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Dynamical systems
Lesson 33 of 75
Standard practice

Lyapunov methods

Objective. Prove stability without explicit solutions.

  1. 1. Learn
  2. 2. Worked example
  3. 3. Practice
  4. 4. Feedback
  5. 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.

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Illustrated card showing ?
  1. 1Choose the candidate V(x,y) = x² + y², which is positive everywhere except zero at the origin.
  2. 2Compute V̇ = 2xẋ + 2yẏ = 2x(−x³) + 2y(−y³) = −2x⁴ − 2y⁴.
  3. 3Since x⁴ ≥ 0 and y⁴ ≥ 0, V̇ ≤ 0, with equality only when x = y = 0.
  4. 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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Common 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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