1986
DOI: 10.1063/1.527231
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Virtual power and thermodynamics for electromagnetic continua with interfaces

Abstract: This paper presents a systematic and rational formulation of the electromagnetic theory of deformable and fluent bodies swept out by singular surfaces that may carry their own thermodynamics (interfaces). The treatment is based on the principle of virtual power for finite velocity fields, which is so formulated that, when combined, for real velocity fields, with the first principle of thermodynamics in global form, it yields directly the so-called energy theorem both in the bulk and at the singular surface. Th… Show more

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Cited by 26 publications
(9 citation statements)
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“…[8]) and starts from the Principle of Least Action or from the Principle of Virtual Works and has been more recently been applied in different contexts (see e.g. [23,24,40,41,[63][64][65].…”
Section: Second Gradient Continua Are a Non-trivial Generalization Ofmentioning
confidence: 99%
“…[8]) and starts from the Principle of Least Action or from the Principle of Virtual Works and has been more recently been applied in different contexts (see e.g. [23,24,40,41,[63][64][65].…”
Section: Second Gradient Continua Are a Non-trivial Generalization Ofmentioning
confidence: 99%
“…[131] and has been always considered by those French mechanicians (see e.g. [59], [60], [61], [62], [110], [29], [30], [84], [87], [88] ) who follow the ideas of D'Alembert and Lagrange as the basic concept in mechanics. More recently we can witness to a revival of the Principle of Virtual Powers: many authors (see e.g.…”
Section: Introductionmentioning
confidence: 99%
“…The method of virtual power (accounting for the first point) is certainly the method most pregnant of generalizations to complex models. This is fully illustrated by the cases of electroelastic semiconductors and media with interfaces (Daher and Maugin, [34]- [36]) where there are necessarily present dissipative effects. It would also provide a safe way to build a rational model when the deformation field itself is specialized to those found in essentially two-dimensional (plates, shells) or one-dimensional (rods) structures.…”
Section: Comments and Conclusionmentioning
confidence: 99%
“…34) at any regular point in V . The set (4.32)-(4.34) is equivalent to the set formed by (4.1) and (4.2) although with a different decomposition of the symmetric part of t. Here,…”
mentioning
confidence: 98%