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144  Chapter 6: Fundamentals of Reaction Rates

                           Table 6.2  Forms for translational, rotational, and vibrational contributions to the molecular
                           partition  function
                                 Mode              Partition  function             Model
                           Q./V  = translational   (2mnkBTlh2)3’2         particle of mass  m  in 3D box of
                             (per unit  volume)                        volume  V,  increases if mass increases
                             Qmt = rotational      (8r2ZkBTlh2)“2        rigid rotating body with moment of
                                                                          inertia I per mode; increases if
                                                                           moment of inertia increases
                            & = vibrational     (1 - exp(-hcvlksT))-’   harmonic vibrator with frequency  v
                                                                         per mode; increases if frequency
                                                                        decreases (force constant decreases)




                                                   Qvib  = Qvib, mode lQvib,  mode 2 . . .

                           with a factor for each normal mode of vibration. The A  factor can then be evaluated by
                           calculating the individual ratios. For the translational, rotational, and vibrational modes
                           of molecular energy, the results obtained from simplified models for the contributions
                           to the molecular partition function are shown in Table 6.2.
                             Generally,   Q,,  > Qrot >  Qvib,  reflecting the decreasing freedom of movement in the
                           modes. Evaluating the partition functions for the reactants is relatively straightforward,
                           since the molecular properties (and the related thermodynamic properties) can be mea-
                           sured. The same parameters for the transition state are not available, except in a few
                           simple systems where the full potential energy surface has been calculated. The prob-
                           lem is simplified by noting that if a mode is unchanged in forming the transition state,
                           the ratio for that mode is equal to 1. Therefore, only the modes that change need to be
                           considered in calculating the ratio. The following two examples illustrate how estimates
                           of rate constants are made, for unimolecular and bimolecular reactions.





                           For the unimolecular reaction in Example 6-4, C,H,Cl -+ HCl + C,H,, the transition state
                            should resemble the configuration below, with the C-Cl and C-H bonds almost broken, and
                            HCl  almost formed:
















                            The ratio of translational partition functions (Qi,./Q,,)  is 1 here, and for all unimolecular
                            reactions, because the mass and number of molecules of the reactants is the same as for
                            the transition state. The rotational ratio (Q&,/Q,,,) is given by the ratio of the moments
                            of inertia:  (Z~Z~ZjlZlZ2Z,)1’2.  The moments of inertia are probably slightly higher in the
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