Stability

Stability of dynamical systems

Equilibrium points

For autonomous systems with the property f(0n×1)=0n×1f (0_{n×1})=0_{n\times1} the equilibrium points are the real roots of f(x)=0f(x)=0, which are points where starting at x(0)=0n×1x(0) = 0_{n×1} will remain there for all time.

If a system has an equilibrium point at an arbitrary point xˉ\bar{x} we can simply define incremental coordinates x~=xxˉ\tilde{x} = x - \bar{x}, allowing the system to described by f(x~)=x~˙f(\tilde{x}) = \dot{\tilde{x}}, which has an equilibrium at x~=0\tilde{x} = 0.

Stability

Origin is a stable equilibrium of x˙=f(x)\dot{x} = f(x) if for each ϵ>0\epsilon>0, there exists a δ>0\delta>0 such that when x(0)<δ||{x(0)|| < \delta} \rightarrow x(t)<ϵ,t0||x(t)|| < \epsilon, \forall t \geq 0

Summary: If initial conditions inside region δ\delta the states will remain inside region ϵ\epsilon

Asymptotic Stability

Origin is asymptotically stable equilibrium of x˙=f(x)\dot{x} = f(x) if its stable and for x(0)<δ||{x(0)|| < \delta} \rightarrow limt\lim_{t\to\infty} x(t)=0x(t) = 0

Summary: If initial conditions inside region δ\delta the states will converge to zero as time goes to infinity.

Asymptotic Stability

Lyapunov Stability

The origin is a stable equilibrium of x˙=f(x)\dot{x} = f(x) if there exists r>0r>0 and a positive definite function V(x)V(x) on Br(0)B_r(0) such that V˙(x)\dot{V}(x) is negative semi-definite on Br(0)B_r(0). Moreover, if V˙(x)\dot{V}(x) is negative definite on Br(0)B_r(0) then the origin is asymptotically stable.

V˙(x)\dot{V}(x) can be calculated using the chain rule:

V˙(x)=dVdt=dVdxdxdt=dVdxf(x)\begin{equation}\dot{V}(x) = \dfrac{dV}{dt} = \dfrac{dV}{dx}\dfrac{dx}{dt} = \dfrac{dV}{dx}f(x)\end{equation}

Lyapunov stability can be summarized by the following conditions:

  1. V(x)V(x) is C1C^1, continuously differentiable
  2. V(0)=0V(0) = 0 V(x)>0R\0V(x) > 0 \in \R \backslash0
  3. V˙(0)=0\dot{V}(0) = 0 V˙(x)0R\0\dot{V}(x) \leq 0 \in \R \backslash0

LaSalle's Invariance Principle

Positively Invariant Set

A set Ω\Omega is said to be positively invariant with respect to x˙=f(x)\dot{x} = f(x) if x(0)Ωx(t)Ω,t0x(0) \in \Omega \rightarrow x(t) \in \Omega, \forall t \geq 0

Summary: If you start in Ω\Omega, you will stay in Ω\Omega

LaSalle's Invariance Theorem can be used to show the asymptotic stability of an equilibrium when the derivative of the Lyapunov function V˙(x)\dot{V}(x) is only negative semi-definite. \newline

  • Let Ω\Omega be a positively invariant set with respect to x˙=f(x)\dot{x} = f(x)
  • Let V(x)V(x) be a continuously differentiable function on Ω\Omega such that V˙(x)0\dot{V} (x) \leq 0 in Ω\Omega
  • Let E Ω\subset \Omega be the set of all points in Ω\Omega such that V˙(x)=0\dot{V}(x) = 0
  • Let M be the largest positively invariant set in E

LaSalle’s Invariance Theorem

Exponential Stability

If there exists a function V:DRV : D \rightarrow \R and constants a,k1,k2,k3>0a,k_1,k_2,k_3 > 0 such that

  1. VV is C1C^1, continuously differentiable
  2. k1xaV(x)k2xak_1||x||^a\leq V(x) \leq k_2||x||^a
  3. V˙(x)k3xa\dot{V}(x) \leq -k_3||x||^a

then x=0x = 0 is exponentially stable.