首页> 外文期刊>The Journal of Chemical Physics >Deconvolution of the relaxations associated with local and segmental motions in poly(methacrylate)s containing dichlorinated benzyl moieties in the ester residue
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Deconvolution of the relaxations associated with local and segmental motions in poly(methacrylate)s containing dichlorinated benzyl moieties in the ester residue

机译:与在酯残基中包含二氯苄基部分的聚(甲基丙烯酸酯)中的局部和链段运动相关的弛豫的反卷积

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摘要

The relaxation behavior of poly(2,3-dichlorobenzyl methacrylate) is studied by broadband dielectric spectroscopy in the frequency range of 10(-1)-10(9) Hz and temperature interval of 303-423 K. The isotherms representing the dielectric loss of the glassy polymer in the frequency domain present a single absorption, called beta process. At temperatures close to T-g, the dynamical alpha relaxation already overlaps with the beta process, the degree of overlapping increasing with temperature. The deconvolution of the alpha and beta relaxations is facilitated using the retardation spectra calculated from the isotherms utilizing linear programming regularization parameter techniques. The temperature dependence of the beta relaxation presents a crossover associated with a change in activation energy of the local processes. The distance between the alpha and beta peaks, expressed as log(f(max;beta)/f(max;alpha)) where f(max) is the frequency at the peak maximum, follows Arrhenius behavior in the temperature range of 310-384 K. Above 384 K, the distance between the peaks remains nearly constant and, as a result, the alpha onset temperature exhibited for many polymers is not reached in this system. The fraction of relaxation carried out through the alpha process, without beta assistance, is larger than 60% in the temperature range of 310-384 K where the so-called Williams ansatz holds. (c) 2005 American Institute of Physics.
机译:通过宽带介电谱研究了聚(2,3-二氯苄基甲基丙烯酸酯)在10(-1)-10(9)Hz的频率范围和303-423 K的温度区间内的弛豫行为。等温线代表介电损耗在频域中,玻璃态聚合物的一部分呈现单一吸收,称为β过程。在接近T-g的温度下,动态α弛豫已经与β过程重叠,重叠程度随温度增加。使用从等温线使用线性规划正则化参数技术计算的延迟光谱,可以方便地进行α和β弛豫的反卷积。 β弛豫的温度依赖性呈现出与局部过程的活化能变化相关的交叉。 alpha和beta峰之间的距离表示为log(f(max(beta)/ f(max; alpha)),其中f(max)是最大峰处的频率,在310°C的温度范围内遵循Arrhenius行为384K。在384 K以上,峰之间的距离几乎保持恒定,结果,在该系统中,没有达到许多聚合物表现出的α起始温度。在没有所谓的beta辅助的情况下,通过alpha过程进行的弛豫分数在所谓的Williams ansatz所处的310-384 K的温度范围内大于60%。 (c)2005年美国物理研究所。

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