Numerical modeling of 3D turbulent free surface flow in natural waterways

Abstract We develop a numerical model capable of simulating three-dimensional, turbulent free surface flows in natural waterways. Free surface motion is captured by coupling the two-phase level set method and the sharp-interface curvilinear immersed boundary (CURVIB) method of Kang et al. [1] . The model solves the three-dimensional, incompressible, unsteady Reynolds-averaged Navier–Stokes (RANS) and continuity equations in generalized curvilinear coordinates using a fractional step method extended to handle multiphase flows. Turbulence is modeled by a two-equation RANS model implemented in the context of the CURVIB method. The accuracy of the level set method is verified by applying it to simulate two- and three-dimensional sloshing problems, and the potential of the model for simulating real life, turbulent free surface flows is demonstrated by applying it to carry out RANS simulation of flow past rock structures in a laboratory flume and flow in a field scale meandering channel. The simulations show that the method is able to accurately predict water surface elevation over complex hydraulic structures and bathymetry, and capture the transition between subcritical and supercritical flows without any special treatment.

[1]  Robert L. Street,et al.  On Simulation of Turbulent Nonlinear Free-Surface Flows , 1999 .

[2]  Catherine Wilson,et al.  Application of a 3D numerical model to a river with vegetated floodplains , 2003 .

[3]  D. L. Rosgen,et al.  The Cross-Vane, W-Weir and J-Hook Vane Structures…Their Description, Design and Application for Stream Stabilization and River Restoration , 2001 .

[4]  G. Tryggvason,et al.  A front-tracking method for viscous, incompressible, multi-fluid flows , 1992 .

[5]  Chi-Wang Shu,et al.  Efficient Implementation of Weighted ENO Schemes , 1995 .

[6]  Tae Hoon Yoon,et al.  Finite volume model for two-dimensional shallow water flows on unstructured grids , 2004 .

[7]  Fotis Sotiropoulos,et al.  A numerical method for solving the 3D unsteady incompressible Navier-Stokes equations in curvilinear domains with complex immersed boundaries , 2007, J. Comput. Phys..

[8]  V. C. Patel,et al.  Large eddy simulation of turbulent open-channel flow with free surface simulated by level set method , 2005 .

[9]  F. Sotiropoulos,et al.  Flow phenomena and mechanisms in a field‐scale experimental meandering channel with a pool‐riffle sequence: Insights gained via numerical simulation , 2011 .

[10]  I. Borazjani,et al.  On the role of form and kinematics on the hydrodynamics of self-propelled body/caudal fin swimming , 2010, Journal of Experimental Biology.

[11]  J. Katz,et al.  On the role of copepod antennae in the production of hydrodynamic force during hopping , 2010, Journal of Experimental Biology.

[12]  I. Borazjani,et al.  Numerical investigation of the hydrodynamics of carangiform swimming in the transitional and inertial flow regimes , 2008, Journal of Experimental Biology.

[13]  M. Hanif Chaudhry,et al.  Depth-averaged open-channel flow model , 1995 .

[14]  S. Osher,et al.  An improved level set method for incompressible two-phase flows , 1998 .

[15]  Fotis Sotiropoulos,et al.  Curvilinear immersed boundary method for simulating coupled flow and bed morphodynamic interactions due to sediment transport phenomena , 2011 .

[16]  Reinaldo García,et al.  Numerical solution of the St. Venant equations with the MacCormack finite‐difference scheme , 1986 .

[17]  Amruthur S. Ramamurthy,et al.  Numerical and experimental study of dividing open-channel flows , 2007 .

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

[19]  D. L. Young,et al.  Arbitrary Lagrangian-Eulerian finite element analysis of free surface flow using a velocity-vorticity formulation , 2004 .

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

[21]  F. Sotiropoulos,et al.  High-resolution numerical simulation of turbulence in natural waterways , 2011 .

[22]  M. Kawahara,et al.  Arbitrary Lagrangian–Eulerianc finite element method for unsteady, convective, incompressible viscous free surface fluid flow , 1987 .

[23]  R. Eatock Taylor,et al.  Finite element analysis of two-dimensional non-linear transient water waves , 1994 .

[24]  V. C. Patel,et al.  Numerical simulation of unsteady multidimensional free surface motions by level set method , 2003 .

[25]  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..

[26]  Seungwon Shin,et al.  Modeling three-dimensional multiphase flow using a level contour reconstruction method for front tracking without connectivity , 2002 .

[27]  Pengzhi Lin,et al.  A numerical study of breaking waves in the surf zone , 1998, Journal of Fluid Mechanics.

[28]  D. Juric,et al.  A front-tracking method for the computations of multiphase flow , 2001 .

[29]  Frederick Stern,et al.  An unsteady single‐phase level set method for viscous free surface flows , 2007 .

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

[31]  G. Wei,et al.  Time-Dependent Numerical Code for Extended Boussinesq Equations , 1995 .

[32]  Frederick Stern,et al.  Sharp interface immersed-boundary/level-set method for wave-body interactions , 2009, J. Comput. Phys..

[33]  Qun Chen,et al.  Volume of Fluid Model for Turbulence Numerical Simulation of Stepped Spillway Overflow , 2002 .

[34]  H. Schlichting Boundary Layer Theory , 1955 .