CN111022254B - Time-lag control method for tracking maximum power point of singular perturbation wind power generation model - Google Patents

Time-lag control method for tracking maximum power point of singular perturbation wind power generation model Download PDF

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CN111022254B
CN111022254B CN201911354431.7A CN201911354431A CN111022254B CN 111022254 B CN111022254 B CN 111022254B CN 201911354431 A CN201911354431 A CN 201911354431A CN 111022254 B CN111022254 B CN 111022254B
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wind power
power generation
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wind
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CN111022254A (en
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张艳
余振中
王逸之
陈丽换
杨忠
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Guodian Power Hunan Langshan Wind Power Development Co ltd
Shenzhen Luchen Information Technology Service Co ltd
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Jinling Institute of Technology
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    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F03MACHINES OR ENGINES FOR LIQUIDS; WIND, SPRING, OR WEIGHT MOTORS; PRODUCING MECHANICAL POWER OR A REACTIVE PROPULSIVE THRUST, NOT OTHERWISE PROVIDED FOR
    • F03DWIND MOTORS
    • F03D7/00Controlling wind motors 
    • F03D7/02Controlling wind motors  the wind motors having rotation axis substantially parallel to the air flow entering the rotor
    • F03D7/04Automatic control; Regulation
    • F03D7/042Automatic control; Regulation by means of an electrical or electronic controller
    • F03D7/043Automatic control; Regulation by means of an electrical or electronic controller characterised by the type of control logic
    • F03D7/045Automatic control; Regulation by means of an electrical or electronic controller characterised by the type of control logic with model-based controls
    • FMECHANICAL ENGINEERING; LIGHTING; HEATING; WEAPONS; BLASTING
    • F05INDEXING SCHEMES RELATING TO ENGINES OR PUMPS IN VARIOUS SUBCLASSES OF CLASSES F01-F04
    • F05BINDEXING SCHEME RELATING TO WIND, SPRING, WEIGHT, INERTIA OR LIKE MOTORS, TO MACHINES OR ENGINES FOR LIQUIDS COVERED BY SUBCLASSES F03B, F03D AND F03G
    • F05B2270/00Control
    • F05B2270/10Purpose of the control system
    • F05B2270/101Purpose of the control system to control rotational speed (n)
    • YGENERAL TAGGING OF NEW TECHNOLOGICAL DEVELOPMENTS; GENERAL TAGGING OF CROSS-SECTIONAL TECHNOLOGIES SPANNING OVER SEVERAL SECTIONS OF THE IPC; TECHNICAL SUBJECTS COVERED BY FORMER USPC CROSS-REFERENCE ART COLLECTIONS [XRACs] AND DIGESTS
    • Y02TECHNOLOGIES OR APPLICATIONS FOR MITIGATION OR ADAPTATION AGAINST CLIMATE CHANGE
    • Y02EREDUCTION OF GREENHOUSE GAS [GHG] EMISSIONS, RELATED TO ENERGY GENERATION, TRANSMISSION OR DISTRIBUTION
    • Y02E10/00Energy generation through renewable energy sources
    • Y02E10/70Wind energy
    • Y02E10/72Wind turbines with rotation axis in wind direction

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Abstract

The invention discloses a time-lag control method for tracking maximum power point of a singular perturbation wind power generation model, which considers the situation that the wind speed is lower than the rated wind speed, collects the related data of a wind power generator system and establishes a variable-speed variable-pitch wind power generatorThe nonlinear singular perturbation model is used for linearizing the wind power generation system model at a plurality of operating points aiming at the singular perturbation wind power generation model, then the nonlinear variable parameter model is adopted to approximate the nonlinear model of the wind power generation system, and the LPV technology and the H technology are adoptedAnd time lag control is carried out, so that the aim of tracking the maximum power point of the wind power generation system is fulfilled. The mathematical model created by the method is closer to the original physical system, more accords with the mechanism characteristics of the wind power generation system, improves the modeling precision, reduces the error caused by modeling, and greatly reduces the conservatism and the calculation complexity of the controller.

Description

Time-lag control method for tracking maximum power point of singular perturbation wind power generation model
Technical Field
The invention relates to the technical field of wind power generation, in particular to a time-lag control method for tracking the maximum power point of a singular perturbation wind power generation model, which is suitable for improving the wind energy capture efficiency.
Background
The singular perturbation model is a very common dynamic system model. The model is a main tool for describing the system behavior with multi-time scale dynamics, overcoming the rigid ill-condition problem brought by the multi-time scale and obtaining satisfactory control effect.
Since the wind power generation system contains both a mechanical part (i.e., a fan part) and an electromagnetic part (i.e., a motor part). The rate of change of the electromagnetic part is very rapid compared to the dynamically changing characteristics of the mechanical part, so the system has obvious double-time scale characteristics. The modeling of the wind power generation system ignores the electromagnetic dynamic characteristics of the motor part. Obviously, this inevitably leads to inaccurate modeling and difficulty in improving the control accuracy.
For a wind Power generation system, in order to improve the wind energy capture efficiency in a region lower than a rated wind speed, a variable-speed constant-frequency wind Power generator set generally adopts a Maximum Power Point Tracking (MPPT) control strategy. The MPPT adjusts the rotation speed of the wind wheel to track a certain function related to the wind speed, so that a high wind energy capture efficiency can be obtained. However, Zaiyu Chen et al have demonstrated thatThe article: chen Z, Yin M, Zou Y, et al. Maximum Wind Energy Extraction for Variable Speed Wind Turbines With narrow Dynamic Behavior [ J]IEEE Transactions on Power Systems,2016 (PP (99):1-2.), the wind turbine tracks slow dynamics in wind speed (namely low-frequency fluctuation components in the wind speed), and can further improve the capture efficiency of wind energy and reduce the mechanical load of the system. This conclusion provides a new concept and method for improving the efficiency of wind energy capture. According to this idea, the fast dynamics of the wind speed (i.e. the high frequency fluctuating components in the wind speed) can be used as external disturbances of the system. And HThe control method is an effective method for overcoming disturbance and improving the robustness of the system. In the current patent literature, the utilization of H does not existThe control method and the singular perturbation theory are used for realizing the technical method for tracking the maximum power point of the wind power generation system.
For MPPT control problems, many scholars design controllers by linearizing the nonlinear system at some point. However, since the natural wind speed changes in real time, the method for linearizing the system and designing the controller under the condition of fixed wind speed has great conservatism, and the controller has a small application range. In addition, intelligent control algorithms, such as neural network control, genetic control algorithms, fuzzy control algorithms, etc., may be employed. The intelligent control algorithm can better process the nonlinear characteristics of the system, only the calculation amount is large, the requirement on a computer is high, the calculation time consumption is large, the calculation error accumulation is easily caused in the computer, and finally the control effect of the system is not good enough.
Disclosure of Invention
The invention aims to provide a time-lag control method for tracking the maximum power point of a singular perturbation wind power generation model, wherein a mechanical part (a fan part) and an electromagnetic part (a motor part) of a wind power generation system are subjected to unified modeling, so that a mathematical model is closer to an original physical system and better accords with the mechanism characteristics of the wind power generation system, the modeling precision is improved, and errors caused by modeling are reduced; in addition, aiming at the singular perturbation wind power generation model, the LPV technology and the H are adoptedTime lag control, the goal of realizing maximum power point tracking of the wind power generation system。
In order to achieve the above purpose, with reference to fig. 1, the present invention provides a time lag control method for tracking a maximum power point of a singular perturbation wind power generation model, where the time lag control method includes:
s1: the method comprises the steps of taking the situation that the wind speed is lower than the rated wind speed into consideration, collecting relevant data of a wind driven generator system, and establishing a nonlinear singular perturbation model for a variable-speed variable-pitch type wind driven generator;
s2: select 5 operating points θjJ is 1,2, …,5, so that a set of vertices with the operation point constitutes a convex hull Θ, and Θ is Co { θ {12345There is a set of non-negative numbers α for any point θ, θ ∈ Θ, within the convex hull Θ j0, j ≧ 1,2, …,5, such that:
Figure BDA0002335510220000021
and is
Figure BDA0002335510220000022
S3: by at a plurality of operating points thetajLinearizing the nonlinear singular shooting model to obtain 5 linear time invariant singular shooting models;
s4: combining a given gamma and each operating point theta for 5 linear time invariant singular perturbation modelsjH is obtained by solving the matrix inequality through designRobust time lag controller Kjj) The closed-loop linear time invariant singular perturbation model is robust and stable, gamma is an index requirement on infinite norm of a system transfer function, namely infinite norm | G(s) | Y of the system transfer function is required<γ;
S5: at tkAt the moment, θ (t) is measuredk) And calculating a weight coefficient alphajSuch that it satisfies:
Figure BDA0002335510220000023
s6: at tkAt the moment, the controller of the original system is designed as follows:
Figure BDA0002335510220000024
s7: calculating a control input u (t) according to the following formulak):u(tk)=K(θ(tk) X (t-h), where K (θ (t)k) X (t-h) is the state variable of the singular perturbation model, t is time, h is time lag, the control input u (t) is calculatedk) The method is applied to the original nonlinear wind power generation system;
s8: let tk=tk+1And repeating the steps S5-S8 to control the wind power generation system in real time.
Compared with the prior art, the technical proposal of the invention has the obvious beneficial effects that,
(1) the double-time scale characteristics of the wind power generation system are fully considered, a singular perturbation method is adopted, the electromagnetic part and the mechanical part are modeled uniformly, and the modeling precision is improved.
(2) The method is characterized in that the wind power generation system model is linearized at a plurality of operating points, and then a Linear Parameter Varying (LPV) model is adopted to approximate to a nonlinear model of the wind power generation system, so that the conservatism of a controller can be greatly reduced, and the method is simple, convenient and effective and has limited calculation complexity; meanwhile, the LPV technology is essentially that flexible switching is realized by a weighted summation method in convex hulls formed by a plurality of operation points and surrounded by the operation points, so that the jitter problem caused by switching control is effectively avoided.
(3) Design HThe robust time-lag controller effectively improves the wind energy capture efficiency of the fan and makes full use of wind energy.
It should be understood that all combinations of the foregoing concepts and additional concepts described in greater detail below can be considered as part of the inventive subject matter of this disclosure unless such concepts are mutually inconsistent. In addition, all combinations of claimed subject matter are considered a part of the presently disclosed subject matter.
The foregoing and other aspects, embodiments and features of the present teachings can be more fully understood from the following description taken in conjunction with the accompanying drawings. Additional aspects of the present invention, such as features and/or advantages of exemplary embodiments, will be apparent from the description which follows, or may be learned by practice of specific embodiments in accordance with the teachings of the present invention.
Drawings
The drawings are not intended to be drawn to scale. In the drawings, each identical or nearly identical component that is illustrated in various figures may be represented by a like numeral. For purposes of clarity, not every component may be labeled in every drawing. Embodiments of various aspects of the present invention will now be described, by way of example, with reference to the accompanying drawings, in which:
fig. 1 is a flowchart of a method for MPPT control of a wind power system based on a singular perturbation modeling theory and a robust time lag control method of the present invention.
Fig. 2 is a schematic diagram comparing the tracking effect of the wind wheel rotating speed under the control of the robust time-lag control method and the optimal torque method of the invention.
Fig. 3 is a schematic diagram comparing the tracking effect of the wind wheel rotating speed under the control of the robust time-lag control method and the optimal torque method of the invention.
Detailed Description
In order to better understand the technical content of the present invention, specific embodiments are described below with reference to the accompanying drawings.
Example one
With reference to fig. 1, the invention provides a time lag control method for tracking a maximum power point of a singular perturbation wind power generation model, which specifically includes the following steps:
step 1: considering the situation that the wind speed is lower than the rated wind speed, determining numerical values of system parameters (a reduction ratio of a gearbox, the efficiency of the gearbox, the inertia moment of a fan, the inertia moment of a motor, the electromagnetic torque of a generator, the rigidity coefficient of a high-speed transmission shaft, the damping coefficient of the high-speed transmission shaft, the resistance of a stator, the stator inductance of d-axis and q-axis components, the number of pole pairs and magnetic flux), and establishing a singular perturbation model for the variable-speed variable-pitch type wind driven generator, wherein the singular perturbation model comprises the following steps:
Figure BDA0002335510220000041
Figure BDA0002335510220000042
Figure BDA0002335510220000043
Figure BDA0002335510220000044
Figure BDA0002335510220000045
wherein, ω isr(t) wind wheel speed, i represents gearbox reduction ratio, η represents gearbox efficiency, JrIs the fan moment of inertia, TrIs an air dynamic moment, omegag(t) motor speed, JgIs the moment of inertia of the motor, TH(T) is the high-speed shaft torque, Tg(t) is the electromagnetic torque of the generator, KgIs the rigidity coefficient of high-speed transmission shaft, BgIs the damping coefficient of high-speed drive shaft, and is a singular perturbation parameter, i ═ 0.01d(t)、Ld、ud(t) and iq(t)、Lq、uq(t) stator currents, inductances and voltages, respectively d-and q-axis components, RsIs the resistance of the stator and is,
Figure BDA0002335510220000046
p is the number of pole pairs, phimIs the magnetic flux.
Air dynamic moment TrIs described as
Figure BDA0002335510220000047
Where ρ is the air density, V (t) is the wind speed, R is the fan plane radius, the power coefficient CQ(λ) is approximated by a quadratic polynomial of the tip speed ratio λ (t): cQ(λ)=CQmax-kQ(λ(t)-λQmax)2,CQmaxIs the maximum moment coefficient, λQmaxRepresenting tip speed ratio, k, corresponding to the maximum moment coefficientQAre approximated coefficients.
Tip speed ratio λ (t) defines:
Figure BDA0002335510220000048
electromagnetic torque T of generatorg(T) is Tg(t)=pφmiq(t)。
Step 2: properly selecting 5 operating points
Figure BDA0002335510220000049
So that the set of vertices with the operation point constitutes a convex hull Θ, i.e., Θ ═ Co { θ }12345}. Then any one point in the convex hull may be represented by the operating point thetajIs shown, i.e. any theta e theta exists in a set of nonnegative numbers alphajNot less than 0, j is not less than 1,2, …,5, so that
Figure BDA00023355102200000410
And step 3: at the operating point
Figure BDA0002335510220000051
Calculating the electromagnetic torque of the corresponding generator
Figure BDA0002335510220000052
And air dynamic moment
Figure BDA0002335510220000053
So that the operating point θ can be obtained by the calculation of equation (3)jCorresponding to
Figure BDA0002335510220000054
Order to
Figure BDA0002335510220000055
δV(t)=V(t)-Vj
Figure BDA0002335510220000056
Figure BDA0002335510220000057
Linearizing the nonlinear singular shooting model to obtain:
Figure BDA0002335510220000058
where δ v (t) is taken as a perturbation, the coefficient matrix is as follows:
Figure BDA0002335510220000059
Figure BDA00023355102200000510
wherein the content of the first and second substances,
Figure BDA00023355102200000511
Figure BDA0002335510220000061
Figure BDA0002335510220000062
then the LPV singular perturbation model can be written:
marking
Figure BDA00023355102200000611
Then
Figure BDA0002335510220000063
Wherein
Figure BDA0002335510220000064
B(θj)=[B1j) B2]。
Known from step 2
Figure BDA0002335510220000065
And because of Bgqj)、Bqgj)、Bgdj)、Bdgj)、Brj)、Krvj) Is thetajSo for any theta e theta, there is a set of positive numbers alphaj> 0, j-1, 2, … 5 so that
Figure BDA0002335510220000066
Therefore, at any operation point theta epsilon theta, a linear variable parameter singular perturbation model can be obtained:
Figure BDA0002335510220000067
Figure BDA0002335510220000068
and 4, step 4: for a given gamma and operating point thetajJ-1, 2, … 5, design HRobust skew controller
Figure BDA0002335510220000069
Substituted into the system (8) to obtain
Figure BDA00023355102200000610
Wherein the content of the first and second substances,
Figure BDA0002335510220000071
to simplify notation, the coefficient matrix A (θ) is conditioned and proved in the matrix inequalityj) Abbreviated as a.
For known ε > 0, h > 0, if a 5 × 5 dimensional matrix P existsεSo that EεPεGreater than 0 true, 2 x 2 dimensional matrix Q,2 x 2 dimensional matrix R1Greater than 0,2 x 2 dimensional matrix R2The > 0 and 5 x 5 dimensional matrix H make the matrix inequality (13) true:
Figure BDA0002335510220000072
wherein
Figure BDA0002335510220000073
Figure BDA0002335510220000074
The closed-loop linear time invariant singular perturbation model (12) is robust and stable, and the gain coefficient of the controller is
Figure BDA0002335510220000075
Wherein
Figure BDA0002335510220000076
Is composed of
Figure BDA0002335510220000077
The generalized inverse matrix of (2).
Next, robust stability verification is performed to verify the reasonable effectiveness of the proposed control scheme.
(1) It was first demonstrated that the closed loop system is asymptotically stable with zero disturbance.
Let δ v (t) be 0
Figure BDA0002335510220000078
Defining the Lyapunov function (for simplification of notation, labeled X)t=X(t)):
Figure BDA0002335510220000079
Wherein the content of the first and second substances,
Figure BDA00023355102200000710
for Lyapunov function
Figure BDA00023355102200000711
Along the system (12) the time t is derived
Figure BDA0002335510220000081
It is known that
Figure BDA0002335510220000082
Figure BDA0002335510220000083
For both side integrals, one can derive
Figure BDA0002335510220000084
So that there are
Figure BDA0002335510220000085
(21) Can be obtained by substituting into the formula (17)
Figure BDA0002335510220000086
Figure BDA0002335510220000087
Figure BDA0002335510220000088
Because for any α, β ∈ RnAnd any symmetric positive definite n x n dimensional matrix H has
-2αTβ≤αTH-1α+βT
Then the matrix R is positively determined for an arbitrary 2 x 2 dimensional symmetry1And a 2 x 2-dimensional symmetric positive definite matrix R2All are provided with
Figure BDA0002335510220000089
Figure BDA00023355102200000810
It is known that
Figure BDA0002335510220000091
Then
Figure BDA0002335510220000092
Figure BDA0002335510220000093
Substituting into formula (22) to obtain
Figure BDA0002335510220000094
Removing the underlined part of the above formula to obtain
Figure BDA0002335510220000101
Further arranging the underline part out for recording
Figure BDA0002335510220000102
Then can be collated to obtain
Figure BDA0002335510220000103
According to Schur's theorem, the matrix inequality (13) can be used to know
Figure BDA0002335510220000104
In combination with the inequality (25), it is easy to know
Figure BDA0002335510220000105
It follows that the equilibrium point of the system (12) is asymptotically stable when the disturbance δ v (t) is 0.
(2) Next, it is proved that the system is robust under the condition of the matrix inequality (13) when δ v (t) ≠ 0.
Figure BDA0002335510220000106
Also using the Lyapunov function as (16)
Figure BDA0002335510220000111
For a function
Figure BDA0002335510220000112
Derivation of time t along the system (26)
Figure BDA0002335510220000113
Figure BDA0002335510220000114
Figure BDA0002335510220000115
Figure BDA0002335510220000116
Figure BDA0002335510220000117
Then there is a change in the number of,
Figure BDA0002335510220000118
by using Schur supplement theory, it can be seen from the condition (13)
Figure BDA0002335510220000119
The above inequality is equivalent to
Figure BDA0002335510220000121
The above inequality can be further converted into
Figure BDA0002335510220000122
Substituted into formula (27)
Figure BDA0002335510220000123
As is also known, the amount of oxygen present,
Figure BDA0002335510220000124
therefore, the first and second electrodes are formed on the substrate,
Figure BDA0002335510220000125
Figure BDA0002335510220000126
based on the demonstration of asymptotic stability, X can be knownt(∞) is 0. Now suppose Xt(0) When the inequality (29) is integrated on both sides, 0 is obtained:
Figure BDA0002335510220000127
namely, it is
Figure BDA0002335510220000128
It is apparent from this that
Figure BDA0002335510220000129
I.e., | | C (sE)ε-A(θ))-1B1(θ)||< gamma. The syndrome is two
By solving the matrix inequality (13), the gain factor of the controller can be obtained as
Figure BDA0002335510220000131
Wherein
Figure BDA0002335510220000132
Is composed of
Figure BDA0002335510220000133
The generalized inverse matrix of (2).
And 5: for the LPV singular perturbation model, at tkAt the moment, the parameter θ (t) is measuredk)=[ωr V ωg idiq]And calculating a weight coefficient alphajSuch that it satisfies:
Figure BDA0002335510220000134
step 6: at tkAnd (3) calculating the controller gain of the original wind power generation system:
Figure BDA0002335510220000135
and 7: calculating a control input u (t)k)=K(θk) X (t-h), using u (t)k) To the original nonlinear wind power generation system;
and 8: at tk+1And (5) repeating the steps 5-8 at any time.
Example two
In the embodiment, a CART3 blade wind turbine built by renewable energy laboratories (NREL) of the national department of energy is adopted as a research object. The parameters of the wind turbine are shown in table 1.
TABLE 1 aerogenerator parameters
Name (R) Symbol Numerical value Name (R) Symbol Numerical value
Optimum tip speed ratio λopt 5.8 Radius of fan R 20m
Optimum coefficient of wind energy utilization CPmax 0.467 Density of air ρ 0.98Kg/m3
Coefficient of gearbox η 1 Inertia of fan Jr 3.88Kg·m2
Inertia of motor Jg 0.22Kg·m2 Number of pole pairs P 3
Gear ratio i 43.165 Magnetic flux φm 0.4382wb
Damping coefficient of motor Bg 0.3Kg·m2/s Coefficient of stiffness of motor Kg 75Nm/rad
Stator d-axis inductor Ld 41.56mH Stator q-axis inductor Lq 41.56mH
Stator damping Rs 3.3Ω
With the parameter values in table 1, a nonlinear singular perturbation model can be established as follows:
Figure BDA0002335510220000136
Figure BDA0002335510220000137
Figure BDA0002335510220000141
Figure BDA0002335510220000142
Figure BDA0002335510220000143
then, the control method provided by the invention is used for controlling the wind power generation system, and compared with an optimal torque method, a tracking effect comparison graph of the rotating speed of the wind wheel can be obtained. As can be seen from FIG. 1, the tracking effect of the robust time-lag control method provided by the invention based on the singular perturbation method is more accurate. FIG. 2 is a tracking error contrast diagram, the tracking error of the wind wheel rotating speed obtained by the robust time-lag control method is smaller than the error of the optimal torque method, and the effectiveness and superiority of the method provided by the invention are further verified.
The robust time-lag control method and the optimal torque control are applied to control the wind driven generator, the simulation time is 500 seconds, the average wind energy capture efficiency of the two methods is calculated, and the result is shown in table 2. It is obvious from table 2 that, compared with the optimal torque control method, the robust time lag control method can achieve higher wind energy capture efficiency and has superiority.
TABLE 2 control effect comparison
Method of producing a composite material Mean windEfficiency of energy capture
Robust skew control 0.4496
Optimal torque control 0.4455
In this disclosure, aspects of the present invention are described with reference to the accompanying drawings, in which a number of illustrative embodiments are shown. Embodiments of the present disclosure are not necessarily defined to include all aspects of the invention. It should be appreciated that the various concepts and embodiments described above, as well as those described in greater detail below, may be implemented in any of numerous ways, as the disclosed concepts and embodiments are not limited to any one implementation. In addition, some aspects of the present disclosure may be used alone, or in any suitable combination with other aspects of the present disclosure.
Although the present invention has been described with reference to the preferred embodiments, it is not intended to be limited thereto. Those skilled in the art can make various changes and modifications without departing from the spirit and scope of the invention. Therefore, the protection scope of the present invention should be determined by the appended claims.

Claims (2)

1. A singular perturbation wind power generation model maximum power point tracking time lag control method is characterized by comprising the following steps:
s1: the method comprises the steps of taking the situation that the wind speed is lower than the rated wind speed into consideration, collecting relevant data of a wind driven generator system, and establishing a nonlinear singular perturbation model for a variable-speed variable-pitch type wind driven generator;
s2: select 5 operating points θjJ is 1,2, …,5, so that a set of vertices with the operation point constitutes a convex hull Θ, and Θ is Co { θ {12345There is a set of non-negative numbers α for any point θ, θ ∈ Θ, within the convex hull Θj0, j ≧ 1,2, …,5, such that:
Figure FDA0002774529020000011
and is
Figure FDA0002774529020000012
S3: by at a plurality of operating points thetajLinearizing the nonlinear singular shooting model to obtain 5 linear time invariant singular shooting models;
s4: combining a given gamma and each operating point theta for 5 linear time invariant singular perturbation modelsjH is obtained by solving the matrix inequality through designRobust time lag controller Kjj) The closed-loop linear time invariant singular perturbation model is robust and stable, and gamma is an index requirement on infinite norm of a system transfer function;
s5: at tkAt the moment, θ (t) is measuredk) And calculating a weight coefficient alphajSuch that it satisfies:
Figure FDA0002774529020000013
s6: at tkAt the moment, the controller of the original system is designed as follows:
Figure FDA0002774529020000014
s7: calculating a control input u (t) according to the following formulak):u(tk)=K(θ(tk) X (t-h), where K (θ (t)k) X (t-h) is the state variable of the singular perturbation model, t is time, h is time lag; will calculate the control input u (t)k) The method is applied to the original nonlinear wind power generation system;
s8: let tk=tk+1Repeating the steps S5-S8 to control the wind power generation system in real time;
in step S1, the nonlinear singular perturbation model is:
Figure FDA0002774529020000015
Figure FDA0002774529020000016
Figure FDA0002774529020000021
Figure FDA0002774529020000022
Figure FDA0002774529020000023
wherein, ω isr(t) wind wheel speed, i represents gearbox reduction ratio, η represents gearbox efficiency, JrIs the fan moment of inertia, TrIs an air dynamic moment, omegag(t) motor speed, JgIs the moment of inertia of the motor, TH(T) is the high-speed shaft torque, Tg(t) is the electromagnetic torque of the generator, KgIs the rigidity coefficient of high-speed transmission shaft, BgIs the damping coefficient of high-speed drive shaft, and is a singular perturbation parameter, i ═ 0.01d(t)、Ld、ud(t) and iq(t)、Lq、uq(t) stator currents, inductances and voltages, respectively d-and q-axis components, RsIs the resistance of the stator and is,
Figure FDA0002774529020000024
p is the number of pole pairs, phimIs the magnetic flux; air dynamic moment TrIs described as
Figure FDA0002774529020000025
Where ρ is the air density, V (t) is the wind speed, R is the fan plane radius, the power coefficient CQ(λ) is approximated by a quadratic polynomial of the tip speed ratio λ (t):
CQ(λ)=CQmax-kQ(λ(t)-λQmax)2,CQmaxis the maximum moment coefficient, λQmaxRepresenting tip speed ratio, k, corresponding to the maximum moment coefficientQIs an approximation coefficient; the tip speed ratio λ (t) is defined as:
Figure FDA0002774529020000026
electromagnetic torque T of generatorg(T) is Tg(t)=pφmiq(t);
In step S2, the 5 operation points θjExpressed as:
Figure FDA0002774529020000027
in step S3, the passing is at a plurality of operating points thetajThe method for linearizing the nonlinear singular shooting model to obtain 5 linear time invariant singular shooting models comprises the following steps:
s31: at the operating point
Figure FDA0002774529020000028
Calculating the electromagnetic torque of the corresponding generator
Figure FDA0002774529020000029
And air dynamic moment
Figure FDA00027745290200000210
Thereby calculating the operation point thetajCorresponding to
Figure FDA00027745290200000211
S32: order to
Figure FDA00027745290200000212
δV(t)=V(t)-Vj
Figure FDA00027745290200000213
Figure FDA00027745290200000214
Figure FDA00027745290200000215
Linearizing the nonlinear singular shooting model to obtain:
Figure FDA0002774529020000031
where δ v (t) is taken as a perturbation, the coefficient matrix is as follows:
Figure FDA0002774529020000032
Figure FDA0002774529020000033
in the formula, Bgqj)、Bqgj)、Bgdj)、Bdgj)、Brj)、Krvj) Is thetajThe affine function of (a) is,
Figure FDA0002774529020000034
Figure FDA0002774529020000035
Figure FDA0002774529020000036
s33: obtaining a linear variable parameter singular perturbation model:
s331: marking
Figure FDA0002774529020000041
z(t)=[δid(t) δiq(t)]T,u(t)=[δud(t) δuq(t)]TThen, then
Figure FDA0002774529020000042
Wherein
Figure FDA0002774529020000043
B(θj)=[B1j) B2];
S332: let there be a set of positive numbers α for any θ ∈ Θj> 0, j ═ 1,2, … 5 such that:
Figure FDA0002774529020000044
then at any operation point theta epsilon theta, the linear variable parameter singular perturbation model is transformed into:
Figure FDA0002774529020000045
Figure FDA0002774529020000046
in step S4, the method combines a given γ and each operation point θ for 5 linear time-invariant singular perturbation modelsjH is obtained by solving the matrix inequality through designRobust time lag controller Kjj) The process for making the closed-loop linear time-invariant singular perturbation model robust and stable comprises the following steps:
s41: for a given gamma and operating point thetajJ-1, 2, … 5, design HThe robust time lag controller is as follows:
Figure FDA0002774529020000047
substituting the linear variable parameter into the singular perturbation model to obtain
Figure FDA0002774529020000048
Wherein the content of the first and second substances,
Figure FDA0002774529020000049
s42: setting matrix inequality conditions and coefficient matrix A (theta) in the proving processj) Abbreviated as a;
for known ε > 0, h > 0, if a 5 × 5 dimensional matrix P existsεSo that EεPεGreater than 0 true, 2 x 2 dimensional matrix Q,2 x 2 dimensional matrix R1Greater than 0,2 x 2 dimensional matrix R2The following matrix inequality is established when the dimension H of the matrix is more than 0 and 5 multiplied by 5, the closed loop linear time invariant singular perturbation model is determined to be robust and stable, and the gain coefficient of the controller is
Figure FDA0002774529020000051
Wherein
Figure FDA0002774529020000052
Is composed of
Figure FDA0002774529020000053
Generalized inverse matrix of (1):
Figure FDA0002774529020000054
wherein:
Figure FDA0002774529020000055
Figure FDA0002774529020000056
2. the singularity perturbation wind power generation model maximum power point tracking time lag control method according to claim 1, wherein the related data of the wind power generator system comprise a gearbox reduction ratio, gearbox efficiency, fan inertia moment, motor inertia moment, electromagnetic torque of a generator, a rigidity coefficient of a high-speed transmission shaft, a damping coefficient of the high-speed transmission shaft, resistance of a stator, stator inductance of d-axis and q-axis components, the number of pole pairs and magnetic flux.
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