4.1 Article

Ring Vortex Dynamics Following Jet Formation of a Bubble Expanding and Collapsing Close to a Flat Solid Boundary Visualized via Dye Advection in the Framework of OpenFOAM

Journal

FLUIDS
Volume 8, Issue 7, Pages -

Publisher

MDPI
DOI: 10.3390/fluids8070200

Keywords

cavitation bubble; vortices; multiphase flow; single bubble; laser-induced cavitation; computational fluid dynamics; OpenFOAM; PIV; PTV; dye advection

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A bubble expanding and collapsing near a solid boundary induces a liquid jet towards the boundary, leaving a torus bubble and persistent vortices in the liquid. The vortices, with different rotation directions and varying amplitude, are studied numerically and compared to experiments. The study reveals a transition interval where the dominating rotational direction of the fluid flow changes, which is accompanied by increased erosion of the solid surface.
A bubble expanding and collapsing near a solid boundary develops a liquid jet toward the boundary. The jet leaves a torus bubble and induces vortices in the liquid that persist long after the bubble oscillations have ceased. The vortices are studied numerically in axial symmetry and compared to experiments in the literature. The flow field is visualized with different methods: vorticity with superimposed flow-direction arrows for maps at a time instant and colored-liquid-layer flow-field maps (dye advection) for following the complete long-term fluid flow up to a chosen time since bubble generation. Bubbles with equal energy-maximum radius in a free liquid R (infinity)max = 500 mu m-are studied for different distances D-init from the solid boundary. The interval of normalized distances D* = D-init/R (infinity)max from 0.4 to 1.8 is covered. Two types of vortices were reported in experiments, one moving toward the solid boundary and one moving away from it. This finding is reproduced numerically with higher resolution of the flow field and in more detail. The higher detail reveals that the two types of vortices have different rotation directions and coexist with individually varying vorticity amplitude throughout the interval studied. In a quite narrow part of the interval, the two types change their strength and extent with the result of a reversal of the dominating rotational direction of the fluid flow. Thereby, the experimentally found transition interval could be reproduced and refined. It is interesting to note that in the vortex transition interval, the erosion of a solid surface is strongly augmented.

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