Abstract
By consistently applying the concepts of Classical Thermodynamics, a general entropy equation is derived which applies to every continuous system both in equilibrium and in non-equilibrium conditions. The established equation reduces to the classical entropy equation when equilibrium conditions are considered. Outside thermodynamic equilibrium, however, it generalizes the classical equation and affords a precise relation to measure the time-rate of entropy. Being independent of the other field equations currently introduced in the theory, the present equation enables to determine the production of non-thermal energy that in non-equilibrium conditions can result from the transformation of part of the heat that flows from the hotter to the colder parts of the system. Such a production of non-thermal energy is ignored by the current theories, since they lack the appropriate equation to determine it.
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References
I.S.Sokolnikoff & R.M.Redheffer: Mathematics of Physics and Modern Engineering. McGraw-Hill, New York 1966.
J.D. Fast: Entropy (2nd ed.). Macmillan, New York 1970.
A. Paglietti: On the Mathematical Formulation of the First Principle of Thermodynamics for Non-Uniform Temperature Processes. Ann. Inst. Henri Poincaré 30 A, 61–82 (1979).
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© 1984 Springer-Verlag
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Paglietti, A. (1984). The equation which governs irreversibility in continuum mechanics. In: Casas-Vázquez, J., Jou, D., Lebon, G. (eds) Recent Developments in Nonequilibrium Thermodynamics. Lecture Notes in Physics, vol 199. Springer, Berlin, Heidelberg. https://doi.org/10.1007/BFb0016055
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DOI: https://doi.org/10.1007/BFb0016055
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