Difference between revisions of "Uniform stability"
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− | + | [[Lyapunov stability|Lyapunov stability]], uniform with respect to the initial time. A solution $ x _ {0} ( t) $, | |
+ | $ t \in \mathbf R ^ {+} $, | ||
+ | of a system of differential equations | ||
− | + | $$ | |
+ | \dot{x} = f ( t, x),\ \ | ||
+ | x \in \mathbf R ^ {n} , | ||
+ | $$ | ||
+ | |||
+ | is called uniformly stable if for every $ \epsilon > 0 $ | ||
+ | there is a $ \delta > 0 $ | ||
+ | such that for every $ t _ {0} \in \mathbf R ^ {+} $ | ||
+ | and every solution $ x ( t) $ | ||
+ | of the system satisfying the inequality | ||
+ | |||
+ | $$ | ||
+ | | x ( t _ {0} ) - x _ {0} ( t _ {0} ) | < \delta , | ||
+ | $$ | ||
the inequality | the inequality | ||
− | + | $$ | |
+ | | x ( t) - x _ {0} ( t) | < \epsilon | ||
+ | $$ | ||
− | holds for all | + | holds for all $ t \geq t _ {0} $. |
− | A Lyapunov-stable fixed point of an autonomous system of differential equations | + | A Lyapunov-stable fixed point of an autonomous system of differential equations $ \dot{x} = f ( x) $, |
+ | $ x \in \mathbf R ^ {n} $, | ||
+ | is uniformly stable, but, in general, a Lyapunov-stable solution need not be uniformly stable. For example, the solution $ x ( t) = 0 $, | ||
+ | $ t \in \mathbf R ^ {+} $, | ||
+ | of the equation | ||
− | + | $$ \tag{1 } | |
+ | \dot{x} = [ \sin \mathop{\rm ln} ( 1 + t) - \alpha ] x | ||
+ | $$ | ||
− | is stable for each | + | is stable for each $ \alpha \in ( 1/ \sqrt 2 , 1) $ |
+ | but is not uniformly stable for such $ \alpha $. | ||
Suppose one is given a linear system of differential equations | Suppose one is given a linear system of differential equations | ||
− | + | $$ \tag{2 } | |
+ | \dot{x} = A ( t) x,\ \ | ||
+ | x \in \mathbf R ^ {n} , | ||
+ | $$ | ||
− | where | + | where $ A ( \cdot ) $ |
+ | is a mapping $ \mathbf R ^ {+} \rightarrow \mathop{\rm Hom} ( \mathbf R ^ {n} , \mathbf R ^ {n} ) $ | ||
+ | that is summable on each interval. | ||
− | In order that the solution | + | In order that the solution $ x = 0 $ |
+ | of (2) be uniformly stable, it is necessary that the upper singular exponent $ \Omega ^ {0} ( A) $ | ||
+ | of (2) be less than or equal to zero (cf. also [[Singular exponents|Singular exponents]]). For example, in the case of equation (1), the upper singular exponent $ \Omega ^ {0} ( A) = 1 - \alpha $, | ||
+ | and the [[Lyapunov characteristic exponent|Lyapunov characteristic exponent]] $ \lambda _ {1} ( A) = ( 1/ \sqrt 2 ) - \alpha $. | ||
+ | For the existence of a $ \delta > 0 $ | ||
+ | such that the solution $ x = 0 $ | ||
+ | of any system | ||
− | + | $$ | |
+ | \dot{x} = A ( t) x + g ( t, x),\ \ | ||
+ | x \in \mathbf R ^ {n} , | ||
+ | $$ | ||
that satisfies the conditions of the existence and uniqueness theorem for the solution of the Cauchy problem as well as the condition | that satisfies the conditions of the existence and uniqueness theorem for the solution of the Cauchy problem as well as the condition | ||
− | < | + | $$ |
+ | | g ( t, x) | < \delta | x | | ||
+ | $$ | ||
− | be uniformly stable, it is necessary and sufficient that the upper singular exponent | + | be uniformly stable, it is necessary and sufficient that the upper singular exponent $ \Omega ^ {0} ( A) $ |
+ | be less than zero. | ||
====References==== | ====References==== | ||
<table><TR><TD valign="top">[1]</TD> <TD valign="top"> K. Persidskii, "On stability of motion in a first approximation" ''Mat. Sb.'' , '''40''' : 3 (1933) pp. 284–293 (In Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> B.P. Demidovich, "Lectures on the mathematical theory of stability" , Moscow (1967) (In Russian)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> Yu.L. Daletskii, M.G. Krein, "Stability of solutions of differential equations in Banach space" , Amer. Math. Soc. (1974) (Translated from Russian)</TD></TR></table> | <table><TR><TD valign="top">[1]</TD> <TD valign="top"> K. Persidskii, "On stability of motion in a first approximation" ''Mat. Sb.'' , '''40''' : 3 (1933) pp. 284–293 (In Russian)</TD></TR><TR><TD valign="top">[2]</TD> <TD valign="top"> B.P. Demidovich, "Lectures on the mathematical theory of stability" , Moscow (1967) (In Russian)</TD></TR><TR><TD valign="top">[3]</TD> <TD valign="top"> Yu.L. Daletskii, M.G. Krein, "Stability of solutions of differential equations in Banach space" , Amer. Math. Soc. (1974) (Translated from Russian)</TD></TR></table> | ||
− | |||
− | |||
====Comments==== | ====Comments==== |
Latest revision as of 08:27, 6 June 2020
Lyapunov stability, uniform with respect to the initial time. A solution $ x _ {0} ( t) $,
$ t \in \mathbf R ^ {+} $,
of a system of differential equations
$$ \dot{x} = f ( t, x),\ \ x \in \mathbf R ^ {n} , $$
is called uniformly stable if for every $ \epsilon > 0 $ there is a $ \delta > 0 $ such that for every $ t _ {0} \in \mathbf R ^ {+} $ and every solution $ x ( t) $ of the system satisfying the inequality
$$ | x ( t _ {0} ) - x _ {0} ( t _ {0} ) | < \delta , $$
the inequality
$$ | x ( t) - x _ {0} ( t) | < \epsilon $$
holds for all $ t \geq t _ {0} $.
A Lyapunov-stable fixed point of an autonomous system of differential equations $ \dot{x} = f ( x) $, $ x \in \mathbf R ^ {n} $, is uniformly stable, but, in general, a Lyapunov-stable solution need not be uniformly stable. For example, the solution $ x ( t) = 0 $, $ t \in \mathbf R ^ {+} $, of the equation
$$ \tag{1 } \dot{x} = [ \sin \mathop{\rm ln} ( 1 + t) - \alpha ] x $$
is stable for each $ \alpha \in ( 1/ \sqrt 2 , 1) $ but is not uniformly stable for such $ \alpha $.
Suppose one is given a linear system of differential equations
$$ \tag{2 } \dot{x} = A ( t) x,\ \ x \in \mathbf R ^ {n} , $$
where $ A ( \cdot ) $ is a mapping $ \mathbf R ^ {+} \rightarrow \mathop{\rm Hom} ( \mathbf R ^ {n} , \mathbf R ^ {n} ) $ that is summable on each interval.
In order that the solution $ x = 0 $ of (2) be uniformly stable, it is necessary that the upper singular exponent $ \Omega ^ {0} ( A) $ of (2) be less than or equal to zero (cf. also Singular exponents). For example, in the case of equation (1), the upper singular exponent $ \Omega ^ {0} ( A) = 1 - \alpha $, and the Lyapunov characteristic exponent $ \lambda _ {1} ( A) = ( 1/ \sqrt 2 ) - \alpha $. For the existence of a $ \delta > 0 $ such that the solution $ x = 0 $ of any system
$$ \dot{x} = A ( t) x + g ( t, x),\ \ x \in \mathbf R ^ {n} , $$
that satisfies the conditions of the existence and uniqueness theorem for the solution of the Cauchy problem as well as the condition
$$ | g ( t, x) | < \delta | x | $$
be uniformly stable, it is necessary and sufficient that the upper singular exponent $ \Omega ^ {0} ( A) $ be less than zero.
References
[1] | K. Persidskii, "On stability of motion in a first approximation" Mat. Sb. , 40 : 3 (1933) pp. 284–293 (In Russian) |
[2] | B.P. Demidovich, "Lectures on the mathematical theory of stability" , Moscow (1967) (In Russian) |
[3] | Yu.L. Daletskii, M.G. Krein, "Stability of solutions of differential equations in Banach space" , Amer. Math. Soc. (1974) (Translated from Russian) |
Comments
The upper singular exponent is also called the Bohl exponent, cf. also Singular exponents.
References
[a1] | N. Rouché, "Stability theory by Liapunov's direct method" , Springer (1977) |
[a2] | J.K. Hale, "Ordinary differential equations" , Wiley (1969) |
[a3] | W.A. Coppel, "Stability and asymptotic behavior of differential equations" , D.C. Heath (1965) |
Uniform stability. Encyclopedia of Mathematics. URL: http://encyclopediaofmath.org/index.php?title=Uniform_stability&oldid=49072