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SOLUTIONSMANUAL TO ACCOMPANY ATKINS' PHYSICAL CHEMISTRY 311 (b) �e delocalisation energy is given by Edeloc = Eπ − Nπ(α + β), where Nπ is the number of π electrons. In the ground state of benzene, two electrons occupy the orbital with energy E0 and four electrons occupy the degenerate pair of orbitals with energy E±1. Hence the π-electron binding energy of benzene is Eπ = 2E0 + 4E±1 = 2(α + 2β) + 4(α + β) = 6α + 8β. �erefore the delocalization energy is Edeloc = 6α + 8β − 6(α + β) = 2β . To calculate the delocalization energy of hexatriene, the energies of the occupied molecular orbitals are required. �e six electrons in the π sys- tem of hexatriene occupy the three lowest energy orbitals, therefore the π-electron binding energy is Eπ = 2E1 + 2E2 + 2E3 = 2[α + 2β cos(π/7)] + 2[α + 2β cos(2π/7)] + 2[α + 2β cos(3π/7)] = 6α + (6.98...)β Hence the delocalization energy of hexatriene is Edeloc = 6α+(6.98...)β− 6(α + β) = 0.99β . �e lowering in energy as a result of delocalization in benzene in greater than in hexatriene, consistent with the ‘aromatic’ system in benzene. (c) �e π-electron binding energy in cyclooctatetraene is Eπ = 2E0 + 4E±1 + 2E±2 = 2(α + 2β) + 4(α + 1.41β) + 2α = 8α + 9.64β �e delocalization energy is therefore Edeloc = 8α + 9.64β − 8(α + β) = 1.64β . �e π-electron binding energy in octatetraene is Eπ = 2E1 + 2E2 + 2E3 + 2E4 = 2[α + 2β cos(π/9)] + 2[α + 2β cos(2π/9)] + 2[α + 2β cos(3π/9)] + 2[α + 2β cos(4π/9)] = 8α + (9.51...)β �erefore the delocalization energy is Edeloc = 8α+(9.51...)β−8(α+β) = 1.52β . �e di�erence in delocalization energies between cyclooctate- traene and octatetraene is much smaller than the di�erence in the values for benzene and hexatriene. �is is taken as an result of benzene being ‘aromatic’ in contrast to cyclooctatetraene which is sometimes described as ‘antiaromatic’. P9E.4 Within the Hückel approximations, the secular determinant of ethene is ∣α − E β β α − E ∣ �e hamiltonian matrix is of the same form, but with diagonal elements α H = ( α β β α ) = α1 + β ( 0 1 1 0 )