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Jetting enhancement from wall-proximal cavitation bubbles by a distant wall
by
An, Hongjie
, Zeng, Qingyun
, Ohl, Claus-Dieter
, Zhang, A-Man
, Tan, Beng Hau
in
Atmospheric pressure
/ Bubbles
/ Cameras
/ Cavitation
/ Distance
/ Experiments
/ Flow velocity
/ High speed photography
/ JFM Rapids
/ Lasers
/ Photography
/ Simulation
/ Velocity
/ Viscosity
2024
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Jetting enhancement from wall-proximal cavitation bubbles by a distant wall
by
An, Hongjie
, Zeng, Qingyun
, Ohl, Claus-Dieter
, Zhang, A-Man
, Tan, Beng Hau
in
Atmospheric pressure
/ Bubbles
/ Cameras
/ Cavitation
/ Distance
/ Experiments
/ Flow velocity
/ High speed photography
/ JFM Rapids
/ Lasers
/ Photography
/ Simulation
/ Velocity
/ Viscosity
2024
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While trying to remove the title from your shelf something went wrong :( Kindly try again later!
Do you wish to request the book?
Jetting enhancement from wall-proximal cavitation bubbles by a distant wall
by
An, Hongjie
, Zeng, Qingyun
, Ohl, Claus-Dieter
, Zhang, A-Man
, Tan, Beng Hau
in
Atmospheric pressure
/ Bubbles
/ Cameras
/ Cavitation
/ Distance
/ Experiments
/ Flow velocity
/ High speed photography
/ JFM Rapids
/ Lasers
/ Photography
/ Simulation
/ Velocity
/ Viscosity
2024
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Jetting enhancement from wall-proximal cavitation bubbles by a distant wall
Journal Article
Jetting enhancement from wall-proximal cavitation bubbles by a distant wall
2024
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Overview
An additional distant wall is known to highly alter the jetting scenarios of wall-proximal bubbles. Here, we combine high-speed photography and axisymmetric volume of fluid (VoF) simulations to quantitatively describe its role in enhancing the micro-jet dynamics within the directed jet regime (Zeng et al., J. Fluid Mech., vol. 896, 2020, A28). Upon a favourable agreement on the bubble and micro-jet dynamics, both experimental and simulation results indicate that the micro-jet velocity increases dramatically as $\\eta$ decreases, where $\\eta =H/R_{max}$ is the distance between two walls $H$ normalized by the maximum bubble radius $R_{max}$. The mechanism is related to the collapsing flow, which is constrained by the distant wall into a reverse stagnation-point flow that builds up pressure near the bubble's top surface and accelerates it into micro-jets. We further derive an equation expressing the micro-jet velocity $U_{jet}=87.94\\gamma ^{0.5}(1+(1/3)(\\eta -\\lambda ^{1.2})^{-2})$, where ${\\gamma =d/R_{max}}$ is the stand-off distance to the proximal wall with $d$ the distance between the initial bubble centre and the wall, $\\lambda =R_{y,m}/R_{max}$ with $R_{y,m}$ the distance between the top surface and the proximal wall at the bubble's maximum expansion. Viscosity has a minimal impact on the jet velocity for small $\\gamma$, where the pressure buildup is predominantly influenced by geometry.
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