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

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s<br />

1.39<br />

1.385<br />

1.38<br />

1.375<br />

1.37<br />

1.365<br />

Hom<br />

p<br />

0.058 0.0585 0.059 0.0595 0.06<br />

(a) (p, s)-space: Black circles correspond to <strong>two</strong> portraits in<br />

(b).<br />

(b) (x1, y)-projection.<br />

Figure 5.8: The dashed green curve indicates where canard orbits start to<br />

occur along Cm,ǫ. For values of p to the left of the dashed green<br />

curve we observe that orbits near the middle branch escape in<br />

backward <strong>time</strong> (upper panel in (b)). For values of p to the right<br />

of the dotted green curve trajectories near Cm,ǫ stay bounded in<br />

backward <strong>time</strong>.<br />

where the trajectory that flows into Cm,ǫ lies to the right of W u (Cl,ǫ) <strong>and</strong> comes<br />

from the periodic orbit or another bounded invariant set. This boundary was<br />

found by computing trajectories starting on Cm,0 backward in <strong>time</strong>. In backward<br />

<strong>time</strong> the middle branch of the <strong>slow</strong> manifold is attracting, so the trajectory first<br />

approaches Cm,ǫ <strong>and</strong> then continues beyond its end when x1 decreases below<br />

x1,−. Figure 5.8(b) illustrates the difference in the behavior of these trajectories<br />

on the <strong>two</strong> sides of the dashed green curve. Figure 5.8 shows that the param-<br />

eters <strong>with</strong> canard orbits for the backward flow have smaller values of p than<br />

those for which W s (q) <strong>and</strong> W u (Cl,ǫ) have a tangential intersection. The turns of<br />

the C-curve do not occur at parameters where the backward flow has canards.<br />

140

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