Hysteretic Systems with Internal Variables

Hysteretic rate-independent constitutive laws are introduced within the framework of continuum thermodynamics with internal variables and revisited using concepts and arguments related to dynamical system theory. The evolution of internal variables is formulated either by a system of differential equations or by the associated phase flow. The restrictions implied by rate independence and thermodynamics are pointed out. Within this framework, the class of models with Masing hysteretic rules and Bouc endochronic relations are reviewed, and notions such as irreversibility, noninvertibility, and memory effects are discussed having recourse to different choices of internal variables. By introducing plastic strain as the internal variable, thermodynamic admissibility is proved for both models. However, while the processes with Masing rules exhibit a limited memory and are therefore noninvertible, the processes based on Bouc models are shown to have full memory and to be invertible though irreversible.

[1]  J. Mander,et al.  Theoretical stress strain model for confined concrete , 1988 .

[2]  P. C. Jennings Periodic Response of a General Yielding Structure , 1964 .

[3]  Zdenek P. Bažant,et al.  ENDOCHRONIC INELASTICITY AND INCREMENTAL PLASTICITY , 1978 .

[4]  Quoc Son Nguyen,et al.  Sur les matériaux standard généralisés , 1975 .

[5]  G. Masing,et al.  Eigenspannungen und Verfestigung beim Messing , 1926 .

[6]  Satya N. Atluri,et al.  Internal time, general internal variable, and multi-yield-surface theories of plasticity and creep: A unification of concepts , 1986 .

[7]  Mayergoyz,et al.  Mathematical models of hysteresis. , 1986, Physical review letters.

[8]  M. Gurtin,et al.  Thermodynamics with Internal State Variables , 1967 .

[9]  Y. Wen Method for Random Vibration of Hysteretic Systems , 1976 .

[10]  Dusan Krajcinovic,et al.  Preisach model and hysteretic behaviour of ductile materials , 1993 .

[11]  Paolo Nistri,et al.  Mathematical Models for Hysteresis , 1993, SIAM Rev..

[12]  A. Nappi,et al.  An internal variable formulation for perfectly plastic and linear hardering relations in plasticity , 1990 .

[13]  J. Chaboche Constitutive equations for cyclic plasticity and cyclic viscoplasticity , 1989 .

[14]  Matti Ristinmaa,et al.  Thermodynamic formulation of plastic work hardening materials , 1999 .

[15]  D. Capecchi Asymptotic motions and stability of the elastoplastic oscillator studied via maps , 1993 .

[16]  J. Bardet Scaled Memory Description of Hysteretic Material Behavior , 1996 .

[17]  J. Chaboche,et al.  Mechanics of solid materials: Viscoplasticity , 1990 .

[18]  Naser Mostaghel,et al.  Analytical Description of Pinching, Degrading Hysteretic Systems , 1999 .

[19]  K. Valanis,et al.  FUNDAMENTAL CONSEQUENCES OF A NEW INTRINSIC TIME MEASURE-PLASTICITY AS A LIMIT OF THE ENDOCHRONIC THEORY , 1980 .

[20]  I. Mayergoyz The Classical Preisach Model of Hysteresis , 1991 .

[21]  Jean-Louis Chaboche,et al.  Mechanics of Solid Materials , 1990 .

[22]  H. J. Sauer,et al.  Engineering thermodynamics, 2nd Ed , 1985 .

[23]  J. Chaboche,et al.  Mechanics of Solid Materials , 1990 .

[24]  Matti Ristinmaa,et al.  Cyclic plasticity model using one yield surface only , 1995 .

[25]  Zenon Mróz,et al.  On the description of anisotropic workhardening , 1967 .

[26]  Percy Williams Bridgman,et al.  The Nature of Thermodynamics , 1941 .

[27]  J. Rice,et al.  PARADOXES IN THE APPLICATION OF THERMODYNAMICS TO STRAINED SOLIDS. , 1969 .

[28]  Michael N. Fardis,et al.  Monotonic and Cyclic Constitutive Law for Concrete , 1983 .

[29]  W. Iwan A Distributed-Element Model for Hysteresis and Its Steady-State Dynamic Response , 1966 .