Eur. Phys. J. E (2015) 38: 11
https://doi.org/10.1140/epje/i2015-15011-x

Regular Article

Simulated glass-forming polymer melts: Dynamic scattering functions, chain length effects, and mode-coupling theory analysis

¹ Institut Charles Sadron, Université de Strasbourg, CNRS UPR 22, 23 rue du Loess, BP 84047, 67034, Strasbourg Cedex 2, France
² Universität Konstanz, Fachbereich Physik, Universitätsstraße 10, 78457, Konstanz, Germany

^* e-mail: jorg.baschnagel@ics-cnrs.unistra.fr

Received: 18 September 2014
Revised: 9 January 2015
Accepted: 28 January 2015
Published online: 26 February 2015

Abstract

We present molecular-dynamics simulations for a fully flexible model of polymer melts with different chain length N ranging from short oligomers (N = 4) to values near the entanglement length (N = 64). For these systems we explore the structural relaxation of the supercooled melt near the critical temperature T _c of mode-coupling theory (MCT). Coherent and incoherent scattering functions are analyzed in terms of the idealized MCT. For temperatures T > T _c we provide evidence for the space-time factorization property of the β relaxation and for the time-temperature superposition principle (TTSP) of the α relaxation, and we also discuss deviations from these predictions for T ≈ T _c. For T larger than the smallest temperature where the TTSP holds we perform a quantitative analysis of the dynamics with the asymptotic MCT predictions for the late β regime. Within MCT a key quantity, in addition to T _c, is the exponent parameter λ. For the fully flexible polymer models studied we find that λ is independent of N and has a value (λ = 0.735 ) typical of simple glass-forming liquids. On the other hand, the critical temperature increases with chain length toward an asymptotic value T _c ^∞ . This increase can be described by T _c ^∞ − T _c(N) ∼ 1/N and may be interpreted in terms of the N dependence of the monomer density ρ, if we assume that the MCT glass transition is ruled by a soft-sphere-like constant coupling parameter Γ _c = ρ _c T _c ^−1/4, where ρ _c is the monomer density at T _c. In addition, we also estimate T _c from a Hansen-Verlet-like criterion and MCT calculations based on structural input from the simulation. For our polymer model both the Hansen-Verlet criterion and the MCT calculations suggest T _c to decrease with increasing chain length, in contrast to the direct analysis of the simulation data.