Page 284 - Mechanism and Theory in Organic Chemistry
P. 284

1,2-Shifts in Carbenium Ions  271











      Figure 6.1 The ideal relationship of  the empty p  orbital to the migrating group  (Z) for  a
               1,2-shift.
      the apparent  1,2-hydride shift  (Equation 6.8) in the 2-adamantyl cation (3)
      was shown to be entirely quenched in highly dilute solution.ll Thus it must be
      an inter-,  not an intramolecular reaction. Further, the apparent 1,2-methyl shift
      in the 2-methyladamantyl cation (4, Equation 6.9) has been shown by isotope










      labeling to occur by  a  complicated skeletal  rearrangement.12 In both  these
      cases the C-Z   bond and the vacant p  orbital, which in 3 and 4 is perpendic-
      ular to the plane of the page, form a dihedral angle of 90°.13 In this worst of
      all possible  stereochemical situations the simple  1,2-shift cannot occur, and










      rearrangement  must take another pathway.


      The Timing of the Migration in Acyclic Alkyl Systems
      Acommon~henomenon in organic chemistry, illustrated further in PrablemsG.1
      amkU&-that    a sroup adiacent to t&  leaving group acts as-a~ intramolecular
      nucleophile. This can occur if  the neighboring  Froup  has  an unshared  pair of
      elsnns or a double ----- bond -  as - shm, -   for example, in  Equations 6.10 and 6.1 1.
      The  cyclic structures  5 or  6  may  sometimes  be  isolated,  but  more  often  are
      attacked by a nucleophile: The ring is  opened  and some (or all) of the product
      may be rearranged.



      l1 P.  v.  R. Schleyer,  L.  K.  M.  Lam,  D. J. Raber, J. L.  Fry,  M. A.  McKervey, J. R. Alford,  B.  D.
      Cuddy, V. G. Keizer, H. W. Geluk, and J. L. M. A. Schlatman, J. Amer. Chem. Soc., 92, 5246 (1970).
      l2 2. Majerski,  P. v.  R. Schleyer, and A.  P.  Wolf, J. Amer. Chem. Soc.,  92, 5731  (1970).
      '3  (a) See notes  11 and 12; (b) D.  M. Brouwer and H. Hogeveen, Rec.  Trav. Chitn. Pays-Bas, 89, 21 1
      (1970).
   279   280   281   282   283   284   285   286   287   288   289