The occurrence of dynamic recrystallization in ferritic iron, which is
a typical dynamic recovery-type material, was confirmed in the presen
t study using a Ti-added interstitial-free (IF) steel. The specimens w
ere hot-compressed at various strain rates at various temperatures wit
hin the ferritic region and quenched immediately after compression. Eq
uiaxed grains surrounded by clearly-etched boundaries appeared prefere
ntially near the initial grain boundaries in the small Zener-Hollomon
parameter (Z) deformations. Microtextural analysis by Kikuchiline meas
urements in TEM or EBSP in SEM clearly showed that these equiaxed grai
ns are dynamically recrystallized with both the high angle grain bound
aries and the dislocation substructures inside. The fraction and the s
ize of the dynamically recrystallized grains increased with decreasing
strain rates or increasing deformation temperature, i.e., decreasing
Z. Consequently, the condition where dynamic recrystallization of ferr
ite occurred was expressed as, Z less than or equal to 10(11) s(-1) in
the present material. Nevertheless, despite the occurrence of dynamic
recrystallization, a large stress drop in stress-strain curves was no
t observed. The size of the dynamically recrystallized grains was much
larger than that of the subgrains formed under the same deformation c
ondition, which suggests that the dynamically recrystallized grains gr
ew immediately after they obtained mobile boundaries. The characterist
ics of the dynamic recrystallization of ferrite were the inhomogeneity
of recrystallization as well as the small drop in stress. Some of the
initial grains were hardly recrystallized even in the small-Z deforma
tion, which is presumably due to the initial orientation dependence of
recrystallization in ferrite. The nucleation of dynamic recrystalliza
tion in ferrite was explained an the basis of the introduction of inho
mogeneous deformation microstructure with large local misorientations.