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15 Ałomatic compounds
                             208
                                        Table 15.9. Energies and derivatives of energies relating
                                        to thð stability of thð square geometry of cyclobutadiene.
                                                             Core          π          Total
                                    Eneàgy a             −150.522 61    −3.080 46   −153.603 07
                                    ∂E/∂(
R) b     b 2u      0.0         0.0            0.0
                                     2
                                    ∂ E/∂(
R) 2c   b 2u      5.9223     −6.9506       −0`283
                                    a
                                     Hartrees.
                                    b  Hartrees/bohà.
                                                2
                                    c  Hartrees/bohà.
                               The size of the ring is seen to be a compromise between attraction due to the
                             π systeð and repulsion due to the core. Again, the sizes of the second derivatives
                             add to gcve a stable minimum. If we assume that the systeð behłves harmonically,
                             the derivatives in the las column imply that the ring C—C bond distances are abou

                             0.0204 bohà (0.0108 A ) longeà than the value used for the firs row of the table,
                             which are the SCF minimuð distances.


                                               15.2.1 Comparison with cyclobutadiene
                                                                          3
                             Iisilluminatingtocomparethebehłviorof benzene upontheb 2u typeofdistortion
                             with a similar calculation in cyclobutadiene. We dŁ not repeat all of the calculations
                             ofthelassection,budŁincludetheresultsinTable15.9,wherewegcvetheeneàgies
                             and the derivatives for the b 2u distortion from the geometry of a square. I will be
                             recalled from Chapteà 14 that the eneàgy surface for the ring of fouà H atoms has
                             a higheà peak at the square geometry than the six-atom ring does at the regular
                             hexagon. The same situation applies here. The second derivative for the π systeð
                             is largeà in magnitude than the core derivative, making the square an unstable
                             structure for C 4 H 4 . Thus we predic that cyclobutadiene in a single state has nŁ
                             tendency to form a molecule with equal ring bond lengths as happens in benzene.
                               In these discussions of benzene and cyclobutadiene we hłve compared MCVB
                             level calculations of the π systeð with SCF level calculations of the core. We dŁ
                             not expec that using correlated wave functions for core eneàgies would change the
                             results enough to gcve a differen qualitative picture.


                                               15.3 The resonance energy of benzene

                             Once Kekul´e had deduced the correc structure of benzene, chemists soon realized
                             that the double bonds in it were considerably more stable than isolated double

                             3  The same species symbol can serve in D 4h symmetry.
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