A2.6 B2.4

Dynamics of Differential Equations | Part II, 2002

(i) Define the terms stable manifold and unstable manifold of a hyperbolic fixed point x0\mathbf{x}_{0} of a dynamical system. State carefully the stable manifold theorem.

Give an approximation, correct to fourth order in x|\mathbf{x}|, for the stable and unstable manifolds of the origin for the system

(x˙y˙)=(x+x2y2y+x2).\left(\begin{array}{c} \dot{x} \\ \dot{y} \end{array}\right)=\left(\begin{array}{c} x+x^{2}-y^{2} \\ -y+x^{2} \end{array}\right) .

(ii) State, without proof, the centre manifold theorem. Show that the fixed point at the origin of the system

x˙=yx+ax3,y˙=rxyzyz˙=z+xy\begin{aligned} &\dot{x}=y-x+a x^{3}, \\ &\dot{y}=r x-y-z y \\ &\dot{z}=-z+x y \end{aligned}

where aa is a constant, is non-hyperbolic at r=1r=1.

Using new coordinates v=x+y,w=xyv=x+y, w=x-y, find the centre manifold in the form

w=αv3+,z=βv2+γv4+w=\alpha v^{3}+\ldots, \quad z=\beta v^{2}+\gamma v^{4}+\ldots

for constants α,β,γ\alpha, \beta, \gamma to be determined. Hence find the evolution equation on the centre manifold in the form

v˙=18(a1)v3+((3a+1)(a+1)128+(a1)32)v5+\dot{v}=\frac{1}{8}(a-1) v^{3}+\left(\frac{(3 a+1)(a+1)}{128}+\frac{(a-1)}{32}\right) v^{5}+\ldots

Ignoring higher order terms, give conditions on aa that guarantee that the origin is asymptotically stable.

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