首页> 外文期刊>The journal of physical chemistry, B. Condensed matter, materials, surfaces, interfaces & biophysical >Atomistic Simulation of Orientation of Methyl Groups and Methylene Bisectors,and Surface Segregation,in Freely Standing Thin Films of Atactic Poly(ethylene-co-propylene)
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Atomistic Simulation of Orientation of Methyl Groups and Methylene Bisectors,and Surface Segregation,in Freely Standing Thin Films of Atactic Poly(ethylene-co-propylene)

机译:自由立构无规立构聚(乙烯-共-丙烯)薄膜中甲基和亚甲基双链取向和表面偏析的原子模拟

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Atomistically detailed models of free-standing thin films of random poly(ethylene-co-propylene) were produced using a method recently applied to atactic polystyrene (Clancy,et al.J.Phys.Chem.B 2001,705,11493).Monte Carlo simulations of the copolymer were carried out at ethylene fractions that cover the entire range of composition investigated in a recent experimental work (Opdahl,et al.J.Phys.Chem.B 2002,706,5212) based on sum-frequency generation (SFG) spectroscopy.We find that there is a minor enrichment of methyl groups on the surface,as compared to the bulk composition.Interestingly,the orientation distribution of methyl and methylene units is not unimodal.For methyl units,there is about 50% probability of orientation perpendicular to the surface.The other 50% are randomly oriented.For the methylene bisector,the simulation shows that the distribution has two broad peaks at opposite angles (at 180 deg apart) to the surface normal.More conclusive results may be obtained by using larger sample sizes and analysis of a larger number of snapshots,both of which increase the computation time significantly.The opposite angle pairs nearly cancel each other in the computation of an average order parameter and give us a misleading net result that the bisectors are randomly oriented.With increasing ethylene fraction,the orientation distribution of methyl and methylene units tends to become more uniform;however,this change is small.The strong average orientation of methyl groups and weak average orientation of methylene groups is in agreement with experiments.However,the simulation does not show the significant relative increase in the surface methyl groups contributing to the SFG signal as compared to the bulk concentration or an increase in average orientation of methylene units,with an increase in the ethylene fraction,as inferred from the experimental results.We find that the raw experimental data obtained with an increase in ethylene fraction can be explained by the changes in the number of methyl and methylene groups on the surface rather than the increase in surface excess of the methyl groups contributing to the SFG signal,trans cancellation,and increase in orientation of methylene bisectors as deduced from the experiments.
机译:使用最近应用于无规聚苯乙烯的方法(Clancy,et al.J.Phys.Chem.B 2001,705,11493)生产了无规聚乙烯(乙烯-丙烯共聚)薄膜的原子学详细模型。共聚物的Carlo模拟是在乙烯馏分下进行的,该馏分涵盖了总和频率的产生(Opdahl等人,J.Phys.Chem.B 2002,706,5212)。 SFG)光谱。我们发现与本体组成相比,表面上甲基的富集程度较小。有趣的是,甲基和亚甲基单元的取向分布不是单峰的。对于甲基单元,大约有50%的概率垂直于表面的方向垂直分布。其余50%是随机取向的。对于亚甲基平分线,模拟显示该分布在与表面法线相反的角度(相距180度)处有两个宽峰,可能会得出更多结论性结果。通过使用大更大的样本数量和大量快照的分析,这两者均显着增加了计算时间。相反的角度对在平均阶数参数的计算中几乎相互抵消,并给人以误解的净结果,即平分线是随机定向的随着乙烯分数的增加,甲基和亚甲基单元的取向分布趋于变得更均匀;但是,这种变化很小。甲基的强平均取向和亚甲基的弱平均取向与实验一致。模拟结果表明,与总浓度相比,对SFG信号有贡献的表面甲基没有显着的相对增加,也没有显示亚甲基单元的平均取向有所增加,而乙烯分数却有所增加,这是根据实验结果得出的。发现乙烯含量增加而获得的原始实验数据可以用由实验推导,表面上甲基和亚甲基数目的增加,而不是甲基表面上过量的增加导致了SFG信号,反式消除和亚甲基平分线的取向增加。

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