LES of a turbulent jet impinging on a heated wall using high-order numerical schemes

Abstract Large-eddy simulations (LES) of a turbulent impinging jet flow with a nozzle-to-plate distance of two jet diameters and a Reynolds number of Re = 10 , 000 are presented in comparison with experimental data and results from a Direct Numerical Simulation (DNS). The impingement wall is heated and both dynamical and thermal features of the flow are discussed. It is shown that highly accurate numerical methods can lead to correct predictions of velocity statistics and heat transfer but only if a procedure is used to regularize the large-scale dynamics computed explicitly. A better regularization is obtained using a numerical dissipation that mimics a spectral vanishing viscosity in comparison to conventional subgrid-scale models based on an eddy viscosity assumption, even though the model is adapted to the wall through an explicit correction or using the dynamic procedure. These observations suggest that, in the present context of high-order schemes, a simple high-order artificial dissipation coherent with the numerical methods is more suitable than a physical subgrid-scale model that does not take the numerical errors into account. The radial evolution of the Nusselt number predicted by DNS is non-monotonous but this specific behavior is not captured by LES. Due to the complexity of the turbulent processes associated with the corresponding secondary peak in the Nusselt number distribution, an explicit calculation of all the significant scales seems to be required. This conclusion goes against the use of a coarse LES grid in this region of the flow.

[1]  S. Lele Compact finite difference schemes with spectral-like resolution , 1992 .

[2]  Sylvain Laizet,et al.  Straightforward high-order numerical dissipation via the viscous term for direct and large eddy simulation , 2011, J. Comput. Phys..

[3]  Richard Pasquetti,et al.  Spectral Vanishing Viscosity Method for Large-Eddy Simulation of Turbulent Flows , 2006, J. Sci. Comput..

[4]  Simulations numériques directes d'un jet impactant , 2011 .

[5]  Sylvain Laizet,et al.  High-order compact schemes for incompressible flows: A simple and efficient method with quasi-spectral accuracy , 2009, J. Comput. Phys..

[6]  Jungho Lee,et al.  STAGNATION REGION HEAT TRANSFER OF A TURBULENT AXISYMMETRIC JET IMPINGEMENT , 1999 .

[7]  M. Fénot,et al.  Local heat transfer due to several configurations of circular air jets impinging on a flat plate with and without semi-confinement , 2005 .

[8]  Ning Li,et al.  Incompact3d: A powerful tool to tackle turbulence problems with up to O(105) computational cores , 2011 .

[9]  P. Moin,et al.  Eddies, streams, and convergence zones in turbulent flows , 1988 .

[10]  George Em Karniadakis,et al.  A Spectral Vanishing Viscosity Method for Large-Eddy Simulations , 2000 .

[11]  N. Lior,et al.  Impingement Heat Transfer: Correlations and Numerical Modeling , 2005 .

[12]  Luc Vervisch,et al.  A compressible wall-adapting similarity mixed model for large-eddy simulation of the impinging round jet , 2009 .

[13]  Ugo Piomelli,et al.  Large-eddy simulation of rotating channel flows using a localized dynamic model , 1995 .

[14]  R. Kneer,et al.  Insights into the local heat transfer of a submerged impinging jet: Influence of local flow acceleration and vortex-wall interaction , 2012 .

[15]  P. Moin,et al.  A dynamic subgrid‐scale eddy viscosity model , 1990 .

[16]  B. L. Button,et al.  A review of heat transfer data for single circular jet impingement , 1992 .

[17]  Dan S. Henningson,et al.  The Fringe Region Technique and the Fourier Method Used in the Direct Numerical Simulation of Spatially Evolving Viscous Flows , 1999, SIAM J. Sci. Comput..

[18]  E. Tadmor,et al.  Convergence of spectral methods for nonlinear conservation laws. Final report , 1989 .

[19]  Yongmann M. Chung,et al.  Numerical study of momentum and heat transfer in unsteady impinging jets , 2002 .

[20]  Toshio Kobayashi,et al.  A numerical study on the eddy structures of impinging jets excited at the inlet , 2003 .

[21]  Kemal Hanjalic,et al.  Vortical structures and heat transfer in a round impinging jet , 2008, Journal of Fluid Mechanics.

[22]  Weizhong Dai,et al.  Fourth‐order compact schemes of a heat conduction problem with Neumann boundary conditions , 2007 .

[23]  M. Olshanskii,et al.  On simulation of outflow boundary conditions in finite difference calculations for incompressible fluid , 2000 .

[24]  F. Nicoud,et al.  Subgrid-Scale Stress Modelling Based on the Square of the Velocity Gradient Tensor , 1999 .

[25]  H. Tal-Ezer Spectral methods in time for parabolic problems , 1989 .

[26]  J. Buell,et al.  Inflow/outflow boundary conditions and global dynamics of spatial mixing layers , 1988 .

[27]  P. Moin,et al.  On the Effect of Numerical Errors in Large Eddy Simulations of Turbulent Flows , 1997 .

[28]  B. Weigand,et al.  LES simulations of an impinging jet: On the origin of the second peak in the Nusselt number distribution , 2013 .

[29]  J. Gauntner,et al.  Survey of literature on flow characteristics of a single turbulent jet impinging on a flat plate , 1970 .

[30]  A. Dewan,et al.  Recent Trends in Computation of Turbulent Jet Impingement Heat Transfer , 2012 .

[31]  Y. Dubief,et al.  On coherent-vortex identification in turbulence , 2000 .

[32]  L. Brizzi,et al.  Experimental investigation of the flow and heat transfer of an impinging jet under acoustic excitation , 2011 .

[33]  J. C. Vassilicos,et al.  A numerical strategy to combine high-order schemes, complex geometry and parallel computing for high resolution DNS of fractal generated turbulence , 2010 .

[34]  M. Fénot,et al.  A heat transfer measurement of jet impingement with high injection temperature , 2005 .

[35]  D. Lilly,et al.  A proposed modification of the Germano subgrid‐scale closure method , 1992 .

[36]  P. Comte,et al.  Large-Eddy Simulations of Turbulence: Vortex dynamics , 2005 .

[37]  B. W. Webb,et al.  Single-Phase Liquid Jet Impingement Heat Transfer , 1995 .