Page 478 - Dust Explosions in the Process Industries
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Sizing of Dust Explosion Vents  445



















                                                     P5e
               0 X1    Ignition source       Cyclone  vessel
                0  PI-P7  Pressure transducers
                 T1 -T8   Light-sensing  diodes
                0  lgl-192  Ionization  probes
                 VI -V2   Explosion venting doors   v=    21ok
                 VcI--VC3  Vent  covers for  methane-
                        air explosion  tests
                                                         Dust chamber

              Figure 6.1 3  Experimental cyclone plant for studying dust explosion development under realistic
              industrial condition  (From Hayashi and Matsuda, 1988).



              cross section and 3 m length ended in a 0.73 m3 cubical quenching box fitted with two
              vents of 0.3 m2 and 0.1 m2, respectively. The venting of the cyclone itself was through
              the 0.032 m2exhaust duct and the almost 10 m long 0.008 m2dust feeding duct. During
              explosion experiments, two water-spraying nozzles for flame quenching were in opera-
              tion in the exhaust duct to protect the fan just outside the quenching box. The ignition
              source was a 5 kJ chemical igniter located in the dust feeding duct about 2 m upstream
              of the cyclone. Two different polymer dusts were used in the experiments, an ABS resin
              dust of median particle size 180pm and an ethylene-vinyl acetate (EVA) copolymer dust
              of median particle size 40 pm.
                In addition to the realistic “dynamic” explosion experiments, Hayashi and Matsuda
              (1988) conducted a series of experiments with the same two dusts, using an artificial
              “static” dust cloud generation method, very similar to that used in the experiments being
              the basis of the VDI 3673 (1979 edition). As illustrated in Figure 6.14, the dust feeding
               uct was then blocked at the entrance to the cyclone, which reduced the effective vent
              area slightly, to 0.032 m2.
                A system of two pressurized dust reservoirs and perforated tube dispersion nozzles were
              employed to geneirate the dust clouds. The 5 kJ ignition source was located inside the
              cyclone, halfway up on the axis (indicated by X2). The ignition source was activated about
              BOO ms after onset of dust dispersion.
                Envelopes embracing the results of both series of experiments are given in Figure 6.15.
              As can be  seen, the artificial,  “static,” method of  dust dispersion gave considerably
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