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Dynamics of single, non-spherical ellipsoidal particles in a turbulent channel flow

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Figure

FIG. 1. Relationship between the inertial]Nplanex[x,y,z, the particlex[x,y,z]and the co-movingx[x,y,z]co-ordinate systems and definition of the Euler angles(,,).[xy,]plane[x,y],  is the angle between the z -axis and z ,  is the angle between thex -axis and N, and  is the angle between the x -axis and N.
FIG. 2. (a, b) Illustration of torque due to resistance on a rotating particle and the location of the centres
FIG. 3. Schematic of the computational domain of the channel flow.
FIG. 4. Instantaneous sub-grid scale turbulence kinetic energy (ksgs / m2 s-2) in the spanwise directionalong a plane at z = 2h.
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