Harper-Dorn creep in Al was investigated under the condition of large strai
ns (more than 0.1). In performing the investigation, two Al grades were cre
ep tested at 923 K. The first grade is of 99.9995% purity (99.9995 Al) wher
eas the second grade is of 99.99% purity (99.99 Al). The results show that
99.99 Al, unlike 99.9995 Al, does not exhibit the Harper-Dorn creep at low
stresses: and that the creep curves associated with Harper-Dorn creep in 99
.9995 Al exhibit regular, periodic accelerations. An examination of the sub
structure developed during creep reveals that the details of the substructu
re in 99.99 Al are significantly different from those characterizing Harper
-Dorn creep in 99.9995 Al. In 99.99 Al, an extensive, regular array of equi
axed subgrains is formed. By contrast, in 99.9995 Al, a wide range of subst
ructural features including new grains, boundaries with high and low disloc
ation densities on opposite sides of the boundary, and localized regions of
very high dislocation density, are observed. Consideration of the present
data leads to three important findings. First, dynamic recovery is the domi
nant restoration mechanism during the creep of 99.99 Al, while dynamic recr
ystallization is the dominant restoration mechanism during the creep of 99.
9995 Al. Second, the occurrence of Harper-Dom creep in Al requires that two
conditions be satisfied: high purity Al and very low dislocation density i
n the annealed samples (10(3)-3X10(4) cm(-2)). Third, while the results ver
ify the Newtonian nature of Harper-Dom creep at small strains (less than 0.
01), they indicate that under the condition of large strains (more than 0.1
), the stress exponent is more than 2. (C) 2001 Acta Materialia Inc. Publis
hed by Elsevier Science Ltd. All rights reserved.