2009
DOI: 10.1016/j.ultsonch.2008.11.013
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Nonlinear ultrasonic waves in bubbly liquids with nonhomogeneous bubble distribution: Numerical experiments

Abstract: This paper deals with the nonlinear propagation of ultrasonic waves in mixtures of air bubbles in water, but for which the bubble distribution is nonhomogeneous. The problem is modelled by means of a set of differential equations which describes the coupling of the acoustic field and bubbles vibration, and solved in the time domain via the use and adaptation of the SNOW-BL code. The attenuation and nonlinear effects are assumed to be due to the bubbles exclusively. The nonhomogeneity of the bubble distribution… Show more

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Cited by 32 publications
(17 citation statements)
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“…The predictions are in reasonable agreement with the experimental results of Mark et al [93]. Other interpretations are linked to the self-attenuation of the acoustic field near the sonotrode tip: larger excitations produce more numerous and violently oscillating bubbles, which may act as a screen for the acoustic waves [94], and dissipate a larger energy [95].…”
Section: Influence Of the Ultrasonic Powersupporting
confidence: 83%
“…The predictions are in reasonable agreement with the experimental results of Mark et al [93]. Other interpretations are linked to the self-attenuation of the acoustic field near the sonotrode tip: larger excitations produce more numerous and violently oscillating bubbles, which may act as a screen for the acoustic waves [94], and dissipate a larger energy [95].…”
Section: Influence Of the Ultrasonic Powersupporting
confidence: 83%
“…This fact has already been observed by the authors in other numerical and experimental works referred to bubbly media [16,9], in particular when waves interferences occur [17,10,13]. The nonlinear bubble vibration strongly affects the distribution of energy in the frequency domain but not the distribution of energy in space, which remains highly concentrated at the focus.…”
Section: Examplesupporting
confidence: 54%
“…The differential system is solved following the 2-D finite-differences scheme given in [14], except for boundary conditions (2), and included in the SNOW-BL code [9,15,10,13]. In this case the dimensionless variables are X = x/X fl , Y = y/, and Τ = co f t, where λ β =c 0l / f is the wavelength in the liquid at the driving frequency.…”
Section: Modelmentioning
confidence: 99%
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“…Correct wave equations are thereby essential for a sufficient understanding of the physics governing the wave behavior. A number of theoretical studies have intensively been performed (Kuznetsov et al, 1978;Commander and Prosperetti, 1989;Nigmatulin, 1991;Gumerov, 1992;Nakoryakov et al, 1993;Akhatov et al, 1996;Khismatullin and Akhatov, 2001;Liang et al, 2008;Vanhille and Campos-Pozuelo, 2009;Ando et al, 2011;Leroy et al, 2011;Grandjean et al, 2012;Louisnard, 2012;Sinelshchikov, 2013, 2014, to name a few), and various nonlinear wave equations describing weakly nonlinear phenomena were submitted. The KdVB equation (e.g., van Wijngaarden, 1968van Wijngaarden, , 1972 and the nonlinear Schr€ odinger (NLS) equation (e.g., Gumerov, 1992;Akhatov et al, 1996) are two well-known nonlinear equations for plane waves in uniform bubbly liquids.…”
Section: Introductionmentioning
confidence: 99%