LYAPUNOV FUNCTION

'Lyapunov functions' are of interest in mathematics, especially in stability theory.

'Lyapunov functions', named after Aleksandr Mikhailovich Lyapunov, are by definition functions which prove the stability of a certain fixed point in a dynamical system or autonomous differential equation.

Functions which might prove the stability of some equilibrium are called 'Lyapunov-candidate-functions'.
There is no general method to construct or find a Lyapunov-candidate-function which proves the stability of an equilibrium, and the inability to find a Lyapunov function is inconclusive with respect to stability, which means, that not finding a Lyapunov function doesn't mean that the system is unstable.
For dynamical systems (e.g. physical systems), conservation laws can often be used to construct a Lyapunov-candiadte-function.
The 'basic Lyapunov Theorems for autonomous systems' which are directly related to Lyapunov (candidate) functions are a useful tool to prove the stability of an equilibrium of an autonomous dynamical system.

One must be aware, that the basic Lyapunov Theorems for autonomous systems are a 'sufficient, but not necessary' tool to prove the stability of an equilibrium.

Finding a Lyapunov Function for a certain equilibrium might be a matter of luck. And trial and error is the method to apply, when testing Lyapunov-candidate-functions on some equilibrium.

Contents
Definition of a Lyapunov candidate function
Definition of the equilibrium point of a system
Basic Lyapunov theorems for autonomous systems
Stable equilibrium
Locally asymptotically stable equilibrium
Globally asymptotically stable equilibrium
See also
References
External Links

Definition of a Lyapunov candidate function


Let
:V:mathbb{R}^n o mathbb{R}
be a scalar function.

V is a Lyapunov-candidate-function if it is a locally positive-definite function, i.e.
:V(0) = 0 ,
:V(x) > 0 quad orall x in U
With U being a neighborhood region around x = 0

Definition of the equilibrium point of a system


Let
:g : mathbb{R}^n o mathbb{R}^n
:dot{y} = g(y) ,
be an arbitrary autonomous dynamical system with equilibrium point y^
★ ,:
:0 = g(y^
★ ) ,
There always exists a coordinate transformation x = y - y^
★ ,, such that:
:dot{x} = g(x + y^
★ ) = f(x) ,
:0 = f(x^
★ ) quad Rightarrow quad x^
★ = 0 ,
So the new system f(x) has an equilibrium point at the origin.

Basic Lyapunov theorems for autonomous systems


:Main articles: Lyapunov stability

Let
:x^
★ = 0 ,
be an equilibrium of the autonomous system
:dot{x} = f(x) ,
And let
:dot{V}(x) = rac{partial V}{partial x} rac{dx}{dt} =
abla V dot{x} =
abla V f(x)
be the time derivative of the Lyapunov-candidate-function V.
Stable equilibrium

If the Lyapunov-candidate-function V is locally positive definite and the time derivative of the Lyapunov-candidate-function is locally negative semidefinite:
:dot{V}(x) le 0 quad orall x in mathcal{B}
for some neighborhood mathcal{B}, then the equilibrium is proven to be 'stable'.
Locally asymptotically stable equilibrium

If the Lyapunov-candidate-function V is locally positive definite and the time derivative of the Lyapunov-candidate-function is locally negative definite:
:dot{V}(x) < 0 quad orall x in mathcal{B}
for some neighborhood mathcal{B}, then the equilibrium is proven to be 'locally asymptotically stable'.
Globally asymptotically stable equilibrium

If the Lyapunov-candidate-function V is globally positive definite and the time derivative of the Lyapunov-candidate-function is globally negative definite:
:dot{V}(x) < 0 quad orall x in mathbb{R}^n,
then the equilibrium is proven to be 'globally asymptotically stable'.

See also



Lyapunov stability

ordinary differential equations

References






External Links



Example of determining the stability of the equilibrium solution of a system of ODEs with a Lyapunov function

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