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156  Chapter 7: Homogeneous Reaction Mechanisms and Rate Laws

                           If we simply add the three steps, we do not recapture (A). To get around this, we introduce
                           the  stoichiometric numbel;  S,  for each step, as the number by which that step must be
                           multiplied so that addition of the steps results in (A):

                                                     sl(l) + d2) + +(3)  = (4                  (7.1-1)

                           where  sl,  s2,  and  s3  are the stoichiometric numbers for the three steps. To determine their
                           values systematically, we utilize the stoichiometric coefficients in the three steps for each
                           species in turn so as to correspond to the coefficient in (A):

                                    N,O,   :  - Is,  + OS, + OS, (from the three steps) = -2 (from (A))
                                    NO,:                             1st  + (- 1 + l)s,  +  2s3  = 4
                                    0,:                                    OS1   +  lS2  + OS3 =  1
                                    NO,:                                   1st   -  ls2   -  ls3  = 0
                                    NO:                                    OS1   +  182  -  ls3  = 0
                           This set of linear equations can be solved by inspection, or, more formally, by Gauss-Jordan
                            reduction of the augmented coefficient matrix:










                            with the result s1 = 2, s2  = 1, and s3  = 1. (Note that in this case the last two of the five
                            equations are redundant in obtaining values of the three stoichiometric numbers.) Thus,
                            the three steps are consistent with (A) if added as

                                                      2(1)   + l(2) +  l(3) =  (A)
                            (b) From the mechanism, step  (2),


                                                         rO*  =  k2  cNO, cNO,                    09

                            We eliminate  cNos  (not allowed in the final rate law) by applying the stationary-state hy-
                            pothesis to NO,,  rNo3  = 0 (and subsequently to NO):
                                     rNO,  =  klCNz05  -  k-1CN02CN03    -  k2cN0,cN0,   -  k3cNOcN03  =  o  (0


                                                 rNO  =  k2CN02   cNO,   -  k3  cNOcNO,  =  o     CD)
                            from (D),

                                                         CNO  = (kdk3h02                           (W

                            from (C) and (E),

                                                                 kl   cNzO,
                                                      cNO,  =                                      (F)
                                                             (k-l  +  2k,k,02
                            from (B) and (F),


                                                               klk2                               63
                                                       ro2  =  kk,  + 2kzCNZo5
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