1984
DOI: 10.1007/978-3-642-69689-3
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Chemical Oscillations, Waves, and Turbulence

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Cited by 6,238 publications
(7,191 citation statements)
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References 73 publications
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“…Using the theory of weakly coupled oscillators (Kuramoto 1984;Malkin 1949;Ermentrout 1984), the dynamics of the HCO can be reduced to the consideration of a "phase model", in which the state of the oscillator is described entirely by its phase θ(t). The phase can be decomposed into two parts: θ(t) = t + φ(t) mod T , where t describes the change in the phase of the oscillator in the absence of the external input, and the relative phase φ(t) quantifies the phase shift that results from the external input.…”
Section: Phase Modelsmentioning
confidence: 99%
“…Using the theory of weakly coupled oscillators (Kuramoto 1984;Malkin 1949;Ermentrout 1984), the dynamics of the HCO can be reduced to the consideration of a "phase model", in which the state of the oscillator is described entirely by its phase θ(t). The phase can be decomposed into two parts: θ(t) = t + φ(t) mod T , where t describes the change in the phase of the oscillator in the absence of the external input, and the relative phase φ(t) quantifies the phase shift that results from the external input.…”
Section: Phase Modelsmentioning
confidence: 99%
“…Under the assumption that the coupling functions G i are weak and the oscillatory dynamics are harmonic [Kuramoto, 1984], the above equations can be reduced to a simpler set written in terms of the oscillators' phase angles θ i asθ…”
Section: Model Of Two Coupled Oscillatorsmentioning
confidence: 99%
“…It is also known as the classical Kuramoto model [Kuramoto, 1984], where K is the coupling gain between the oscillators. It is assumed to be isotropic for both oscillators.…”
Section: Extending the Kuramoto Modelmentioning
confidence: 99%
“…It is a well known fact (see, e.g. Malkin, 1949Malkin, , 1956Blechman, 1971;Neu, 1979;Ermentrout, 1981;Kuramoto, 1984;Ermentrout and Kopell, 1991) that the entire system (1, 2) can be approximated by a phase model that is defined on the n+ 1 dimensional torus T n + 1 . Hoppensteadt and Izhikevich (1997) have gone further and proved that there is actually a continuous change of variables that transforms (1, 2) into the phase model.…”
Section: Autonomous Oscillationsmentioning
confidence: 99%