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Oscillations, Waves, and Interactions - GWDG

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Dynamics of pulsed laser tissue ablation 225<br />

Figure 5. (a) Development of a thermoelastic stress wave in water calculated for F0 =<br />

2 J/cm 2 ; µa = 200 cm −1 <strong>and</strong> tp = 8 ns. (b) Pressure as a function of time at a depth of<br />

50 µm. (Reprinted with permission from Ref. [45]. Copyright 1996 Springer).<br />

tochemical mechanisms. In this article, we focus on the kinetics of phase transitions<br />

in purely photothermal ablation processes such as in IR ablation. When UV lasers<br />

are used, photochemical bond dissociation may contribute to ablation. For a detailed<br />

discussion of the role of these photochemical processes, the reader is referred to a<br />

recent review by two of the authors [6].<br />

4.1 Phase diagrams<br />

We use the pressure vs. temperature projection of the phase diagram for liquid <strong>and</strong><br />

gaseous water (Fig. 6) <strong>and</strong> the pressure vs. specific volume projection of the thermodynamic<br />

phase diagram (Fig. 7) to discuss the thermodynamics of phase transitions.<br />

The solid curve A–C on Fig. 6 represents those pressure/temperature pairs where<br />

liquid <strong>and</strong> gaseous water are in equilibrium with each other <strong>and</strong> is known as the<br />

“binodal”. The curve B–C–D, the “spinodal”, denotes a locus of states with infinite

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