Abstract:Using non-equilibrium molecular dynamics simulations we study the yielding behaviour of a model cluster crystal formed by ultrasoft particles under shear. We investigate the evolution of stress as a function of strain for different shear rates, γ, and temperatures. The stress-strain relation displays a pronounced maximum at the yielding point; the height of this maximum, σ p , increases via a power law with an increasing shear range and tends to saturate to a finite value if the limit shear rate goes to zero (… Show more
“…Of course, within a short time this vacancy will be filled up by another particle arriving from another, neighboring lattice site. In our previous work 55 we have demonstrated that cluster crystals exhibit an overshoot in their stress-strain response. For a fixed temperature, the height of this overshoot decreases with a decreasing shear rate.…”
Section: Introductionmentioning
confidence: 91%
“…Starting our reasoning from Equ. (9) this master curve has thus the form [33,44]: In panel (b) of Fig. 3 we show this master curve onto which the different σ p ( γ)-curves can be mapped.…”
In real crystals and at finite temperatures point defects are inevitable. Under shear their dynamics severely influence the mechanical properties of these crystals, giving rise to non-linear effects, such as...
“…Of course, within a short time this vacancy will be filled up by another particle arriving from another, neighboring lattice site. In our previous work 55 we have demonstrated that cluster crystals exhibit an overshoot in their stress-strain response. For a fixed temperature, the height of this overshoot decreases with a decreasing shear rate.…”
Section: Introductionmentioning
confidence: 91%
“…Starting our reasoning from Equ. (9) this master curve has thus the form [33,44]: In panel (b) of Fig. 3 we show this master curve onto which the different σ p ( γ)-curves can be mapped.…”
In real crystals and at finite temperatures point defects are inevitable. Under shear their dynamics severely influence the mechanical properties of these crystals, giving rise to non-linear effects, such as...
In complex crystals close to melting or at finite temperatures, different types of defects are ubiquitous and their role becomes relevant in the mechanical response of these solids. Conventional elasticity theory fails to provide a microscopic basis to include and account for the motion of point-defects in an otherwise ordered crystalline structure. We study the elastic properties of a point-defect rich crystal within a first principles theoretical framework derived from microscopic equations of motion. This framework allows us to make specific predictions pertaining to the mechanical properties which we can validate through deformation experiments performed in Molecular Dynamics simulations.
In complex crystals close to melting or at finite temperatures, different types of defects are ubiquitous and their role becomes relevant in the mechanical response of these solids. Conventional elasticity theory fails to provide a microscopic basis to include and account for the motion of point defects in an otherwise ordered crystalline structure. We study the elastic properties of a point-defect rich crystal within a first principles theoretical framework derived from the microscopic equations of motion. This framework allows us to make specific predictions pertaining to the mechanical properties that we can validate through deformation experiments performed in molecular dynamics simulations.
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