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Lesson 17. MECHANISMS OF FLUIDIZATION, CHARACTERISTICS OF GAS FLUIDIZATION SYSTEMS, MINIMUM POROSITY, BED WEIGHT, PRESSURE DROP IN FLUIDIZED BED
Module 3. Fluidization
Lesson 17
MECHANISM OF FLUIDIZATION, CHARACTERISTICS OF GAS FLUIDIZATION SYSTEM, MINIMUM POROSITY, BED WEIGHT, PRESSURE DROP IN FLUIDIZED BED
Fig. 17.1 Fluidization regimes
Fluidization of fixed bed takes place in distinct stages of air velocity and trans bed pressure drop. Initially, the air cannot escape the bed, and the bed remains stagnant. As the pressure drop across the bed keeps increasing, the bed slowly expands in its height. After a certain peak, the air finds paths to escape and there is a slight dip in the pressure drop. At this stage we can call it as the beginning of the fludization of the bed, but the flow is smooth and the particles are not showing much movement. On further increase in the velocity and flow rate of air, the bed expands further and the particles are separate from each neighbouring particle and there significant turbulence among the particles and air flow. Any further increase in the air velocity, will make the particles to be carried away by the air and passes into the region of Pneumatic transport.
Mechanism of Fluidization
The powdered products are made to flow through a permeable support on which material rests, when gas is passed. The packing of the bed of material will become less dense. i.e. the bed will start to expand when a certain velocity is reached. At still greater velocities the particles in the bed will begin to be in turbulent motion. All particles of the product are thoroughly mixed in the turbulent layer and they dry therefore at a uniform rate. A further increase in the stream of gas finally leads to a velocity at which the particles float, which occurs when the upward force equals the force of gravity acting on the particles. Beyond this velocity it is impossible to maintain a fluidized bed and the particles are carried away in the gas stream (pneumatic conveying). A fluidized bed therefore maintained at air velocities which lie between those at which the bed starts to expand and those at which the particles float. The velocity at which the bed starts to expand is reached when the pressure drop on passing through the bed equals the force of gravity acting on the whole mass of the bed. shows perforated plate for directional air flow, (Fig. 17.2) shows animation of fluidized bed dryer and (Fig. 17.3) shows animation of vibro fluidized bed dryer.
Force of gravity acting on the bed:
ΔP = H0 . g (ρk - ρA) (1- ψ0)
Where,
H0 = depth of the bed of material at rest
ρk = density of the individual particles
ρA = density of the air
ψ0 = porocity of the bed at rest (usually ψ0 = 0.4)
The pressure drop of the gas on passing through the bed is:
ΔP = 64 (μ1/ ψ2) { (1/Re) + (ξ∞/64)} (H0/d*) (ρA/2) V2
μ1 = factor due to increase in length of the path, μ1= 0.75 for beds
Re = Reynold’s number, composed of d* and Vέ = v/έ0
ξ = resistance coefficient for turbulent flow
V = velocity of gas based on the cross section of empty tower
d* = the hydraulic diameter of the pores
The above equation is valid for laminar, transition and turbulent flow. Conbining the two equations yields the velocity at which the bed starts to expand.
If particles stick together initially, stable fluidized beds can be produced by using mechanical stirrer to break up particle agglomerates. Another possibility of forced mixing, which at the same time, also provides forced transport is the much employed vibration fluidized bed drier. The dryer is based on a vibrating conveyor trough which can be up to 10 m long and up to 1 m wide. Eccentric motors produce the vibration of the drier which may be supported on helical or leaf springs. The direction of the vibration can be changed by rotating the motor and the amplitude by changing its eccentricity.
To ensure a uniform distribution of air over the whole area of the air permeable base plate the resistance offered by the plate to the air flow should be in the range of 1000 to 2000 Pa, depending on the type of product and the depth of the bed. The perforations occupy usually between 1.5 and 5 % of the area of the plate, and the depth of the bed, which can be adjusted by means of an overflow weir, is usually between 50 and 300 mm. The vibration fluidized bed has the advantage of forced conveyance in a given direction, fluidization even at low air velocities and a residence time of the product which can be at least partially controlled.