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In certain ranges of parameters, grain boundary dislocations undergo splitting transformations followed by emission of partial dislocations from high-angle boundaries into adjacent grain interiors.
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We consider such transformations as decay of low-angle grain boundaries, bowing of high-angle grain boundaries, and emission of partial dislocations by grain boundaries in deformed nanocrystalline materials.
The sequential emission of partials results in the observation of full dislocations and twinning.
It is found to be achieved by the emission of 16⟨111⟩ partial dislocations on the {1 1 2} slip plane.
In 〈1 1 0〉 columnar grains, the deformation is dominated by twinning, which nucleates primarily from the grain boundaries by successive emission of twinning partials and thickens by jog nucleation in the grain interiors.
The method is based on modelling front-face fluorescence emission spectra by means of partial least squares class modelling (PLS-CM).
Based on the above, the threshold normal scratching load for the emission of a partial dislocation is determined by means of the energy criterion.
McKenzie's partial realism — her astonishingly intimate and tactile proximity to her characters — is balanced by an element of partial transcendence.
The emission of a Shockley partial from one step of Ni tip will result in stress release, while unreleased high stresses near other steps tend to trigger the emission of Shockley partials more easily.
After thermally activated emission of the first partial dislocation, there is then a competition between two other thermally activated processes: twinning and full dislocation emission.
This proceeds by the emission of a special type of dislocation shear loop, which can expand as a partial or perfect dislocation, evolve into a prismatic loop through reaction, or develop into twins.
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