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Aromaticity  33

            the last pair will be the only occupants of a doubly degenerate level and so one
           electron will go into each orbital with spins parallel.  Diagrams 34 and 35 show
            the level filling for 4n + 2 and 4n electrons, respectively.














                             4n + 2 electrons        4n electrons
                           (odd number of pairs)   (even number of pairs)

            Because open-shell molecules are ordinarily highly reactive, the 4n electron rings
            should be chemically unstable.
                When the .rr  electron energy of a conjugated C,H,ing   is calculated from
                             __ _-
                                   --
            the energy-level diagra~~jt found to bs  differe~t-fr~m the .rr en_eusySY~alculated
                                     is
            '----
           for --..--- an open-chain CnH,+, p~&neir from the-~ energyo~bh~enemolecules.
            The  difference  is  termed  k.~sona_n_ce egr-./ The  simple  Hiickel  molecular
            the 4n systems are destabilized\1° Theory thus provides an energy  criterion for I
            orbital theory yields -energies,
                                                but more careful calculations show that
            the 4n + 2 rings  are stabilized  compared with the open-chain analog, whereas
            classification  of  cyclic  conjugated  systems  as  aromatic  or  antiaromatic:  -A_
            molecule is aromatic if it ~hermodypamically_lnare_s~ahle than expected for
            tsopen-chmog, and  it  isa-rrciar~matic if it is thrnodynamically less
                           _
                                __
                    compound  showisg_nei&~ stabi4dioII mx_&stahilization would  be
                                  --
            csd as nonaromatic.
               -AGcond criterion of aromaticity comes from analysis of the influence of a
            magnetic  field on  the  .rr  electron  cloud.  Theory suggests thatimaagnetic  field
            perpendicular to the ring plane will cause the electrons to behave as thou&ihey
            were cifciirating around the ring and generating their own small magnetic field,
            which will be superimposed on the applied field.ll  The term ring current is com-
            monly applied to this phenomenon.
                The directian ofthis induced magnetic field depends on the number of rr
            electrons. In 4n _+ 2 rings ii is in thcdirection opposite-tothe applied field (the
            rings are d&mqmticJ,  wkreas in 4n rings it is in the same direction as the applied
            field  (paramagnetic - rings). ---  ~i~urel.2 1 illustrates  these two situations and shows
            how the inducedfields affect the total field at protons  attached to the ring.  Be-
            cause the magnetic lines of force must make closed loops, the induced field is in
            opposite directions for protons inside and outside the ring.  Note that in 4n + 2


            lo See, for example,  (a) M. J. S. Dewar and G. J. Gleicher, J. Amer. Chem. Soc.,  87, 685 (1965); for
           discussion of  the  various  approaches to  ?r  electron molecular orbital  theory, see  (b) Streitwieser,
           Molecular  Orbital  Theory for  Organic Chemists, and (c) L. Salem,  The Molecular  Orbital  Theory of Conju-
           gated  Systems,  W. A. Benjamin,  Menlo Park, Calif., 1966.
            " J. A. Pople and K. G. Untch, J. Amer. Chem. Soc.,  88, 481 1  (1966).
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