Turbulence Models in Pulsating Flows

The performances of four low-Reynolds-number models are compared for the unsteady Reynolds-average d Navier–Stokes equations applied to the ow in a channel driven by a pressure gradient oscillating around a nonzero mean. The models considered are the one-equation Spalart–Allmaras model, the k–" model with the wall functions of Lam and Bremhorst, the k–! 2 model of Saffman and Wilcox, and the k–"–v 2 model of Durbin. The results are compared with experiments, direct simulations, and large-eddy simulations. The models give similar and reasonably accurate results as far as predicting the velocity proŽle in the channel as a func tion of the phase and reproduce the observed behavior during part of the cycle. However, large differences exist between the models themselves, as well as with respect to the large eddy simulations, at the level of the Reynolds shear stress, turbulent kinetic energy, and dissipation rate. The k–"–v2 model is overall superior to the other models considered.

[1]  U. Piomelli High Reynolds number calculations using the dynamic subgrid‐scale stress model , 1993 .

[2]  David C. Wilcox,et al.  Comparison of two-equation turbulence models for boundary layers with pressure gradient , 1993 .

[3]  S. K. Robinson,et al.  The kinematics of turbulent boundary layer structure , 1991 .

[4]  P. Spalart A One-Equation Turbulence Model for Aerodynamic Flows , 1992 .

[5]  Philippe R. Spalart,et al.  Direct simulation of a turbulent oscillating boundary layer , 1989 .

[6]  Reda R. Mankbadi,et al.  Near-wall response in turbulent shear flows subjected to imposed unsteadiness , 1992, Journal of Fluid Mechanics.

[7]  Mehmet Yasar Gundogdu,et al.  Present State of Art on Pulsatile Flow Theory. Part 2. Turbulent Flow Regime. , 1999 .

[8]  B. R. Ramaprian,et al.  Fully developed periodic turbulent pipe flow. Part 1. Main experimental results and comparison with predictions , 1983, Journal of Fluid Mechanics.

[9]  Ugo Piomelli,et al.  Numerical simulation of pulsating turbulent channel flow , 2000 .

[10]  LES AND RANS STUDIES OF OSCILLATING FLOWS OVER FLAT PLATE , 2000 .

[11]  M. Gundogdu,et al.  Present State of Art on Pulsatile Flow Theory : Part 1:Laminar and Transitional Flow Regimes , 1999 .

[12]  C. Ahrens,et al.  Wall shear stress caused by small amplitude perturbations of turbulent boundary-layer flow: an experimental investigation , 1977, Journal of Fluid Mechanics.

[13]  O. Madsen,et al.  The continental-shelf bottom boundary layer , 1986 .

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

[15]  B. R. Ramaprian,et al.  Fully developed periodic turbulent pipe flow. Part 2. The detailed structure of the flow , 1983, Journal of Fluid Mechanics.

[16]  D. C. Wilcox,et al.  Turbulence-Model Predictions for Turbulent Boundary Layers , 1974 .

[17]  Yang Moon Koh,et al.  Turbulent Flow near a Wall , 1991 .

[18]  V. C. Patel,et al.  Turbulence models for near-wall and low Reynolds number flows - A review , 1985 .

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

[20]  Thomas J. Hanratty,et al.  Studies of the wall shear stress in a turbulent pulsating pipe flow , 1984, Journal of Fluid Mechanics.

[21]  G. Binder,et al.  Wall shear stress modulation in unsteady turbulent channel flow with high imposed frequencies , 1993 .

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

[23]  P. Moin,et al.  Turbulence statistics in fully developed channel flow at low Reynolds number , 1987, Journal of Fluid Mechanics.

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

[25]  S. Tardu,et al.  Cyclic modulation of Reynolds stresses and length scales in pulsed turbulent channel flow , 1995, Proceedings of the Royal Society of London. Series A: Mathematical and Physical Sciences.

[26]  W. Reynolds,et al.  DYNAMIC RESPONSE OF BOUNDARY-LAYER TURBULENCE TO OSCILLATORY SHEAR , 1991 .

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

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

[29]  P. Saffman,et al.  A model for inhomogeneous turbulent flow , 1970, Proceedings of the Royal Society of London. A. Mathematical and Physical Sciences.

[30]  Sedat F. Tardu,et al.  Turbulent channel flow with large-amplitude velocity oscillations , 1994, Journal of Fluid Mechanics.

[31]  S. Jacobs Mass transport in a turbulent boundary layer under a progressive water wave , 1984, Journal of Fluid Mechanics.

[32]  Klaus Bremhorst,et al.  A Modified Form of the k-ε Model for Predicting Wall Turbulence , 1981 .

[33]  P. Durbin SEPARATED FLOW COMPUTATIONS WITH THE K-E-V2 MODEL , 1995 .

[34]  Remo Guidieri Res , 1995, RES: Anthropology and Aesthetics.

[35]  Qingyan Chen,et al.  Buoyancy-driven single-sided natural ventilation in buildings with large openings , 2003 .

[36]  Thomas J. Hanratty,et al.  Influence of large‐amplitude oscillations on turbulent drag , 1994 .

[37]  Giles Brereton,et al.  Response of a turbulent boundary layer to sinusoidal free-stream unsteadiness , 1990, Journal of Fluid Mechanics.