The invention relates to the field of operating methods for rotating electrical machines. It is based on a method for operating a rotating electrical machine in accordance with the precharacterizing clause of the independent claim.
High-power voltage converter circuits are used in many applications today. Such a converter circuit usually connects three voltage levels and is often used for operating rotating electrical machines, in particular in synchronous and asynchronous machines, which rotating electrical machines generally have three stator windings. In a conventional method for operating a rotating electrical machine, it is connected in terms of phase to such a converter circuit, having a DC voltage circuit, for connecting generally m voltage levels, where m≧2. In the case of a converter circuit for connecting typically three voltage levels, the DC voltage circuit is formed by a first capacitor and by a second capacitor which is connected in series with the first capacitor, the DC voltage circuit also having a first main connection at the first capacitor, a second main connection at the second capacitor and a subconnection formed by the two series-connected capacitors. Furthermore, the converter circuit for connecting three voltage levels comprises power semiconductor switches, which are generally interconnected. In relation thereto,
The selection of the corresponding switching state combinations takes place, for example, according to the known “direct torque control” (DTC) method, in which the latest actual value for the torque of the rotating electrical machine, the magnetic stator flux of the rotating electrical machine and the potential at the subconnection are initially in each case compared with an associated predetermined value range. The respectively predetermined value range is or can be time-variant and is usually determined by an upstream closed-loop control circuit from reference values for the torque of the rotating electrical machine, the magnetic stator flux of the rotating electrical machine and the potential at the subconnection. If a latest actual value now exceeds its associated predetermined value range, a switching state combination is selected from a table as a function of the preceding selected switching state combination such that the latest value resulting for this switching state combination could, if need be, again be within the associated value range, this not being guaranteed. In addition, a switching state combination is always only selected either with respect to the latest actual value for the torque, the magnetic stator flux or the potential when the associated value range is exceeded. The latest actual value for the torque, the magnetic stator flux and the potential is not considered jointly.
One problem with a method described above for operating a rotating electrical machine by means of the known “direct torque control” is the fact that there are typically a plurality of transitions between the preceding selected switching state combination and the latest selected switching state combination, these transitions being illustrated in
It is therefore the object of the invention to specify a method for operating a rotating electrical machine, by means of which the switching frequency of power semiconductor switches in a converter circuit, which is connected in terms of phase to the rotating electrical machine, for connecting m voltage levels can be reduced, where m≧2. This object is achieved by the features of claim 1. Advantageous developments of the invention are specified in the dependent claims.
In the method according to the invention for operating a rotating electrical machine, the rotating electrical machine is connected in terms of phase to a converter circuit, having a DC voltage circuit, for connecting m voltage levels, where m≧2. In accordance with the method, in one step (a) the phases of the converter circuit are connected to the DC voltage circuit in accordance with a selected switching state combination of switching states for power semiconductor switches in the converter circuit. According to the invention, the selection of this switching state combination takes place in the following further steps:
By means of steps (b) to (j), the optimum switching state combination is always advantageously selected on the basis of the preceding selected switching state combination and with respect to the number of transitions from the preceding selected switching state combination to the selected switching state combination and with respect to the respective predetermined value range for the torque of the rotating electrical machine and for the magnetic stator flux of the rotating electrical machine. The number of switching operations of the power semiconductor switches in the converter circuit can thus advantageously be reduced, and thus the switching frequency of the power semiconductor switches can be reduced. The reduced switching frequency results in less heat loss being produced in the power semiconductor switches, as a result of which the power semiconductor switches age more slowly and can be protected to a large extent against damage or destruction. In addition, the respective value ranges are overall adhered to more effectively.
In general, the method according to the invention thus makes it possible to predict the behavior of the rotating electrical machine over more than one sampling time for determined switching state sequences, the horizon of N sampling times being shifted through one sampling time by step (j), after the application of steps (a) to (i), and then, however, always only the first switching state combination, in particular the k-th switching state combination, of a switching state sequence being selected. A quality criterion then approximates or simulates the switching frequency.
Finally, in the method according to the invention, the switching state combinations are also considered jointly with respect to all of the relevant variables, in particular the torque and the magnetic stator flux, when the associated value range is exceeded.
These and further objects, advantages and features of the present invention will be disclosed in the description detailed below relating to preferred embodiments of the invention in conjunction with the drawing.
In the drawings:
The references used in the drawing and their significance are listed by way of summary in the list of references. In principle, identical parts are provided with the same references in the figures. The embodiments described represent examples of the subject matter of the invention and have no restrictive effect.
According to the method, the phases u, v, w of the converter circuit 2, which is generally a converter circuit 2 for connecting m voltage levels, are now connected, in a first step (a), to the DC voltage circuit 3 in accordance with a selected switching state combination SKa,k of switching states for the power semiconductor switches in the converter circuit 2. As has already been mentioned at the outset,
According to the invention, the selection of the abovementioned switching state combination SKa,k takes place in the following further steps:
In step (b), beginning with a starting sampling time k for a selectable number N of sampling times, all the permissible switching state combinations SKk, . . . , SKk+N−1 are determined at each of the N sampling times, preferably starting from the respectively preceding determined switching state combination SKk−1, where N≧1, and where the first preceding determined switching state combination SKk−1 is preferably the preceding selected switching state combination SKa,k−1, i.e. at sampling time k−1.
In step (c), switching state sequences SSK for each determined switching state combination SKk are formed at the starting sampling time k, each switching state sequence SSK being an arrangement of determined switching state combinations SKk, . . . , Skk+N−1 of the N sampling times next to one another in a row, said switching state combinations SKk, . . . , Skk+N−1 being associated with the respective switching state combination SKk at the starting sampling time k. As can be seen in the illustrations, such a switching state sequence SSK represents, by way of example, a series of possible switching state combinations SKk, . . . , Skk+N−1 in accordance with
In step (d), for each of the switching state sequences SSK, a torque trajectory M of the rotating electrical machine 1 and a magnetic stator flux trajectory φ of the rotating electrical machine 1 is then calculated from determined state value sets Xa,k, . . . , Xe,k+N of the rotating electrical machine and the converter circuit for the starting sampling time k up to the sampling time k+N. Each of the abovementioned determined state value sets Xe,k, . . . , Xe,k+N contains, for example, two stator flux values φeS1,k, . . . , φeS1,k+N; φeS2,k, . . . , eS2,k+N, two rotor flux values φeR1,k, . . . , φeR1,k+N; φeR2,k, . . . , φeR2,k+N and possibly a speed value Ve,k, . . . , Ve,k+N. In order to determine the state value sets Xe,k, . . . , Xe,k+N, initially the two stator flux values φeS1,k; φeS2,k at the sampling time k, the two rotor flux values φeR1,k; φeR2,k at the sampling time k and possibly the speed value Ve,k at the sampling time k are determined, for example, by measurement or estimation, these values forming the state value set Xe,k at the sampling time k. From the state value set Xe,k at the sampling time k, trajectory values MT,k; φT,k at the sampling time k of the torque trajectory M and the magnetic stator flux trajectory φ are then calculated according to a calculation model known to those skilled in the art which describes or functionally simulates the electrical machine 1 and the converter circuit 2. Then, in accordance with the calculation model, the state value set Xe,k+1 at the sampling time k+1 is determined by calculation as a function of the state value set Xe,k at the sampling time k and as a function of the determined switching state combinations SKk at the sampling time k of the associated switching state sequence SSK and, from this, the trajectory values MT,k+1; φT,k+1 at the sampling time k+1 of the torque trajectory M and the magnetic stator flux trajectory φ are then calculated. The calculation of the state value sets Xe,k+2, . . . , Xe,k+N for the sampling times k+2 to k+N takes place in analogy to the above-explained calculation of the state value set Xe,k+1, in which case, for each calculation of the state value sets Xe,k+2, . . . , Xe,k+N, in each case the associated preceding calculated state value sets Xe,k+1, . . . , Xe,k+N−1 and the determined switching state combinations SKk+1, . . . , Skk+N−1 at the sampling time k+1 l to k+N−1 of the associated switching state sequence SSK are used. The calculation, following from the state value sets Xe,k+2, . . . , Xe,k+N, of the trajectory values MT,k+2, . . . , MT,k+N; φT,k+2, . . . , φT,k+N for the sampling times k+2 to k+N likewise takes place in analogy to the above-described calculation of the trajectory values MT,k; φT,k; MT,k+1; φT,k+1 for the sampling times k and k+1. Owing to the above-described calculation of the trajectory values MT,k, . . . , MT,k+N; φT,k, . . . , φT,k+N, said torque trajectory M of the rotating electrical machine 1 and a magnetic stator flux trajectory φ of the rotating electrical machine 1 result for each switching state sequence SSK, a schematic profile being shown in
In the further step (e), the switching state sequences SSKa are then selected in which an associated torque trajectory M and a magnetic stator flux trajectory φ at the (k+N)-th sampling time are in each case within a predetermined value range. Based on the torque trajectories M shown in
In step (f), for each of the selected switching state sequences SSKa, the number of times n is thereupon determined until the extrapolation of the trajectory values MT,k+N−1, MT,k+N of the associated torque trajectory M or the trajectory values φT,k+N−1, φT,k+N of the magnetic stator flux trajectory φ with respect to the (k+N−1)-th sampling time and (k+N)-th sampling time is outside the respective predetermined value range, i.e. until one of the extrapolations leaves the respective predetermined value range first or crosses the boundaries of the respective predetermined value range. In
In addition, in step (g), for each of the selected switching state sequences SSKa, the total number of switching transitions s of the associated determined switching state combinations SKk, . . . , Skk+N−1 is determined.
Furthermore, in step (h), for each of the selected switching state sequences SSKa, a quality value c is calculated from the number of times n and the total number of switching transitions s. The quality value c is preferably calculated by dividing the total number of switching transitions s by the number of times n.
In a further step (i), that determined switching state combination SKk at the starting sampling time k is set as the selected switching state combination SKa,k with which the quality value c of the associated selected switching state sequence SSKa is at its smallest.
Finally, in step (j), the steps (a) to (i) are repeated, where k=k+1, i.e. the selection of the switching state combination SKa,k takes place, for k=k+1, in accordance with the sequence described above according to steps (a) to (i). N is constant for each of steps (a) to (j).
By means of steps (b) to (j) and, in particular, by means of the extrapolation, it is possible to predict the further behavior of the overall system, i.e. the rotating electrical machine 1 and the converter circuit 2 associated therewith and, accordingly, it is advantageously always possible to select the optimum switching state combination SKa,k on the basis of the preceding selected switching state combination SKa,k−1 and with respect to the number of transitions from the preceding selected switching state combination SKa,k−1 to the selected switching state combination SKa,k and with respect to the respective predetermined value range for the torque of the rotating electrical machine 1 and for the magnetic stator flux of the rotating electrical machine 1. It is thus advantageously possible to reduce the number of switching operations for the power semiconductor switches in the converter circuit 2 and thus to reduce the switching frequency of the power semiconductor switches. The power semiconductor switches advantageously generate less heat loss owing to the reduced switching frequency and, as a result, have a lower energy consumption such that the power semiconductor switches, as a result, age more slowly and can be protected to a large extent against damage or destruction.
Mention will be made of the fact that steps (a) to (j) can be implemented in the form of software and this software can then be loaded, for example, onto a computer system, in particular using a digital signal processor, and run on this computer system.
As mentioned above,
For m≧3, it is now possible, by means of the steps (b) to (j) and, in particular, by means of the extrapolation, to predict the further behavior of the overall system, i.e. the rotating electrical machine 1 and the converter circuit 2 associated therewith, and, accordingly, it is advantageously always possible to select the optimum switching state combination SKa,k on the basis of the preceding selected switching state combination SKa,k−1 and with respect to the number of transitions from the preceding selected switching state combination SKa,k−1 to the selected switching state combination SKa,k and with respect to the respective predetermined value range for the torque of the rotating electrical machine 1, for the magnetic stator flux of the rotating electrical machine 1 and for the m−2 potential at the m−2 subconnections NP. It is thus advantageously possible to reduce the number of switching operations for the power semiconductor switches in the converter circuit 2, as has already been mentioned, and thus to reduce the switching frequency of the power semiconductor switches.
In general, steps (b) and (c) are advantageously omitted in a step (k), and a switching state sequence SSK for the preceding selected switching state combination SKa,k−1 is formed, the switching state sequence SSK in this case being an arrangement of N preceding selected switching state combinations SKa,k−1 next to one another in a row and, in addition, the preceding selected switching state combination SKa,k−1 being set as the selected switching state combination SKa,k and finally step (d) is applied and steps (e) to (i) are omitted if the trajectory values MT,k, . . . , MT,k+N of the associated torque trajectory M and the trajectory values φT,k, . . . , φT,k+N of the associated magnetic stator flux trajectory φ with respect to the k-th sampling time up to the (k+N)-th sampling time are within the respective predetermined value range. For m≧3, in step (k), steps (b) and (c) are omitted and a switching state sequence SSK for the preceding selected switching state combination SKa,k−1 is formed, the switching state sequence SSK in this case being an arrangement of N preceding selected switching state combinations SKa,k−1 next to one another in a row, and, in addition, the preceding selected switching state combination SKa,k−1 being set as the selected switching state combination SKa,k and finally step (d) being applied and steps (e) to (i) being omitted if the trajectory values MT,k, . . . , MT,k+N of the associated torque trajectory M, the trajectory values φT,k, . . . , φT,k+N of the associated magnetic stator flux trajectory φ and the trajectory values UNP,k, . . . , UNP,k+N of associated m−2 potential trajectories UNP with respect to the k-th sampling time up to the (k+N)-th sampling time are within the respective predetermined value range. In this manner, computation time can be saved since steps (b) and (c) and steps (e) to (i) are omitted. It goes without saying that steps (b) to (i) are then applied and step (k) is not applied if the abovementioned criteria for the trajectory values MT,k, . . . , MT,k+N; φTk, . . . , φT,k+N; UNP,k, . . . , UNP,k+N are not fulfilled.
Mention will be made of the fact that step (k) can likewise be implemented in the form of software and this software can then be loaded, for example, onto a computer system, in particular using a digital signal processor, and run on this computer system.
It has proven to be advantageous for a linear extrapolation to be selected for the extrapolation of the trajectory values MT,k+N−1, MT,k+N of the torque trajectory M, and for a quadratic extrapolation to be selected for the extrapolation of the trajectory values φT,k+N−1, φT,k+N of the magnetic stator flux trajectory φ. In this case, by selection of a quadratic extrapolation for the magnetic stator flux trajectory φ in combination with the selection of a linear extrapolation for the torque trajectory M, it becomes possible to predict particularly accurately the behavior of the overall system, with the result that the selection of the switching state combination SKa,k can be made even more precise and, as a result, a further reduction in the switching frequency of the power semiconductor switches results. As an alternative, for m≧3, in each case a linear extrapolation can be selected for the extrapolation of the trajectory values MT,k+N−1, MT,k+N of the torque trajectory M and the trajectory values UNP,k+N−1, UNP,k+N of the m−2 potential trajectories UNP, and a quadratic extrapolation can be selected for the extrapolation of the trajectory values φT,k+N−1, φT,k+N of the magnetic stator flux trajectory φ, in which case the same mentioned advantages result.
It is also conceivable for in each case a linear extrapolation to be selected for the extrapolation of the trajectory values MT,k+N−1, MT,k+N of the torque trajectory M and the trajectory values φT,k+N−1, φT,k+N of the magnetic stator flux trajectory φ, in which case, for m≧3, in each case a linear extrapolation is selected for the extrapolation of the trajectory values MT,k+N−1, MT,k+N of the torque trajectory M, the trajectory values φT,k+N−1, φT,k+N of the magnetic stator flux trajectory φ and, in addition, for the extrapolation of the trajectory values UNP,k+N−1, UNP,k+N of the m−2 potential trajectories UNP.
One further possibility consists in in each case a quadratic extrapolation being selected for the extrapolation of the trajectory values MT,k+N−1, MT,k+N of the torque trajectory M and the trajectory values φT,k+N−1, φT,k+N of the magnetic stator flux trajectory φ, in which case, for m≧3, in each case a quadratic extrapolation is selected for the extrapolation of the trajectory values MT,k+N−1, MT,k+N of the torque trajectory M and the trajectory values φT,k+N−1, φT,k+N of the magnetic stator flux trajectory φ, and, in addition, a linear extrapolation is selected for the extrapolation of the trajectory values UNP,k+N−1, UNP,k+N of the m−2 potential trajectories UNP.
| Number | Date | Country | Kind |
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| 04405767 | Dec 2004 | EP | regional |
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| 4763060 | Takahashi | Aug 1988 | A |
| 20050209045 | Lewis | Sep 2005 | A1 |
| Number | Date | Country |
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| 0 812 059 | Dec 1997 | EP |
| 2 791 488 | Sep 2000 | FR |
| 9953607 | Oct 1999 | WO |
| Number | Date | Country | |
|---|---|---|---|
| 20060125435 A1 | Jun 2006 | US |