Softening and residual loss modulus of jammed grains under oscillatory shear in an absorbing state
arXiv:2101.07473 · doi:10.1103/PhysRevLett.128.208002
Abstract
From a theoretical study of the mechanical response of jammed materials comprising frictionless and overdamped particles under oscillatory shear, we find that the material becomes soft, and the loss modulus remains finite even in an absorbing state where any irreversible plastic deformation does not exist. The trajectories of the particles in this region exhibit hysteresis loops. We succeed in clarifying the origin of the softening of the material and the residual loss modulus with the aid of Fourier analysis. We also clarify the roles of the yielding point in the softening to distinguish the plastic deformation from reversible deformation in the absorbing state.
References in corpus (7)
- A microscopic view of the yielding transition in concentrated emulsions
- Multiple transient memories in experiments on sheared non-Brownian suspensions
- Reversible plasticity in amorphous materials
- Period proliferation in periodic states in cyclically sheared jammed solids
- Contact Changes near Jamming
- Shear jamming and shear melting in mechanically trained frictionless particles
- Shear modulus and reversible particle trajectories of frictional granular materials under oscillatory shear
Cited by in corpus (6)
- Perspective on Reversible to Irreversible Transitions in Periodic Driven Many Body Systems and Future Directions For Classical and Quantum Systems
- Complete mathematical theory of the jamming transition: A perspective
- Eigenvalue analysis of stress-strain curve of two-dimensional amorphous solids of dispersed frictional grains with finite shear strain
- Rigidity transition of a highly compressible granular medium
- An exact expression of three-body system for the complex shear modulus of frictional granular materials
- Theory of rigidity and numerical analysis of density of states of two-dimensional amorphous solids with dispersed frictional grains in the linear response regime