LES, Zonal and Seamless Hybrid LES/RANS: Rationale and Application to Free and Wall-Bounded Flows Involving Separation and Swirl

An overview is given of the activities in the framework of the German-French Research Group on ”LES of Complex Flows” (DFG-CNRS FOR 507) with respect to the development of zonal and seamless hybrid LES/RANS computational methods based on a near-wall Eddy-Viscosity Model (EVM) and a near-wall Second-Moment Closure (SMC) respectively. The zonal scheme represents a two layer model with a two-equation EVM-RANS model covering the near-wall layer and the true LES employing the zero-equation subgrid-scale (SGS) model of Smagorinsky resolving the core flow. Due attention was payed to the exchange of the variables between the ensemble-averaged RANS field and the spatially-filtered LES field across the discrete interface separating the two sub-regions. A procedure for controlling the interface position in the flow domain was also in focus of the present investigations. After considering a few introductory test cases (fully-developed channel flow, flows separating from sharp-edged surfaces) the feasibility of the method was validated against the available experiments in a single tubo-annular, swirl combustor configuration (Exp.: Palm et al., [39]) and in the separated flows in a 3-D diffuser (Exp. Cherry et al., [10]) and over a 2-D hump including the case with the separation control by steady suction (Exp.Greenblatt et al., [23]). The seamless LES/RANS method employs the so-called Elliptic-Blending Reynolds-Stress Model (EB-RSM, Manceau, [33]; Manceau and Hanjalic, [34]) being active in the entire flow field. This RANS-based SGS model represents a near-wall Second-Moment Closure model relying on the elliptic relaxation method. The model coefficient multiplying the destruction term in the transport equation for the scale-supplying variable e (dissipation rate of the turbulence kinetic energy) was made filter-width (corresponding to the grid spacing) dependent, i.e. dependent on the location of the spectral cutoff, by applying a multiscale modelling procedure originating from spectral splitting of filtered turbulence in line with the Partially Integrated Transport Model (PITM) proposed by Dejoan and Schiestel, [48] and Chaouat and Schiestel, [8]. Herewith, the dissipation rate level was obtained, which suppresses the turbulence intensity towards the subgrid (i.e. subscale) level in the regions where large coherent structures dominate the flow. The resulting model was validated by computing some free flows (a temporal mixing layer) and wall-bounded flows (a fully-developed channel flow). Finally, the PITM method applied to the high-Reynolds number RSM model due to Speziale et al., [53] was used to compute the flow separated from a 2-D hill (with reference LES by Frohlich et al., [19] and Breuer, [6]). In addition, all relevant cases were computed by the conventional LES method aiming at mutual comparison of the predictive capabilities of the afore-mentioned methods with respect to the quality of results and space-time resolution issues.

[1]  Roland Schiestel,et al.  Towards a new partially integrated transport model for coarse grid and unsteady turbulent flow simulations , 2005 .

[2]  F. R. Menter,et al.  SAS Turbulence Modelling of Technical Flows , 2006 .

[3]  John K. Eaton,et al.  Combined Heat Transfer and Fluid Dynamic Measurements Downstream of a Backward-Facing Step , 1985 .

[4]  S. Ghosal An Analysis of Numerical Errors in Large-Eddy Simulations of Turbulence , 1996 .

[5]  M. P. Escudier,et al.  Recirculation in swirling flow - A manifestation of vortex breakdown , 1985 .

[6]  Anthony E. Washburn,et al.  A Separation Control CFD Validation Test Case. Part 1; Baseline and Steady Suction , 2004 .

[7]  Dominique Laurence,et al.  Modeling the response of turbulence subjected to cyclic irrotational strain , 2001 .

[8]  Jong Keun Shin,et al.  Refinement of a second moment closure by the elliptic blending equation and its application to turbulent rotating channel flows , 2003 .

[9]  Suad Jakirlić,et al.  A new approach to modelling near-wall turbulence energy and stress dissipation , 2002, Journal of Fluid Mechanics.

[10]  Alistair Revell,et al.  A Stress-Strain Lag Eddy Viscosity Model for Unsteady Mean Flow , 2005 .

[11]  Khellil Sefiane,et al.  Experimental investigation of self-induced thermocapillary convection for an evaporating meniscus in capillary tubes using micro-PIV , 2005 .

[12]  Suad Jakirlić,et al.  Computational Study of Mean Flow and Turbulence Structure in Inflow System of a Swirl Combustor , 2007 .

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

[14]  Branislav Basara,et al.  SWIRL INTENSITY INFLUENCE ON INTERACTION BETWEEN NON-SWIRLING AND SWIRLING CO-AXIAL JETS IN A COMBUSTOR CONFIGURATION: LES AND MODELLING STUDY , 2007, Proceeding of Fifth International Symposium on Turbulence and Shear Flow Phenomena.

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

[16]  P. J. Mason,et al.  On the magnitude of the subgrid-scale eddy coefficient in large-eddy simulations of turbulent channel flow , 1986, Journal of Fluid Mechanics.

[17]  M. Hadžiabdić,et al.  A robust near-wall elliptic-relaxation eddy-viscosity turbulence model for CFD , 2004 .

[18]  B. Launder,et al.  Application of the energy-dissipation model of turbulence to the calculation of flow near a spinning disc , 1974 .

[19]  F. Archambeau,et al.  Code Saturne: A Finite Volume Code for the computation of turbulent incompressible flows - Industrial Applications , 2004 .

[20]  K. Chien,et al.  Predictions of Channel and Boundary-Layer Flows with a Low-Reynolds-Number Turbulence Model , 1982 .

[21]  Remi Manceau,et al.  Turbulence modelling of statistically periodic flows: synthetic jet into quiescent air , 2006 .

[22]  Masud Behnia,et al.  Reynolds averaged simulation of unsteady separated flow , 2003 .

[23]  Remi Manceau An improved version of the Elliptic Blending Model. Application to non-rotating and rotating channel flows. , 2005 .

[24]  K. Hanjalic,et al.  Prediction of Cascade Flows With Innovative Second-Moment Closures , 2005 .

[25]  Alistair Revell,et al.  A stress strain lag eddy viscosity model for unsteady mean flow , 2006 .

[26]  Suad Jakirlić,et al.  Experimental characterization and modelling of inflow conditions for a gas turbine swirl combustor , 2006 .

[27]  Robert D. Moser,et al.  Direct Simulation of a Self-Similar Turbulent Mixing Layer , 1994 .

[28]  Christopher J. Elkins,et al.  GEOMETRIC SENSITIVITY OF THREE-DIMENSIONAL SEPARATED FLOWS , 2008, Proceeding of Fifth International Symposium on Turbulence and Shear Flow Phenomena.

[29]  A. Sadiki,et al.  A digital filter based generation of inflow data for spatially developing direct numerical or large eddy simulations , 2003 .

[30]  Remi Manceau,et al.  Predictions of flow and heat transfer in multiple-impinging jets with an elliptic-blending second-moment closure , 2005 .

[31]  T. Gatski,et al.  Modelling the pressure–strain correlation of turbulence: an invariant dynamical systems approach , 1991, Journal of Fluid Mechanics.

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

[33]  Parviz Moin,et al.  Method for Generating Equilibrium Swirling Inflow Conditions , 1998 .

[34]  S. Girimaji Partially-Averaged Navier-Stokes Model for Turbulence: A Reynolds-Averaged Navier-Stokes to Direct Numerical Simulation Bridging Method , 2006 .

[35]  Parviz Moin,et al.  ADVANCES IN LARGE EDDY SIMULATION METHODOLOGY FOR COMPLEX FLOWS , 2002, Proceeding of Second Symposium on Turbulence and Shear Flow Phenomena.

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

[37]  Paul Batten,et al.  LNS - An approach towards embedded LES , 2002 .

[38]  P. Sagaut Large Eddy Simulation for Incompressible Flows , 2001 .

[39]  Peter Bradshaw,et al.  Numerical study of stress-transport turbulence models: Implementation and validation issues , 2007 .

[40]  Yannick Hoarau,et al.  Advances in turbulence modelling for unsteady flows — IMFT , 2006 .

[41]  L. Temmerman,et al.  A hybrid two-layer URANS–LES approach for large eddy simulation at high Reynolds numbers , 2005 .

[42]  P. Durbin A Reynolds stress model for near-wall turbulence , 1993, Journal of Fluid Mechanics.

[43]  Sedat F. Tardu,et al.  Experiments and modeling of an unsteady turbulent channel flow , 2005 .

[44]  Francis H. Harlow,et al.  Transport Equations in Turbulence , 1970 .

[45]  P. Durbin Near-wall turbulence closure modeling without “damping functions” , 1991, Theoretical and Computational Fluid Dynamics.

[46]  Remi Manceau,et al.  Elliptic blending model: A new near-wall Reynolds-stress turbulence closure , 2002 .

[47]  Bruno Chaouat,et al.  A new partially integrated transport model for subgrid-scale stresses and dissipation rate for turbulent developing flows , 2005 .

[48]  Yuichi Matsuo,et al.  Surface heat-flux fluctuations in a turbulent channel flow up to Reτ=1020 with Pr=0.025 and 0.71 , 2004 .

[49]  Akira Yoshizawa,et al.  A Statistically-Derived Subgrid-Scale Kinetic Energy Model for the Large-Eddy Simulation of Turbulent Flows , 1985 .

[50]  M. Germano,et al.  Turbulence: the filtering approach , 1992, Journal of Fluid Mechanics.

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

[52]  Seong-O Kim,et al.  Computation of a turbulent natural convection in a rectangular cavity with the elliptic-blending second-moment closure , 2006 .

[53]  Maurizio Quadrio,et al.  Initial response of a turbulent channel flow to spanwise oscillation of the walls , 2003 .

[54]  C. G. Speziale Turbulence modeling for time-dependent RANS and VLES : a review , 1998 .

[55]  P. Spalart Strategies for turbulence modelling and simulations , 2000 .

[56]  Robert J. Poole,et al.  Influence of outlet geometry on strongly swirling turbulent flow through a circular tube , 2006 .