W. Ling et al., DIRECT NUMERICAL-SIMULATION OF A 3-DIMENSIONAL TEMPORAL MIXING LAYER WITH PARTICLE DISPERSION, Journal of Fluid Mechanics, 358, 1998, pp. 61-85
The three-dimensional mixing layer is characterized by both two-dimens
ional and streamwise large-scale structures. Understanding the effects
of those large-scale structures on the dispersion of particles is ver
y important. Using a pseudospectral method, the large-scale structures
of a three-dimensional temporally developing mixing layer and the ass
ociated dispersion patterns of particles were simulated, The Fourier e
xpansion was used for-spatial derivatives due to the periodic boundary
conditions in the streamwise and the spanwise directions and the free
-slip boundary condition in the transverse direction. A second-order A
dam-Bashforth scheme was used in the time integration. Both a two-dime
nsional perturbation, which was based on the unstable wavenumbers of t
he streamwise direction, and a three-dimensional perturbation, derived
from an isotropic energy spectrum, were imposed initially, Particles
with different Stokes numbers were traced by the Lagrangian approach b
ased on one-way coupling between the continuous and the dispersed phas
es. The time scale and length scale for the pairing were found to be t
wice those for the rollup. The streamwise large-scale structures devel
op from the initial perturbation and the most unstable wavelength in t
he spanwise direction was found to be about two thirds of that in the
streamwise direction. The pairing of the spanwise vortices was also fo
und to have a suppressing effect on the development of the three-dimen
sionality. Particles with Stokes number of the order of unity were fou
nd to have the largest concentration on the circumference of the two-d
imensional large-scale structures, The presence of the streamwise larg
e-scale structures causes the variation of the particle concentrations
along the spanwise and the transverse directions, The extent of varia
tion also increases with the development of the three-dimensionality,
which results in the 'mushroom' shape of the particle distribution.