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Variational formulations in continuum mechanics
Author(s) -
Scholle Markus
Publication year - 2011
Publication title -
pamm
Language(s) - English
Resource type - Journals
ISSN - 1617-7061
DOI - 10.1002/pamm.201110336
Subject(s) - noether's theorem , continuum mechanics , lagrangian mechanics , lagrangian , analytical mechanics , variational principle , classical mechanics , variational integrator , hamilton's principle , mathematics , analytical dynamics , finite element method , calculus (dental) , physics , equations of motion , quantum mechanics , thermodynamics , medicine , integrator , voltage , quantum dynamics , quantum , dentistry
Variational formulations of the governing equations are of great interest in continuum mechanics: on the one hand a deeper theoretical insight in the respective system is possible, on the other hand variational formulations give rise for the development of semi‐analytical and numerical methods like Ritz' direct method, especially FEM. Despite these benefits, there are many problems in continuum mechanics for which a variational principle is not available. The reason for this is that in contrast to conservative Newtonian mechanics, where the Lagrangian is given as difference between kinetic and potential energy, no generally valid construction rule for the Lagrangian has been established in the past. In this paper a construction rule is developed, on the Galilei‐invariance of the system, leading to a general scheme for Lagrangians the individual analytical form of which is determined by an inverse treatment of Noether's theorem. This procedure is demonstrated for an elastically deforming body. (© 2011 Wiley‐VCH Verlag GmbH & Co. KGaA, Weinheim)