Titlebook: Mechanics and Geometry of Enriched Continua; Luis Espath Book 2023 The Editor(s) (if applicable) and The Author(s), under exclusive licens

conservative

rating the important interplay between theory and experiment.This book introduces the fascinating world of plasmonics and physics at the nanoscale, with a focus on simulations and the theoretical aspects of optics and nanotechnology. A research field with numerous applications, plasmonics bridges th

耕種

敵意

怎樣才咆哮

Power Balance, Fields, and HyperfieldsNowadays, it is probably the most prevalent tool when it comes to deriving mechanical theories for enriched continua. However, it was not until the two works by Toupin [15, 16] that . were in focus. According to Edelen [11], Voigt [9] thought and elaborated the idea of nonlocalities to augment the h

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想象

Thermodynamicstulates, we obtain the pointwise version of the entropy imbalance and free-energy imbalance. These imbalances are useful tools to propose thermodynamically consistent constitutive relations. We then present and extend ideas of Larché–Cahn about derivatives on constrained spaces for the case in which

匍匐前進(jìn)

Couplingd fluid materials. In this chapter, based on the Coleman–Noll procedure, we augment the system of equations with appropriate constitutive relations. Moreover, we aim to determine the constitutive equations for certain particular types of couplings between motion and multiple transition layers. That

蘆筍

Environmental Surface Balances and Imbalanceshe surface balances of forces, microforces, torques, and microtorques as well as the surface power balances as similarly proposed by Espath & Calo [32]. Analogous boundary conditions to those presented by Fried & Gurtin [20] are also provided by Espath et al. [33] and Duda et al. [61]. In taking the

vibrant

演繹

Bulk-Surface Dynamicscher, Maass, & Dieterich [62], Goldstein, Miranville, & Schimperna [63], and Knopf, Lam, Liu & Metzger, [64]. As a byproduct, we generalize these theories. These types of dynamic boundary conditions are described by the coupling between the bulk and surface partial differential equations for phase f