AGGREGATION AND DISPERSION OF SPHERES FALLING IN VISCOELASTIC LIQUIDS

This paper focuses on the settling on one sphere near another or near a wall. We find maximum differences between Newtonian and viscoelastic liquids, with repulsion between nearby bodies in the Newtonian case a nd attraction in the viscoelastic case. Side-by-side arrangements of s edimenting spheres are unstable in exactly the same way that broadside -on settling of long bodies is unstable at subcritical speeds in a vis coelastic fluid. The line of centers between the spheres rotates from across to along the stream as the spheres are sucked together. The res ulting chain of two spheres is a long body which is stable when the li ne between centers is parallel to the fall, but this configuration bre aks up at subcritical speeds where inertia again dominates. To explain the orientation of particles in the supercritical case, we correlate the aggregative power of a viscoelastic fluid with a zero shear value of the coefficient of ratio of the first normal stress difference to t he shear stress and for exceptional cases we introduce the idea of the memory of shear-thinning leading to corridors of reduced viscosity.