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multiple time scale dynamics with two fast variables and one slow ...

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5.4 Interaction of Invariant Manifolds<br />

The <strong>slow</strong> manifold Cl,ǫ is normally hyperbolic away from the fold point x1,−,<br />

<strong>with</strong> <strong>one</strong> attracting direction <strong>and</strong> <strong>one</strong> repelling direction. We recently intro-<br />

duced a method [55] for computing <strong>slow</strong> manifolds of saddle type. This algo-<br />

rithm is used here to help determine whether there are connecting orbits from<br />

a neighborhood of Cl,ǫ to the equilibrium point q. Our numerical strategy for<br />

finding connecting orbits has three steps:<br />

1. Choose the cross section<br />

transverse to Cl,ǫ,<br />

Σ0.09={(x1, x2, y)∈R 3 : y=0.09}<br />

2. Compute intersections of trajectories in W s (q) <strong>with</strong>Σ0.09. These points are<br />

found either by backward integration from initial conditions that lie in a<br />

small disk D containing q in W s (q) or by solving a boundary value problem<br />

for trajectories that have <strong>one</strong> end inΣ0.09 <strong>and</strong> <strong>one</strong> end on the boundary of<br />

D.<br />

3. Compute the intersection pl∈ Cl,ǫ∩Σ0.09 <strong>with</strong> the algorithm described in<br />

Guckenheimer <strong>and</strong> Kuehn [55] <strong>and</strong> determine the directions of the posi-<br />

tive <strong>and</strong> negative eigenvectors of the Jacobian of the <strong>fast</strong> subsystem at pl.<br />

Figure 5.3 shows the result of these computations forǫ= 0.01, s=1.37 <strong>and</strong><br />

three values of p. 3 The intersections of W s (q) <strong>with</strong>Σ0.09 lies close to W s (Cl,ǫ).<br />

3 The second step above was carried out <strong>with</strong> <strong>two</strong> different initial value solvers, ode15s in<br />

MatLab [100] <strong>and</strong> dop853 [61], <strong>and</strong> <strong>with</strong> AUTO [34] producing similar results.<br />

127

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