Abstract

Modeling of turbulent flow over cylinders at high Reynolds numbers continues to be a challenge despite extensive work available in the literature. Most models suffer from loss of accuracy or require extremely refined grids both of which render their usage very difficult for practical problems. A wall model has been developed for solving supercritical turbulent flows using the Turbulent Boundary Layer Equations (TBLE). A new way to calculate the shear stress using the model has been introduced in this work. The TBLE model requires an input velocity from the off wall Large Eddy Simulation (LES) model. The method to obtain the same has been devised using the Log-Law. Also, the calculation of the turbulent viscosity in the near wall region has been modified by varying the Von Karman coefficient as a function of velocity in the adverse pressure gradient region. The results obtained with this enhanced TBLE model have been compared with other popular turbulence models for a Re of 1.0 × 106. The TBLE model has then been used to solve two more Re of 6.5 × 105 and 2.0 × 106. The performance of the model has been compared with respect to mean drag coefficient, Root Mean Square (RMS) of lift coefficient, Strouhal number, base pressure coefficient, adverse pressure recovery and separation angle as well as the profiles for pressure and shear stress variation over the cylinder. The model is shown to be fairly accurate, robust and computationally efficient on account of its ability to work with relatively coarse grids.

Highlights

  • Flow over bluff bodies is one of the most commonly occurring flows in nature as well as in several industrial applications

  • The Turbulent Boundary Layer Equations (TBLE) models show an increase in the base pressure coefficient while the results show better agreement in the attached flow region

  • The hybrid models show a significant increase in the skin friction coefficient with grid refinement

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Summary

Introduction

Flow over bluff bodies is one of the most commonly occurring flows in nature as well as in several industrial applications. Such flows are encountered in aviation, automobile, refrigeration, power plants and civil engineering. At a certain Re, turbulence sets in within the attached boundary layer leading to delayed separation resulting in a sudden drop in drag coefficient known as the “Drag Crisis”. While there may be slight variations in the flow regime classification and the corresponding transition Re in the literature, it is an accepted point that as the flow physics constantly changes modeling of the flow is quite challenging. A single satisfactory model for all ranges of Re is still elusive despite many decades of research

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