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首页> 外文期刊>Photochemical & photobiological sciences: the official journal of the European Photochemistry Association and the European Society for Photobiology >Kinetics of benzophenone ketyl free radicals recombination in a polymer: reactivity in the polymer cage vs. reactivity in the polymer bulk
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Kinetics of benzophenone ketyl free radicals recombination in a polymer: reactivity in the polymer cage vs. reactivity in the polymer bulk

机译:聚合物中二苯甲酮酮基自由基重组的动力学:聚合物笼中的反应性与聚合物本体中的反应性

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The decay kinetics of intermediates produced under photolysis of benzophenone (B) dissolved in soft rubber poly(ethylene-co-butylene) films (abbreviated as E) was studied by ns laser flash photolysis in the temperature range of 263-313 K. We monitored decay kinetics of the triplet state of B-3* and of benzophenone ketyl free radical BH-. The fast exponential decay of 3B* (life-time tau(T) approximate to 200 ns) is accompanied by hydrogen atom abstraction from E with a formation of BH-and a polymer free radical R-. Decay of B-3* was followed by decay of BH-in the polymer cage (geminate recombination) with tau(c) approximate to 1 mu s. Cage recombination in turn was followed by a decay of BH-in the polymer bulk (tau(b) approximate to 100 mu s). Fortunately, all three processes are separated in time. Both cage and bulk reactions were decelerated by the application of magnetic field (MF) of 0.2 T by approximately 20%. Geminate recombination was fit to the first-order kinetic law, and recombination in the solvent bulk fits well to the second-order law. Both geminate recombination and recombination in the solvent bulk are predominantly a reaction between BH-and R-. It was assumed that the reaction radius rho(12) and a mutual diffusion coefficient D-12 of BH-and R-are the same for the cage and bulk recombination, respectively. This led to an estimation of rho(12) = 3.3 nm and D12 = 1 x 10(-7) cm(2) s(-1). These values are discussed. We obtained activation energy, E-act, equal to 6 kcal mol(-1) and 7 kcal mol(-1) for cage decay and for recombination in the polymer bulk, respectively. These Eact coincide with each other within experimental error of their determination (+/- 0.5 kcal mol(-1)). This indicates the same diffusion character in the cage and in the polymer bulk. It was demonstrated that an exponential model of cage effect sufficiently describes the obtained experimental data in rubber.
机译:通过ns激光闪光光解法在263-313 K的温度范围内研究了溶解在软橡胶聚(乙烯-共-丁烯)薄膜(缩写为E)中的二苯甲酮(B)的光解过程中产生的中间体的衰减动力学。 B-3 *和二苯甲酮酮基自由基BH-的三重态的衰变动力学。 3B *的快速指数衰减(寿命tau(T)约200 ns)伴随着E的氢原子抽象,形成BH-和聚合物自由基R-。在B-3 *衰变之后,BH-在聚合物笼中发生衰变(双链重组),tau(c)大约为1 s。笼重组之后,BH-在聚合物本体中衰减(tau(b)大约为100μs)。幸运的是,这三个过程在时间上是分开的。笼式反应和本体反应都通过施加0.2 T的磁场(MF)降低了约20%。萌芽重组符合一级动力学定律,溶剂体积中的重组符合二级定律。萌芽重组和溶剂本体中的重组主要是BH-和R-之间的反应。假设笼型和本体复合的反应半径rho(12)和BH-和R-的相互扩散系数D-12相同。这导致对rho(12)= 3.3 nm和D12 = 1 x 10(-7)cm(2)s(-1)的估计。讨论了这些值。我们获得的活化能E-act分别等于6 kcal mol(-1)和7 kcal mol(-1),用于笼衰变和聚合物本体中的重组。这些Eact在其确定的实验误差内(+/- 0.5 kcal mol(-1))彼此重合。这表明在笼子和聚合物本体中具有相同的扩散特性。结果表明,笼效应的指数模型足以描述所获得的橡胶实验数据。

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