Abstract

We present large-scale molecular dynamics simulations for a coarse-grained model of polymer melts in equilibrium. From detailed Rouse mode analysis we show that the time-dependent relaxation of the autocorrelation function (ACF) of modes p can be well described by the effective stretched exponential function due to the crossover from Rouse to reptation regime. The ACF is independent of chain sizes N for N/p < Ne (Ne is the entanglement length), and there exists a minimum of the stretching exponent as N/p → Ne. As N/p increases, we verify the crossover scaling behavior of the effective relaxation time τeff,p from the Rouse regime to the reptation regime. We have also provided evidence that the incoherent dynamic scattering function follows the same crossover scaling behavior of the mean square displacement of monomers at the corresponding characteristic time scales. The decay of the coherent dynamic scattering function is slowed down and a plateau develops as chain sizes increase at the intermediate time and wave length scales. The tube diameter extracted from the coherent dynamic scattering function is equivalent to the previous estimate from the mean square displacement of monomers.

Highlights

  • The dynamics of polymer chains in a melt is a complicated many-body problem where the motion of chains depends on different length scales and time scales

  • We have studied the dynamics of fully equilibrated polymer melts, characterized by the mean square displacement of monomers, and determined the characteristic time scales: the characteristic time τ0, the entanglement time τe ≈ τ0Ne2, the Rouse time τR ≈ τ0N 2, and the disentanglement time τd ≈ τ0N 2(N/Ne)1.4, according to the predictions given by the Rouse model and the reptation theory, where Ne is the entanglement length and N is the chain size

  • Based on this work, we are interested in understanding to what extent the dynamics of single chains can be analyzed through the Rouse mode analysis and check the scaling predictions of the relaxation of the Rouse modes in the literature [1,2,3,4,5,6,7,8,9, 14,15,16] whenever it is possible

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Summary

Introduction

The dynamics of polymer chains in a melt is a complicated many-body problem where the motion of chains depends on different length scales and time scales. We have studied the dynamics of fully equilibrated polymer melts, characterized by the mean square displacement of monomers, and determined the characteristic time scales: the characteristic time τ0, the entanglement time τe ≈ τ0Ne2, the Rouse time τR ≈ τ0N 2, and the disentanglement time τd ≈ τ0N 2(N/Ne)1.4, according to the predictions given by the Rouse model and the reptation theory, where Ne is the entanglement length and N is the chain size. Based on this work, we are interested in understanding to what extent the dynamics of single chains can be analyzed through the Rouse mode analysis and check the scaling predictions of the relaxation of the Rouse modes in the literature [1,2,3,4,5,6,7,8,9, 14,15,16] whenever it is possible.

Rouse mode analysis
Dynamic structure factors
Conclusion
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