Abstract
Isothermal rheological behavior is described by free energyφ(ε,p) and potentialΩ(p,P) with\(\dot p = \partial \Omega /\partial P,P = - \partial \phi /\partial P,\sigma = \partial \phi /\partial \varepsilon \). A number of usual rheological effects can be explained with only one or two (scalar or tensorial) internal state variablesp.
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Weber, J.D., Eberhardt, A. Internal state variables and normality in viscoplastic flow. Rheol Acta 21, 403–405 (1982). https://doi.org/10.1007/BF01534302
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DOI: https://doi.org/10.1007/BF01534302