Free-surface flows under impacting droplets

A numerical method which fulfils the free-surface boundary conditions and extrapolates the fluid velocity into empty grid cells outside the fluid region on a fixed Cartesian grid system is presented. The complex, three-dimensional, vortex structures formed via surface/vortex interaction and induction between vortices have been computed using the proposed technique implemented within a level-set method for both vertical and oblique droplet impacts in incompressible fluids. The present results have been validated through numerical tests which confirm zero tangential shear at the free-surface and comparisons with experimental observations of cavity and vortex ring formation underneath the impact location. In some cases, transitions from a concentric vortex ring to a fully three-dimensional vortex structure has been confirmed. Whilst the primary vortex ring is initiated at the highly curved contact surface between the droplet and receiving surface, azimuthal instabilities are manifested in the shear layer around the cavity crater developing after the vertical impact, resulting in axial counter-rotating vorticity between the cavity and descending vortex ring. Underlying mechanisms which induce local deformation of the free-surface, creating a so-called scar, due to the sub-surface vortices at the oblique impacts are also discussed.

[1]  Djamel Lakehal,et al.  Large-eddy simulation of sheared interfacial flow , 2006 .

[2]  S. Osher,et al.  A Level Set Formulation of Eulerian Interface Capturing Methods for Incompressible Fluid Flows , 1996 .

[3]  Murray Rudman,et al.  An investigation of the flow regimes resulting from splashing drops , 2000 .

[4]  S. Zaleski,et al.  DIRECT NUMERICAL SIMULATION OF FREE-SURFACE AND INTERFACIAL FLOW , 1999 .

[5]  Pierre Lubin,et al.  Three-dimensional Large Eddy Simulation of air entrainment under plunging breaking waves , 2006 .

[6]  A. Yarin Drop Impact Dynamics: Splashing, Spreading, Receding, Bouncing ... , 2006 .

[7]  Erik Damgaard Christensen,et al.  Large eddy simulation of breaking waves , 2001 .

[8]  Gretar Tryggvason,et al.  Direct numerical simulations of bubbly flows. Part 1. Low Reynolds number arrays , 1998, Journal of Fluid Mechanics.

[9]  Luis Gustavo Nonato,et al.  A front-tracking/front-capturing method for the simulation of 3D multi-fluid flows with free surfaces , 2004 .

[10]  S. Orszag,et al.  Renormalization group analysis of turbulence. I. Basic theory , 1986 .

[11]  Mark Sussman,et al.  An Efficient, Interface-Preserving Level Set Redistancing Algorithm and Its Application to Interfacial Incompressible Fluid Flow , 1999, SIAM J. Sci. Comput..

[12]  K. Roesner,et al.  Regimes of drop morphology in oblique impact on deep fluids , 2005, Journal of Fluid Mechanics.

[13]  S. Osher,et al.  Algorithms Based on Hamilton-Jacobi Formulations , 1988 .

[14]  L. Leng Splash formation by spherical drops , 2001, Journal of Fluid Mechanics.

[15]  Pierre Sagaut,et al.  Towards large eddy simulation of isothermal two-phase flows: Governing equations and a priori tests , 2007 .

[16]  Robert L. Street,et al.  A computer study of finite-amplitude water waves , 1970 .

[17]  Stéphane Popinet,et al.  Bubble collapse near a solid boundary: a numerical study of the influence of viscosity , 2002, Journal of Fluid Mechanics.

[18]  C. W. Hirt,et al.  Volume of fluid (VOF) method for the dynamics of free boundaries , 1981 .

[19]  S. Zaleski,et al.  Volume-of-Fluid Interface Tracking with Smoothed Surface Stress Methods for Three-Dimensional Flows , 1999 .

[20]  Hiroshi Saeki,et al.  Three-dimensional vortex structures under breaking waves , 2005, Journal of Fluid Mechanics.

[21]  S. Osher,et al.  A level set approach for computing solutions to incompressible two-phase flow , 1994 .

[22]  M. Longuet-Higgins,et al.  Capillary rollers and bores , 1992, Journal of Fluid Mechanics.

[23]  S. Osher,et al.  A Non-oscillatory Eulerian Approach to Interfaces in Multimaterial Flows (the Ghost Fluid Method) , 1999 .

[24]  S. Osher,et al.  Spatially adaptive techniques for level set methods and incompressible flow , 2006 .

[25]  Lorenz Sigurdson,et al.  The three-dimensional vortex structure of an impacting water drop , 1994 .

[26]  Hiroshi Saeki,et al.  Velocity field after wave breaking , 2002 .

[27]  H. K. Moffatt,et al.  Free-surface cusps associated with flow at low Reynolds number , 1992, Journal of Fluid Mechanics.

[28]  S. Orszag,et al.  Renormalization group analysis of turbulence. I. Basic theory , 1986, Physical review letters.

[29]  J. Sethian,et al.  Fronts propagating with curvature-dependent speed: algorithms based on Hamilton-Jacobi formulations , 1988 .

[30]  S. Zaleski,et al.  Droplet splashing on a thin liquid film , 2003 .

[31]  Jinhee Jeong,et al.  On the identification of a vortex , 1995, Journal of Fluid Mechanics.

[32]  Hiroshi Saeki,et al.  Three-Dimensional Large Eddy Simulation of Breaking Waves , 1999 .