JP2006153117A - Magnetic bearing - Google Patents

Abstract

<P>PROBLEM TO BE SOLVED: To provide a magnetic bearing having excellent controllability and capable of being miniaturized and reducing its weight. <P>SOLUTION: A stator 1 has a plurality of main poles 3 and a plurality of auxiliary poles 4 adjacent to one of the main poles 3 in the peripheral direction and forming a permanent magnet 16 for supplying bias magnetic flux to a tip part. An axial exciting coil 15 for controlling a position in the axial direction of a rotor 2 by increasing intensity of bias magnetic flux at a position in the axial direction and reducing its intensity at another position is formed in each main pole 3. Exciting current flowing in the axial exciting coil 15 is controlled based on outputs detected by a plurality of magnetic flux sensors 17 formed at tips of the plurality of auxiliary poles 4. <P>COPYRIGHT: (C)2006,JPO&NCIPI

Description

  The present invention relates to a magnetic bearing that supports a rotor in a non-contact state by a magnetic force, and more particularly to a magnetic bearing that can control the rotor in an axial direction (axial direction).

  Since the magnetic bearing can support the rotating body in a non-contact manner, it has been used for various bearings with the development of control technology. Recently, there has been a demand for magnetic bearings for micro rotating bodies. However, since the magnetic bearing using an electromagnet requires a large current to float the rotor, the power consumption increases. Further, in order to increase the magnetic force with a small current, it is required that the gap between the rotor and the stator is small, and high machining accuracy is required.

As a promising method for solving these problems, in recent years, a hybrid type magnetic bearing using a bias magnetic flux of a permanent magnet whose performance has been remarkably improved has been used. This hybrid type magnetic bearing is proposed by patent documents 1-3, for example.
JP 2003-21140 (paragraphs 0053 to 0056, FIG. 6) Japanese Patent Laid-Open No. 2001-41138 (paragraphs 0011 to 0014, FIG. 1) Japanese Patent Laid-Open No. 2001-101234 (paragraph 0009, FIG. 1)

However, in the magnetic bearing disclosed in the above-mentioned patent document, it is necessary to rely on passive stability for the stability in the axial direction (axial direction). For this reason, when an axial load is applied to the rotor, the magnetic bearing is inclined and rotated. There is a problem that control becomes difficult due to vibration or vibration.
The present invention has been made in view of such problems, and an object of the present invention is to provide a magnetic bearing that is excellent in axial controllability and can be reduced in size and weight.

  The magnetic bearing according to the present invention is a magnetic bearing having a stator and a rotor that is supported by the stator in a non-contact state by a magnetic force and rotates about a rotation axis. The stator has a predetermined gap in the rotor. A plurality of main poles that are opposed to each other and have a magnetic flux concentrating portion in which a magnetic flux including an axial component is concentrated, and are arranged at predetermined intervals in the circumferential direction of the stator, and a tip of the rotor via a predetermined gap And a plurality of complementary poles arranged at positions shifted in the circumferential direction with respect to the plurality of main poles, and a magnetic flux concentration of the main poles adjacent to each other with a tip portion of the complementary pole as a first polarity A permanent magnet for supplying a bias magnetic flux with the second polarity as a portion, and a strength of the bias magnetic flux provided on the plurality of main poles on one side in the axial direction and on the other side An axial excitation coil for generating an axial control magnetic flux for controlling the axial position of the rotor, a plurality of magnetic flux sensors provided at the tips of the plurality of auxiliary poles, and the axial based on detection signals of the plurality of magnetic flux sensors And a control unit for controlling the excitation current flowing in the excitation coil.

  ADVANTAGE OF THE INVENTION According to this invention, it becomes possible to provide the magnetic bearing which is excellent in controllability of an axial direction, and can be reduced in size and weight.

  First, a magnetic bearing according to a first embodiment of the present invention will be described with reference to FIG. FIG. 1A is a plan view of the magnetic bearing as viewed from the axial direction, and FIG. 1B is a cross-sectional view taken along line A-A ′ in FIG. The magnetic bearing has an annular stator 1 disposed outside and a rotor 2 disposed inside the stator 1.

  The stator 1 is composed of a yoke 11. The yoke 11 is made of a magnetic material such as a laminated steel plate, and has an annular portion 12, two main salient pole portions 13, and two auxiliary salient pole portions 14. On the other hand, the rotor 2 has a magnetic material such as a laminated steel plate or electromagnetic material disposed on at least an outer peripheral surface thereof, and is disposed inside the stator 1 so as to be rotatable about a rotating shaft 2a.

  The two main salient pole portions 13 protrude from the inside of the annular portion 12 toward the center, and have a magnetic concentration portion facing the outer peripheral surface of the rotor 2 via a predetermined gap, and 180 ° in the circumferential direction. Are arranged at intervals. Further, as shown in FIG. 1B, the main salient pole portion 13 includes an axial excitation coil 15 wound around an axis parallel to the axial direction (Z-axis direction) of the rotor 2. The main salient pole portion 13 and the axial excitation coil 15 form two main poles 3 (3 (1), 3 (2)). The axial excitation coil 15 is for performing axial position control of the rotor 2 by changing the magnitude and direction of the excitation current based on the detection output of the magnetic flux sensor 17 described later.

  Further, the supplementary salient pole part 14 is formed at a position shifted by 90 ° in the circumferential direction from the main salient pole part 13, and a permanent magnet 16 is attached to the tip thereof. The complementary salient pole portion 14 and the permanent magnet 16 form two complementary poles 4 (4 (1) to 4 (2)). The permanent magnet 16 is for providing a bias magnetic flux φb to the main pole 3. The permanent magnet 16 is mounted with the first polarity (for example, the S pole) set to the tip side toward the rotor 2. When the south pole is on the tip side, the bias magnetic flux φb reaches from the bottom of the auxiliary salient pole part 14 to the adjacent main salient pole part 13 via the annular part 12 and then returns to the auxiliary salient pole part 14 via the rotor 2. Formed in the path. Thereby, the magnetic flux concentration part which is the front-end | tip of the main pole 3 turns into N pole.

  Further, magnetic flux sensors 17A (i) and 17B (i) for detecting magnetic flux are attached to the tip of each auxiliary pole 4 (i), that is, the tip of the permanent magnet 16 (i = 1, 2). The magnetic flux sensor 17 is, for example, a Hall element. The magnetic flux sensors 17A (i) and 17B (i) attached to one permanent magnet 16 are attached at different positions in the axial direction (Z direction) as shown in FIG. 1 (b). Here, it is assumed that the magnetic flux sensor 17A (i) is present above the Z direction with respect to 17B (i).

As shown in FIG. 1B, at least the outer peripheral surface side of the rotor 2 is formed in a disc shape, and the axial width of the outer peripheral surface is set to be at least smaller than the axial width of the main salient pole portion 13. ing. Therefore, in the gap portion between the main pole 3 and the rotor 2, the bias magnetic flux φb is a magnetic flux φba that goes from the upper side of the main pole 3 to the lower side, and a magnetic flux φbb that goes from the lower side of the main pole 3 to the upper side. Become.
When no excitation current flows through the axial excitation coil 15, the axial components of the magnetic fluxes φba and φbb are equal and cancel each other, so that no magnetic flux of the axial component is generated and the rotor 2 also has an axial direction. No power is applied.

  When an exciting current flows through the axial exciting coil 15 in the direction shown in FIG. 1B, for example, the axial control magnetic flux φca is formed in the direction shown by the arrow in FIG. The axial control magnetic flux φca acts to strengthen the magnetic flux φbb while weakening the magnetic flux φba. Thereby, a downward force (Z-axis negative direction) force F is applied to the rotor 2 as shown in FIG. 1B, and the rotor 2 moves downward. When the exciting current of the axial exciting coil 15 flows in the direction opposite to that shown in FIG. 1B, the force F also becomes downward as opposed to FIG. In this way, by controlling the magnitude and direction of the excitation current of the axial excitation coil 15, the axial position of the rotor 2 can be controlled. The excitation current is controlled by the control circuit 102 based on the detection output of the magnetic flux sensor 17. For example, the difference between the sum of the upper magnetic flux sensors 17A (1) and 17A (2) and the sum of the lower magnetic flux sensors 17B (1) and 17B (2) is calculated by the comparator 101, and based on this calculation output The control circuit 102 can control the excitation current.

FIG. 2 shows a three-pole magnetic bearing according to the second embodiment of the present invention. The same components as those in FIG. 1 are denoted by the same reference numerals, and detailed description thereof is omitted. This magnetic bearing makes it possible to perform tilt control (tilt control) of the rotor 2 and control in the radial direction (radial direction) of the stator 1 in addition to position control of the rotor 2 in the axial direction. That is, the main poles 3 are formed at intervals of 120 ° in the circumferential direction of the stator 1, and the auxiliary poles 4 are formed at positions shifted by 60 ° from the main poles 3 at intervals of 120 ° in the circumferential direction. The main pole 3 is provided with a radial excitation coil 18 wound around the radial direction as an axis. The radial excitation coil 18 is for generating a radial excitation magnetic flux φr for strengthening or weakening the magnetic pole at the tip (magnetic flux concentrating portion) of the main pole 3 formed by the bias magnetic flux φb. The position of the rotor 2 in the radial direction is controlled by controlling the magnetic pole of the main pole 3 based on the change in the radial excitation magnetic flux φr.
In this embodiment, the excitation currents flowing through the three axial excitation coils 120 provided on the three main poles 3 are made different from each other, so that not only the axial position control of the rotor 2 but also the inclination (X axis The tilt angle θx in the direction and the tilt angle θy in the Y-axis direction can also be controlled.

The excitation current of the radial excitation coil 18 is controlled based on the detection output of the magnetic flux sensor 17 in the same manner as the axial excitation coil 15.
A configuration of a control system including a control circuit for performing this control is shown in FIG. This control system includes an axial control system 100 and a radial control system 200.
The axial control system 100 includes a comparator 101A-C, a coordinate conversion circuit 103, a control circuit 102 ′, a coordinate conversion circuit 104, and a power amplifier 105A-C. The comparators 101A-C calculate the difference between the detection outputs of the magnetic flux sensors 17A (i) and 17B (i) installed on the complementary pole 4 (i), respectively.
The coordinate conversion circuit 103 obtains an axial displacement (Z) and a tilt angle (θx, θy) with reference to the XY coordinates shown in FIG. 3 based on the detection output detected by the magnetic flux sensor 17, and a z-direction displacement signal. , Θx direction displacement signal and θy direction displacement signal are output to the control circuit 102 ′. The control circuit 102 ′ outputs, for example, a PID control signal based on these displacement signals. The coordinate conversion circuit 104 converts the PID control signal into a three-phase coordinate system signal corresponding to the position of the axial excitation coil 15, amplifies the signal by the power amplifier 105 </ b> A-C, and applies it to the axial excitation coil 15. . When the tilt angles θx and θy are detected, the tilt angle of the rotor 2 can be controlled by making the magnitudes of the excitation currents flowing through the three axial excitation coils 15 different from each other.

The radial control system 200 includes an adder 201A-C, a coordinate conversion circuit 202, a control circuit 203, and a power amplifier 204A-C.
Each of the comparators 201A-C outputs the sum of the detection outputs of the two magnetic flux sensors 17A (i) and 17B (i) installed on one complementary pole 4 (i). The coordinate conversion circuit 202 obtains an X-direction displacement (x) and a Y-direction displacement (y) based on the XY coordinates shown in FIG. 3 based on the detection output detected by the magnetic flux sensor 17, and obtains an X-direction displacement signal, A Y direction displacement signal is output to the control circuit 203.
Based on these displacement signals, the control circuit 203 generates a PID control signal in accordance with a three-phase coordinate system corresponding to the position of the radial excitation coil 18, and amplifies the PID control signal with the power amplifier 204A-C to generate the radial excitation coil. 18 is applied.

FIG. 4 shows the configuration of a four-pole magnetic bearing according to the third embodiment of the present invention.
In the magnetic bearing, four main poles 3 (i) are formed at intervals of 0 °, 90 °, 180 °, and 170 ° in the circumferential direction in the XY coordinate system shown in FIG. Four complementary poles (i) are formed at intervals of 45 °, 135 °, 225 °, 315 ° and 90 ° at positions shifted from the main pole 3 (i) by 45 ° in the circumferential direction. Others are the same as in the above embodiment.

FIG. 5 shows the configuration of a control system including a control circuit for performing the control of the embodiment of FIG. The axial control system 100 includes a comparator 101A′-C ′, a control circuit 102A′-C ′, and an operational amplifier 106A-C.
The comparator 101A ′ includes the sum of the detection outputs of the magnetic flux sensors 17A (i) (i = 1 to 4) installed in the respective complementary electrodes 4 (i) and the magnetic flux sensors 17B (i) (i = 1 to 4). The difference between the sums of the detection outputs is calculated. This difference is output to the control circuit 102A ′ as a Z direction displacement signal of the rotor 2.
Further, the comparator 101B ′ includes the sum of the detection outputs of the upper magnetic flux sensors 17A (1) and 17A (4) of the complementary poles 4 (1) and 4 (4) and the lower magnetic flux sensors 17B (1) and 17B. The difference with the sum of (4) is calculated. This difference is output to the control circuit 102B ′ as a displacement signal of the rotor 2 in the θx direction.
Further, the comparator 101C ′ includes the sum of the detection outputs of the upper magnetic flux sensors 17A (1) and 17A (2) of the complementary poles 4 (1) and 4 (2) and the lower magnetic flux sensors 17B (1) and 17B. The difference from the sum of (2) is calculated. This difference is output to the control circuit 102C ′ as a displacement signal of the rotor 2 in the θy direction.

  Based on these displacement signals, the control circuits 102 </ b> A ′ to C ′ generate a PID control signal according to a three-phase coordinate system corresponding to the position of the radial excitation coil 18. The operational amplifiers 106A-D control the excitation current of each axial excitation coil 15 based on this PID control signal.

  FIG. 6 shows a three-pole magnetic bearing according to the fourth embodiment of the present invention. This embodiment differs from the above embodiment in that the permanent magnet 16 'is formed over the entire outer peripheral surface of the rotor 2 instead of forming the permanent magnet 16 at the tip of each auxiliary pole 4. . The radial control system 200 is almost the same as in the second embodiment. However, since the positions of the main pole 3 and the complementary pole 4 with respect to the XY coordinate system are different, the conversion formula in the coordinate conversion circuit 202 is different from that in the second embodiment.

Further, the axial control system 100 includes comparators 101A ″ to C ″, control circuits 102A ″ to C ″, and operational amplifiers 106A ′ to C ′.
The comparator 101A ″ includes the sum of the detection outputs of the magnetic flux sensors 17A (i) (i = 1 to 3) installed in the respective complementary electrodes 4 (i) and the magnetic flux sensors 17B (i) (i = 1 to 3). This is to calculate a difference from the sum of the detection outputs. This difference is output to the control circuit 102A ″ as a Z direction displacement signal of the rotor 2.
Further, the comparator 101B ″ detects the tilt angle θx of the rotor 2 in the X-axis direction, so that the sum of the magnetic flux sensors 17A (1), 17B (2) and 17B (3) and the magnetic flux sensors 17A (2), 17A The difference between the sum of (3) and 17B (1) is calculated, and this difference is output to the control circuit 102B ′ as a displacement signal in the θx direction of the rotor 2.

  Further, the comparator 101C ′ detects the tilt angle θy of the rotor 2 in the Y-axis direction, and the sum of the magnetic flux sensors 17A (1), 17B (1), 17B (2) and 17A (3), and the magnetic flux sensor 17A. The difference between the sum of (2) and 17B (3) is calculated. This difference is output to the control circuit 102C ′ as a displacement signal of the rotor 2 in the θy direction.

Based on these displacement signals, the control circuits 102A ″ to C ″ generate PID control signals according to a three-phase coordinate system corresponding to the position of the radial excitation coil 18. The operational amplifiers 106A ′ to C ′ control the excitation current of each axial excitation coil 15 based on the PID control signal.
The configuration of the radial control system 200 and the axial control system 100 shown in FIG. 6 can be replaced with the configuration shown in FIG.

  FIG. 7 shows a first modification of the second embodiment. This example is different from the second embodiment in that the permanent magnet 16 ″ is formed not only at the auxiliary pole 4 but also at the tip of the main pole 3. Note that the axial control system 100 and radial are different. The configuration of the control system 200 is the same as the configuration of FIG. 6, but it goes without saying that it may be the same as the configuration of FIG.

  FIG. 8 shows a second modification of the second embodiment. This example is different from the second embodiment in that the permanent magnet 16 is embedded in the annular portion 12 of the stator in an annular shape. In addition to this annular permanent magnet, it is also possible to install a permanent magnet at the same position as in the above embodiment. Note that the configurations of the axial control system 100 and the radial control system 200 may be any of the configurations shown in FIGS. 3 and 6.

  Although the embodiments of the invention have been described above, the present invention is not limited to these embodiments, and various modifications, additions, substitutions, and the like can be made without departing from the spirit of the invention.

It is the top view and sectional view of a magnetic bearing concerning a 1st embodiment of the present invention. It is a top view and a sectional view of a 3 pole type magnetic bearing concerning a 2nd embodiment of the present invention. The structure of the control system containing the control circuit for controlling the magnetic bearing of 2nd Embodiment is shown. It is the top view and sectional view of a 4 pole type magnetic bearing concerning a 3rd embodiment of the present invention. The structure of the control system containing the control circuit for controlling the magnetic bearing of 3rd Embodiment is shown. It is the top view and sectional drawing of a 3 pole type magnetic bearing which concern on the 4th Embodiment of this invention. The 1st modification of 2nd Embodiment is shown. The 2nd modification of 2nd Embodiment is shown.

Explanation of symbols

  DESCRIPTION OF SYMBOLS 1 ... Stator, 2 ... Rotor, 3 ... Main pole, 4 ... Supplementary pole, 111 ... Relay, 12 ... Annular part, 13 ... Main salient pole part, 14 ... complementary salient poles, 15 ... axial excitation coil, 16 ... permanent magnet, 17 ... magnetic flux sensor, 18 ... radial excitation coil.

Claims (7)

In a magnetic bearing having a stator and a rotor that is supported by the stator in a non-contact state by a magnetic force and rotates about a rotation axis,
The stator has a plurality of main poles that are opposed to the rotor via a predetermined gap and have a magnetic flux concentrating portion in which a magnetic flux including an axial component is concentrated, and are arranged at predetermined intervals in the circumferential direction of the stator, and A plurality of complementary poles disposed at positions that are opposed to the rotor via a predetermined gap at the tip and are displaced in the circumferential direction with respect to the plurality of main poles;
A permanent magnet for supplying a bias magnetic flux so that the tip of the auxiliary pole has a first polarity and the magnetic flux concentrating portion of the adjacent main pole has a second polarity;
An axial excitation coil that is provided in the plurality of main poles and generates an axial control magnetic flux that controls the position of the rotor in the axial direction by increasing the intensity of the bias magnetic flux on one side in the axial direction and weakening it on the other side. When,
A plurality of magnetic flux sensors provided at tips of the plurality of complementary poles;
A magnetic bearing comprising: a control unit that controls an excitation current flowing through the axial excitation coil based on detection signals of the plurality of magnetic flux sensors.   The magnetic bearing according to claim 1, wherein the stator is formed thicker than the rotor.   The magnetic bearing according to claim 1, wherein a plurality of the magnetic flux sensors are provided at different positions in the axial direction in each of the plurality of auxiliary poles.   The magnetic bearing according to claim 3, wherein the control unit controls an excitation current of the axial excitation coil based on a difference in detection output of the magnetic flux sensor provided in one of the plurality of auxiliary poles.   The magnetic bearing according to claim 1, wherein the permanent magnet is provided at a tip of the auxiliary pole.   The magnetic bearing according to claim 1, wherein the permanent magnet is provided on an outer peripheral surface of the rotor.   The magnetic bearing according to claim 1, wherein the permanent magnet is provided in an annular portion of the stator.

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