CN113708686A - Inertia identification method for permanent magnet synchronous motor driving system - Google Patents

Inertia identification method for permanent magnet synchronous motor driving system Download PDF

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CN113708686A
CN113708686A CN202111007182.1A CN202111007182A CN113708686A CN 113708686 A CN113708686 A CN 113708686A CN 202111007182 A CN202111007182 A CN 202111007182A CN 113708686 A CN113708686 A CN 113708686A
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inertia
extended
equation
permanent magnet
synchronous motor
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CN113708686B (en
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宋宝
杨承博
唐小琦
周向东
李虎
钟靖龙
姜茂文
李渝
张泽之
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Huazhong University of Science and Technology
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    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P21/00Arrangements or methods for the control of electric machines by vector control, e.g. by control of field orientation
    • H02P21/0003Control strategies in general, e.g. linear type, e.g. P, PI, PID, using robust control
    • H02P21/0007Control strategies in general, e.g. linear type, e.g. P, PI, PID, using robust control using sliding mode control
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P21/00Arrangements or methods for the control of electric machines by vector control, e.g. by control of field orientation
    • H02P21/13Observer control, e.g. using Luenberger observers or Kalman filters
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P21/00Arrangements or methods for the control of electric machines by vector control, e.g. by control of field orientation
    • H02P21/14Estimation or adaptation of machine parameters, e.g. flux, current or voltage
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P21/00Arrangements or methods for the control of electric machines by vector control, e.g. by control of field orientation
    • H02P21/14Estimation or adaptation of machine parameters, e.g. flux, current or voltage
    • H02P21/18Estimation of position or speed
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P21/00Arrangements or methods for the control of electric machines by vector control, e.g. by control of field orientation
    • H02P21/14Estimation or adaptation of machine parameters, e.g. flux, current or voltage
    • H02P21/20Estimation of torque
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P25/00Arrangements or methods for the control of AC motors characterised by the kind of AC motor or by structural details
    • H02P25/02Arrangements or methods for the control of AC motors characterised by the kind of AC motor or by structural details characterised by the kind of motor
    • H02P25/022Synchronous motors
    • HELECTRICITY
    • H02GENERATION; CONVERSION OR DISTRIBUTION OF ELECTRIC POWER
    • H02PCONTROL OR REGULATION OF ELECTRIC MOTORS, ELECTRIC GENERATORS OR DYNAMO-ELECTRIC CONVERTERS; CONTROLLING TRANSFORMERS, REACTORS OR CHOKE COILS
    • H02P2207/00Indexing scheme relating to controlling arrangements characterised by the type of motor
    • H02P2207/05Synchronous machines, e.g. with permanent magnets or DC excitation

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  • Power Engineering (AREA)
  • Control Of Electric Motors In General (AREA)

Abstract

The invention provides an inertia identification method of a permanent magnet synchronous motor driving system, which comprises the following steps: expanding the inertia into a new system state, and constructing an expanded mechanical motion equation; introducing an extended sliding mode observer technology into the field of inertia identification, and developing a novel extended sliding mode observer with time-varying feedback gain based on a constructed mechanical motion equation to identify inertia; an extended state observer is designed, and then required lumped disturbance information is provided for the novel extended sliding mode observer to ensure that the inertia is successfully estimated. The invention successfully applies the technology of expanding the sliding-mode observer to the field of inertia identification, and ensures the strong robust capability of the inertia identification process on noise interference; in addition, the method does not involve any matrix operation, and thus the computational burden is small. In general, the method provided by the invention has the characteristic of low computational burden while having excellent anti-noise interference performance.

Description

Inertia identification method for permanent magnet synchronous motor driving system
Technical Field
The invention relates to the field of motor driving, in particular to an inertia identification method of a permanent magnet synchronous motor driving system.
Background
The permanent magnet synchronous motor has the excellent characteristics of good reliability, large torque inertia ratio, high power density, high efficiency and the like, so the permanent magnet synchronous motor is widely applied in the industrial field. Meeting the requirement of high performance control is a key sign of the driving system of the modern permanent magnet synchronous motor, and the speed ring is an important factor for determining the performance of the driving system. Currently, some algorithms for improving the control performance of the speed ring cannot keep accurate inertia identification results, such as speed ring self-tuning and load torque observation. High precision inertia data is critical to ensure superior performance of these methods. Therefore, it is very important and necessary to accurately estimate the inertia of the drive system.
Inertia identification techniques can be largely divided into two main categories: offline identification and online identification. Offline identification techniques can only be used during drive system commissioning, and such methods are only applicable to fixed inertia systems. Compared with offline recognition, online recognition technology is widely concerned due to its applicability to more complex situations. Model reference adaptive method, recursive least square method and gradient algorithm are common inertia online identification algorithms, and are popular because of low calculation burden. However, these mentioned inertia online identification techniques do not take into account friction torques, which makes their estimation less accurate. Fortunately, the orthogonal principle based methods (I.Awaya, Y.Kato, I.Miyake, and M.Ito, "New motion control with inertia identification function using interference generator," in Proc.IECON, San Diego, CA, USA,1992, pp.77-81.) and the method based On optimal parameter estimation (L.Niu, D.Xu, M.Yang, X.Gui, and Z.Liu, "On-line inertia identification algorithm for PI parameter optimization in speed loop," IEEE ns.Power Electron, vol.30, No.2, pp.849-859, Feb.2015.) overcome the above deficiencies. It should be noted that conventional approaches based on the orthogonal principle are limited by the periodic speed limitation. Although the latest improved quadrature-principle-based approach (y. chen, m. yang, j. long, w. qu, d. xu, and f. blaabjerg, "a model only line controller parameter selected-tuning method vision variable-periodic inertia identification," IEEE trans. power electron, vol.34, No.12, pp.12165-12180, dec.2019.) overcomes this limitation, it cannot be used in drive systems that require or only allow unidirectional rotation. In contrast, the method based on optimal parameter estimation does not have these limitations. Meanwhile, the method has excellent robustness to noise interference. Despite the attractive advantages mentioned above of an optimal parameter estimation based approach, such an approach still faces challenges in practical applications: this method involves a large number of matrix operations, so that its industrial implementation is rather time-consuming.
Disclosure of Invention
The invention provides an inertia identification method of a permanent magnet synchronous motor driving system aiming at the technical problems in the prior art, which comprises the following steps:
step 1, expanding inertia into a new system state, and constructing an expanded mechanical motion equation of a permanent magnet synchronous motor driving system;
step 2, constructing a novel extended sliding-mode observer with time-varying feedback gain based on the extended mechanical motion equation;
and 3, constructing an extended state observer, estimating lumped disturbance information of the permanent magnet synchronous motor driving system, and providing the lumped disturbance information to the developed novel extended sliding mode observer so that the novel extended sliding mode observer can successfully identify the inertia of the permanent magnet synchronous motor driving system.
The invention provides an inertia identification method of a permanent magnet synchronous motor driving system, which expands inertia into a new system state and constructs an expanded mechanical motion equation; introducing an extended sliding mode observer technology into the field of inertia identification, and developing a novel extended sliding mode observer with time-varying feedback gain based on a constructed mechanical motion equation to identify inertia; an extended state observer is designed, and then required lumped disturbance information is provided for the novel extended sliding mode observer to ensure that the inertia is successfully estimated. The invention successfully applies the technology of expanding the sliding-mode observer to the field of inertia identification, and ensures the strong robust capability of the inertia identification process on noise interference; in addition, the method does not involve any matrix operation, and thus the computational burden is small. In general, the method provided by the invention has the characteristic of low computational burden while having excellent anti-noise interference performance.
Drawings
Fig. 1 is a flowchart of an inertia identification method for a driving system of a permanent magnet synchronous motor according to the present invention;
FIG. 2 is a schematic block diagram of a designed extended sliding-mode observer;
FIG. 3 is a schematic block diagram of an inertia online identification technique provided by the present invention;
FIG. 4(a) is a comparative simulation result of the inertia estimation technique, the model reference adaptive method, and the optimal parameter estimation-based method provided by the present invention in the absence of noise;
FIG. 4(b) is a comparative simulation result of the inertia estimation technique, the model reference adaptive method, and the method based on the optimal parameter estimation provided by the present invention in the presence of slight noise interference;
FIG. 4(c) is a comparative simulation result of the inertia estimation technique, the model reference adaptive method, and the method based on the optimal parameter estimation provided by the present invention in the presence of severe noise interference;
fig. 5 is a schematic diagram showing the comparison of the actual execution time of the inertia estimation technique and the method based on the optimal parameter estimation in the STM32F103 microprocessor.
Detailed Description
The following detailed description of embodiments of the present invention is provided in connection with the accompanying drawings and examples. The following examples are intended to illustrate the invention but are not intended to limit the scope of the invention.
Fig. 1 is a flowchart of an inertia identification method for a driving system of a permanent magnet synchronous motor according to the present invention, and as shown in fig. 1, the method includes: step 1, expanding inertia into a new system state, and constructing an expanded mechanical motion equation of a permanent magnet synchronous motor driving system; step 2, constructing an extended sliding mode observer with time-varying feedback gain based on the extended mechanical motion equation; and 3, constructing an extended state observer, estimating lumped disturbance information of the permanent magnet synchronous motor driving system, and providing the lumped disturbance information to the developed novel extended sliding mode observer so that the novel extended sliding mode observer can successfully identify the inertia of the permanent magnet synchronous motor driving system.
It can be understood that, based on the defects in the background art, the embodiment of the invention provides an online inertia identification technology for a permanent magnet synchronous motor driving system, which is resistant to noise interference and has low calculation burden. According to the method, inertia is firstly expanded to be a new system state, then the technology of the expanded sliding-mode observer is introduced into the field of inertia identification, a novel expanded sliding-mode observer with time-varying feedback gain is developed to identify the inertia, and finally an expanded state observer is constructed to provide required lumped disturbance information for the novel expanded sliding-mode observer so as to successfully estimate the inertia. The inertia identification technology provided by the invention solves the problem that the prior art cannot give consideration to both the anti-noise performance and the calculated amount, namely the inertia identification technology has low calculation burden while having excellent anti-noise performance.
In one possible embodiment, the step 1 of constructing the extended mechanical motion equation comprises the following steps:
the mechanical equations of motion for a permanent magnet synchronous motor drive system can be described as follows:
Figure BDA0003237616040000051
wherein ωmIs the rotational speed, B is the coefficient of viscous friction, J is the inertia, TlFor load torque, C is the Coulomb coefficient of friction, TeIs an electromagnetic torque.
Defining the reciprocal of inertia as J ═ 1/J, and expanding the reciprocal to a new system state, and then constructing an expanded mechanical motion equation based on equation (1) as follows:
Figure BDA0003237616040000052
wherein ,DLRepresents a lumped perturbation, which is defined as
Figure BDA0003237616040000053
djThe derivative of j is indicated.
Step 2, introducing the technology of the extended sliding-mode observer into the field of inertia identification, and developing a novel extended sliding-mode observer with time-varying feedback gain based on the mechanical motion equation constructed in the step 1 to identify inertia, wherein the specific method comprises the following steps:
an extended sliding mode observer for estimating inertia is developed based on the extended mechanical motion equation constructed in the step 1 as follows:
Figure BDA0003237616040000054
wherein
Figure BDA0003237616040000055
Respectively represent omegam,j,DLAn estimated value of (d); f is the feedback gain; u shapeESMORepresents a sliding mode observer signal, which is designed to:
UESMO=g·sign(S);(4)
wherein g is sliding mode switching gain; s is a slip form surface designed as
Figure BDA0003237616040000056
In order to determine the sliding mode switching gain g and the feedback gain f, the invention carries out the following specific design process:
first subtracting equation (2) from equation (3), the error equation of the extended sliding-mode observer can be derived as:
Figure BDA0003237616040000061
wherein
Figure BDA0003237616040000062
Figure BDA0003237616040000063
Figure BDA0003237616040000064
Let eD、ej and TeAre all bounded and define
Figure BDA0003237616040000065
Figure BDA0003237616040000066
Figure BDA0003237616040000067
Selecting a Lyapunov function as V ═ 0.5S2It is possible to obtain:
Figure BDA0003237616040000068
from equation (6), when the sliding mode switching gain g is designed to be
Figure BDA0003237616040000069
When we can derive
Figure BDA00032376160400000610
Is satisfied, which means that the sliding mode reachable condition is satisfied. Thus, after sliding mode has taken place, eωAnd derivatives thereof
Figure BDA00032376160400000611
Will converge to 0 in a finite time, i.e.
Figure BDA00032376160400000612
Then, equation (5) can be rewritten as:
Figure BDA00032376160400000613
from equation (7), one can obtain:
Figure BDA00032376160400000614
typically, the frequency of the inertia change is much lower than the sampling frequency of the drive system. Therefore, it can be reasonably considered that d is satisfied in a short time j0. Then, equation (8) can be rewritten as:
Figure BDA0003237616040000071
when feDIs controlled to be feDWhen the value is approximately equal to 0, the following can be obtained:
Figure BDA0003237616040000072
then, the analytical solution of equation (10) can be derived as:
Figure BDA0003237616040000073
where C is a constant, it can be seen that when fT is satisfiedeInertia estimation > 0Error ejWill asymptotically approach 0. Therefore, the invention designs the feedback gain as f ═ mTe(m > 0) to satisfy fTeIs greater than 0. It can be seen that the provided extended sliding-mode observer has a time-varying feedback gain, and the design ensures that the inertia estimation error gradually converges to 0. Notably, feDThe key point for the conclusion is that the value is approximately equal to 0, and fe can be ensured by selecting a proper value of mDSmall enough, i.e. able to ensure feD≈0。
In summary, the final expression of the extended sliding-mode observer provided by the present invention is:
Figure BDA0003237616040000074
wherein, T in the above formula (12)e and ωmIs provided by a permanent magnet synchronous motor driving system which is frequently adopted
Figure BDA0003237616040000075
So that the electromagnetic torque TeCan be calculated as Te=1.5Pnψfiq(PnIs a logarithm of poles,. psifIs a flux linkage, iqQ-axis current), the rotation speed ωmAnd obtaining through an encoder. Fig. 2 shows a schematic block diagram of the extended sliding-mode observer provided.
It should be noted that, after the sliding mode occurs, the rotation speed ω ismCan be described as
Figure BDA0003237616040000076
Therefore, equation (3) can be rewritten as:
Figure BDA0003237616040000077
combining equation (2) and equation (13), one can obtain:
Figure BDA0003237616040000081
wherein G ═ fTe,
Figure BDA0003237616040000082
It is noted that equation (14) can be equivalent to a low-pass filter with a cut-off frequency G, and the transfer function can be expressed as:
Figure BDA0003237616040000083
therefore, the inertia estimation effect of the designed extended sliding mode observer is equivalent to the output of a low-pass filter. This means that the extended sliding mode observer itself is designed with an equivalent low pass filter function, and therefore sliding mode buffeting can be suppressed without additional buffeting suppression.
It can be understood that, when the extended sliding mode observer is used for estimating and identifying the inertia of the driving system of the permanent magnet synchronous motor, see formula (12), wherein one important variable is lumped disturbance information of the driving system. The specific method for designing the extended state observer comprises the following steps:
to provide a real-time lumped disturbance estimate (i.e., to the extended sliding-mode observer developed in step 2)
Figure BDA0003237616040000084
) In order to ensure that the inertia is successfully identified, the invention designs a linear extended state observer. First, considering the lumped disturbance as a new system state, the following extended mechanical motion equation is obtained based on equation (1):
Figure BDA0003237616040000085
based on equation (16) above, the designed linear extended state observer can be expressed as follows:
Figure BDA0003237616040000086
wherein p is an expected pole of the extended state observer and satisfies p > 0. Considering that j is unknown, it is extended by the output of the sliding-mode observer
Figure BDA0003237616040000091
Instead, the final expression of the designed linear extended state observer is as follows:
Figure BDA0003237616040000092
in summary, a schematic block diagram of the provided inertia online identification technology can be obtained, as shown in fig. 3.
In order to verify the feasibility and the effectiveness of the inertia identification technology provided by the invention, a corresponding simulation model is set up for research, and the simulation model adopts
Figure BDA0003237616040000093
The vector control strategy of (1). In simulation, the robustness of the provided inertia identification technology to noise is evaluated, and a model reference self-adaption method and an optimal parameter estimation method are selected to compare the inertia identification technology provided by the invention. The relevant simulation parameters are set as follows: number of pole pairs Pn4; resistance Rs0.801 Ω; inductance L ═ 3.675 mH; rotor flux linkage psif0.278 Wb; the speed command is selected as a periodic square wave with an amplitude of 500r/min and a period of 0.1 s. In addition, the purpose of the simulation is to compare the noise-resistant performance of the three methods, and thus to eliminate the influence of other factors on the inertia recognition result, the viscous friction coefficient, the load torque, and the coulomb friction coefficient are all set to 0. The gain factor of the model reference adaptive method is chosen to be 0.001; observer in method based on optimal parameter estimationThe coefficient l is-0.06, and the initial value of the matrix P is designed to be P (0) ═ diag {0.2,0,0,0.1 }. The parameter design of the inertia identification technology provided by the invention is that m is 0.1, P is 20, and g is-1000. Fig. 4(a) is the estimation result under the noise-free condition, from which it can be found that the inertia can be accurately estimated by all three methods in the absence of noise. Fig. 4(b) is an estimation result under slight noise interference, it can be found that a model reference adaptive method has obvious errors, and the inertia can still be accurately estimated based on the method of optimal parameter estimation and the method provided by the present invention. When the drive system suffers from severe noise interference, fig. 4(c) shows that the model reference adaptive method estimates have diverged, while the other two methods only show slight errors. The results of fig. 4 illustrate that the noise immunity of the method provided by the present invention is comparable to the method based on optimal parameter estimation. In addition, fig. 5 compares the actual execution time of the method based on the optimal parameter estimation and the inertia estimation technique provided by the present invention in the driving system based on the STM32F103 microprocessor. It can be found that the actual execution time of the inertia identification technology provided by the invention is far lower than that of the method based on the optimal parameter estimation, which means that the invention has low calculation load while having excellent anti-noise performance.
According to the inertia identification method of the permanent magnet synchronous motor driving system provided by the embodiment of the invention, the inertia is expanded into a new system state, and an expanded mechanical motion equation is constructed; introducing an extended sliding mode observer technology into the field of inertia identification, and developing a novel extended sliding mode observer with time-varying feedback gain based on a constructed mechanical motion equation to identify inertia; an extended state observer is designed, and then required lumped disturbance information is provided for the novel extended sliding mode observer to ensure that the inertia is successfully estimated. The invention successfully applies the technology of expanding the sliding-mode observer to the field of inertia identification, and ensures the strong robust capability of the inertia identification process on noise interference; in addition, the method does not involve any matrix operation, and thus the computational burden is small. In general, the method provided by the invention has the characteristic of low computational burden while having excellent anti-noise interference performance.
While preferred embodiments of the present invention have been described, additional variations and modifications in those embodiments may occur to those skilled in the art once they learn of the basic inventive concepts. Therefore, it is intended that the appended claims be interpreted as including preferred embodiments and all such alterations and modifications as fall within the scope of the invention.
It will be apparent to those skilled in the art that various changes and modifications may be made in the present invention without departing from the spirit and scope of the invention. Thus, if such modifications and variations of the present invention fall within the scope of the claims of the present invention and their equivalents, the present invention is also intended to include such modifications and variations.

Claims (5)

1. An inertia identification method for a permanent magnet synchronous motor driving system is characterized by comprising the following steps:
step 1, expanding inertia into a new system state, and constructing an expanded mechanical motion equation of a permanent magnet synchronous motor driving system;
step 2, constructing a novel extended sliding-mode observer with time-varying feedback gain based on the extended mechanical motion equation;
and 3, constructing an extended state observer, estimating lumped disturbance information of the permanent magnet synchronous motor driving system, and providing the lumped disturbance information to the developed novel extended sliding mode observer so that the novel extended sliding mode observer can successfully identify the inertia of the permanent magnet synchronous motor driving system.
2. The inertia identification method according to claim 1, wherein the step 1 comprises:
the mechanical equation of motion of a permanent magnet synchronous motor drive system is described as follows:
Figure FDA0003237616030000011
wherein ,ωmIs the rotational speed, B is the coefficient of viscous friction, J is the inertia, TlFor load torque, C is the Coulomb coefficient of friction,TeFor electromagnetic torque, Te and ωmProvided by a permanent magnet synchronous motor driving system;
defining the reciprocal of inertia as J to be 1/J, expanding the inertia to a new system state, and constructing an expanded mechanical motion equation of the permanent magnet synchronous motor driving system as follows:
Figure FDA0003237616030000012
wherein ,DLIs lumped disturbance information of a permanent magnet synchronous motor driving system, which is defined as
Figure FDA0003237616030000021
djThe derivative of j is indicated.
3. The inertia identification method of claim 2, wherein the step 2 comprises:
constructing an extended sliding-mode observer for estimating inertia of a permanent magnet synchronous motor driving system:
Figure FDA0003237616030000022
wherein ,
Figure FDA0003237616030000023
respectively represent omegam,j,DLF is the feedback gain; u shapeESMORepresents a sliding mode observer signal, which is designed to:
UESMO=g·sign(S); (4)
where g is the sliding mode switching gain and S is the sliding mode surface, which is designed as
Figure FDA0003237616030000028
4. The inertia identification method of claim 3, wherein the step 1 further comprises determining a sliding mode switching gain g and a feedback gain f, comprising:
calculating an error equation of the extended sliding-mode observer:
Figure FDA0003237616030000024
wherein ,
Figure FDA0003237616030000025
let eD、ej and TeAre all bounded and define
Figure FDA0003237616030000026
Figure FDA0003237616030000027
Selecting a Lyapunov function as V ═ 0.5S2The following can be obtained:
Figure FDA0003237616030000031
according to equation (6), the gain g is designed to be when sliding mode switching
Figure FDA0003237616030000032
Can derive
Figure FDA0003237616030000033
Is satisfied, which means that the sliding mode accessibility condition is satisfied;
after the sliding form occurs, eωAnd derivatives thereof
Figure FDA0003237616030000034
Will converge to 0 in a finite time, i.e.
Figure FDA0003237616030000035
Equation (5) is rewritten as:
Figure FDA0003237616030000036
from equation (7), one can obtain:
Figure FDA0003237616030000037
wherein the variation frequency of the inertia is far lower than the sampling frequency of the driving system, and d is satisfied in a short timejThen equation (8) can be rewritten as:
Figure FDA0003237616030000038
when feDIs controlled to be feDWhen the value is approximately equal to 0, the following can be obtained:
Figure FDA0003237616030000039
the analytical solution of equation (10) can be derived as:
Figure FDA00032376160300000310
wherein C is a constant when fT is satisfiedeInertia estimation error e > 0jWill gradually go to 0, so the feedback gain is designed to be f mTe(m > 0) to satisfy fTe> 0, notably feDThe key point for the conclusion is that the value is approximately equal to 0, and fe can be ensured by selecting a proper value of mDSmall enough, i.e. able to ensure feD≈0;
Therefore, the final expression of the designed extended sliding-mode observer with time-varying feedback gain is as follows:
Figure FDA0003237616030000041
5. the inertia identification method of claim 2, wherein the step 3 comprises:
considering the lumped disturbance as a new system state, the following extended mechanical motion equation is obtained based on equation (1):
Figure FDA0003237616030000042
based on equation (13) above, the designed linear extended state observer can be expressed as follows:
Figure FDA0003237616030000043
where p is the desired pole of the extended state observer, satisfying p > 0, and is extended by the output of the sliding-mode observer given that j is unknown
Figure FDA0003237616030000044
Instead, the final expression of the designed linear extended state observer is as follows:
Figure FDA0003237616030000045
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CN106533291A (en) * 2016-08-31 2017-03-22 东菱技术有限公司 Inertia identification and load torque observation-based speed loop response improvement method
CN109347391A (en) * 2018-10-29 2019-02-15 江苏大学 A kind of adaptive method for identification of rotational inertia of Landau considering system noise
CN110557070A (en) * 2019-09-30 2019-12-10 山东深川变频科技股份有限公司 permanent magnet synchronous motor parameter identification method based on second-order sliding-mode observer
CN113406895A (en) * 2020-02-28 2021-09-17 南京理工大学 Method for constructing control system of intelligent valve electric actuator

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