(633g) Observation of Reverse Core-Annulus Behavior in Risers and Its Relation to Stokes Number | AIChE

(633g) Observation of Reverse Core-Annulus Behavior in Risers and Its Relation to Stokes Number

Authors 

Chew, J. W. - Presenter, University of Colorado at Boulder
Hrenya, C. M. - Presenter, University of Colorado at Boulder
Cocco, R. - Presenter, Particulate Solid Research, Inc. (PSRI)
Hays, R. C. - Presenter, Particulate Solid Research, Inc.
Findlay, J. G. - Presenter, Particulate Solid Research, Inc.
Karri, S. B. R. - Presenter, Particulate Solid Research, Inc.
Knowlton, T. - Presenter, Particulate Solid Research, Inc. (PSRI)


         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.