2019
DOI: 10.3934/mbe.2019255
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Coordinate-independent singular perturbation reduction for systems with three time scales

Abstract: On the basis of recent work by Cardin and Teixeira on ordinary differential equations with more than two time scales, we devise a coordinateindependent reduction for systems with three time scales; thus no a priori separation of variables into fast, slow etc. is required. Moreover we consider arbitrary parameter dependent systems and extend earlier work on Tikhonov-Fenichel parameter values -i.e. parameter values from which singularly perturbed systems emanate upon small perturbations -to the three time-scale … Show more

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Cited by 14 publications
(17 citation statements)
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“…Our first result generalizes [40, Proposition 1 (ii)]. The proof is straightforward by induction using the argument in [40,Lemma 3] and its proof.…”
Section: Verification Of Hyperbolic Attractivitysupporting
confidence: 58%
See 2 more Smart Citations
“…Our first result generalizes [40, Proposition 1 (ii)]. The proof is straightforward by induction using the argument in [40,Lemma 3] and its proof.…”
Section: Verification Of Hyperbolic Attractivitysupporting
confidence: 58%
“…Our next result allows a suitable first-order formulation without quantifier alternation. Its proof combines [40,Lemma 3] with our Lemma 3. . .…”
Section: Verification Of Hyperbolic Attractivitymentioning
confidence: 94%
See 1 more Smart Citation
“…We emphasise that here, the presence of two singular perturbation parameters indicates the presence of three timescales, however, which distinguishes the relaxation oscillations observed for 0 < v 0 < v ss from vdP-type relaxation oscillations, despite the 'four strokes'. It is also important to note that in the presence of multiple small parameters, the number of timescales in general systems (2.9) can exceed the number of variables [70]. This is exemplified by system (3.43); see also [59], where the authors identify a nonstandard relaxation oscillation in a three timescale model for glycolitic oscillations in the plane.…”
Section: Three Timescales Stick-slip and Ducksmentioning
confidence: 99%
“…70) has the entire plane { = 0} as a manifold of equilibria, containing the degenerate subset Σ × {0} = {(x, 0, 0) : x ∈ R} ⊂ R 3 (i.e. the switching manifold) along which the system is non-smooth.…”
mentioning
confidence: 99%