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Correspondence relation with respect to entanglement among different simulation models: comparison between bead-spring and bond fluctuation model

机译:不同仿真模型之间关于缠结的对应关系:珠-弹簧和键涨落模型之间的比较

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摘要

A novel index for comparing different simulation model polymers with respect to entanglement is proposed. It is the number of elements N_e~* of ring polymers whose average number of entanglement per molecule is unity; N_e~* can be calculated with a small-scale computer simulation. We also proposed a method to equilibrate the entangled ring polymers. As an example we calculated N_e~* with a molecular dynamics simulation using a bead-spring (BS) model which is equivalent to the model proposed by Kremer and Grest [J Chem Phys 92 (1990) 5057], and with a Monte Carlo simulation using bond fluctuation (BF) model. We obtained N_e~* = 82 ± 1 for BS model with volume fraction φ = 0.43 and N_e~* = 59 ± 1 for BF model with φ = 0.5. By comparing with the recent result of our group, N_e = 89 for BF model with φ = 0.5, we can assume that N_e approx= 1.5 N_e~*. If this assumption holds for BS model, its N_e is estimated to be 120, which is 3.4 times greater than the estimated value by Kremer and Grest. The origin of this difference is discussed.
机译:提出了一种新的指标,用于比较不同模拟模型聚合物的缠结。它是指每分子平均缠结数为1的环聚合物的元素数N_e〜*。 N_e〜*可以通过小型计算机仿真来计算。我们还提出了一种平衡纠缠环聚合物的方法。例如,我们使用分子动力学模拟,使用与Kremer和Grest [J Chem Phys 92(1990)5057]提出的模型相同的珠子弹簧(BS)模型进行分子动力学模拟,并使用Monte Carlo模拟计算了N_e〜*。使用债券波动(BF)模型。对于体积分数φ= 0.43的BS模型,我们获得N_e〜* = 82±1,对于φ= 0.5的BF模型,我们获得N_e〜* = 59±1。通过与小组最近的结果比较,对于φ= 0.5的BF模型,N_e = 89,我们可以假设N_e大约= 1.5 N_e〜*。如果该假设适用于BS模型,则其N_e估计为120,这是Kremer和Grest估计值的3.4倍。讨论了这种差异的由来。

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