1983
DOI: 10.1016/0378-4371(83)90196-6
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On the Lagrangian formulation of continuum mechanics

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1984
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Cited by 11 publications
(16 citation statements)
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“…In the spirit of several prior investigators [2,[11][12][13][14][15][25][26][27], we subject the action (1) to a set of transformations of both independent and dependent fields:…”
Section: Balance Lawsmentioning
confidence: 99%
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“…In the spirit of several prior investigators [2,[11][12][13][14][15][25][26][27], we subject the action (1) to a set of transformations of both independent and dependent fields:…”
Section: Balance Lawsmentioning
confidence: 99%
“…Because Eqs. (24)(25)(26) arise from a continuous shift in material coordinates made possible by a continuum description of a body, they have no analogue in a discrete set of particles [11,13].…”
Section: Simple Elastic Solidmentioning
confidence: 99%
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“…The differential operator (d/dt) denotes the total time derivative at fixed X. By following the treatment of Golebiewska and Herrmann [21], evaluate the total gradient of L and write…”
Section: Dynamicsmentioning
confidence: 99%
“…This tensor was named the Maxwell tensor of elasticity by Eshelby in 1951, in the context of linear elasticity [18]. In the literature that is concerned with the configurational material forces, b is currently known as the Eshelby tensor [4][5][6][7][8][19][20][21].…”
Section: Elasticitymentioning
confidence: 99%