Lyapunov's Direct Method
Lyapunov's direct (or second) method determines stability without solving the differential equation, by finding an appropriate energy-like function.
Statement
Theorem7.7Lyapunov stability theorem (complete)
Let be an equilibrium of and let be a function on a neighborhood of with .
- If is positive definite and (negative semi-definite), then is stable.
- If is positive definite and is negative definite, then is asymptotically stable.
- If is positive definite, is negative semi-definite, and the only solution of that stays in is , then is asymptotically stable (LaSalle).
Proof of Part 1 (Stability)
Proof
Given , let . Since is positive definite and continuous, .
Since is continuous and , there exists such that for .
For : . Since , for all .
If ever reached , then , contradicting . Therefore for all .
■
Instability Theorem
Theorem7.8Chetaev's instability theorem
Let be with . If in every neighborhood of there exists a point where , and on the set , then is unstable.
ExampleInstability via Chetaev
For , : try .
for .
Since near the origin and , the origin is unstable.
RemarkComparison with linearization
Lyapunov's method and linearization are complementary:
- Linearization is easy when eigenvalues have nonzero real parts.
- Lyapunov functions handle non-hyperbolic cases and provide stability regions.
- For nonlinear systems, Lyapunov functions can prove global stability, which linearization cannot.