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Controlling material parameters are strength (brittle mode) and yield stress or hardness (plastic mode).
This discovery of the reversible plastic mode of fcc twinning should find important application in the theory and modeling of large plastic deformations of fcc materials, including cyclic deformation phenomena.
The numerical solution for the homogenisation problem and the performances of the proposed coupled-damage plastic mode and Fourier-based homogenisation scheme verified by detailed case studies are presented.
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By theoretical analysis, the new formulae have been introduced for both the elastic and plastic mode-mixity parameters, accounting for ratios between the I/II, II/III and III/I modes.
Andrews [10] studied the contact between two spheres in the elasto-plastic mode as they impact each other with an initial velocity of V0.
Consequently, the strength in elasto-plastic mode, maximum deflection and plastic strain of the equipped system representing the permanent damage is obtained in order to achieve lower losses.
Extrapolations of these relations into the quasi-plastic region are shown to be non-conservative, highlighting the need for further understanding of the deleterious quasi-plastic mode in tougher ceramics.
Secondary damage at large numbers of cycles and high loads consists of shear-driven distributed microdamage ("quasi-plastic" mode), with attendant radial cracks and a new form of deeply penetrating subsidiary cone cracks.
Shear banding is the main plastic deformation mode in metallic glasses.
The faulting process and its associated plastic deformation mode is compared using several material models.
Twinning in certain metals or under certain conditions is a major plastic deformation mode.
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