Abstract

Single crystals of Cu-10.5-at.%-Al alloys with the [\ifmmode\bar\else\textasciimacron\fi{}12\ifmmode\bar\else\textasciimacron\fi{}5] {1\ifmmode\bar\else\textasciimacron\fi{}2\ifmmode\bar\else\textasciimacron\fi{}1} {\ifmmode\bar\else\textasciimacron\fi{}2\ifmmode\bar\else\textasciimacron\fi{}10} orientation experience discontinuous elongations under tensile stress at 4.2 \ifmmode^\circ\else\textdegree\fi{}K. The processes are initiated at a resolved shear stress of 3.01 Kg ${\mathrm{mm}}^{\ensuremath{-}2}$ on the {\ifmmode\bar\else\textasciimacron\fi{}1\ifmmode\bar\else\textasciimacron\fi{}11} 101> glide system. They introduce slip bands with a mean width of 47 $\overline{\mathrm{m}}$ and produce a mean integrated shear displacement of 5.7 \ensuremath{\mu}m corresponding to the motion of 3.5 \ifmmode\times\else\texttimes\fi{} ${10}^{4}$ dislocations in near-edge orientations. Simultaneous elongation-time and stress-time records have been obtained with capacitive and ceramic piezoelectric transducers located near the site of relaxation in the cryostat. After an initial interval of 30 $\overline{\mathrm{s}}$ec, elongation proceeds at a constant rate of 1.1 cm ${\mathrm{sec}}^{\ensuremath{-}1}$ for 400 \ensuremath{\mu}sec. During this process, the shear stress is 0.024 kg ${\mathrm{mm}}^{\ensuremath{-}2}$ lower than at the onset of relaxation. The rate of elongation, which is determined by the mechanical properties of the system, gives a value for the product of the number and velocity of the moving dislocations of 3.76 \ifmmode\times\else\texttimes\fi{} ${10}^{7}$ cm ${\mathrm{sec}}^{\ensuremath{-}1}$. Observations of the surface topography of the slip bands and of the dislocation-etch-pit distributions within them are used to establish a model for the sequence of events during the relaxation process. With this model, the mean velocity of the dislocations is found to be 2.1 \ifmmode\times\else\texttimes\fi{} ${10}^{4}$ cm ${\mathrm{sec}}^{\ensuremath{-}1}$ at a resolved shear stress of 2.98 kg ${\mathrm{mm}}^{\ensuremath{-}2}$ and a local steady-state temperature of 17 \ifmmode^\circ\else\textdegree\fi{}K.

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