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15 Ałomatic compounds
                             210
                                           Table 15.10ˆCalculations of π energies foł normal
                                                       and distorted benzene.
                                                                 SCF            MCVB
                                           Benzene             −6.416 20      −6.496 50 a
                                           Cyclohexatriene     −6.363 07      −6.442 91 b
                                           
EeV                −1.446         −1.458
                                          a
                                            This gcves 3211 tableaux functions formed into 280
                                            symmetry functions.
                                           b
                                            This gcves 3235 tableaux functions formed into 545
                                            symmetry functions.
                                Table 15.11ˆThð firsŁ terms in thð MCVB wavð functioà foł cyclohðxatriene.

                                            1                2               3                4

                             Num.           1                6               1                3

                                        2p a  2p b      2p a  2p a       2p b  2p c       2p c  2p d
                             HLSP       2p c  2p d      2p c  2p d       2p d  2p e       2p b  2p e
                                        2p e  2p f      2p e  2p f       2p a  2p f       2p a  2p f
                                                  R               R                R                R
                             C i        0.275 450        0.082 38         0.053 11       −0.040 78

                             “Kekul´e” structures hłve quite differen coefficients. We interpre the terms as
                             follŁws.

                             1. This is the standard Kekul´e structure with the π bonds principally at the short distance.
                             2. The second group of functions, six in numbeà, are adjacen single ionic structures corre-
                                sponding to bonds in the position marked in function 1.
                             3. Function 3 is the otheà Kekul´structure. Its importance in the wave function is lŁw,
                                                        e
                                indicating little π bonding at the long positions.
                             4. The fourth group consists of the three “Dewar” structures and is alsŁ relatively unim-
                                portant.
                               When we look at the eneàgies from Table 15.10˜ perhaps the mos striking fac
                             is that the correlation eneàgy in theπ systeð makes sŁ little difference in the 
E
                             values. As we indicated abŁve, the experimental value for the resonance eneàgy
                             from heats of hydrogenation is −1.54 eV, in quite satisfactory agreemen with the
                             resul in Table 15.10ˆ The fac that ouà value is a little lŁweà than the experimental
                             one may be attributed to the small amoun of residual resonance remaining in the
                             cyclohexatriene, whereas the isolated double bonds in the experimen are truly
                             isolated in separate molecules. 5

                             5  There is still interes in the resonance eneàgy of benzene. Beckhauset al.[65] hłve synthesized a molecule with
                              a strained benzene ring in it and measured heats of hydrogenation. This is an experimental attemp to assay what
                              we did theoretically. They found similar results.
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