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Appendix G - Stress from electronic structure

Published online by Cambridge University Press:  05 June 2012

Richard M. Martin
Affiliation:
University of Illinois, Urbana-Champaign
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Summary

Summary

The subject of this appendix is the macroscopic stress that enters mechanical properties of matter in the form of stress–strain relations. The stress tensor is the generalization of pressure to all the independent components of dilation and shear, and the “stress theorem” is the generalization of the virial theorem for scalar pressure to all components of the stress tensor. In condensed matter, the state of the system is specified by the forces on each atom and the stress, which is an independent variable. The conditions for equilibrium are: (1) that the total force vanishes on each atom, and (2) that the macroscopic stress equals the externally applied stress.

Macroscopic stress and strain

Stress and strain are important concepts in characterizing the states of condensed matter [177, 721, 722, 890]. A body is in a state of stress if it is acted upon by external forces or if one part of the body exerts forces upon another part. If we consider two types of forces as illustrated in Fig. G.1: those acting interior to a volume element and those that act upon (or through) the surface of the element due to the surrounding material, which are shown as arrows in the figure. The latter forces (per unit area) are the stresses transmitted throughout the interior of the volume. Since these forces balance on any surface in equilibrium, the stress can be determined in terms of only the intrinsic internal forces; i.e. stress is an intrinsic property of a material in a given state.

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Electronic Structure
Basic Theory and Practical Methods
, pp. 512 - 518
Publisher: Cambridge University Press
Print publication year: 2004

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