1. Field of the Invention
A three-gap motor has a “U” shaped rotor, with permanent magnets on the radial inner surfaces and axial surfaces, that rotate over coils positioned radially on a stator.
2. Description of Related Art
At present most commercial motors have radial gaps separating the rotor and stator. Those with permanent magnets have cylindrical rotors attached to a rotating shaft covered by stationary lamination stacks, with the rotor and stator separated by a radial gap. Arc shaped permanent magnets are mounted around the outer periphery of the rotor and face radially outward. Several pairs of magnets of alternating polarity are disposed around the rotor producing rotating magnetic fields within the radial air gap. Stator windings are placed in slots within the stationary lamination stack and loop from one slot to another. Conductor segments within the slots link gap fields to produce torque. Coil segments that are outside the field, called end windings produce no torque. Examples are G. Kasabian (U.S. Pat. No. 4,625,135, issued Nov. 25, 1986) and Leupold et al (U.S. Pat. No. 5,280,209, issued Jan. 18, 1994).
Few commercial motors are of the axial gap type, that employ flat disc shaped rotors and toroidal cores separated by an axial gap. Permanent magnets, that face the stator axially, are mounted on the flat surface of the rotor. Several pairs of flat magnets of alternating polarity generate a rotating magnetic field within the axial air gap. The stator windings are placed within the slots of the toroidal core, and loop from one slot to another. Conductor segments within the slots link the gap field to produce torque. Conductors outside the segments, called end windings, do not produce torque, but do contribute to loss. Examples of such patents are K. Sakai (U.S. Pat. No. 5,619,087, issued Apr. 8, 1997) and Hawsey et al (U.S. Pat. No. 4,996,457, issued Feb. 26, 1991).
Recently, a few patents have combined both approaches and employed both axial gaps and radial gaps to produce torque. Examples are N. Akiyama (U.S. Pat. No. 5,245,270, issued Sep. 14, 1993), Ewing et al (U.S. Pat. No. 5,625,241, issued Apr. 29, 1997), Morohashi et al (U.S. Pat. No. 5,838,079, issued Nov. 17, 1998), Naito et al (U.S. Pat. No. 5,864,197, issued Jan. 26, 1999), Hsu et al (U.S. Pat. No. 5,952,756, issued Sep. 14, 1999) F. Schmider (U.S. Pat. No. 6,232,690, issued May 15, 2001) and Lucidarme et al (U.S. Pat. No. 6,462,449 issued Oct. 8, 2002).
Hsu et al (U.S. Pat. No. 5,952,756, issued Sep. 14, 1999) describe an outer stator type motor. Three sets of permanent magnets are attached at the center of a shaft and three sets of corresponding stators are fastened to a surrounding frame. Two sets of flat permanent magnets create fields in the two axial gaps and one set of permanent magnets around the periphery create fields in one radial gap. The coil windings loop around the slots. Such 3-gap motors however suffer from several disadvantages. These 3-gapped motors in the prior art do not offer high torque density, are very expensive and have poor efficiency and can run hot.
Soghomoniam et al (U.S. Pat. No. 6,891,306, issued May 10, 2005) show another invention that uses 3 gaps, but with an outer rotor. The rotor uses two sets of flat magnets to energize two axial gaps and two sets of peripheral magnets of relatively smaller size to energize the radial gaps. The flat magnet facing one axial gap is polarized North, while that facing another axial gap is polarized South. A set of solenoidal electromagnets with annular windings generate alternating fields that interact with rotating fields to produce the motor torque.
The invention discloses a novel stator winding and core configuration with no slots. The invention relates to permanent magnet motors. Of special interest are those with rotors enclosing an internal stator. Such motors are used in wide ranging applications such as bike motors, hub motors, reaction wheels, momentum wheels, gyroscopes etc. The invention centers around motors that use multiple air gaps between the rotor and stator and multiple coil segments to produce higher torque per unit volume.
A “U” shaped rotor has axial magnets facing two axial sides of a stator and radial magnets facing the radial side of the stator. The permanent magnets are arranged with alternating polarities. The axial and radial permanent magnets on the rotor are arranged so that any plane through the axis of rotation intersects magnets of like polarity. The coils are arranged on a toroid between alternate pole pieces and coils.
With reference to
The radial magnets 26 extend over essentially the full axial length of the rotor inner shell 23 surface and are spaced equidistantly around essentially the circumference of the shell. The magnets are arranged with alternating polarity. The magnets are attached to a circular ring of back iron 29 using epoxy. The number, size and shape of the magnets depend on the application and torque requirements. The radial magnets 26 are polarized in the radial direction. All magnets on any radial line have the same polarity. For example,
Two sets of flat magnets 27, 28 are attached to the inner flat surface of each rotor bracket 21, 22 respectively via back iron discs 51, 52. These magnets are arranged in a circular ring fashion. The number of flat magnets is identical to that of the radial magnets 26. The flat axial magnets 27, 28 on the rotor brackets 21, 22 are alined so that the polarity of the magnets is the same across the air gaps. The axial magnets 27, 28 can be sector shaped as shown in
Both the radial magnets 26 and axial magnets 27, 28 generate magnetic fields that energize respectively the radial 53 and the axial gaps 54, 55. As shown in
How the hubs 58, 59 connect the stator 3 to the shaft 4 can be seen in
The pole piece 62 is shown in
The pole piece is a “U” shaped iron part. It has radial legs 77 with pole faces 73 and one axial shoe 72 with pole face 71. The outwardly facing pole faces present a relatively large iron area to the magnets. The axial pole shoe 72 is aligned with the radial magnets 26, while the radial legs 77 are aligned with the axial magnets 27, 28. The leg faces 73 face toward and adjacent the axial magnets 27, 28 and the shoe 72 pole face 71 faces toward and adjacent the radial magnets 26. The pole pieces 62 taper radially inwards. The pole piece legs 77 also have two blind grooves 76 at the bottom to catch or engage tongues 61 on the hubs. It has an opening or slot 75 at the center to slide over the toroid, shown in
The construction in
If this toroid design of
The coil flat front face 68 and flat rear face 88 extend in planes that essentially extend through the shift centerline with the coil outer axial extent and inner axial extent essentially parallel to the shaft centerline 45. The coil first radial extent 93 and second radial extent 94 are essentially perpendicular to the shaft centerline 45.
As shown in
The coil has three active segments, radial segment AB, axial segment CD and radial segment EF. As shown the radial segment AB carries current that travels radially outward. The axial magnet 28 has its north pole facing the axial pole face 73; it emanates field Bz1 that travels from left to right into the gap. Per Lenz law, the radially outward current links with this axially inward field. Since both the field and current are perpendicular to each other, their interaction produces a force that is perpendicular to both, in the tangential direction. This force is tangential to the stator and is into the plane of the paper as shown. This force produces torque.
In a similar manner, radial segment of coil EF carries a radially inward current I. The axial magnet 27 also has a north pole facing the iron of the stator pole shoe 73. It generates a field that is axial and travels from right to left. Again this field and current link to produce a magnetic force which results in torque. This torque adds to that produced by the conductor AB.
The coil also has an axial segment CD. Current is traveling from left to right in this segment of the coil. The radial magnets generated magnetic field, travels downwards. The current traveling from left to right link with the field Br traveling downward produce an additional magnetic force that is tangential to the stator ring. This force also contributes torque. This torque adds to the torque produced by AB and EF. The net result is that all three segments, AB, CD and EF of the coil participate in the production of torque, thereby increasing the torque significantly.
In
It is believed that the construction, operation and advantages of this invention will be apparent to those skilled in the art. It is to be understood that the present disclosure is illustrative only and that changes, variations, substitutions, modifications and equivalents will be readily apparent to one skilled in the art and that such may be made without departing from the spirit of the invention as defined by the following claims.
Number | Name | Date | Kind |
---|---|---|---|
3549926 | Pentland | Dec 1970 | A |
3868766 | Gramlich et al. | Mar 1975 | A |
4441043 | DeCesare | Apr 1984 | A |
4591751 | Ono | May 1986 | A |
4625135 | Kasabian | Nov 1986 | A |
4996457 | Hawsey et al. | Feb 1991 | A |
5117141 | Hawsey et al. | May 1992 | A |
5245270 | Akiyama | Sep 1993 | A |
5280209 | Leupold et al. | Jan 1994 | A |
5541460 | Dunfield et al. | Jul 1996 | A |
5561335 | Dunfield et al. | Oct 1996 | A |
5619087 | Sakai | Apr 1997 | A |
5625241 | Ewing et al. | Apr 1997 | A |
5838079 | Morohashi et al. | Nov 1998 | A |
5864197 | Naito et al. | Jan 1999 | A |
5894902 | Cho | Apr 1999 | A |
5952756 | Hsu et al. | Sep 1999 | A |
6137394 | Holmes et al. | Oct 2000 | A |
6232690 | Schmider | May 2001 | B1 |
6346759 | Suzuki et al. | Feb 2002 | B1 |
6426577 | Sekiyama et al. | Jul 2002 | B1 |
6462449 | Lucidarme et al. | Oct 2002 | B1 |
6555942 | Hsu | Apr 2003 | B1 |
6891306 | Soghomonian et al. | May 2005 | B1 |
Number | Date | Country | |
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20070228860 A1 | Oct 2007 | US |