This is the author’s version of a work that was accepted for publication in the journal, International Journal of Plasticity. Changes resulting from the publishing process, such as peer review, editing, corrections, structural formatting, and other quality control mechanisms may not be reflected in this document. Changes may have been made to this work since it was submitted for publication. A definitive version was subsequently published at: http://dx.doi.org/10.1016/j.ijplas.2011.07.003Discrete dislocation dynamics (DDD) has been used to model the deformation of nickelbased\ud single crystal superalloys with a high volume fraction of precipitates at high temperature.\ud A representative volume cell (RVC), comprising of both the precipitate and the\ud matrix phase, was employed in the simulation where a periodic boundary condition was\ud applied. The dislocation Frank–Read sources were randomly assigned with an initial density\ud on the 12 octahedral slip systems in the matrix channel. Precipitate shearing by superdislocations\ud was modelled using a back force model, and the coherency stress was\ud considered by applying an initial internal stress field. Strain-controlled loading was applied\ud to the RVC in the [0 0 1] direction. In addition to dislocation structure and density evolution,\ud global stress–strain responses were also modelled considering the influence of precipitate\ud shearing, precipitate morphology, internal microstructure scale (channel width and\ud precipitate size) and coherency stress. A three-stage stress–strain response observed in\ud the experiments was modelled when precipitate shearing by superdislocations was considered.\ud The polarised dislocation structure deposited on the precipitate/matrix interface was\ud found to be the dominant strain hardening mechanism. Internal microstructure size, precipitate\ud shape and arrangement can significantly affect the deformation of the single crystal\ud superalloy by changing the constraint effect and dislocation mobility. The coherency\ud stress field has a negligible influence on the stress–strain response, at least for cuboidal\ud precipitates considered in the simulation. Preliminary work was also carried out to simulate\ud the cyclic deformation in a single crystal Ni-based superalloy using the DDD model,\ud although no cyclic hardening or softening was captured due to the lack of precipitate\ud shearing and dislocation cross slip for the applied strain considered
1 September 2006 in International Journal of Solids and Structures
This is an open access article under the CC BY license (http://\ud creativecommons.org/licenses/by/4.0/).Using crystal plasticity, finite element analyses were carried out to model cyclic deformation for a low\ud solvus high refractory (LSHR) nickel superalloy at elevated temperature. The analyses were implemented\ud using a representative volume element (RVE), consisting of realistic microstructure obtained from SEM\ud images of the material. Monotonic, stress-relaxation and cyclic test data at 725 C were used to determine\ud the model parameters from a fitting process and their sensitivity to RVE size and random grain orientation.\ud In combination with extended finite element method (XFEM), the crystal plasticity model was further\ud applied to predict surface crack growth, for which accumulated plastic strain was used as a fracture\ud criterion. Again, realistic microstructure, taken from the cracking site on the surface of a plain fatigue\ud specimen, was used to create the finite element model for crack growth analyses. The prediction was conducted\ud for a pseudo-3D geometrical model, resembling the plane stress condition at specimen surface.\ud The loading level at the cracking site was determined from a viscoplasticity finite element analysis of\ud the fatigue specimen. The proposed model is capable of predicting the variation in growth rate in grains\ud with different orientations