Detailed Molecular-Dynamics Study On Structural and Dynamical Properties of Unentangled Ring Polyethylene Melts: Comprehensive Analysis of the Rouse Theory and Simulation

Wednesday, November 10, 2010: 5:05 PM
252 A/B Room (Salt Palace Convention Center)
Georgia Tsolou1, Nikos Stratikis2, Chunggi Baig3, Pavlos Stephanou3 and Vlasis Mavrantzas4, (1)Institute of Chemical Engineering and High temperature Chemical Processes (ICE-HT/FORTH), Senior Researcher, Patras, Greece, (2)Chemical Engineering, University of Patras, Greece, (3)Chemical Engineering, The University of Patras, Patras, Greece, (4)Chemical Engineering, University of Patras, Patras, Greece

Motivated by recently reported experimental data [1] on the peculiar rheological behaviour of polymer rings, we have undertaken a systematic and detailed investigation of the structural and mainly the dynamical and rheological properties of model ring polyethylene (PE) melts, ranging in molecular length from N =24 up to N=400 carbon atoms per molecule [C24, C400] with the help of atomistic Molecular Dynamics (MD) simulations at temperature T=450 K [2]. We present results concerning the size of the ring molecules and their spatial packing which show that ring systems are characterized by a more compact and denser structure than their linear analogues; this is consistent with previous theoretical [3] and experimental studies [4]. Additionally, we investigate the dynamical and rheological characteristics of these systems obtained either directly from the atomistic MD trajectories (e.g., the chain self-diffusion coefficient D, the terminal relaxation time τd, and the dynamic structure factor S(q,t)) or indirectly (e.g., the friction coefficient ζ, the spectrum of relaxation times τp, and the zero-shear rate viscosity η0) by mapping the MD results onto the predictions of the Rouse theory for cyclic systems [2]. In agreement with previous experimental studies [5], our simulations support that ring systems exhibit a faster dynamics and a lower viscosity than linear PE melts of the same molecular weight. Furthermore, the dependence of D, τp, ζ and η0 on molecular weight reveals that all ring PE systems examined here follow a Rouse-like dynamical behavior even for chain lengths as long as N=400 which is above the crossover regime from Rouse to reptation for linear PE melts [6].

[1] M. Kapnistos, M. Lang, D. Vlassopoulos, W. Pyckhout-Hintzen, D. Richter, D. Cho, T. Chang, M. Rubinstein, Nature Materials 7, 997 (2008). [2] G. Tsolou, N. Stratikis, C. Baig, P. S. Stephanou, V. G. Mavrantzas, in preparation. [3] B. H. Zimm and W. H. Stockmayer, J. Chem. Phys. 17, 1301 (1949). [4] V. S. Arrighi, S. Gagliardi, A. C. Dagger, J. A. Semlyen, J. S. Higgins, M. J. Shenton, Macromolecules 37, 8057 (2004). [5] J. Roovers, Macromolecules 21, 1517 (1988). [6] P. S. Stephanou, C. Baig, G. Tsolou, V. G. Mavrantzas, M. Kröger, J. Chem. Phys. 132, 124904 (2010).


Extended Abstract: File Not Uploaded
See more of this Session: Modeling and Simulation of Polymers
See more of this Group/Topical: Materials Engineering and Sciences Division