On the dynamically stored energy of cold work in pure single crystal and polycrystalline copper

2012 ◽  
Vol 60 (9) ◽  
pp. 3719-3728 ◽  
Author(s):  
D. Rittel ◽  
A.A. Kidane ◽  
M. Alkhader ◽  
A. Venkert ◽  
P. Landau ◽  
...  
1969 ◽  
Vol 47 (12) ◽  
pp. 1253-1255 ◽  
Author(s):  
Douglas L. Martin

Within the error limits of the measurement there is no difference between the specific heats of pure single-crystal and pure polycrystalline copper below 3 °K. It is suggested that previous observation of such a difference was because the single crystal had not been degassed before measurement.


The evolution of stored energy during heating for specimens of deformed α-brass is quite different from that previously observed for pure metals; the stored energy is much larger and at least three stages of evolution exist. These have been studied for deformation in torsion and tension and the results correlated with measurements of electrical resistivity, density and hardness. The large release of energy in the first two stages is attributed mainly to the return of order destroyed by plastic deformation; the degree of disorder after heavy cold work is much greater than after quenching (part II). However, slight deformation (10% tension) increases the degree of order slightly. The first stage of energy release, below 120 °C, is probably due to rapid reordering assisted by vacancies created during deformation. The second stage represents the bulk of the reordering and some recovery involving rearrangement and annihilation of dislocations. The deformed specimens are probably strain-aged and thus recovery is accompanied by the dispersal of atmospheres of zinc which increases resistivity and decreases density, to some extent counteracting the effects of recovery. The balance of these three processes in stage 2 causes complex behaviour, the magnitude and even the sign of some changes in properties varies with the deformation. Reordering is complete before the beginning of the third stage of further recovery and recrystallization, in which dispersal of atmospheres is again important. Comparison of measurements of energy, resistivity and density suggests that the high concentration of stacking faults contributes to the resistivity. Anneal hardening is observed for the higher deformations and the maximum hardness coincides with the maximum degree of order.


2006 ◽  
Vol 427 (1-2) ◽  
pp. 301-305 ◽  
Author(s):  
S.F. Castro ◽  
J. Gallego ◽  
F.J.G. Landgraf ◽  
H.-J. Kestenbach

2012 ◽  
Vol 715-716 ◽  
pp. 758-763 ◽  
Author(s):  
Jacek Tarasiuk ◽  
Brigitte Bacroix ◽  
Krzysztof Wierzbanowski ◽  
Sebastian Wroński ◽  
P. Gerber

Eight years ago recrystallization of OFE (oxygen-free electronic) copper was examined in detail using various techniques. In 2008 exactly the same material was measured using EBSD microscopy. The deformed state and fully recrystallized state have been analyzed and compared with data obtained eight years ago. The stored energy (SE) estimated by Image Quality (IQ) analysis was compared in these two cases. A significant amount of recovery took place in the sample, but only in some texture components. Some others present more or less the same SE as eight years ago. The textures of recrystallized samples were compared. We observed that the difference in SE distribution between the two deformed state has an influence on the final textures after recrystallization. Our study confirms the hypothesis that if a grain (orientation) has distinctly lower SE than other orientations - it has the highest growth preference (threshold hypothesis). Such grains (orientations) are dominant in the recrystallization texture.


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