Abstract

The previous concepts of differential geometry, in particular aspects related to incompatibility, shall be applied to the kinematics of firstand second-order (nonlinear) elasto-plasticity. Thereby it shall be noted that the intermediate configuration of first- and second-order elasto-plasticity is incompatible, see Fig. 8.1. Then two cases may be considered: firstly the incompatibility of the intermediate configuration is measured based on the nonintegrability of plastic tensorial quantities; secondly the situation is reversed: the incompatibility of the intermediate configuration is measured based on the non-integrability of elastic tensorial quantities. Thereby distinction can be made between straightforward measures in terms of the non-integrable plastic or elastic distortions (and double-distortions) and more involved measures in terms of the non-integrable plastic or elastic (strain) metrics (and doublemetrics). The former leads to various dislocation density tensors, whereas the latter results in various incompatibility density tensors.

Comprehensive accounts on first- and second-order elasto-plasticity in Euclidean space are provided for the sake of reference at the end of the chapter in two extended supplements.

Keywords

Deformation Gradient Free Energy Density Density Tensor Elastic Distortion Material Time Derivative 
These keywords were added by machine and not by the authors. This process is experimental and the keywords may be updated as the learning algorithm improves.

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Copyright information

© Springer-Verlag Berlin Heidelberg 2015

Authors and Affiliations

  1. 1.University of Erlangen-NurembergErlangenGermany

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