Abstract
The thermomechanics of electromagnetic continua is a branch of energetics which deals with a unification of continuum mechanics and electrodynamics of material media under the umbrella of general thermodynamics. This obviously goes in the direction indicated by the great P.Duhem early in this century (Duhem, 1911, 1914/1954). This ambitious, somewhat Aristotelian-like, scheme also adds one difficulty to the other. In effect, in addition to the cumbersome and rather heavy framework of nonlinear continuum mechanics (such as exposed in modern treatises, e.g., Truesdell and Toupin, I960, Truesdell and Noll, 1965; Eringen 1980, Eringen 1971–1976), one has to consider electromagnet ism (e.g., Jackson, 1962) and then combine them (in an nonlinear manner; this is not a linear superposition) in the harmonious frame of thermodynamics. Some of the difficulties met have to do with the electrodynamics of moving bodies (writing of fields and equations in appropriate frames), while others relate to the introduction of a general deformation field (“material” writing of fields). Finally, there are difficulties connected with the inherent complexity of some of the behaviors (e.g., hysteresis), and even more so, the non-unique thermodynamical framework at the time of writing!
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Maugin, G.A. (1993). Non-Equilibrium Thermodynamics of Electromagnetic Solids. In: Muschik, W. (eds) Non-Equilibrium Thermodynamics with Application to Solids. International Centre for Mechanical Sciences, vol 336. Springer, Vienna. https://doi.org/10.1007/978-3-7091-4321-6_4
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DOI: https://doi.org/10.1007/978-3-7091-4321-6_4
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