2001
DOI: 10.1088/0951-7715/15/1/302
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Periodic orbit theory applied to a chaotically oscillating gas bubble in water

Abstract: This study investigates the dynamics of an acoustically driven air bubble in water. Depending on the values of external parameters, the radial oscillations of the bubble can be either stable or chaotic. The necessary condition of chaotic behaviour is identified to be the non-zero amplitude of the bubble's afterbounces at the beginning of the next acoustic cycle, which brings memory into the system. We show that for some parameter values in the chaotic regime the dynamics can be reduced to a unimodal map. At th… Show more

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Cited by 29 publications
(23 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%
“…In addition, this condition was used to plot the bifurcation diagram of a cavitation bubble in [45,48]. This method continued through increasing the control parameter and the new resulting discrete points were plotted in the bifurcation diagrams versus the altered control parameters.…”
Section: Bifurcation Diagramsmentioning
confidence: 99%
“…In our analysis the following condition was used: P max R fðR; _ RÞ : _ R ¼ 0g which gives the maximal radius from each acoustic period. Also, this condition was used to plot the bifurcation diagram of a cavitation bubble in [60]. In order to generate the bifurcation points, the equation of the microbubble motion was solved numerically for 900 acoustic cycles of the lower frequency and then a Poincaré section was constructed.…”
Section: Bifurcation Diagramsmentioning
confidence: 99%