TY - JOUR
T1 - Bubble Bursting
T2 - Universal Cavity and Jet Profiles
AU - Lai, Ching Yao
AU - Eggers, Jens
AU - Deike, Luc
N1 - Publisher Copyright:
© 2018 American Physical Society.
PY - 2018/10/2
Y1 - 2018/10/2
N2 - After a bubble bursts at a liquid surface, the collapse of the cavity generates capillary waves, which focus on the axis of symmetry to produce a jet. The cavity and jet dynamics are primarily controlled by a nondimensional number that compares capillary inertia and viscous forces, i.e., the Laplace number La=ργR0/μ2, where ρ, μ, γ, and R0 are the liquid density, viscosity, interfacial tension, and the initial bubble radius, respectively. In this Letter, we show that the time-dependent profiles of cavity collapse (tt0) both obey a |t-t0|2/3 inviscid scaling, which results from a balance between surface tension and inertia forces. Moreover, we present a scaling law, valid above a critical Laplace number, which reconciles the time-dependent scaling with the recent scaling theory that links the Laplace number to the final jet velocity and ejected droplet size. This leads to a self-similar formula which describes the history of the jetting process, from cavity collapse to droplet formation.
AB - After a bubble bursts at a liquid surface, the collapse of the cavity generates capillary waves, which focus on the axis of symmetry to produce a jet. The cavity and jet dynamics are primarily controlled by a nondimensional number that compares capillary inertia and viscous forces, i.e., the Laplace number La=ργR0/μ2, where ρ, μ, γ, and R0 are the liquid density, viscosity, interfacial tension, and the initial bubble radius, respectively. In this Letter, we show that the time-dependent profiles of cavity collapse (tt0) both obey a |t-t0|2/3 inviscid scaling, which results from a balance between surface tension and inertia forces. Moreover, we present a scaling law, valid above a critical Laplace number, which reconciles the time-dependent scaling with the recent scaling theory that links the Laplace number to the final jet velocity and ejected droplet size. This leads to a self-similar formula which describes the history of the jetting process, from cavity collapse to droplet formation.
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U2 - 10.1103/PhysRevLett.121.144501
DO - 10.1103/PhysRevLett.121.144501
M3 - Article
C2 - 30339416
AN - SCOPUS:85054477465
SN - 0031-9007
VL - 121
JO - Physical review letters
JF - Physical review letters
IS - 14
M1 - 144501
ER -