VISCOPLASTIC BEHAVIOR AND MODELIZATION OF A RECRYSTALLIZED ZIRCALOY-4ALLOY UNDER UNIAXIAL AND MULTIAXIAL LOADINGS

Citation
P. Delobelle et P. Robinet, VISCOPLASTIC BEHAVIOR AND MODELIZATION OF A RECRYSTALLIZED ZIRCALOY-4ALLOY UNDER UNIAXIAL AND MULTIAXIAL LOADINGS, Journal de physique. III, 4(8), 1994, pp. 1347-1382
Citations number
47
Categorie Soggetti
Material Science","Phsycs, Fluid & Plasmas","Physics, Applied
Journal title
ISSN journal
11554320
Volume
4
Issue
8
Year of publication
1994
Pages
1347 - 1382
Database
ISI
SICI code
1155-4320(1994)4:8<1347:VBAMOA>2.0.ZU;2-8
Abstract
The results of experiment performed on a recrystallized zircaloy 4 all oy in the intermediate temperature domain 20 less-than-or-equal-to T l ess-than-or-equal-to 400-degrees-C are presented. To characterize the anisotropy, especially at 350-degrees-C, the tests were made under bot h monotonic and cyclic uni- and bidirectional loadings, i.e. tension-c ompression, tension-torsion and tension-internal pressure tests. The d ifferent anisotropy coefficients and especially [GRAPHICS] seem to be temperature independent. An important feature of the behavior of this alloy in the neighbourhood of 300-degrees-C is attributed to the dislo cations-point defects interactions (dynamic strain aging), phenomena o ften observed in the solid solutions. For the 2D cyclic non proportion al loadings it is shown that a weak supplementary hardening appears, w hich is a function of the degree of the phase lag. We propose to parti cularize and to apply a unified viscoplastic model with internal varia bles to the considered alloy, as the model as already been developed a nd identified elsewhere for other isotropic materials. From a general point of view the introduction of the anisotropy in the model is made by four tensors of rank 4; [M] is assigned to the flow directions, [N] to the linear parts of the kinematical hardening variables and [Q], [ R] respectively to the dynamic and static recoveries of these tensoria l variables. This phenomenological formulation leads to a correct repr esentation of the set of the experimental results presented at 350-deg rees-C, which provides an a posteriori confirmation of the formalism u sed.