Modeling the Relaxation of Polymer Glasses under Shear and Elongational Loads
arXiv:1209.0929 · doi:10.1063/1.4769253
Abstract
Glassy polymers show strain hardening: at constant extensional load, their flow first accelerates, then arrests. Recent experiments under such loading have found this to be accompanied by a striking dip in the segmental relaxation time. This can be explained by a minimal nonfactorable model combining flow-induced melting of a glass with the buildup of stress carried by strained polymers. Within this model, liquefaction of segmental motion permits strong flow that creates polymer-borne stress, slowing the deformation enough for the segmental (or solvent) modes to then re-vitrify. Here we present new results for the corresponding behavior under step-stress shear loading, to which very similar physics applies. To explain the unloading behavior in the extensional case requires introduction of a crinkle factor describing a rapid loss of segmental ordering. We discuss in more detail here the physics of this, which we argue involves non-entropic contributions to the polymer stress, and which might lead to some important differences between shear and elongation. We also discuss some fundamental and possibly testable issues concerning the physical meaning of entropic elasticity in vitrified polymers. Finally we present new results for the startup of steady shear flow, addressing the possible role of transient shear banding.
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- Triggers and signatures of shear banding in steady and time-dependent flows
- Shear banding in large amplitude oscillatory shear (LAOStrain and LAOStress) of soft glassy materials
- Yielding, shear banding and brittle failure of amorphous materials
- Comparison of mechanical and molecular measures of mobility during constant strain rate deformation of a PMMA glass
- Shear banding in large amplitude oscillatory shear (LAOStrain and LAOStress) of polymers and wormlike micelles