Direct Numerical Simulation of a Fully Developed Turbulent Channel Flow With Respect to the Reynolds Number Dependence

Direct numerical simulation (DNS) of a fully developed turbulent channel flow for various Reynolds numbers has been carried out to investigate the Reynolds number dependence. The Reynolds number is set to be Re τ = 180, 395, and 640, where Re τ is the Reynolds number based on the friction velocity and the channel half width. The computation has been executed with the use of the finite difference method. Various turbulence statistics such as turbulence intensities, vorticity fluctuations, Reynolds stresses, their budget terms, two-point correlation coefficients, and energy spectra are obtained and discussed. The present results are compared with the ones of the DNSs for the turbulent boundary layer and the plane turbulent Poiseuille flow and the experiments for the channel flow. The closure models are also tested using the present results for the dissipation rate of the Reynolds normal stresses. In addition, the instantaneous flow field is visualized in order to examine the Reynolds number dependence for the quasi-coherent structures such as the vortices and streaks

[1]  Takeo Kajishima Conservation Properties of Finite Difference Method for Convection. , 1994 .

[2]  J. Dukowicz,et al.  Approximate factorization as a high order splitting for the implicit incompressible flow equations , 1992 .

[3]  Helmut Eckelmann,et al.  Behavior of the three fluctuating velocity components in the wall region of a turbulent channel flow , 1979 .

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

[5]  S. Gavrilakis,et al.  Numerical simulation of low-Reynolds-number turbulent flow through a straight square duct , 1992, Journal of Fluid Mechanics.

[6]  P. Moin,et al.  Reynolds-stress and dissipation-rate budgets in a turbulent channel flow , 1987, Journal of Fluid Mechanics.

[7]  P. Moin,et al.  Numerical investigation of turbulent channel flow , 1981, Journal of Fluid Mechanics.

[8]  R. A. Antonia,et al.  Low-Reynolds-number effects in a fully developed turbulent channel flow , 1992, Journal of Fluid Mechanics.

[9]  Hiroshi Kawamura,et al.  DNS of turbulent heat transfer in channel flow with low to medium-high Prandtl number fluid , 1998 .

[10]  N. Kasagi,et al.  Direct Numerical Simulation of Passive Scalar Field in a Turbulent Channel Flow , 1992 .

[11]  Seyed G. Saddoughi,et al.  Local isotropy in turbulent boundary layers at high Reynolds number , 1994, Journal of Fluid Mechanics.

[12]  Parviz Moin,et al.  Direct simulations of turbulent flow using finite-difference schemes , 1991 .

[13]  H. Eckelmann,et al.  The fluctuating wall‐shear stress and the velocity field in the viscous sublayer , 1988 .

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

[15]  H. Kawamura,et al.  Consistency of Finite-Difference Scheme in Direct Numerical Simulation of Turbulence. , 1994 .

[16]  P. Spalart,et al.  Anisotropy of the dissipation tensor in a turbulent boundary layer , 1994 .

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

[18]  R. B. Dean Reynolds Number Dependence of Skin Friction and Other Bulk Flow Variables in Two-Dimensional Rectangular Duct Flow , 1978 .

[19]  J. Lumley,et al.  A First Course in Turbulence , 1972 .

[20]  Arne V. Johansson,et al.  On the structure of turbulent channel flow , 1982, Journal of Fluid Mechanics.

[21]  宮内 敏雄,et al.  乱流予混合火炎のDirect Numerical Simulation , 1997 .

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

[23]  P. Moin,et al.  Direct numerical simulation of transition and turbulence in a spatially evolving boundary layer , 1991 .

[24]  Anders Lundbladh,et al.  Very large structures in plane turbulent Couette flow , 1996, Journal of Fluid Mechanics.

[25]  W. Willmarth,et al.  Reynolds-number effects on the structure of a turbulent channel flow , 1989, Journal of Fluid Mechanics.

[26]  U. Schumann Subgrid Scale Model for Finite Difference Simulations of Turbulent Flows in Plane Channels and Annuli , 1975 .

[27]  William C. Reynolds,et al.  Measurements in fully developed turbulent channel flow , 1975 .

[28]  M. S. Chong,et al.  A general classification of three-dimensional flow fields , 1990 .

[29]  Hiroshi Kawamura,et al.  Direct numerical simulation of turbulent channel flow by parallel computation , 1999 .

[30]  G. S. Patterson,et al.  Numerical Simulation of Three-Dimensional Homogeneous Isotropic Turbulence , 1972 .

[31]  Yuichi Matsuo,et al.  DNS of turbulent heat transfer in channel flow with respect to Reynolds and Prandtl number effects , 1999 .

[32]  W. C. Reynolds,et al.  Asymptotic near‐wall stress dissipation rates in a turbulent flow , 1983 .

[33]  R. A. Antonia,et al.  Low-Reynolds-number effects on near-wall turbulence , 1994, Journal of Fluid Mechanics.

[34]  John Kim,et al.  On the structure of pressure fluctuations in simulated turbulent channel flow , 1989, Journal of Fluid Mechanics.

[35]  J. Laufer,et al.  Investigation of turbulent flow in a two-dimensional channel , 1951 .