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Assuming that the interlayer thickness tends to zero, a constant normal stress is prescribed in the zone of mechanical yielding and a saturated electrical displacement is prescribed in the zone of electrical saturation.
To avoid the singularities, which are typical for the Griffith crack model, two distinct zones – a zone of mechanical yielding and a zone of electrical saturation – of unknown lengths are introduced as crack continuations.
Similar(58)
Mechanical yielding of all arrays is initiated between 0.03 and 0.12 strain and arises from localized coordinated plastic buckling.
The unknown yield and saturated zones lengths are found from the conditions of finiteness of stress and electrical displacement at the ends of these zones for the both cases when the electrical saturated zone is longer and shorter than the zone of mechanical yielding.
These lengths can be essentially different, with the zone of mechanical yielding significantly longer or shorter than the zone of electrical saturation.
It was found that the mechanical yielding of α-crystallitic iPP is dominated by the plastic flow of crystalline structural units whereas the yield process of α-spherulitic iPP quenched at 80 °C is caused by the fracture or fragmentation of crystalline structural units.
Matrix yielding and micro mechanical damage due to debonding at the fibre matrix interface are the main consequences after interlaminar shear load is applied on the RVE.
These methods enable us to explore phenomena such as elastic anisotropy in rocks, changes in strain partitioning during plastic yielding, and stress-induced mechanical twinning.
Non-linear mechanical behavior such as phase transformation, discontinuous yielding and micro-damage of four kinds of commercial stainless steel-based material were quantitatively investigated by measuring transformation induced plasticity (TRIP) and threshold strain for 2nd hardening.
The surface deformation features are also consistent with mechanisms such as localized shear flow, serrated yielding and adiabatic heating, which are observed during macroscopic mechanical tests.
The molecular dynamics of two polyurethanes with different architecture (linear and hyperbranched) and their blends with compositions 80/20 and 65/35 have been studied by dielectric spectroscopy and dynamic mechanical analysis yielding results complementary to those obtained by differential scanning calorimetry.
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