Page 444 - Dust Explosions in the Process Industries
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Ignition of Dust Clouds and Dust Deposits  4 1 1


               velocity of the particles in quiescent air (=2 cds for lycopodium)dominate,and the par-
               ticles above the spark approach the hot gas core.


                  30
               -
                E
                E
               u
               ac          NCE  FROM SPARK  CENTER TO
               w
               b-          CLE  WITH  INITIAL  DISTANCE  20 mm
               z
               w
               u  20
               x
               ac
               2
               in
               E
               0
               ar
               LL
                  10
               z
               s
               c“
               [3
                                                 CONTOURS  OF  HOT
                   0
                    10-2   10-1   100    10’     102    103    104     105    106
                            TIME  AFTER  INITIATION  OF  SPARK  DISCHARGE  Lpsl


               Figure 5.1 6  Summary of theoretical prediction of positions of dust particles and radius of the hot
               gas kernel following a ”short” discharge ofa  1.5J electric spark in a cloud of lycopodium in air (From
               Ensrad,  19811.

                 The 1000 K and 700 K radii of the hot gas sphere as functions of time are also given
               in Figure 5.16. The minimum ignition temperature of  lycopodium clouds in air at
               atmospheric pressure, as determined in the standard Godbert-Greenwald furnace, is
               about 700 K. From Figure 5.16, it therefore follows that a dust-free, cool zone, sepa-
               rating the dust cloud from the incendivepart of the hot gas core, is gradually formed from
               100 ps after the spark discharge and onward, making ignition impossible. Figure 5.16
               indicates that, from less than 1ps to about 100ps after the spark discharge, particles with
               initial positions 2 to 5 mm from the spark center are trapped in the spark. However, this
               is unlikely to cause ignition, because the induction period for “long” spark ignition of
               lycopodium clouds in air, as shown by high-speed photography by Line et al. (1959), is
               on the order of  1ms.
                 It is of interest to note that the radius of the dust-free zone 2 ms after spark discharge,
               as predicted by Figure 5.16, is in close agreement with the experimentalvalue of about
               10 mm found by Line et al. (1959) for the same spark energy, type of dust, and instant
               after spark disch.arge.
                 The Schlieren flash photograph of a rising hot spark kernel in Figure 5.17 may sug-
               gest that Enstad’s assumption, that the buoyancy of the spark kernel can be neglected,
               may not be entirely valid.
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