A classical way to formulate in three dimensions the phenomena identified in one dimension as described for damage in Chapter 1 is to postulate the existence of energy potentials from which one can derive the state laws and the kinetic constitutive equations. In the thermodynamics of irreversible processes, two potentials are introduced and identified within the framework of the “State Kinetic Coupling theory” (J. Lemaitre, D. Marquis, 1988).
CITATION STYLE
Lemaitre, J. (1992). Thermodynamics and Micromechanics of Damage. In A Course on Damage Mechanics (pp. 39–94). Springer Berlin Heidelberg. https://doi.org/10.1007/978-3-662-02761-5_2
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