Abstract

The effect of shear history on the evolution of the polystyrene—alum floc size, density, and structure is investigated by small-angle light scattering during cycled-shear and tapered-shear flocculation in a stirred tank using a Rushton impeller. First, various sampling schemes are experimentally evaluated. The floc structure is characterized by the mass fractal dimension, D f , and the relative floc density. During turbulent shear flocculation, small floc structures are shown to be more open ( D f = 2.1) than larger floc structures ( D f = 2.5) as a result of shear-induced restructuring during steady state attainment. Flocs produced by cycled-shear flocculation are grown at shear rate G-50 s −1 for 30 min, are fragmented at G b = 100, 300, or 500 s −1 for one minute, and then are regrown at G = 50 s −1. This shear schedule decreases the floc size but compacts the floc structure. When flocs are produced by gradual reduction of the shear rate from G-300 to 50 s −1 (tapered-shear flocculation), smaller though equally dense flocs are produced compared with cycled-shear flocculation. The cycled-shear flocculation method produces the largest flocs with the highest potential for sedimentation when the fragmentation shear rate is G b = 300 s −1.

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