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Here, y is the distance from the bubble--liquid interface. The upper curve corresponds to peak center temperature while the lower curve indicates the temperature profile at maximum expansion. The predicted temperature increase of the liquid in a shell adjacent to the bubble is -+40 K. 5 x 105 K/ram. (After Kamath et al. ) of chemical equations (the case of an air bubble)--was carried out by Yasui [65]. 1). 4 Supersonic Collapse: The Formation of a Converging Shock Wave In the preceding paragraphs, it was assumed that the intracavity pressure was uniform on collapse.

9 9 . ~ i ........................... ; [......................... i............. ~9 , . . . e ........! -" i .......................... ~ i ...................................................... ......................... ~ ............. " i . 91 ! " ............. : " i : i ~ ........................... " ............. : . . . . . . ... . . . . . . 9 ~ ............. : -. : , .. : i i .. " ............. : , (a) =14,111 ' ' ..... o (b) , , Figure 26. 5 kHz. 1 its. (b) Blow-up of the last frame of (a).

49]. For Pac which is likely to induce SL with a single bubble or in stable (multibubble) cavitation, the bubble expansion is greater and greater as the initial bubble radius becomes close to Rres/100 (Figure 10). At 20 kI-Iz the resolution of the RP equation modified according to Prosperetti et al. [49] indicates that the most violent type of collapse should be a characteristic of bubbles which start to grow from an initial radius of about 2 gm (by way of comparison, the resonance radius determined via Minneart's law [Eq.

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