6533b7dbfe1ef96bd1271463

RESEARCH PRODUCT

Residual Stresses in Glasses

Kevin J. MutchGeorge PetekidisMiriam SiebenbürgerThomas VoigtmannMatthias KrügerMatthias KrügerMatthias BallauffNick KoumakisMarco LauratiJoseph M. BraderJochen ZauschStefan U. EgelhaafMatthias FuchsJürgen Horbach

subject

Length scaleThermodynamic stateFOS: Physical sciencesGeneral Physics and Astronomy02 engineering and technologyCondensed Matter - Soft Condensed Matterglasses01 natural sciencesMolecular dynamicsResidual stress0103 physical sciencesddc:530Ideal (ring theory)010306 general physicsPhysicsCondensed Matter - Materials ScienceCondensed matter physicsMaterials Science (cond-mat.mtrl-sci)021001 nanoscience & nanotechnologyShear rateCondensed Matter::Soft Condensed MatterFlow (mathematics)residual stressesSoft Condensed Matter (cond-mat.soft)Relaxation (physics)rheology0210 nano-technologyRheology Glasses Residual Stresses Mode Coupling Theory

description

The history dependence of the glasses formed from flow-melted steady states by a sudden cessation of the shear rate $\dot\gamma$ is studied in colloidal suspensions, by molecular dynamics simulations, and mode-coupling theory. In an ideal glass, stresses relax only partially, leaving behind a finite persistent residual stress. For intermediate times, relaxation curves scale as a function of $\dot\gamma t$, even though no flow is present. The macroscopic stress evolution is connected to a length scale of residual liquefaction displayed by microscopic mean-squared displacements. The theory describes this history dependence of glasses sharing the same thermodynamic state variables, but differing static properties.

10.1103/physrevlett.110.215701http://arxiv.org/abs/1302.3914