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Oscillations, Waves, and Interactions - GWDG

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2.3 Response curves<br />

The single bubble – a hot microlaboratory 143<br />

Oscillators are often described by response curves. In linear systems the amplitude of<br />

the (then sinusoidal) steady state oscillation is plotted versus the driving frequency<br />

to give the amplitude response curve or resonance curve. It shows just one peak,<br />

the resonance, when the damping is sufficiently small. With nonlinear oscillators<br />

this main resonance starts to lean over to higher or lower frequencies of the driving,<br />

eventually developing hysteresis, where there exist two steady states at the same<br />

frequency of the driving each with its own basin of attraction (set of initial conditions)<br />

leading to the respective steady state (attractor). Such basins can be found in<br />

Parlitz et al. [10]. Moreover, additional resonances appear at or near rational numbers<br />

of the ratio of driving frequency <strong>and</strong> linear resonance frequency of the bubble,<br />

called harmonic resonances, subharmonics resonances <strong>and</strong> ultraharmonic (or ultrasubharmonic)<br />

resonances [6]. They also may show hysteresis. And even more, period<br />

doubling sets in along with the resonances with incomplete (“period bubbling”) <strong>and</strong><br />

complete routes to chaos.<br />

Figure 3 shows a set of response curves with the bubble radius at rest as the control<br />

parameter instead of the driving sound field frequency. The maximum relative<br />

response, (Rmax − Rn)/Rn, for a driving frequency of 20 kHz <strong>and</strong> for sound pressure<br />

amplitudes from 10 to 70 kPa is plotted versus Rn. The emerging peaks are<br />

resonances that can be labelled with two numbers, the torsion number <strong>and</strong> the period<br />

number (both natural numbers) [6,10]. Two sets of resonances are to be seen:<br />

the large peaks that fall off towards lower radii, labeled with a ‘1’ in the denomi-<br />

(Rmax - Rn) / Rn<br />

1.6<br />

1.4<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

70 kPa<br />

3/1<br />

4/1<br />

5/1<br />

6/1<br />

0<br />

10 20 50 100 200 500<br />

Rn [ µm ]<br />

Figure 3. Response curves for bubbles of different sizes subject to driving at a fixed<br />

frequency of 20 kHz. Driving amplitudes are 10 (bottom curve), 30, 50, <strong>and</strong> 70 kPa (upper<br />

curve). Initial condition is the respective bubble at rest. The logarithmic radius scale<br />

stretches the harmonic resonances for better viewing.<br />

5/2<br />

2/1<br />

3/2<br />

1/1<br />

1/2

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