A phenomenological relativistic theory of thermoelastic solids whose equations form a hyperbolic system is proposed. As required by compatibility with irreversible thermodynamics, for the heat flux it is deduced a nonstationary transport equation containing new cross-effect terms so determining the complete system describing the evolution of a thermoelastic solid. Then the theory is extended to the study of Kelvin-Voigt viscoelastic bodies,

A phenomenological relativistic theory of thermoelasticity

PALUMBO, Annunziata
1985-01-01

Abstract

A phenomenological relativistic theory of thermoelastic solids whose equations form a hyperbolic system is proposed. As required by compatibility with irreversible thermodynamics, for the heat flux it is deduced a nonstationary transport equation containing new cross-effect terms so determining the complete system describing the evolution of a thermoelastic solid. Then the theory is extended to the study of Kelvin-Voigt viscoelastic bodies,
1985
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11570/14872
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