Work hardening in heterogeneous alloys - A microstructural approach based on three internal state variables

Abstract A new work-hardening model for homogeneous and heterogeneous cell-forming alloys is introduced. It distinguishes three internal state variables in terms of three categories of dislocations: mobile dislocations, immobile dislocations in the cell interiors and immobile dislocations in the cell walls. For each dislocation population an evolution law is derived taking into account dislocation generation, annihilation and storage by dipole and lock formation. In particular, these rate equations take into account the number of active glide systems and, thus, introduce texture in the model in addition to the Taylor factor. Microstructure is represented by the dislocation cell structure as well as second-phase particles, which may undergo changes by precipitation and Ostwald ripening. Interaction of mobile dislocations with the microstructure is taken into account through an effective slip length of the mobile dislocations. For the same set of parameters, the predictions are in excellent agreement with measured stress–strain curves of both a precipitation-hardened aluminium alloy (Al–4.16 wt% Cu–1.37 wt% Mg, AlCuMg2) and a precipitation-free model alloy (Al–0.35 wt% Cu–0.25 wt% Mg), the composition of which corresponds to the matrix of the two-phase alloy.

[1]  Y. Estrin,et al.  Implementation of Precipitation and Ripening of Second-Phase Particles in the Constitutive Modelling of Creep , 1998 .

[2]  Yuri Estrin,et al.  A unified phenomenological description of work hardening and creep based on one-parameter models , 1984 .

[3]  Clarence Zener,et al.  Interference of Growing Spherical Precipitate Particles , 1950 .

[4]  Laszlo S. Toth,et al.  A dislocation-based model for all hardening stages in large strain deformation , 1998 .

[5]  I. Lifshitz,et al.  The kinetics of precipitation from supersaturated solid solutions , 1961 .

[6]  F. Prinz,et al.  The evolution of plastic resistance in large strain plastic flow of single phase subgrain forming metals , 1984 .

[7]  H. Mughrabi,et al.  Annihilation of dislocations during tensile and cyclic deformation and limits of dislocation densities , 1979 .

[8]  T. Abe Deformation of Polycrystalline Metal Composed of Anisotropic Crystals Having Linear Stress-Strain Relation , 1969 .

[9]  A. Granato,et al.  Entropy Factors for Thermally Activated Unpinning of Dislocations , 1964 .

[10]  A. Argon,et al.  Dislocation theory of steady state deformation and its approach in creep and dynamic tests , 1987 .

[11]  U. F. Kocks,et al.  The relation between macroscopic and microscopic strain hardening in F.C.C. polycrystals , 1984 .

[12]  H. Mughrabi A two-parameter description of heterogeneous dislocation distributions in deformed metal crystals , 1987 .

[13]  U. F. Kocks,et al.  Kinetics of flow and strain-hardening☆ , 1981 .

[14]  P. Hähner,et al.  The Dislocation Microstructure of Cyclically Deformed Nickel Single Crystals at Different Temperatures , 1997 .

[15]  H. Mughrabi,et al.  Dislocation wall and cell structures and long-range internal stresses in deformed metal crystals , 1983 .