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              Organic Chemical Systems, Theory                                                            455

              largest for small cycles and decrease as the number of
              AOs in the cycle increases. It has become customary to
              refer to the pericyclic reaction paths proceeding through
              aromatic transition states as “allowed” and to those pro-
              ceeding through antiaromatic transition states as “forbid-
              den.” Pericyclic reactions of both types can occur, but the
              former are normally strongly favored if all other factors
              are the same. Many different theoretical approaches, of
              which we mention only two here, have been used to derive
              simple rules that enable one to predict whether a particu-
              lar pericyclic process will be of the allowed or forbidden
              kind. The rules have become known as the Woodward–
              Hoffmann rules, although many other workers have also
              made fundamental contributions to their formulation.  FIGURE 9 Molecular orbital correlation diagrams for the con-
                Although it is possible to distinguish allowed from  certed face-to-face cycloaddition of two ethylene molecules (A)
              forbidden pericyclic reaction paths readily using the  and for the concerted Diels–Alder cycloaddition of ethylene with
                                                                butadiene (B). Symmetry planes preserved throughout the re-
              aromaticity criterion for the transition state, developed
                                                                action path are indicated by dashed lines at the bottom. Their
              originally by Dewar and Zimmerman and just outlined,  numbering on the left is keyed to the subscript on the symmetry
              correlation diagrams are also often used for this purpose.  symbols S (symmetric) and A (antisymmetric) on the molecular
              They are particularly advantageous in the consideration  orbitals.
              of photochemical processes (see Section IV.B). In order
              to construct an MO correlation diagram, the MO energies
                                                                ing. Between them, they contain two electrons, and these
              of the reactant are plotted vertically on one side and those
                                                                two electrons do not contribute to bonding in the molecule
              of the products on the other side. They are identified as
                                                                at the transition state geometry. In effect, the molecule is
              symmetric (S) or antisymmetric (A) with respect to those
                                                                a biradical and contains one less bond than its number of
              symmetry elements that are preserved through the whole
                                                                valence electrons would in principle allow it to have. The
              assumed reaction path and that cut through the bonds be-
                                                                transition state is unfavorable and is of the antiaromatic
              ing formed or broken. The energies of those MOs that have
                                                                type, containing fourelectrons in an array of fourAOs with
              equal symmetries on both sides are then connected, taking  all positive overlaps (isoelectronic with cyclobutadiene).
              account of the noncrossing rule. This rule states that lines  Although it is already apparent which of the two reac-
              corresponding to wave functions of like symmetries must  tions chosen as examples is allowed and which is for-
              not cross. The result is shown in Fig. 9 for the face-to-  bidden, it is useful to consider the construction of the
              face cycloadditions of two ethylenes and of ethylene with  configuration correlation diagram as well (Fig. 10). Here
              butadiene.
                In the latter case (Fig. 9B), all occupied and bonding or-
              bitals of the reactant electronic ground state remain bond-
              ing throughout the reaction path and in the product as well.
              Similarly, all antibonding unoccupied MOs of the starting
              electronic ground state material remain antibonding and
              unoccupied. Clearly, bonding is preserved throughout the
              reaction path, and one would expect the transition state
              to be of relatively favorable energy. Indeed, the transition
              state is of the aromatic type, containing six electrons in
              the cyclic area of orbitals, with positive overlaps of all the
              orbitals (isoelectronic with the π system of benzene).
                On the other hand, in the former case of two ethylenes
              one of the originally occupied bonding MOs of the reac-
              tant becomes antibonding and unoccupied in the ground
              electronic state of the product, and one of the antibonding
              and unoccupied orbitals of the reactant becomes bonding  FIGURE 10 Configuration (thin lines) and state (thick lines) corre-
                                                                lation diagrams for the concerted face-to-face cycloaddition of two
              and occupied in the ground state of the product. In the
                                                                ethylene molecules (A) and for the concerted Diels–Alder cycload-
              region of transition state geometries halfway through the  dition of ethylene to butadiene (B). Full lines, singlets; dashed
              reaction path, both orbitals are approximately nonbond-  lines, triplets. See legend to Fig. 9.
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