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Oscillations, Waves, and Interactions - GWDG

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174 R. Mettin<br />

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Figure 2. Free nucleation into a cluster in a 20 kHz sound field (high-speed recording<br />

with 1000 frames per second (fps), exposure time 1.5 µs). An object that appears as a germ<br />

bubble (arrow first frame) develops into a conglomerate of bubbles that travels to the right.<br />

The visibility of the cluster changes, because the relative phase of the sub-period exposure<br />

time is drifting from frame to frame, <strong>and</strong> the cluster bubbles oscillate with strong volume<br />

changes. On some frames they are close to collapse <strong>and</strong> too small to be resolved.<br />

observed similar events [8] <strong>and</strong> termed them “comets”. Possibly they are triggered<br />

by an advected microbubble, or ionizing particle radiation.<br />

Another typical picture of nucleation is shown in Fig. 3. A quasi-continuous stream<br />

of small bubbles appears out of the bulk, forming a trail of bubbles, or a “streamer”.<br />

Bubbles travel along directional paths from the invisible source in the liquid towards<br />

junctions with other streamers, which causes a dendritic form. The invisible sources<br />

of bubbles remain active over many acoustic cycles. Probably, invisible sub-micron<br />

bubbles, stabilized or from degassing processes in the liquid, migrate to the apparent<br />

bubble source <strong>and</strong> merge to visible size, feeding the stream of bubbles.<br />

Further sources of small bubbles are larger ones: driven by the acoustic field, they<br />

can undergo surface instabilities. By pinch-off or even by apparent “explosions” [9]<br />

one or many daughter bubbles can be produced. The generating bubble may be<br />

freely floating in the liquid, or be attached to an immersed object or a wall. If fixed,

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