Seefelder Maximilian, Heubes Markus, Quast Helmut, Edwards W Daniel, Armantrout John R, Williams Richard Vaughan, Cramer Christopher J, Goren Alan C, Hrovat David A, Borden Weston Thatcher
Institut für Organische Chemie der Universität Würzburg, Am Hubland, D-97074 Würzburg, Germany.
J Org Chem. 2005 Apr 29;70(9):3437-49. doi: 10.1021/jo0502089.
[reaction: see text] UV/vis spectra of thermochromic semibullvalenes 1 and barbaralanes 2, which undergo rapid degenerate Cope rearrangements, display temperature-dependent shoulders (1b, 1d, 1e) or absorption maxima (1c, 2c, 2f) at the low-energy side of their strong UV bands. These long-wavelength absorptions are ascribed to Franck-Condon transitions from delocalized structures 1(deloc) and 2(deloc). Gibbs free energy differences, DeltaG*, between delocalized and localized forms were calculated from the temperature dependence of the long-wavelength absorptions. Dipolar and polarizable solvents strongly affect and even may reverse the relative stabilities of the localized and delocalized forms of 1c, 2c, and 2f. For example, DeltaG*(2c) = 8 kJ mol(-)(1) in cyclohexane, 2 kJ mol(-)(1) in dimethylformamide, and -3 kJ mol(-)(1) in N,N'-dimethylpropylene urea (DMPU), so that (2c(deloc))(DMPU) becomes the global minimum. In contrast to the case for 2c, the intensities of the long-wavelength shoulders of the yellow semibullvalenes 1b, 1d, and 1e are only moderately influenced by solvents, and the rates of Cope rearrangements of the nonthermochromic, colorless barbaralanes 2a and 2b, determined by NMR methods, are almost solvent-invariant. In search of the solute properties that are decisive in determining the influence of solvent upon DeltaG*, electrical dipole and quadrupole moments and molecular polarizabilities have been calculated using the B3LYP/6-31G* method and solvation energies have been computed with the conductorlike polarized continuum model (CPCM). The results of these calculations indicate that the solvent effects are due to the greater polarity and polarizability of the delocalized structures relative to the localized structures.
[反应:见正文] 热致变色半环戊二烯1和巴拉巴拉烯2会发生快速简并的科普重排,其紫外/可见光谱在强紫外吸收带的低能量侧呈现出与温度相关的肩峰(1b、1d、1e)或吸收最大值(1c、2c、2f)。这些长波长吸收归因于从离域结构1(deloc)和2(deloc)的弗兰克 - 康登跃迁。离域形式和局域形式之间的吉布斯自由能差ΔG*,是根据长波长吸收的温度依赖性计算得出的。偶极和可极化溶剂会强烈影响甚至可能反转1c、2c和2f的局域形式和离域形式的相对稳定性。例如,在环己烷中ΔG*(2c) = 8 kJ mol⁻¹,在二甲基甲酰胺中为2 kJ mol⁻¹,在N,N'-二甲基丙烯脲(DMPU)中为 - 3 kJ mol⁻¹,因此(2c(deloc))(DMPU)成为全局最小值。与2c的情况相反,黄色半环戊二烯1b、1d和1e的长波长肩峰强度仅受到溶剂的适度影响,并且通过核磁共振方法测定的非热致变色无色巴拉巴拉烯2a和2b的科普重排速率几乎与溶剂无关。为了寻找在决定溶剂对ΔG的影响方面起决定性作用的溶质性质,使用B3LYP / 6 - 31G方法计算了电偶极矩、电四极矩和分子极化率,并使用导体类极化连续介质模型(CPCM)计算了溶剂化能。这些计算结果表明,溶剂效应是由于离域结构相对于局域结构具有更大的极性和极化率。