Lyapunov methods
Objective. Prove stability without explicit solutions.
- 1. Learn
- 2. Worked example
- 3. Practice
- 4. Feedback
- 5. Continue
Learn: the key idea
Lyapunov methods establish stability of a fixed point without solving the differential equation, by finding a scalar function that decreases along all trajectories near that point. A function V(x,y) is a Lyapunov function at a fixed point if V is positive everywhere nearby except zero at the point itself, and its derivative along trajectories, V̇ = ∇V·(ẋ,ẏ), is negative (or non-positive) there. If such V exists, the fixed point is stable, and strict negativity of V̇ away from the point gives asymptotic stability. Example: for ẋ = −x³, the function V(x) = x² gives V̇ = 2xẋ = −2x⁴ ≤ 0, proving the origin is asymptotically stable.
Worked example
Use a Lyapunov function to show the origin is asymptotically stable for ẋ = −x + xy², ẏ = −y − x²y... actually use ẋ = −x³, ẏ = −y³.
- 1Choose the candidate V(x,y) = x² + y², which is positive everywhere except zero at the origin.
- 2Compute V̇ = 2xẋ + 2yẏ = 2x(−x³) + 2y(−y³) = −2x⁴ − 2y⁴.
- 3Since x⁴ ≥ 0 and y⁴ ≥ 0, V̇ ≤ 0, with equality only when x = y = 0.
- 4As V is positive definite and V̇ is negative definite away from the origin, the origin is asymptotically stable.
Answer: Origin is asymptotically stable, using V = x² + y²
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Practice
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Start practisingCommon mistake. Students often pick V(x,y) = x² + y² automatically for every system; this only works if V̇ turns out negative for that specific system, and for many nonlinear systems a different or weighted Lyapunov function is needed.
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