JP4491260B2 - Rotor for bearingless motor and bearingless motor - Google Patents

Description

  The present invention relates to a rotor for a bearingless motor and a bearingless motor.

  In recent years, bearingless motors have been researched and developed in order to solve various problems caused by mechanical bearings and problems still remaining in magnetic bearings used to solve these problems. A bearingless motor is an electromagnetic device that intentionally unbalances the magnetic flux in the gap to generate torque and support force, and integrates the motor and magnetic bearings. It is a response.

  Various types of bearing-less motors have been proposed. Permanent magnet type is small and light by using rare earth magnets with strong magnetomotive force. ・ Compact and lightweight ・ High power factor, high efficiency ・ Excitation current It has the feature that it can generate supporting force without using it.

  Bearingless motors such as surface-mounted, embedded, Inset, disc, and consequent pole types have already been developed, and there are some examples that have been put to practical use in disc-type and small liquid pumps.

  Among the above bearingless motors, embedded bearingless motors can be used for variable speed operation over a wide speed range and reluctance torque by embedding a permanent magnet in the rotor core and providing magnetic flux weakening control with saliency. Occurring and high efficiency operation becomes possible. Further, since it is an embedded type, there is no need for a cover for preventing the magnets from scattering during high-speed rotation, so that the gap length (gap between the stator and the rotor) can be reduced. For this reason, there is a feature that the ratio of supporting force to current can be increased (for example, see Patent Document 1). FIG. 9 shows an example of a salient pole embedded rotor. The rotor 100 includes salient poles 106 for obtaining reluctance torque, and the thickness of the magnet 102 is reduced in order to increase the supporting force when no load is applied. Further, in order to avoid irreversible demagnetization in the magnet 102, the magnet 102 is divided not into one magnet but as an aggregate of small magnets 102. Furthermore, the provision of the bridge 104 between the magnets 102 generates a leakage magnetic flux and increases the demagnetization strength.

However, the rotor 100 of the embedded magnet structure bearingless motor already proposed by the inventors in the above-mentioned patent document uses a thin magnet 102 to increase the supporting force at the time of no load or light load. The reluctance torque, which is a feature of the embedded bearingless motor, cannot be effectively used because the ratio is small and the field magnetic flux becomes weak due to the leakage magnetic flux from the bridge 104, making it difficult to increase the torque. Performance did not increase. That is, the features of the embedded magnet structure synchronous motor such as “variable speed operation in a wide speed range” and “high efficiency operation is possible by generating reluctance torque” are not utilized.
JP 2002-272028 A

  In view of the above-described facts, an object of the present invention is to provide a bearingless motor rotor and a bearingless motor that are inexpensive and capable of efficient variable speed operation in a wide speed range.

The bearingless motor rotor according to claim 1, wherein a plurality of salient poles formed at a predetermined interval in a circumferential direction of the rotor core and each of the rotor cores between the salient poles are the rotor. In a rotor for a bearingless motor having a plurality of insertion portions formed with the substantially circumferential direction of the iron core as a longitudinal direction and a plurality of magnetic poles each inserted into each of the insertion portions, each of the magnetic poles has a rectangular parallelepiped shape. A pair of laminated parts configured by laminating a plurality of permanent magnet pieces in such a manner that the magnetization direction faces the direction intersecting the longitudinal direction of the insertion part, and the pair of laminated parts are connected and the magnetization direction is A plurality of rectangular parallelepiped permanent magnet pieces arranged in the same direction as the magnetization direction of each laminated portion, and the arrangement of the permanent magnet pieces of the magnetic poles is a plan view of the rotor At least radially outside As the surface is recessed radially inward, wherein the connecting portion is formed thinner in the radial direction from the laminate.

In the invention with the above configuration, by making the thickness of the magnetic pole center portion thinner than the end portion and making the end portion thicker, a supporting force for supporting the shaft of the bearingless motor is secured, and an irreversible reduction occurring at the magnetic pole end portion Magnetism can be prevented.

In addition, each magnetic pole is configured by stacking and arranging rectangular parallelepiped small permanent magnet pieces so that the magnetization direction is the same direction, so that it is possible to reduce costs without using expensive special-shaped magnets. Irreversible demagnetization can be prevented by stacking the stacked portions that are both ends in the direction so as to have a thickness in a substantially radial direction.

The rotor for a bearingless motor according to claim 2 , wherein the arrangement of the permanent magnet pieces of the magnetic poles is such that the radially outer surface is recessed radially inward and the radially inner surface is recessed radially outward in plan view of the rotor. As described above, the connecting portion and the laminated portion are substantially H-shaped .

In the invention having the above-described configuration, the supporting force for supporting the shaft of the bearingless motor is ensured and the salient poles of the rotor can be enlarged, so that the reluctance torque can be increased.

The rotor for a bearingless motor according to claim 3 is a rectangular parallelepiped that is arranged on the outer surface of each of the stacked portions with a magnetization direction orthogonal to the stacked direction so that the magnetic flux density of the stacked portions is increased. The permanent magnet piece is further included.

In the present aspect, to increase the magnetomotive force by adding the permanent magnet pieces on each outer side of the laminate, it is possible to increase the magnetic flux density of the laminate.

The bearingless motor according to claim 4, wherein a stator including a winding for generating a magnetic flux for generating torque and a winding for generating a magnetic flux for supporting the rotor is disposed rotatably in the stator. And a bearingless motor rotor according to claim 1 or 2 .

  In the invention with the above configuration, it is possible to provide a bearingless motor that is inexpensive and capable of efficient variable speed operation in a wide speed range.

  As described above, according to the present invention, a rotor for a bearingless motor and a bearingless motor capable of efficient variable speed operation at a low cost and in a wide speed range can be obtained.

  FIG. 1 shows a bearingless motor rotor according to a first embodiment of the present invention.

  The rotor 10 has a substantially disk shape with a magnet 12 and salient poles 14, and the rotor 10 itself is formed by laminating thin plates 10 a having a shape as shown in FIG. 2 in the motor axis direction (white arrow direction). It has a structure. Moreover, it is good also as a structure which improves the torque further by laminating | stacking the some rotor 10 in a motor axial direction. At this time, in order to prevent ripples, the rotor 10 and the adjacent rotor 10b may be offset (skewed) in the rotation direction as shown in FIG.

  A magnet 12 is inserted into the rotor 10 in the direction of the black arrow to form a magnetic pole of the rotor 10. As will be described later, the magnet 12 has a substantially H-shaped cross section. A pair of laminated portions having a thickness in the radial direction is provided in the circumferential direction, and a thin connecting portion is connected to the pair of laminated portions. The magnet 12 is configured. An additional portion is provided on the outer side in the circumferential direction of the laminated portion and on the side not in contact with the connecting portion, thereby increasing the magnetomotive force of the entire magnet.

  FIG. 2 shows a dimension example of a thin plate constituting the bearingless motor rotor according to the first embodiment of the present invention. (Unit: mm) The numerical value is merely an example, and the present embodiment is not limited to this numerical value.

  FIG. 3 shows the structure of the magnet of the bearingless motor rotor according to the first embodiment of the present invention.

  The magnet 12 includes a laminated portion 12a at both ends in the circumferential direction, and connecting portions 12b that connect the two 12a, and an additional portion 12c that is provided on the outer side in the circumferential direction of the 12a. The black arrow in the figure represents the magnetization direction from the S pole to the N pole.

  As shown in FIG. 3, the magnet 12 has a rectangular parallelepiped magnet piece 16 formed therein to form a laminated portion 12a, a connecting portion 12b, and an additional portion 12c. The laminated portion 12a, which is both ends in the circumferential direction, is substantially in the radial direction. The irreversible demagnetization is prevented by being laminated so as to have a thickness. Further, the connecting portion 12b increases the supporting force for supporting the shaft of the bearingless motor by reducing the thickness of the magnet having a low magnetic permeability in the substantially radial direction. Further, by dividing the magnet 12 into small magnet pieces 16 in this way, generation of eddy currents that reduce the efficiency of the motor can be suppressed.

  Further, by embedding the connecting portion 12b in a portion deeper than the surface of the rotor 10, the distance d in FIG. 3 can be increased and the generated reluctance torque can be further increased. A magnetomotive force can be increased by disposing a magnet magnetized in the direction orthogonal to the laminated portion 12a in the additional portion 12c.

FIG. 4 shows a rotor for a bearingless motor as a reference example .

  The rotor 11 has a substantially disk shape with magnetic poles 13 and salient poles 15. The magnetic pole 13 is a substantially arc-shaped magnet that follows the outer peripheral shape of the rotor 11, and has a shape that increases the thickness of both ends in the circumferential direction.

The rotor 11 shown in FIG. 4 is not leakage flux occurs since the bridge 104 as compared with the salient pole with embedded rotor 100 of FIG. 9 uses a magnet integrally formed absence, the integrally molded Since it is necessary to use a magnet and the magnet 13 is embedded along the outer peripheral surface of the rotor 11, an improvement in reluctance torque cannot be expected .

  FIG. 5 shows the relationship of torque / current phase angle for each salient pole width of the bearingless motor rotor according to the first embodiment of the present invention.

  As a result of analyzing the relationship between the current phase angle and the torque when changing the salient pole width of the rotor 10 according to the first embodiment of the present invention using the finite element method, the salient pole width 33 is shown in FIG. It has been clarified that the maximum torque can be obtained when the current phase angle β is around −20 ° to −30 °. Here, the current phase angle β is 0 in the q-axis direction, and a minus sign means that the d-axis current is negative, that is, the magnetic flux is weakened.

  FIG. 6 shows the torque / current phase angle relationship of the bearingless motor rotor according to the first embodiment of the present invention.

    The salient pole width of the rotor 10 according to the first embodiment of the present invention was set to 33 °, and the relationship between the current phase angle β and the torque was analyzed. As a result, as shown in FIG. 6, the salient pole width 33 ° and the current phase angle β It became clear that the maximum torque was obtained near -25 °. However, since the present embodiment is a four-pole motor, the optimum salient pole width naturally varies depending on the number of poles.

  FIG. 7 shows a torque comparison between the bearingless motor rotor according to the first embodiment of the present invention and the conventional example shown in FIG.

  FIG. 7 shows a comparison of torque when the q-axis current imq is changed at the support current isd = 8 A. It can be seen that a larger torque is obtained in the present embodiment than in the conventional type. This is thought to be because the leakage flux is eliminated and the field flux is increased by not providing the rotor 10 with the conventional bridge 104.

  In the configuration of this embodiment, since the salient pole ratio is increased, reluctance torque is generated in addition to the magnet torque, and as a whole, the maximum is approximately 1.72 times that of a bearingless motor using a conventional salient pole embedded rotor. Torque is obtained.

  FIG. 8 shows a comparison in bearing force between the bearingless motor rotor according to the first embodiment of the present invention and the conventional example shown in FIG.

  FIG. 8 shows a comparison of the supporting force when the q-axis current imq is changed. Compared with the conventional type, this embodiment has a q-axis current imq <7A and a larger supporting force than the conventional type. I understand. The rated current of the motor is 7.8A.

  In the region of q-axis current imq> 7A, increasing the magnet thickness of the magnetic pole tip 12a causes the q-axis magnetic flux to concentrate on the stator yoke part and some of the teeth of the stator, resulting in magnetic saturation and reducing the supporting force. ing. However, the usefulness of the present embodiment is clear from the fact that the rated current is 7.8 A and the reduction in the supporting force is about 12% compared to the peak even at the q-axis current imq = 10 A.

  As described above, according to the present invention, a rotor for a bearingless motor and a bearingless motor capable of efficient variable speed operation at a low cost and in a wide speed range can be obtained. In addition, although the said Example is a 4-pole motor, it cannot be overemphasized that this invention is applicable to the motor etc. from which pole number differs besides the said Example.

FIG. 1 is a perspective view illustrating an appearance of a rotor according to the first embodiment. FIG. 2 is a plan view showing the structure of the rotor according to the first embodiment. FIG. 3 is a plan view showing the structure of the rotor according to the first embodiment. FIG. 4 is a plan view showing the structure of the rotor of the reference example . FIG. 5 is a diagram illustrating a relationship between the salient pole width and torque of the rotor according to the first embodiment. FIG. 6 is a diagram illustrating the relationship between the current phase angle and torque of the rotor according to the first embodiment. FIG. 7 is a diagram illustrating a torque relationship between the rotor according to the first embodiment and a conventional example. FIG. 8 is a diagram illustrating the relationship of the supporting force between the rotor according to the first embodiment and the conventional example. FIG. 9 is a plan view showing the structure of a conventional rotor.

10 rotor 12 magnet 14 salient pole 16 magnet piece

Claims (4)

A plurality of salient poles formed at predetermined intervals in the circumferential direction of the rotor core;
A plurality of insertion portions formed between the salient poles of the rotor core, each having a substantially circumferential direction of the rotor core as a longitudinal direction;
In the bearingless motor rotor provided with a plurality of magnetic poles each inserted into each insertion portion,
Each of the magnetic poles includes a pair of stacked portions formed by stacking a plurality of rectangular parallelepiped permanent magnet pieces so that the magnetization direction is in a direction crossing the longitudinal direction of the insertion portion, and the pair of stacked portions. And a connecting portion composed of a plurality of rectangular parallelepiped permanent magnet pieces arranged so that the magnetization direction is the same as the magnetization direction of each of the laminated portions .
The arrangement of the permanent magnet pieces of the magnetic pole is characterized in that the connecting portion is formed to be thinner in the radial direction than the laminated portion so that at least the radially outer surface is recessed radially inward in a plan view of the rotor. Bearingless motor rotor. In the arrangement of the permanent magnet pieces of the magnetic pole, the connecting portion and the laminated portion are substantially H so that the radially outer surface is recessed radially inward and the radially inner surface is recessed radially outward in plan view of the rotor. The rotor for a bearingless motor according to claim 1, wherein the rotor has a letter shape. The rectangular magnet-like permanent magnet pieces are further arranged on the outer surface of each of the stacked portions so that the magnetization direction is perpendicular to the stacked direction so that the magnetic flux density of the stacked portions is increased. The rotor for bearingless motors according to claim 1 or 2 . A stator having a winding for generating a magnetic flux for generating torque and a winding for generating a magnetic flux for supporting the rotor;
The rotor for a bearingless motor according to any one of claims 1 to 3, which is rotatably disposed in the stator.
A bearingless motor characterized by comprising:

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