2021
DOI: 10.3390/molecules26051317
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The Life of a Surface Bubble

Abstract: Surface bubbles are present in many industrial processes and in nature, as well as in carbonated beverages. They have motivated many theoretical, numerical and experimental works. This paper presents the current knowledge on the physics of surface bubbles lifetime and shows the diversity of mechanisms at play that depend on the properties of the bath, the interfaces and the ambient air. In particular, we explore the role of drainage and evaporation on film thinning. We highlight the existence of two different … Show more

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Cited by 21 publications
(17 citation statements)
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“…It can remain stable in a fixed vertical position, limited by the diffusion rates of the gas from the surface‐anchored microbubbles into the bulk water and up to few hours. [ 49 ]…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…It can remain stable in a fixed vertical position, limited by the diffusion rates of the gas from the surface‐anchored microbubbles into the bulk water and up to few hours. [ 49 ]…”
Section: Resultsmentioning
confidence: 99%
“…It can remain stable in a fixed vertical position, limited by the diffusion rates of the gas from the surfaceanchored microbubbles into the bulk water and up to few hours. [49] Figure 7 shows a variety of motion patterns in the vertical direction, generated by manual control (Figure 7a,b, see also Video S2, Supporting Information) and autonomous control (Figure 7c,d). In the manual mode, the operator chooses two control signals: one for the electrodes and one for the motor generating the mechanical vibrations.…”
Section: Buoyancy Autoregulationmentioning
confidence: 99%
“…On the other end, a simple exponential distribution, approximated by b = 1 , is expected for systems where a purely stochastic mechanism such as thermal or mechanical fluctuations or hole nucleation is the dominant rupture mechanism (Casteletto et al 2003;Langevin 2020). As shown by Lhuissier and Villermaux (2012) and discussed by Miguet et al (2021), a b = 4∕3 is expected for systems containing impurities in presence of Marangoni recirculation (or to be specific marginal regeneration in their case). Finally, the b ≃ 3.6 corresponds to a symmetric distribution, which so far has been observed for films at finite Ca numbers with simple interfaces whose rupture is controlled by the evolution of spontaneously growing thickness fluctuations .…”
Section: Coalescence Time Distributionsmentioning
confidence: 86%
“…Although coalescence times and film lifetimes are typically reported with large standard deviations, as distributions, or as scattered single data points Dudek et al 2020;Mazutis and Griffiths 2012;Suja et al 2018;Dinh et al 2021;Exerowa et al 1983;Suja et al 2020;Saulnier et al 2014;Miguet et al 2021;Poulain et al 2018;Vitry et al 2019;Tian et al 2022), the origin of this scatter is rarely addressed, mostly because of the difficulties that such a practice entails (i.e., decoupling the scatter due to experimental control, extrinsic factors such as impurities, and intrinsic ones such as thermocapillary waves and surface concentration fluctuations). Here, we will investigate two of the main contributions to the scatter, namely that of extrinsic factors like impurities and variations in the collision angle.…”
Section: Quantifying Scatter In Coalescence Timementioning
confidence: 99%
“…Indeed, the film surrounding surface bubbles has been proven to thin down to a few tens of nanometers, the thickness at which bursting occurs. To understand and to be able to predict the lifetime of these bubbles, it is therefore necessary to consider their thinning dynamics [6].…”
Section: Introductionmentioning
confidence: 99%