Materials Science Forum
Vol. 570
Vol. 570
Materials Science Forum
Vol. 569
Vol. 569
Materials Science Forum
Vols. 567-568
Vols. 567-568
Materials Science Forum
Vol. 566
Vol. 566
Materials Science Forum
Vols. 561-565
Vols. 561-565
Materials Science Forum
Vol. 560
Vol. 560
Materials Science Forum
Vols. 558-559
Vols. 558-559
Materials Science Forum
Vols. 556-557
Vols. 556-557
Materials Science Forum
Vol. 555
Vol. 555
Materials Science Forum
Vol. 554
Vol. 554
Materials Science Forum
Vol. 553
Vol. 553
Materials Science Forum
Vols. 551-552
Vols. 551-552
Materials Science Forum
Vol. 550
Vol. 550
Materials Science Forum Vols. 558-559
Paper Title Page
Abstract: Effects of the crystallographic misorientation across boundaries between recrystallising grains and
the neighbouring deformed matrices are discussed and exemplified by recrystallisation
investigations of fcc metals. Classic misorientation observations are reviewed in the introduction,
whereas the main parts of the paper focuses on two special boundary migration phenomena
observed by in-situ recrystallisation experiments; namely protrusions and facets.
85
Abstract: The drawing textures of aluminum, copper, gold, silver, and Cu-7.3% Al bronze wires
are approximated by major <111>+minor <100>, except silver wire, which can have the <100>
texture at extremely high reductions. The <111> component in the drawing textures of aluminum,
copper, gold, and silver transform to the <100> component after recrystallization. On the other
hand, the <111> deformation texture of the Cu-7.3% Al bronze wire, which has very low stackingfault-
energy, remains unchanged after recrystallization. The <100> + <111> recrystallization
textures change to the <111> texture after abnormal grain growth. The Brass component
{110}<112> in rolling textures of high stacking-fault-energy metals such as aluminum, copper, Cu-
16% Mn, and Cu-1% P changes to the Goss orientation {110}<001> after recrystallization.
However, the Brass orientation in rolling textures of low stacking-fault-energy fcc metals such as
brass and silver appears to change to an orientation approximated by the {236}<385> orientation
after annealing. The texture changes are discussed based on the strain-energy-release-maximization
model for medium to high stacking-fault-energy metals and on grain growth for low stacking-fault
energy metals.
93
Abstract: This paper showed an example of the phenomena that a strong deformed texture does not
change after the annealing process in steels. An Fe – 22%Cr – 3%Ni ferritic stainless steel was
processed by bar rolling/swaging to a total strain of 4.4 at an ambient temperature, and its annealing
behaviour was studied in a temperature range of 400 ~ 700oC. The deformed sample showed a grain
size of 200nm, a fraction of high-angle boundary (HAB) of about 0.6, and a strong fiber texture of
<110>{uvw}. This texture showed very little change after annealing which was characterised by the
development of continuous recrystallization involving recovery processes and followed by a normal
grain growth. On the other hand, by annealing a sample that was deformed to total strain of 2.0
containing rather fine grains (270nm) but without a large enough fraction of HAB (0.3), a
discontinuous recrystallization took place, and its deformed texture changed considerably.
101
Abstract: The effects of alloying elements and impurities on the microstructure and
properties of metals and alloys are important. Understanding of these effects may help
to control and produce products with desired properties at lower cost. In the present
work the effects of Al, Si and Mn on the recrystallization behavior, hardness and
microstructural changes of an Fe- containing brass during annealing were studied. The
results show that alloying elements strongly affect recrystallization kinetics and
resulted finer microstructures. Hardness variations during annealing are consistent with
microstructural observations and the presence of alloying elements. All elements slow
down recrystallization progress and increase resulted hardness values. The resulted
microstructures in the presence of alloying elements are much finer than that of plain
70B brass. It was concluded that the present alloying elements affect the
recrystallization behavior of 70B brass in a similar manner. Their mechanism of
interactions is solute drag effect and their effects sum up when they present together.
107
Abstract: Several studies have shown that recrystallization of cold rolled martensite results in low
carbon steels with very fine microstructures. Correspondingly, these materials exhibit promising
combinations of strength and elongation. Most of the work on this processing route has focused on
low carbon steels (0.1-0.2wt% carbon) where the interstitial content may play an important role in
the microstructure refinement. In this note we describe experiments performed on a low interstitial
stainless steel containing 0.02wt%C. It has been possible to achieve materials with high strengths
(UTS > 1 GPa) and significant uniform elongation (> 8%), however, the microstructures associated
with these properties are very different from those previously reported for low carbon steels.
113
Abstract: 15%Cr ferritic stainless steel was machined in rectangular samples and then processed by
multiple forging to a total cumulative strain of 7.2 at an ambient temperature. The large strain
deformation resulted in almost equiaxed submicrocrystalline structure with a mean grain/subgrain
size of 230 nm and about 2.2×1014 m-2 dislocation density in grain/subgrain interiors. The annealing
at a relatively low temperature of 500oC did not lead to any discontinuous recrystallizations. The
grain/subgrain size and the interior dislocation density slightly changed to 240 nm and 2.1×1014 m-2,
respectively, after annealing for 30 min, while the Vickers hardness decreased from 3140 MPa in
the as-processed state to 2900 MPa. This annealing softening was attributed to remarkable release
(by 50%) of internal stresses, which are associated with a non-equilibrium character of
strain-induced grain/subgrain boundaries.
119
Abstract: High-purity niobium single crystals were deformed by equal-channel angular extrusion
(ECAE) at room temperature to an equivalent Von Mises strain of about 1.15. Deformed samples
were annealed in vacuum from 500 to 800oC for 1 hour to investigate their microstructure evolution.
The microstructure of deformed and annealed samples was characterized by scanning electron
microscopy (SEM), electron backscatter diffraction (EBSD), and Vickers microhardness testing.
The deformed structure after one ECAE pass is rather inhomogenous and consists of parallel sets of
coarse shear bands whose spacing varies from one region to another in the cylindrical billet. the
microstructure within the shear bands consists of elongated subgrains with sizes below 3 μm and
lamellar boundaries. The remaining non-sheared regions display a coarser subgrain structure.
Recrystallization is virtually absent in samples annealed at 500oC for 1 hour. Nucleation begins
mostly within shear bands. The new grains with sizes ranging from 10 to 50 μm are arranged in
clusters rather than being homogenously distributed. The recrystallized volume fraction also varies
from one region to another indicating an inhomogenous distribution of stored energy. At 700oC,
recrystallization is complete after annealing for 1 hour resulting in a structure with a mean grain size
of about 100 μm.
125
Abstract: The recrystallization behavior of 71% cold rolled aluminum alloy 3103 was investigated
by measuring the crystallographic texture and the grain microstructure during heat treatment at
288°C, 310°C and 330°C in a magnetic field of 17 T. The results revealed that the application of a
magnetic field substantially enhances recrystallization kinetics.
131
Abstract: The recrystallization behaviour of a cold rolled austenitic Fe-Mn steel is studied to
explain the fine grained final microstructure. Thorough investigation of the kinetics, the
microstructure and the texture evolution during recrystallization showed that the fast
recrystallization kinetics is responsible for the final microstructure, while an oriented nucleation
mechanism determines the texture evolution. The reason for the fast recrystallization kinetics is the
low amount of recovery prior to recrystallization, resulting in a high driving force for the latter.
137