TY - JOUR
T1 - A dislocation-crystal plasticity simulation on large deformation considering geometrically necessary dislocation density and incompatibility (1st report, definitions of GN crystal defects and multiscale modeling)
AU - Aoyagi, Yoshiteru
AU - Shizawa, Kazuyuki
PY - 2006/7
Y1 - 2006/7
N2 - Plastic deformation and work-hardening of a crystal are caused by dislocation motions and dislocation accumulations, respectively. Recently, studies of crystal plasticity with the dislocation information have actively been done by many researchers. In this paper, both densities of isolated dislocation and dislocation pair corresponding respectively to the conventional GN and SS dislocation densities are uniformly defined as geometrical quantities, i.e., GN dislocation density and GN incompatibility tensors by extending Kroner's dislocation density and incompatibility tensors so that they are suitable for a crystal plasticity framework. Furthermore, we newly introduce a term of dynamic recovery that occurs in stage III of work-hardening of a single crystal into the expression of dislocation density. A new model of dislocation-crystal plasticity coupling deformation field with dislocation field is developed by introducing these dislocation densities into a hardening modulus matrix of crystal plasticity through the Bailey-Hirsch relation.
AB - Plastic deformation and work-hardening of a crystal are caused by dislocation motions and dislocation accumulations, respectively. Recently, studies of crystal plasticity with the dislocation information have actively been done by many researchers. In this paper, both densities of isolated dislocation and dislocation pair corresponding respectively to the conventional GN and SS dislocation densities are uniformly defined as geometrical quantities, i.e., GN dislocation density and GN incompatibility tensors by extending Kroner's dislocation density and incompatibility tensors so that they are suitable for a crystal plasticity framework. Furthermore, we newly introduce a term of dynamic recovery that occurs in stage III of work-hardening of a single crystal into the expression of dislocation density. A new model of dislocation-crystal plasticity coupling deformation field with dislocation field is developed by introducing these dislocation densities into a hardening modulus matrix of crystal plasticity through the Bailey-Hirsch relation.
KW - Constitutive Equation
KW - Crystal Plasticity
KW - Dislocation
KW - Dislocation Dipole
KW - Geometrically Necessary Dislocation
KW - Incompatibility
KW - Large Deformation
KW - Plasticity
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U2 - 10.1299/kikaia.72.1009
DO - 10.1299/kikaia.72.1009
M3 - Article
AN - SCOPUS:33749539353
SN - 0387-5008
VL - 72
SP - 1009
EP - 1016
JO - Nihon Kikai Gakkai Ronbunshu, A Hen/Transactions of the Japan Society of Mechanical Engineers, Part A
JF - Nihon Kikai Gakkai Ronbunshu, A Hen/Transactions of the Japan Society of Mechanical Engineers, Part A
IS - 7
ER -