Page 1070 - Advanced Organic Chemistry Part A - Structure and Mechanisms, 5th ed (2007) - Carey _ Sundberg
P. 1070

1054                  Larson and Cremer have explored another approach to dissecting BDE into
                       inherent and RSE effects. 228  There is a relationship between C−H BDE and the vibra-
     CHAPTER 11        tional frequencies of the bonds. 229  Furthermore, the vibrations can be determined for
     Free Radical Reactions  C−H bonds in specific conformations, for example, the equatorial and axial bonds in
                       cyclohexanes or the anti and gauche bonds in amines.

                                                               .
                                            H                  .  H gauche 2955.4 cm –1
                                             2891 cm –1    H
                                                               N
                                              H
                                             2923 cm –1     H     H
                                                               H
                                                                     –1
                                                            anti  2879.5 cm
                                          Ref. 230                  Ref. 231
                                   Variation in vibrational frequencies of stereochemically distinct bonds
                           The measurement of the vibrational frequencies provides a means to compare the
                       relative stabilization in radicals with effects already present in the reactant molecules.
                       Following up on experimental work that demonstrated that spectroscopic C−H-bond-
                       stretching frequencies correlate with bond strength, 229  Larson and Cremer developed
                       reliable computation methods for calculating C−H frequencies and from them inherent
                       (or ideal) bond energies. The difference is the radical stabilization (or destabilization
                       energy), as indicated in Figure 11.16.



                                       Energy

                                            D e ideal       SE = ΔD  = D   exp  – D   ideal
                                                                    e
                                                                 e
                                                                         e
                                                 D (0) ideal
                                                  0


                                                           D (0) exp  D e exp
                                                            0



                                              A – B              A•    +    B•
                                                    Bond Distance A – B
                                       Fig. 11.16. Determination of fragment stabilization energy
                                       (SE) by comparison of D e (exp) with D e (ideal). D 0 includes
                                       correction for zero point energy. Reproduced from J. Mol.
                                       Struct., 485/486, 385 (1999), by permission of Elsevier.


                       228   J. A. Larson and D. Cremer, J. Mol. Struct., 485/486, 385 (1999).
                       229
                          D. C. McKean, Chem. Soc. Rev., 7, 399 (1978); D. C. McKean, Int. J. Chem. Kinetics, 21, 445 (1989).
                       230   J. Caillod, O. Saur, and J.-C. Lavalley, Spectrochim Acta, 36A, 185 (1980).
                       231
                          J. L. Duncan, D. C. McKean, J. Torto, A. Brown, and A. M. Ferguson, J. Chem. Soc., Faraday Trans.,
                          II, 84, 1423 (1988).
   1065   1066   1067   1068   1069   1070   1071   1072   1073   1074   1075