We identify in this paper that stress relaxation in metals is a “strain-free” process. The corresponding self-consistent relations between the strain, and stress variations of a grain and of its aggregate are derived from Eshelby’s solution of an ellipsoidal inclusion. It is shown that, under such a process, the strain in a more favorably oriented grain continues to rise and that its stress decreases more drastically than that of the aggregate; conversely, for a less favorably oriented grain, its strain decreases and its stress relaxes less. The self-consistent relations are supplemented with a temperature-dependent, physically consistent constitutive equation for the slip system. Such an equation enables us to determine the single crystal constants at one temperature from the polycrystal data at another temperature; it also makes the self-consistent scheme applicable to the varying-temperature environment. The established theory was finally applied to predict the relaxation behavior of an RR-59 aluminum alloy under combined stress; the results showed reasonably good agreement with the experimental data.
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December 1981
Research Papers
A Self-Consistent Scheme for the Relaxation Behavior of Metals
G. J. Weng
G. J. Weng
Department of Mechanics and Materials Science, Rutgers University, New Brunswick, N.J. 08903
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G. J. Weng
Department of Mechanics and Materials Science, Rutgers University, New Brunswick, N.J. 08903
J. Appl. Mech. Dec 1981, 48(4): 779-784 (6 pages)
Published Online: December 1, 1981
Article history
Received:
November 1, 1980
Revised:
March 1, 1981
Online:
July 21, 2009
Citation
Weng, G. J. (December 1, 1981). "A Self-Consistent Scheme for the Relaxation Behavior of Metals." ASME. J. Appl. Mech. December 1981; 48(4): 779–784. https://doi.org/10.1115/1.3157733
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