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Polymer diffusion in PBMA latex films using a polymerizable benzophenone derivative as an energy transfer acceptor

机译:使用可聚合的二苯甲酮衍生物作为能量转移受体的PBMA乳胶膜中的聚合物扩散

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Fluorescence resonance energy transfer (FRET) measurements were used to monitor polymer diffusion in poly(butyl methacrylate) latex films with a polymer molar mass of M-w approximate to 125 000 (M-w/M-n = 2.5). These experiments employed the nonfluorescent acceptor chromophore NBen, which allowed faster data acquisition at lower acceptor dye concentration (0.3, 0.5 mol %) than previous experiments with anthracene (I mol %) as the acceptor. The data were analyzed in two distinct ways. Our traditional simplified approach involved calculating f(m) values for the quantum efficiencies of FRET (Phi(ET)). Apparent diffusion coefficients D-app were calculated by making rather severe assumptions about f(m). In addition, we carried out mathematical simulations of diffusion which satisfied Fick's laws in a spherical geometry. The concentration profiles of donor and acceptor were introduced into equations that describe the rate for of energy transfer, and donor decay profiles were simulated I-D(s)(t). By comparing simulated and experimental decay profiles as a function of sample annealing time, optimum values of the mean diffusion coefficient (D) were obtained. A comparison of the two different methods of data analysis indicates that Dapp values are larger than (D) values by a factor of 2-4 but track the "true" diffusion coefficients rather well. From the temperature dependence of the diffusion coefficients, we found effective activation energies for diffusion of E-a = 33.5 2.5 kcal/mol from D-app and 38 +/- 5 kcal/mol from . These values are very similar to the value of E-a = 39 kcal/mol from D-app obtained in earlier experiments in which anthracene served as the acceptor chromophore. [References: 32]
机译:荧光共振能量转移(FRET)测量用于监测聚合物摩尔质量为M-w约125 000(M-w / M-n = 2.5)的聚甲基丙烯酸丁酯胶乳薄膜中的聚合物扩散。这些实验使用了非荧光受体生色团NBen,与以前以蒽(I mol%)为受体的实验相比,它可以在较低的受体染料浓度(0.3,0.5 mol%)下更快地获取数据。数据以两种不同的方式进行了分析。我们的传统简化方法涉及计算FRET(Phi(ET))的量子效率的f(m)值。通过对f(m)进行相当严格的假设来计算表观扩散系数D-app。另外,我们进行了球形扩散的数学模拟,该扩散模拟满足菲克定律。将供体和受体的浓度曲线引入描述能量转移速率的方程式中,并用I-D(s)(t)模拟供体衰减曲线。通过比较模拟和实验衰减曲线作为样品退火时间的函数,可以得出平均扩散系数(D)的最佳值。两种不同数据分析方法的比较表明,Dapp值比(D)值大2-4倍,但很好地跟踪了“真实”扩散系数。从扩散系数的温度依赖性,我们发现有效的活化能从D-app扩散到E-a = 33.5 2.5 kcal / mol,从扩散到38 +/- 5 kcal / mol。这些值与早期的实验中由D-app得到的E-a = 39 kcal / mol的值非常相似,在早期的实验中,蒽用作受体生色团。 [参考:32]

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