Direct numerical simulation is utilized to generate statistics in particle-
laden homogeneous plane strain turbulent flows. Assuming that the two-phase
flow is dilute (one-way coupling), a variety of cases are considered to in
vestigate the effects of the particle time constant. The carrier phase is i
ncompressible and is treated in the Eulerian frame whereas the particles ar
e tracked individually in a Lagrangian frame. For small particle Reynolds n
umbers, an analytical expression for the particle mean velocity is found, w
hich is different from the fluid one, and the dispersed phase is shown to b
e homogeneous. This is not the case for particles with large Reynolds numbe
rs and no statistics involving particle fluctuating velocity is presented f
or large particles. The results show that the root mean square (r.m.s.) of
the particle velocity in the squeezed direction exceeds that of the fluid i
n the same direction and increases with the particle time constant. The mea
n velocity gradient component in the elongated direction has the opposite e
ffect, that is the r.m.s. of the particle velocity is decreased below that
of the fluid in this direction. Further, the dispersed phase exhibits a lar
ger anisotropy than the fluid phase, and its anisotropy increases with the
particle inertia. Dispersion is shown to depend strongly on the injection l
ocation and quantified dispersion results show that increasing the injectio
n location coordinates in the strained directions increases the dispersion.
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