Page 267 - Biomass Gasification, Pyrolysis And Torrefaction Practical Design and Theory
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Chapter | 7  Gasification Theory                             243


             entire zone. Therefore, each zone shows a homogeneous char concentration
             in the bed material and a uniform temperature. Additional input parameters
             to the model are geometric data, particle properties, and flow-rates.

             7.6.2.1 Hydrodynamic Submodel (Bubbling Bed)
             The dense zone (assumed to be the bubbling bed) is modeled according to
             the modified two-phase theory. Bubble size is calculated as a function of bed
             height (Darton and LaNauze, 1977), and it is assumed that all bubbles at any
             cross-section are of uniform size:
                                                      ffiffiffiffiffiffiffi  0:8
                                             0:4     r
                                     ðU2U mf Þ         A
                             d b 5 0:54          z14                   (7.81)
                                        g 0:2         N or
             where (N or /A) is the number of orifices per unit of cross-section area of the
             bed.
                The interphase mass transfer between bubbles and emulsion, essential for
             the gas solid reactions, is modeled semiempirically using the specific bubble
             surface as the exchange area, the concentration gradient, and the mass-transfer
             coefficient. The mass-transfer coefficient, K BE , based on the bubble emulsion
             surface area (Sit and Grace, 1978), is:
                                             r ffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffiffi
                                       U mf    4ε mf D r U B
                                  K BE 5   1                           (7.82)
                                        4         πd B
             where U mf and ε mf are, respectively, minimum fluidization velocity and voi-
             dage at a minimum fluidizing condition, D r is the bed diameter, and U B is
             the rise velocity of a bubble of size d B .
                The axial mean voidage in the freeboard is calculated using an exponen-
             tial decay function.


             7.6.2.2 Reaction Submodel
             Gasification reactions proceed at a finite speed; this process is divided into
             three steps: drying, devolatilization, and gasification. The time taken for dry-
             ing and devolatilization of the fuel is much shorter than the time taken for
             gasification of the remaining char. Some models assume instantaneous dry-
             ing and devolatilization because the rate of reaction of the char, which is the
             slowest, largely governs the overall process.
                The products of devolatilization are CO 2 , CO, H 2 O, H 2 , and CH 4 .The
             gases released during drying and devolatilization are not added instantaneously
             to the upflowing gas stream, but are added along the height of the gasifier in a
             predefined pattern. The total mass devolatilized, m volatile , is therefore the sum
             of the carbon, hydrogen, and oxygen volatilized from the solid biomass.

                                                                       (7.83)
                              m volatile 5 m char 1 m hydrogen 1 m oxygen
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