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11.3  Gaussian-Plume Dispersion Models                          335

            Fig. 11.8 Calculated ground  70
            level SO 2 concentration based
                                     Ground  concentration (ug/m3)  40
            on Gaussian dispersion model  60
                                      50


                                      30
                                      20
                                      10
                                      0
                                        0   1000  2000  3000  4000  5000  6000  7000
                                                 Distance from the stack  (m)

                The plot is shown in Fig. 11.8.

              The aforementioned analyses are applicable to simple cases where the following
            factors are not considered.
            • Varialbe plume rise
            • Variable wind
            • Mixing height
            • Unstable release from source, i.e., puff effect
              Improved models that take one or more of these factors into consideration are
            introduced as follows.



            11.3.2 Plume Rise


            In addition to the effect of the meteorology on the plume dispersion itself, the plume
            rise of a plume also depends on the meteorological parameters. As seen in Fig. 11.7,
            the plume rises gradually and the centerline reaches its highest value eventually.
            Several equations have been developed for plume rise, and the most widely used
            ones are, again by Briggs [4] as follows.
              Plume rise is a result of buoyancy and momentum. They are charaterized with
            the following two parameters called buoyancy flux ðF B Þ and momentum fluxðF M Þ,
            respectively.

                                              q  d
                                                  2
                                    F B ¼  1    s  s  gv s              ð11:35Þ
                                              q a  4
                                             q s  d s  2
                                                 2
                                      F M ¼       v s                   ð11:36Þ
                                            q a  4
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