Page 163 - Advanced Organic Chemistry Part A - Structure and Mechanisms, 5th ed (2007) - Carey _ Sundberg
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staggered conformation at any given instant, but each molecule can rapidly traverse  143
                                                                    9 −1

          through the eclipsed conformation. The rate of rotation is about 6×10 s  at 25 C.
                                                                                          SECTION 2.2
                                                                                          Conformation
                                      H a H        H a
                                          a    H c    H a
                                  H c     H     H     H b
                                    H c  H b  b  c  H b



              Shortly,wewilllearnthatforsomehydrocarbonmolecules,vanderWaalsrepulsions
          are a major factor in conformational preferences and energy barriers, but that is not the
          case for ethane. Careful analysis of the van der Waals radii show that the hydrogens do not
                                                      15
          come close enough to account for the barrier to rotation. Furthermore, the barrier of just
          under 3 kcal is applicable to more highly substituted single bonds. The barrier becomes
          significantly larger only when additional steric components are added, so the barrier must
          be an intrinsic property of the bond and not directly dependent on substituent size. The
          barrier to rotation is called the torsional barrier. There are analogous (although smaller)
          barriers to rotation about C−N and C−O bonds. Topic 1.3 probes further into the origin
          of the torsional barrier in small molecules. The conclusion reached is that the main factor
                                             ∗
          responsible for the torsional barrier is  -  delocalization (hyperconjugation), which
          favors the staggered conformation.


                                               H

                                         H
                                      hyperconjugation
                                      in anti conformation


              The interplay between the torsional barrier and nonbonded (van der Waals) inter-
          actions can be illustrated by examining the conformations of n-butane. The relationship
          between energy and the torsion angle for rotation about the C(2)−C(3) bond is
          presented in Figure 2.11. The potential energy diagram of n-butane resembles that
          of ethane in having three maxima and three minima, but differs in that one of the
          minima is lower than the other two and one of the maxima is of higher energy than
          the other two. The minima correspond to staggered conformations. Of these, the anti
          is lower in energy than the two gauche conformations. The energy difference between
          the anti and gauche conformations in n-butane is about 0.6 kcal/mol. 16  The maxima
          correspond to eclipsed conformations, with the highest-energy conformation being the
          one with the two methyl groups eclipsed with each other.
              The rotational profile of n-butane can be understood as a superimposition of
          van der Waals repulsion on the ethane rotational energy profile. The two gauche
          conformations are raised in energy relative to the anti by an energy increment resulting
          from the van der Waals repulsion between the two methyl groups of 0.6 kcal/mol. The

           15	  E. Eliel and S. H. Wilen, Stereochemistry of Organic Compounds, Wiley, New York, 1994, p. 599.
           16
             G. J. Szasz, N. Sheppard, and D. H. Rank, J. Chem. Phys., 16, 704 (1948); P. B. Woller and
             E. W. Garbisch, Jr., J. Am. Chem. Soc., 94, 5310 (1972).
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