PARTIALLY AVERAGED NAVIER-STOKES METHOD FOR TURBULENCE CLOSURES: CHARACTERIZATION OF FLUCTUATIONS AND EXTENSION TO WALL BOUNDED FLOWS

Partially Averaged Navier-Stokes Method for Turbulence Closures: Characterization of Fluctuations and Extension to Wall Bounded Flows. (May 2009) Sunil Lakshmipathy, B.E., Bangalore University; M.S., Texas A&M University Chair of Advisory Committee: Dr. Sharath S. Girimaji The work presented in this dissertation concerns continued development, validation and verification of the partially averaged Navier-Stokes (PANS) method – a variable resolution closure model for turbulence. Linear eddy viscosity models (LEVM), which are popular because of their simplicity and affordability in terms of computational cost have fundamental deficiencies and cannot be trusted to accurately represent turbulence in realistic complex flows. The more high fidelity approaches such as large eddy simulations (LES) and direct numerical simulations (DNS) are out of realm of engineering applicability because of their high requirements in computing power. PANS, a variable resolution approach considered in this study, lies between LEVM and LES in terms of computational cost and is designed to prudently utilize the available computing power to improve accuracy. This dissertation presents the various studies performed to characterize the PANS fluctuations and extend the model for use in various wall bounded flows. The road map towards our goal includes: (i) Comparing a-priori and a-posteriori eddy viscosity values to establish whether PANS is capable of producing the pre-specified level of reduction. (ii) Investigating the scaling of PANS fluctuations for different levels of prescribed resolution and establishing if the fluctuations abide by known turbulence scaling laws. (iii) Extending PANS to k-ω formulation which is better suited for wall-bounded shear

[1]  Mehdi R. Khorrami,et al.  Time-Accurate Simulations and Acoustic Analysis of Slat Free Shear Layer , 2002 .

[2]  D. Wilcox Reassessment of the scale-determining equation for advanced turbulence models , 1988 .

[3]  Pierre Sagaut,et al.  Multiscale And Multiresolution Approaches In Turbulence , 2006 .

[4]  H. L. Seegmiller,et al.  Time-dependent behavior of a reattaching shear layer , 1987 .

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

[6]  P. Durbin On the k-3 stagnation point anomaly , 1996 .

[7]  S. Ghosal Mathematical and Physical Constraints on Large-Eddy Simulation of Turbulence , 1999 .

[8]  A. Elmiligui,et al.  Numerical Study of Flow Past a Circular Cylinder Using RANS, Hybrid RANS/LES and PANS Formulations , 2004 .

[9]  Awatef Hamed,et al.  DES, Hybrid RANS/LES and PANS Models for Unsteady Separated Turbulent Flow Simulations , 2005 .

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

[11]  B. Launder,et al.  Development and application of a cubic eddy-viscosity model of turbulence , 1996 .

[12]  Sanjay Mittal,et al.  Energy Spectra of Flow Past a Circular Cylinder , 2004 .

[13]  H. L. Seegmiller,et al.  Features of a reattaching turbulent shear layer in divergent channel flow , 1985 .

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

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

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

[17]  B. Cantwell,et al.  An experimental study of entrainment and transport in the turbulent near wake of a circular cylinder , 1983, Journal of Fluid Mechanics.

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

[19]  Bart A. Singer,et al.  Evaluation of a Second-Order Accurate Navier-Stokes Code for Detached Eddy Simulation Past a Circular Cylinder , 2003 .

[20]  Sunil Lakshmipathy,et al.  Partially-averaged Navier-Stokes method for turbulent flows: k-w model implementation , 2006 .

[21]  S. Lakshmipathy PANS method of turbulence: simulation of high and low Reynolds number flows past a circular cylinder , 2006 .

[22]  S. Girimaji Fully explicit and self-consistent algebraic Reynolds stress model , 1995 .

[23]  P. Sagaut BOOK REVIEW: Large Eddy Simulation for Incompressible Flows. An Introduction , 2001 .

[24]  Eunhwan Jeong,et al.  Partially averaged navier-stokes method for turbulence : Fixed point analysis and comparison with unsteady partially averaged navier-stokes , 2006 .

[25]  Aditya Murthi,et al.  Effect of turbulent transport models and grid spacing on pans calculations of a lid-driven cavity , 2005 .

[26]  Jochen Fröhlich,et al.  Lessons from LESFOIL Project on Large-Eddy Simulation of Flow Around an Airfoil , 2003 .

[27]  P. Moin,et al.  Cross correlation and length scales in turbulent flows near surfaces , 1989 .

[28]  Sunil Lakshmipathy,et al.  Extension of Boussinesq turbulence constitutive relation for bridging methods , 2007 .

[29]  Sharath S. Girimaji,et al.  Flow Past a Backward-Facing Step: Comparison of PANS, DES and URANS Results with Experiments , 2006 .

[30]  S. Girimaji,et al.  Partially-averaged Navier Stokes Model for Turbulence: Implementation and Validation , 2005 .

[31]  Charles G. Speziale Computing non-equilibrium turbulent flows with time-dependent rans and vles , 1997 .

[32]  Strategies for turbulence modelling and simulations , 2000 .

[33]  Andreas Muschinski,et al.  A similarity theory of locally homogeneous and isotropic turbulence generated by a Smagorinsky-type LES , 1996, Journal of Fluid Mechanics.

[34]  Tucker Alan Lavin Reynolds and Favre-averaged rapid distortion theory for compressible, ideal-gas turbulence , 2007 .

[35]  F. R. Menter,et al.  Influence of freestream values on k-omega turbulence model predictions , 1992 .

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

[37]  Philippe R. Spalart,et al.  Detached-Eddy Simulations Past a Circular Cylinder , 2000 .

[38]  Richard D. Sandberg,et al.  A Methodology for Simulating Compressible Turbulent Flows , 2003 .

[39]  M. Breuer A CHALLENGING TEST CASE FOR LARGE EDDY SIMULATION: HIGH REYNOLDS NUMBER CIRCULAR CYLINDER FLOW , 2000, Proceeding of First Symposium on Turbulence and Shear Flow Phenomena.

[40]  S. Girimaji,et al.  Lattice Boltzmann DNS of decaying compressible isotropic turbulence with temperature fluctuations , 2006 .

[41]  Kemal Hanjalic Will RANS Survive LES? A View of Perspectives , 2004 .

[42]  M. Germano,et al.  From RANS to DNS: Towards a Bridging Model , 1999 .

[43]  A. N. Kolmogorov Equations of turbulent motion in an incompressible fluid , 1941 .

[44]  D. Wilcox Turbulence modeling for CFD , 1993 .