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160  Chapter 7: Homogeneous Reaction Mechanisms and Rate Laws
                           We eliminate  ~~.u,~.  by applying the stationary-state hypothesis to  C,HsO’,  ~C2u5@  = 0,
                           and also to the other chain carrier, CHj.


                                       rCzHsO’  =  kc,   -  hCC2H50*  +  hcAcCH;  -  2k4c&2Hs0a  =  o
                                                 ‘Cl-I;  =  k2Cc2H5v   -  k3CACCH;  =  o
                           Addition of these last two equations results in

                                                                      112   112
                                                      CC2H50*  =  (WW  cA
                           and substitution for  cc2n500  in the equation for  ru  gives

                                                       rB  =  k2(k1/2k,)“2c~2

                           which is the rate law predicted by the mechanism. According to this, the reaction is  half-
                           order.
                           (b) If we calculate the  vah.te of  kobs  = (-rA)/cA1’2  for each of the five experiments, we
                           obtain an approximately constant value of 0.044 (mol  m-3)1’2  s-t.  Testing other reaction
                           orders in similar fashion results in values of  kobs that are not constant. We conclude that
                           the experimental results support the proposed mechanism.
                           (c) From (b), we also conclude that

                                                        k obs  =  k2(k1/2k4)  112
                           from which

                                               dlnkobs   _  dlnk2  1 dln k, -  1 dln k4 -
                                                                  -
                                                                            -
                                               -  c  -  -  dT  +z  dT      2  dT
                           or, from the Arrhenius equation, 3.1-6,


                                                     EA  =  EA,  + $A, -  EAI)

                           (d) From equation 7.1-2, the chain length is

                                                    CL = k2(k1/2k4) 1’2ca/2/kl  cA
                                                        =  k2(2kl  k4cA)-“2


                             The rate law obtained from a chain-reaction mechanism is not necessarily of the
                           power-law form obtained in Example 7-2. The following example for the reaction of
                           H,  and Br,  illustrates how a more complex form (with respect to concentrations of
                           reactants and products) can result. This reaction is of historical importance because it
                           helped to establish the reality of the free-radical chain mechanism. Following the ex-
                           perimental determination of the rate law by Bodenstein and Lind (1907),  the task was
                           to construct a mechanism consistent with their results. This was solved independently
                           by Christiansen, Herzfeld, and Polanyi in 1919-1920, as indicated in the example.






                           The gas-phase reaction between  H,  and  Br,  to form HBr  is considered to be a chain reac-
                           tion in which the chain is initiated by the thermal dissociation of  Brz  molecules. The chain
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