H. Inui et al., TEMPERATURE-DEPENDENCE OF YIELD STRESS, DEFORMATION MODE AND DEFORMATION STRUCTURE IN SINGLE-CRYSTALS OF TIAL (TI-56 AT-PERCENT AL), Philosophical magazine. A. Physics of condensed matter. Structure, defects and mechanical properties, 75(2), 1997, pp. 395-423
The plastic deformation behaviour of single crystals of TiAl with a co
mposition of Ti-56 at.% Al has been studied in compression as a functi
on of crystal orientation in the temperature range from -196 to 1100 d
egrees C. The profile of yield stress-temperature curves for all orien
tations studied can be divided into three temperature regions; the yie
ld stress rapidly decreases with increasing temperature at both low an
d high temperatures and an anomalous increase in yield stress is obser
ved at intermediate temperatures, exhibiting a peak at 700-1000 degree
s C depending on crystal orientation. Both ordinary and [101] superlat
tice slip exhibit an anomalous increase in critical resolved shear str
ess (CRSS). However, the extent of the anomaly associated with the for
mer slip is much smaller than that for the latter slip. The CRSS for [
101] slip depends on crystal orientation. In the anomalous temperature
region, the CRSS exhibits very small strain-rate sensitivity and ther
mal reversibility. Superlattice dislocations with b = [101] in specime
ns deformed in the anomalous temperature region mostly align along the
ir screw orientation and adopt a locked configuration. These features
are very similar to those observed for the anomalous strengthening of
Ni3Al. The CRSS for ordinary slip is considerably larger than that for
[101] superlattice slip at temperatures below 600 degrees C. This res
ults in a limited orientation range for the operation of ordinary slip
. In the anomalous temperature region, the strain-rate sensitivity of
CRSS for ordinary slip is also very small and 1/2[110] dislocations wi
th many cusps are observed to align along their screw orientation The
dislocation mechanisms of the anomaly for ordinary slip may be differe
nt from those for [101] superlattice slip. Above the peak temperature,
[110] slip, twinning and [112] superlattice slip are identified to be
operative. Slip along [110] occurs not only on {111} but also on (001
) and {110), depending on orientation. Twinning and [112] superlattice
slip occur only for limited orientations.