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280  Dust Explosions in the Process Industries


     the vertical experimental glass duct of 0.2 m x 0.2 m cross section and 2 m height by
     low-velocity elutriation from a fluidized bed of 600 g of starch resting on a porous mem-
     brane at the bottom of the system. The average vertical air velocity was on the order of
     0.1 m/s. A battery of parallel vertical steel plates 0.5 mm thick was inserted across the
     whole cross section of the duct when quenching distances were measured. Average dust
     concentrations were determined from the dust mass lost from the fluidized bed  as a
     function of time and the airflow through the system. A laser tomography system was used
    to control the homogeneity of the dust cloud.
      Laminar burning velocities were determined from the measured flame speeds and
    photographically  estimated flame surface areas, as in the case of  Kaesche-Krischer
     (1959), but the applicability of this method to flame propagation in tubes is not obvious.
     (See specific comment in Section 9.2.4.2 in Chapter 9.) To obtain proper laminar flame
    propagation, it is necessary to avoid the buildup of fundamental-mode standing acoustic
    wave motion in the duct. Such waves are easily generated by the gas expansion follow-
    ing the initial flame and can subsequently interfere with the flame propagation. Proust
     and Veyssiere solved this problem by fitting a special damping diaphragm at the open
    bottom end of the duct (see Guenoche, 1964).
      A series of photographs of the propagating laminar maize starch flame is shown in
    Figure 4.15. Figure 4.16 shows the upwards laminar flame front velocity (duct closed at
     the upper end) as a function of the dust concentration. The velocity was measured by
    means of ionization probes. The maximum value of 0.63 m/s occurred close to the stoi-
    chiometric dust concentration 235 g/m3.  A corresponding laminar burning velocity of 0.27
     m/s was deduced by  assuming that its value normal to the flame surface was uniform
     across the entire flame hemisphere. However, this assumption is not necessarily justified.
































     Figure 4.1 5  Photographic records of an upward propagating laminar flame in a  120 g/m' cloud oi
     maize starch in air  (from Proust and Veyssiere, 1988).
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