Bulletin of the American Physical Society
71st Annual Meeting of the APS Division of Fluid Dynamics
Volume 63, Number 13
Sunday–Tuesday, November 18–20, 2018; Atlanta, Georgia
Session G05: Free-surface Flows: General
10:35 AM–12:45 PM,
Monday, November 19, 2018
Georgia World Congress Center
Room: B207
Chair: William Schultz, University of Michigan
Abstract ID: BAPS.2018.DFD.G05.8
Abstract: G05.00008 : Do drop-impact craters produce singular jets?*
12:06 PM–12:19 PM
Presenter:
Sigurdur T Thoroddsen
(King Abdullah Univ of Sci & Tech (KAUST), Saudi Arabia)
Authors:
Sigurdur T Thoroddsen
(King Abdullah Univ of Sci & Tech (KAUST), Saudi Arabia)
Kohsei Takehara
(Kindai University, Osaka, Japan)
N. D. Nguyen
(Hanoi University of Science and Technology, Hanoi, Vietnam)
T. G. Etoh
(Kindai University, Osaka, Japan)
Drop-impact craters rebound and usually produce prominent Worthington jets. For a limited range of drop-impact Weber numbers, capillary waves travel down the crater surface and a dimple forms at the bottom of the crater. This dimple can pinch off and entrap a bubble into the pool, in a process call regular bubble entrapment. This bubble oscillates and emits sound. This parameter range is also associated with the appearance of high-speed fine jets. It has been suggested that the fastest jets are driven by a singularity in the surface curvature at the bottom of the dimple. Herein we use two ultra-high-speed video cameras to simultaneously image the jetting and the dimple evolution*. Our imaging at micro-second resolution never shows any curvature singularity at the bottom of the dimple. Furthermore, the fastest jets emerge when the inertial focusing drives the jet without pinch-off of a bubble. In contrast the bottom dimple air-cylinder is pushed up at high velocity when its diameter is of the order of 25 microns, producing jets which emerge at speeds as fast as 50 m/s.
*Thoroddsen et al., J. Fluid Mech., 848, R3 (2018).
*This work was partly funded by King Abdullah University of Science and Technology (KAUST) under Grant No. URF/1/2621-01-01.
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DFD.G05.8
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