Abstract: The direct numerical simulation (hereafter, DNS) of turbulent heat transfer in a plane Couette flow at Reynolds number equal to 8600 (based on the relative wall speed and the channel width) has been performed with emphasis on a large-scale turbulence structure (LSS). Two kinds of boundary temperature conditions are employed; these are the uniform heat flux heating (UHF) and the constant temperature difference between the both walls (CTD). A series of present DNS has been carried out for several larger computational box-sizes than those of existing DNS to examine their effect upon the LSSs and the statistical quantities such as temperature variance. The differences caused by the box-size and the boundary conditions of temperature f...
© 2014 Dr. Sumon SahaTurbulent heat transfer (THT) for internal geometry (pipe or channel) has a wid...
Abstract submitted to EE250 Direct Numerical Simulations (DNS) of the velocity/temperature fields at...
Large eddy simulations of two basic configurations (decay of isotropic turbulence, and the academic ...
The turbulence structure and passive scalar (heat) transport in plane Couette flow at Reynolds numbe...
[EN] We present a new set of direct numerical simulation data of a passive thermal flow in a turbule...
[EN] We present a new set of direct numerical simulation data of a passive thermal flow in a turbule...
Direct numerical simulation techniques are used to study wall turbulence and turbulent dispersion.Tu...
Nearly all moving objects on Earth pass through fluids and many of them move at high speed. This mak...
A turbulent convective flow of an incompressible fluid inside a staggered ribbed channel with high b...
A turbulent convective flow of an incompressible fluid inside a staggered ribbed channel with high b...
A turbulent convective flow of an incompressible fluid inside a staggered ribbed channel with high b...
A turbulent convective flow of an incompressible fluid inside a staggered ribbed channel with high b...
A direct numerical simulation (DNS) of a wall jet is performed at Re=7500. To the authors’ knowledge...
Abstract — The present paper is concerned with a model satisfying the linearity principle and also t...
A direct numerical simulation (DNS) of a wall jet is performed at Re=7500. To the authors’ knowledge...
© 2014 Dr. Sumon SahaTurbulent heat transfer (THT) for internal geometry (pipe or channel) has a wid...
Abstract submitted to EE250 Direct Numerical Simulations (DNS) of the velocity/temperature fields at...
Large eddy simulations of two basic configurations (decay of isotropic turbulence, and the academic ...
The turbulence structure and passive scalar (heat) transport in plane Couette flow at Reynolds numbe...
[EN] We present a new set of direct numerical simulation data of a passive thermal flow in a turbule...
[EN] We present a new set of direct numerical simulation data of a passive thermal flow in a turbule...
Direct numerical simulation techniques are used to study wall turbulence and turbulent dispersion.Tu...
Nearly all moving objects on Earth pass through fluids and many of them move at high speed. This mak...
A turbulent convective flow of an incompressible fluid inside a staggered ribbed channel with high b...
A turbulent convective flow of an incompressible fluid inside a staggered ribbed channel with high b...
A turbulent convective flow of an incompressible fluid inside a staggered ribbed channel with high b...
A turbulent convective flow of an incompressible fluid inside a staggered ribbed channel with high b...
A direct numerical simulation (DNS) of a wall jet is performed at Re=7500. To the authors’ knowledge...
Abstract — The present paper is concerned with a model satisfying the linearity principle and also t...
A direct numerical simulation (DNS) of a wall jet is performed at Re=7500. To the authors’ knowledge...
© 2014 Dr. Sumon SahaTurbulent heat transfer (THT) for internal geometry (pipe or channel) has a wid...
Abstract submitted to EE250 Direct Numerical Simulations (DNS) of the velocity/temperature fields at...
Large eddy simulations of two basic configurations (decay of isotropic turbulence, and the academic ...