Abstract

Relaxation dynamics of entangled polymer liquids are investigated in nonlinear step shear flow using mechanical rheometry experiments and theory. Entangled solutions of high molar mass polystyrenes (PS), 3 × 105 ≤ φM̄w ≤ 1.6 × 106 g/mol, in diethyl phthalate (DEP) are the main focus of this study. Cone-and-plate rheometer fixtures roughened by attachment of a single layer of 10−30 μm silica glass beads are used to eliminate interfacial slip during step shear measurements. A simple theory for stress relaxation dynamics that accounts for coupled relaxation of molecular orientation, chain stretching, and entanglement density is used to analyze the experimental results. In PS/DEP solutions with φM̄w ≥ 5 × 105 and in which PS forms an average of eight or more entanglements per chain, we find that the nonlinear relaxation modulus can be factorized into separate strain-dependent and time-dependent functions only after a time λk2 ≈ τd0 ∼ (φM̄w)3 substantially larger than the longest Rouse relaxation time τRouse of the solution. This finding is consistent with results from a previous study of step shear dynamics in solutions of ultrahigh molecular weight polystyrene, M̄w = 2.06 × 107 [Sanchez-Reyes, J.; Archer, L. A. Macromolecules 2002, 35, 5194], but contradicts expectations from current theories for entangled polymer dynamics, which predict λk2 ≈ (3 − 5)τRouse. The origin of this discrepancy is traced to a greater than expected influence of entanglement loss and recovery processes on polymer relaxation dynamics in nonlinear step shear flow.

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