TY - GEN
T1 - Dislocation dynamics and multiplication via atomistic simulations
AU - Clapp, P. C.
AU - Glazov, M. V.
AU - Rifkin, J. A.
PY - 1993
Y1 - 1993
N2 - Molecular Dynamics simulations of edge dislocation mobility under stress in ordered Ll2Ni3Al have been performed between 10K and 1000K, and at applied shear stresses ranging from 0.01 to 0. 08C44. In this way it has been possible to determine the Peierls stress and mobility parameters as a function of stress and temperature. (100) edge dislocations were studied, which split into closely spaced partials under stress. Under all levels of applied stress (and at lower temperatures) the initial partial dislocations would intermittently stop moving and recombine, then dissociate and move again. In all cases the dislocations exhibited a soliton-like behavior infinite acceleration at the onset of movement, and further movement at a steady velocity (which was only weakly dependent on stress) on the order of 25% of the acoustic shear velocity. Non-classical, highly non-linear behavior was observed indicating the probability that a soliton picture of dislocation motion is more appropriate than the classical, 'massive string' model that is traditionally used. Furthermore, as both the temperature and the stress were increased, dislocation multiplication became increasingly frequent, ultimately resulting in a spontaneous amorphization transition which has signs of being a percolation process.
AB - Molecular Dynamics simulations of edge dislocation mobility under stress in ordered Ll2Ni3Al have been performed between 10K and 1000K, and at applied shear stresses ranging from 0.01 to 0. 08C44. In this way it has been possible to determine the Peierls stress and mobility parameters as a function of stress and temperature. (100) edge dislocations were studied, which split into closely spaced partials under stress. Under all levels of applied stress (and at lower temperatures) the initial partial dislocations would intermittently stop moving and recombine, then dissociate and move again. In all cases the dislocations exhibited a soliton-like behavior infinite acceleration at the onset of movement, and further movement at a steady velocity (which was only weakly dependent on stress) on the order of 25% of the acoustic shear velocity. Non-classical, highly non-linear behavior was observed indicating the probability that a soliton picture of dislocation motion is more appropriate than the classical, 'massive string' model that is traditionally used. Furthermore, as both the temperature and the stress were increased, dislocation multiplication became increasingly frequent, ultimately resulting in a spontaneous amorphization transition which has signs of being a percolation process.
UR - https://www.scopus.com/pages/publications/0027702428
U2 - 10.1051/jp4:19937320
DO - 10.1051/jp4:19937320
M3 - Conference contribution
AN - SCOPUS:0027702428
SN - 2868832067
SN - 9782868832061
T3 - Journal De Physique
SP - 2005
EP - 2014
BT - Journal De Physique
PB - Publ by Editions de Physique
T2 - Proceedings of the 3rd European Conference on Advanced Materials and Processes. Part 3 (of 3)
Y2 - 8 June 1993 through 10 June 1993
ER -