Paper 2, Section II, 32E

Dynamical Systems | Part II, 2018

Consider the system

x˙=y,y˙=xx3+ϵ(1αx2)y,\dot{x}=y, \quad \dot{y}=x-x^{3}+\epsilon\left(1-\alpha x^{2}\right) y,

where α\alpha and ϵ\epsilon are real constants, and 0ϵ10 \leqslant \epsilon \ll 1. Find and classify the fixed points.

Show that when ϵ=0\epsilon=0 the system is Hamiltonian and find HH. Sketch the phase plane for this case.

Suppose now that 0<ϵ10<\epsilon \ll 1. Show that the small change in HH following a trajectory of the perturbed system around an orbit H=H0H=H_{0} of the unperturbed system is given to leading order by an equation of the form

ΔH=ϵx1x2F(x;α,H0)dx\Delta H=\epsilon \int_{x_{1}}^{x_{2}} F\left(x ; \alpha, H_{0}\right) d x

where FF should be found explicitly, and where x1x_{1} and x2x_{2} are the minimum and maximum values of xx on the unperturbed orbit.

Use the energy-balance method to find the value of α\alpha, correct to leading order in ϵ\epsilon, for which the system has a homoclinic orbit. [Hint: The substitution u=112x2u=1-\frac{1}{2} x^{2} may prove useful.]

Over what range of α\alpha would you expect there to be periodic solutions that enclose only one of the fixed points?

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