Page 469 - Advanced Organic Chemistry Part A - Structure and Mechanisms, 5th ed (2007) - Carey _ Sundberg
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450               that 3,2- and 6,2-hydride shifts were occurring under stable ion conditions. Activation
                       energies of 10.8 and 5.9 kcal/mol, respectively, were measured for these processes.
     CHAPTER 4
     Nucleophilic Substitution
                                              2,6-shift         2,3-shift
                                                                               +
                                    +         E  = 5.9  H  +  H  E  = 10.8
                                                                 a
                                               a
                                        H              6      3             H
                           These results, which pertain to stable ion conditions, provide a strong case that
                       the most stable structure for the norbornyl cation is the symmetrically bridged ion.
                       How much stabilization does the bridging provide? An estimate based on molecular
                       mechanics calculations and a thermodynamic cycle suggests a stabilization of about
                       6 ± 1kcal/mol. 140  A gas phase value based on mass spectrometric measurements is
                       11 kcal/mol. 141  Gas phase hydride affinity and chloride affinity data also show the
                                                                                     ∗
                       norbornyl cation to be especially stable. 142  MO calculations (MP2/6-31G ) give a
                       bridged structure that is 13.6 kcal more stable than the classical secondary structure and
                              13
                       predicts C chemical shifts and coupling in agreement with the experimental results. 143
                       The C(1)−C(6)=C(2)−C(6) distance is found to be 1.832 Å by an MBPT(2)/DZP
                       computation. 144  The difference in energy between the two structures is reduced only
                       slightly when calculations include the effect of solvation, indicating that the bridged
                       ion would be more stable than the classical ion, even in solution. 145  There is also good
                       agreement between calculated and observed infrared spectra. 146
                           Werstiuk and Muchall computed the structure at the B3LYP and QCISD levels.
                       The minimum energy structure was found to be a bridged ion with a C(1)−C(6)
                       distance of 1.892 Å and a C(1)−C(2) distance of 1.389 Å (B3LYP/6-311+G(2d,2p)).
                       They applied AIM concepts to a description of the structure. 147  This analysis resulted
                       in the description of the norbornyl cation as a   complex, consistent with the relatively
                       long C(1)−C(6) and C(2)−C(6) and short C(1)−C(2) distances indicated above. The
                       bond critical points found by the AIM analysis show a T-configuration with the bond
                       from C(6) intersecting with the C(1)−C(2) critical point. There is no bond path directly
                       to C(1) or C(2). Carbon 6 is then best described as tetravalent, with the C(1)−C(2)
                       double bond as the fourth ligand. These computations also examined the effect of
                       bringing C(6) closer to C(1) and C(2) to form the more strongly bridged structure that
                       would be implied by a corner-protonated cyclopropane representation.

                                             H     H     H     H
                                                +
                                                            +
                                              π complex   corner-protonated
                                                          cyclopropane
                       140   P. v. R. Schleyer and J. Chandrasekhar, J. Org. Chem., 46, 225 (1981).
                       141   M. C. Blanchette, J. L. Holmes, and F. P. Lossing, J. Am. Chem. Soc., 109, 1392 (1987).
                       142
                          R. B. Sharma, D. K. S. Sharma, K. Hiraoka, and P. Kebarle, J. Am. Chem. Soc., 107, 3747 (1985).
                       143   P. v. R. Schleyer and S. Sieber, Angew. Chem. Int. Ed. Engl., 32, 1606 (1993).
                       144
                          S. A. Perera and R. J. Bartlett, J. Am. Chem. Soc., 118, 7849 (1996).
                       145
                          P. R. Schreiner, D. L. Severance, W. L. Jorgensen, P. v. R. Schleyer, and H. F. Schaefer, III, J. Am.
                          Chem. Soc., 117, 2663 (1995).
                       146   W. Koch, B. Liu, D. J.DeFrees, D. E. Sunko, and H.Vancik, Angew. Chem. Int. Ed. Engl., 29, 183
                          (1990).
                       147
                          N. H. Werstiuk and H. M. Muchall, J. Phys. Chem. A, 104, 2054 (2000); N. H. Werstiuk and
                          H. M. Muchall, Theochem, 463, 225 (1999).
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