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Oscillations, Waves, and Interactions - GWDG

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(a) 1 mm<br />

(b)<br />

Acoustic cavitation 175<br />

Figure 3. Nucleation from the bulk liquid into streamers in a 20 kHz sound field (two<br />

frames from a high-speed recording, exposure time 1.5 µs). Several streamer sources on<br />

frame (a) change into a single one on frame (b) within the interframe time of 30 ms.<br />

it can form a spatially stable source of a continuous bubble stream. To control such<br />

attached bubble sources can be one way of a cavitation structure control [10].<br />

Examples of microbubble generation are shown later in Figs. 7 <strong>and</strong> 9. The process<br />

of repetitive ejection seems to be a common cavitation bubble source if objects or<br />

walls are contributing, <strong>and</strong> for a complete description, gas diffusion into such source<br />

bubbles has to be taken into account. The attached bubbles might even be very<br />

small, as recent investigations on “nano-bubbles” suggest [11].<br />

3 Bubble dynamics<br />

Once a bubble is created in the liquid, it will show variations of size <strong>and</strong> possibly<br />

shape as a reaction to the sound field. On a longer time scale, translational <strong>and</strong><br />

diffusional processes can take place. From the point of view of a single, individual<br />

bubble, these issues are captured by the term bubble dynamics. A very useful model<br />

for investigation of bubble dynamics is a spherical gas <strong>and</strong> vapour bubble. Here it<br />

is usually assumed that the gas inside the bubble is non-condensable (<strong>and</strong> thus its<br />

mass is conserved, at least on a fast time scale), <strong>and</strong> the vapour is instantaneously<br />

evaporating or condensing at the bubble walls, leading always to the equilibrium<br />

vapour pressure inside. 3 The presence of a non-condensable gas (in many cases air)<br />

can be questioned, but keeping in mind the nucleation mechanism from stabilized<br />

micro (or nano) gas bubbles, this assumption usually makes sense. 4 Indeed, an<br />

3 Refinements of this model include gas diffusion <strong>and</strong> vapour evaporation <strong>and</strong> condensation<br />

dynamics, but they lead in many parameter regimes in water to rather small corrections.<br />

They are important for a good description of the collapse, which is not central here, <strong>and</strong><br />

thus they are neglected in the following.<br />

4 Of course, also pure vapour cavitation might be encountered in some situations, like<br />

in liquid helium [12]. However, here we are dealing mainly with water-air systems under<br />

normal conditions.

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