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首页> 外文期刊>Macromolecules >Low-Temperature Heat Capacity, Glass-Transition Cooperaivity, and Glass-Structure Vault Breakdown in a Series of Poly(n-alkyl methacrylate)s
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Low-Temperature Heat Capacity, Glass-Transition Cooperaivity, and Glass-Structure Vault Breakdown in a Series of Poly(n-alkyl methacrylate)s

机译:一系列聚(甲基丙烯酸正烷基酯)的低温热容,玻璃化转变合作性和玻璃结构穹顶破坏

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摘要

Heat capacity in the 1 K range and close to T_g was studied in a series of poly(n-alkyl methacrylate)s, PnAMA, including some random copolymers. We report on two findings: (i) The glass transition temperature T_g and the cooperativity of he #alpha# process that freezes-in at T_g, N_#alpha#(T_g), decrease smoothly between methyl (PMMA) and hexyl member (PnHMA); the cooperativity from N_#alpha#(T_g) = 35 to N_#alpha#(T_g) (approx =) 1. (ii) The tunnel density measured in the 1 K range as c_1 constant of the heat capacity function increase between PMMA and the ethyl member (PEMA), shows, after a maximum near PEMA, a sharp drop (factor of 6) to the butyl member (PnBMA), and remains constant at a low level up to the octyl member (PnOMA). The cooperativity of the #alpha# process near T_g and the tunnel density will be correlated assuming that freezing-in (vitrification) fixes the dynamic heterogeneity in the self-organized equilibrium liquid near T_g. We try to explain how freezing of cynamic heterogeneities in the PnAMA series is responsible for the trend in the tunnel density including the sharp drop: Freezing-in of cooperativity shells around Glarum defects forms some vaults that enlarge the free volume near these defects in comparison to a situation without vaults. The maximum in c_1 is promoted by this additional free volume; the drop in c_1 is caused by a vault breakdown effect if the cooperativity shell is too small for vault fomation, N_#alpha#(T_g) < 15.
机译:在一系列聚甲基丙烯酸正丁酯(PnAMA)中,包括一些无规共聚物,研究了在1 K范围内且接近T_g的热容量。我们报告了两个发现:(i)玻璃化转变温度T_g和冻结在T_g N_#alpha#(T_g)的he#alpha#过程的协同作用,在甲基(PMMA)和己基成员(PnHMA)之间平稳地降低);从N_#alpha#(T_g)= 35到N_#alpha#(T_g)(大约=)1的协作性。(ii)在1 K范围内测得的隧道密度作为热容量函数的c_1常数在PMMA和PMMA之间增加。乙基成员(PEMA)在接近最大PEMA后显示出对丁基成员(PnBMA)的急剧下降(6的因数),并一直保持低水平直至辛基成员(PnOMA)。假设冻结(玻璃化)固定了T_g附近的自组织平衡液体中的动态异质性,则T_g附近的#alpha#过程的合作性与隧道密度将相互关联。我们试图解释PnAMA系列中的动态异质性冻结是如何导致隧道密度趋势(包括急剧下降)的:与Glarum缺陷周围的协同壳的冻结形成了一些拱顶,与之相比,这些拱顶扩大了这些缺陷附近的自由体积。没有保险库的情况。 c_1中的最大值由此额外的空闲卷提升;如果协作性外壳对于Vault构架而言太小,N_#alpha#(T_g)<15,则c_1下降是由Vault击穿效应引起的。

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