 of the ferrite bonded magnet 20, the rare-earth bonded magnets 30 can be firmly fixed to the ferrite bonded magnet 20. That is, detachment of the rare-earth bonded magnets 30 can be prevented, even when separation occurs at the interface between the ferrite bonded magnet 20 and each rare-earth bonded magnet 30 due to a difference in thermal expansion coefficient between the ferrite bonded magnet 20 and the rare-earth bonded magnet 30 or when a centrifugal force due to rotation of the rotor 1C is exerted thereon.
Except for the aspects described above, the rotor 1C of the fourth embodiment is configured in a similar manner to the rotor 1 of the first embodiment.
As described above, in the fourth embodiment, since the protrusions 36 of the rare-earth bonded magnets 30 are engaged with the receiving portions 26 of the ferrite bonded magnet 20, detachment of the rare-earth bonded magnets 30 from the ferrite bonded magnet 20 can be prevented, and reliability of the motor can be enhanced. In addition, since the protrusions 36 of the rare-earth bonded magnets 30 are formed at an end of the rotor magnet 50 on the first end surface 50a side, molding by means of a mold can be facilitated.
In this regard, although the rotor magnet 50 includes the recesses 25 and the projections 35 described in the third embodiment in
Next, a fifth embodiment will be described. A motor according to the fifth embodiment is different from the motor 100 of the first embodiment in a configuration of a rotor 1D.
Similarly to the rotor 1 of the first embodiment, the rotor 1D includes the shaft 10 and the rotor magnet 50. The rotor magnet 50 includes the ferrite bonded magnet 20 as a first magnet and the plurality of rare-earth bonded magnets 30 as second magnets. The rotor magnet 50 includes the stator-facing portion 51 and the overhang portion 52 in the axial direction.
Accordingly, in the rotor 1D, the outer diameter of the overhang portion 52 is larger than the outer diameter of the stator-facing portion 51. More specifically, a distance R1 from the center axis Ax to the outer circumference of the stator-facing portion 51 and a distance R2 from the center axis Ax to the outer circumference of the overhang portion 52 satisfy R1<R2.
The stator-facing portion 51 faces the stator core 61 via an air gap, and thus there is a limitation in increasing the outer diameter of the stator-facing portion 51. On the other hand, the overhang portion 52 protrudes from the stator core 61 in the axial direction, and thus the outer diameter of the overhang portion 52 can be made larger than the outer diameter of the stator-facing portion 51.
By increasing the outer diameter of the overhang portion 52 as above, magnetic fluxes flowing into the stator core 61 by way of the overhang portion 52 can be increased.
Except for the aspects described above, the rotor 1D of the fifth embodiment is configured in a similar manner to the rotor 1 of the first embodiment.
As described above, in the fifth embodiment, since the outer diameter of the overhang portion 52 is larger than the outer diameter of the stator-facing portion 51, magnetic fluxes flowing into the stator core 61 can be increased.
The fifth embodiment may be combined with features described in the second embodiment, the third embodiment, the modification, or the fourth embodiment.
Next, a sixth embodiment will be described. A motor according to the sixth embodiment is different from the motor 100 of the first embodiment in a configuration of a rotor 1E.
Similarly to the rotor 1 of the first embodiment, the rotor 1E includes the shaft 10 and the rotor magnet 50. The rotor magnet 50 includes the ferrite bonded magnet 20 as a first magnet and the plurality of rare-earth bonded magnets 30 as second magnets. The rotor magnet 50 includes the stator-facing portion 51 and the overhang portion 52 in the axial direction.
As illustrated in
The cover member 70 is made of a resin. More specifically, the cover member 70 is made of a resin different from those of the ferrite bonded magnet and the rare-earth bonded magnets. In particular, the cover member 70 is preferably made of the same material as the resin portion 40, for example, a thermoplastic resin such as PBT.
As illustrated in
As illustrated in
In this case, a natural frequency and an inertia of the rotor 1E can be adjusted by adjusting dimensions and the like of ribs 43 of the resin portion 40.
The natural frequency of the rotor 1E depends on rigidity of the rotor 1E, and thus the natural frequency can be adjusted by changing the radial length of the ribs 43, the circumferential width of the ribs 43, or the number of the ribs 43. The adjustment of the natural frequency of the rotor 1E can reduce vibrations caused by resonance.
The inertia of the rotor 1E depends on the mass of the rotor 1E, and thus the inertia of the rotor 1E can be adjusted by changing the radial length of the ribs 43, the circumferential width of the ribs 43, or the number of the ribs 43. When the inertia of the rotor 1E is increased, a torque necessary for start increases, but rotation of the rotation 1E can be stabilized.
In this embodiment, the cover member 70 is provided at the first end surface 50a of the rotor magnet 50, but the cover member 70 may be provided at each of the first end surface 50a and the second end surface 50b. In this case, integrity of the rotor 1E can be further enhanced.
Alternatively, the end surface 20a of the ferrite bonded magnet 20 and the end surfaces 30a of the rare-earth bonded magnets 30 may be provided with convexes and concaves, and the cover members 70 may be provided to cover the convexes and concaves.
Except for the aspects described above, the rotor 1E of the sixth embodiment is configured in a similar manner to the rotor 1 of the first embodiment.
As described above, the rotor 1E of the sixth embodiment includes the cover member 70 covering at least a portion of each of the ferrite bonded magnet 20 and at least a portion of each rare-earth bonded magnet 30 at the first end surface 50a of the rotor magnet 50. Thus, the rare-earth bonded magnets 30 can be firmly fixed to the ferrite bonded magnet 20. Accordingly, detachment of the rare-earth bonded magnets 30 from the ferrite bonded magnet 20 can be prevented against a temperature change or a centrifugal force.
Further, in a case where the cover member 70 is made of the same material as the resin portion 40 and integrally molded with the resin portion 40, the resin portion 40 and the cover member 70 can be integrally molded by placing the shaft 10 and the rotor magnet 50 in the mold and filling the mold with a resin. Accordingly, the manufacturing process of the rotor 1E can be simplified.
The sixth embodiment may be combined with features described in the second embodiment, the third embodiment, the modification, the fourth embodiment, or the fifth embodiment.
Next, a configuration of a blower 200 according to a seventh embodiment will be described.
As illustrated in
The blower 200 according to the seventh embodiment includes the motor 100 described in the first embodiment, and thus the manufacturing cost can be reduced while suppressing decrease in output and efficiency of the blower 200. In the case of using the motor described in any one of the second through sixth embodiments instead of the motor 100 described in the first embodiment, similar advantages can be obtained.
Next, a configuration of an air conditioner 300 including the blower 200 according to an eighth embodiment will be described.
As illustrated in
The indoor unit 310 includes an indoor blower 311 and a housing 312 housing the indoor blower 311. The indoor blower 311 includes a motor 311a and a fan 311b that is driven by the motor 311a. The fan 311b is attached to a shaft of the motor 311a. When the shaft of the motor 311a rotates, the fan 311b rotates, and an airflow is generated. The fan 311b is, for example, a crossflow fan.
The outdoor unit 320 includes a blower 200 as an outdoor blower, a compressor 321, and a housing 322 housing the blower 200 and the compressor 321. The compressor 321 includes a compressor mechanism 321a that compresses a refrigerant, and a motor 321b that drives the compressor mechanism 321a. The compressor mechanism 321a and the motor 321b are coupled to each other by a shaft 321c. The motor 100 according to the first embodiment may be used as the motor 321b of the compressor 321.
For example, in a cooling operation of the air conditioner 300, heat is released when the refrigerant compressed by the compressor 321 is condensed by a condenser (not shown), and the heat is released to the outside with air sent from the blower 200. The outdoor unit 320 further includes a four-way valve (not shown) that switches a flow direction of refrigerant. The four-way valve of the outdoor unit 320 causes a high-temperature and high-pressure gas sent from the compressor 321 to flow to a heat exchanger of the outdoor unit 320 in a cooling operation and to flow to a heat exchanger of the indoor unit 310 in a heating operation.
The blower 200 is not limited to the outdoor blower of the outdoor unit 320, and may be used as the indoor blower 311 described above. The blower 200 is not limited to the air conditioner 300, and may be included in other electric equipment.
The air conditioner 300 according to the eighth embodiment includes the blower 200 described in the seventh embodiment, and thus the manufacturing cost can be reduced while suppressing decrease in output and efficiency of the air conditioner 300.
Although the preferred embodiments have been specifically described above, the present disclosure is not limited to these embodiments, and various improvements and modifications may be made.
This application is a U.S. national stage application of PCT/JP2022/017114 filed Apr. 5, 2022, the contents of which are incorporated herein by reference.
| Filing Document | Filing Date | Country | Kind |
|---|---|---|---|
| PCT/JP2022/017114 | 4/5/2022 | WO |