TY - JOUR
T1 - Axial segregation in spherical and cylindrical rotating tumblers
AU - D'Ortona, Umberto
AU - Thomas, Nathalie
AU - Lueptow, Richard M.
N1 - Publisher Copyright:
© The Authors, published by EDP Sciences, 2017.
PY - 2017/6/30
Y1 - 2017/6/30
N2 - Monodisperse and bidisperse granular flows are studied in rotating tumblers using DEM. In spherical tumblers, flowing particles' trajectories do not follow straight lines but are curved. At the same time particles near the surface drift toward the pole, inducing two global recirculation cells. Combined with radial segregation, drift and curvature compete to impose the axial segregation pattern: Small-Large-Small (SLS) or Large-Small-Large (LSL). Fill level, rotation speed and wall roughness influence drift and curvature, and modify the resulting segregation pattern. In cylindrical tumblers, equivalent recirculation cells occur next to the end walls. A second pair of recirculation cells with a weak drift in the opposite direction appears at the center for long enough tumblers. Unlike the sphere case, curvature and drift in the primary cells combine to push large particles toward the end walls, explaining why large particle bands appear at the end walls for axial segregation in cylinder.
AB - Monodisperse and bidisperse granular flows are studied in rotating tumblers using DEM. In spherical tumblers, flowing particles' trajectories do not follow straight lines but are curved. At the same time particles near the surface drift toward the pole, inducing two global recirculation cells. Combined with radial segregation, drift and curvature compete to impose the axial segregation pattern: Small-Large-Small (SLS) or Large-Small-Large (LSL). Fill level, rotation speed and wall roughness influence drift and curvature, and modify the resulting segregation pattern. In cylindrical tumblers, equivalent recirculation cells occur next to the end walls. A second pair of recirculation cells with a weak drift in the opposite direction appears at the center for long enough tumblers. Unlike the sphere case, curvature and drift in the primary cells combine to push large particles toward the end walls, explaining why large particle bands appear at the end walls for axial segregation in cylinder.
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U2 - 10.1051/epjconf/201714003011
DO - 10.1051/epjconf/201714003011
M3 - Conference article
AN - SCOPUS:85024113143
SN - 2101-6275
VL - 140
JO - EPJ Web of Conferences
JF - EPJ Web of Conferences
M1 - 03011
T2 - 8th International Conference on Micromechanics on Granular Media, Powders and Grains 2017
Y2 - 3 July 2017 through 7 July 2017
ER -