聚乙烯中的均匀成核:分子量依赖性。

Gaylon S Ross, Lois J Frolen
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引用次数: 26

摘要

液滴技术用于获得线性聚乙烯的8个表征级分(重均分子量为3100至249000)的高度过冷熔体中均匀晶体成核的等温速率的估计值。根据目前链折叠晶体均匀成核的理论,对这些实验获得的数据进行了分析。量σ2σe的值,其中σ和σe是晶体的横向和端面自由能,被估计为分子量的函数。发现样品3.2K的成核行为异常。当我们假设该样品以延伸链形式结晶并计算σ3而不是σ2σe时,发现σ的值为10.57 ergs/cm2,这与其他研究人员发现的线性烃的值9.6 ergs/cm2合理一致。然而,样品3.2K是否经历过均匀成核仍然存在问题。对于9.70、11.74和23.0 K的样品,发现σ2σe随着分子量的增加而迅速增加,这是由于每链倍纤毛数量的减少。对于较高的分子量,σ2σe的值趋于平稳,并且发现样品23.0至249 K的σ2σe的平均值为19000 ergs3/cm6。绝对成核频率I0的实验值与理论值相差约1×1012。如果假设表面自由能与温度有关[即σ=σ1(1+xΔT)和σe=σe1(1+yΔT),其中x=-0.0073和y=0.014],则由于温度校正符号中的补偿效应,σ2σe>的平均值仅略有变化(达到19800 ergs3/cm6),I0接近理论值,1×1034个核/cm3/s。
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Homogeneous Nucleation in Polyethylene: Molecular Weight Dependence.

The droplet technique was used to obtain estimates of the isothermal rate of homogeneous crystal nucleation in highly supercooled melts of 8 characterized fractions of linear polyethylene (weight average molecular weights from 3,100 to 249,000). The data obtained from these experiments were analyzed in accord with current theories of homogeneous nucleation of chain folded crystals. Values for the quantity σ2σ e , where σ and σ e are the lateral and end-surface free energies of the crystal, were estimated as a function of molecular weight. Sample 3.2 K was found to be anomalous in its nucleation behavior. When we assume that this sample crystallizes in the extended chain form and calculate σ3 instead of σ 2 σ e the value for σ is found to be 10.57 ergs/cm2 which is in reasonable agreement with the value 9.6 ergs/cm2 found by other investigators for linear hydrocarbons. However, there remains the question as to whether sample 3.2 K ever underwent homogeneous nucleation. For samples 9.70, 11.74, and 23.0 K, σ2σ e was found to increase rapidly due to a decrease in the number of cilia per chain fold as the molecular weight increases. For higher molecular weights the value for σ2σ e levels off and the average value of σ2σ e for samples 23.0 to 249 K was found to be 19,000 ergs3/cm6. The experimental value of the absolute nucleation frequency I 0, was found to differ from the theoretical value by approximately 1 × 1012. If one assumes that the surface free energies are temperature dependent [i.e., σ = σ 1 ( 1 + x ¯ Δ T ) and σ e = σ e 1 ( 1 + y ¯ Δ T ) where x ¯ = - 0.0073 and y ¯ = 0.014 ] the average value of σ2σ e > changes only slightly (to 19,800 ergs3/cm6) due to the compensating effects in the signs of the temperature corrections and I 0 is close to the theoretical value, 1 × 1034 nuclei/cm3/s.

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