Effect of wall boundary condition on scalar transfer in a fully developed turbulent flume

We performed direct numerical simulation of fully developed turbulent velocity and temperature fields in a flume, for Reynolds number, based on the wall shear velocity and the height of the flume, Re=171 and Prandtl numbers Pr=1.0 and Pr=5.4. To elucidate exactly the role of the wall boundary condition for passive scalar, the system considered was the flow at constant properties of the fluid. Two types of thermal wall boundary conditions (BCs) for the dimensionless temperature equation were studied: isothermal wall boundary condition—H1, and isoflux wall boundary condition—H2. The profile of the mean temperature was not affected by the type of BC. However, the type of BC has a profound effect on the statistics of the temperature fluctuations in the near-wall region y+<10. Comparison of near-wall statistics of temperature fluctuations shows that at Pr=1 the buffer part of the turbulent boundary layer significantly influences the scalar transfer in the conductive sublayer, whereas at Pr=5.4 the near-wall te...

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

[2]  F. Anselmet,et al.  Statistics of temperature increments in fully developed turbulence, part II: experiments , 1995 .

[3]  Parviz Moin,et al.  Transport of Passive Scalars in a Turbulent Channel Flow , 1989 .

[4]  S. Corrsin On the Spectrum of Isotropic Temperature Fluctuations in an Isotropic Turbulence , 1951 .

[5]  R. Friedrich,et al.  On Direct and Large Eddy Simulation of Turbulence , 1986 .

[6]  J. L. Zakin,et al.  Low-speed streaks in drag-reduced turbulent flow , 1997 .

[7]  Z. Zarić,et al.  Wall turbulence structure and convection heat transfer , 1975 .

[8]  J. Pinton,et al.  Some new features of the passive scalar mixing in a turbulent flow , 1999 .

[9]  Ron F. Blackwelder,et al.  Large-scale motion in a turbulent boundary layer: a study using temperature contamination , 1978, Journal of Fluid Mechanics.

[10]  T. J. Hanratty,et al.  Turbulent velocity fluctuations that control mass transfer to a solid boundary , 1983 .

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

[12]  John Kim,et al.  A numerical study of local isotropy of turbulence , 1994 .

[13]  E. M. Khabakhpasheva EXPERIMENTAL INVESTIGATION OF TURBULENT MOMENTUM AND HEAT TRANSFER IN THE PROXIMITY OF THE WALL , 1986 .

[14]  Isabelle Calmet,et al.  Large-eddy simulation of high-Schmidt number mass transfer in a turbulent channel flow , 1997 .

[15]  Thomas J. Hanratty,et al.  Limiting behavior of turbulent scalar transport close to a wall , 2000 .

[16]  Fazle Hussain,et al.  Coherent structure dynamics in near-wall turbulence , 2000 .

[17]  R. So,et al.  Heat Transfer Modeling and the Assumption of Zero Wall Temperature Fluctuations , 1994 .

[18]  Stavros Tavoularis,et al.  On the skewness of the temperature derivative in turbulent flows , 1980, Journal of Fluid Mechanics.

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

[20]  Masaru Hirata,et al.  Heat Transfer Mechanism and Associated Turbulence Structure in the Near-Wall Region of a Turbulent Boundary Layer , 1985 .

[21]  P. Moin,et al.  DIRECT NUMERICAL SIMULATION: A Tool in Turbulence Research , 1998 .

[22]  R. A. Antonia,et al.  THE PHENOMENOLOGY OF SMALL-SCALE TURBULENCE , 1997 .

[23]  B. A. Kader Temperature and concentration profiles in fully turbulent boundary layers , 1981 .

[24]  F. Wubs Notes on numerical fluid mechanics , 1985 .

[25]  D. B. Spalding,et al.  Turbulent shear flows , 1980 .

[26]  N. Kasagi,et al.  PROGRESS IN DIRECT NUMERICAL SIMULATION OF TURBULENT HEAT TRANSFER , 1999 .

[27]  Numerical Investigation of Near-Wall Turbulent Heat Transfer Taking Into Account the Unsteady Heat Conduction in the Solid Wall , 1989 .

[28]  R. Antonia,et al.  Temperature-dissipation measurements in a turbulent boundary layer , 1987, Journal of Fluid Mechanics.