86
.pdfChapter 1. Absolute stability and Aizerman’s problem of one-dimensional regulated systems
Since matrices |
A, |
A ( ), 0 |
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< |
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are Hurwitz matrices, then, by definition 1, |
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the trivial solution |
x(t) 0, |
t I of the system (1.1), (1.2) is absolutely stable. |
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When 0 |
= 0 , > 0 is an arbitrarily small number, then all the conditions |
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of definition 3 are satisfied, therefore, in the sector [0, |
0 |
] Iserman's problem has a |
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solution. The theorem is proved.
Iserman's problem. The question arises: is it possible to single out a class of controlled systems for which the Iserman problem has a solution without resorting to checking the conditions of absolute stability from Theorem 6?
Theorem 7. Let the following conditions be satisfied:
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1. |
Matrices A are Hurwitz matrices, function |
( ) |
0 |
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2. |
There is a row vector |
= ( 1, , n ) |
such as |
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n 2 |
B = 0, |
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B = 1; |
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B = 0, AB = 0, , A |
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= A |
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3. |
Matrix rank R = |
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*n 1 |
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is equal to |
n; |
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, A |
, , A |
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4. |
The conditions of Theorems 2-4 are satisfied, where N0 0, N1 0, N2 > 0, , Nn > 0. |
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Then in the sector [0, 0 |
] Iserman's problem has a solution, where 0 = 0 , |
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> 0 is an arbitrarily small number, the value 0 |
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is the limiting value of the Hurwitz |
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matrix |
A ( ) = A B S, |
0 |
0 |
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0 |
. |
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1 |
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Proof. Let the conditions of the theorem be satisfied. Then the improper integral |
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2 |
N y2 |
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y2 |
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I = |
( (t)) (t)dt = |
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N |
n |
]dt l = c, | l |< , | c |< , |
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1 |
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0 |
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1 1 |
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n |
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consequently,
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[N |
2 |
N y |
2 |
N |
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]dt = c1 l1 |
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| | l1 |< . |
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(1.29)
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By the hypothesis of the theorem N0 |
0, N1 0, , Nn |
> 0. |
Then from (1.29) |
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for |
N |
> 0 it follows that |
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1 |
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[N0 2 |
N1 y12 Nn yn2 ]dt < |
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(1.30) |
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0 |
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Further, repeating the proofs of Theorem 6, from (1.30) we have lim y(t) = 0. As |
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t |
(t) = 1 y1 (t) n yn (t), t I , |
then |
lim (t) = 0. Then |
lim |
( (t)) = 0 due to |
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t |
t |
21
Lectures on the stability of the solution of an equation with differential inclusions
continuity of the function |
( ). |
In this case, the value |
0 |
is determined from the |
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Hurwitz condition for the matrix |
A B S, consequently, |
0 |
= 0 . In the sector |
[0, 0 ] Iserman's problem has a solution
Consider the case when |
N = 0. |
In this case, inequality (1.30) can be written as |
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[N |
2 |
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(t) N |
2 |
(t)]dt < . |
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y |
(t) N y |
y |
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3 |
3 |
n |
n |
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0 |
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(1.31)
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It follows from (1.31) that |
lim |
y (t) = 0, , lim |
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y |
(t) = 0. |
From equation (1.30) |
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for |
t , |
we get |
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lim |
y (t) = lim |
y (t) = |
0, |
lim |
y |
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(t) = lim |
y |
(t) = lim |
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y (t) = 0, , |
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t |
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lim |
y |
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(t) = lim |
y |
(n 1) |
(t) = lim |
y |
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(t) = 0. |
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Let lim |
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y (t) = y |
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Then from the last |
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n 1 |
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t |
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t |
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1* |
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equation (1.4) for |
t , |
we get |
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0 = a |
y |
( |
* |
), |
where |
* |
= lim |
(t) = y |
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0 |
1* |
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t |
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1 1* |
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( |
* |
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. This is only possible when |
* |
= 0, y |
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= 0. Consequently, lim y(t) = 0 |
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0 |
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1* |
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t |
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and according to the proof above in the sector |
[0, |
0 |
] |
Iserman's problem has a solu- |
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tion. The theorem is proved. |
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It should be noted that the quantities |
Ni |
= Ni (a0 , , an 1 |
, 1, , n ), i = 0, n , |
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therefore, the fulfillment of inequalities N0 |
0, N1 |
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0, N2 |
> 0, , Nn |
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> 0 depends |
on the Hurwitz matrix
A
and vector
S = (s |
, , s |
). |
1 |
n |
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As
A = R |
* 1 |
* |
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AR |
A B S = R |
* 1 |
* |
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( A B S)R |
then matrices
A,
A B S
are similar to matrices
A,
A B S. |
Consequently, the Hurwitz conditions for the matrix |
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replaced by the Hurwitz conditions for matrices |
A, A B S |
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quently, implementation of inequalities |
N0 |
0, N1 0, N2 |
> 0, |
A, A B S |
can be |
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respectively. Conse-
, Nn |
> 0 |
depends |
on the Hurwitz matrix
A
and vector
S = SR* 1.
Lecture 5.
Solution of a model problem in the main case
The constructiveness of the proposed method for determining the conditions of absolute stability and solving the Aizerman problem will be shown using an example.
The differential equation of the regulated system has the form
̇ = |
+ |
, ̇ = −2 |
− 1.03 |
− 0.03 |
− 0.75 ( ), |
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1 |
1 |
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2 |
1 |
2 |
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3 |
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(1.32) |
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̇ = −0.01 |
− 1.01 |
− 0.25 ( ), = |
+ |
, ( ) . |
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3 |
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22
Chapter 1. Absolute stability and Aizerman’s problem of one-dimensional regulated systems
For this example, the matrix
A
, vectors
B,
S are equal to:
1 |
1 |
0 |
0 |
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= (−2 |
−1.03 |
−0.03) , = (−0.75) , = (0 |
1 1), = 1, = 3. |
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0 |
−0.01 |
−1.01 |
−0.25 |
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1. Nonsingular transformation. The characteristic polynomial of the matrix is equal to:
( ) = | 3 − | = 3 + 1.04 2 + + 0.98 = 0 = 3 + 2 2 + 1 + 0,
A
where 0 = 0.98, 1 = 1, 2 = 1.04. Matrix |
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A |
is a Hurwitz matrix. |
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The characteristic equation of the matrix |
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A B S |
is equal to: |
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1( ) = | 3 − − | = 3 + (1.04 + ) 2 + + (0.98 − 0.5 ) = 0. |
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Matrix |
A B S |
is a Hurwitz matrix if 0 ≤ < 1.96 = 0. |
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As |
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0; |
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0, |
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B = 1. |
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4 |
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= |
3 |
; 2 , then B = 0, AB = |
A |
Vectors A = |
3 |
3 |
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A |
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= |
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0 |
4/3 |
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R = |
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2/3 |
2/3 |
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32 |
0. |
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Therefore, the rank of the matrix R is equal to
relative to variables |
y = ( y |
, y |
, y ) |
has a form: |
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1 |
2 |
3 |
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̇ = |
, ̇ = |
, ̇ = −0.98 |
− |
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1 |
2 |
2 |
3 |
3 |
1 |
2 |
n = 3. |
The equation of motion |
− 1.04 3 + ( ),
The row vector
S = (0,1,1)
is represented in the form
S = A A |
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From here
(t) = |
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y |
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where
we find |
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= |
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= 0, |
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= 1. Then = |
1 |
y |
y . |
Derivative |
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(t) (t), |
where (t) = y3 (t). As a result, we have |
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y |
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= Ay B ( ), |
= S y, ( ) 0 , |
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(1.33) |
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= ( 0 |
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0 1). |
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23
Lectures on the stability of the solution of an equation with differential inclusions
2. Improper integrals. The identities follow from (1.33):
( ( )) = ( ) + 0.98 1( ) + 2( ) + 1.04 3( ), , |
(1.34) |
(t) = 12 y1 (t) y3 (t), (t) = 12 y2 (t) (t), t I , (t) = y3 (t), t I.
Then
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∞ |
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∞ |
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= ∫ ( ( )) ̇( ) = ∫ |
[− 2( ) + 0.5 2( ) + 0.5 2( )] + |
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d |
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1 |
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dt |
[F (t)]dt = |
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0 |
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(0) |
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where
N |
= |
1 |
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where
( ) = [0.245 2 + 0.98 |
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+ 0.75 2 |
− 0.5 |
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− 0.52 2], t I |
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0, 2 = 0.5, 3 = 0.5; |
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( (t))]dt |
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(t) M y |
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(t) |
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= [ ( (t)) (t) |
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[M |
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= [ |
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y ]dt = |
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(t)F y(t), |
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3. Absolute stability. As follows from formula (1.28), we have the inequalities:
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0 : |
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1 2 0; |
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(1.37) |
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24
Chapter 1. Absolute stability and Aizerman’s problem of one-dimensional regulated systems
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> 0. |
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Solving the system of algebraic equations (1.35)-(1.38) we find the limiting value |
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2, |
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> 0 |
is an arbitrarily small number. Define the value |
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from the Hurwitz condition |
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for the matrix |
A1( ) = A B S, |
0 < |
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The characteristic equation of the matrix |
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A B S |
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It follows that the matrix |
A B S |
is a Hurwitz matrix if 0 ≤ < 1.96 = 0. |
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Notice that 0 |
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[0, |
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man's problem has no solution. |
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Consider the absolute stability of the equilibrium system (1.32), when the func- |
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tion |
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Unlike inclusion ( ) 0 |
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input transfer function |
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( ) = ( − )−1 = |
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2 − 0.5 |
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3 |
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where |
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According to the frequency condition of V.M. Popov [15] the value of |
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1 |
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( ) = ( ) + ( ) = |
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Modified |
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W* (i ) = X iY , X = ReW (i ), Y = ImW (i ). |
For variables X ,Y the frequency condition of V.M. Popov will be written as X = qY 0 1 > 0 for all , 0 < . As
25
Lectures on the stability of the solution of an equation with differential inclusions
= |
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then the values = 2 0 for which Y = 0, are equal to 1 = 0, 2 = 0.280776. For these values 1, 2 , values ( 1) = −0.51020408, ( 2) = −0.868396526. Note that the value − 0−1 < −0.868396526. Then 0 < 1.1515476744 < 1.24, where the value 0 = 1.24 is obtained by the method proposed above.
To construct a modified partial characteristic, the values of X ( ), Y ( ) : can be calculated:
1.0 = 0, (0) = −0.51020408, (0) = 0;
2.= 0.05, (0.05) = −0.56316, (0.05) = 0.022;
3.= 0.1, (0.1) = −0.6196, (0.1) = 0.04;
4.= 0.15, (0.15) = −0.6802, (0.15) = 0.0481;
5.= 0.2, (0.2) = −0.74, (0.2) = 0.0438;
6.= 0.25, (0.25) = −0.8194, (0.25) = 0.0237;
7.= 0.28, (0.28) = −0.86, (0.28) = 0.000723;
8.= 0.280776, (0.280776) = −0.868396526, (0.280776) = 0;
9.= 0.3, (0.3) = −0.9, (0.3) = 0.02;
10.= 0.4, (0.4) = −1.098, (0.4) = −0.225;
11.= 0.7, (0.7) = −2.39, (0.7) = −5.75;
12.= 10, (10) = 0.11, (10) = −1.28;
13.= ∞, (∞) = 0, (∞) = −1.
Based on these data, a modified frequency response is constructed and values are found 0−1 = 0.868, = 2.2727. Then 0 = 1.152 < 1.24, therefore, the proposed method allows us to select in the space of system parameters the region of absolute stability wider than the known results.
Iserman's problem. Consider the equations of the following form
̇= |
+ |
, ̇= −2 − 1.03 |
− 0.03 − 0.75 ( ) |
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then the transformed system has the form
26
Chapter 1. Absolute stability and Aizerman’s problem of one-dimensional regulated systems
̇= , ̇= |
, ̇= −0.98 |
− |
− 1.04 |
+ ( ), |
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( ) = 0.5 1 |
+ 0.5 2 |
+ 0.01 3, ( ) Φ0. |
(1.40) |
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Notice that |
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A = R* AR* 1 , B = R* B, S = SR* 1 , |
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where = (− 2 |
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; − |
; −0.02), = (0.5; 0.5; 0.01). |
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3 |
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For (1.40) the identities are true:
( ( )) = ( ) + 0.98 1( ) + 2( ) + 1.04 3( ), ,
( ) = 0.5 1( ) + 0.5 2( ) + 0.01 3( ), ,̇( ) = 0.5 2( ) + 0.5 3( ) + 0.01 ( ), ,
where
(
)
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As matricies |
0 |
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01
= ( 0 0
−0.98 −1
A, B, |
are equal to: |
S |
00
1), = (0) , = (12 12 0.01), −1.04 1
then the characteristic polynomial of the matrix |
A B S |
is equal to |
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( ) = | |
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1 |
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Matrix |
A B S |
is a Hurwitz matrix if 0 ≤ < 1.96 = 0. |
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Improper integral |
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∞ |
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∞ |
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= ∫ ( ( )) ̇( ) = ∫ |
[0.01 2( ) + 0.01 2 |
( ) + 0.01 2 |
( )] + |
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+ ∫ |
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( ( )) |
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, | | < ∞, |
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( ) = 0.495 2 + 0.015 2 |
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+ 0.005 2, = 0.01, |
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where |
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+ 0.5 |
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= 0, = 0.01, |
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3 = 0.01. From here it follows that |
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∫ |
0.01 2( ) < ∞, ∫ 0.01 2( ) < ∞, ∫ |
0.01 2( ) < ∞. |
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Consequently,
lim y |
2 |
(t) = 0, |
t |
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lim y |
(t) = 0. |
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t |
3 |
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Then lim y |
(t) = lim y |
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(t) = 0, |
t 1 |
t |
2 |
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lim y |
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(t) = lim |
y (t) = 0, |
lim ̇( ) = 0, lim ̇( ) = −0.98 lim |
( ) + lim ( ( )), |
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t |
2 |
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t |
3 |
→∞ 3 |
→∞ 3 |
→∞ 1 |
→∞ |
lim ( ) |
= 0.5 lim ( ). |
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→∞ |
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Notice that |
y3 (t), t I is a uniformly continuous function due to the fact that the |
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functions |
y1 (t), y2 (t), y3 (t), ( (t)), t I are uniformly continuous functions. Then |
27
Lectures on the stability of the solution of an equation with differential inclusions
condition |
lim y3 (t) = |
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t |
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[14; § 21, |
lemma |
0
1].
entails
Let
lim y |
(t) = 0 |
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by virtue of the Barbalat lemma |
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t |
3 |
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lim y (t) = y |
. |
Then 0 = −0.98 |
+ (0.5 |
) = |
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t |
1 |
1* |
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1 |
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−1.96(0.5 ) + (0.5 1 ). This equation has a unique solution y* = 0. So, y1(t) 0,
y2 (t) 0, y3 (t) 0 when t .
As all the conditions of Theorem 7 are satisfied, then in the sector [0,1.96 − ],> 0 is a sufficiently small number, for system (1.39) the Iserman problem has a solution.
1. We study the absolute stability of the equilibrium position of the system (1.40) by applying Theorem 6. To do this, we calculate improper integrals
∞
− 2 = − ∫ [ ( ( )) 1 ( ) − 1 0−1 2( ( ))] =
∞0
=∫ [ 1 0−1 2( ) + (−0.49 1 +
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+ 0.9604 |
−1) 2( ) + (0.0298 |
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− 1.0384 |
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−0.9184 −1)] + ∫ |
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= |
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∫ |
(0.01 2 |
+ 0.01 2 |
+ 0.01 2) + |
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( ) = , | | < ∞. |
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∫ [ |
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( )] |
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As follows from formula (1.28), the inequalities |
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− |
− Γ |
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≥ 0: 0.01 |
2 |
+ |
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−1 − 2 ≥ 0; |
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Γ = 2 |
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is any number. |
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28
Chapter 1. Absolute stability and Aizerman’s problem of one-dimensional regulated systems
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Find the |
limit |
value |
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from |
equalities: |
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0.01 |
+ |
−1 − 2 |
= 0; −0.49 + |
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+ 0.9604 −1 |
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= 0; 0.01 |
+ 0.0298 |
− 1.0384 −1 |
− 2 |
+ 2 |
= 0; 0.01 + |
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+ 0.4896 |
− 0.9184 −1 − 2 |
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From here when |
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we |
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+ 2; −0.49 |
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+ 0.9604 −1 = 0; |
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= 0.5102040816, |
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+ 2 − 2 |
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Then |
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= |
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= 1.96, |
= 0.9899 2 |
> 0, 2 |
= 0.51576371 2, |
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These results confirm that in the sector [0,1.96 − ] Iserman problem |
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2. We study the absolute stability of the equilibrium position of the system (1.40) |
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~ |
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by applying the theorem of V.M. Popov [15]. Input transfer function |
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or system (1.40) is equal |
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( ) = ( − |
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It is easy to verify that |
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̃1( ) = |
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−0.75 − 0.75 |
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̃( ̃), ̃2 |
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Frequency response W1(iω) = ReW1(iω) + iImW1(iω), where |
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1( ) = |
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Modified frequency response |
W* (i ) = X1 iY1, |
where |
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29
Lectures on the stability of the solution of an equation with differential inclusions
lues For
The value of |
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is determined from the condition |
X |
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qY |
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> 0, |
, 0. Va- |
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these |
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1, 2 , 3 |
values 1( 1) = −0.51020408, 1( 2) = −0.50557, |
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( |
) = −16.4071225. Value |
– −1 |
< |
( |
) = −16.4071225. Then |
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< 0.060949 < |
1 |
3 |
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3 |
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< 1.96, where 0 = 1.96 is obtained above. It follows that the frequency condition of V.M. Popov is not effective for studying the absolute stability of regulated systems with limited resources.
To build a modified frequency response calculated values |
X1 ( ), Y1 ( ) : |
1.= 0, 1(0) = −0.51020408, 1(0) = 0;
2.= 0.01, 1(0.01) = −0.50535, 1(0.01) = 0.000003158;
3.= 0.0103126, 1(0.0103126) = −0.50557, 1(0.0103126) = 0;
4.= 0.02, 1(0.02) = −0.5006, 1(0.02) = 0.000196;
5.= 0.05, 1(0.05) = −0.487, 1(0.05) = 0.002;
6.= 0.1, 1(0.1) = −0.466, 1(0.1) = 0.009249;
7.= 0.5, 1(0.5) = −0.37, 1(0.5) = 0.34165;
8.= 0.8, 1(0.8) = −0.66, 1(0.8) = −1.988;
9.= 0.9, 1(0.9) = −2.505, 1(0.9) = −5.084;
10.= 0.96, 1(0.96) = −14.75, 1(0.96) = −4.7115;
11.= 0.9696874, 1(0.9696874) = −16.4071225, 1(0.9696874) = 0;
12.= 0.98, 1(0.98) = −14.83, 1(0.98) = 5.08;
13.= 1, 1(1) = −8.3333, 1(1) = 8.3333;
14.= 2, 1(2) = −0.20249, 1(2) = 1.277;
15.= ∞, 1(∞) = 0, 1(∞) = 1.
Based on these data, a modified frequency response is constructed and values
0 = 0.058823, = 0.285714 are found.
The inefficiency of the frequency method of V.M. Popov for studying the absolute stability of the system (1.39) is explained by the following factors: firstly when deriving the frequency condition, the boundedness of the improper integral 1 is not taken into account; secondly, the boundedness of the system solutions (1.40) is not used; thirdly, the properties of the improper integral 3 are not taken into account.
Lecture 6.
Absolute stability and the Iserman problem in a simple critical case. Formulation of the problem. Nonsingular transformation
Statement of the problem. The equation of motion of controlled systems in a simple critical case has the form:
x = Ax B ( ), = ( ), = Dx E ,
(1.41)
x(0) = x0 , (0) = 0 , t I = [0, ),
where |
A, B, D, E are constant matrices of n n, n 1,1 n,1 1 orders, respectively, |
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matrix |
A is a Hurwitz matrix, i.e. Re j ( A) < 0, j = 1, n, j ( A) are eigenvalues of the |
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matrix |
А. |
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