Observation of Reverse Core-Annulus Behavior in Risers and Its Relation to Stokes Number

Thursday, November 11, 2010: 2:10 PM
251 F Room (Salt Palace Convention Center)
Jia Wei Chew1, Christine M. Hrenya2, Ray A. Cocco3, Roy C. Hays3, John G. Findlay3, S.B. Reddy Karri3 and Ted M. Knowlton3, (1)Chemical and Biological Engineering, University of Colorado at Boulder, Boulder, CO, (2)University of Colorado, Boulder, CO, (3)Particulate Solid Research, Inc., Chicago, IL

         This work is part of a larger collaborative effort to develop first-principles, continuum models for polydisperse, gas-solid risers using a combination of theory, simulations, and experiments. The focus of this portion of the effort is to generate a comprehensive experimental dataset for purposes of model validation. Experiments involving monodisperse Geldart Group B particles have been carried out in the pneumatic conveying regime of a riser with a rounded elbow exit.  Several combinations of superficial gas velocity (Us), solids flux (Gs), average particle diameter (dave), and material density (ρp) were investigated. "Core-annulus" profiles (i.e., a dilute core with a dense annulus) have been widely reported in literature to date, mostly for FCC particles (Geldart Group A). Surprisingly, the experiments performed here reveal the presence of a "reverse" core-annulus profile (i.e., a dense core with a dilute annulus) under some conditions.  Three monodisperse materials were investigated, namely large glass beads (dave = 650 μm, ρp = 2500 kg/m3), large high-density polyethylene, HDPE (dave = 650 μm, ρp = 900 kg/m3), and small glass beads (dave = 170 μm, ρp = 2500 kg/m3). Specifically, for larger glass beads the reverse core-annulus profile was observed near the top of the riser for all Us and Gs combinations examined. For HDPE, reverse core-annulus was observed at the top of the riser only at relatively low Gs (i.e., Gs = 120 kg/m2s). Finally, for the smaller glass beads, the traditional core-annulus profile was not observed under any condition. The unexpected reverse core-annulus profile noted above appears correlated with the Stokes number (St) of the material, i.e., the bigger the St, the greater the likelihood and extent of reverse core-annulus behavior.


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