INVESTIGADORES
BRINGA Eduardo Marcial
artículos
Título:
Void growth in metals: Atomistic calculations
Autor/es:
S. TRAIVIRATANA; E.M. BRINGA; D.J. BENSON; M.A. MEYERS
Revista:
ACTA MATERIALIA
Editorial:
PERGAMON-ELSEVIER SCIENCE LTD
Referencias:
Año: 2008 vol. 56 p. 3874 - 3886
ISSN:
1359-6454
Resumen:
Molecular dynamics simulations in monocrystalline and bicrystalline
copper were carried out with LAMMPS (Large-scale Atomic/Molecular
Massively Parallel Simulator) to reveal void growth mechanisms. The
specimens were subjected to tensile uniaxial strains; the results
confirm that the emission of (shear) loops is the primary mechanism of
void growth. It is observed that many of these shear loops develop along
two slip planes (and not one, as previously thought), in a heretofore
unidentified mechanism of cooperative growth. The emission of
dislocations from voids is the first stage, and their reaction and
interaction is the second stage. These loops, forming initially on
different {1 1 1} planes, join at the intersection, if the Burgers
vector of the dislocations is parallel to the intersection of two
{1 1 1} planes: a 〈1 1 0〉 direction. Thus, the two dislocations cancel
at the intersection and a biplanar shear loop is formed. The expansion
of the loops and their cross slip leads to the severely work-hardened
region surrounding a growing void. Calculations were carried out on
voids with different sizes, and a size dependence of the stress
threshold to emit dislocations was obtained by MD, in disagreement with
the Gurson model which is scale independent. This disagreement is most
marked for the nanometer sized voids. The scale dependence of the stress
required to grow voids is interpreted in terms of the decreasing
availability of optimally oriented shear planes and increased stress
required to nucleate shear loops as the void size is reduced. The growth
of voids simulated by MD is compared with the CocksAshby constitutive
model and significant agreement is found. The density of geometrically
necessary dislocations as a function of void size is calculated based on
the emission of shear loops and their outward propagation. Calculations
are also carried out for a void at the interface between two grains to
simulate polycrystalline response. The dislocation emission pattern is
qualitatively similar to microscope observations.