S. Stanley et S. Sarkar, SIMULATIONS OF SPATIALLY DEVELOPING 2-DIMENSIONAL SHEAR LAYERS AND JETS, Theoretical and computational fluid dynamics, 9(2), 1997, pp. 121-147
A computational study of spatially evolving two-dimensional free shear
flows has been performed using direct numerical simulation of the Nav
ier-Stokes equations in order to investigate the ability of these two-
dimensional simulations to predict the overall Bow-field quantities of
the corresponding three-dimensional ''real'' turbulent flows. The eff
ects of inflow forcing on these two-dimensional Bows has also been stu
died. Simulations were performed of shear layers, as well as weak (lar
ge co-flow and relatively weak shear) and strong (small co-flow and re
latively strong shear) jets. Several combinations of discrete forcing
with and without a broadband background spectrum were used. Although s
patially evolving direct simulations of shear layers have been perform
ed in the past, no such simulations of the plane jet have been perform
ed to the best of our knowledge. It was found that. in the two-dimensi
onal shear layers, external forcing led to a strong increase in the in
itial growth of the shear-layer thickness, followed by a region of dec
reased growth as in physical experiments. The final downstream growth
rate was essentially unaffected by forcing. The mean velocity profile
and the naturally evolving growth Fate of the shear layer in the case
of broadband forcing compare well with experimental data. However, the
total and transverse fluctuation intensities are larger in the two-di
mensional simulations with respect to experimental data. In the weak-j
et simulations it was found that symmetric forcing completely overwhel
ms the natural tendency to transition to the asymmetric jet column mod
e downstream. It was observed that two-dimensional simulations of ''st
rong'' jets with a low speed co-flow led to a fundamentally different
flow with large differences even in mean velocity profiles with respec
t to experimental data for planar jets. This was a result of the domin
ance of the two-dimensional mechanism of vertex dipole ejection in the
flow due to the lack of spanwise instabilities. Experimental studies
of planar jets do not show vortex dipole formation and ejection. A thr
ee-dimensional ''strong''-jet simulation showed the rapid evolution of
three-dimensionality effectively preventing this two-dimensional mech
anism, as expected from experimental results.