• 专利附录
  • 专利说明
  • 权利要求
  • 类似技术
  • 同族专利
  • 引用文献
  • 法律状态
  • 优先权
    • 专利摘要:
    Device (40) for the magnetic axial bearing of a rotor bearing a thrust bearing plate (32) in an axial magnetic bearing (54) with at least two independently controllable bearing branches (3, 4, 41), each having at least one coil (5, 42), wherein a magnetic flux separation of the bearing branches (3, 4, 41) is provided. According to the invention, the flux separation consists in that at least two of the bearing branches (3, 4) are arranged successively in the circumferential direction and have a single common pole (9) which has a circularly closed circumference, and which concentric with the center of rotation (35) the rotor is arranged, wherein the coils (5) with the common pole (9) connected to the associated pole segments (11) and the common pole (9) either radially inside or radially outside of the pole segments (11) is arranged.
    公开号:AT513498A4
    申请号:T50040/2013
    申请日:2013-01-22
    公开日:2014-05-15
    发明作者:Alexander Schulz；Harald Sima；Thomas Hinterdorfer；Johann Wassermann；Manfred Neumann
    申请人:Tech Universität Wien；
    IPC主号:
    专利说明:

    The invention relates to a device and a method for the magnetic axial bearing of a, having it connected thrust bearing rotor having in a Axialmagnetlager with at least two independently controllable bearing branches, each having at least one coil.
    The non-contact storage of rotors by means of magnetic bearings has compared to conventional Wälzkörper- or plain bearings on several advantages. Because of the freedom from contact, the losses during operation are comparatively low, even at speeds above 100,000 rpm. The speed limit of conventional bearings, given a shaft diameter, is significantly lower than that of magnetic bearings, which is limited only by the strength of the rotating parts. The freedom of contact allows the use of magnetic bearings even in vacuum applications.
    In US 5,969,451 A a magnetic bearing with a plurality of coils is shown, wherein the stator arranged on the stator can have more than one coil. For example, two coils are arranged in an annular core having an E-shaped profile, so that the middle part of the core is at the same time the inner pole of the outer coil and the outer pole of the inner coil. A disadvantage of this and similar magnetic bearings is the non-monotonous force curve at non-uniform BeStrömung and the required diameter of the thrust bearing plates and thereby achieved due to the limited mechanical strength relatively low maximum speed. In the bearings shown in US Pat. No. 5,969,451, as well as bearings constructed in a fundamentally similar manner, considerable assembly work is also to be expected during installation and removal.
    WO 2012/135586 A2 describes an axial magnetic bearing, wherein both the stator and the rotor are composed of layers or lamellae of weichmagnetischeffl material for the reduction of eddy currents. On one side of the stator, a circular arrangement of a plurality of kidney-shaped joints is provided, in which coils are mounted. Even if a reduction of eddy currents is achieved with this structure, the dimensions of the thrust bearing plate remain substantially unchanged. A further disadvantage of the coil arrangement shown here is that in the circumferential direction between the coils, a magnetic field which is opposite to the interior of the coils is generated. The rotating Axiallagerplätte is thus exposed to a magnetic field with alternating sign, which induces eddy currents, and thus exerts a braking effect on the rotor. The maximum speed is further reduced due to the significantly lower strength of the laminated rotor compared to designs made of solid material.
    [0öQ5] Compared to the devices known in the prior art, it is an object of the invention to achieve a higher maximum speed with at least comparable reliability and safety, which would be particularly advantageous for flywheel energy storage (Ely-wheel Energy Storage System, FESS). In addition, a high energy efficiency and easy assembly and disassembly of the device with the highest dimensional stability and stability can be achieved.
    This object is achieved in that a magnetic flux separation of the bearing branches is provided, wherein the flow separation consists in that at least two of the bearing branches are arranged sequentially in the circumferential direction and have a single common pole, which has a circularly closed circumference, and which is arranged with the center on the axis of rotation of the rotor, either radially inwardly or radially outwardly of the bearing branches, the coils surrounding pole segments connected to the common pole (not referring to segments in a geometric sense, but generally to sections of the composite yoke) ), and / or in that the thrust bearing plate is divided into at least two coaxial, each one bearing branch associated plate members, which are separated by non-ferromagnetic material, wherein the bearing parts associated with the bearing parts coaxially partially into one another or overlapping are ordered. Simplified, the flow separation is achieved via an azimuthal separation of the bearing branches and / or a radial or axial separation of the thrust bearing plate, since the only common pole in the azimuthal separation 3/54 3 of the bearing branches only on one side of the coil assembly and not is arranged on both sides, the magnetic flux is concentrated on a particularly small area. This applies in particular to a common pole arranged radially inside the pole segments. Both in a radially inner side and in a radially outer side arrangement of the common pole, a thrust bearing plate can be used with small radial dimensions. This is advantageous in order to achieve a mechanical load of the axial bearing plate, which is reduced compared to the prior art, and thus a higher maximum rotational speed. Due to the arrangement according to a subdivision in the circumferential direction instead of a radial subdivision, the magnetic bearing can be compact, without sacrificing the reliability and reliability guaranteed by several coils. In this case, the coils are not arranged in one another, but furthermore connected to only one common pole, so that along this common pole an azimuthal, i. in the circumferential direction, largely homogeneous magnetic field is generated. This also minimizes core losses in the thrust bearing plate. By surrounding the coils with pole segments connected to the common pole, stray fluxes are reduced or avoided and the magnetic flux lines are concentrated in the common pole. The pole segments thus form the coil cores, the coils in the best case are applied directly to the pole segments or are wound around these, so that the entire magnetic flux generated by the coils passes through the pole segments. Since the pole segments are connected to the common pole, most of the magnetic flux can be directed through the single common pole.
    Alternatively or additionally, the flow separation according to the invention can be achieved by means of a division or separation of the axial bearing plate in coaxial partially interleaved or overlapping bearing branches. As a result, stray fluxes and interactions between the bearing branches, in particular between the separately controlled electromagnet, via the thrust bearing plate, which could lead to non-monotonous force curves at different energizations, can be reduced or avoided. This simplifies the regulation of the coil control and contributes to the energy efficiency of the magnetic bearing at 4/54 4
    In this case, an axial separation is particularly advantageous since in this case the plate parts can each be connected directly to a shaft of the rotor. In addition, the diameters of the plate parts may be smaller than in a purely radial separation.
    In order to achieve a particularly advantageous azimuthal homogeneity of the magnetic field, it is advantageous if the common pole has an annular pole face and the coils essentially describe concentric circular arcs with the pole face. The pole face is that surface of the pole which faces a thrust bearing plate and is separated from the thrust bearing plate only by a gap, preferably a constant width. Preferably, the coils are designed so that the coils substantially follow one another in the circumferential direction substantially immediately, i. essentially form a continuous circle and cover approximately the entire angular range of 360 °.
    In addition, it is advantageous if the pole segments have substantially concentric with the pole face of the common pole, circular arc-shaped pole faces. As a result, an approximately homogeneous distribution of the flux lines emanating from the pole segments over the entire angular range can be achieved.
    The azimuthal homogeneity of the magnetic field can be further improved and the dimensions of the Axialmagnetlagers can be further reduced if the pole faces of the pole segments in the circumferential direction substantially immediately adjoin one another. The thus directly circumferentially consecutive pole faces allow a uniform distribution of the magnetic field and prevent between the pole segments gaps with less or even effectively reversed poled current induce eddy currents in the thrust plate and ultimately exert a braking effect.
    It has been found to be particularly advantageous if the inner diameter of the outer bearing branch is larger than the outer diameter of the inner bearing branch associated plate part of the thrust bearing plate in the partially interleaved or overlapping arranged bearing branches. The advantage of a 5/54 5-type design is the easy removability of the rotor from the axial magnetic bearing or the greatly simplified assembly and disassembly of the entire assembly.
    A particularly small required Axiallagerplattenfläche can be achieved if the distance between the inner and outer pole with increasing distance to the thrust bearing plate is larger. As a result, on the one hand, the formation of stray fluxes is counteracted and, on the other hand, the available installation space for the coil (s) is increased.
    An additional reduction of the required Axiallagerplattenfläche can be achieved by a decreasing in the direction of the thrust bearing plate distance between the inner and outer contour of at least one pole piece, which both ring-shaped poles or Pölringe as well as pole segments are meant reach. As a result, the flux density in the region of the pole faces can be increased and thus better material utilization with regard to flux distribution can be achieved. The resulting possible reduction in flux density leads to a reduction in the re-magnetization losses.
    In order to produce a homogeneous magnetic field in the circumferential direction and to avoid field gradients in the circumferential direction even at a distance between the Polringsegmenten, it is advantageous if the Polringsegmente below the coil, in particular in a region between the coil and pole face, in the circumferential direction a projection have, wherein the length of the projection corresponds approximately to the distance between the end faces of the Polringsegmente, so that no or only a minimal gap between the pole faces arises with respect to low flow gradients in the rotating thrust bearing plate, or in terms of the best possible separation of the flows of the magnetic branches as large a distance makes sense, with a compromise between the achieved flow separation and the avoidance of Ummagnetisierungsverlusten is selected.
    The advantages of the previously described embodiments can be used particularly effectively if the surface of the thrust bearing plate in a plane perpendicular to the axis of rotation is smaller than the sum of the surfaces of the coils and poles in a plane 6/54 6 perpendicular to the axis of rotation. Due to the relatively small thrust bearing plate, higher maximum speeds can be used over larger thrust bearing plates of the same material since the mechanical load on the smaller thrust plate is less for the same material (i.e., same density and strength) and speed.
    In order to achieve an equilibrium of forces with respect to the axis of rotation even with uneven energization of the independent coil arms and to avoid any aligned perpendicular to the rotational axis torques is an even number of symmetrically arranged to the rotation axis, with respect to the rotation axis opposite arrangement of each jointly controlled coils advantageous. By symmetry is meant in this context a single or multiple mirror symmetry. But it also means n-fold rotational symmetries, where n can take any integer value greater than two (n> 2). In this case, in general, one or two coils of a coil opposite, so that if one coil fails either a coil can be disabled or two coils can be fed with less power.
    In connection with the subdivision of the thrust bearing plate, the reliability of the magnetic bearing can be further increased when the axial magnetic bearing has an additional, substantially annular coil which interacts with a different part of the thrust bearing than the successive circumferentially coils. It has been found to be particularly advantageous if the annular coil has a full-surface inner pole, wherein the inner pole opposite part of the thrust bearing plate forms a full-surface disc, which is arranged at the end of the rotor. With this arrangement, the diameter of the thrust bearing plate part can be kept small for a given area or predetermined magnetic flux density.
    The energy efficiency of the axial magnetic bearing is particularly advantageous if the axial magnetic bearing has at least one permanent magnet, preferably at least one hybrid magnet with a permanent magnet and an electromagnet. In particular, the permanent magnet can be dimensioned so that the expected average bearing forces applied by the permanent magnet and the coils are used only for stabilization or for corrections.
    If at least one of the coils has a larger dimension in the axial direction than in the radial direction, the axial magnetic bearing can be compact, especially in the radial direction, and the overall length of the coil can be reduced to reduce electrical losses.
    In order to achieve a particularly good utilization of the available installation space, at least one of the coils may have a cross-section converging to the axial bearing plate and / or decreasing radius. This is particularly advantageous in connection with pole shoes converging towards or decreasing in radius, since thus clearances and stray fluxes resulting therefrom can be reduced and the maximum rotor speed increases due to the possible smaller plate diameter.
    In order to improve the reliability of the Axialmagnetlagers and to ensure the bearing functionality despite any failure of a bearing branch can be provided that the Axialmagnetlager has at least two position sensors, which are each assigned to different bearing branches. The position sensors may be, for example, eddy current sensors.
    The coils can be controlled in particular by decoupled control systems and in case of failure of a coil, the remaining coils can take over the storage and stabilization of the rotor. Thus, with the exception of the rotor, completely closed-loop control circuits may be provided for controlling the coils, so that if one element, for example a coil, a position sensor or control electronics fails, only the respective control loop is affected and the bearing is affected by the remaining control loop can be stabilized further. The invention will be further elucidated on the basis of particularly preferred exemplary embodiments, to which, however, it should not be restricted, and with reference to the drawing. In detail in the drawing:
    1 shows a device with a Axialmagnetlager with two semicircular coils in a sectional view transverse to a rotation axis.
    FIG. 2 is a perspective view of the axial magnetic bearing according to FIG. 1; FIG.
    3 schematically shows a radial section of a coil of an axial magnetic bearing according to FIG. 2 with a thrust bearing plate and a possible course of the magnetic field lines;
    4 shows a magnetically supported shaft with an axial magnetic bearing according to FIGS. 1 to 3 at each end of the shaft in a sectional view along an axis of rotation;
    5 shows a device with an axial magnetic bearing with two semicircular rinses and with a central bearing branch in a sectional view transversely to a rotation axis;
    6 schematically shows a radial section of the central bearing branch according to FIG. 5 with a possible course of the magnetic field lines;
    7 shows a magnetically supported shaft with an axial magnetic bearing according to FIGS. 1 to 3 at one end of the shaft and an axial magnetic bearing according to FIG. 5 at the other end of the shaft in a sectional view along the axis of rotation;
    FIG. 8 shows a variant of the magnetically supported shaft according to FIG. 7 without a permanent magnet; FIG.
    FIG. 9 shows a further variant of the magnetically supported shaft according to FIG. 7 with convergent semicircular coils; FIG.
    FIG. 10 shows a further variant of the magnetically supported shaft according to FIG. 7 with rounded bobbins and non-linearly converging pole rings; FIG.
    11 is a schematic block diagram of a control circuit for one of the devices according to FIGS. 7 to 10;
    FIG. 12 shows an axial magnetic bearing with three coils arranged in the shape of a circular ring segment in a sectional view transversely to the axis of rotation; FIG.
    FIG. 13 shows an axial magnetic bearing according to FIG. 12 in a sectional view along the axis of rotation along the line XIII-XIII in FIG. 12;
    FIG. 14 shows a perspective view of the axial magnetic bearing 9/54 9 according to FIGS. 12 and 13;
    FIG. 15 shows a magnetically supported shaft with an axial magnetic bearing according to FIG. 1 at one end of the shaft and an axial magnetic bearing according to FIG. 12 at the other end of the shaft in a sectional view along the axis of rotation;
    FIG. 16 shows a FESS external rotor with two axial magnetic bearings (FESS - Flywheel Energy Storage System); FIG. and
    17 shows a magnetically supported shaft with axial magnetic bearings at both ends of the shaft in a sectional view along the axis of rotation; In Fig. 1 is a section through a device 1 for magnetic axial bearing of a rotor is shown. The device 1 has an axial magnetic bearing 2 with two bearing branches 3, 4, each having a substantially semicircular coil 5. Since the coils 5 naturally have a closed course, each coil 5 has two semicircular sections 6, which are connected at both ends via radially extending sections 7. The two bearing branches 3, 4 are arranged consecutively in the circumferential direction and arranged opposite one another with respect to an axis of rotation 8 in the center of the axial magnetic bearing 2, the sections 7 being substantially parallel to one another at the coil ends of the adjacent coils 5 of the bearing branches 3, 4. Between the bearing branches 3, 4 or on a radial inner side of the bearing branches 3, 4, the axial magnetic bearing 2 has only one common, closed pole in the form of a pole ring 9. The single common pole ring 9 has a continuous annular cutting surface 10 and is substantially concentric with the coils 5, arranged radially inside the bearing branches 3, 4, wherein the center of the cutting surface 10 is located on the axis of rotation 8. The circumferentially successively arranged bearing branches 3, 4 surround the entire pole ring 9 and cover the entire angular range of 360 ° substantially completely. Since the two coils 5 are preferably constructed identically, the two bearing branches 3, 4 bearing branches of the axial magnetic bearing 2 are substantially identical and cover each about half of the pole ring 9 from.
    In the interior of the coils 5, substantially 10/54 10 circular pole segments 11 are respectively arranged, which substantially fill the coils 5, for example because the coils 5 are wound around the pole segments 11. The windings of the coils 5 are in the illustrated example in the display plane, so that the magnetic field induced by current flowing through the coils 5 in the pole segments 11 magnetic field is aligned at least partially parallel to the axis of rotation 8 (see Fig .. 3). The pole segments 11 are parts which are produced separately from the common pole ring 9 and which, in the assembled state of the axial magnetic bearing 2, are in contact with the pole ring 9 and are preferably connected thereto (see FIG. 4). The axial magnetic bearing 2 is surrounded by a jacket 12 (see Fig. 1), which serves as a carrier or for stable mounting and possibly the shielding magnetic leakage flux. In the Polringsegmenten 11 and in the shell 12 are parallel to the axis of rotation or perpendicular to the drawing plane connecting elements 13 and 14, for example, screws, for mounting the device 1 is provided.
    Since no magnetic material is arranged between the coils 5, a flow separation between the bearing branches 3, 4 can be achieved by the sequential arrangement in the circumferential direction of the bearing branches 3, 4. At the same time, due to the common pole ring 9, optimum azimuthal magnetic flux density homogeneity, i. optimal homogeneity in the direction of rotation, can be achieved and thus can be reduced magnetization losses in the thrust bearing plate.
    2, a part of the device 1 shown in FIG. 1, wherein for better visibility of the coil 5, among other things, the jacket 12 is not shown. At the visible bottom side 15 of the Axialmagnetlagers 2, the only annular pole face 16 of the single common pole ring 9 is just as recognizable as the pole faces 17 of the two pole segments 11. The pole faces 17 of the pole segments 11 form a pole face 16 of the pole ring 9 concentric circular ring, which only is interrupted at the two abutting surfaces of the pole segments 11. Although the pole segments 11 are beabsLandet in the coil 5, as can be seen in particular from the sectional surface in Fig. 1, the pole faces 17 of the pole segments 11 in the circumferential direction directly adjacent to each other by the pole segments 11 below 11/54 11 of the coils in the circumferential direction have protruding projections 18. Between the pole surface 16 of the pole ring 9 and the pole faces 17 of the pole segments 11, a distance 19 is provided, which in the example shown is greater than the distance 20 of the pole faces 16, 17 to a thrust bearing plate 21 (see Fig. 3). The pole segments 11 have a radius decreasing towards the respective pole face 17, i. they extend below the coils 5 radially inwards, towards the axis of rotation 8, or they are formed to the pole faces 17 in the form of a truncated cone tapering. The common pole ring 9 has a decreasing over the entire height radius or is tapering over the entire height tapered. It is thus achieved that the pole faces 16, 17 have a smaller radius and are smaller than the sectional areas of the pole ring 9 and the pole ring segments 11 in the region of the coils 5 shown in FIG. 1. The pole face 16 of the pole ring 9 is slightly wider than the radially Pole surfaces 17 of the two pole segments 11, so that the pole face 16 of the pole ring 9 corresponds approximately to the sum of the pole faces 17 of the two pole segments 11.
    In Fig. 3 is a radial cross section of the axial magnetic bearing 2 according to the line III-III in Fig. 1 with a Axiallagerplätte 21 is shown. It schematically shows a possible course of magnetic field lines 22 in order to illustrate the magnetic flux density. The field lines 22 correspond to the equipotential lines of the magnetic flux. The arrow size of the illustrated directional arrows 23 on the field lines 22 is approximately proportional to the local flux density. In the indicated direction of the magnetic field, a current flows in the radially inner, lying between the pole ring 9 and the pole segment or Pol-ring segment 11 coil portion 24 in the plane and in the radially outer coil portion 25 in the direction of the plane of the drawing. The magnetic field lines 22 are closed via the thrust bearing plate 21, whereby it is magnetically attracted. Both the pole ring 9 and the lowermost portion 26 of the pole segment 11 has a cross-section converging to the pole face 16 or 17, whereby the flux density in the region of the pole faces 16, 17 is increased in relation to the flux density in the region of the coil 5. In addition, the radius of both pole bodies 9, 11 (referred to collectively as the pole ring 9 and the pole segments 11 12/54 12 or generally all pole elements forming a magnetic core) to the pole faces 16, 17 decreases, which due to decreasing magnitude in addition to increasing the flux density. Due to the relatively small pole faces 16, 17 and the small distance between the pole faces, the thrust bearing plate 21 can have a correspondingly small radius and cross section, and the mechanical loads acting at high rotational speeds can be reduced compared to larger thrust bearing plates. On the other hand, owing to the relatively low flux density in the region of the coils 5, lower magnetization and thus, due to the nonlinear relationship between flux density and magnetic resistance in real soft magnetic materials, lower magnetic resistance of the pole bodies 9, 11 and lower core losses can be obtained, which is useful to reduce stray flux outside the polar bodies 9, 11.
    4, a device 27 with a magnetically mounted shaft 28 is shown. For the sake of simplicity, only the axial magnetic bearings 29, 30 but no radial bearings are shown. The shaft 28 is shown shortened with a schematic interruption 31 (similar also in Fig. 7, 8, etc.), to indicate that the length of the shaft 28 is not shown here proportionally. The axial magnetic bearings 29, 30 respectively correspond to the device 1 shown in FIG. 1, each having two semicircular opposite coils 5 with a common pole ring 9 and separate pole segments 11. The axial magnetic bearings 29, 30 each interact with a disc-shaped thrust bearing plate 32, 33, wherein the Axiallagerplatten 32, 33 arranged in the region of one end of the shaft 28 and non-rotatably connected to the shaft 28, for example, screwed, are. However, it is immediately apparent to those skilled in the art that the shaft 28 may also be made in one piece with the thrust bearing plates 32, 33, for example entirely made of soft magnetic iron or steel. In addition, such a shaft could also have a constant diameter, so that instead of the offset thrust bearing plates 32, 33, the shaft would have only one axial bearing plate surface at each end or the shaft would correspond to a single, very thick axial bearing plate. The diameter of the thrust bearing plates 32, 33 is selected so that the radius of the thrust bearing plates 32, 33 is slightly larger than the outer radius of the pole face 17 of the pole segments 11, so that the pole faces 17 of the pole segments 11 of the thrust bearing plates 32, 33 are completely covered.
    Radially within the annular axial magnetic bearings 29, 30 are compared to two thrust plates 32, 33 also distance sensors 34, for example, eddy current sensors arranged. The distance sensors 34 are arranged away from the axis of rotation 35 and detect their own distance to the Axiallägerplatte 32 ·, 33 and thus the relative position of the thrust bearing plate 32, 33 and the shaft 28 in the Axialmagnetlagern 29, 30. Based on the measured position, the coils 5 of the axial magnetic bearings 29, 30 so controlled that the rotor (only partially shown) between the axial magnetic bearings 29, 30 remains centered or will.
    In operation, changes in the operating temperature typically lead to different thermal expansions of the rotor and the stator. A heating of the rotor, for example due to the losses of a motor rotor, in this case leads to an elongation of the rotor. On the other hand, an increase in the RoLord rohzah L due to the centrifugal forces acting to reduce the rotor length. In order to enable a stable axial position of the rotor despite these effects, preferably the differential arrangement of the distance sensors 34 shown in FIG. 4 can be used. Here, the axial distance of the rotor relative to the stator at both rotor ends by means of the distance sensors 34 is detected, and their signals /, or z2 are used, for example, as follows for determining the desired position: _ zl + z2 • h, .so // Λ The axial magnetic bearings 29, 30 are each mounted on a carrier unit 36 and surrounded by a jacket 12, which is made of aluminum or non-ferromagnetic stainless steel, for example The coils 5 and the pole bodies 9, 11 are each arranged on an opposite side of the carrier unit 37 to the shaft 28. The jackets 12 extend like covers over the axial magnetic bearings 29, 30 and terminate with the support units 37. The pole bodies 9, 11 are connected to the sheaths 12, for example screwed together, w ei three screws 13 per pole segment 11 (see. Fig. Lj pass through the jacket 12 and the pole ring 9 and anchored in the pole segments 11. Horizontal portions 38 of the pole rings 9 are in each case flat against the inside of the sheaths 12 '. The pole segments 11 are shaped so that the coils 5 can be easily attached and fixed by means of the horizontal portion 38 of the respective pole ring 9 on the pole segments 11. Both coats 12 have a removable central part 39, which closes off in the manner of a cover, the respective jacket 12 from above or below the center. In the middle part 39, the distance sensors 34 are arranged, which extend within the shell 12 to just below the respective thrust bearing plate 32, 33. The nominal distance between the distance sensors 34 and the thrust bearing plates 32, 33 corresponds approximately to the nominal distance between the pole faces 16, 17 and the thrust bearing plates 32, 33.
    In Fig. 5 with a device 1 in Fig, 1 comparable device 40 is shown, which in addition to the two opposite bearing branches 3, 4 has a central bearing arm 41 with an annular coil 42 (hereinafter called annular coil 42). The illustrated section transverse to the axis of rotation 8 corresponds to the line VV in Fig. 7. The toroidal coil 42 of the central bearing arm 41 (hereinafter also called central warehouse 41) surrounds a cylindrical inner pole 43 and in turn by an outer pole ring 44 around (not to be confused with the single common pole ring 9 of the opposing coils 5). A cylindrical inner contour of the toroid 42 promotes ease of manufacture and minimizes any eddy currents caused by rotation. Between the outer pole ring 44 of the annular coil 42 and the common pole ring 9 of the opposite outer bearing branches 3, 4, a distance 45 is provided in order to achieve a flow separation of the magnetic bearing branches 3, 4, 41. The magnetic circuit of the central bearing 41 formed by the ring pump 41, the inner pole 43 and the outer pole ring 44 is closed by its own plate part 46 of the axial bearing plate 32 (compare FIG. The inner pole 43 is essentially solid and has a central recess 47 on a side facing the axial bearing plate 32, which serves to receive fastening elements 48 projecting from the plate part 46 for fixing the plate part 46 to a shaft: 49.
    As can be seen in FIG. 6 with reference to the corresponding field lines 50 or aeguipotential lines, the central bearing 41 is a hybrid bearing, which has a permanent magnet 51 (in the form of a permanent magnetic section 51) of the inner pole 43 in addition to the electromagnet formed by the annular coil 42 and the permanent magnetic is superimposed on the electromagnetic flux. The permanent magnetic section 51 or permanent magnet 51 generates a parallel to the axis of rotation 35 aligned magnetic field, which can be amplified or attenuated by the electromagnet. The permanent magnet 51 is preferably designed so that its magnetic field carries the weight of the rotor at a nominal air gap alone. The applied by the permanent magnet 51 magnetic force FG corresponds to the product of the mass mRotor of the rotor with the acceleration due to gravity g: FG = mRo-tor'lg. As a result, a particularly high energy efficiency and safety can be achieved with little required tree space.
    The design of the annular coil 42 is such that hei maximum current density in the toroidal coil 42 both the increase and the reduction of the static force FG corresponding to a fraction of the total control force Fges, which depends on the number n of independently controllable thrust bearing branches 3, 4, 41 (Fges / n), is possible. The total control force Fges of all bearing branches 3, 4, 41 is preferably at least large enough to allow storage and stabilization of the structure in case of failure of a bearing branch 3, 4, 41 with the other bearing branches 3, 4, 41. For example, the total control force Fges may correspond to three times the gravitational force acting on the rotor, i. Fges = mRo-gate · (± 3g). In this case, the control force of the central, hybrid bearing branch 41 results as Fhybrld = FG + Fges / n, or in the case of three independent bearing branches 3, 4, 41 to Fhybrld = FG + Fges / 3, which means that at maximum current density in the toroid 42 can be either doubled or canceled depending on the direction of the current from the per 16 outgoing 16 manentmagnet 51 outgoing force. The exclusively electromagnetic, outer bearing branches 3, 4 are, analogous to the electromagnetic part of the hybrid bearing, designed so that the respective control force results in FEM = Fges / n.
    In order to achieve the most compact central storage 41 and a small diameter of the associated plate member 46, the cross section of the outer pole ring 44 and / or the annular coil 42 of the hybrid bearing 41 converges towards the pole face 52. Although the inner pole 43 of the toroidal coil 42 can basically be shaped to taper in the shape of a truncated cone to the axial bearing plate 32 or to the plate part 46, a cylindrical shape is preferred for this because of the simpler manufacture. In particular, the outer pole ring 44 of the hybrid bearing 41 can taper radially towards the axial bearing plate 32. Of course, the compact structure described for the hybrid bearing 41 can also be used without a permanent magnet 51, i. be used for a purely electromagnetic bearing branch (see Fig. 8).
    In Fig. 7, a device 53 is shown with a magnetically mounted shaft 49, and here - as in Fig. 4 - for simplicity, only the Axialmagnetlager 30, 54, but no radial bearings are shown and shortens the shaft 49, is shown with a schematic break 55. In the lower end region 56, the shaft 49 has a tapered section, onto which the lower axial bearing plate 33 is plugged and with the end face 57 of which a sensor plate 58 is connected. Between the thrust bearing plate 33 and the sensor plate 58, a spacer ring 59 is disposed of non-magnetic material. In addition, the shaft 49, at least in the region of the axial magnetic bearings 30, 54 made of non-magnetic material. In contrast to the device 27 shown in FIG. 4, the distance sensors 34 are not arranged opposite the thrust bearing plate 33, but opposite the sensor plate 58 provided for this purpose. The structure of the axial magnetic bearing 30, however, is otherwise identical, for which reason - to avoid repetition - in this regard Reference is made to the above statements. The upper end of the shaft 49 is mounted in a device 40 according to FIG. 5, wherein the view in FIG. 5 corresponds to a sectional view along 17/54 17 of the line V-V in Fig. 7. In the apparatus 40 shown here, an axially separate thrust bearing plate 32 is arranged at the upper end, which has two axially separated by a spacer ring 60 of non-magnetic material plate members 46, 61 to a decoupling of the magnetic fluxes or a flow separation of the magnetic branches. 3 , 4, 41 and a greater distance between the stator units, ie in this case between the outer bearing branches 3, 4 and the inner, central bearing branch 41 to achieve. Thus, any flow density gradients on rotation due to the control currents in the hybrid bearing can be minimized. As can be seen here, the central bearing branch 41 is arranged coaxially partially within or overlapping the two outer bearing branches 3, 4. The larger of the two plate parts 61, which is closer to the center of the shaft 49, is magnetically supported by the outer circumferentially successive bearing branches 3, 4 with opposite coils 5. The smaller diameter plate member 46 is disposed at the upper end of the shaft 49 and supported on a hybrid bearing of FIG. 5 and FIG. 6 forming the inner and central bearing arms 41, respectively. The hybrid bearing 41 consists of an outer pole ring 44, which encloses a toroid 42 of converging cross section. In the toroid 42, a solid cylindrical inner pole 43 is arranged, which is divided in the direction of the axis of rotation 35 into two soft magnetic portions 62 and the permanent magnetic portion 51 therebetween. The inner pole 43 is in contact with the outer pole ring 44 on a side of the annular coil 42 opposite the axial bearing plate 32.
    On the side of the pole faces 52, 63, the pole bodies 43, 44 are separated up to the plate part 46 by the toroid 42, d, h. one side of the annular coil 42 substantially terminates with the pole faces 52, 63.
    Between the bearing branches 3, 4, 41 of the upper axial magnetic bearing 54, a cavity 64 or spacing 45 (cf., Fig. 5) is provided in order to avoid stray flux and transverse effects between the bearing branches 3, 4, 41. The distance 45 between the outer pole ring 44 of the central hybrid bearing 41 and the inner joint Pölring 9 of the outer bearing branches 3, 4 is greater than the distance between the two pole bodies 9 and 11 and 43 and 44 of each bearing branch 3, 4, 41st The distance between the bearing branches 3, 4, 41 or the radial cross section of the cavity 64 decreases towards the plate parts 46, 61, since several bearing elements have a radius decreasing towards the plate parts 46, 61. The Axialmagnetläger 54 also has a flow separation between the outer bearing branches 3, 4 and the inner bearing arm 41, wherein the inner bearing arm 41 is a separate from the other plate members 61 plate member 46 of the thrust bearing plate 32 assigned.
    Comparable to the differential arrangement of the distance sensors 34 described in connection with FIG. 4, a differential evaluation of the measured distances is also conceivable in arrangements with hybrid bearings 41, for example with a distance sensor in the center of the hybrid bearing 41. For minimal required point energy in the hybrid bearing 41 the set position for "normal" Operating conditions chosen so that the permanent magnetic branch or the permanent magnet 51 of the hybrid bearing 41, the weight of the rotor (and any additional, acting on the rotor static forces) compensated. Here, zx is used as a setpoint for the control, as long as the rotor at the lower end is far enough away from the stator. For those operating cases in which the desired minimum distance between the rotor and the lower stator part is not given, for example, the rotor is brought into a position in which it has the same distance from the upper and lower stator sz, soii = sz, soi.i2 · Another possibility in the latter case is to bring the rotor into the position sz, soii = sz, soii2 'in which it has straight, for example as a distance from the lower stator. Thus, a lower static current through the coil 42 is required in the hybrid bearing 41 (see equations (2) to (4)). 19/54 (2) 19 sz, so Zi for z2 ^ zb with Zl + Z2 (2) 19 5 z, soll2 &quot; yz, soII '~ 2 for z2 <Zh or Z1 + Z2 ~ ZA 2 for zi <zb (3) (4) The sheath assembly 65, 66 of the device 40 is supported in a radially outer sheath 65 and optionally for the shielding of the segment bearing 67 formed by the outer bearing branches 3, 4, and a radially inner jacket 66 for carrying and optionally for shielding the hybrid bearing 41. The inner jacket 66 is arranged in a central opening 68 of the outer jacket 65 and projects beyond this accordingly. The height of the device 40, i. the extent in the direction of the axis of rotation 35, is greatest in the region of the hybrid bearing 41, on the one hand, the plate member 46 mounted on the hybrid bearing 41 axially offset from the bearing on the segment bearing 67 plate member 61 on the shaft 49 and on the other hand, the hybrid bearing 41 in the direction of As well as the common pole ring 9 of the segment bearing 67 is connected to the inner shell 66, the inner pole 43 of the hybrid bearing 41 is connected to the inside of the outer shell 66, in particular screwed. In this case, in addition to the connections 69 radially outside the annular coil 42, which connect the jacket 66 with the inner pole 43 and the outer pole ring 44, connections 70 are provided approximately at half the radius of the inner pole 43. These additional connections 70 serve to transfer the load of the rotor, which is always largely borne by the hybrid bearing 41 due to the permanent magnet 51, as directly as possible to the casing 66, in order to keep the mechanical load on the polar bodies 43, 44 low.
    In Fig. 8 is a similar device 71 as shown in Fig. 7, with the difference that here a central bearing branch or central warehouse 72 is used without a permanent magnet 51. The bearing forces must therefore always be exercised by the electromagnetic bearing branches 3, 4, 72. In order to minimize rotational losses due to magnetic reversals in the rotor part, only the central bearing 72 is preferably active with small forces required. Compared to the device 53 described above, this results in a lower efficiency of the central bearing 72, but it allows for lower production costs / because the supporting inner pole 73 of the central bearing 72 has no permanent magnetic section. The rest of the structure is identical to the device 53 described above, so reference is made here to avoid repetition of the above statements.
    The device 74 shown in Fig. 9 also has a great similarity with respect to the operation with the device 53 described in connection with Fig. 7. However, the outer bearing branches 3, 4 of the axial magnetic bearings 75, 76 here constructed differently in geometry ; only the common pole ring 9, which forms the radially inner, common pole, is unchanged. The radially inner portions 77 of the successive coils 78 are over the entire height of the pole ring 9, to the thrust bearing plate 33 and the plate member 61 on the radially outer side of the respective pole ring 9 and the end surfaces 79 of the coils 78 on the side of the thrust bearing plate 33 and the plate member 61 close with the pole face 16 of the pole ring 9 from. In addition, the cross section of the coils 78 converges toward the respectively assigned thrust bearing plate 33 and the plate part 61, wherein the dimension in the radial direction is smaller than the dimension in the axial direction. Arranged inside the coils 78 are pole ring segments 80 which have a decreasing radius and a converging cross section, the cross section of the pole ring segments 80 being approximately equal to that of the radially inner coil section 77. The same applies to the radially outer portions 81 of the coils 78, so that the coils 78 and the polar bodies 9, 80 in the radial cross-section fan-like manner from the thrust bearing plate 33 and the plate member 61 extend away, wherein each adjacent side surfaces of a polar body 9, 80 or a coil portion 77, 81 are not parallel in radial cross-section, but also divergent.
    The lower axial magnetic bearing 76 is constructed symmetrically to the outer bearing branches 3, 4 of the upper axial magnetic bearing 75 and differs from the lower axial magnetic bearing 30 described in connection with FIG the thrust bearing plate 33 is in contact. In this case, no spacer ring is provided between the sensor plate 82 and the thrust bearing plate 33.
    A further variant of a device 83 with a magnetically mounted to the invention Axialmagnetlagern 84, 85 shaft 49 is shown in Fig. 10. The elements and the basic structure of the axial magnetic bearings 84, 85 essentially correspond to the devices 27 and 53 described in connection with FIGS. 4 and 7, respectively, for which reason only the differences are discussed here and otherwise referred to the above explanations , The plate parts 86, 87 mounted on the outer bearing branches 3, 4 each have a rounded outer edge 88 on a side facing the shaft 49. The side surface on the radially outer sides of the outer pole ring 89 of the inner bearing branch 90 of the upper axial magnetic bearing 84: and the common pole rings 91 of the outer bearing branches 3, 4 deviate from a truncated cone shape and have a curved shape in cross-section, i. the contour of said polar bodies 89, 91 is not only composed of straight lines, but also follows higher order curves. As a result, the pole bodies 89, 91 are not strictly linearly convergent, but have a nonlinear taper. In addition, both the opposing coils 92 of the outer bearing branches 3, 4 and the annular coil 93 of the central bearing arm 90 on a side remote from the plate members 86, 87, 94 side edges 95, wherein the adjacent pole body 89, 91, 96, 97 ie the outer pole ring 89, the common pole rings 91, the inner pole 96 of the central bearing: 90 and the pole ring segments 97, are adapted to the rounded profile, so that no additional cavities between coils 92, 93 and Polkörpern 89, 91, 96, 97 arise. Likewise, the contact surface between the Polringsegmenten 97 and the respective common pole ring 91 is rounded. The illustrated and described rounding or the avoidance of edges advantageously supports the minimization of stray fields by the profiles of those elements which are part of a magnetic circuit, adapted to the course of the magnetic flux lines 22/54 22 s.
    [0046]; 11 shows a schematic block diagram 98 for illustrating a control circuit or method for controlling one or more axial magnetic bearings for stabilizing a rotor, for example in a device 53, 71, 74, 83 according to one of FIGS. 7 to 10. The block diagram 98 shows three independently operating and energized control units 99, 100, 101, wherein the first control unit 99 provides a single regulated output current Ii while the other two control units 100, 101 each provide two independently controlled output currents I2a, I2bf I3a / I3b. A control unit 99, preferably assigned to a central bearing branch, in particular a central hybrid bearing, can be equipped with a PID position controller 102, the other control units 100, 101 assigned to, for example, two outer bearing branches 3, 4 with a PDD for simplicity and robustness. Position controller 103 may be equipped with a subordinate P-current controller, as will be described in more detail below.
    The control units 100, 101 with two output currents are preferably designed to control two opposing bearing branches 3, 4. The control units 99, 100, 101 control the output currents Ii, 1.2a, I2b, 13a, 13b in response to a signal Si, S2, S3 of a respective position sensor 104 and a predetermined setpoint value Si, SQn, S2, soii, S3, soii of the respective Signal Su S2, S3, for example, the distance between the position sensor 104 and a sensor plate and the predetermined, desired distance.
    However, other sensors for detecting the actual state, for example current sensors or temperature sensors, may also be connected to the control units 99, 100, 101 together with the respectively applicable nominal values. The position sensors 104 are preferably arranged and evaluated in a differential sensor arrangement, as already explained in greater detail in connection with FIGS. 4 and 7.
    [Όo47] The sensor signals Si, S2, S3 may be passed to analog-to-digital converters after filtering and signal conditioning (e.g., anti-aliasing filters, level and offset adjustment). The corresponding signal processing can for example be integrated directly in a micro-controller, which can also integrate some 23/54 23 of the following units. The control unit 99 (the same applies analogously to the other control units 100, 101, which is expressed by the index i, which depending on the control unit considered the value 1, 2 or 3 anninxmt) determines a position deviation ei and gives them to a position controller 102, 103 further. In addition, in the case of the two further control units 100, 101, the position deviations e 1 in the threshold value switches 105 are evaluated. The two threshold switches 105 are connected to the position controllers 103 of the respective control unit 100, 101 and arranged to deactivate or activate the position controllers 103; i.e. if a threshold preconfigured in a threshold switch 105 is not exceeded, the associated: position controller 103 operates as if the position deviation ea were zero, i. sd = 0.
    The position controller 102 or 103 (when the threshold value of the threshold switches 105 is exceeded), determined from the obtained position deviation ei a required force Fi, son to possibly move the rotor back to a desired position. From this force Fi, sou and the measured position S ±, a conversion unit 106 determines the corresponding set currents 1 iä> söii / 1 ib, soii for the coils of the axial magnetic bearing. For this purpose, the conversion unit 106 uses a map I-; (F - ;, so ;;, S-;) of the coils or the bearing branches, which indicates the current as a function of the desired force action and the position of the rotor. The characteristic field Ii (Fi, sou, S ±) can be determined empirically in advance, for example, or calculated from the coil characteristics and the pole forms. The setpoint currents Iia, son, Iib.soii determined in this way are transmitted to a, n independent current regulation units 107, which are each assigned to an output current Ιχ or I2a, I2b or I3a, I3b.
    The current regulation units 107 have a difference unit 108, a current regulator 109, a limiter 110, a pulse width modulator 111, an H-bridge power converter 112, and a current sensor 113. The current sensor 113, in particular a Hall effect sensor, Hall effect sensor according to the flux compensation principle or a magneto-resistive sensor, measures e.g. in the case of the control unit 104, an output current I2a 24/54 24 of the current regulation units 107, so that the difference unit 108 can determine a current deviation eI # 2a between the output current I2a and the target current 12a / soll. The determined current deviation ei, 2a uses the current controller 109 to control the pulse width modulator 111, wherein the interposed limiter 110 ensures that, for example, a certain maximum current can not be exceeded. The pulse width modulator 111 generates a switching signal in a manner known per se, which controls the output current of the power converter 112. The control unit 99 with a single output current Ix for a single coil operates substantially identically, wherein the conversion unit 106 determines only a desired current Ii, Soii and the control unit 99 accordingly only has one current control unit 107.
    The control units 99, 100, 101 are each part of an Axiallägerzweig-control system, wherein in the ideal case, each control system has an independent power supply and its own sensors, in particular its own position sensor 104. As already described in connection with the design of the bearing forces, the bearing branches controlled by the independent control systems are preferably balanced in such a way that each bearing branch can apply the same maximum or minimum bearing force.
    In normal operation, for example, only one of the control unit 99 associated hybrid bearing be in use, with small disturbing forces without the other bearing branches, in particular without any segment bearings, can be compensated. In this context, a monitoring of certain operating conditions, for example with regard to exceeding a predefined maximum deflection and / or deflection speed, for example in the form of the threshold switch 105 may be set and be provided upon occurrence of such operating condition, an automatic activation of the respective bearing branch.
    Figures 12 to 14 show an advantageous three-segment hybrid bearing 114. As in particular in cross section perpendicular to the axis of rotation - as shown in FIG. 12 - recognizable, are the three coils 115 of the hybrid bearing 114, which each form an independent bearing branch , each other with respect to the rotation axis 116 opposite one another or arranged in the circumferential direction one behind the other and 25/54 25 surround a common pole body 117. As a result, a flow separation of the bearing branches is achieved. The arranged between the coil 115 portion of the pole body 117 is cylindrical and thus has a circularly closed perimeter, wherein the longitudinal axis of the cylinder is disposed substantially on the axis of rotation 116 of the rotor. Arranged inside the coils 115 are pole segments or pole ring segments 118, the contour of which corresponds to concentric circular arcs on a radial inner side and a radial outer side, the common center of which lies on the axis of rotation 116. Consequently, the turns of the coils 115 follow a circular arc-shaped course, which is closed by radial connecting portions 119 at the end faces of the pole ring segments 118 (see Fig. 12).
    In particular, in the cross section along the axis of rotation 116 of FIG. 13 (corresponding to the line XIII-XIII in Fig. 12), it can be seen that both the coils 115 and the Pölringseg- elements 118, for example, one to a thrust plate 120 hin. have converging cross section. The inner surface of each coil 115 is preferably arranged adjacent to the outer surface of the Polringsegments 118, so that the Polringsegment 118 and the radially outer coil portion 121 have a to the thrust bearing plate 120 toward decreasing radius. The radius of the thrust bearing plate 120 is slightly larger than the outer radius of the pole face 122 of the Polringsegments 118 and is thus smaller than the radius of the Polringsegments 118 in the coil 115, the Polringsegment 118 has a permanent magnet 123, whereby the hybrid bearing 114 in the non energized state of the coils 115 generates a magnetic field. An equipotential line 124 schematically shows the course of the magnetic circuit, which is closed via the thrust bearing plate 120. In contrast to previous illustrations, the arrow sizes are not proportional to the magnetic flux density. The line XII-XII in Fig. 13 indicates the axial position of the cross section shown in Fig. 12.
    The perspective view of the three-segment Hybridla-ger 114 in Fig. 14 shows the reason for the apparent in Fig. 12 distance 125 between the coils 115 in the circumferential direction: due to the converging coil cross-section fill the Spu- 26/54 26th len 115 below its top 126 not the entire distance between the parallel to the axis arranged end surfaces 127 of the Polringsegmente 118, since this distance depends on the maximum coil cross-section at the top 126. In order to generate a magnetic field which is as homogeneous as possible in the circumferential direction despite this distance and to avoid field gradients in the circumferential direction, the pole ring segments 118 have a position below the coil 115, i. in a region between the coil 115 and pole face 122 in the circumferential direction a projection 128. The length of the projection 128 corresponds approximately to the distance between the end surfaces 127 of the pole ring segments 118, so that no or only a minimal gap between the pole faces 122 arises with respect to low flow gradients in the rotating thrust bearing plate, or in terms of the best possible separation of the flows of the magnetic branches the greatest possible distance makes sense, a compromise between the achieved flow separation and the avoidance of re-magnetization losses is selected. On a side facing away from the thrust bearing plate 120 side of the common pole body 117 Monta-bores 129 for attachment of the hybrid bearing 114: provided on a jacket 130.
    In Fig. 15, a device 131 with a magnetically mounted shaft 132 with two axial magnetic bearings 30, 114 is shown. The lower axial magnetic bearing 30 corresponds to an arrangement already described in connection with FIG. 4, for which reason reference is made to earlier descriptions in this regard. The upper axial magnetic bearing 114 is a Pro i -Soqment.-ilybr i d i aqer 114 of FIG. 12 to 14, which is connected to a jacket 130, wherein the jacket 130 is mounted on a support unit 133. In this variant, the hybrid bearing 114 is adapted to carry the static load and to regulate accelerations of the rotor, the maximum negative force acting on the rotor by the bearing resulting in complete compensation of the permanent magnetic flux, thus in the best case correspondingly -lg effective Acceleration on the rotor. For larger negative accelerations, the lower axial magnetic bearing 30 is additionally activated. If the absolute value of the acceleration to be compensated by means of the axial bearing is smaller than the gravitational force acting on the rotor, the lower axial magnetic bearing 30 can be dispensed with. Fig. 16 shows a device 134 with a magnetically supported external rotor construction 135. The flywheel rotor 136 is mounted in a conventional manner on a plurality of radial magnetic bearings 137 and enclosed in a sheath 138. At the outer ends of the rotor 136 along the axis of rotation 139 each an annular thrust bearing plate 140 is arranged, each of which is in magnetic interaction with a built in principle similar to the bearing 29 of FIG. 4 axial magnetic bearing 141. The two Axialmagnetlager 141 are the same. Each Axialmagnetläger 141 has two with respect to the rotation axis 139 opposite or circumferentially successively arranged bearing branches 142, 143, each with a coil 144 and only a single common pole 145, which pole 145 is arranged radially outside of the bearing branches 142, 143. Accordingly, there is no magnetic material between the bearing branches 142, 143, so that a flow separation of the bearing branches 142, 143 is achieved. The common pole 145 is annular with an L-shaped cross section, wherein a side wall 146 is arranged substantially parallel to the axis of rotation 139 and a base 147 perpendicular to the axis of rotation 139. The side wall 146 has a cross-section converging towards the thrust bearing plate 140, wherein the outside 148 is substantially cylindrical. The coils 144 are disposed on the radially inner side of the side wall 146 and penetrated by pole segments 149. The pole segments or Polringsegmente 149 extend from the base 147 of the common pole 145 parallel to the axis of rotation 139 through the coil 144 through to the opposite side, where they expand radially outward and finally branches off at about 45 ° to the thrust bearing plate 140 out to form a circular ring-shaped pole face 150, which is arranged concentrically within and in a plane with a pole face 151 of the common pole 145. A portion 152 of the pole ring segments 149 is permanently magnetic or has a permanent magnet and thus generates a constant magnetic field even without current. Due to the profile of the common pole 145 and in particular the Polringsegmente 149, the thrust bearing plate 140 may have a small radial extent and surface perpendicular to the rotation axis 139, which is in particular smaller than the side surfaces of the coils 144 perpendicular to the axis of rotation 139. The coils have 144 in this example 28/54 28 has an approximately square cross-section, which allows easy production. The small surface of the thrust bearing plate 140 allows for particularly small overall dimensions, in particular a relatively large inner diameter, thereby allowing on the one hand easy assembly and on the other hand a large outer diameter of the inner mandrel 153, whereby its rigidity increases and thus higher rotor speeds below the first natural frequency of the cathedral are possible ,
    In Fig. 17, a device 154 is shown, whose basic structure has some similarity with the device 53 shown in Fig. 7 / why comparable parts are denoted by like reference numerals. The thrust bearing plate 32 at the upper end of the shaft 49 has two axially separate plate parts 46, 61, which are mounted in a Axialmagnetlager 155. Between the plate members 46, 61, a spacer ring 60 is disposed of non-magnetic material whose diameter is slightly smaller than that of the smaller of the adjacent plate members 46. The side surfaces of both plate members 46, 61 are cylindrical and parallel to the axis of rotation 35. The axial magnetic bearing 155 points two bearing branches 156, 157, which are arranged coaxially partially in one another or overlapping each other. The inner bearing branch 156 is formed by a hybrid bearing 41 and the outer bearing branch 157 by an annular bearing, hereinafter referred to as ring bearing 158. Accordingly, the upper, smaller plate member 46 of the axial bearing plate 32 is assigned to the hybrid bearing 41. The hybrid bearing 41 consists of an outer pole ring 44, which encloses an annular coil 42 with a rectangular cross-section. In the toroid 42, a solid cylindrical inner pole 43 is arranged, which is divided in the direction of the rotation axis 35 in two soft magnetic portions 62 and a permanent magnet 51 therebetween. The inner pole 43 is in contact with the outer, cylindrical pole ring 44 on a side of the annular coil 42 opposite the plate part 46. On the side of the pole faces 52, 63, the pole bodies 43, 44 are separated to the plate member 46 by the toroid 42, i. one of the thrust bearing plate 32 facing side of the annular coil 42 terminates substantially with the pole faces 52, 63 of the hybrid bearing 41 from. 29/54 29 The larger of the two plate parts 61 is mounted on the ring bearing 158, which has a single, concentric annular coil 159. The annular coil 159 surrounds an inner pole ring 160 and in turn is surrounded by a sweeter pole ring 161, wherein the two pole rings 160, 161 are connected to each other in an operative state of the annular bearing 158. Due to the concentric, completely annular structure of the annular bearing 158, the magnetic field generated for the storage of the associated plate member 61 has a continuous azimuthal homogeneous flux density and it can thus be achieved approximately we-belstromfreie storage.
    The profiles of the pole rings or pole shoes 160, 161 in this example have no lines inclined relative to the axis, but exclusively parallel or vertical lines, ie. There are generally given rectangular cross-sectional shapes. This does not change the basic functionality of the bearing shown and the advantage of such pole pieces 160, 161 lies above all in the simple and inexpensive production. Analogous to the device 53 shown and described in FIG. 7, the axial magnetic bearing 155 also has a flow separation between the bearing branches 156, 157, which is characterized by the complete separation of the bearings 41, 158 and at the same time subdivision of the axial bearing plate 32 into the plate parts 46, 61. and magnetic separation of the plate members 46, 61 is achieved. As can be seen particularly clearly in FIG. 17, the inner diameter of the outer bearing branch 157 or of the annular bearing 158 is greater than the outer diameter of the plate part 46 assigned to the inner bearing branch 156, so that a simple disassembly of the device 154 is achieved.
    Although in the preferred embodiments shown here, the specific Polformen has been described only in conjunction with a flow separation between two bearing branches, it is obvious to those skilled in the art that some of the advantages of the present invention can be achieved with only one bearing branch. In particular, the advantageously small dimensions of the thrust bearing plates can be achieved on the basis of the special pole shapes described here, regardless of whether one or more bearing branches are present. Accordingly, the invention relates to the compact pole forms even if only a single coil is used. In particular, this means quite generally those pole shapes of axial magnetic bearings, which have a linear or non-linear convergence in the direction of a Axiallagerplab te converging cross section and / or a decreasing from a coil to a thrust bearing radial pole spacing. 31/54
    权利要求:
    Claims (15)
    [1]
    1. An apparatus (40) for magnetic axial bearing of a rotor bearing a thrust bearing (32) in an axial magnetic bearing (54) with at least two independently controllable bearing branches (3, 4, 41), each having at least one sink ( 5, 42), characterized in that a magnetic flux separation of the bearing branches (3, 4, 41) is provided, wherein the flow separation consists in that at least two of the bearing branches (3, 4) are arranged sequentially in the circumferential direction and a single common pole (9), which has a circularly closed circumference, and which is arranged with the center on the axis of rotation: (35) of the rotor either radially inside or radially outside of the bearing branches (3, 4), wherein the coils (5) surrounded with the common pole (9) connected pole segments (11), and / or in that the thrust bearing plate (32) in at least two coaxial, each different position Branched (3, 4 and 41): associated plate members (46, 61) is divided, which are separated by a non-magnetic material, for example in the form of a spacer ring (60), wherein the plate members (46, 61) associated Bearing branches (3, 4 and 41) are arranged coaxially partially in one another or overlapping.
    [2]
    2. Device (40) according to claim 1, characterized in that: the common pole (9) has a single, continuous circular or annular pole face (16) and describe the coils (5) substantially with the pole face (16) concentric circular arcs ,
    [3]
    3. Device (40) according to claim 1 or 2, characterized in that the coils (5) in the circumferential direction substantially immediately follow one another.
    [4]
    4. Device (40) according to one of claims 1 to 3, characterized in that the pole segments (11) substantially with the pole face (16) of the common pole (9) concentric, circular arc-shaped pole faces (17).
    [5]
    5. Device (40) according to one of claims 1 to 4, characterized 32/54 32 characterized in that the pole faces (1317 of the pole segments: (11) in the circumferential direction substantially immediately adjoin one another.
    [6]
    6. Device (40) according to any one of claims 1 to 5, characterized in that in the partially interleaved or overlapping arranged bearing branches (3, 4 or 41), the inner diameter of an outer bearing arm (3, 4) is greater than that Outer diameter of an inner bearing branch (41) associated with the plate part (46) of the Axiallagerplätte (32).
    [7]
    7. Device (40) according to one of claims 1 to 6, characterized in that the distance between the inner and outer pole of at least one bearing branch (3, 4, 41) with increasing distance to the thrust bearing plate (32) becomes larger.
    [8]
    8. Device (43) according to one of claims 1 to 7, characterized in that the distance between the inner and outer contour of at least one pole piece (9, 11) in the direction of the axial bearing plate (32) decreases towards.
    [9]
    9. Device (114) according to one of claims 1 to 8, characterized in that the pole ring segments (118) below the coil (115), in particular in a region between the coil (115) and pole face (122), in the circumferential direction a projection ( 128), wherein the length of the projection (128) corresponds approximately to the distance (125) between the end surfaces (127) of the pole ring segments (118).
    [10]
    10. Device (134) according to one of claims 1 to 9, characterized in that the surface of the thrust bearing plate (140) in a plane perpendicular to the rotation axis (139) is smaller than the sum of the surfaces of the coils (144) and poles ( 145, 149) in a plane perpendicular to the axis of rotation (139).
    [11]
    11. Device (40) according to one of the claims 1 to 10, characterized in that an axial magnetic bearing (54) arranged an even number of symmetrically to the rotation axis (35), in the circumferential direction successive coils (5). 33/54 33
    [12]
    12. Device (ΊΟ) according to one of claims 1 to 11, characterized in that the Axialmagnetlager (54) at least one permanent magnet (51), preferably at least one hybrid magnet (43, 51) with a permanent magnet (51) and an electromagnet (43 ), having.
    [13]
    13. Device (40) according to one of claims 1 to 12, characterized in that at least one of the coils (5) has a thrust to the axial bearing plate (32) converging cross-section and / or decreasing radius.
    [14]
    14. Device (40) according to one of claims 1 to 13, characterized in that at least two position sensors (34, 104) are provided, which are each associated with different bearing branches (2, 3, 41).
    [15]
    15. A method for magnetic bearing of a rotor with a device (40) according to one of claims 1 to 14, characterized in that the coils (5, 42) by decoupled control systems (99, 100, 101) are driven and in case of failure of a coil (.5., 42), the remaining coils (42, 5) take over the storage and stabilization of the rotor. 34/54
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    同族专利:
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    法律状态:
    2018-09-15| MM01| Lapse because of not paying annual fees|Effective date: 20180122 |
    优先权:
    申请号 | 申请日 | 专利标题
    ATA50040/2013A|AT513498B1|2013-01-22|2013-01-22|Apparatus and method for magnetic axial bearing of a rotor|ATA50040/2013A| AT513498B1|2013-01-22|2013-01-22|Apparatus and method for magnetic axial bearing of a rotor|
    EP14706265.7A| EP2948689A1|2013-01-22|2014-01-17|Device and method for magnetically axially supporting a rotor|
    US14/762,688| US20150362015A1|2013-01-22|2014-01-17|Device and Method for Magnetically Axially Supporting a Rotor|
    PCT/AT2014/050017| WO2014113829A1|2013-01-22|2014-01-17|Device and method for magnetically axially supporting a rotor|
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