ELECTRIC MOTOR HAVING SPLIT CORE STATOR
20200313473 ยท 2020-10-01
Assignee
Inventors
Cpc classification
H02K1/18
ELECTRICITY
H02K19/103
ELECTRICITY
International classification
H02K1/18
ELECTRICITY
Abstract
An electric motor includes a rotor; a first stator provided with a plurality of teeth, and a second stator stacked in an axial direction of the first stator, the teeth of the second rotor being disposed and aligned with the corresponding plurality of teeth of the first stator in the axial direction. The first and the second stator are formed of a plurality of split cores being split along a plurality of split surfaces. A position of each of the split surfaces of the second stator is displaced from a position of the corresponding one of the split surfaces of the first stator in the circumferential direction by an angle (=(2/N)/2+n(2/N), where N is a least common multiple of the number of magnetic poles of the rotor and the number of split cores, and n is an integer).
Claims
1. An electric motor comprising: a rotor having a plurality of magnetic poles; a first stator provided with a plurality of teeth for winding a coil on its inner circumferential side, the first stator being disposed in an annular shape radially facing the rotor, the first stator being formed of a plurality of split cores each having teeth identical in number, the split cores being split along a plurality of split surfaces in a circumferential direction; and a second stator stacked in an axial direction of the first stator, the second stator provided with a plurality of teeth identical in number with the teeth of the first stator, the teeth being disposed and aligned with the corresponding teeth of the first stator in the axial direction, the second stator being formed of a plurality of split cores being split along a plurality of split surfaces in the circumferential direction, wherein a position of each of the split surfaces of the second stator is displaced from a position of the corresponding one of the split surfaces of the first stator in the circumferential direction by an angle , and the angle being determined by an equation,
=(2/N)/2+n(2/N), where N is a least common multiple of the number of magnetic poles of the rotor and the number of split cores, and n is an integer.
2. The electric motor of claim 1, wherein one split core being freely selected of the plurality of split cores of the second stator has a shape acquired by inverting a split core of the plurality of split cores of the first stator across an inversion symmetry axis, the split core disposed to at least partly overlap the one split core, the inversion symmetry axis passes through a predetermined tooth included in the split core of the first stator and a center of the first stator or passes through a predetermined slot and the center of the first stator, an interior angle of the split core of the first stator is designated as , an angle formed by the inversion symmetry axis and a split surface of the split core of the first stator is represented by /2/2, and an angle formed by the inversion symmetry axis and a split surface of the one split core of the second stator is represented by /2+/2.
3. The electric motor of claim 1, wherein at least one split surface of the plurality of split surfaces of the first stator and at least one split surface of the plurality of split surfaces of the second stator are each disposed in a region between adjacent teeth of the plurality of teeth.
4. The electric motor of claim 1, wherein the first stator has a length in the axial direction equal to a length of the second stator in the axial direction.
Description
BRIEF DESCRIPTION OF THE DRAWINGS
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DETAILED DESCRIPTION
[0020] Hereinafter, an electric motor according to the present disclosure is described with reference to the drawings. However, the technical scope of the invention is not limited to these embodiments and includes the invention described in the scope of claims and elements equivalent thereto.
[0021]
[0022] The rotor 1 has a plurality of magnetic poles. For example, the rotor 1 has 42 magnetic poles. However, the present disclosure is not limited to these examples.
[0023] The first stator 2 includes a plurality of teeth (211, 212, . . . , 216, 221, 222, . . . , 226, . . . , 261, . . . , 266) on its inner circumferential side for winding a coil (not illustrated). In the example illustrated in
[0024] The first stator 2 includes a plurality of split cores (21, 22, . . . , 26) disposed in an annular shape facing radially the rotor 1, each having teeth identical in number (e.g., six), the split cores being split along a plurality of split surfaces (21a, 22a, . . . , 26a) in a circumferential direction. In the example illustrated in
[0025] The split cores are preferably manufactured by stacking a plurality of electromagnetic steel plates. Here, when the plurality of split cores has the same shape, each split core can be manufactured by stacking electromagnetic steel plates having a single shape.
[0026] The second stator 3 is layered on the first stator 2 in its axial direction. The second stator 3 includes a plurality of teeth identical in number with the plurality of teeth of the first stator 2, being disposed and aligned with the corresponding plurality of teeth of the first stator 2. In other words, as illustrated in
[0027] The first stator 2 preferably has a length in the axial direction equal to a length of the second stator 3 in the axial direction.
[0028] When the electromagnetic steel plate constituting the first stator 2 has a thickness equal to a thickness of the electromagnetic steel plate constituting the second stator 3, the first stator 2 preferably has stacked electromagnetic steel plates identical in number or substantially identical in number with stacked electromagnetic steel plates of the second stator 3.
[0029] While
[0030] When a minimum unit of each of the first stator 2 and the second stator 3 is considered as one electromagnetic steel plate, even the first stator 2 and the second stator 3 being each formed by layering the same or substantially same number of electromagnetic steel plates can be applied to the electric motor according to the present example. In addition, the first stator 2 and the second stator 3 may be layered one by one.
[0031] The second stator 3 includes a plurality of split cores (31, 32, . . . , 36) split along a plurality of split surfaces (31a, 32a, . . . , 36a) in the circumferential direction.
[0032] The split surfaces (31a, 32a, . . . , 36a) of the second stator are positioned displaced from the corresponding split surfaces (21a, 22a, . . . , 26a) of the first stator by an angle in the circumferential direction, and the angle is determined by the following equation;
=(2/N)/2+n(2/N),
[0033] where N is a least common multiple of the number of magnetic poles of the rotor and the number of split cores, and n is an integer.
[0034] In this case, when the number of magnetic poles of the rotor is set to 42 and the number of split cores is set to 6, a least common multiple of the numbers is 42. Thus, the value of is determined as /42, 3/42, 5/42, . . . (rad).
[0035] As described below, the split core 21 and the Split core 31 each have a shape inverted across an inversion symmetry axis 21c. Other split cores of the first stator 2 and the second stator 3 also have shapes inverted across respective inversion symmetry axes 22c to 26c.
[0036] Next, a relationship between positions of the split surfaces and torque pulsation will be described. First, torque pulsation caused by the first stator 2 provided alone will be described.
[0037] When the first stator 2 has the split surfaces at the same positions in the axial direction as those of the corresponding split surfaces of the second stator 3, torque pulsation are caused in the split surfaces of the second stator 3 at the same positions as those of the corresponding split surfaces of the first stator 2. In other words, this case causes torque pulsation to be twice as large as the torque pulsation illustrated in
[0038] In contrast, the electric motor according to the present example is configured such that the split surfaces of the second stator 3 are disposed at positions displaced from positions of the corresponding split surfaces of the first stator 2 to suppress torque pulsation.
[0039] As illustrated in
[0040] The torque pulsation is caused when the magnetic poles of the rotor 1 pass through the split surfaces. Thus, when the split surfaces of the second stator 3 are provided at respective positions different from positions of the corresponding split surfaces of the first stator, the period of the torque pulsation caused in the first stator 2 can be deviated from the period of the torque pulsation caused in the second stator 3. Total torque pulsation acquired by synthesizing the torque pulsation caused in the first stator 2 and the torque pulsation caused in the second stator 3 becomes minimum when the torque pulsation caused in the first stator 2 and the torque pulsation caused in the second stator 3 deviate by a half-period. The torque pulsation has a period of 2/N, such that the half-period is (2/N)/2. Thus, the split surfaces of the second stator 3 are provided at respective positions displaced from positions of the corresponding split surfaces of the first stator by the half-period, i.e., (2/N)/2.
[0041] While the above description relates to the case where the position of each of the split surfaces of the second stator 3 is displaced by the half-period from the position of the corresponding one of the split surfaces of the first stator, the torque pulsation can be suppressed due to further displacement by n periods (n is an integer). Accordingly, when the position of the split surface (e.g., 31a) of the second stator 3 is displaced from the position of the split surface (e.g., 21a) of the first stator 2 by the angle in the circumferential direction, torque pulsation can be suppressed by setting the angle as in the following equation (1).
=(2/N)/2+n(2/N)(1)
[0042] where N is a least common multiple of the number of magnetic poles of the rotor and the number of split cores, and n is an integer.
[0043] As described above, when the positions of the split surfaces of the second stator 3 are each displaced by the angle with respect to the position of the corresponding one of the split surfaces of the first stator, the torque pulsation is approximately flat on the whole as illustrated in
[0044] In addition, as illustrated in
[0045] When a center line between the center lines 210 and 260 designated as 21c, an angle from the center line 21c to the split surface 21a is /2+/2, and an angle from the center line 21c to the split surface 31a is /2/2. Similarly, an angle from the center line 21c to the split surface 26a is /2/2, and an angle from the center line 21c to the split surface 36a is /2+/2. From the above, it can be seen that the split core 21 and the split core 31 are disposed at respective positions inverted across the center line 21c serving as an inversion symmetry axis.
[0046]
[0047] As described above, one split core being freely selected (e.g., 31) of the plurality of split cores of the second stator 3 has a shape acquired by inverting a split core (e.g., 21) of the plurality of split cores of the first stator 2 across an inversion symmetry axis (e.g. 21c), the split core disposed to at least partly overlap with the one split core. In addition, when the inversion symmetry axis 21c passes through a predetermined tooth (e.g., 213) included in the split core 21 of the first stator 2 and the center O of the first stator 2 or passes through a predetermined slot and the center of the first stator 2, and an interior angle of the split core 21 of the first stator 2 is designated as , an angle formed by the inversion symmetry axis 21c and the split surface 26a of the split core 21 of the first stator 2 is represented by /2/2, and an angle formed by the inversion symmetry axis 21c and the split surface 36a of the one split core 31 of the second stator 3 is represented by /2+/2.
[0048] As described above, the angle that determines a position of a split surface can take a plurality of values. Thus, the split surface can be set to various positions on the circumference according to the set value of . However, at least one split surface of the plurality of split surfaces of the first stator 2 and at least one split surface of the plurality of split surfaces of the second stator 3 are each preferably disposed in a region between adjacent teeth of the plurality of teeth. This is because, when the split surface is disposed in a portion formed with a tooth, the cross-sectional area of the split surface increases compared to when the split surface is formed in a portion formed with no tooth, and torque pulsation caused by the split surface increases.
[0049] Next, a method of disposing the split cores of the first stator 2 and the split cores of the second stator 3 will be described.
[0050]
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[0052] As illustrated in
[0053] Next, an electromagnetic device according to Example 2 of the present disclosure will be described.
[0054] Since the torque pulsation is caused at the same period in each of the first stator and the second stator, the torque pulsation can be suppressed by providing a phase difference a. The required phase difference a is determined by the following equation.
=(2/12)/2+n(2/12)=/12,3/12,5/12, . . . (rad) (n=0,1,2 . . . )
[0055] A suitable value is selected from values of calculated as described above. The first stator and the second stator are inverted and stacked, so that the first stator and the second stator may be displaced from respective split surfaces to have inversion symmetry by /2.
[0056] As described above, in the electric motor according to the example of the present disclosure, a stator capable of suppressing torque pulsation caused by split surfaces can be easily manufactured.