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110                                               Advanced Mine Ventilation

         Table 8.3 Aerodynamic Shape Factors (ASFs)


          Author                Material         Instrument   ASF
          Timbrell [6]          Ground glass     Elutriator   1.49
          Timbrell [6]          Coal             Elutriator   1.35
          Sawyer and Walton [8]  South Wales coal  Conifuge   1.35
          Sawyer and Walton [8]  Lancashire coal  Conifuge    1.31
          Sawyer and Walton [8]  Cumberland coal  Conifuge    1.35
          Sawyer andWalton [8]  China clay       Conifuge     1.61
          Sawyer and Walton [8]  Quartz          Conifuge     1.67
          Thakur [1]            Bituminous coal  Elutriator   1.42 (1.34e1.48) a

         a
          ASF ¼ 1.34 for Stoke’s diameter of 3.98 mm.
         ASF ¼ 1.37 for Stoke’s diameter of 2.77 mm; ASF ¼ 1.38 for Stoke’s diameter of 1.97 mm; ASF ¼ 1.48 for Stoke’s
         diameter of 1.48 mm.

         8.3   NonSettling Fraction of Respirable Dust


         Thakur [1] postulated that a small portion of respirable dust (under 1 mm of unit den-
         sity) may not settle by gravity or be affected by water sprays. As the particle size goes
         down, its settling velocity reduces but its random movement owing to Brownian mo-
         tion increases. The nonsettling dust size upper limit is defined as the size for which
         settling velocity equals Brownian displacement [1].
            Settling velocity for a particle was already derived in article 8.1. Brownian motion
         of particle suspended in air is given by Einstein [9] in Eq. (8.12).

               2
             X ¼ 2 Dt                                                   (8.12)
               B
                2
         where X is the mean square displacement with respect to any coordinate axis in time,
                B
         t. D is the diffusion coefficient of the particle.
            Einstein defined,
             D ¼ KTB                                                    (8.13)

         where K is the Boltzmann constant; T, absolute temp in Kelvin; B, particle mobility
         defined in Eq. (8.10).
            Fuchs [2] expanded Eq. (8.13) further and concluded:

                                            1
                                         4D  2

             X ¼ Average displacement=s ¼                               (8.14)
                                         p
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