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. 2014 Jun 25;4:5445. doi: 10.1038/srep05445

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(A) Maximum temperature rise ΔT as a function of the laser pulse energy (E_laser) for both chamber geometries. (B) Half width at half maximum of the initial temperature distribution after the bubble collapse (W₀). (C) Maximum bubble radius R_max as a function of laser energy obtained from experiments in bright field at 450,000 fps. The dashed lines, , where a is the constant. Inset: sample of high speed video frames of a single cavitation event (microfluidic gap). (D) Time it takes the maximum temperature to drop by 1/e (τ) as a function of E_laser. Thin liquid gap: black circles, semi-infinite liquid: red triangles.

Inline graphic — (A) Maximum temperature rise ΔT as a function of the laser pulse energy (E_laser) for both chamber geometries. (B) Half width at half maximum of the initial temperature distribution after the bubble collapse (W₀). (C) Maximum bubble radius R_max as a function of laser energy obtained from experiments in bright field at 450,000 fps. The dashed lines, , where a is the constant. Inset: sample of high speed video frames of a single cavitation event (microfluidic gap). (D) Time it takes the maximum temperature to drop by 1/e (τ) as a function of E_laser. Thin liquid gap: black circles, semi-infinite liquid: red triangles.