TY - JOUR
T1 - Reactions between a 1/2⟨111⟩ screw dislocation and ⟨100⟩ interstitial dislocation loops in alpha-iron modelled at atomic scale
AU - Terentyev, Dmitry
AU - Bacon, D.J.
AU - Osetsky, Yu.N.
N1 - Score=10
PY - 2009/9/8
Y1 - 2009/9/8
N2 - Interstitial dislocation loops with Burgers vector of type are observed in α-iron irradiated by neutrons or heavy ions, and their population increases with increasing temperature. Their effect on motion of a edge dislocation was reported earlier 1. Results are presented of a molecular dynamics study of interactions between a screw dislocation and loops in iron at temperature in the range 100 to 600 K. A variety of reaction mechanisms and outcomes are observed and classified in terms of the resulting dislocation configuration and the maximum stress required for the dislocation to break away. The highest obstacle resistance arises when the loop is absorbed to form a helical turn on the screw dislocation line, for the dislocation cannot glide away until the turn closes and a loop is released with the same Burgers vector as the line. Other than one situation found, in which no dislocation–loop reaction occurs, the weakest obstacle strength is found when the original loop is restored at the end of the reaction. The important role of the cross-slip and the influence of model boundary conditions are emphasised and demonstrated by examples.
AB - Interstitial dislocation loops with Burgers vector of type are observed in α-iron irradiated by neutrons or heavy ions, and their population increases with increasing temperature. Their effect on motion of a edge dislocation was reported earlier 1. Results are presented of a molecular dynamics study of interactions between a screw dislocation and loops in iron at temperature in the range 100 to 600 K. A variety of reaction mechanisms and outcomes are observed and classified in terms of the resulting dislocation configuration and the maximum stress required for the dislocation to break away. The highest obstacle resistance arises when the loop is absorbed to form a helical turn on the screw dislocation line, for the dislocation cannot glide away until the turn closes and a loop is released with the same Burgers vector as the line. Other than one situation found, in which no dislocation–loop reaction occurs, the weakest obstacle strength is found when the original loop is restored at the end of the reaction. The important role of the cross-slip and the influence of model boundary conditions are emphasised and demonstrated by examples.
KW - Iron
KW - Neutron irradiation damage
KW - Intersitial dislocation loops
KW - Screw dislocation
KW - Dislocation-loop interaction
KW - Molecular dynamics
KW - Strengthening mechanism
UR - http://ecm.sckcen.be/OTCS/llisapi.dll/open/ezp_105002
U2 - 10.1080/14786430903019073
DO - 10.1080/14786430903019073
M3 - Article
SN - 0031-8086
VL - 90
SP - 1019
EP - 1033
JO - Philosophical Magazine
JF - Philosophical Magazine
IS - 7-8
ER -