Wall modeling via function enrichment: Extension to detached-eddy simulation

Abstract We extend the approach of wall modeling via function enrichment to detached-eddy simulation. The wall model aims at using coarse cells in the near-wall region by modeling the velocity profile in the viscous sublayer and log-layer. In our approach however, unlike other wall models, the full Navier–Stokes equations are still discretely satisfied, including the pressure gradient and convective term. This is achieved by enriching the elements of the high-order discontinuous Galerkin method with the law-of-the-wall. As a result, the Galerkin method can “choose” the optimal solution among the polynomial and enrichment shape functions. The detached-eddy simulation methodology provides a suitable turbulence model for the coarse near-wall cells. The approach is applied to wall-modeled LES of turbulent channel flow in a wide range of Reynolds numbers. Flow over periodic hills shows the superiority compared to an equilibrium wall model under separated flow conditions.

[1]  U. Piomelli Wall-layer models for large-eddy simulations , 2008 .

[2]  Wolfgang A. Wall,et al.  Direct Numerical Simulation of Flow over Periodic Hills up to ReH=10,595\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document} , 2018, Flow, Turbulence and Combustion.

[3]  David Wells,et al.  The deal.II library, version 8.5 , 2013, J. Num. Math..

[4]  Michael Manhart,et al.  Flow over periodic hills: an experimental study , 2011 .

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

[6]  Benjamin Krank,et al.  Wall Modeling via Function Enrichment for Computational Fluid Dynamics , 2019 .

[7]  Katharina Kormann,et al.  A generic interface for parallel cell-based finite element operator application , 2012 .

[8]  Wolfgang A. Wall,et al.  A new approach to wall modeling in LES of incompressible flow via function enrichment , 2015, J. Comput. Phys..

[9]  P. Spalart Comments on the feasibility of LES for wings, and on a hybrid RANS/LES approach , 1997 .

[10]  Philippe R. Spalart,et al.  Detached-eddy simulation of an airfoil at high angle of attack , 1999 .

[11]  Danna Zhou,et al.  d. , 1840, Microbial pathogenesis.

[12]  Manuel Kessler,et al.  Aerodynamic and acoustic analysis of an extruded airfoil with a trailing edge device using Detached Eddy Simulation with a Discontinuous Galerkin method , 2013 .

[13]  P. Spalart,et al.  A New Version of Detached-eddy Simulation, Resistant to Ambiguous Grid Densities , 2006 .

[14]  P. Moin,et al.  Log-layer mismatch and modeling of the fluctuating wall stress in wall-modeled large-eddy simulations. , 2017, Physical review fluids.

[15]  P. Spalart,et al.  A hybrid RANS-LES approach with delayed-DES and wall-modelled LES capabilities , 2008 .

[16]  Wolfgang A. Wall,et al.  Wall modeling via function enrichment within a high‐order DG method for RANS simulations of incompressible flow , 2016, 1610.08205.

[17]  R. Moser,et al.  Direct numerical simulation of turbulent channel flow up to $\mathit{Re}_{{\it\tau}}\approx 5200$ , 2014, Journal of Fluid Mechanics.

[18]  Scott M. Murman,et al.  Assessment of Wall-modeled LES Strategies Within a Discontinuous-Galerkin Spectral-element Framework , 2017 .

[19]  Johan Larsson,et al.  Large eddy simulation with modeled wall-stress: recent progress and future directions , 2016 .

[20]  John Kim,et al.  DIRECT NUMERICAL SIMULATION OF TURBULENT CHANNEL FLOWS UP TO RE=590 , 1999 .

[21]  J. Fröhlich,et al.  Hybrid LES/RANS methods for the simulation of turbulent flows , 2008 .

[22]  Thomas Blacha,et al.  Application of the Adjoint Method for Vehicle Aerodynamic Optimization , 2016 .

[23]  S. Orszag,et al.  High-order splitting methods for the incompressible Navier-Stokes equations , 1991 .

[24]  Spencer J. Sherwin,et al.  On the eddy-resolving capability of high-order discontinuous Galerkin approaches to implicit LES / under-resolved DNS of Euler turbulence , 2017, J. Comput. Phys..

[25]  Javier Jiménez,et al.  Scaling of the velocity fluctuations in turbulent channels up to Reτ=2003 , 2006 .

[26]  D. Spalding A Single Formula for the “Law of the Wall” , 1961 .

[27]  Martin Kronbichler,et al.  A multiscale approach to hybrid RANS/LES wall modeling within a high‐order discontinuous Galerkin scheme using function enrichment , 2017, International Journal for Numerical Methods in Fluids.

[28]  Martin Kronbichler,et al.  A high-order semi-explicit discontinuous Galerkin solver for 3D incompressible flow with application to DNS and LES of turbulent channel flow , 2016, J. Comput. Phys..

[29]  Dieter Schwamborn,et al.  ATAAC – An EU-Project Dedicated to Hybrid RANS/LES Methods , 2012 .

[30]  Javier Jiménez,et al.  Spectra of the very large anisotropic scales in turbulent channels , 2003 .