TY - BOOK
T1 - Characterisation of polycrystal deformation by numerical modelling and neutron diffraction measurements
AU - Clausen, Bjørn
PY - 1997
Y1 - 1997
N2 - The uniaxial deformation of polycrystals are modelled using three incremental rate-insensitive micro-mechanic models; the Taylor model, the Sachs model and Hutchinson’s self-consistent model. The predictions of the two rigid plastic upper- and lower-bound models (Taylor and Sachs) are compared with the predictions of the elastic-plastic self-consistent model. As expected, the results of the self-consistent model is about half-way between the upper- and lower-bound models. The average number of active slip systems is about 3.6 compared to the five active slip systems in the Taylor model and the one active slip system in the Sachs model. The average m-factor is about 2.6 compared to the 3.06 in the Taylor model and the 2.23 in the Sachs model. The predicted rotation pattern of the self-consistent model is closest to the Taylor model, but the orientation distribution of the m-factor is closest to the Sachs model. The influence of the elastic anisotropy is investigated by comparing the self-consistent predictions for aluminium, copper and a hypothetical material (hybrid) with the elastic anisotropy of copper and the Young’s modulus and work hardening behaviour of aluminium. It is concluded, that the effect of the elastic anisotropy is limited to the very early stages of plasticity (εP < ∼0.1%), as the deformation pattern is almost identical for the
three materials at higher strains.
The predictions of the three models are evaluated by neutron diffraction mea-surements of elastic lattice strains in grain sub-sets within the polycrystal. In the evaluation of the rigid plastic Taylor and Sachs models, the ’elastic’ strain is determined as the calculated stress divided by the diffraction elastic constants (cal-culated as the Kr¨oner elastic stiffnesses for the grain sub-sets). The comparison of calculated and measured lattice strains are made for three different materials; alu-minium, copper and austenitic stainless steel. The predictions of the self-consistent model is more accurate and detailed than the predictions of the Taylor and Sachs models, though some discrepancies are noted for some reflections.
The self-consistent model is used to determine the most suitable reflection for technological applications of neutron diffraction, where focus is on the volume av-erage stress state in engineering components. To be able to successfully convert the measured elastic lattice strains for a specific reflection into overall volume average stresses, there must be a linear relation between the lattice strain of the reflection and the overall stress. According to the model predictions the 311-reflection is the most suitable reflection, as it shows the smallest deviations from linearity and thereby also the smallest build-up of residual lattice strains. Below 5% deforma-tion the deviations from linearity and the residual strains are below the normal strain resolution of a neutron diffraction measurement.
The model predictions have pinpointed, that the selection of the reflection is crucial for the validity of stresses calculated from the measured elastic lattice strains. The calculations are limited to uniaxial tension with an initially random texture, and in normal measurements with unknown stress state and texture, the complexity of the measurements increases. If the stress state is unknown, there will not be a unique solution to the macroscopic stress state, and the introduction of texture will inherently change the intergranular stresses and strains within the material, and therefore it might not be the 311-reflections, that is the most suitable reflection under all conditions.
AB - The uniaxial deformation of polycrystals are modelled using three incremental rate-insensitive micro-mechanic models; the Taylor model, the Sachs model and Hutchinson’s self-consistent model. The predictions of the two rigid plastic upper- and lower-bound models (Taylor and Sachs) are compared with the predictions of the elastic-plastic self-consistent model. As expected, the results of the self-consistent model is about half-way between the upper- and lower-bound models. The average number of active slip systems is about 3.6 compared to the five active slip systems in the Taylor model and the one active slip system in the Sachs model. The average m-factor is about 2.6 compared to the 3.06 in the Taylor model and the 2.23 in the Sachs model. The predicted rotation pattern of the self-consistent model is closest to the Taylor model, but the orientation distribution of the m-factor is closest to the Sachs model. The influence of the elastic anisotropy is investigated by comparing the self-consistent predictions for aluminium, copper and a hypothetical material (hybrid) with the elastic anisotropy of copper and the Young’s modulus and work hardening behaviour of aluminium. It is concluded, that the effect of the elastic anisotropy is limited to the very early stages of plasticity (εP < ∼0.1%), as the deformation pattern is almost identical for the
three materials at higher strains.
The predictions of the three models are evaluated by neutron diffraction mea-surements of elastic lattice strains in grain sub-sets within the polycrystal. In the evaluation of the rigid plastic Taylor and Sachs models, the ’elastic’ strain is determined as the calculated stress divided by the diffraction elastic constants (cal-culated as the Kr¨oner elastic stiffnesses for the grain sub-sets). The comparison of calculated and measured lattice strains are made for three different materials; alu-minium, copper and austenitic stainless steel. The predictions of the self-consistent model is more accurate and detailed than the predictions of the Taylor and Sachs models, though some discrepancies are noted for some reflections.
The self-consistent model is used to determine the most suitable reflection for technological applications of neutron diffraction, where focus is on the volume av-erage stress state in engineering components. To be able to successfully convert the measured elastic lattice strains for a specific reflection into overall volume average stresses, there must be a linear relation between the lattice strain of the reflection and the overall stress. According to the model predictions the 311-reflection is the most suitable reflection, as it shows the smallest deviations from linearity and thereby also the smallest build-up of residual lattice strains. Below 5% deforma-tion the deviations from linearity and the residual strains are below the normal strain resolution of a neutron diffraction measurement.
The model predictions have pinpointed, that the selection of the reflection is crucial for the validity of stresses calculated from the measured elastic lattice strains. The calculations are limited to uniaxial tension with an initially random texture, and in normal measurements with unknown stress state and texture, the complexity of the measurements increases. If the stress state is unknown, there will not be a unique solution to the macroscopic stress state, and the introduction of texture will inherently change the intergranular stresses and strains within the material, and therefore it might not be the 311-reflections, that is the most suitable reflection under all conditions.
KW - Risø-R-985(EN)
KW - Risø-R-985
M3 - Book
SN - 87–550–2304–5
T3 - Denmark. Forskningscenter Risoe. Risoe-R
BT - Characterisation of polycrystal deformation by numerical modelling and neutron diffraction measurements
PB - Risø National Laboratory
CY - Roskilde
ER -