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 E03: Shock Interactions and Focusing
5:10 PM–6:28 PM,
Sunday, November 18, 2018
Georgia World Congress Center
Room: B204
Chair: Lian Duan, Missouri University of Science and Technology
Abstract ID: BAPS.2018.DFD.E03.2
Abstract: E03.00002 : Shockwave / foam film interaction*
5:23 PM–5:36 PM
Presenter:
Quentin Raimbaud
(Univ Rennes, CNRS, IPR (Institut de Physique de Rennes) - UMR 6251, F- 35000 Rennes)
Authors:
Quentin Raimbaud
(Univ Rennes, CNRS, IPR (Institut de Physique de Rennes) - UMR 6251, F- 35000 Rennes)
Martin Monloubou
(Institut de Recherche Dupuy de Lôme (IRDL — UMR CNRS 6027))
Steven Kerampran
(Institut de Recherche Dupuy de Lôme (IRDL — UMR CNRS 6027))
Isabelle Cantat
(Univ Rennes, CNRS, IPR (Institut de Physique de Rennes) - UMR 6251, F- 35000 Rennes)
Foams are very efficient to absorb shock waves, and are used in demining situations. The wave/film interaction involves complex processes (Bremond & Villermaux, J. Fluid. Mech. 2005) not fully understood yet. To elucidate the various processes leading to film rupture under shock, we produce foam films in a transparent shock tube and image them at 200000 fps, by direct visualization or ombroscopy. Deformations at a millimetric scale are observed before the film eventually ruptures, in which the film thickness heterogeneities play a crucial role : pieces of film of different thicknesses are accelerated at various rates, leading to film tear out, and only the most homogeneous films have time to destabilize via the Rayleigh Taylor instability described in the literature. The orientation of the film with respect of the incoming wave also influences the film deformation and, using dedicated film structure, we show that the tangential component of the acceleration generates wrinkling of well defined wave length. The pressure signals induced by the shock / film interaction are in good agreement with numerical simulations and show the short delay generated by the film, contributing to the wave attenuation.
*Q. Raimaud acknowledges a financial support of the DGA
To cite this abstract, use the following reference: http://meetings.aps.org/link/BAPS.2018.DFD.E03.2
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