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 adopted∞Time 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 {1,θ2,θ3,θ4,θ5There 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:
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 design∞Robust time lag controller Kj(θj) 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:
s6: at tkAt the moment, the controller of the original system is designed as follows:
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 H∞The 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.
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:
wherein, ω is
r(t) wind wheel speed, i represents gearbox reduction ratio, η represents gearbox efficiency, J
rIs the fan moment of inertia, T
rIs an air dynamic moment, omega
g(t) motor speed, J
gIs the moment of inertia of the motor, T
H(T) is the high-speed shaft torque, T
g(t) is the electromagnetic torque of the generator, K
gIs the rigidity coefficient of high-speed transmission shaft, B
gIs the damping coefficient of high-speed drive shaft, and is a singular perturbation parameter, i ═ 0.01
d(t)、L
d、u
d(t) and i
q(t)、L
q、u
q(t) stator currents, inductances and voltages, respectively d-and q-axis components, R
sIs the resistance of the stator and is,
p is the number of pole pairs, phi
mIs the magnetic flux.
Air dynamic moment T
rIs described as
Where ρ is the air density, V (t) is the wind speed, R is the fan plane radius, the power coefficient C
Q(λ) is approximated by a quadratic polynomial of the tip speed ratio λ (t): c
Q(λ)=C
Qmax-k
Q(λ(t)-λ
Qmax)
2,C
QmaxIs the maximum moment coefficient, λ
QmaxRepresenting tip speed ratio, k, corresponding to the maximum moment coefficient
QAre approximated coefficients.
Tip speed ratio λ (t) defines:
electromagnetic torque T of generator
g(T) is T
g(t)=pφ
mi
q(t)。
Step 2: properly selecting 5 operating points
So that the set of vertices with the operation point constitutes a convex hull Θ, i.e., Θ ═ Co { θ }
1,θ
2,θ
3,θ
4,θ
5}. Then any one point in the convex hull may be represented by the operating point theta
jIs shown, i.e. any theta e theta exists in a set of nonnegative numbers alpha
jNot less than 0, j is not less than 1,2, …,5, so that
And step 3: at the operating point
Calculating the electromagnetic torque of the corresponding generator
And air dynamic moment
So that the operating point θ can be obtained by the calculation of equation (3)
jCorresponding to
Order to
δV(t)=V(t)-V
j,
Linearizing the nonlinear singular shooting model to obtain:
where δ v (t) is taken as a perturbation, the coefficient matrix is as follows:
wherein the content of the first and second substances,
then the LPV singular perturbation model can be written:
Wherein
B(θ
j)=[B
1(θ
j) B
2]。
Known from step 2
And because of B
gq(θ
j)、B
qg(θ
j)、B
gd(θ
j)、B
dg(θ
j)、B
r(θ
j)、K
rv(θ
j) Is theta
jSo for any theta e theta, there is a set of positive numbers alpha
j> 0, j-1, 2, … 5 so that
Therefore, at any operation point theta epsilon theta, a linear variable parameter singular perturbation model can be obtained:
and 4, step 4: for a given gamma and operating point theta
jJ-1, 2, … 5, design H
∞Robust skew controller
Substituted into the system (8) to obtain
Wherein the content of the first and second substances,
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:
wherein
The closed-loop linear time invariant singular perturbation model (12) is robust and stable, and the gain coefficient of the controller is
Wherein
Is composed of
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
Defining the Lyapunov function (for simplification of notation, labeled X)
t=X(t)):
Wherein the content of the first and second substances,
for Lyapunov function
Along the system (12) the time t is derived
For both side integrals, one can derive
So that there are
(21) Can be obtained by substituting into the formula (17)
Because for any α, β ∈ RnAnd any symmetric positive definite n x n dimensional matrix H has
-2αTβ≤αTH-1α+βTHβ
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
It is known that
Then
Substituting into formula (22) to obtain
Removing the underlined part of the above formula to obtain
Further arranging the underline part out for recording
Then can be collated to obtain
According to Schur's theorem, the matrix inequality (13) can be used to know
In combination with the inequality (25), it is easy to know
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.
Also using the Lyapunov function as (16)
For a function
Derivation of time t along the system (26)
Then there is a change in the number of,
by using Schur supplement theory, it can be seen from the condition (13)
The above inequality is equivalent to
The above inequality can be further converted into
Substituted into formula (27)
As is also known, the amount of oxygen present,
therefore, the first and second electrodes are formed on the substrate,
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:
It is apparent from this that
I.e., | | C (sE)
ε-A(θ))
-1B
1(θ)||
∞< gamma. The syndrome is two
By solving the matrix inequality (13), the gain factor of the controller can be obtained as
Wherein
Is composed of
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:
step 6: at tkAnd (3) calculating the controller gain of the original wind power generation system:
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:
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.