Lyapunov fractal with the sequence AAAABBB
In mathematics, Lyapunov functions are functions which can be used to prove the stability of a certain fixed point in a dynamical system or autonomous differential equation. Named after the Russian mathematician Aleksandr Mikhailovich Lyapunov, Lyapunov functions are important to stability theory and control theory. A similar concept appears in the theory of general state space Markov Chains, usually under the name Lyapunov-Foster functions.
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-candidate-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. Trial and error is the method to apply, when testing Lyapunov-candidate-functions on some equilibrium. As the areas of equal stability often follow lines in 2D, the computer generated images of Lyapunov exponents look nice and are very popular.
Definition of a Lyapunov candidate function
Let

be a scalar function.
V is a Lyapunov-candidate-function if it is a locally positive-definite function, i.e.


With U being a neighborhood region around x = 0
Definition of the equilibrium point of a system
Let


be an arbitrary autonomous dynamical system with equilibrium point
:

There always exists a coordinate transformation
, such that:


So the new system f(x) has an equilibrium point at the origin.
Basic Lyapunov theorems for autonomous systems
-
Let

be an equilibrium of the autonomous system

And let

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:

for some neighborhood
of 0, 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:

for some neighborhood
of 0, then the equilibrium is proven to be locally asymptotically stable.
Globally asymptotically stable equilibrium
If the Lyapunov-candidate-function V is globally positive definite, radially unbounded and the time derivative of the Lyapunov-candidate-function is globally negative definite:

then the equilibrium is proven to be globally asymptotically stable.
The Lyapunov-candidate function V(x) is radially unbounded if
.
Example
Consider the following differential equation on
:

The velocity vector points always towards the origin, so the distance from it decreases with time and is a natural candidate for a Lyapunov function. Take V(x) = | x | on
. Then

This correctly shows that the origin is asymptotically stable.
See also
References
External links