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Combustion Technology           59




             TABLE 5.2  Fundamental parameters of design.

              Parameter                                            Values
              Bed material size range, μm (U.S. mesh)    1 680–177 (10–80)
              U gas velocity in bed, m/s (ft/sec)        0.75–1 (2.5–3)
                o
              U gas velocity in freeboard, m/s (ft/sec)  0.76–0.64 (2.5–2.1)
                f
              Excess air, over stoichiometry             40%
              Freeboard temperature, °C (°F)             843 (1 550)
              Residence time in freeboard, sec           6.5 minimum
              Combustion air temperature                 Depends on percent total solids



                 There are several fundamental parameters: excess air, size, bed material, bed gas
             spatial velocity, freeboard gas spatial velocity, temperature in freeboard, and gas resi-
             dence time. See Table 5.2.

             4.1.1 Size of Bed Material and Gas Velocities
             In designing the fluid bed system, the selection of bed material is critical. As shown in
             Figure 5.5, solid particle size has a direct effect on the quality of fluidization. For incin-
             eration of WWTP solids, sandlike material with a median size of 550 μm (30 mesh) is
             typically used. At bed operating conditions, using equation 5.1, the minimum fluidiza-
             tion gas velocity U  of the 550 μm (30 mesh) particle equals 0.33 m/s (1 ft/sec).
                             mf
                 Because optimal bed fluidizing gas velocity is in the range of 2.5 to 3 U , U is
                                                                                 mf  o
             equal to 0.75 to 1 m/s (2.5 to 3 ft/sec) for the selected solid. Gas corrected to bed tem-
             perature and pressure should be used in sizing of the bed section.
                 Because entrainment increases with freeboard gas velocity, U is maintained as
                                                                        f
             low as possible. It is typically in the range of 0.76 to 0.64 m/s (2.5 to 2.1 ft/sec).
             4.1.2 Excess Air
             If the ultimate analysis of the feed and feed rates is known, then combustion air can
             be calculated from the oxidation reactions shown in Table 5.1, with an excess of 40%
             greater than stoichiometry. Because the combustion of dewatered wastewater solids
             is a two-phase process (evaporation followed by combustion), almost one-half the
             volume of gas in the reactor is water vapor. Therefore, designing the system based on
             an excess air of less than 40% presents the risk of having incomplete combustion.
             Greater than 40% excess air is not efficient and can generate higher emission of
             nitrogen oxides (Dangtran and Holst, 2001).
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