Multiple necking patterns in elasto-plastic rings subjected to rapid radial expansion: The effect of random distributions of geometric imperfections

Abstract

In this paper we have investigated, using finite element calculations performed in ABAQUS/Explicit [1], the effect of ab initio geometric imperfections in the development of multiple necking patterns in ductile rings subjected to dynamic expansion. Specifically, we have extended the work of , who studied the formation of necks in rings with sinusoidal spatial perturbations of predefined amplitude and constant wavelength, by considering specimens with random distributions of perturbations of varying amplitude and wavelength. The idea, which is based on the work of El Maï et al. [4], is to provide an idealized modeling of the surface defects and initial roughness of the rings and explore their effect on the collective behavior and spacing of the necks. The material behavior has been modeled with von Mises plasticity and constant yield stress, and the finite element simulations have been performed for expanding velocities ranging from 10 m/s to 1000 m/s, as in ref. [33]. For each speed, we have performed calculations varying the number of imperfections in the ring from 5 to 150. In order to obtain statistically significant results, for each number of imperfections, the computations have been run with five random distributions of imperfection wavelengths.For a small number of imperfections, the variability in the wavelengths distribution is large, which makes the imperfections play a major role in the necking pattern, largely controlling the spacing and growth rate of the necks. As the number of imperfections increases, the variability in the wavelengths distribution decreases, giving rise to an array of more regularly spaced necks which grow at more similar speed. A key outcome is to show that, for a large number of imperfections, the number of necks formed in the ring comes closer to the number of necks obtained in the absence of ab initio geometric imperfections.

Finite element analysis to determine the role of porosity in dynamic localization and fragmentation: Application to porous microstructures obtained from additively manufactured materials

“…The loading condition is a radial velocity, V r , applied in the inner surface of the ring which remains constant throughout the entire analysis (Rusinek and Zaera, 2007; Vadillo et al, 2012; Rodríguez-Martínez et al, 2013b;Vaz-Romero et al, 2019). The initial condition is a radial velocity of the same value V (t = 0) = V r applied to all the nodes of the finite element mesh (Vaz-Romero et al, 2019;Marvi-Mashhadi and Rodríguez-Martínez, 2020). The application of this initial condition minimizes the propagation of waves through the thickness of the ring due to the abrupt motion of the inner surface at t = 0.…”

The effect of initial texture on multiple necking formation in polycrystalline thin rings subjected to dynamic expansion

“…1(b). The loading condition is a radial velocity 𝑉 𝑅 applied in the inner surface of the ring which remains constant during the entire analysis (Rusinek and Zaera, 2007;Vadillo et al, 2012;Vaz-Romero et al, 2019), whereas the initial condition is a radial velocity of the same value applied to all material points (Marvi-Mashhadi and Rodríguez-Martínez, 2020;Marvi-Mashhadi et al, 2021). The application of this initial condition minimizes the propagation of waves through the radial thickness of the ring caused by the abrupt motion of the inner surface at 𝑡 = 0, precluding instantaneous plastic localization due to the velocity loading condition (Needleman, 1991;Xue et al, 2008;Vaz-Romero et al, 2019).…”

Influence on strain-rate history effects on the development of necking instabilities under dynamic loading conditions

“…The development of necking instabilities is known to be very sensitive to imperfections (Hutchinson and Neale, 1977;Han and Tvergaard, 1995;Xavier et al, 2020;Marvi-Mashhadi and Rodríguez-Martínez, 2020). In the present simulations, a random material imperfection has been used to break the symmetry of the problem and favour necking localisation.…”