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}

We present fully resolved computations of flow over periodic hills at the hill-Reynolds numbers ReH=5,600$\text {Re}_{H}= 5{,}600$ and ReH=10,595$\text {Re}_{H}= 10{,}595$ with the highest fidelity to date. The calculations are performed using spectral incompressible discontinuous Galerkin schemes of 8th$8^{\text {th}}$ and 7th$7^{\text {th}}$ order spatial accuracy, 3rd$3^{\text {rd}}$ order temporal accuracy, as well as 34 and 180 million grid points, respectively. We show that the remaining discretization error is small by comparing the results to h- and p-coarsened simulations. We quantify the statistical averaging error of the reattachment length, as this quantity is widely used as an ‘error norm’ in comparing numerical schemes. The results exhibit good agreement with the experimental and numerical reference data, but the reattachment length at ReH=10,595$\text {Re}_{H}= 10{,}595$ is predicted slightly shorter than in the most widely used LES references. In the second part of this paper, we show the broad range of capabilities of the numerical method by assessing the scheme for underresolved simulations (implicit large-eddy simulation) of the higher Reynolds number in a detailed h/p convergence study.

[1]  J. Fröhlich,et al.  Investigation of wall-function approximations and subgrid-scale models in large eddy simulation of separated flow in a channel with streamwise periodic constrictions , 2003 .

[2]  S. Pope Turbulent Flows: FUNDAMENTALS , 2000 .

[3]  Claus-Dieter Munz,et al.  Simulation of underresolved turbulent flows by adaptive filtering using the high order discontinuous Galerkin spectral element method , 2016, J. Comput. Phys..

[4]  Koen Hillewaert,et al.  Assessment of a discontinuous Galerkin method for the simulation of vortical flows at high Reynolds number , 2014 .

[5]  Gregor Gassner,et al.  On the use of kinetic energy preserving DG-schemes for large eddy simulation , 2017, J. Comput. Phys..

[6]  Claus-Dieter Munz,et al.  High-Order Discontinuous Galerkin Schemes for Large-Eddy Simulations of Moderate Reynolds Number Flows , 2015 .

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

[8]  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..

[9]  Gregor Gassner,et al.  A Comparison of the Dispersion and Dissipation Errors of Gauss and Gauss-Lobatto Discontinuous Galerkin Spectral Element Methods , 2011, SIAM J. Sci. Comput..

[10]  Laslo T. Diosady,et al.  DNS of Flows over Periodic Hills using a Discontinuous-Galerkin Spectral-Element Method , 2014 .

[11]  M. de la Llave Plata,et al.  Development of a multiscale LES model in the context of a modal discontinuous Galerkin method , 2016 .

[12]  Claus-Dieter Munz,et al.  Explicit Discontinuous Galerkin methods for unsteady problems , 2012 .

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

[14]  Sven Scharnowski,et al.  Highly resolved experimental results of the separated flow in a channel with streamwise periodic constrictions , 2016, Journal of Fluid Mechanics.

[15]  Wolfgang A. Wall,et al.  Wall modeling via function enrichment: Extension to detached-eddy simulation , 2017, Computers & Fluids.

[16]  Christoph Rapp,et al.  Experimentelle Studie der turbulenten Strömung über periodische Hügel , 2009 .

[17]  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..

[18]  Jochen Fröhlich,et al.  Highly resolved large-eddy simulation of separated flow in a channel with streamwise periodic constrictions , 2005, Journal of Fluid Mechanics.

[19]  P. Moin,et al.  DIRECT NUMERICAL SIMULATION: A Tool in Turbulence Research , 1998 .

[20]  Spencer J. Sherwin,et al.  Linear dispersion-diffusion analysis and its application to under-resolved turbulence simulations using discontinuous Galerkin spectral/hp methods , 2015, J. Comput. Phys..

[21]  Martin Kronbichler,et al.  On the stability of projection methods for the incompressible Navier-Stokes equations based on high-order discontinuous Galerkin discretizations , 2017, J. Comput. Phys..

[22]  Alessandro Colombo,et al.  On the development of an implicit high-order Discontinuous Galerkin method for DNS and implicit LES of turbulent flows , 2016 .

[23]  Martin Kronbichler,et al.  Efficiency of high‐performance discontinuous Galerkin spectral element methods for under‐resolved turbulent incompressible flows , 2018, 1802.01439.

[24]  Vincent Couaillier,et al.  On the use of a high-order discontinuous Galerkin method for DNS and LES of wall-bounded turbulence , 2017, Computers & Fluids.

[25]  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.

[26]  D. Arnold An Interior Penalty Finite Element Method with Discontinuous Elements , 1982 .

[27]  Martin Kronbichler,et al.  A Performance Comparison of Continuous and Discontinuous Galerkin Methods with Fast Multigrid Solvers , 2016, SIAM J. Sci. Comput..

[28]  Claus-Dieter Munz,et al.  Discontinuous Galerkin for High Performance Computational Fluid Dynamics (hpcdg) , 2011, High Performance Computing in Science and Engineering.

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

[30]  Alfredo Pinelli,et al.  The role of the forcing term in the large eddy simulation of equilibrium channel flow , 1990 .

[31]  Martin Kronbichler,et al.  Robust and efficient discontinuous Galerkin methods for under-resolved turbulent incompressible flows , 2018, J. Comput. Phys..

[32]  Katharina Kormann,et al.  Fast Matrix-Free Evaluation of Discontinuous Galerkin Finite Element Operators , 2017, ACM Trans. Math. Softw..

[33]  Claus-Dieter Munz,et al.  Discontinuous Galerkin for High Performance Computational Fluid Dynamics , 2013, High Performance Computing in Science and Engineering.

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

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

[36]  A. Beck,et al.  On the accuracy of high-order discretizations for underresolved turbulence simulations , 2013 .

[37]  Wolfgang A. Wall,et al.  A New High-Order Discontinuous Galerkin Solver for DNS and LES of Turbulent Incompressible Flow , 2018 .

[38]  Michael Manhart,et al.  Flow over periodic hills – Numerical and experimental study in a wide range of Reynolds numbers , 2009 .

[39]  G. Kreiss,et al.  Analysis of stretched grids as buffer zones in simulations of wave propagation , 2016 .

[40]  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.

[41]  Koen Hillewaert,et al.  Application of wall-models to discontinuous Galerkin LES , 2017 .

[42]  George Em Karniadakis,et al.  De-aliasing on non-uniform grids: algorithms and applications , 2003 .