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Lyapunov function

 
Sci-Tech Dictionary: Lyapunov function
(lē′ap·ə′nöf ′fəŋk·shən)

(mathematics) A function of a vector and of time which is positive-definite and has a negative-definite derivative with respect to time for nonzero vectors, is identically zero for the zero vector, and approaches infinity as the norm of the vector approaches infinity; used in determining the stability of control systems. Also spelled Liapunov function.


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Wikipedia: Lyapunov function
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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.

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Definition of a Lyapunov candidate function

Let

V:\mathbb{R}^n \to \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 \forall x \in U\setminus\{0\}

With U being a neighborhood region around x = 0

Definition of the equilibrium point of a system

Let

g : \mathbb{R}^n \to \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) \,
 f(0) = 0 \,

So the new system f(x) has an equilibrium point at the origin.

Basic Lyapunov theorems for autonomous systems

Let

x^* = 0 \,

be an equilibrium of the autonomous system

\dot{x} = f(x) \,

And let

\dot{V}(x) = \frac{\partial V}{\partial x}\cdot \frac{dx}{dt} = \nabla V \cdot \dot{x} = \nabla V\cdot 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 \forall x \in \mathcal{B}\setminus\{0\}

for some neighborhood \mathcal{B} 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:

\dot{V}(x) < 0 \quad \forall x \in \mathcal{B}\setminus\{0\}

for some neighborhood \mathcal{B} 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:

\dot{V}(x) < 0 \quad \forall x \in \mathbb{R}^n\setminus\{0\},

then the equilibrium is proven to be globally asymptotically stable.

The Lyapunov-candidate function V(x) is radially unbounded if

\| x \| \to \infty  \Rightarrow V(x) \to \infty .

Example

Consider the following differential equation on \mathbb{R}:

\dot x = -x.

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 \mathbb{R}\setminus\{0\}. Then

\dot V(x) = V'(x) f(x) = \mathrm{sign}(x)\cdot (-x) = -|x|<0.

This correctly shows that the origin is asymptotically stable.

See also

References


External links


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