2010
DOI: 10.1016/j.ijengsci.2010.07.011
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On material velocities and non-locality in the thermo-mechanics of continua

Abstract: a b s t r a c tFollowing is a discussion of several issues surrounding the continuum modeling of discrete particulate systems, particularly the uncertainty in the definition of continuum-level material particles and velocities. The work is motivated in part by various proposals for the introduction of supplemental velocity fields into the thermo-mechanics of single-component fluids. A review and modification are given of the relevant continuum field equations, based on the Eulerian rather than the conventional… Show more

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Cited by 11 publications
(13 citation statements)
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“…With no attempt to resolve that problem, the present note is focused on a source-flux construct introduced in [2] 1 . This construct establishes a fairly direct connection between Newton's and Cauchy's laws and provides an expression for Cauchy stress suggested by the statistical mechanics of point-particles [4]. Furthermore, it appears to offer a useful mathematical foundation for the "peridynamics" of Stilling and coworkers [5].…”
Section: Introductionmentioning
confidence: 79%
“…With no attempt to resolve that problem, the present note is focused on a source-flux construct introduced in [2] 1 . This construct establishes a fairly direct connection between Newton's and Cauchy's laws and provides an expression for Cauchy stress suggested by the statistical mechanics of point-particles [4]. Furthermore, it appears to offer a useful mathematical foundation for the "peridynamics" of Stilling and coworkers [5].…”
Section: Introductionmentioning
confidence: 79%
“…It is plausible that the simple-material model employed here will always allow a certain latitude in such definitions (cf. [14]). …”
Section: Balance Equations and Thermodynamic Frameworkmentioning
confidence: 99%
“…Based on his view of thermo-electricity as irreversible, [29] represents the linear theory by means of his phenomenological relations for forces and fluxes, such as those in (14), by…”
Section: Thermodynamic Orthogonality and The Modification Of Onsager'mentioning
confidence: 99%
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“…For the present purposes, we consider the case of an isotropic conductor with forces and fluxes given by (14), so that − ∇φ e = y e − cĵ e + N eSĵS + R ee j e + R eS j S , and …”
Section: Thermodynamic Orthogonality and The Modification Of Onsager'mentioning
confidence: 99%