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Figure 4.28 shows a complete view of the computational domain defined for the BE12500. The computational domain is made of 308464 finite volumes.
Figures 4.29 and 4.30 show the computational grid adopted.
A regular meshing is used for the discretization of the cylindrical body
of the tank. Distortion of the grid is locally produced to
simulate accurately the shape of the baffles, as shown in Figure 4.30,
A distorted grid is used also for the round bottom of the vessel (red part in
Figure 4.29)
to reproduce the curvature and to model the shape of the impeller.
A very fine grid is used in the bottom region
for the detailed modeling of the turbofoil turbine.
Figure 4.31 shows
the grid accurately shaped to reproduce the variable curvature of the
blades. Constant thickness (equal to )
is assumed for the blades. Impeller rotation is counter-clockwise.
Simulations made on this model are aimed at evaluating the different performances of the turbofoil turbine with respect to the retreated curved blade impeller. Performances of the two agitators are evaluated with respect to power consumption and pumping capability. For this reason, a number of simulations is required to characterize the behavior of BE12500 in the same operative conditions for which characterization of the CE12500 is available. Simulations made are gathered in Table 4.10.
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For BE12500, simulations at different Reynolds number are made
changing the fluid viscosity only.
Density and angular velocity are set to
and
and are kept constant for all the simulations.
Reynolds numbers in the range
have been explored.
Simulation S1 is made with a very viscous fluid
(
) to evaluate the effects of high viscosity
on the flow field distribution. Simulation S4 is made with water.
Conditions selected for simulation S3 and S4 are used
to verify independency of power
consumption from fluid viscosity in the fully turbulent range
(
).
Numerical simulations are made with the full transient approach
(see Appendix A
for details) starting from fluid at rest in the tank.
The sliding mesh approach is used
to account for the relative motion of impeller and vessel.
The portion of the domain containing
the turbofoil in which conservation equations are solved in a rotating
frame of reference is shown in red in Figure 4.29.
The sliding boundary (in red in Figure 4.33) is shown together
with the other
boundary conditions used for the simulation in
Figure 4.33.
No slip condition is used for the wall of the vessel
(
)
and for the surface of the turbofoil turbine (
).
Free shear condition is used at the top of the vessel to simulate a
flat free surface.