Non-Riemannian geometry and the theory of lattice imperfections
dc.contributor.author | Povstenko, Jurij | pl_PL |
dc.date.accessioned | 2019-09-06T10:45:11Z | |
dc.date.available | 2019-09-06T10:45:11Z | |
dc.date.issued | 2003 | |
dc.identifier.citation | Annales Academiae Paedagogicae Cracoviensis. 16, Studia Mathematica 3 (2003), s. [197]-200 | pl_PL |
dc.identifier.uri | http://hdl.handle.net/11716/5754 | |
dc.description.abstract | Creation and development of continuum theory of imperfections of a crystal structure (dislocations and disclinations) is closely associated with ideas and methods of non-Euclidean and non-Riemannian geometry. In the geometrical interpretation of the continuum theory of lattice defects Kondo [1] and Bilbi et at. [2] identified the Cartan torsion tensor with the dislocation density, Anthony [3] used the Riemann-Christoffcl curvature tensor to describe disclination. The above-mentioned authors considered static imperfections. To give a differential- geometrical interpretation of the imperfection kinematics it is necessary to take time into consideration. We discuss a three-dimensional space of affine connection with time as a parameter and introduce the material time derivative using the “time-connection" tensor. | en_EN |
dc.language.iso | en | pl_PL |
dc.title | Non-Riemannian geometry and the theory of lattice imperfections | en_EN |
dc.type | Article | pl_PL |