The present disclosure relates to a rotating electric machine, a compressor, and a refrigeration apparatus.
Japanese Unexamined Patent Publication No. H10-89252 describes a motor with a rotor having an end surface protruding more upward than an end surface of a stator. In this motor, the height of the center of the rotor in the axial directions shifts upward from the height of the center of the stator in the axial directions. The effect of the magnetic pull force biases the rotor downward. This reduces the vertical vibration of the drive shaft below the motor.
A first aspect is directed to a rotating electric machine including: a rotor including a rotor core configured to rotate about a rotation axis and a plurality of permanent magnets in magnet holes provided in the rotor core; and a stator including a stator core radially outside the rotor. When a first direction represents one of axial directions of the rotation axis and a second direction represents the other, the rotor core includes: a first core section at least partially opposed to the stator core in radial directions, and having substantially the same cross sectional shape perpendicular to the axial directions of the rotation axis; and a second core section adjacent to an end of the first core section in the first direction and having substantially the same cross sectional shape perpendicular to the axial directions of the rotation axis. The second core section is at least partially ahead of an end of the stator core in the first direction, and has a magnetic resistance structure with a lower magnetic permeability than the first core section. The magnetic resistance structure is formed in a magnetic pole section of the rotor and radially outside the plurality of permanent magnets.
Embodiments of the present invention will be described in detail below with reference to the drawings. The following embodiments are merely exemplary ones in nature, and are not intended to limit the scope, applications, or use of the invention. Features of the embodiments, variations, and other examples described below can be combined or partially substituted within the range where the present invention can be embodied. In the drawings described below, hatching indicating a cross section is partly omitted in some cases.
As shown in
In the refrigeration cycle, the refrigerant compressed by the compressor (10) dissipates heat to air in the radiator (2). The refrigerant which has dissipated the heat is decompressed by the expansion valve (3) and evaporates in the evaporator (4). The evaporated refrigerant is sucked into the compressor (10) (see the arrows in
As shown in
The casing (11) is a hermetic container. The inside of the casing (11) is filled with high-pressure refrigerant discharged from the compression mechanism (50).
The casing (11) is made of a metal material. The casing (11) includes a barrel (12), a bottom (13), and a top (14). The barrel (12) is a tubular member extending in the vertical direction. The axial directions of the tube of the barrel (12) correspond to the vertical direction. The bottom (13) closes the lower end of the barrel (12), while the top (14) closes the upper end of the barrel (12).
The casing (11) houses the motor (20), the drive shaft (40), and the compression mechanism (50). The motor (20), the drive shaft (40), and the compression mechanism (50) are arranged in the casing (11) in this order from the top.
As shown in
The stator (21) is fixed to the inner circumferential surface of the barrel (12). The stator (21) includes a stator core (22). The stator core (22) is disposed radially outside the rotor (31). The stator core (22) is formed by stacking a plurality of electromagnetic steel sheets in the axial directions. The stator core (22) includes an annular back yoke (24) and teeth (25). Six core cuts (26) are provided in the outer circumferential surface of the back yoke (24). The core cuts (26) are grooves extending in the axial directions of the stator core (22). The teeth (25) extend radially inward from the inner circumferential surface of the back yoke (24). In this embodiment, six teeth (25) are aligned at equal pitches (specifically, 60° pitches) in the circumferential directions. The stator (21) includes a coil (23). The coil (23) is wound around the teeth (25) (see
As shown in
The permanent magnets (33) are arranged inside the rotor core (32). The permanent magnets (33) according to this embodiment are ferrite magnets. The permanent magnets (33) are arranged inside slots (34) in the rotor core (32). The slots (34) penetrate the rotor core (32) in the axial directions. The slots (34) extend radially outward from the center of the rotation axis (O) as viewed in the axial directions. Specifically, six slots (34) each in a V-shape as viewed from above are arranged at equal intervals in the circumferential directions of the rotor (31).
Each of the permanent magnets (33) is provided in one of the six slots (34). That is, the rotor (31) according to this embodiment includes six permanent magnets (33). The six permanent magnets (33) are arranged in the circumferential directions of the rotor core (32) and penetrate the rotor core (32) in the axial directions. Each of the permanent magnets (33) has the same cross-sectional shape orthogonal to the axial directions (see
As viewed in the axial directions, the permanent magnets (33) are each configured in the V-shape to be fitted in the associated slot (34). Specifically, each of the permanent magnets (33) includes a first magnetic part (33a) in a V-shape as viewed in the axial directions, and a second magnetic part (33b) and a third magnetic part (33c) each extending radially outward from an end of the first magnetic part (33a). As viewed in the axial directions, the second magnetic part (33b) and the third magnetic part (33c) extend linearly to the vicinity of the outer circumferential end of the rotor (31). The second magnetic part (33b) and the third magnetic part (33c) are adjacent to each other in the circumferential directions of the rotor (31).
As shown in
The compression mechanism (50) has a cylinder (51) and a piston (52) provided inside the cylinder (51). A cylinder chamber (53) is formed between the inner peripheral surface of the cylinder (51) and the outer peripheral surface of the piston (52). In the cylinder chamber (53), the fluid is compressed by the piston (52) driven by the drive shaft (40).
The compressor (10) has a suction pipe (15) and a discharge pipe (16). The suction pipe (15) penetrates the barrel (12) in the radial directions, and communicates with the cylinder chamber (53). A low-pressure refrigerant in the refrigerant circuit (1a) is sucked through the suction pipe (15) into the cylinder chamber (53). The discharge pipe (16) penetrates the top (14) in the axial directions, and communicates with the internal space of the casing (11). The refrigerant compressed in the compression mechanism (50) flows through portions, such as the core cuts (26) of the motor (20), and is then sent through the discharge pipe (16) to the refrigerant circuit (1a).
In view of the manufacturing costs of the motor, relatively inexpensive ferrite magnets are preferably applied to the motor. However, since the ferrite magnets have a relatively low magnetic force, there is a need to increase the surface areas of the ferrite magnets provided in the rotor core so that the motor exhibits predetermined performance. For example, the surface areas of the ferrite magnets can be increased by increasing the thickness of the rotor in the axial directions.
In the rotary compressor according to this embodiment, there is a demand to reduce the anomalous sound from the compression mechanism, which is generated when the drive shaft is vibrated vertically by driving the motor. To meet this demand, if the drive shaft is biased downward, a relatively strong thrust force then acts on the lower bearing, which reduces the vertical vibration of the drive shaft. As a method of biasing the drive shaft downward in this manner, the use of a pull force acting between the rotor and the stator is conceivable. That is, if the rotor core is disposed to protrude more upward than the stator core in the axial directions, pull force of pulling the rotor downward acts.
Specifically, as shown in
However, as shown in
In contrast to this, by largely deviating the magnetic center of the rotor core upward from the magnetic center of the stator core, a sufficient pull force biasing the rotor downward can be provided. However, with an increase in the area of the part of the stator core not opposed to the rotor core, the magnetic flux density between the stator core and the rotor core decreases, which may deteriorate the performance (particularly, the torque performance) of the motor. If the magnetic centers of the stator core and the rotor core are largely apart from each other, the length of the entire motor in the axial directions increases and eventually the size of the motor increases.
To address such a problem, the rotor core (32) of the motor (20) according to this embodiment has the magnetic resistance structures (R). These magnetic resistance structures (R) reduce the deterioration in the performance of the motor (20) and can sufficiently generate a downward pull force on the rotor (31). The rotor core (32) and the magnetic resistance structures (R) according to this embodiment will be described in detail below.
As shown in
The first core section (32a) is at least partially opposed to the stator core (22) in radial directions, and has a substantially constant cross sectional shape perpendicular to the axial directions of the rotation axis (O). The length D1 of the first core section (32a) in the axial directions (i.e., the vertical direction) is equal to the length D2 of the stator core (22) in the axial directions (i.e., the vertical direction). The upper end of the first core section (32a) shifts upward from the upper end of the stator core (22). The lower end of the first core section (32a) shifts upward from the lower end of the stator core (22).
The second core section (32b) is adjacent to the upper end of the first core section (32a). The second core section (32b) is disposed above the upper end of the stator core (22). That is, the second core section (32b) protrudes more upward than the upper end of the stator core (22).
The third core section (32c) is adjacent to the lower end of the first core section (32a). A part of the third core section (32c) is disposed below the lower end of the stator core (22). That is, a part of the third core section (32c) protrudes more downward than the lower end of the stator core (22).
In this manner, the rotor core (32) is longer than the stator core (22) in the axial directions. The center (i.e., the magnetic center) of the rotor core (32) in the axial directions shifts upward from the center (i.e., the magnetic center) of the stator core (22) in the axial directions.
The first core section (32a), the second core section (32b), and the third core section (32c) have the completely or substantially constant cross-sectional shape perpendicular to the axial directions of the rotation axis (O). The range of “substantially the same” includes variations in the rotor core (32) at the time of manufacturing, the case where the rotor (31) has skews (oblique grooves), or slight differences that have relatively small influences on the motor characteristics.
The first core section (32a) and the second core section (32b) have the completely or substantially constant cross-sectional shape perpendicular to the axial directions, except for the magnetic resistance structure (R). The first core section (32a) and the third core section (32c) have the completely or substantially constant cross-sectional shape perpendicular to the axial directions, except for the magnetic resistance structure (R).
On the outer circumferential surface of the rotor core (32), the first core section (32a) and the second core section (32b) are smoothly connected to each other, and the first core section (32a) and the third core section (32c) are smoothly connected to each other. In other words, the outer circumferential surfaces of the first core section (32a) and the second core section (32b) are connected to be substantially flush with each other. The outer circumferential surfaces of the first core section (32a) and the third core section (32c) are also connected to be substantially flush with each other. In this manner, when the rotor (31) is viewed along the rotation axis (O), the rotor core (32) has a constant cross-sectional shape in the axial directions.
Each of the second core section (32b) and the third core section (32c) is provided with a magnetic resistance structure (R). The magnetic resistance structure (R) has a lower magnetic permeability than the first core section (32a). The second core section (32b) and the third core section (32c) are in the same shape. Since the magnetic resistance structures (R) in the second core section (32b) and the third core section (32c) are the same, only the magnetic resistance structure (R) of the second core section (32b) will be described below and the description of the magnetic resistance structure (R) of the third core section (32c) will be omitted.
As shown in
Specifically, the magnetic pole section(S) in each permanent magnet (33) of the rotor (31) according to this embodiment includes areas facing in the circumferential directions of the permanent magnet (33) as viewed in the axial directions and an area around the areas (including the permanent magnet (33)) (i.e., the area surrounded by the broken line in
As shown in
The voids (R) according to this embodiment are through holes that penetrate the second core section (32b) and the third core section (32c) from the upper and lower ends. That is, the lower end of each void (R) of the second core section (32b) is flush with the upper end of the first core section (32a). The upper end of the void (R) of the third core section (32c) is flush with the lower end of the first core section (32a).
The second core section (32b) of the rotor core (32) is at least partially located above the upper end of the stator core (22) and has a magnetic resistance structure (R) with a lower magnetic permeability than the first core section (32a). The magnetic resistance structure (R) is formed in a magnetic pole section(S) of the rotor (31) and radially outside the permanent magnet (33).
Here, as shown in
As shown in
In this manner, the magnetic flux of the second core section (32b) is guided to the stator core (22) via the first core section (32a). Accordingly, the magnetic flux of the part of the second core section (32b) not opposed to the stator core (22) is concentrated on the first core section (32a). This can result in less decrease in the magnetic force between the rotor (31) and the stator (21) and less deterioration in the performance of the rotating electric machine (20).
The center of the rotor core (32) in the axial directions shifts upward from the center of the stator core (22) in the axial directions. In other words, the magnetic center of the rotor core (32) shifts upward, that is, in the first direction, from the magnetic center of the stator core (22).
With this configuration, the magnetic center of the rotor core (32) shifts from the magnetic center of the stator core (22) toward the second core section (32b). This can apply a downward pull force on the rotor (31). Accordingly, the thrust force acting on the lower bearing to cause less vertical vibration of the drive shaft (40), which can result in less anomalous sound.
The upper end of the first core section (32a) shifts upward from the upper end of the stator core (22). The lower end of the first core section (32a) shifts upward from the lower end of the stator core (22).
This causes a pull force biasing both the ends of the rotor (31) in the axial directions downward, and can thus reliably apply a thrust force to the lower bearing.
The motor (20) further includes: the third core section (32c) having the magnetic resistance structure (R), being adjacent to the lower end of the first core section (32a) and having a substantially constant cross sectional shape perpendicular to the axial directions of the rotation axis (O).
This provides the magnetic resistance structure (R) at each end of the rotor (31) in the axial directions and can thus increase the downward stack thickness of the rotor (31) in addition to the upward stack thickness. Accordingly, the surface areas of the permanent magnets (33) increase, which can provide a strong magnetic force and reduce an increase in the size of the motor.
The upper end of the first core section (32a) shifts upward from the upper end of the stator core (22). The lower end of the first core section (32a) shifts upward from the lower end of the stator core (22). A part of the third core section (32c) is disposed below the lower end of the stator core (22).
With this configuration, a downward pull force acts on the upper and lower parts of the rotor (31), which can improve the force for reducing the vertical vibration of the drive shaft. In this manner, in addition to the advantages of the fourth feature, the anomalous sound can be reliably reduced.
The magnetic resistance structure (R) is a void (R) in the rotor core (32). The magnetic resistance structure (R) can be easily provided by simply opening the void (R) in the rotor core (32). In this embodiment, the void (R) is provided in an area radially outside a line connecting the radially outer ends of the second magnetic part (33b) and the third magnetic part (33c). The void (R) extends along the outer circumferential surfaces of the second core section (32b) and the third core section (32c).
When the rotor (31) is viewed along the rotation axis (O), the rotor core (32) has an outer circumferential end with a constant cross-sectional shape perpendicular to the axial directions. The outer circumferential surface of the rotor core (32) can be formed smoothly. This can reduce the flow resistance of the refrigerant flowing through the space (i.e., the air gap) between the stator core (22) and the rotor core (32).
The permanent magnets (33) are ferrite magnets. The ferrite magnets have a relatively weak magnetic force, which may be strengthened by increasing the stack thickness of the rotor (31). The stack thickness of the rotor (31) then causes an increase in the size of the motor (20). However, with the magnetic resistance structure (R) provided, the magnetic force can be strengthened without relatively increasing the stack thickness of the rotor (31), which can reduce an increase in the size of the motor (20).
The permanent magnets (33) are arranged in the circumferential directions of the rotor core (32) and penetrate the rotor core (32) in the axial directions. Each of the permanent magnets (33) has a constant cross-sectional shape orthogonal to the axial directions. This can provide the permanent magnets (33) easily in the rotor without a need to shorten or lengthen some of the permanent magnets (33) in accordance with the shape of the rotor core (32).
The above-described embodiments may be modified as follows.
As shown in
The second core section (32b) and the third core section (32c) are not necessarily in the same shape. Specifically, the second core section (32b) may be longer or shorter than the third core section (32c) in the axial directions. The magnetic resistance structures (R) in the second core section (32b) and the third core section (32c) are not necessarily the same or in the same shape.
As shown in
As shown in
Each magnetic resistance structure (R) may be provided in an area of the rotor core (32) that blocks the flow of the magnetic flux directed radially outward from the associated permanent magnet (33). For example, the magnetic resistance structure (R) may be provided in an area between a first magnetic pole (corresponding to the second magnetic part (33b) according to the embodiment described above) of each permanent magnet and a second magnetic pole (corresponding to the third magnetic part (33c) according to the embodiment described above) of the permanent magnet (33), or in an area radially outside the area. The second magnetic pole has the same polarity as the first magnetic pole and is adjacent to the first magnetic pole in the circumferential directions of the rotor core (32).
The magnetic resistance structure (R) may be provided in an area between radially outer ends of permanent magnets (corresponding to the second magnetic part (33b) and the third magnetic part (33c) of the above embodiment) adjacent to each other in the circumferential directions of the rotor core (32) with the magnetic pole center line interposed therebetween, or in an area radially outside the area, when the rotor (31) is viewed in the axial directions.
Each permanent magnet (33) may be divided into a plurality of parts. For example, each permanent magnet (33) according to the embodiment described above may be divided into a first magnetic part (33a), a second magnetic part (33b), and a third magnetic part (33c). In an assembly of such permanent magnets (33), the magnetic resistance structure (R) may be provided in an area between the permanent magnets (33) arranged at both ends in the circumferential directions out of the assembly of the permanent magnets (33) arranged in the magnetic pole section(S) of the rotor (31) or in an area radially outside the area, when the rotor (31) is viewed in the axial directions.
The magnetic resistance structure (R) may be formed orthogonally to the flow of the magnetic flux directed radially outside the first core section (32a).
The magnetic resistance structures (R) of the second core section (32b) and the third core section (32c) may be in different shapes. For example, when the magnetic resistance structures (R) has a void (R) structure, the shapes of the voids (R) in the axial directions may be different between the second core section (32b) and the third core section (32c).
The motor (20) only needs to include the second core section (32b) and not necessarily include the third core section (32c).
With an increase in the distance between the magnetic center of the rotor core (32) and the magnetic center of the stator core (22), the rotor core (32) can obtain a stronger pull force. The rotor core (32) and the stator core (22) may thus be arranged with their magnetic centers being relatively distant from each other.
While the embodiments and variations thereof have been described above, it will be understood that various changes in form and details may be made without departing from the spirit and scope of the claims. The embodiments and the variations thereof may be combined and replaced with each other without deteriorating intended functions of the present disclosure. The expressions of “first,” “second,” . . . described above are used to distinguish the terms to which these expressions are given, and do not limit the number and order of the terms.
As described above, the present disclosure is useful for a rotating electric machine, a compressor, and a refrigeration apparatus.
Number | Date | Country | Kind |
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2022-152625 | Sep 2022 | JP | national |
This is a continuation of International Application No. PCT/JP2023/031599 filed on Aug. 30, 2023, which claims priority under 35 U.S.C. § 119 (a) to Patent Application No. 2022-152625, filed in Japan on Sep. 26, 2022, all of which are hereby expressly incorporated by reference into the present application.
Number | Date | Country | |
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Parent | PCT/JP2023/031599 | Aug 2023 | WO |
Child | 19090041 | US |