A robust method for generating inflow conditions for direct simulations of spatially-developing turbulent boundary layers

A method for generating inflow conditions for direct numerical simulations (DNS) of spatially-developing turbulent boundary layers is presented. The method is a modification of that of Lund et al. [J. Comput. Phys. 140 (1998) 233]. The approach of Lund et al. is based on having an auxiliary simulation (Code-A) in a three-dimensional domain similar to that of the main simulation (Code-B). The instantaneous velocity field on a selected plane in Code-A is used as the instantaneous inflow conditions for Code-B. The inflow conditions for Code-A are generated through a sequence of operations in which the velocity field at a downstream station is rescaled and re-introduced at the inlet plane. Our present method modifies the operations in Code-A by introducing a set of additional steps preceding the rescaling process. This set involves imposing at the inlet plane an appropriate spectrum E(k) for the turbulence kinetic energy (TKE) and a condition for insuring that the statistical correlation 〈u' 1 u' 3 〉 between the streamwise and vertical velocity fluctuations retain a non-vanishing magnitude. This modification is essential for sustaining the production rate of TKE near the wall throughout the domain. Our DNS results obtained with the new modification are in excellent agreement with the experimental data of DeGraaff and Eaton [J. Fluid Mech. 422 (2000) 319] for Re 0 = 1430.

[1]  P. Moin,et al.  Direct numerical simulation of turbulent flow over a backward-facing step , 1997, Journal of Fluid Mechanics.

[2]  F. Antonino Reduction of skin-friction in a microbubble-laden spatially developing turbulent boundary layer over a flat plate , 2004 .

[3]  D. Coles The law of the wake in the turbulent boundary layer , 1956, Journal of Fluid Mechanics.

[4]  Robert B. Wilhelmson,et al.  Direct solutions for Poisson's equation in three dimensions , 1977 .

[5]  T. Lund,et al.  Generation of Turbulent Inflow Data for Spatially-Developing Boundary Layer Simulations , 1998 .

[6]  L. Prandtl 7. Bericht über Untersuchungen zur ausgebildeten Turbulenz , 1925 .

[7]  P. Spalart Direct simulation of a turbulent boundary layer up to Rθ = 1410 , 1988, Journal of Fluid Mechanics.

[8]  T. Kármán,et al.  Mechanische Ahnlichkeit und Turbulenz , 1930 .

[9]  J. Eaton,et al.  Reynolds-number scaling of the flat-plate turbulent boundary layer , 2000, Journal of Fluid Mechanics.

[10]  F. Harlow,et al.  Numerical Calculation of Time‐Dependent Viscous Incompressible Flow of Fluid with Free Surface , 1965 .

[11]  A. Leonard,et al.  Direct Numerical Simulation of Equilibrium Turbulent Boundary Layers , 1987 .

[12]  Hartmut Höller,et al.  A Mesoscale Model for the Simulation of Turbulence, Clouds and Flow over Mountains: Formulation and Validation Examples , 1987 .

[13]  T. Gerz,et al.  Direct numerical simulation of stratified homogeneous turbulent shear flows , 1989, Journal of Fluid Mechanics.

[14]  P. Moin,et al.  Simulation of spatially evolving turbulence and the applicability of Taylor's hypothesis in compressible flow , 1992 .