Magnetically journalled rotational arrangement including a rotor for generating a unipolar bias magnetic flux

A magnetically journalled rotational arrangement includes a substantially disc-shaped or ring-shaped rotor and a stator. The stator includes structure for the production of a field which produces a rotation of the rotor. The rotor has structure which produce a unipolar bias magnetization flux which is spatially modulated when viewed in the circumferential direction.

BACKGROUND OF THE INVENTION

1. Field of the Invention

The invention relates to a magnetically journalled rotational arrangement including a substantially disc-shaped or ring-shaped magnetically journalled rotor and stator.

2. Description of the Prior Art

Magnetically journalled rotational arrangements are used today in numerous fields of application, in particular, where mechanically journalled rotational arrangements have considerable disadvantages, thus e.g., in stirrers or forwarding apparatuses for highly pure or biological liquids such as, for example, blood. Magnetically journalled rotational arrangements are also useful in applications such as clean room blowers or carrier apparatuses for wafers (so-called wafer carriers) where high demands are placed on cleanliness and no contamination, such as is caused e.g., by gases which can escape from the lubricants of mechanical bearings, may be tolerated. In these applications, both the journalling of the rotor (which can be designed, e.g., as the vaned wheel of a pump) and a rotational movement of the same must be possible.

A magnetically journalled rotational arrangement with a flywheel is described in EP-A-0,130,541. Apparatuses of this kind are used, for example, in the control of the orientation of satellites. Ring-shaped permanent magnets for the magnetic journalling of the rotor are provided both in the rotor and in the stator; moreover the stator also comprises control windings in order to be able to correct possible deflections of the rotor from the desired position. Further separate drive means for driving the rotor are also provided in the rotor and in the stator. This has the result that the total construction is relatively complicated and expensive.

SUMMARY OF THE INVENTION

The object of the present invention is to provide a magnetically journalled rotational arrangement by means of which a magnetic journalling as well as a rotation of the rotor can be produced at the same time. The magnetically journalled rotational arrangement should be as uncomplicated and inexpensive as possible and should, in particular, also permit the initially named uses.

DETAILED DESCRIPTION OF THE PREFERRED EXEMPLARY EMBODIMENTS

InFIG. 1one recognizes three exemplary embodiments of a rotor1of the rotational arrangement in accordance with the invention. The three rotors1each comprise axially magnetized, discrete permanent magnets M arranged at the one side of the rotor—at the upper surface of a ring10consisting of a ferromagnetic material. These permanent magnets produce a unipolar (the magnets on this side of the rotor are all magnetized in the same direction) bias magnetization flux which emerges radially from the ring10. In the region of the ring10, (between the permanent magnets M) the bias magnetization flux is right homogeneous when viewed in the circumferential direction. In all, it is considerably spatially modulated in the circumferential direction because gaps are continually provided between the individual discrete permanent magnets M. Through the interaction of a corresponding rotary or alternating field with the spatially modulated unipolar bias magnetization flux, a torque is produced in the rotor1. The three rotors shown inFIG. 1differ essentially in the number of poles or pole pairs. The rotor at the top has exactly four poles (two pole pairs), whereas the middle rotor has six poles (three pole pairs) and the bottom has eight poles (four pole pairs).

The exemplary embodiments of the rotor1shown inFIG. 2have permanent magnets M which are arranged on both sides of the rotor (that is, at the upper and the lower surface of the rotor) with the direction of magnetization of the permanent magnets M at the upper surface of the rotor being opposite to the direction of magnetization of the permanent magnets M at the lower surface of the rotor (both at the upper and the lower surface always having the same direction, that is, being unipolar).

FIG. 3shows exemplary embodiments of the rotor1in which permanent magnets M are arranged at one side of the rotor only, whereas permanent magnets are arranged at both sides of the rotor in the exemplary embodiments of the rotor in accordance withFIG. 4. Contrary to the exemplary embodiments ofFIG. 1andFIG. 2, the permanent magnets M are radially magnetized. Furthermore, additional ferromagnetic elements F (e.g., of iron) are provided for a better conduction of the magnetic flux.

FIG. 5shows an exemplary embodiment of the rotor1in which permanent magnets M are arranged at both sides of the rotor; on the one (here: the lower) side of the rotor, axially magnetized permanent magnets; on the other (here: the upper) side of the rotor, radially magnetized permanent magnets.FIG. 6shows an exemplary embodiment of the rotor with projections12and recesses11in which the modulation of the unipolar bias magnetization flux is thus produced by soft magnetic anisotropy. This type of rotor is also known as a reluctance rotor.

InFIG. 7, a plurality of embodiments of possible arrangements of the permanent magnets are illustrated. There one recognizes, beginning in the left column from top to bottom and then in the right column from top to bottom:axially magnetized permanent magnets M on both sides of the rotor1as well as in the stator2radially magnetized permanent magnets M on one side of the rotor1as well as in the stator2radially magnetized permanent magnets M on both sides of the rotor1as well as in the stator2radially magnetized permanent magnets M on both sides of the rotor1and axially magnetized permanent magnets M on both sides in the stator2radially magnetized permanent magnets M on one side of the rotor1and axially magnetized permanent magnets M on one side in the stator2axially magnetized permanent magnets M on both sides of the rotor1and radially magnetized permanent magnets M on both sides in the stator2axially magnetized permanent magnets M on one side of the rotor1and radially magnetized permanent magnets M on one side in the stator2axially magnetized permanent magnets M in the stator2and no permanent magnets on the rotor1(reluctance rotor), only one control winding20in the stator2axially magnetized permanent magnets M in the stator2and no permanent magnets on the rotor1(reluctance rotor), two control windings20in the stator2axially magnetized permanent magnets M in the stator2and in the rotor1, two control windings in the stator2. The magnetizations shown here can, in principle, also be oriented in reverse.

InFIG. 8, an exemplary embodiment of a rotational arrangement in accordance with the invention can be recognized in an exploded view. In this exemplary embodiment, the stator also comprises, in addition to a ring-shaped bearing stator21which produces the magnetic journalling of the rotor1in the bearing plane, two further motor stators22and23, of which the one motor stator22is arranged in a first motor plane parallel to the bearing plane on the one (here: the upper) side of the bearing stator21and the other motor stator23is arranged in a second motor plane parallel to the bearing plane on the other (here: the lower) side of the bearing stator21.

If one observes the bearing plane, one recognizes that the rotor1has axially magnetized permanent magnets M which are arranged on both sides of the rotor. Furthermore, a sensor ring13of a magnetically poorly conducting material, which is, however, of good electrical conductivity (e.g., aluminum), in which eddy currents arise during operation, which in turn produce magnetic fields which can be evaluated with the help of sensors S1, S2in the bearing stator21, is provided at the rotor1. In this manner, (which is known per se), the position of the rotor1can be precisely determined and, where required, corrected at any point in time.

The ring-shaped bearing stator21has teeth210which point in the radial direction toward the rotor1and on which, on the one hand, the stator-side permanent magnets M and, on the other hand, the control windings20are arranged. With the help of the control windings the permanent magnet flux can be selectively reinforced or weakened so that when a deviation of the rotor1away from the desired position of the rotor1arises, the rotor1can be moved back to the desired position again.

The two ring-shaped motor stators22and23likewise have teeth220and230pointing inwardly in the radial direction. Furthermore, they are each provided with a rotary field winding221and231, respectively, by means of which a corresponding rotary field can be produced in order to drive the rotor1rotationally. Rotary field windings221and231of this kind are known per se—they are therefore only schematically illustrated inFIG. 8. Since the number of poles or pole pairs in the rotor and the stator must agree, and since the rotor has a number of poles of four (two pole pairs) on both sides, the rotary field windings must also be designed in such a manner that a four-pole rotary field is produced in the motor stator. Naturally, it is also possible to omit one of the two motor stators, through which the torque is halved. In this case, it is also sensible to omit the permanent magnets on the corresponding side of the rotor. In this manner, the constructional height of the arrangement can be reduced.

FIG. 9shows the exemplary embodiment ofFIG. 8in a section. One recognizes inFIG. 9, on the one hand, the distribution of the magnetic flux produced by the permanent magnets M (solid line PF), which goes out from the permanent magnets M to the rotor1, leads via the air gap into the motor stator22or23, respectively, (consisting of a ferromagnetic material), leads further from there via the permanent magnets M in the bearing stator21, through the ferromagnetic material (e.g., iron) of the bearing stator21and its teeth210via the air gap between the bearing stator21and the rotor1back into the ferromagnetic material (e.g., iron) of the rotor1, and then finally closes again in the permanent magnets M of the rotor1. A part of the permanent magnet flux also passes directly from the permanent magnets M on the rotor1into the permanent magnets M on the bearing stator21, which is not illustrated inFIG. 9.

Furthermore, inFIG. 9one also recognizes in the air gap between the bearing stator21and the rotor1, the control flux (broken line CF) which can be produced with the help of the control windings20for the correction of deviations of the rotor from the desired position. The closed magnetic circuit of the control flux is not recognizable inFIG. 9since it extends in the bearing plane and thus, in principle, in a plane perpendicular to the plane of the permanent magnet flux (for this, seeFIG. 12). A reinforcement or a weakening of the permanent magnet flux can be produced only in the region of the teeth210and in the air gap between the bearing stator21and the rotor1(and naturally also at the entry into the rotor), because here the two field components, which otherwise do not influence each other, have the same orientation.FIG. 10andFIG. 11each show an arrangement analogous toFIG. 8in an illustration analogous toFIG. 9. In contrast toFIG. 8andFIG. 9, the permanent magnets M in the rotor1and in the bearing stator21inFIG. 10are both radially magnetized; inFIG. 1the permanent magnets M in the rotor1are radially magnetized whereas they are axially magnetized in the bearing stator21.

FIG. 12shows a plan view of the rotor in accordance with the exemplary embodiment ofFIG. 8, that is, a plan view onto the bearing plane. In this illustration, one now better recognizes the distribution of the control flux CF (broken line) which can be produced with the help of the control windings20in order to be able to move the rotor1back into the desired position in the event of a deviation from its desired position. It is clear that a part of the control flux is also closed back via the two other stator teeth, which is not illustrated here for reasons of greater clarity. Furthermore, the path of the permanent magnet flux PF (solid line) naturally does not show up well in this illustration; for the distribution of the permanent magnet flux seeFIG. 9. Finally, inFIG. 12, one also recognizes the two additional sensors S3and S4, which are not recognizable in the illustration in accordance withFIG. 8.

FIG. 13shows a section along the line XIII—XIII inFIG. 8, that is, a section in the first motor plane. One recognizes here the motor stator22and the distribution of the permanent magnet flux produced by the permanent magnets M. Furthermore, one also recognizes the—here four poled—rotary field winding221which is embedded into the individual grooves of the motor stator22(the rotary field itself is not illustrated). How a rotary field of this kind can be executed is sufficiently known to the expert and will therefore not be discussed here in further detail.

FIG. 14shows a further exemplary embodiment of the rotational arrangement in accordance with the invention, in this case, a segment arrangement. This designation derives from the fact that the means for the production of the rotary field (or the alternating field) are also arranged in the individual segments between the permanent magnets M in the bearing stator21, namely in the form of U-shaped coil cores24(e.g., iron cores) on which windings241are wound by means of which a rotary field (or an alternating field) can be produced. The U-shaped coil cores24are arranged here in the bearing plane, so to speak. The advantage is a low constructional height. One recognizes that the exemplary embodiment shown inFIG. 14is a rotor with the pole number sixteen (eight pole pairs). The arrangement illustrated here is a two phase arrangement which in principle can have 2, 4, 6, 8, . . . etc., U-shaped coil cores24; here it has four coil cores24, two of which are illustrated (due to the half-section illustration).

InFIG. 15, the arrangement of the U-shaped coil cores24and the windings241which are wound around these coil cores24can be recognized in an illustration of the principle. The windings of mutually oppositely lying coil cores are each flowed through by the same current; they can be connected in series or in parallel. The two phases P1and P2(it is a two-phase arrangement) are mutually electrically displaced by 90°. The pole division Tp amounts to:
Tp=(π.Di)/2p
where Di designates the inner diameter of a circle which is tangent to the poles of the U-shaped coil cores24near the rotor1; hence, Di/2 represents the radius of this circle (seeFIG. 15), and p the number of pole pairs.

The permanent magnets M on the rotor1each follow one another displaced by an angle of 45° (there are eight permanent magnets M which are uniformly distributed over an angle of 360°). If one were now to likewise arrange the four U-shaped coil cores24over the angle of 360° with the same regularity (thus displaced with respect to one another by a geometrical angle of 90°), then exactly one permanent magnet M of the rotor each would come to lie between and in front of the U-shaped coil cores at the same time. Completely independently of the electrical displacement angle of the two phases P1and P2, no starting up of the rotor1can take place in this manner since when the magnetic field increases or decreases, the respective permanent magnet on the rotor1will only be more or less strongly attracted or repelled by the respective U-shaped coil core24. One would thus have to supply an impulse (e.g., mechanically) to the rotor at first in order to set it rotating.

In order now that an electrical start-up of the rotor be possible, the two phases P1and P2(which are electrically displaced by 90°) must be mutually geometrically displaced, and indeed, ideally in such a manner that one permanent magnet comes to lie completely in front of the coil core of the one phase when another permanent magnet comes to lie exactly half in front of the coil core of the other phase so that a torque acting on the rotor1can always be produced with one of the two phases P1or P2. This geometrical displacement amounts to:
(360°/2p)·((1/m)+k),
where p stands for the number of pole pairs (here 8), m designates the number of phases (here 2) and k is a natural number, which amounts here, in principle, to the displacement angle 11.25°+k 22.5°; in particular, in the exemplary embodiment shown, k=4. One recognizes inFIG. 15the angle α=11.25° and the corresponding displacement of the coil cores24. Analogously to this example, arrangements with any desired phase numbers, in particular, also one and three phase arrangements as well as any desired numbers of pole pairs, are possible. It is also conceivable to use motor segments with a plurality of grooves per pole division and with an approximately sinusoidal flux distribution. Air gap windings are likewise conceivable in order to prevent groove latch torques where possible.

FIG. 16shows a further exemplary embodiment of the rotational arrangement in accordance with the invention which corresponds to the exemplary embodiment ofFIG. 14as regards the basic principle in which the coil cores24are arranged perpendicular to the bearing plane. Moreover, permanent magnets M are also arranged on both sides of the rotor1; the corresponding is true of the bearing stator21as well.FIG. 17shows a corresponding section along the line XVII—XVII inFIG. 16. An arrangement of this kind corresponds to a “transversal flux motor” shown here as a segment motor with split phase.

FIG. 18shows a further exemplary embodiment of the rotational arrangement in accordance with the invention. In this exemplary embodiment, the rotor1comprises two rings10aand10bconsisting of a ferromagnetic material which has projections12aand recesses11a(or12band11b, respectively, which are not recognizable) (reluctance rotor). An axially magnetized permanent magnet ring MR, which is not structured, is arranged between the two rings10aand10b. The ring-shaped bearing stator21likewise comprises two rings21aand21b, with two axially magnetized permanent magnets M being arranged between the teeth210aand210bof the two rings. Furthermore, one also recognizes the control windings20aand20b(in principle, only one control winding is required) as well as the sensors S1and S2for the determination of the respective current position of the rotor. The means for driving the rotor1are formed on at the upper ring21aof the bearing stator21in the form of coil cores24a, with corresponding windings241abeing wound around the coil cores24a. This exemplary embodiment is distinguished by a high permanent magnetic bias magnetization flux, which enables the air gap between the stator and the rotor to be enlarged for certain applications and nevertheless enables a reliable magnetic journalling to be achieved.

The exemplary embodiment ofFIG. 19differs from the exemplary embodiment ofFIG. 18substantially through the different embodiment of the rotor1. The latter comprises no permanent magnets, but is of a ferromagnetic material, has the said structure with the projections12and recesses11and is surrounded by a sensor ring13of a magnetically poorly conducting but electrically well conducting material (e.g., of aluminum). This exemplary embodiment is advantageous, in particular, for applications in which the rotor1must be thrown away or recycled after a single use because this is dictated by the corresponding application (e.g., when pumping blood). The rotor1is namely comparatively simple and economical to manufacture due to the absence of or, respectively, the presence of non-existent, permanent magnets.

FIG. 20shows an exemplary embodiment of a rotor1which is manufactured of a ferromagnetic material and has a U-shaped profile. It is surrounded by a sensor ring13. Through the U-shaped profile the rotor1has an upper ring10aand a lower ring10bwhich are connected to one another via the web. Whereas the upper ring10ahas a structure with projections12aand recesses11a, the lower ring10bhas no structure. A rotor of this kind is advantageous in so far as the vibratory forces which arise as a result of the structuring are reduced, since the lower ring10bhas no structure. In addition, it is possible to measure the position of the rotor with the help of Hall sensors in the air gap of the lower ring. Otherwise, the advantages correspond to those of the rotor in accordance withFIG. 19. In addition, the reluctance forces with respect to an axial journalling of the rotor are greater (due to the groove between the individual “rings” of the U-shaped profile).

FIG. 21shows an exemplary embodiment of the rotational arrangement in accordance with the invention with a bearing stator21of the already described kind with axially magnetized permanent magnets M arranged at one side and with a motor stator25with a disc rotor winding250. A disc rotor winding is, so to speak, a flat winding which is arranged in a plane for the production of a rotary field. Disc rotor windings are known per se and can, in particular, have a multiple layer structure. The disc rotor winding is preferably without iron, through which axial drawing forces on the rotor1are practically completely avoided.

FIG. 22shows an exemplary embodiment of the rotational arrangement in accordance with the invention in which the rotation of the rotor1is produced with the help of a drive which can be permanent magnetically coupled to the rotor1. The bearing stator21and the rotor1correspond here to the bearing stator21and the rotor1ofFIG. 21. Only the drive is designed differently; here it comprises namely a disc26consisting of ferromagnetic material on which axially magnetized permanent magnets M are arranged, with the arrangement of the permanent magnets M on the disc26corresponding to the arrangement of the permanent magnets M on the rotor1. The disc26is drivably mechanically journalled. When the disc26is driven, the rotor1synchronously follows the rotation of the disc26via the permanent magnetic coupling (here permanent magnetic axial coupling) as a result of the reluctance forces.

The exemplary embodiment in accordance with the invention ofFIG. 23differs from the exemplary embodiment ofFIG. 22only in that the permanent magnets M of the drive are not mounted on a ferromagnetic disc but on a ferromagnetic ring27which in turn is connected to a connecting rod28which is drivably mechanically journalled. The operating principle is the same: As a result of the reluctance forces, the rotor1follows synchronously during a rotation of the connecting rod. Finally,FIG. 24shows a use of the rotational arrangement in accordance with the invention in the form of a pump, in particular, for highly pure or biological liquids, especially blood. The bearing stator21and the drive26correspond here to the corresponding parts of the exemplary embodiment in accordance withFIG. 22. The rotor is designed here as a vaned wheel1aand is arranged in a closed pump housing3of a magnetically poorly conducting material (e.g., plastic or chrome steel). The pump housing3has two connection pieces30and31for the intake and outlet of the liquid to be forwarded, for example, blood. A pump of this kind must be regularly disposed of after a single use. This can be done in a simple manner by pulling the intake and outlet lines off the connection pieces30and31and inserting a new pump housing. The remaining apparatus can be reused; moreover, the replacement of the pump housing can be carried out simply and comfortably.

Furthermore, it should be mentioned that in the rotational arrangement in accordance with the invention, in particular, with respect to its use as a blood pump, a number of aspects from WO-A-96/31934 are conceivable. Thus, both an inner rotor and an outer rotor are conceivable. Furthermore, as already mentioned, a hermetic partition (such as e.g., a gap tube or a vessel) can be arranged between the stator and the rotor. The rotor itself can be encapsulated with a plastic, with a ceramic or with another non-metallic material. Furthermore, as has already partially been described, a ring of electrically well conducting but magnetically poorly conducting material which is arranged around the rotor can be provided and can serve as a sensor ring for the position measurement by means of eddy currents. The determination of the respective angular position of the rotor can be done by means of Hall sensors, which can likewise serve as position sensors, which is advantageous in the measurement across an electrically conducting gap tube. The rotor together with the vessel surrounding it (see e.g., the blood pump described with reference toFIG. 24) can be replaceable and disposable or recyclable in order to be able to guarantee sterility. More details on all these topics can be found in WO-A-96/31934.

In particular, the sensor system, in uses in which a vessel is arranged between the stator and the rotor (e.g., the pump housing3inFIG. 24), shall again be discussed because the eddy current sensors which are typically used for the determination of the position of the rotor1relatively quickly reach their limits when certain materials (e.g., chrome steel) are used for the vessel (or for the pump housing, respectively). Here magnetic sensors, in particular, the above-mentioned Hall sensors, prove particularly advantageous. How Hall sensors of this kind can be arranged is shown in the exemplary embodiment ofFIG. 25. The exemplary embodiment illustrated there corresponds to the exemplary embodiment ofFIG. 14(segment arrangement); here, the sensors are arranged and/or designed differently.

In principle, the Hall sensors can be arranged in the air gap between the bearing stator21and the rotor1. They can, in particular, also be mounted (e.g., adhesively fixed) on the teeth210of the bearing stator21, as the Hall sensors SH1, SH2, SH3are. In this case, the Hall sensors are arranged on a separate permanent magnet. In both variants, the Hall sensors are permeated by a relatively large rest flux (in the adhesively fixed variant this is produced by permanent magnets in the stator, in the other variant by the separate permanent magnet located directly at the sensor) so that the possible influence of stray fields, which are produced by the coil cores24and their windings241, is slight. Without a rest flux, comparatively large fluctuations in the flux would otherwise arise through the permanent magnets moving past. For the determination of the position of the rotor in the respective direction, the difference of the signals from two geometrically oppositely disposed sensors is particularly suitable, even if one sensor per direction would theoretically be sufficient.