Peierls stress (also known as the lattice friction stress ) is the force (first described by Rudolf Peierls and modified by Frank Nabarro) needed to move a dislocation within a plane of atoms in the unit cell. The magnitude varies periodically as the dislocation moves within the plane. Peierls stress depends on the size and width of a dislocation and the distance between planes. Because of this, Peierls stress decreases with increasing distance between atomic planes. Yet since the d…

Full article: Peierls barrier characteristic and anomalous strain ...

WebbDOI: 10.1098/rspa.1973.0014 Corpus ID: 137197020; The effect of shear stress on the screw dislocation core structure in body-centred cubic lattices @article{Duesbery1973TheEO, title={The effect of shear stress on the screw dislocation core structure in body-centred cubic lattices}, author={Michael S. Duesbery and … WebbDislocations in a simple cubic lattice. F R N Nabarro 1. Published under licence by IOP Publishing Ltd ... Peierls R 1940 Proc. Phys. Soc. 52 34 . IOPscience Google Scholar Taylor G I 1934 Proc. Roy. Soc. ... Calculating the Peierls energy and Peierls stress from atomistic simulations of screw dislocation dynamics: ... dethleffs camper 2008

Intrinsic freedom of dislocation structures and Peierls stress …

Webbfree from stress? Fig. 1 shows the result of Peierls’s calculations [4] for a simple rectangular lattice. Here, we have taken spacing a between slip planes to be different from the unit slip distance, the Burgers vector b. The early calculations were made for a simple square or cubic lattice with a = b. WebbThe size-dependent plasticity of body centered cubic (bcc) metals is different from face centered cubic (fcc) metals: the size-effect exponent n varies for different bcc metal nanopillars (n¼0.8–1.0 for V, Nb; n¼0.3–0.5 for Ta, Mo, W). This inconsistency is first explained through a simple model based on the temperature-dependent Peierls ... Webbbution comes from the Peierls stress required to move an isolated dislocation in the perfect lattice. Silicon has a diamond cubic lattice with strong bonding and undergoes a brittle-to-ductile transition at approximately 873 K [1]. In this material, dislocations are strongly pinned by the Peierls barriers. dethleffs beduin scandinavia 670 bet