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Mechanisms Intermediate Between SN1 and SN2  249






















      Figure 5.12 Projection of the limiting SN1 reaction coordinate. Transition state of the rate-
                determining step is *,.  The central minimum,  o,,  is the solvated  ion pair.

                       +-N    C    X+            N+   C  c-X
                           Motion  1,              Motion  I,
                              38                      39
      and 39 is a  displacement  toward  the upper  right. These four  motions we  have
      indicated in Figure 5.1 1. Greater electron supply to C (for example from a more
      electron-releasing  substituent) will make N  less eager to bond and will allow X
      to  depart more  easily;  since  part  of  motion  R,  (or R,)  is  helped  and  part  is
      hindered, the position of the transition state along the reaction coordinate will be
      little affected.  The same change, however, assists 1, and makes  1, less favor-
      able; the transition state will therefore shift in the direction of I,, to *'. The new
      reaction coordinate, the dashed line in Figure 5.11 brings the system to a transi-
      tion state that is still symmetric with respect to bond making and breaking, but is
      looser; that is, the bond to N is less formed and that to X is more broken at the
      transition state than before the structural change. Electron withdrawal at C will
      have the opposite effect.
          If the structure is changed further, so as to make electron density even more
      available to C, the curve will eventually move all the way  to the edge and will
      follow the line in Figure 5.12. The transition between  SN2 and SN1 is  perhaps
      most easily seen by starting from  SN1, Figure 5.12. Suppose that we make C+ a
      less good cation  by  electron withdrawal from  C. At  the ion-pair  intermediate,
      oi, all motions are bound vibrations.  If .C+ is made  a worse cation, N  and X-
      will  tend  to  draw  closer  and  the  shift  will  be  toward  the  upper  right,  to  o;,
      Figure  5.13.  At  the  same  time,  0;  will  be  raised  in  energy  compared with  oi,
      because the carbocation  is  less well stabilized.  The transition  state *,  will  also
      move. Motion along the reaction coordinate, R,,  is C-X   breaking only, and it is
      hindered by making C+ a poorer ion, so the transition state moves in the direction
      R,.  But motion  I,, Figure 5.13, is approach of N; it is a bound vibration and is
      assisted by making C+ a poorer ion, and so the transition state should also move in
      direction 1,. Since motion along the reaction coordinate is expected to dominate
      when  both  kinds  occur  (rule 3,  Section  2.6,  p.  104), we  expect  the  resultant
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