Abstract
In the present work, a qualitative analysis of the
time-averaged gas–solid drag force in gas–solid fluidized
beds is carried out. The analysis is based on a large
number of transient Eulerian–Eulerian 3D CFD simulations
of small bubbling, turbulent and circulating fluidized
beds. The obtained results significantly differ from
corresponding data previously obtained from 2D
simulations, especially at high solid concentrations.
This confirms that to accurately model the gas–solid drag
force in a steady state 3D simulation, the drag model
should not be based on data from transient 2D
simulations. In the present work, the average drag force
is expressed as the product of the drag force calculated
from time-averaged velocities and volume fractions and a
correction coefficient. The study shows that even when
the third dimension is described in the mesh with only
three nodes, the 3D character of the flow is captured in
the drag correction coefficient. Thus, a large number of
parametric studies could be carried out in a reasonable
time frame. In the paper, the parameters affecting the
time-averaged drag force are identified and the nature of
the effects are analyzed. The analysis shows that solid
volume fraction, particle size, solid density, gas
viscosity, the slip velocity between gas and solids and
the lateral distance to a wall have significant effects
on the drag correction coefficient. At high gas densities
typical e.g. of pressurized fluidization even the gas
density has significant effects. A closure relation for
the time-averaged drag force for a wide range of
fluidization conditions should include these seven
variables as inputs.
Original language | English |
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Pages (from-to) | 227-238 |
Journal | Powder Technology |
Volume | 274 |
DOIs | |
Publication status | Published - 2015 |
MoE publication type | A1 Journal article-refereed |
Keywords
- drag force
- fluidized bed
- time-averaged
- 3D simulation