Page 86 - Advanced Organic Chemistry Part A - Structure and Mechanisms, 5th ed (2007) - Carey _ Sundberg
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                                                                                          SECTION 1.4
                                                                                        Representation of
                                                                                        Electron Density
                                                                                           Distribution











           Fig. 1.28. (a) Electron density of the methyl cation in the plane of the atoms (truncated at C); (b) gradient
           vector field !  r  of the electron density distribution terminating at H  I H  ,C  I C  ; the bond path and
           critical point (II); and the zero flux surfaces (III) partitioning the ion into C and H atoms. From E. Kraka
           and D. Cremer, in Theoretical Models of Chemical Bonding, Part 2, Z. B. Maksic, ed., Springer Verlag,
           Berlin, 1990, pp. 459, 461.

          where ' and ' are vectors to a specified electron density in the two dimensions
                        2
                 1
          perpendicular to the bond path at the bond critical point.












          The ellipticity of the electron density in benzene is 0.23, while that in ethene is
          0.45 using HF/6-31G electron density. Ellipticity can provide structural insight as
                            ∗
          an indicator of   character. For example, the ellipticity of the C(2)–C(3) bond in
          1,3-butadiene is about one-seventh that of the 1,2-bond, indicating a modest contri-
          bution from the   bond. Bond ellipticity can also indicate delocalization through
          hyperconjugation. For example, the C(2)–C(3) bond in propene has an ellipticity of
          0.03, reflecting the   −  interactions in the molecule (see pp. 22–23).
                               ∗
              We would expect the electron density to respond to the electronegativity of
          the atoms forming the bond. This relationship has been examined for the hydrogen
          compounds of the second-row elements. Table 1.15 gives the AIM radius for each of
          the second-row elements in its compound with hydrogen. Note that the bond critical
          point moves closer to the hydrogen as the other element becomes more electronegative.
          That is, the hydrogen gets smaller as electron density shifts to the more electronegative
          element. The charge density at the bond critical point,   , rises rapidly at first, but
                                                          c
          then levels off going toward the right in the periodic table. The initial increase reflects
          the increasing covalent character of the bond. The bonds to Li and Be are largely ionic
          in character, whereas the other bonds have increasing covalent character.
              These relationships are depicted in Figure 1.29. Note that the hydrogen changes
          from hydridelike character in LiH to the much diminished electron density in H–F.
          There is steadily greater sharing of electron density from Li to C, as indicated by the
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