Permanent Magnetized Synchronous Machine Designed According to the Transverse Flux Principle

In the art, it is known to arrange the magnets in a permanent magnetized synchronous machine so as to cause the magnetic flux to flow in paths at right angles to the direction of rotation of the rotor. A machine of this type, designed according to what is called the transverse flux principle, is illustrated in FIG. 1. The rotor of such a machine is made up of permanent magnets of alternate polarity. The magnets are secured to bars of magnetic material which serve as magnetic return conductors. The stator consists of U-shaped stator elements of magnetic material, the number of which is equal to half the number of magnets. The stator winding is designed as a ring winding. This means that, if the distance between the magnet bars, known as the pole pitch, is small, the copper volume per stator element becomes small, like the copper losses.

When the rotor is in a given position, the magnetic flux flows through all the stator elements in the same direction. When the rotor has rotated through one pole pitch, the direction of the flux through the stator elements has been reversed. When the rotor has rotated through another pole pitch, the direction of the flux through the stator elements has again been reversed. Thus, the flux through the ring winding accomplishes one cycle as the rotor rotates through two pole pitches.

As compared with a machine of the longitudinal flux type, the transverse flux machine of the invention offers the following advantages:

The cross-sectional area of the magnetic flux is practically constant throughout the path of flux. The iron losses in such a machine therefore are smaller than in a longitudinal machine, where locally, especially in the tooth area, the flux density is considerably higher than in the rest of the magnetic circuit.

In a transverse flux machine, the active amount of copper, consisting of the copper ring between the stator elements, is considerably smaller than in a longitudinal machine where the inactive amount of copper consists of the coil ends.

Thus, the transverse flux machine represents, in terms of weight and volume, an energy-dense machine of high efficiency. The shorter the pole pitch is, the smaller becomes the active amount of copper and the higher the efficiency.

The present invention aims at further considerably increasing the efficiency and the energy density per unit volume in a transverse flux machine. The inventive concept resides in radically changing both the stator and the rotor design, thereby making it possible to double the number of stator elements, which thus becomes equal to the number of magnets. In this manner, the power is doubled for a given volume.

The invention will now be described in more detail with reference to the accompanying drawings, in which:

FIG. 1 shows an existing machine of the transverse flux type;

FIG. 2 shows the machine according to the invention seen in the direction of the machine axis;

FIG. 2a is a part sectional view taken along the line A--A in FIG. 2, and FIG. 2b is a part sectional view taken along the line B--B in FIG. 2;

FIGS. 3, 3a and 3b show the machine of the invention in double-sided design;

FIGS. 4, 4a, and 4b show the machine of the invention designed as a shield pole type motor; and

FIGS. 5, 5a and 5b show a variant of the machine in FIGS. 2, 2a and 2b.

The permanent magnets in FIGS. 2a and 2b are magnetized in opposite directions. In FIGS. 2, 2a and 2b, numeral 1 designates a ring winding, and numerals 2 and 3 designate stator elements made of laminated sheet metal. All the stator elements are identical, but every other element is turned 180.degree. with respect to the magnet axis 8. Numeral 4 designates the permanent magnets. These magnets are centrally fixed on bars of soft iron or laminated sheet metal 5, which in turn are fixed to the rotor hub 6. In the bars 5 are generally U-shaped in cross section with radially outwardly extending legs. The stator elements 2 and 3 are generally rectangular in cross section with a central aperture formed for the ring 1. The stator elements are asymmetrical, each having a lower wall opening formed therein bounded by a pair of radially inwardly extending legs, one leg being adjacent the permanent magnet 4 and the other leg being adjacent one of the legs of the bar 5. The position shown in FIG. 2, the magnetic flux in all of the stator elements flows along the ring winding in the same direction. When the rotor has rotated through one pole pitch, the magnetic flux in all stator elements flows along the ring winding in the opposite direction. The frequency of the electromotive force induced in the ring winding is equal to the product of the rotor speed and half the number of poles.

The new generator, here called G2, offers the following advantages over the generator in FIG. 1, here called G1.

G2 has twice as many stator elements within the same volume as G1 and, hence, a power density per unit volume that is twice as high for the same amount of permanent-magnetic material. G2 has higher efficiency than G1 since the copper losses are equal in both machines.

It is known that the generator of FIG. 1 can be given a double-sided design, e.g. for two-phase operation. The generator according to the invention can also be given a double-sided design. For the sake of simplicity, such a design is shown in FIGS. 3, 3a and 3b as a linear machine. The numerals in these Figures refer to equivalent parts in FIGS. 2, 2a and 2b.

The machine in FIG. 2 can also be used as a motor. However, since it is a one-phase machine, this embodiment has no starting torque. By designing the machine as a shield pole type machine, it can generate, also in the one-phase embodiment, a certain starting torque. FIGS. 4, 4a, and 4b show a shield pole type motor design. A portion of the iron surface facing the air gap is grooved and provided with a short-circuit ring 7. In the case of one-phase feed, the flux through the short-circuit ring will be delayed in relation to the flux that does not pass through the short-circuit ring, this yielding a rotary flux and hence a torque in the same way as in a conventional shield pole type motor.

The machine in FIG. 2 can also be designed as a multi-phase machine for a phase number=3, 4, 5 . . . . In this case, m unit machines are arranged on the same axis, the stators or the rotors being offset 360/m electric degrees in relation to each other.

A variant of the machine in FIGS. 2, 2a and 2b is shown in FIGS. 5, 5a and 5b. In these machines, the stator and the rotor have a slightly different appearance, but the principle of operation remains the same in both machines.