WO2009139278A1 - 磁気誘導子型回転機およびそれを用いた流体移送装置 - Google Patents
磁気誘導子型回転機およびそれを用いた流体移送装置 Download PDFInfo
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- WO2009139278A1 WO2009139278A1 PCT/JP2009/057972 JP2009057972W WO2009139278A1 WO 2009139278 A1 WO2009139278 A1 WO 2009139278A1 JP 2009057972 W JP2009057972 W JP 2009057972W WO 2009139278 A1 WO2009139278 A1 WO 2009139278A1
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K19/00—Synchronous motors or generators
- H02K19/02—Synchronous motors
- H02K19/10—Synchronous motors for multi-phase current
- H02K19/103—Motors having windings on the stator and a variable reluctance soft-iron rotor without windings
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K1/00—Details of the magnetic circuit
- H02K1/06—Details of the magnetic circuit characterised by the shape, form or construction
- H02K1/12—Stationary parts of the magnetic circuit
- H02K1/14—Stator cores with salient poles
- H02K1/145—Stator cores with salient poles having an annular coil, e.g. of the claw-pole type
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K16/00—Machines with more than one rotor or stator
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K16/00—Machines with more than one rotor or stator
- H02K16/02—Machines with one stator and two or more rotors
-
- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K2201/00—Specific aspects not provided for in the other groups of this subclass relating to the magnetic circuits
- H02K2201/12—Transversal flux machines
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- H—ELECTRICITY
- H02—GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
- H02K—DYNAMO-ELECTRIC MACHINES
- H02K29/00—Motors or generators having non-mechanical commutating devices, e.g. discharge tubes or semiconductor devices
- H02K29/03—Motors or generators having non-mechanical commutating devices, e.g. discharge tubes or semiconductor devices with a magnetic circuit specially adapted for avoiding torque ripples or self-starting problems
Definitions
- the present invention relates to a magnetic inductor type rotating machine suitable for being driven in a high-speed rotation region in which iron loss components are dominant among motor losses, and a fluid transfer device using the same.
- a magnet as a field means is mounted on a rotor.
- a motor used in a so-called electric assist turbo in which a motor is arranged between a turbine and a compressor of an automobile supercharger, requires ultra-high speed rotation exceeding 100,000 rotations / minute, and in a high temperature environment. Therefore, when a conventional permanent magnet type synchronous rotating machine is used for the motor, problems such as magnet holding strength and thermal demagnetization occur.
- one phase and one coil are wound across a plurality of slots, and the coils and coil ends of each phase intersect with each other in the circumferential direction.
- the distributed winding method for example, Patent Document 1
- one-phase one-coil is wound around the teeth without straddling the slot, and the coils and coil ends of each phase do not have overlapping overlapping in the circumferential direction.
- rotor field methods include a coil (for example, Patent Document 2) and a permanent magnet (for example, Patent Document 1).
- the combination of the stator coil winding method and the rotor field method is free in principle.
- the rotating shaft of the rotor is pivotally supported by bearings arranged on both sides of the rotor in the axial direction, so that the rotating shaft constitutes a resonance system and bends and vibrates.
- This axial resonance is more likely to occur as the distance between the bearings is longer and the rotational speed of the rotor is higher. In the worst case, the rotor comes into contact with the stator.
- the bearing is desired to have a large diameter from the viewpoint of securing rigidity and securing an oil cooling channel. Therefore, when the bearing is disposed on the inner diameter side of the coil end of the stator coil, a problem of interference between the bearing and the coil end of the stator coil occurs. Therefore, in order to avoid interference between the bearing and the coil end of the stator coil and reduce the distance between the bearings, it is effective to shorten the axial length of the coil end of the stator coil as much as possible.
- JP 2004-8880 A Japanese Patent Application Laid-Open No. 08-214519
- the magnetic flux generated by the field source enters the salient pole on one axial side of the rotor from the teeth on one axial side of the stator, and enters the rotor. Flows radially inward, flows through the rotating shaft to the other axial side, and then flows radially outward through the rotor, from the salient poles on the other axial side of the rotor to the other axial side of the stator.
- a magnetic circuit is formed that enters the teeth, flows radially outward in the stator, and flows axially in the outer frame of the stator.
- the magnetic path coupling state between the salient poles of the rotor and the teeth of the stator changes as the rotor rotates, and the amount of axial magnetic flux flowing inside the rotating machine increases or decreases.
- in-plane eddy current loss occurs in the laminated iron core, and eddy current loss also occurs in massive magnetic bodies such as the outer frame and the rotating shaft. Since this eddy current loss increases in proportion to the square of the frequency, this eddy current loss is a serious problem when driving at a high frequency such that the fundamental frequency exceeds 1 kHz in a conventional magnetic inductor type rotating machine. Become.
- the number of slots is smaller than that of the distributed winding type, and the slot pitch is designed to be large. Therefore, since the circumferential width of the slot opening of the stator is formed larger than the circumferential width of the salient pole of the rotor, the salient pole of the rotor faces the stator teeth as the rotor rotates. It shifts from the state which is facing the teeth of the stator through the state where it is not opposed to the teeth of the stator at all.
- the width of change in the magnetic path coupling state between the salient poles of the rotor and the teeth of the stator is large, and the width of increase / decrease in the amount of axial magnetic flux flowing inside the rotating machine is also large. As a result, eddy current loss increases and motor efficiency decreases.
- This problem of fluctuation of the amount of magnetic flux in the axial direction is peculiar to a magnetic inductor type rotating machine equipped with a concentrated winding type stator coil.
- the iron loss due to the fluctuation of the axial magnetic flux amount does not reach a problem level. That is, in the distributed winding type, the opening width of the slot is narrow due to the structure, and the salient poles of the rotor are always opposed to the plurality of slots of the stator. Therefore, the salient poles of the rotor rotate while exchanging a part of the opposing teeth, and the magnetic resistance between the rotor and the stator is always kept small.
- the present applicant has found a phenomenon that the iron loss becomes larger than expected by operating a magnetic inductor type rotating machine equipped with a concentrated winding type stator coil, and carefully examined the cause of the iron loss.
- the present invention has been invented based on the knowledge that fluctuations in the amount of magnetic flux in the axial direction cause iron loss.
- the present invention has been made to solve such a problem, and even when driven at an ultra-high speed rotation, the eddy current loss is small and a highly efficient magnetic inductor type rotating machine and a fluid using the same The purpose is to obtain a transfer device.
- teeth that define a slot that opens to the inner peripheral side project radially inward from the inner peripheral surface of the cylindrical core back, and a plurality of teeth are arranged in the circumferential direction.
- the first stator core and the second stator core that are formed to have the same shape are arranged so as to be separated from each other by a predetermined distance in the axial direction and coaxially with the circumferential positions of the teeth aligned.
- a stator having a stator core and a stator coil wound around the stator core in a concentrated manner, and a first shape made of salient poles arranged at an equiangular pitch in the circumferential direction.
- the rotor core and the second rotor core are respectively positioned on the inner peripheral side of the first stator core and the second stator core, and are offset from each other by a semi-salient pole pitch in the circumferential direction, and are coaxially fixed to the rotation shaft. And a rotor that is provided. Further, the present magnetic inductor type rotating machine is disposed on the stator and generates a field magnetic flux so that the salient pole of the first rotor core and the salient pole of the second rotor core have different polarities.
- Field generating means an axial magnetic path forming member extending in the axial direction so as to connect the core back outer peripheral surface of the first stator core and the core back outer peripheral surface of the second stator core; It is equipped with.
- the salient pole width ⁇ r of the salient poles of the first rotor core and the second rotor core is configured to be larger than the opening width ⁇ s of the slot of the stator.
- the salient pole width ⁇ r of the salient poles of the first rotor core and the second rotor core is configured to be larger than the opening width ⁇ s of the slot of the stator. Rotates with the teeth facing the stator teeth. Therefore, the magnetic resistance between the rotor and the stator can be kept small, and the fluctuation of the magnetic flux amount is limited to the minimum. Thereby, the fluctuation
- FIG. 1 is a partially broken perspective view showing a configuration of a rotating machine according to Embodiment 1 of the present invention
- FIG. 2 is a perspective view showing a configuration of a rotor applied to the rotating machine according to Embodiment 1 of the present invention. It is.
- a rotating machine 1 is a magnetic inductor type synchronous rotating machine, and includes a rotor 3 coaxially fixed to a rotating shaft 2 made of a block-like magnetic body such as iron, and a rotor 3.
- a stator 7 formed by winding a stator coil 11 as a torque generating drive coil around a stator core 8 disposed so as to surround; a field coil 12 as field means; a rotor 3; And a housing 13 that houses the stator 7 and the field coil 12.
- the rotor 3 is produced by laminating and integrating a predetermined number of magnetic steel plates and the first and second rotor cores 4 and 5 produced by laminating and integrating a large number of magnetic steel plates formed in a predetermined shape, for example. And a disk-shaped partition wall 6 in which an insertion hole (not shown) is formed at the axial center position.
- the first and second rotor cores 4 and 5 are formed in the same shape, and cylindrical base portions 4a and 5a each having a rotation shaft insertion hole (not shown) drilled at an axial center position, and the base portions 4a and 5a.
- the projecting poles 4b and 5b are provided so as to project radially outward from the outer circumferential surface of the steel plate and extend in the axial direction, and are provided at two equiangular pitches in the circumferential direction.
- the first and second rotor cores 4, 5 are arranged in semicircular salient pitches in the circumferential direction, are arranged in close contact with each other via the partition wall 6, and are rotational shafts inserted through the rotational shaft insertion holes. 2 to be fixed.
- the rotor 3 is rotatably disposed in the housing 13 with both ends of the rotating shaft 2 supported by bearings (not shown).
- the stator core 8 includes first and second stator cores 9 and 10 that are produced by laminating and integrating a large number of magnetic steel plates formed in a predetermined shape.
- the first stator core 9 includes a cylindrical core back 9a, and teeth 9b that are provided radially inwardly from the inner peripheral surface of the core back 9a and are provided with six equiangular pitches in the circumferential direction. Prepare.
- a slot 9c that opens to the inner peripheral side is defined by a core back 9a and an adjacent tooth 9b.
- the second stator core 10 is manufactured in the same shape as the first stator core 9, and has a cylindrical core back 10 a and is projected radially inward from the inner peripheral surface of the core back 10 a, and the like in the circumferential direction.
- a slot 10c that opens to the inner peripheral side is defined by a core back 10a and an adjacent tooth 10b.
- the first and second stator cores 9 and 10 are arranged so that the circumferential positions of the teeth 9b and 10b coincide with each other, and the first and second rotor cores 4 and 5 are separated between the axial thickness separation of the partition walls 6, respectively. Is disposed in the housing 13 so as to surround the housing.
- the stator coil 11 is a three-phase coil wound in a so-called concentrated winding method in which conductor wires are wound around teeth 9b and 10b that are paired in the axial direction without straddling the slots 9c and 10c.
- the stator coil 11 is configured by sequentially winding three phases of U, V, and W twice in a concentrated manner on six pairs of teeth 9b and 10b facing in the axial direction.
- the coil end of the phase coil of each phase does not have the mutually cross
- the field coil 12 is a cylindrical coil in which a conductor wire is wound in a cylindrical shape, and is interposed between the core backs 9 a and 10 a of the first and second stator cores 9 and 10.
- the housing 13 is made of a massive magnetic material such as iron and is disposed so as to be in close contact with the outer peripheral surface of the core back 9a of the first stator core 9 and the outer peripheral surface of the core back of the second stator core 10.
- a directional magnetic path forming member is configured.
- FIG. 3 is a partially broken perspective view for explaining the flow of magnetic flux in the rotating machine according to the first embodiment of the present invention.
- the field coil 12 When the field coil 12 is energized, it enters the salient pole 4b of the first rotor core 4 from the teeth 9b of the first stator core 9 as indicated by arrows in FIG. , Then a part of the magnetic flux flows axially in the base 4a and the partition wall 6, and the remaining part of the magnetic flux flows axially in the rotary shaft 2.
- the magnetic flux enters the second rotor core 5 and flows radially outward in the second rotor core 5 from the salient poles 5b of the second rotor core 5 to the teeth 10b of the second stator core 10. Then, a magnetic flux is formed that flows radially outward in the second stator core 10, flows axially in the housing 13, and returns to the first stator core 9.
- the rotating machine 1 has a 6-slot concentrated winding stator coil 11 for a 4-pole rotor 3 composed of 2-pole N-pole and 2-pole S-pole arranged in the axial direction. Operates as a magnetic inductor type synchronous rotating machine.
- FIG. 4 is a front view for explaining the operation of the rotating machine according to Embodiment 1 of the present invention
- FIG. 5 is a front view for explaining the operation of the rotating machine as a comparative example.
- the slot opening width ⁇ s of the stator is expressed as an angle (center angle) formed by a line segment connecting the circumferential ends of the slot opening and the axis of the rotation axis on a plane orthogonal to the axis of the rotation axis. Is done.
- the salient pole width ⁇ r of the rotor is an angle (center angle) formed by a line segment connecting both ends in the circumferential direction of the outer peripheral surface of the salient pole and the axis of the rotation axis on a plane orthogonal to the axis of the rotation axis. It is represented by In the rotating machine 100 of the comparative example, the slot opening width ⁇ s of the stator 7 is formed larger than the salient pole width ⁇ r of the rotor 3A. In FIG. 5, for convenience of explanation, the same or corresponding parts as those in the rotating machine shown in FIG. In FIGS. 4 and 5, the magnitude relation of the magnetic flux amount is represented by the thickness of the arrow.
- the salient pole 4b faces the teeth 9b, so the magnetic resistance between the stator 7 and the rotor 3A is small. Therefore, the magnetic flux generated by the field coil 12 enters the first stator core 9 from the housing 13 and flows radially inward within the first stator core 9, and passes through the gap between the salient pole 4b and the teeth 9b. Through the salient pole 4b. Next, the magnetic flux flows radially inward in the first rotor core 4, a part of the magnetic flux flows axially in the base 4 a and the partition wall 6, and the remaining part of the magnetic flux flows in the rotary shaft 2 in the axial direction. .
- the magnetic flux enters the second rotor core 5 flows radially outward, enters the second stator core 10 from the salient poles 5 b, and enters the second stator core 10 in the radial direction. It flows outward, flows through the housing 13 in the axial direction, and returns to the first stator core 9. Thus, a magnetic path that circulates around the field coil 12 is formed.
- the amount of magnetic flux flowing in the radial direction in the first and second stator cores 9 and 10 and the first and second rotor cores 4 and 5 The amount of magnetic flux flowing in the axial direction in the rotary shaft 2 and the housing 13 is large.
- the first and second stator cores 9 and 10 and the magnetic flux components flowing in the radial direction in the first and second rotor cores 4 and 5, and the rotating shaft 2 and The magnetic flux component flowing in the axial direction in the housing 13 varies greatly.
- the first and second stator cores 9 and 10 are formed of a laminated body of magnetic steel plates, eddy currents due to fluctuations in magnetic flux components that flow in the radial direction through the first and second stator cores 9 and 10.
- the generation of iron is suppressed and does not become a big problem as iron loss.
- the fluctuation of the magnetic flux component flowing in the radial direction through the first and second rotor cores 4 and 5 does not cause a big problem as iron loss.
- the laminated body of magnetic steel plates generates eddy currents in the laminated surface due to increase / decrease (fluctuation) of the magnetic flux component flowing in the axial direction through the rotating shaft 2 and the housing 13, resulting in a large iron loss.
- instead of using a magnetic steel sheet laminate there is electrical conductivity even when using a compacted iron core that is compression-molded with resin-coated iron powder. Iron loss will occur.
- the salient pole width ⁇ r of the rotor 3 is formed larger than the slot opening width ⁇ s of the stator 7. Therefore, along with the rotation of the rotor 3, the salient pole 4b faces two adjacent teeth 9b shown in FIG. 4B from the state facing the teeth 9b shown in FIG. After the state, the state shifts to a state facing the adjacent tooth 9b shown in FIG. Thus, even if the rotor 3 rotates, the salient pole 4b is always in a state of facing the teeth 9b, so that the magnetic resistance between the rotor 3 and the stator 7 can be kept small, Variations in the amount of magnetic flux are limited to a minimum.
- variation of the magnetic flux amount which flows into the axial direction used as the cause of an eddy current decreases, generation
- the heat generated in the rotor 3 is transmitted to the bearing via the rotating shaft 2, causing thermal deterioration of the lubricating oil and grease in the bearing and shortening the bearing life. And in the super-high-speed rotation operation driven at high frequency, the heat generation in the rotor 3 becomes remarkable.
- production of an eddy current is suppressed and the heat_generation
- FIGS. 6A and 6B are views for explaining the structure of the rotor with a salient pole width ⁇ r of 100 °.
- FIG. 6A is a front view thereof
- FIG. 6B is a development in which the rotor is developed in the circumferential direction.
- FIG. 7A and 7B are diagrams for explaining the structure of the rotor with the salient pole width ⁇ r of 60 °.
- FIG. 7A is a front view thereof
- FIG. 7B is a development in which the rotor is developed in the circumferential direction. It is a top view.
- the partition 6 is abbreviate
- 6 has a salient pole number Nr of 2 and a salient pole width ⁇ r of 100 °. 6A and 6B, as indicated by the overlapping portion ⁇ , a part of the salient pole 4b (N pole) of the first rotor core 4 and the salient pole 5b (S pole) of the second rotor core 5 are used. ) Partly overlaps in the axial direction.
- this overlapping portion ⁇ is integrated in the axial direction, it does not act as an effective magnetic pole and generates an ineffective axial component leakage magnetic flux 40 that does not contribute to torque.
- This leakage magnetic flux 40 not only contributes to torque but also reduces the output by reducing the effective magnetic flux contributing to torque by magnetically saturating each magnetic path of the rotating machine. Further, since the amount of the invalid leakage magnetic flux 40 varies depending on the position of the rotor 3B, it causes iron loss and becomes a problem.
- the magnetic resistance between the salient pole 4b and the tooth 9b increases, so that the amount of magnetic flux of the leakage magnetic flux 40 is small, And the component of the magnetic flux mainly has a circumferential direction component and a radial direction component. Therefore, when the rotor position changes in the leakage magnetic flux 40, the magnitude of the magnetic flux varies like a three-dimensional vector.
- the axial magnetic flux component fluctuates.
- the fluctuation of the leakage magnetic flux 40 occurs particularly in the vicinity of the air gap in the rotor and stator laminated parts, but the eddy current generated due to the increase / decrease in the axial magnetic flux component does not occur in the plane of the laminated iron core. Therefore, the effect of configuring the rotor and the stator as a laminated body cannot be obtained.
- the magnetic flux generated in the overlapping portion ⁇ is a part of the main magnetic flux, and therefore the amount of magnetic flux is large and fluctuates at a high frequency. As a result, the fluctuation of the axial magnetic flux component becomes a large iron loss.
- the rotor 3 shown in FIG. 7 has a salient pole number Nr of 2 and a salient pole width ⁇ r of 60 °.
- Nr salient pole number
- ⁇ r salient pole width
- FIGS. 7A and 7B in this rotor structure, the salient pole 4b (N pole) of the first rotor core 4 and the salient pole 5b (S pole) of the second rotor core 5
- the overlapping portion ⁇ in the axial direction is eliminated. Therefore, in this rotor 3, since the overlapping portion ⁇ in the axial direction between the salient pole 4b of the first rotor core 4 and the salient pole 5b of the second rotor core 5 is not formed, the leakage magnetic flux 40 described above is generated. It does not occur and iron loss can be reduced.
- the rotor when a magnetic inductor type rotating machine having a concentrated winding type stator coil is operated at an ultra-high speed, the rotor can be configured to satisfy 180 / Nr> ⁇ r> ⁇ s. desirable.
- the number of salient poles Nr of the rotor corresponds to half the number of poles (total number of salient poles) of the rotor. That is, the number of salient poles Nr of the rotor is the number of salient poles of the first rotor core 4 (second rotor core 5).
- Embodiment 1 described above a rotating machine is described in which the number of salient poles of the rotor is 2 (number of poles of the rotor is 4) and the number of slots of the stator is 6, but the number of salient poles of the rotor is described.
- the number of slots of the stator is not limited to this.
- a slot number that is a multiple of 3 can be selected.
- the greatest common divisor of the number of salient poles of the rotor and the number of slots of the stator is 1, the radial magnetic attractive force increases and vibration noise is generated.
- the number of salient poles of the rotor is equal to the number of slots of the stator, the three-phase motor is not established.
- the number of stator slots decreases, the number of stator coils decreases, and high mass productivity and cost reduction of the stator can be expected. From these facts, it is realistic to select the number of stator slots from 6, 9, and 12.
- 2 or 4, 3 or 6, 4 or 8 can be considered except 1 where it is obvious that a weight imbalance occurs.
- the housing 13 is made of a block magnetic material and used as an axial magnetic path forming member.
- the housing 13 is made of a block or circular arc shape made of a block magnetic material such as iron.
- a member may be constructed so as to connect the outer peripheral surfaces of the core backs 9a and 10a to constitute an axial magnetic path forming member.
- the housing need not be made of a magnetic material, but may be made of a metal such as stainless steel or a resin.
- FIG. FIG. 8 is a partially broken perspective view showing a rotating machine according to Embodiment 2 of the present invention.
- the stator coil is omitted.
- the first stator core 9A has a cylindrical core back 9a, and teeth that are provided radially inward from the inner peripheral surface of the core back 9a and are provided at six equiangular pitches in the circumferential direction. 9b.
- the collar part 9d is extended in the both sides of the circumferential direction from the inner peripheral edge part of each teeth 9b, and is reducing the opening width of the slot 9c.
- the second stator core 10A is manufactured in the same shape as the first stator core 9A, and the flange portions 10d are extended from the inner peripheral ends of the teeth 10b to both sides in the circumferential direction to reduce the opening width of the slots 10c. is doing.
- Other configurations are the same as those in the first embodiment.
- the number of teeth Ns of the stator 7A is 6, the number of salient poles Nr of the rotor 3 is 2, and 180 / Nr, as in the rotating machine 1 of the first embodiment. > ⁇ r> ⁇ s is satisfied. Therefore, also in the second embodiment, the same effect as in the first embodiment can be obtained.
- the flange portions 9d and 10d are extended from the inner peripheral ends of the teeth 9b and 10b to both sides in the circumferential direction, even if the salient pole width ⁇ r cannot be increased, ⁇ r A stator that satisfies> ⁇ s can be easily designed.
- FIG. 9 is a partially broken perspective view showing a rotating machine according to Embodiment 3 of the present invention.
- the stator coil is omitted.
- a first permanent magnet 41 as a field means is interposed between the outer peripheral surface of the core back 9a of the first stator core 9A and the housing 13, and the magnetization direction 43 is radially inward. It is magnetized and oriented to face the direction.
- a second permanent magnet 42 as a field means is interposed between the outer peripheral surface of the core back 10a of the second stator core 10A and the housing 13 so that the magnetizing direction 43 is radially outward. It is magnetized and oriented so that it faces.
- Other configurations are the same as those in the second embodiment.
- the rotating machine 1B configured as described above uses the first and second permanent magnets 41 and 42 instead of the field coil 12, and operates in the same manner as the rotating machine 1 of the first embodiment. Therefore, also in the third embodiment, the same effect as in the first embodiment can be obtained.
- first and second permanent magnets 41, 42 sintered rare earth magnets such as neodymium / iron / boron magnets and samarium cobalt magnets having high magnetic flux density are used.
- rare earth magnets are used as the first and second permanent magnets 41 and 42, the magnet itself is also conductive, so that the rotation 3 is caused by a change in the relative position between the salient pole of the rotor 3 and the teeth of the stator 7A.
- the magnetic resistance between the child and the stator 7A fluctuates, that is, the operating points of the first and second permanent magnets 41 and 42 change, and the amount of magnetic flux passing through the magnet itself fluctuates. Eddy currents will be generated.
- the permanent magnet is disposed on the outer periphery of both core backs of the first and second stator cores.
- the permanent magnet is at least one of the first and second stator cores. What is necessary is just to arrange
- the pair of first and second stator cores are described as constituting the stator core.
- the stator core includes a plurality of pairs of first and second stators. The cores may be configured by coaxially arranging the cores in the axial direction so that the circumferential positions of the teeth coincide.
- the rotor also includes a plurality of pairs of the first and second rotor cores, the circumferential positions of the salient poles of the first rotor cores being matched, and the circumference of the salient poles of the second rotor cores.
- the directional positions are made coincident and arranged coaxially.
- FIG. 10 is a system configuration diagram having an automobile supercharger according to Embodiment 4 of the present invention.
- the present system includes a generator motor 25 driven by the rotational torque of the engine 21, and an electric assist turbo 30 as an automobile supercharger connected to the exhaust system of the engine 21.
- the generator motor 25 has a pulley 26 connected to a pulley 23 fixed to a crankshaft 22 of the engine 21 via a belt 24.
- the generator motor 25 converts the driving force of the engine 21 transmitted through the belt 24 into AC power.
- This AC power is converted into DC power by an inverter 27 that is integrally attached to the opposite side of the pulley 26 of the generator motor 25, charges the battery 29, and is supplied to an in-vehicle load (not shown).
- the electric assist turbo 30 is fixed to the turbine 31 disposed in the exhaust system 36 of the engine 21, the rotation shaft 32 of the turbine 31, and the compressor 33 disposed in the intake system 35 of the engine 21, and the rotation shaft 32. And an ultra-high speed rotating machine 34 attached coaxially.
- the ultra high speed rotating machine 34 has a power generation function and an electric function, and is electrically connected to the inverter 27 of the generator motor 25 via a large current wiring 28.
- the intake gas A is supplied to the engine 21 via the intake system 35 and burned inside the engine 21.
- the exhaust gas B after combustion is exhausted to the outside through the exhaust system 36.
- the turbine 31 is driven by the exhaust gas B flowing through the exhaust system 36.
- the compressor 33 fixed to the rotating shaft 32 of the turbine 31 is rotationally driven, and the intake gas A is supercharged to atmospheric pressure or higher.
- the exhaust gas B has fluid energy more than that required for the electric assist turbo 30.
- electric power can be supplied to the battery 29 and the vehicle-mounted load by operating the super high speed rotating machine 34 as a generator and operating the inverter 27 in the regeneration mode.
- the performance of the turbo can be dramatically improved by adding the super high speed rotating machine 34, but the conventional permanent magnet synchronous rotating machine is changed to the ultra high speed rotating machine 34.
- the problem of holding the magnet as the field means occurs.
- a conventional magnetic inductor type rotating machine having a distributed winding type stator coil is applied to an ultra-high speed rotating machine 34, the axial length of the coil end of the stator coil is reduced. And the distance between the bearings that support the rotating shaft is increased, which causes a problem of shaft resonance.
- the rotating machine 1 includes the concentrated winding type stator coil, the distance between the bearings can be shortened, the shaft rigidity can be increased, and the problem of shaft resonance during the ultra high speed rotation operation can be avoided. Further, since the rotating machine 1 can extremely reduce the fluctuation of the amount of magnetic flux in the axial direction, the iron loss is reduced and the heat generation of the rotating machine 1 itself can be suppressed. Therefore, by applying the rotating machine 1 to the ultra-high speed rotating machine 34, a high-performance and small electric assist turbo 30 that does not have a problem of axial resonance and does not require a large-scale cooling mechanism can be realized at low cost. can do.
- the rotating machine is described as being applied to an ultra-high-speed rotating machine for an electric assist turbo as a fluid transfer device.
- the rotating machine is not limited to an electric assist turbo
- the present invention can be applied to a fluid transfer device that operates at high speed, for example, a motor such as a vacuum cleaner or a jet towel (dryer) that rotates a centrifugal fan at high speed.
- the teeth of the stator cores are arranged at an equiangular pitch in the circumferential direction, and the arrangement pitch at the circumferential center of the slot opening is an equiangular pitch.
- the arrangement pitch at the center in the circumferential direction of the slot openings is not necessarily an equiangular pitch, and may be an unequal pitch.
- the arrangement pitch at the center in the circumferential direction of the slot openings can be made unequal.
- the array pitch at the center in the circumferential direction of the slot openings is made unequal. Can do.
- the opening widths of all the slots are formed to be equal, but the opening width of each slot is formed smaller than the salient pole width of the first and second rotor cores. If so, the opening widths of all slots need not be equal.
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Abstract
Description
図1はこの発明の実施の形態1に係る回転機の構成を示す一部破断斜視図、図2はこの発明の実施の形態1に係る回転機に適用される回転子の構成を示す斜視図である。
ハウジング13は、鉄などの塊状磁性体で作製され、第1固定子コア9のコアバック9aの外周面と第2固定子コア10のコアバック外周面とに密接するように配設され、軸方向磁路形成部材を構成している。
回転子3Aの回転に伴い、突極4bは、図5の(a)に示されるティース9bと対向する状態から、図5の(b)に示されるスロット9cの開口と対向する状態を経て、図5の(c)に示される隣のティース9bに対向する状態に移行する。
このように、比較例の回転機100においては、第1および第2固定子コア9,10および第1および第2回転子コア4,5内を径方向に流れる磁束成分、および回転軸2およびハウジング13内を軸方向に流れる磁束成分が大きく変動する。
しかし、磁性鋼板の積層体は、回転軸2およびハウジング13を軸方向に流れる磁束成分の増減(変動)によりその積層面内に渦電流を発生し、大きな鉄損となる。また、磁性鋼板の積層体に代えて、樹脂コーティングされた鉄粉を圧縮成型した圧粉鉄心を用いた場合でも、導電率があるので、磁束変動に起因して渦電流損やヒステリシス損などの鉄損が生じてしまう。
そこで、回転子3の回転に伴い、突極4bは、図4の(a)に示されるティース9bと対向する状態から、図4の(b)に示される隣り合う2つのティース9bと対向する状態を経て、図4の(c)に示される隣のティース9bに対向する状態に移行する。
このように、回転子3が回転しても、突極4bは常にティース9bと対向する状態となっているので、回転子3と固定子7との間の磁気抵抗を小さく保つことができ、磁束量の変動が最小限に制限される。
また、回転子3での発熱は、回転軸2を介して軸受に伝達され、軸受での潤滑油やグリースの熱劣化をもたらし、軸受寿命の短縮をもたらす。そして、高周波駆動される超高速回転運転では、回転子3での発熱が顕著となる。しかし、この実施の形態1によれば、渦電流の発生が抑制され、回転子3での発熱が少なくなる。
そこで、本回転機1を超高速回転が要求される電動アシストターボなどのモータに適用すれば、超高速回転における軸共振の問題もなく、かつ軸受の長寿命化が図られる。
重なり部δが第1固定子コア9のティース9bと対向する位置にくると、第1固定子コア9のティース9bから第1回転子コア4の突極4bおよび第2回転子コア5の突極5bを経て第2固定子コア10のティース10bに至る経路で軸方向の漏れ磁束40が流れる。この経路の磁気抵抗は小さいので、この漏れ磁束40の磁束量は大きく、しかもその磁束の成分は軸方向成分が主となる。そして、重なり部δが第1固定子コア9のスロット9cと対向する位置にくると、突極4bとティース9bとの間の磁気抵抗が大きくなるので、この漏れ磁束40の磁束量は小さく、かつその磁束の成分は周方向成分と径方向成分とが主となる。したがって、漏れ磁束40は回転子位置が変化すると、磁束量の大きさが3次元ベクトル的に変動する。
Ns=3×(N+1)
Nr=M×(N+1)
180/Nr>βr>θs
を満足するように、回転機を設計することが望ましい。但し、M=1,2、N=1,2,3である。
図8はこの発明の実施の形態2に係る回転機を示す一部破断斜視図である。なお、図8において、固定子コイルは省略されている。
図8において、第1固定子コア9Aは、円筒状のコアバック9aと、コアバック9aの内周面から径方向内方に突設されて周方向に等角ピッチで6つ設けられたティース9bと、を備える。そして、鍔部9dが各ティース9bの内周端部から周方向の両側に延設され、スロット9cの開口幅を縮小している。第2固定子コア10Aは、第1固定子コア9Aと同一形状に作製され、鍔部10dが各ティース10bの内周端部から周方向の両側に延設され、スロット10cの開口幅を縮小している。
なお、他の構成は上記実施の形態1と同様に構成されている。
従って、この実施の形態2においても、上記実施の形態1と同様の効果が得られる。
また、この実施の形態2では、鍔部9d、10dをティース9b,10bの内周端部から周方向の両側に延設しているので、突極幅βrを大きくできないような場合でも、βr>θsを満足する固定子の設計が容易となる。
図9はこの発明の実施の形態3に係る回転機を示す一部破断斜視図である。なお、図8において、固定子コイルは省略されている。
図9において、界磁手段としての第1永久磁石41が第1固定子コア9Aのコアバック9aの外周面とハウジング13との間に密接状態に介装され、着磁方向43が径方向内方に向くように着磁配向されている。また、界磁手段としての第2永久磁石42が第2固定子コア10Aのコアバック10aの外周面とハウジング13との間に密接状態に介装され、着磁方向43が径方向外方に向くように着磁配向されている。
なお、他の構成は上記実施の形態2と同様に構成されている。
従って、この実施の形態3においても、上記実施の形態1と同様の効果が得られる。
また、上記実施の形態1~3では、一対の第1および第2固定子コアにより固定子コアを構成するものとして説明しているが、固定子コアは複数対の第1および第2固定子コアをティースの周方向位置を一致させて軸方向に同軸に配列して構成してもよい。この場合、回転子も、複数対の第1および第2回転子コアを、第1回転子コア同士の突極の周方向位置を一致させて、かつ第2回転子コア同士の突極の周方向位置を一致させて同軸に配列して構成することになる。
図10はこの発明の実施の形態4に係る自動車用過給器を有するシステム構成図である。
図10において、本システムでは、エンジン21の回転トルクにより駆動される発電電動機25と、エンジン21の排気システムに接続された自動車用過給器としての電動アシストターボ30と、を備える。
発電電動機25は、プーリ26をエンジン21のクランクシャフト22に固着されたプーリ23にベルト24を介して連結されている。発電電動機25は、ベルト24を介して伝達されたエンジン21の駆動力を交流電力に変換する。この交流電力は、発電電動機25のプーリ26と反対側に一体に取り付けられたインバータ27により直流電力に変換され、バッテリ29を充電するとともに、車載負荷(図示せず)に供給される。
まず、通常状態では、吸気ガスAが、吸気系統35を介してエンジン21に供給され、エンジン21の内部で燃焼される。燃焼後の排気ガスBが、排気系統36を介して外部に排気される。タービン31は、排気系統36を流通する排気ガスBにより駆動される。これにより、タービン31の回転軸32に固着されたコンプレッサ33が回転駆動され、吸気ガスAが大気圧以上に過給される。
Claims (7)
- 内周側に開口するスロットを画成するティースが円筒状のコアバックの内周面から径方向内方に突設されて周方向に並べて複数配設されてなる同一形状に作製された第1固定子コアおよび第2固定子コアを、軸方向に所定距離離反して、かつ上記ティースの周方向位置を一致させて同軸に配置して構成された固定子コア、および上記固定子コアに集中巻きに巻装された固定子コイルを有する固定子と、
突極が周方向に等角ピッチで配設されてなる同一形状に作製された第1回転子コアおよび第2回転子コアを、それぞれ上記第1固定子コアおよび上記第2固定子コアの内周側に位置させ、かつ互いに周方向に半突極ピッチずらして回転軸に同軸に固着された回転子と、
上記固定子に配設され、上記第1回転子コアの突極と上記第2回転子コアの突極とが異なる極性となるように界磁磁束を発生する界磁手段と、
上記第1固定子コアのコアバック外周面と上記第2固定子コアのコアバック外周面とを連結するように軸方向に延設された軸方向磁路形成部材と、を備え、
上記第1回転子コアおよび上記第2回転子コアの突極の突極幅βrが、上記固定子の上記スロットの開口幅θsより大きく構成されていることを特徴とする磁気誘導子型回転機。 - 上記第1回転子コアおよび上記第2回転子コアの突極の突極幅βrが、(180/Nr)°(但し、Nrは上記第1回転子コアおよび上記第2回転子コアの各突極数である)より小さく構成されていることを特徴とする請求項1記載の磁気誘導子型回転機。
- 上記界磁手段は上記第1固定子コアおよび上記第2固定子コアの少なくとも一方のコアバックと上記軸方向磁路形成部材との間に配設された永久磁石であることを特徴とする請求項1又は請求項2記載の磁気誘導子型回転機。
- 上記界磁手段は上記第1固定子コアと上記第2固定子コアのコアバック間に介装された円筒状コイルであることを特徴とする請求項1又は請求項2記載の磁気誘導子型回転機。
- 上記第1固定子コア、上記第2固定子コア、上記第1回転子コア、および上記第2回転子コアが磁性鋼板を積層して作製され、上記回転軸、および上記軸方向磁路形成部材が塊状磁性体で作製されていることを特徴とする請求項1乃至請求項4のいずれか1項に記載の磁気誘導子型回転機。
- 上記第1固定子コアおよび上記第2固定子コアの各ティース数Nsが、Ns=3×(N+1)を満足し、上記第1回転子コアおよび上記第2回転子コアの各突極数Nrが、Nr=M×(N+1)を満足するように構成されている(但し、Mは1,2、Nは1,2,3である)ことを特徴とする請求項1乃至請求項5のいずれか1項に記載の磁気誘導子型回転機。
- 請求項1乃至請求項6のいずれか1項に記載の上記磁気誘導子型回転機をモータとして用いた流体移送装置。
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JP2011200081A (ja) * | 2010-03-23 | 2011-10-06 | Mitsubishi Electric Corp | 高速回転電動機およびそれに用いられる回転子 |
CN101951077A (zh) * | 2010-09-29 | 2011-01-19 | 沁阳市电业综合公司 | 一种电动装置 |
US20130234540A1 (en) * | 2010-12-01 | 2013-09-12 | Kabushiki Kaisha Kobe Seiko Sho (Kobe Steel, Ltd) | Dc brushless motor and method for controlling the same |
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JP2016537948A (ja) * | 2013-11-13 | 2016-12-01 | ブルックス オートメーション インコーポレイテッド | 密封スイッチトリラクタンスモータ |
KR20210148417A (ko) * | 2013-11-13 | 2021-12-07 | 브룩스 오토메이션 인코퍼레이티드 | 밀봉된 스위치드 릴럭턴스 모터 |
KR102591049B1 (ko) | 2013-11-13 | 2023-10-18 | 브룩스 오토메이션 인코퍼레이티드 | 밀봉된 스위치드 릴럭턴스 모터 |
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Also Published As
Publication number | Publication date |
---|---|
DE112009001165T5 (de) | 2012-01-12 |
JP5539191B2 (ja) | 2014-07-02 |
CN102027658A (zh) | 2011-04-20 |
US20110058967A1 (en) | 2011-03-10 |
JPWO2009139278A1 (ja) | 2011-09-15 |
US8749105B2 (en) | 2014-06-10 |
CN102027658B (zh) | 2014-11-12 |
DE112009001165A5 (de) | 2012-04-19 |
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