A large gas cavity can be stably “levitated” below a gas-liquid interface by strong vertical vibrations. The gas-liquid interface breaks up under strong vertical vibrations, and the bubbles generated there move downward against buoyancy to the bottom of the container.1–3 Under proper conditions, these bubbles subsequently coalesce, and the gas cavity thus produced rises to an intermediate depth where it remains for all time. The vertical vibrations also cause the free surface of the gas cavity to break up into jets and droplets just like the gas-liquid interface above it. The downward bubble motion and the stable gas cavity below the gas-liquid interface are manifestations of the bubble Bjerknes force, which is well known at acoustic frequencies but also exists at low frequencies, for which the liquid is incompressible.3 

Experiments are performed in a thin, quasi-two-dimensional rectangular acrylic test cell (0.6 cm thick, 7.6 cm wide) subjected to sinusoidal vertical vibrations (Fig. 1). The liquid in these experiments is polydimethylsiloxane (PDMS) silicone oil, and the gas is air. The levitated gas cavity spans the cell thickness, and the gas-cavity free surface breaks up into inward-traveling jets and droplets (Figs. 2 and 3 and video). Under certain conditions, the waves on the gas-cavity free surface and the gas-liquid interface are modulated 180° out of phase (Fig. 3). The gas-cavity free surface undergoes minimal breakup under these conditions, and gas-cavity lifetimes of hours have been observed.

FIG. 1.

(Left) Experiment. (Right) Gas cavity stably levitated by vibration. Free-surface breakup generates small bubbles that descend and coalesce to form the gas cavity, which then rises to reach position of stable levitation. Liquid is 20-cSt PDMS silicone oil; gas is air. Vibration conditions are 280 Hz, 15-g peak acceleration, and 94-μm peak-to-peak displacement.

FIG. 1.

(Left) Experiment. (Right) Gas cavity stably levitated by vibration. Free-surface breakup generates small bubbles that descend and coalesce to form the gas cavity, which then rises to reach position of stable levitation. Liquid is 20-cSt PDMS silicone oil; gas is air. Vibration conditions are 280 Hz, 15-g peak acceleration, and 94-μm peak-to-peak displacement.

Close modal
FIG. 2.

Closeup showing interior of gas cavity stably levitated by vibration at conditions of Fig. 1. Breakup of its free surface sends liquid jets and droplets through its interior. The video shows it in motion (enhanced online). [URL: http://dx.doi.org/10.1063/1.4747165.1]

FIG. 2.

Closeup showing interior of gas cavity stably levitated by vibration at conditions of Fig. 1. Breakup of its free surface sends liquid jets and droplets through its interior. The video shows it in motion (enhanced online). [URL: http://dx.doi.org/10.1063/1.4747165.1]

Close modal
FIG. 3.

Breakup of gas-cavity free surface can sometimes be much weaker than in Figs. 1 and 2. Waves on gas-liquid interface and gas-cavity free surface are modulated 180° out of phase. Gas-cavity major axis is 1.2 cm. Liquid is 50-cSt PDMS; gas is air. Vibration conditions are 300 Hz, 22-g peak acceleration, and 120-μm peak-to-peak displacement. Images are 0.00197 s apart.

FIG. 3.

Breakup of gas-cavity free surface can sometimes be much weaker than in Figs. 1 and 2. Waves on gas-liquid interface and gas-cavity free surface are modulated 180° out of phase. Gas-cavity major axis is 1.2 cm. Liquid is 50-cSt PDMS; gas is air. Vibration conditions are 300 Hz, 22-g peak acceleration, and 120-μm peak-to-peak displacement. Images are 0.00197 s apart.

Close modal

Sandia National Laboratories is a multi-program laboratory managed and operated by Sandia Corporation, a wholly owned subsidiary of Lockheed Martin Corporation, for the U.S. Department of Energy's National Nuclear Security Administration under Contract No. DE-AC04-94AL85000.

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