Page 191 - Advanced Mine Ventilation
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Diesel Exhaust Control                                            171

              Initial Condition 1: Just before the engine starts working, concentration of diesel
           exhaust in the mine air is zero, i.e.,

               c ¼ 0at t ¼ 0 for all x > 0                               (11.12)

              The solution of Eq. (11.9) with the above boundary and initial condition is derived
           by Thakur [8] and is given below:
                                ⎡   xV t ⎛  −  V x  Vr ⎞  2t  V x  ⎤
                                ⎢  erfc  r  −  ⎜  1+  r  +  ⎟  e  r  erfc ⎥
                            qc ⎢     2E t  ⎝   E x   E x ⎠  E x   ⎥
                                       x
                        c=    i  ⎢                               2 ⎥     (11.13)
                           2FV                    1/2    ⎛
                               r  ⎢  x+V t +  2V  ⎛  t ⎞  exp −  x V t ⎞ −  r  ⎥
                                     r
                                ⎢  2E t    r ⎜  E π      ⎜ ⎟  ⎜  2 E t  ⎟  ⎟  ⎥
                                ⎣    x      ⎝  x ⎠       ⎝   x ⎠  ⎦
              Concentration, c, assumes its maximum value at x ¼ 0 and is readily obtained from
           Eq. (11.13).
                                   ⎡     Vt  ⎛ −  V t ⎞  2        ⎤
                                   ⎢  erfc  r  −  ⎜  1+  r  ⎟  erfc  ⎥
                               qc i ⎢  2E t ⎝  x  E x ⎠           ⎥
                        c   =      ⎢                              ⎥      (11.14)
                         x=0
                              2FV r  ⎢  Vt     ⎛  t ⎞  1/2  ⎛  V t ⎞  r 2  ⎥
                                       r
                                   ⎢  ⎣  2E t  +  2V r ⎜  ⎝  E π ⎟  exp −  ⎜  ⎝  4 E x ⎠  ⎟  ⎥  ⎦
                                                 x ⎠
                                        x
              Now, if we let t /N, the limiting value of the maximum concentration at x ¼ 0is

                     qc i             qc i
               C L ¼     ð1 þ erfðNÞÞ ¼                                  (11.15)
                    2FV r             FV r
              This is the same as the effective ventilation formula of Holtz and Dalzell [10].
           Mathematically, the maximum concentration growth around the engine for any finite
           travel time will, of course, be less than that predicted by the effective ventilation for-
           mula. However, for large travel times the concentration around the engine is likely to
           reach the limiting value.
              To evaluate Eq. (11.13), q and c i are available from engine test data. E x can be
           calculated from friction factors. For noncircular roadways, the radius, a, is substituted
           by the hydraulic radius defined as R h ¼ (2[Area]/[Perimeter]). To determine the con-
           centration growth around the engine with time, several evaluations of Eq. (11.13) are
           needed for different x and t. A computer program was written to solve Eq. (11.13) and
           is available in Thakur’s thesis [8].
              A special case of Eq. (11.13) is when the diesel engine travels in the same direction
           as the air current with the same velocity. This is the worst possible situation. In this
                                                                      q vc
           condition, the only convective term results from exhaust emissions, i.e.,  2F vx  instead
               vc
           of V r vx  in Eq. (11.9). All other terms have the same meaning as before.
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