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dc.contributor.authorNjoroge, Kennedy D
dc.date.accessioned2015-08-21T07:38:49Z
dc.date.available2015-08-21T07:38:49Z
dc.date.issued2015
dc.identifier.urihttp://hdl.handle.net/11295/89889
dc.descriptionThesisen_US
dc.description.abstractMulti-scale simulation techniques are increasingly being applied to the study of engineering problems, where characterizing phenomena occur at different length scales and where phenomena occurring at some length scale influences phenomena occurring at a different length scale. In material performance studies, it is understood that bonding at the atomic length scale, aggregation of grains, the existence and evolution of defects, all contribute to material behaviour. The goal of this research was to develop models that enabled the simulation at various length scales intended to capture a metal’s behaviour, and to link these models to enable data transfer up the length scales. The study was founded on the application of the embedded atom method (EAM) to the iron (Fe) and iron carbide (Fe-C) lattices, and on the understanding that plasticity is primarily driven by the motion of dislocations. The work involved the development of Fortran code for the implementation of the EAM, the simulation of the stress fields for both static and dynamic dislocation cores, the assembly of dislocation lines within slip planes, the assembly of slip planes within a material’s lattice, and the implementation of grain evolution using finite element code. The models at the lower length scales were validated using empirical and Ab-initio Peierl’s stress data. The work was carried out in five stages corresponding to the length scales considered. The lowest level length scale (dislocation core-length scale) was used to study the evolution of the dislocation core. This was done by simulating the motion of dislocation core atoms in a lattice containing a single dislocation line, under an externally applied load, and tracking the resulting stress around the dislocation core. The principle result was the establishment of the link between the Peierl’s stress and the smallest peak amplitude of the direct stress components for a dislocation line in the [111�] direction. This work gave rise to the path of least resistance (POLR) method used to predict the Peierls stress peak around the dislocation core. A mechanism for the motion of dislocation core atoms was established and the POLR stresses for different dislocation types were evaluated. The line-length scale was used to characterize the effects of the dislocation core’s distortion extended over a wider region than that possible within the capability of the EAM. This was done by the simulation of the stress profile resulting from a dislocation line, with the peak POLR stress This work gave rise to the misfit potential (MP) which enabled the determination of the longer range dislocation stress field through which, interactions with other lattice defects would take place. The results of the simulation of the behaviour of the interaction of dislocations dipoles are reported. The plane-length scale accounted for the interaction of dislocation lines within the slip plane. The theory of generalized functions (distributions) was applied to profile the spatial position of interacting dislocations, and to relate them to the resulting stress amplitude profile. This work gave rise to the plane structure factor (PSF), which was used to determine the planar dislocation density which was used as an input at the next higher length scale. The model was used to determine the resulting stress field over a slip plane containing assemblies of planar dislocation structures, and the stress field was then used to predict the evolution of the dislocation assembly. The structure-length scale accounted for the assembly of slip planes to construct 3-dimensional (3D) dislocation structures. This stage accounted for the peak POLR stress and applied the misfit potential in the study of 2-dimensional (2-D) dislocation lines assembled into a 3-D dislocation structure. Simulations were carried out to determine the resulting stress field, which was used to characterize a 3-D dislocation structure factor. This work gave rise to the network structure factor (NSF), which was used to determine the network dislocation density which was used as an input at the next higher length scale. The model was used to determine the resulting stress field in a lattice containing dislocation structures. The network structure factor was then used as an input into a finite element formulation that was used at the meso-length scale. This factor captured the mechanistic events at the underlying l incorporate the physics of the material’s behaviour in the prediction of its deformation. The outputs of this research are the POLR model, the MP model, the PSF model, the NSF model, the meso-scale model, the linkages between these models, the linking of these models with Peierls stress data and dislocation density data, and the link to grain size driven yield stresses of materials. These results are expected to complement current and future work in materials characterization and alloy development, and enhance the value of simulation in engineering designen_US
dc.language.isoenen_US
dc.publisherUniversity of Nairobien_US
dc.titleA multi-scale dislocation model applied to metal plasticityen_US
dc.typeThesisen_US
dc.type.materialen_USen_US


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