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6.4 Simple Collision Theory of Reaction Rates  133

                             For the bimolecular reaction 2A  + products, by combining equations 6.4-12 and -13,
                           using equation 6.4-7a to eliminate ZAA, and converting completely to a molar basis, with
                           (rSCT)  in mol  L-i s-i, ck, = 1000  NA,,cA,  where  cA  is in mol L-l,  and  k,lm* = RIM,,
                           where MA is the molar mass of A, we obtain



                                             =  2000pN,,d&i-R/M,)1’2T1’2,-E”‘RTc~            (6.4-14)
                                        TSCT                                    =  k,,,Ci
                            where
                                              kSCT =  2000pN,,d&rRIM,)“2T1’2,-E*‘RT          (6.4-15)

                             We may compare these results with a second-order rate law which exhibits Arrhenius
                           temperature dependence:

                                                             c2  =  A~-EAIRT~~
                                                    r  ohs  =  k ohs   A   A                   (6.1-1)
                           We note that the concentration dependence (ci)  is the same, but that the temperature
                           dependence differs by the factor T1”  in rscr. Although we do not have an independent
                           value for E* in equations 6.4-14 and -15, we may compare E* with EA  by equating r,cT
                           and  r,b,;  thus,

                                                           k ohs  =  kSCT
                                                    d In k,,,ldT  = d In k,,,/dT

                           and, from the Arrhenius equation, 3.1-6,

                                                     E,IRT2  =  1/2T   +  E*IRT2

                           or


                                                         EA  =  ~RT+E*                        (6.4-16)

                           Similarly, the pre-exponential factor AsCT can be obtained by substitution of E* from
                           6.4-16 into 6.4-15:

                                               ASCT =  2000pN,,d;(~RIMA)1”e1’2T”2            (6.4-16a)

                           According to equations 6.4-16 and -16a, EA  and A are somewhat dependent on T. The
                           calculated values for A,,, usually agree with measured values within an order of mag-
                           nitude, which, considering the approximations made regarding the cross-sections, is sat-
                           isfactory support for the general concepts of the theory. SCT provides a basis for the
                           estimation of rate constants, especially where experimental values exist for related reac-
                           tions. Then, values of  p  and  E*  can be estimated by comparison with the known system.






                           For the reaction 2HI + H, + I,, the observed rate constant (2k in r,, = 2kc&) is 2.42 X
                            10e3  L mol-’  s-l at 700 K, and the observed activation energy, EA,  is 186 kJ mol-’
                           (Moelwyn-Hughes, 1957 p. 1109). If the collision diameter,  dHI,   is 3 5 X  lo-lo  m for HI
                            (M  =  128),  calculate the value of the (“steric”)  p  factor necessary for’agreement between
                           the observed rate constant and that calculated from the SCT.
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