Page 195 - Advanced Mine Ventilation
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Diesel Exhaust Control                                            175

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           expansion of [u 0 exp( a 0 x)], i.e., u ¼ u 0 (1   a 0 x). Additionally, some of the compo-
           nents of diesel exhaust, e.g., oxides of nitrogen, sulfur dioxide, etc., are likely to be
           absorbed by the walls of roadways, especially if they are wet. Let g be the coefficient
           of absorption. Using a concept similar to previous cases, it is seen that in a differential
           element Dx of the roadway, the input of the material is represented by the term
                          vc
           ½v þ u 0 ð1   a 0 xފ , whereas the loss of material from that same element Dx is given
                          vx
                          2
                          v c
           by the sum of E x v x 2  and gc, which are due to turbulent dispersion and absorption,
           respectively. It is assumed here that walls of roadways are perfect sinks, i.e., concen-
           tration of gases at the wall is zero. These terms are identical in the first two models to
           be developed here.

           11.4.4 Diesel Engines Moving Continuously in a Cycle in a
                   Roadway With Considerable Leakage
           Making a mass balance on a small element Dx of the roadway, the equation of convec-
           tive diffusion is obtained as

                  2
                 v c                   vc
               E x  2   ½v   u 0  ð1   a 0 xފ  þ c ¼ 0                  (11.21)
                 vx                    vx
              The þ and   signs in the second term of the above equation to opposite and con-
           current movement of diesel engine with respect to the air current. The value of E x for
           this situation can be approximated by substituting the velocity v for u, and vDt for the
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           characteristic length d; i.e., E x ¼ Av Dt where A is a constant whose value is given by
               p ffiffiffiffiffiffiffiffiffi
           14.4  l=l r . The value of l is obtained using Reynold’s analogy [11] as
                   l
               l ¼   u 0 ð1   a 0 xÞ                                     (11.22)
                   8a

              Define

                         h   a 0 x i
               u 0     u 0                 u 0
                  ¼ U 0 ;  1      ¼ U m ; and  ð1   a 0 xÞ¼ U L .
                v      v      2             v
              With the above definitions and substituting for E x and l, Eq. (11.21) reduces to

                2
               v c  1   U L vc  lU L
                             þ       c ¼ 0                               (11.23)
               vx 2  AvDt vx   8aAvDt




           1
            For blowing type ventilation, x ¼ 0 plane is at the face and u ¼ u 0 (1 þ a 0 x). The value of a 0 is not
            necessarily same in both cases and is best obtained by actual observations.
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