Stickrath Andrew B, Carroll Elizabeth C, Dai Xiaochuan, Harris D Ahmasi, Rury Aaron, Smith Broc, Tang Kuo-Chun, Wert Jonathan, Sension Roseanne J
Department of Chemistry, University of Michigan, 930 North University Avenue, Ann Arbor, Michigan 48109-1055, USA.
J Phys Chem A. 2009 Jul 30;113(30):8513-22. doi: 10.1021/jp9017986.
Time-resolved transient absorption spectroscopy was used to investigate the primary geminate recombination and cage escape of alkyl radicals in solution over a temperature range from 0 to 80 degrees C. Radical pairs were produced by photoexcitation of methyl, ethyl, propyl, hexylnitrile, and adenosylcobalamin in water, ethylene glycol, mixtures of water and ethylene glycol, and sucrose solutions. In contrast to previous studies of cage escape and geminate recombination, these experiments demonstrate that cage escape for these radical pairs occurs on time scales ranging from a hundred picoseconds to over a nanosecond as a function of solvent fluidity and radical size. Ultrafast cage escape (<100 ps) is only observed for the methyl radical where the radical pair is produced through excitation to a directly dissociative electronic state. The data are interpreted using a unimolecular model with competition between geminate recombination and cage escape. The escape rate constant, k(e), is not a simple function of the solvent fluidity (T/eta) but depends on the nature of the solvent as well. The slope of k(e) as a function of T/eta for the adenosyl radical in water is in near quantitative agreement with the slope calculated using a hydrodynamic model and the Stokes-Einstein equation for the diffusion coefficients. The solvent dependence is reproduced when diffusion constants are calculated taking into account the relative volume and mass of both solvent and solute using the expression proposed by Akgerman (Akgerman, A.; Gainer, J. L. Ind. Eng. Chem. Fundam. 1972, 11, 373-379). Rate constants for cage escape of the other radicals investigated are consistently smaller than the calculated values suggesting a systematic correction for radical size or coupled radical pair motion.
采用时间分辨瞬态吸收光谱法,研究了在0至80摄氏度温度范围内溶液中烷基自由基的初级双分子复合和笼逃逸过程。通过在水、乙二醇、水与乙二醇的混合物以及蔗糖溶液中对甲基、乙基、丙基、己腈和腺苷钴胺素进行光激发来产生自由基对。与先前关于笼逃逸和双分子复合的研究不同,这些实验表明,这些自由基对的笼逃逸发生在从一百皮秒到超过一纳秒的时间尺度上,这是溶剂流动性和自由基大小的函数。仅在甲基自由基中观察到超快笼逃逸(<100皮秒),其中自由基对是通过激发到直接解离的电子态产生的。使用双分子复合和笼逃逸之间存在竞争的单分子模型来解释这些数据。逃逸速率常数k(e)不是溶剂流动性(T/η)的简单函数,还取决于溶剂的性质。水中腺苷自由基的k(e)随T/η变化的斜率与使用流体动力学模型和扩散系数的斯托克斯-爱因斯坦方程计算出的斜率几乎在定量上一致。当使用Akgerman提出的表达式(Akgerman, A.; Gainer, J. L. Ind. Eng. Chem. Fundam. 1972, 11, 373 - 379)考虑溶剂和溶质的相对体积和质量来计算扩散常数时,能够再现溶剂依赖性。所研究的其他自由基的笼逃逸速率常数始终小于计算值,这表明需要对自由基大小或耦合自由基对运动进行系统校正。