Page 121 - Air pollution and greenhouse gases from basic concepts to engineering applications for air emission control
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4.1 Particle Motion                                             95

                                               j
                                          3pld p u   vj
                                     F D ¼                               ð4:10Þ
                                              C c
              The Cunningham correction factor for aerosol particles can be determined using
            the following equation recommended by Allen and Raabe [2]


                                                        0:999
                           C c ¼ 1 þ Kn 1:142 þ 0:558 exp                ð4:11Þ
                                                         Kn
            where k is the gas mean free path that was introduced in Sect. 2.1.7.
              There are several alternative equations for the Cunningham correction factor,
            differing only in the numerical factors. For example, Whitby et al. [28] (cited by
            Otto et al. [19]) used a formula as

                                   C c ¼ 1 þ 1:392Kn 1:0783              ð4:12Þ

              And Flagan and Seinfeld [9] give a more complex one as follows.
                      8
                        1 þ 1:257Kn   1:0            Kn\0:001
                      <

                                               1:10
                 C c ¼  1 þ Kn 1:257 þ 0:40 exp      0:001\Kn\100        ð4:13Þ
                                                Kn
                        1 þ 1:657Kn                  Kn [ 100
                      :
              Equation (4.11) is used in this book unless otherwise specified. However,
            readers are suggested to choose the equations in accordance to their specific
            applications.
              Both Knudsen number and Cunningham correction factor are dimensionless
            parameters. Since the theoretical value of C c is always greater than 1, the drag force
            experienced with slipping effect considered is always smaller than the value cal-
            culated with nonslipping assumption.
              For a small particle with irregular shape, both slip factor and shape factor are
            supposed to be considered for particle dynamics analysis. However, the task is so
            complicated that it outvalues the outcome. In air emission engineering, it is well
            acceptable to use the approximate factor calculated for the equivalent volume
            sphere for most irregular particles. The slip factor for randomly oriented fibers
            (L=d\20) is 0–12 % greater than that for the equivalent volume sphere. Drag
            coefficients of different particle shapes are available in the literature (e.g., [12, 15]).



            4.2 Rectilinear Particle Motion


            Steady rectilinear particle motion is the simplest yet important type of particle
            motion in particle dynamics. It is the foundation for the mechanisms of particle
            separation from air stream, namely particulate air pollution control.
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