Atomic-scale origin of dynamic viscoelastic response and creep in disordered solids
arXiv:1702.00620 · doi:10.1103/PhysRevE.95.023001
Abstract
Viscoelasticity has been described since the time of Maxwell as an interpolation of purely viscous and purely elastic response, but its microscopic atomic-level mechanism in solids has remained elusive. We studied three model disordered solids: a random lattice, the bond-depleted fcc lattice, and the fcc lattice with vacancies. Within the harmonic approximation for central-force lattices, we applied sum-rules for viscoelastic response derived on the basis of non-affine atomic motions. The latter motions are a direct result of local structural disorder, and in particular, of the lack of inversion-symmetry in disordered lattices. By defining a suitable quantitative and general atomic-level measure of nonaffinity and inversion-symmetry, we show that the viscoelastic responses of all three systems collapse onto a master curve upon normalizing by the overall strength of inversion-symmetry breaking in each system. Close to the isostatic point for central-force lattices, power-law creep emerges as a consequence of the interplay between soft vibrational modes and non-affine dynamics, and various analytical scalings, supported by numerical calculations, are predicted by the theory.
References in corpus (15)
- Jamming at Zero Temperature and Zero Applied Stress: the Epitome of Disorder
- Amorphous Systems in Athermal, Quasistatic Shear
- Irreversible reorganization in a supercooled liquid originates from localised soft modes
- Vibrations and diverging length scales near the unjamming transition
- Criticality and isostaticity in fiber networks
- Approximate analytical description of the nonaffine response of amorphous solids
- Continuum limit of amorphous elastic bodies (III): Three dimensional systems
- Universal Spectrum of Normal Modes in Low-Temperature Glasses: an Exact Solution
- Local inversion-symmetry breaking controls the boson peak in glasses and crystals
- Non-affine response: jammed packings versus spring networks
- Relaxations and rheology near jamming
- Rigidity Loss in Disordered Systems: Three Scenarios
- Floppiness, cutting, and freezing: Dynamic critical scaling near isostaticity
- Dynamical behavior of disordered spring networks
- Thermalized connectivity networks of jammed packings
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- Non-affine deformation of semiflexible polymer and fiber networks
- Molecular interpretation of the non-Newtonian viscoelastic behavior of liquid water at high frequencies
- Equilibrium and non-equilibrium molecular dynamics approaches for the linear viscoelasticity of polymer melts
- Possible origin of -relaxation in amorphous metal alloys from atomic-mass differences of the constituents
- Scaling up the lattice dynamics of amorphous materials by orders of magnitude
- Predicting plasticity of amorphous solids from instantaneous normal modes
- Complete mathematical theory of the jamming transition: A perspective
- Strain-controlled critical slowing down in the rheology of disordered networks
- Timescale bridging in atomistic simulations of epoxy polymer mechanics using non-affine deformation theory
- Ioffe-Regel criterion and viscoelastic properties of amorphous solids
- Theory of heavy-quarks contribution to the quark-gluon plasma viscosity
- Viscosity of polymer melts using non-affine theory based on vibrational modes
- Effective medium theory for viscoelasticity of soft jammed solids
- Unified study of viscoelasticity and sound damping in hard and soft amorphous solids
- Viscoelastic scaling regimes for marginally-rigid fractal spring networks
- A Linear Time-Variant Rheological Model for Frictional Aging, Stress Relaxation, and Creep