433345 Atomistic Simulation of Dynamics of Individual Molecules in Entangled Polymers Undergoing Homogenous Shear and Planer Elongational Flows

Thursday, November 12, 2015: 3:45 PM
251B (Salt Palace Convention Center)
Mohammad Hadi Nafar Sefiddashti, Brian J. Edwards and Bamin Khomami, Chemical and Biomolecular Engineering, University of Tennessee, Knoxville, TN

Nonequilibrium molecular dynamics (NEMD) simulations of an entangled C700H1402 linear polyethylene system were performed to investigate the chain dynamics over a wide range of Weissenberg numbers (Wi) under steady shearing flow. Similar to the unentangled (C78H158) and moderately entangled (C400H802) melts examined in prior simulation studies, the distribution of the chain end-to-end distance, |Rete|, at high Wi was bimodal with a peak at low |Rete| which is associated with the dynamical rotation/retraction cycles experienced by individual chains, and a peak at high |Rete| which corresponds to the highly stretched and oriented macromolecules. To understand the underlying physics, the relevant system time scales including the entanglement time, Rouse time, and disengagement time were determined using segmental mean square displacement analysis of the chain molecules. The longest (τd) and rotational (τrot) relaxation times of the system at high Wi were extracted by fitting a functional form of A*exp(-t/τd)cos(2πt/τrot) to the end-to-end vector autocorrelation data. The number of entanglements and other topological features of the liquid were also computed as functions of Wi.

NEMD simulations of linear polyethylene melts with different chain lengths (C400H802, C700H1402, and C1000H2002) were also performed in planer extensional flow and rheological and topological behavior of entangled systems were studied in the nonlinear regime. Specifically, we studied the behavior of extensional viscosity as a function of strain rate, , to examine the thinning exponents and determine if there is any signs of an upturn in the viscosity for extensional rates on the order of the inverse Rouse time, as predicted by standard theories. The effects of the chain stretch, entanglement density, and chain disentangling on the system behavior will also be discussed.

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