DOI: 10.3990/1.9789036538145
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Growing bubbles and freezing drops: depletion effects and tip singularities

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Cited by 1 publication
(2 citation statements)
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“…Indeed, the radius evolution is proportional to the square root of time as expected for a diffusive growth, figure 5.3(a). However, the nominal value of the slope d /dx is lower than the theoretical one [145] and independent of d [99], caused by the influence of each bubble growing next to a neighbouring one and the rapid merging of the two concentration boundary layers [146]. In figure 5.3(b), we plot the theoretical dimensionless radius derivative (1/S * )d /dx = 1 [following the representation depicted in 34] and compare it with the experimental derivative.…”
Section: Diffusive Bubble Growthmentioning
confidence: 70%
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“…Indeed, the radius evolution is proportional to the square root of time as expected for a diffusive growth, figure 5.3(a). However, the nominal value of the slope d /dx is lower than the theoretical one [145] and independent of d [99], caused by the influence of each bubble growing next to a neighbouring one and the rapid merging of the two concentration boundary layers [146]. In figure 5.3(b), we plot the theoretical dimensionless radius derivative (1/S * )d /dx = 1 [following the representation depicted in 34] and compare it with the experimental derivative.…”
Section: Diffusive Bubble Growthmentioning
confidence: 70%
“…Because the two neighbouring growing bubbles compete for the dissolved gas, their growth is influenced by the distance d separating them [99]. However, the corresponding concentration boundary layers growing around each bubble as √ πDt merge in one concentration layer from which both bubbles absorb gas from the very early stages of the bubbles growth.…”
Section: Diffusive Bubble Growthmentioning
confidence: 99%