On thermodynamics of wave processes of heat transport

Murashkin, E.V.; Radayev, Y.N.

Авторы: Murashkin E.V., Radayev Y.N.
Сборник: Mechanics for Materials and Technologies
Серия: Advanced Structured Materials
Том: 46
Год издания: 2017
Место издания: Springer
Первая страница: 363
Последняя страница: 376
DOI: 10.1007/978-3-319-56050-2_21
Аннотация: The present paper is devoted to formulations of constitutive equations for the non-linear Green-Naghdi type-III thermoelastic continuum consistent with the principle of thermodynamic (or thermomechanical) orthogonality. Contrary to the original Green-Naghdi model the Lagrange description is employed. The principle of thermodynamic orthogonality originally proposed by Ziegler as a generalization of the Onsager linear irreversible thermodynamics states that the irreversible constituent of thermodynamic flux is orthogonal to the convex dissipative potential level surface in the space of thermodynamic forces for any process of heat transport. The principle of the thermomechanical orthogonality takes its origin from the von Mises maximum principle of the perfect plasticity, where it provides existence of a yield surface, its convexity, and the associated flow rule. Non-linear constitutive laws of heat propagation as of type-III thermoelasticity complying with the principle of thermomechanical orthogonality are discussed. Important for applied thermoelasticity cases covered by type-III theory are studied: GNI/CTE–conventional thermoelasticity based on the Fourier heat conduction law and GNII–dissipationless hyperbolic thermoelasticity. In the latter case the internal entropy production equals zero for any heat transport process having the form of the undamped thermoelastic wave propagating at finite speed.
Добавил в систему: Левитин Александр Леонидович

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