Paper 2, Section II, A

Dynamical Systems
Part II, 2017

(a) State Liapunov's first theorem and La Salle's invariance principle. Use these results to show that the fixed point at the origin of the system

x¨+kx˙+sin3x=0,k>0,\ddot{x}+k \dot{x}+\sin ^{3} x=0, \quad k>0,

is asymptotically stable.

(b) State the Poincaré-Bendixson theorem. Show that the forced damped pendulum

θ˙=p,p˙=kpsinθ+F,k>0,\dot{\theta}=p, \quad \dot{p}=-k p-\sin \theta+F, \quad k>0,

with F>1F>1, has a periodic orbit that encircles the cylindrical phase space (θ,p)R[mod2π]×R(\theta, p) \in \mathbb{R}[\bmod 2 \pi] \times \mathbb{R}, and that it is unique.

[You may assume that the Poincaré-Bendixson theorem also holds on a cylinder, and comment, without proof, on the use of any other standard results.]

(c) Now consider ()(*) for F,k=O(ϵ)F, k=O(\epsilon), where ϵ1\epsilon \ll 1. Use the energy-balance method to show that there is a homoclinic orbit in p0p \geqslant 0 if F=Fh(k)F=F_{h}(k), where Fh4k/π>0F_{h} \approx 4 k / \pi>0.

Explain briefly why there is no homoclinic orbit in p0p \leqslant 0 for F>0F>0.