2012
DOI: 10.1063/1.4769179
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Oscillations of a gas pocket on a liquid-covered solid surface

Abstract: The dynamic response of a gas bubble entrapped in a cavity on the surface of a submerged solid subject to an acoustic field is investigated in the linear approximation. We derive semi-analytical expressions for the resonance frequency, damping and interface shape of the bubble. For the liquid phase, we consider two limit cases: potential flow and unsteady Stokes flow. The oscillation frequency and interface shape are found to depend on two dimensionless parameters: the ratio of the gas stiffness to the surface… Show more

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Cited by 19 publications
(27 citation statements)
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References 19 publications
(25 reference statements)
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“…The driving frequency is approximately twice the linear resonance frequency (98 kHz) of the pit and lies below the first higher harmonic of 243 kHz [36]. Similar to previous observations, there is a threshold for the pressure above which bubble pinch-off occurs corresponding to an input power of 50 mW.…”
Section: Driving At 200 Khzsupporting
confidence: 85%
See 1 more Smart Citation
“…The driving frequency is approximately twice the linear resonance frequency (98 kHz) of the pit and lies below the first higher harmonic of 243 kHz [36]. Similar to previous observations, there is a threshold for the pressure above which bubble pinch-off occurs corresponding to an input power of 50 mW.…”
Section: Driving At 200 Khzsupporting
confidence: 85%
“…In comparison, the resonance frequencies for the first and second surface mode for this pit are 139 kHz and 276 kHz respectively, based on linear potential flow analysis [36]. This explains the larger amplitude response of the pit bubble compared to that of the ejected bubbles.…”
Section: Discussionmentioning
confidence: 81%
“…The resonance frequency of the pits is of the order of 150 kHz and the radius of bubbles resonating at the applied frequency of 200 kHz is about 15 lm [44,45]. Thus one would expect that, under the action of Bjerknes forces, bubbles smaller than this size would be repelled by the pits while larger ones would be attracted.…”
Section: Description Of the Observed Phenomenamentioning
confidence: 99%
“…This however requires both (i) a resolution of the axial oscillation mode amplitudes A mn as functions of frequency (see e.g. Gelderblom et al 2012;Wang et al 2013), and (ii) a detailed description of both oscillatory and steady no-stress boundary layers due to these flow modes, accurate up to O(δ 2 ) (see e.g. Davidson & Riley 1971;Longuet-Higgins 1998;Rallabandi et al 2014).…”
mentioning
confidence: 99%