Hybrid Hamilton–Jacobi–Poisson wall distance function model

Abstract Expensive to compute wall distances are used in key turbulence models and also for the modeling of peripheral physics. A potentially economical, robust, readily parallel processed, accuracy improving, differential equation based distance algorithm is described. It is hybrid, partly utilising an approximate Poisson equation. This also allows auxiliary front propagation direction/velocity information to be estimated, effectively giving wall normals. The Poisson normal can be used fully, in an approximate solution of the eikonal equation (the exact differential equation for wall distance). Alternatively, a weighted fraction of this Poisson front direction (effectively, front velocity, in terms of the eikonal equation input) information and that implied by the eikonal equation can be used. Either results in a hybrid Poisson–eikonal wall distance algorithm. To improve compatibility of wall distance functions with turbulence physics a Laplacian is added to the eikonal equation. This gives what is termed a Hamilton–Jacobi equation. This hybrid Poisson–Hamilton–Jacobi approach is found to be robust on poor quality grids. The robustness largely results from the elliptic background presence of the Poisson equation. This elliptic component prevents fronts propagated from solid surfaces, by the hyperbolic eikonal equation element, reflecting off zones of rapidly changing grid density. Where this reflection (due to poor grid quality) is extreme, the transition of front velocity information from the Poisson to Hamilton–Jacobi equation can be done more gradually. Consistent with turbulence modeling physics, under user control, the hybrid equation can overestimate the distance function strongly around convex surfaces and underestimate it around concave. If the former trait is not desired the current approach is amenable to zonalisation. With this, the Poisson element is automatically removed around convex geometry zones.

[1]  J. A. Sethian,et al.  Fast Marching Methods , 1999, SIAM Rev..

[2]  Michel Deville,et al.  On predicting the turbulence‐induced secondary flows using nonlinear k‐ε models , 1996 .

[3]  M. Hafez,et al.  Frontiers of Computational Fluid Dynamics 2002 , 2001 .

[4]  Paul G. Tucker,et al.  Turbulence modeling for flows around convex features giving rapid eddy distortion , 2007 .

[5]  A. N. Secundov,et al.  Generalization of νt-92 Turbulence Model for Shear-Free and Stagnation Point Flows , 2001 .

[6]  C. Rumsey,et al.  Transport Equation Based Wall Distance Computations Aimed at Flows with Time-Dependent Geometry , 2013 .

[7]  H. Xia,et al.  Finite volume distance field and its application to medial axis transforms , 2010 .

[8]  B. Launder,et al.  Progress in the development of a Reynolds-stress turbulence closure , 1975, Journal of Fluid Mechanics.

[9]  David A. Boger,et al.  Efficient Method for Calculating Wall Proximity , 2001 .

[10]  Philippe R. Spalart,et al.  Trends in turbulence treatments , 2000 .

[11]  Paul G. Tucker,et al.  Computations of Wall Distances Based on Differential Equations , 2005 .

[12]  M. Wolfshtein The velocity and temperature distribution in one-dimensional flow with turbulence augmentation and pressure gradient , 1969 .

[13]  Laurence B. Wigton Optimizing CFD Codes and Algorithms for use on Cray Computers , 1998 .

[14]  Wolfgang Schröder,et al.  A differential equation for approximate wall distance , 2002 .

[15]  Paul G. Tucker,et al.  Wall distance calculation using the Eikonal/Hamilton‐Jacobi equations on unstructured meshes: A finite element approach , 2010 .

[16]  F. Menter Improved two-equation k-omega turbulence models for aerodynamic flows , 1992 .

[17]  Paul G. Tucker,et al.  Differential equation-based wall distance computation for DES and RANS , 2003 .

[18]  Franck Nicoud,et al.  An approach to wall modeling in large-eddy simulations , 2000 .

[19]  H. Lomax,et al.  Thin-layer approximation and algebraic model for separated turbulent flows , 1978 .

[20]  T. Barth,et al.  A one-equation turbulence transport model for high Reynolds number wall-bounded flows , 1990 .

[21]  Paul G. Tucker,et al.  Unstructured Grid Solution of the Eikonal Equation for Acoustics , 2009 .

[22]  P. Spalart A One-Equation Turbulence Model for Aerodynamic Flows , 1992 .