Page 449 - Dust Explosions in the Process Industries
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               1000
                800
                600
             I 400
             7
             E
             I
             >
                200
             z
             w
             z
             o_
             k  100
             z
             9  80
             f  60
             I
             z
             z  40
                20
                 10   I  I  I   I  I  I   I  I  I
                  0                5               10
                            SPARK  GAP LENGTH  Lmml

             Figure 5.21  Influence of electrode gap length on the minimum ignition energy of clouds of four metal
             dusts in air  at atmospheric  pressure. Dust  concentration corresponds  to equivalence  ratio 0.65.
             Surfaceholume mean particle size is 40 pm (From Ballal,  1980).



             optimum gap length. This is consistent with the general picture for premixed gases, for
             which a close correlationbetween quenching distance and minimum ignition energy has
             been established.
               Norberg, Xu, and Zhang (1988) found that the optimum spark gap length for igniting
             clouds in air of various easily ignitable powders was in the range 6-8  mm. The capaci-
             tive sparks were of the short-duration type (low series inductance and resistance). The
             minimum ignition energies were in the range 1-6  mJ.



             5.3.5
             THEORIES OF ELECTRIC SPARK IGNITION OF DUST CLOUDS

             Smielkow and Rutkowski (1971) derived a semi-empirical equation for the minimum
             electric spark ignition energy of dust clouds. Their experiments disclosed the following
             empirical relationship:

                                                                                     (5.29)

             where Eminis the minimum ignition energy (mJ) and S’   is the spatial laminar flame front
             speed (cds) of the dust cloud in question, and A is a constant.
               The semi-empirical equation was obtained by inserting a Mallard-le Chatelier-type
             expression for S’(see  Section 4.2.1 in Chapter 4) into equation (5.29).
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