Recent data of unentangled polystyrene melts in startup elongational flow and subsequent relaxation [Matsumiya, Y.; Watanabe, H.; Masubuchi, Y.; Huang, Q.; Hassager, O. Nonlinear Elongational Rheology of Unentangled Polystyrene and Poly(p-Tert-Butylstyrene) Melts. Macromolecules 2018, 51 (23), 9710-9729 ] are here compared to the predictions of Brownian simulations of Fraenkel chains endowed with a monomeric friction coefficient that decreases with increasing the order parameter of the Kuhn segments. The model compares favorably with all startup data if a time delay in reducing the monomeric friction coefficient is accounted for in the fastest flows, a feature already observed by Matsumiya et al. The same model also describes the relaxation data except for a minor discrepancy in the longest relaxation time, probably due to the imperfect monodispersity of the sample and/or to a minor influence of topological interactions, not strong enough to be called entanglements. A discrepancy is also observed at the beginning of relaxation after fast flows, the origin of which remains unexplained.
Modeling unentangled polystyrene melts in fast elongational flows / Ianniruberto, G.; Brasiello, A.; Marrucci, G.. - In: MACROMOLECULES. - ISSN 0024-9297. - 52:12(2019), pp. 4610-4616. [10.1021/acs.macromol.9b00658]
Modeling unentangled polystyrene melts in fast elongational flows
Brasiello A.;
2019
Abstract
Recent data of unentangled polystyrene melts in startup elongational flow and subsequent relaxation [Matsumiya, Y.; Watanabe, H.; Masubuchi, Y.; Huang, Q.; Hassager, O. Nonlinear Elongational Rheology of Unentangled Polystyrene and Poly(p-Tert-Butylstyrene) Melts. Macromolecules 2018, 51 (23), 9710-9729 ] are here compared to the predictions of Brownian simulations of Fraenkel chains endowed with a monomeric friction coefficient that decreases with increasing the order parameter of the Kuhn segments. The model compares favorably with all startup data if a time delay in reducing the monomeric friction coefficient is accounted for in the fastest flows, a feature already observed by Matsumiya et al. The same model also describes the relaxation data except for a minor discrepancy in the longest relaxation time, probably due to the imperfect monodispersity of the sample and/or to a minor influence of topological interactions, not strong enough to be called entanglements. A discrepancy is also observed at the beginning of relaxation after fast flows, the origin of which remains unexplained.File | Dimensione | Formato | |
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