1990
DOI: 10.1121/1.399855
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Bifurcation structure of bubble oscillators

Abstract: Methods from chaos physics are applied to a model of a driven spherical gas bubble in water to determine its dynamic properties, especially its resonance behavior and bifurcation structure. The dynamic properties are described in a growing level of abstraction by radius-time curves, trajectories in state space, strange attractors in the Poincar6 plane, basins of attraction, bifurcation diagrams, winding number diagrams, and phase diagrams. A sequence of bifurcation diagrams is given, exemplifying the recurrent… Show more

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Cited by 244 publications
(195 citation statements)
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“…The accumulated knowledge of this nonlinear behavior has been summarized in many reviews [18][19][20] and papers [1,[21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36]. The most important findings are the existence of period-doubling cascades in the bifurcation structure [1,21,30,31,35], the appearance of resonance horns in the amplitude-frequency plane of the driving [24,27,34] or the alternation of chaotic and periodic windows [21,23,33]. These structures show similarities with the results obtained on other nonlinear oscillators such as Toda [37], Duffing [38][39][40][41] and others [42], implying that they are universal features of nonlinear systems rather than unique properties of oscillating bubbles.…”
Section: Introductionmentioning
confidence: 99%
“…The accumulated knowledge of this nonlinear behavior has been summarized in many reviews [18][19][20] and papers [1,[21][22][23][24][25][26][27][28][29][30][31][32][33][34][35][36]. The most important findings are the existence of period-doubling cascades in the bifurcation structure [1,21,30,31,35], the appearance of resonance horns in the amplitude-frequency plane of the driving [24,27,34] or the alternation of chaotic and periodic windows [21,23,33]. These structures show similarities with the results obtained on other nonlinear oscillators such as Toda [37], Duffing [38][39][40][41] and others [42], implying that they are universal features of nonlinear systems rather than unique properties of oscillating bubbles.…”
Section: Introductionmentioning
confidence: 99%
“…This happens because the basins of the attractors deform under the change of the parameters of equation (1). If such a change is large enough, a point which was in a small neighborhood of one of the coexisting attractors can appear in the basin of another attractor at the next value of the parameter.…”
Section: Main Equation and Resultsmentioning
confidence: 99%
“…Let us numerically investigate the dynamics of the gas bubbles governed by equation (1). An attractor is called hidden if its basin of attraction does not intersect with small neighborhoods of equilibria.…”
Section: Main Equation and Resultsmentioning
confidence: 99%
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“…This method continued through increasing the control parameter and the new resulting discrete points were plotted in the bifurcation diagram versus the new control parameter. For a full discussion on the bifurcation diagram and Lyapunov exponent spectrum, their utilization in order to study the bubble dynamics, one can refer to [43,44].…”
Section: Bifurcation Diagramsmentioning
confidence: 99%