Abstract:
A magnetically journalled electrical drive comprises a magnetically journalled electrical machine with windings which are inserted in the stator or rotor for the production of the torque and the suspension force and an analog or digital electronic circuitry for control, regulation, monitoring and excitation of the magnetically journalled machine. The magnetically journalled machine is equipped in the stator or rotor with windings ( 24, 25, 26, 27 ) which are utilised via a corresponding excitation through the electronic circuitry both for the production of the suspension force and for the production of the torque.

Description:
The invention relates to a magnetically journalled electrical drive in accordance with the preamble of the independent patent claim. 
     BACKGROUND OF THE INVENTION 
     Magnetic journalling technology opens up fields of application of machine and apparatus construction with extremely high requirements on the speed of rotation region, the lifetime, the purity and the sealing tightness of the drive system—thus substantially fields of application which can not or can only with difficulty be realised using conventional journalling techniques. Various embodiments, such as for example high speed milling and grinding spindles, turbocompressors, vacuum pumps, or pumps for chemical or medical products of high purity are already being equipped with magnetic bearings. 
     A conventional magnetically journalled electrical machine (FIG. 1) requires, in addition to a machine unit  1 , two radial magnetic bearings  2  and  3  respectively, an axial magnetic bearing  4 , two mechanical interception bearings  5  and  6  respectively and a total of thirteen power controllers  7 ,  8 ,  9  and  10  for the excitation of the motoric and magnetic bearing loops. 
     There are proposals (FIG. 2) in the literature for integrating machine and radial magnetic bearings in a magnetic stator unit. Two separate winding systems  11  and  12  for the torque and suspension force winding are inserted into multiply layered into grooves in a stator. Both winding systems are three-looped and differ by one in the number of pole pairs. The coils are distributed over a plurality of grooves. The example of FIG. 2 shows: 
     a four-pole machine winding  11  (outside): first loop  13 , second loop  14 , third loop  15   
     a two-pole suspension winding  12  (inside): first loop  16 , second loop  17 , third loop  18 . 
     The arrows (without reference symbols) from the rotor in the direction towards the stator or from the stator in the direction towards the rotor stand for the direction of the magnetisation of the four magnetic rotor segments (e.g. radial or diametral magnetisation). 
     In applications which require no rigid-axis rotor guidance, such as for example in ventilators, fans, pumps or mixers, the axial magnetic bearing and the second radial magnetic bearing can be omitted from the integrated machine-magnetic-bearing embodiment. A prerequisite for this is a disc-shaped embodiment of the rotor with a length dimension (FIG. 3) which is small with respect to the rotor diameter. Thus a passive stabilization of the rotor position in the axial direction and the tilt directions can be achieved via the magnetic traction  41  between the stator  39  and the rotor  40 . 
     In many cases however the complicated and expensive system construction and therewith the higher manufacturing costs stand in the way of the technical use of magnetic journalling. The object of the invention consists therefore in the simplification of the mechanical construction of the machine and magnetic bearing unit taking into consideration the electronic excitation which is suitable for this. 
     SUMMARY OF THE INVENTION 
     A magnetically journalled electrical drive comprises a magnetically journalled electrical machine with windings which are inserted in the stator or rotor for the production of torque and the suspension for it. An analog or digital electronic circuitry is used for control, regulation, monitoring, and excitation of the magnetically journalled machine. The magnetically journalled machine is equipped in the stator with windings which are utilized via a corresponding excitation through the electronic circuitry, both for the production of the suspension force for the rotor and for the production of torque. The rotor is of a type generating its own magnetic flux. 
     Of particular advantage in the solution of the object in accordance with the invention is the considerably simplified stator or rotor construction respectively and the winding construction of the magnetically journalled machine with respect to previously known solutions as well as the saving of power controllers. 
    
    
     BRIEF DESCRIPTION OF THE DRAWINGS 
     Exemplary embodiments of the invention are explained in the following with reference to the drawings. Shown in schematic illustration are: 
     FIG. 1 is an exemplary embodiment of a conventional magnetically journalled electrical machine of the prior art, 
     FIG. 2 is an exemplary embodiment of a conventional magnetically journalled electrical machine in which the machine and the radial magnetic bearing are integrated into a magnetic stator unit of the prior art, 
     FIG. 3 is an exemplary embodiment of a magnetically journalled electrical drive in accordance with the invention, 
     FIG. 4 is the exemplary embodiment of FIG. 3 with an individual illustration of the first current component, which serves for the production of a torque (four-pole field), 
     FIG. 5 is the exemplary embodiment of the drive in FIG. 3 with an individual illustration of the second current component, which forms one of the two current components for the production of a radially acting suspension force (two-pole field), 
     FIG. 6 is the exemplary embodiment of the drive in FIG. 3 with an individual illustration of the third current component, which forms the other of the two current components for the production of a radially acting suspension force (two-pole field), 
     FIG. 7 is an exemplary embodiment of a bridge circuit for the excitation of the windings of the drive in accordance with FIG. 3, 
     FIG. 8 is an exemplary embodiment of the drive with fractionally pitched concentrated windings and with pronounced poles and auxiliary poles, 
     FIG. 9 is a technical winding variant of a drive which has three loops, 
     FIG. 10 is an exemplary embodiment of the drive in accordance with the invention with an asymmetric sheet metal cut in the region of the winding poles, 
     FIG. 11 is an exemplary embodiment of a drive with a disc-shaped rotor and passive stabilisation in the axial direction and in the tilt directions, 
     FIG. 12 is an illustration of the angle dependent force fluctuations in non-sinusoidal stator current layer distributions and non-sinusoidal excitation field distribution in the air gap, 
     FIG. 13 is an exemplary embodiment of a drive in accordance with the invention with an auxiliary magnet for ensuring the start-up in a motor operation with an alternating field. 
     FIG. 14 is an exemplary embodiment of a drive in accordance with the invention short-circuit rings which are arranged one-sidedly on the stator poles, 
     FIG. 15 illustrates coils connected together to form pole windings, 
     FIG. 16 demonstrates a possibility of the controlled rolling down of the rotor at the stator poles; 
     and, 
     FIG. 17 is an exemplary embodiment of a drive in accordance with the invention with a special shaping of the rotor magnets for achieving a sinusoidal excitation field distribution in the air gap. 
    
    
     DESCRIPTION OF THE PREFERRED EMBODIMENT 
     FIG. 3 shows an embodiment of an integrated machine-magnetic-bearing unit. In this, two separate winding systems with different numbers of pole pairs are not introduced into the stator, as in conventional embodiment in accordance with FIG. 2, but rather the functions of the torque and suspension force production are integrated in one winding system. This winding system is composed of individual pole windings  24 ,  25 ,  26 ,  27  which are distributed at the periphery. Since these pole windings, as will still be described in the following, are excited by separate current supplies, magnetic fields with different numbers of pole pairs can be realised in the air gap such as are required for the torque and suspension force production. It should also be mentioned here that a machine of this kind can be operated both as a motor and as a generator depending on the application. An arrangement in accordance with FIG. 3 is selected as an exemplary embodiment, of which the stator is formed of a sheet metal cut  19  with four pronounced poles  20 ,  21 ,  22 ,  23  and four concentrated pole windings  24 ,  25 ,  26 ,  27  and of which the rotor is formed of a four-pole permanent magnet rotor. In contrast to the embodiment of FIG. 2, the winding coils of a loop are not distributed over a plurality of grooves. Fractionally pitching for the reduction of the harmonic content of the voltage and current is not provided in the sheet metal cut  19 , but could take place through a shortening of the pole widths  28  (see FIG.  8 ), In the event of strong fractionally pitching it is favourable under certain conditions for the smooth running of the machine to largely close the large groove gap  29  which arises through shortening of the pole widths with a ferromagnetic auxiliary pole  86  (see FIG.  8 ), which can remain without a winding. For a better cooling the sheet metal cut  19  is for example fitted in an aluminium ring or aluminum cylinder respectively which surrounds it. 
     Referring to FIG. 15, a sinusoidal flux linking can also be achieved via a distribution of a plurality of coils (two are illustrated). In contrast to the previously known embodiments of magnetically journalled drives, the coils  57 ,  58  and  59 ,  60  are however, as illustrated e.g. in FIG. 15, connected together to pole windings  55  and  56  respectively with separate electronics connection  53   a ,  53   b  (together these form the connection  53 ) and  54   a ,  54   b  (together these form the connection  54 ) respectively. The distributed winding coils can be inserted into grooves or else realized as an iron-less air gap winding similarly to the bell anchor motors. FIG. 15 shows in an exemplary manner two of the total of four pole windings in accordance with FIG. 3 in a distributed embodiment rather than in a concentrated one. 
     In contrast to the embodiment in FIG. 2 there are no separate torque and suspension windings. Each of the four pole windings  24 ,  25 ,  26 ,  27  is responsible both for the torque production and the suspension force production. The realization of both functions can take place via a corresponding current excitation with three current components which are superimposed in the pole windings: 
     first current component (machine operation) for the production of a four-pole alternating field, 
     second and third component (magnetic bearing operation) for the production of a two-pole rotary field. 
     FIG. 4, FIG.  5  and FIG. 6 show these components in individual illustration for an arbitrarily chosen operating state of the magnetically journalled machine. The current layers of the eight pole winding cross-sections are the same in amount within a figure. Likewise the current directions in the single pole windings are mutually determined within a figure. When the sign of the current component changes, the current direction thus changes in all pole winding cross-sections of a figure. The amplitude and the sign of each current component can be set freely and independently of the other current components. A variation of the first current component therefore leads, as is made clear in FIG. 4, to the setting of the amplitude and the direction of a four-pole alternating field. This stands in interaction with the four-pole rotor and produces a torque. 
     In FIG. 5 the direction of the second current component is illustrated. One recognises that the pole winding cross-sections  24   a  and  27   b  as well as  25   b  and  26   a  cancel one another within a groove. The remaining pole winding cross-sections  24   b  and  25   a  as well as  26   b  and  27   a  thus act as one loop of a two-pole winding. 
     FIG. 6 shows the direction of the third current component  3 . The distribution of the current layer takes place in the same manner as in FIG. 5, however rotated by ninety degrees. With the second and third current component thus a two-pole rotary field can be built up and the radial suspension force can be set in magnitude and direction through the choice of the amplitude and phase of the two current components. 
     The determination of the individual current components takes place while taking into account the specified desired values and the actual values for example of the rotor position and speed of rotation, the rotor angle of rotation or torque after the evaluation of the sensor signals for the rotor position and rotor angle of rotation by means of an analog circuit or of a high speed computer unit. The signals of the current components are superimposed referred to pole windings, are amplified by means of a power electronic circuitry and supplied to the four pole windings  24 ,  25 ,  26 ,  27  via clocked switches or analog power amplifiers. A possible bridge circuit is given in FIG.  7 . Instead of the impression of a current an impression of the voltage can also take place taking into account the characteristic of the regulation path. 
     FIG. 9 shows a technical winding variant with three loops in which a separate loop (machine loop:  30   a ,  30   b ,  31   a ,  31   b ,  32   a ,  32   b ,  33   a ,  33   b ; first magnetic bearing loop:  34   a ,  34   b ,  35   a ,  35   b ; second magnetic bearing loop:  36   a ,  36   b ,  37   a ,  37   b ) is associated with each current component, with it being possible to connect the coils of a loop in series or in parallel. The superposition thus does not take place at the current level as in FIG. 3, but rather at the current layer or field level respectively. The position of the individual loop coils results from the observations on FIGS. 4 to  6 . The currents of the loops I-IV (loop I: pole winding  24 , loop II: pole winding  25 , loop III: pole winding  26 , loop IV: 
     pole winding  27 ) and of the loops I′-III′ (loop I′: windings  30 - 33 , loop II′: 
     windings  34 - 35 , loop III′: windings  36 - 37 ) can be conducted across into one another. 
     The following transformation relations hold for the chosen current direction symbols: 
     
       
         i I =i I′ ,−i II′ +i III′ ; i II =i I′ ,−i II′ ,−i III′ ; i III =i I′ ,+i II′ ,−i III′ ; i IV =i I′ ,+i II′ +i III′   
       
     
     The winding arrangement of FIG. 9 is more complicated and expensive in manufacture than the winding arrangement in FIG. 3, but requires only the electric excitation of three loops rather than four, however. Which arrangement is more favourable from the economical point of view must be considered on a case by case basis. Of technical interest under certain circumstances in the arrangement in FIG. 3 is the possibility of being able to freely associate the weighting between the first as well as the second and the third current components. Thus for example in an idling machine the total available winding cross-section is nearly entirely used for the production of suspension force or, respectively, in a machine which is unstressed in regard to suspension, nearly the entire winding cross-section is used for the production of a torque. In a winding arrangement in accordance with FIG. 9 such a free association is not possible, since for example during the idling of the machine only the winding cross-section of the suspension force winding is available. 
     The rotor type of the machine can in principle be chosen freely, in particular when the machine operation takes place via a rotary field instead of an alternating field. Usable are for example permanent magnet rotors, short-circuit cage rotors, rotors with an electrically highly conducting metal jacketing instead of the short-circuit cage or reluctance rotors with angle-dependent air gap variations. 
     In the event of insufficient fractionally pitching or distribution respectively of the windings and in the event of non-sinusoidal excitation field distributions, angle dependent radial force fluctuations  42 , such as are illustrated for example in FIG. 12, arise through the harmonic content of the air gap fields in the current excitation of the winding in accordance with FIG. 5 or FIG. 6 or, respectively, of the loops II′ or III′ in accordance with FIG. 9 with a constant current amplitude when the rotor is rotated. This effect should be taken into account in the current excitation of the windings in order to achieve a good operating behaviour. 
     An approximately sinusoidal excitation field distribution can be achieved in the use of permanent magnet rotors  85  for example through a shaping of the permanent magnets  82  with an angularly dependent air gap between the rotor and the stator  84  in accordance with FIG. 17. A diametral magnetisation of the permanent magnets also acts favourably with respect to a sinusoidal field distribution. The ferromagnetic rear contact or yoke of the rotor is designated by  83 . For reasons of cost it can however be advantageous to use concentrated windings and radially or diametrally magnetised magnets without a special shaping. 
     Since only an alternating field is available for the machine operation in the magnetically journalled machine in FIG. 3 or FIG. 9 respectively, an auxiliary torque is to be provided where appropriate at the time point of the start-up for overcoming the dead zone. This can for example be done through an asymmetrical sheet metal cut  38  in the region of the winding poles (FIG.  10 ). A further proposed solution (FIG. 13) provides one or more auxiliary magnets  43  which are arranged axially or radially with respect to the rotor, and which for example bring the four-pole permanent magnet rotor  50  into a favourable starting position  44  with the angle φ as a result of their drawing force. In the position  45  of the magnet pole boundary the starting torque would be zero with an arbitrarily high current. The winding poles are indicated by the positions  46 ,  47 ,  48  and  49 . In order to assist the drawing force the auxiliary magnets can additionally be provided with an iron yoke. 
     A change in the magnet pole position could also be produced through a rolling down of the rotor  66  at the end side of the air gap of the stator pole  65  which is controlled by the magnetic bearing part (FIG.  16 ). As a result of the different diameters there results in the rolling down a growing angular displacement between the magnet and stator poles so that the rotor can be rotated out of the dead zone in which a torque development is not possible. The midpoint movement of the rotor during the rolling down is represented by  67 . It may be necessary to provide means at the periphery of the rotor and/or stator for preventing a sliding between the rotor and the stator during the rolling down movement (e.g. use of materials with high frictional values, roughening of the surfaces, toothing, etc.) 
     A further proposed solution is illustrated in FIG.  14 . The stator poles are provided on one side with a short-circuit ring  52  so that as a result of the short-circuit currents a highly elliptical rotary field develops in the air gap instead of the alternating field. 
     In FIGS. 3,  4 ,  5 ,  6 ,  9 ,  10 ,  13 ,  14 ,  16  and  17  magnetically journalled machines with an inner rotor were illustrated in each case. There is also the possibility of operating the magnetically journalled machine in an outer rotor embodiment. For this the rotor is to be executed as a ring or a bell; the stator poles point outwards. 
     FIGS. 3,  4 ,  5 ,  6 ,  9 ,  10 ,  13 ,  14 ,  16  and  17  are to be considered as exemplary both with respect to the number of pole pairs for the torque and suspension force production and with respect to the loop number. Modified numbers of pole pairs can also be realized, with it being necessary for the condition p M =p ML ±1 to be fulfilled between the number of pole pairs pM for the machine operation and the number of pole pairs p ML  for the magnetic bearing operation. Through enlargement of the loop number and the number of bridge branches in the electronic power circuitry a rotary field machine can also be integrated in accordance with the invention into the magnetically journalled drive instead of the alternating field machine.