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1.
The interface migration rate behavior during recrystallization of a deformed
iron single crystal is considered in detail. A spheroidal growth, site-saturated nucleation model of recrystallization is
developed for iron which quantitatively takes into account the effect of concurrent recovery in the deformed regions ahead
of the advancing recrystallization interfaces. The recovery kinetics model incorporated into the growth model was devised
based on the experimental data of Michalak and Paxton.[10] Explanations are advanced for the nonlinear growth of grains during
recrystallization of iron. Deformation-induced stored energy gradients are proposed to explain the aspects of nonlinear growth
not accounted for by recovery and are introduced into the growth model also. A localized shear band deformation mechanism
developed by Harataniet al.[14] is used to rationalize the presence of stored energy gradients in the deformed
iron single crystal. 相似文献
2.
Recrystallization kinetics in a (111)[1
0] iron single crystal deformed 70 pet by rolling were characterized experimentally at temperatures between 500°C and 600°C
by means of quantitative metallography. A Laplace transform method was applied to the time-dependent global microstructural
properties, volume fraction, interface area per unit volume, and the largest intercept-free length (recrystallized grain)
to separate nucleation and interface migration effects from the overall recrystallization kinetics. A comprehensive nucleation
and growth model was derived from analysis of the microstructural data. The model consisted of the following salient features:
(a) nucleation was random and approximately site-saturated with zero incubation time at all temperatures; (b) the recrystallized
grains grew three-dimensionally in the shape of prolate spheroids; and (c) interface migration rates were highly anisotropic,
the grains growing at an approximately constant rate in one dimension and at a strongly decreasing rate in the other two dimensions.
The present findings were compared to a similar earlier study of a deformed iron (111)[
2] single crystal. The time dependencies of the interface migration rates were rationalized in terms of a deformation-induced,
nonuniform distribution of stored energy and an orientation-dependent grain boundary mobility. 相似文献
3.
K. Kakehi 《Metallurgical and Materials Transactions A》1999,30(5):1249-1259
The effect of crystallographic orientation and aging heat treatment at 850 °C on the creep rupture strength of single crystals
of a nickel-based superalloy was examined at 700 °C in detail. Initial tensile orientations were selected over a wide range
on the standard stereographic triangle. The {111}〈112〉-type slip systems were found to be operative during the creep deformation.
The creep behavior was found to be greatly influenced by the additional aging at 850 °C for 20 hours. It was found that the
effect of the aging at 850 °C was quite different between orientations favored for the
slip system and those favored for the (111)
slip system and that the creep deformation mechanisms of these two slip systems were different. In the orientations favored
for
slip systems, in the single-aged specimens, a small mean surface-to-surface spacing due to hyperfine γ′ precipitates in the matrix channel promoted the
slip and the primary creep. As a result of the additional aging at 850 °C, the hyperfine γ′ precipitates were dissolved into the matrix, and the resultant large mean surface-to-surface spacing between the cuboidal
precipitates inhibited extensive shearing of the γ-γ′ structure by the
slip system. As a result, the creep strengths of these orientations were increased in double-aged specimens; however, the
low ductility associated with the difficulty of secondary noncoplanar slip did not enlarge rupture lifetime in the double-aged
[001] specimen. In the orientations favored for the (111)
slip system, creep deformation occurred by twinning shear through γ and γ′ precipitates, and a distinct effect of the aging at 850 °C was not observed. In the multiple orientation of the {111}
-type slip systems, i.e., the
and
orientations, hyperfine precipitates improved creep strength because they prevented dislocations from gliding in the matrix
channel in the single-aged specimens. 相似文献
4.
The crystallographic direction of growth in directionally solidified magnesium alloy AZ91 has been studied by TEM and EBSP
techniques in SEM. The main direction of growth is found to be
. The dendrites have sixfold symmetry around the main direction, with secondary arms lying along the traces of the (0001),
, and
-planes, respectively. The secondary arms lying in the basal plane are crystallographically of the same type as the main direction:
and
. 相似文献
5.
Two interstitial-free (IF) steels and a high-purity α-iron were deformed in torsion over the temperature range of 600 °C to
840 °C, and the textures produced were measured using conventional X-ray techniques. The conditions were chosen so that dynamic
recrystallization (DRX) would take place in the ferrite and static recrystallization would be avoided during cooling after
deformation. The DRX textures differ from those observed at room temperature and are dominated by the D1 (
)[111], D2(
)[111], and E2 (
)[111] components. The D2 becomes increasingly important as the strain is increased, which leads to weakening of the D1 and
disappearance of the E2 at large strains. Texture simulations were carried out using a DRX model based on sequential deformation,
nucleation, and growth steps. The types of oriented nucleation and selective growth required to reproduce the experimentally
observed textures are discussed. The simulations indicate that the low-energy nucleation mechanism plays a dominant role in
the formation of bcc DRX textures. The results are also interpreted in terms of the continuous (in situ) and discontinuous mechanisms of dynamic recrystallization. 相似文献
6.
This work deals with a transmission electron microscopy investigation of plate martensite in an Fe-8Cr-lC alloy, which exhibits
a typical (252)f martensite transformation. It was found that macroscopic martensite plates, such as those used for optical microscopy determination
of the habit plane and the shape strain, actually consist of many individual small plates having the same crystallographic
orientation and habit plane. Individual plates within a macroscopic plate appear to form by auto-catalytic nucleation. The
coalescence plane between individual plates is usually parallel to (011)b = (lll)f because the growth of the plates is restricted by stacking faults and twins on (lll)f, formed as a result of accommodation of the shape strain. Deformation of the martensite at the coalescence sites, mainly
on the twin system (112)b
b, leads to a complex substructure of the macroscopic plates. Stacking faults and twins in the austenite may be inherited in
the martensite, which leads to further complexity. Prior to the coalescence, the substructure of individual martensite plates
is simple, and consists of a low density of irregularly distributed twins on (112)b
b and dislocations having Burgers vector ab/2
. These defects are probably caused by accommodation deformation. The martensite/austenite interface contains a set of parallel
dislocations having a spacing of about 13 A. These dislocations are likely to be screw dislocations with Burgers vector ab/2
= af/2
, which accomplish the complementary shear in the phenomenological crystallographic theory.
Formerly with the University of Illinois 相似文献
7.
The deformation behavior of a Burgers oriented α-β-Ti-13Mn bimetallic bicrystal was studied at two plastic strains, 0.52 and
2.08 pct. Two single crystals, α and β, each corresponding to the orientation of its respective bicrystal component were also
investigated. The stress axes were
and [1218]β. The interface planes were
and
and lay in the x’-z’ plane. The deformation behavior of the a component differed from that of the a single crystal because
of plastically induced stresses,T
y’z’
,T
x’z’
,T
x’y’
, and σ
x’x’
. Prismatic slip and
twinning were found in the single crystal α whereas the bicrystal revealed additionally pyramidal andc + a slip, the latter at the interface. Slip on the front and back surfaces was different and both thec + a and twinning systems acted to maintain compatibility. Slip in the β single crystal and the β bicrystal component were quite
similar. However, there were differences in the intensity and amount of primary slip, (231)
, on the front and back surfaces. The diminished amount of (231)
slip on the back surface was due to plastically induced stresses, and on the front surface the primary slip cross slipped
to
slip which triggeredc + a slip in α. On the back surface the dominant slip system was
which acted in response to the plastically induced stresses. An approximate calculation revealed that the interface deformation
zone had about twice the flow stress of the average bicrystal stress.
Formerly a Graduate Student in the Department of Physical and Engineering Metallurgy at Polytechnic Institute of New York,
Brooklyn, NY 相似文献
8.
Interactions between deformation twin and 120 deg-rotational domain boundary were studied by transmission electron microscopy
in a two-phase TiAl-based alloy with fully lamellar structure deformed at room temperature. Three types of the interaction
were observed, depending on the interaction geometry and crystallography faced by the incident twinning Shockleys. It was
found that the incident twinning shear could be accommodated into the barrier domain by a reaction involving emission of 1/2
{111}
B
slip in all the three types of interactions presumably since the slip required a small critical resolved shear stress (CRSS)
and was always favored by the pile-up stress. Several reaction schemes involving 1/2
{111}
B
slip for each type of the interactions were proposed by considering whether the reaction resulted in a reduced elastic energy
and if the dissociated dislocations were able to glide away to minimize the total elastic energy associated with a long-range
stress field of a pileup of the incident twinning partials. It is suggested that whether a reaction scheme is feasible would
depend on behavior of other product dislocation except 1/2
{111}
B
. 相似文献
9.
R. Bai C. L. Briant D. C. Paine J. R. Beresford 《Metallurgical and Materials Transactions A》1998,29(3):757-764
This article presents a study of the evolution of the annealing texture in hafnium, as measured by electron backscattering
diffraction patterns (EBSPs). It was found that the annealing texture of asreceived extruded rod depended on the annealing
temperature. After low-temperature recrystallization, the deformation axis was parallel to
or
and the basal planes were approximately parallel to the deformation axis. These orientations were deduced by the position
of the points in the standard stereographic triangle used to produce the inverse pole figure. As the annealing temperature
was raised to 1700 °C, the direction parallel to the rolling direction changed to
and the grain size increased. It appeared that the increase in grain size occurred by a process of abnormal grain growth,
and this abnormal grain growth appeared to be the cause of the change in the texture. Texture was also examined in samples
that had been warm rolled to thickness reductions between 10 and 90 pct and then annealed at 1700 °C. In these samples, the
main feature of the texture was that the basal plane became parallel to the rolling plane as the amount of rolling increased.
The maximum grain size was observed in samples that had been rolled to a reduction in thickness of 50 pct. 相似文献
10.
Ternary interdiffusion coefficients were measured in the Ni solid solution γ (fcc) phase of the Ni-Cr-Al system at 1100 and
1200 °C. Extensive use was made of both γ/γ and γ/γ + β (β-NiAl structure) diffusion couples. Two analysis techniques were
employed to calculate the interdiffusion coefficients. When the Matano planes for Al and Cr were not coincident, numerous
integral calculations were made to determine an average diffusion coefficient and to assess the effect of the noncoincidence
of the Matano planes. The results of the diffusivity measurements showed that
is approximately four times greater than
, while
and
are of the same magnitude. For all concentrations,
is two to three times greater than
. Both
and
increase with increasing Al concentration, whereas
and
show little concentration dependence on Cr alone. A ternary, finite-difference interdiffusion model was employed to predict
concentration profiles for the γ/γ couples utilizing the concentration dependence of the measured diffusivities. Good agreement
was observed between the predicted and measured concentration profiles for both 1100 and 1200 °C. 相似文献
11.
M2C carbides were observed to precipitate within the austenite matrix of an Fe-24.6Mn-6.6Al-3. IMo-1.0C alloy after quenching
from 1200 °C and aging at 750 °C. By means of transmission electron microscopy (TEM) and diffraction techniques, the orientation
relationships between M2C (p) and the austenite (γ) matrix were determined to be: (0001)p//(111)γ, (11–
0)p// (1
0)γ, (
100)p//(11
)γ. M2C carbide has been reported by many researchers to precipitate from the ferrite matrix or along austenite/ferrite boundaries
in alloy steels containing Mo. However, little information concerning the formation of M2C in the austenite matrix has been provided. This investigation presents the first evidence for the existence of M2C carbide wholly within the austenite matrix and its relationship to the austenite. The energy-dispersive spectrometry (EDS)
analyses were performed on M2C carbides, and the results indicate that the solubility of the M2C carbide for foreign atoms other than Mo is very limited. 相似文献
12.
Electron-backscattered diffraction (EBSD) has been used to investigate the texture evolution during tensile deformation at
temperatures between 673 and 773 K of a coarse-grained commercial AZ31 magnesium alloy. A weak (0001) fiber texture was initially
present in the hot-rolled magnesium alloy plate. The [0001] directions of the grains spread 0 to 45 deg around the normal
direction (ND) of the magnesium alloy plate. This pre-existing weak texture evolved during tensile deformation into a strong
texture close to the {0001} 〈1
00〉. The [0001] directions of the grains rotated toward the orientations perpendicular to the tension axis of the samples,
indicating that the 〈11
0〉 slip system appeared to be the most active slip system, especially in the early stages of deformation. The EBSD Schmid-factor
analysis revealed that, however, with an increase in strain and the rotation of the (0001) slip plane, the {11
2} 〈11
〉 slip system appeared to be more favorable. The {1
00} 〈11
0〉 and {1
01} 〈11
0〉 slip systems remained favored throughout the strains investigated, indicating that {1
00} and {1
01} are two important slip planes for cross slip using the 〈11
0〉 slip vector. It is found that the misorientation across one coarse grain (as high as 38.2 deg) is accommodated by low-angle
grain boundaries (LAGBs). The formation of these LAGBs may be an intermediate stage of the coarse grain refinement that occurred
during deformation.
This article is based on a presentation made in the symposium entitled “Processing and Properties of Structural Materials,”
which occurred during the Fall TMS meeting in Chicago, Illinois, November 9–12, 2003, under the auspices of the Structural
Materials Committee. 相似文献
13.
The deformation characteristics contributing to the superior cavitation erosion properties of HCP cobalt single crystals have
been determined. Results indicate that its erosion response is highly orientation sensitive. A homogeneous distribution of
and
glide occurs in {0110} crystals, whereas slip in the (0001) crystals is much more heterogeneous and consists mainly of
dislocations. Continued exposure to cavitation nucleates a large number of twins, predominantly on the
and
planes in the
and (0001) crystals respectively. The former twins are finer and more needle-like than the latter. The
crystals are also significantly more erosion resistant than the (0001) crystals. The twin density increases continuously
with cavitation exposure until a dense network of twins spans the entire exposed area. This fine-scale twinning is considered
responsible for the superior erosion resistance of the metal. 相似文献
14.
S. Skolianos T. Z. Kattamis Y. R. Chung H. D. Merchant 《Metallurgical and Materials Transactions A》1987,18(7):1179-1190
Dendritic monocrystals of Al-4.5 wt pct Cu-2 wt pct Mn were directionally solidified at 0.20 m/h under a thermal gradient
of 3 × 103 K/m. Crystal pulling was stopped for various lengths of time prior to quenching the remaining liquid, thus making it possible
to evaluate the transformation and coarsening kinetics of dispersed intermetallic phases, Al6Mn and Al20Cu2Mn3, as a function of temperature. Coarsening of Al6Mn intermetallic particles surrounded by liquid (Type II) follows an average particle size
relationship much closer than it does a
relationship. This suggests that convection plays no important role in coarsening. For coarsening of Al6Mn particles in a solid matrix (Type I) the relationship
fits the experimental measurements reasonably well. Coarsening kinetics studies were extended to intermetallic particle sizes
an order of magnitude finer than those occurring in directionally solidified alloy, in order to derive information required
by an on-going project on the effect of intermetallic phase geometry on corrosion behavior. Jt was found that coarsening of
Al20Cu2Mn3 particles contained in a melt-spun ribbon follows a
relationship, as predicted by Kirchner for grain-boundary diffusion-controlled ripening. Finally, coarsening of Al6Mn particles surrounded by liquid indium film and contained in a plastically deformed matrix follows a
relationship, as predicted by LSW theory for liquid diffusion-controlled ripening. Shortening the time required to obtain
coarse intermetallic particles during a homogenization treatment is important in deep drawing.
Formerly Graduate Student, Department of Metallurgy, University of Connecticut, Storrs, CT 06268 相似文献
15.
16.
S. Tsuji 《Metallurgical and Materials Transactions A》1994,25(4):741-751
Mathematical relationships describing the multiphase binary diffusions are deduced under the condition that
in an infinite medium, and also under the condition that
and the fluxes of both the species occur in each other’s opposite direction through the surface in a semi-infinite medium,
where
are the interdiffusion coefficient and the partial molal volume of componenti in phasej, respectively, and are composition independent. Two graphical evaluation methods for obtaining the interdiffusion coefficients
for all the phases present in the diffusion zone have been developed in infinite and semi-infinite media. Concentration-distance
curves of both the components for an infinite medium and those curves and also mass change of the couple per unit area of
the surface before and after the diffusion anneal for a semi-infinite medium must be prepared to calculate an interdiffusion
coefficient for each phase. 相似文献
17.
The boundary structure of {10
1}, {10
2}, {11
1} and, {11
2} twins in hexagonal-close-packed (hcp) metals and the interaction of crystal dislocations with the first two twin types
have been studied previously using atomic-scale computer simulation. The interaction of crystal dislocations with {11
1} and {11
2} twin boundaries is described here and compared with the results for {10
1} and {10
2} twins. These four twins are found to create barriers to the motion of crystal dislocations gliding on the basal plane,
and the strength of the barrier depends in a relatively complex manner on crystallographic parameters and details of the atomic
structures of the interfaces. In some circumstances, crystal dislocations can be transmitted through the twin boundary, thereby
creating twinning dislocations.
This article is based on a presentation made in the symposium entitled “Defect Properties and Mechanical Behavior of HCP Metals
and Alloys” at the TMS Annual Meeting, February 11–15, 2001, in New Orleans, Louisiana, under the auspices of the following
ASM committees: Materials Science Critical Technology Sector, Structural Materials Division, Electronic, Magnetic & Photonic
Materials Division, Chemistry & Physics of Materials Committee, Joint Nuclear Materials Committee, and Titanium Committee. 相似文献
18.
The kinetics of recrystallization of a (111) {
} single crystal of pure iron deformed 70 pct by rolling were characterized experimentally at temperatures between 450°C and
600°C, using quantitative metallography. The method of Laplace transforms was applied to the overall recrystallization kinetic
behavior to separate nucleation from interface migration kinematics. A comprehensive nucleation and growth model was developed
to explain all observations quantitatively. the model consisted of the following important features: (a) nucleation sites
were distributed randomly; (b) nucleation was site-saturated and occurred with no practical incubation time at all annealing
temperatures; (c) recrystallized grains grew three-dimensionally and were spheroidally shaped; (d) all recrystallized grains
grew at approximatelly the same rate within experimental error; and (e) interface migration rates were not constant but decreased
with time according to at
−0.38 law at all temperatures. The time dependency of the interface migration rate was rationalized in terms of deformation-induced,
nonuniform distribution of stored energy, Recovery processes competing with recrystallization were evident at long annealing
times at the two lowest annealing temperatures. 相似文献
19.
X. W. Li X. M. Wu Z. G. Wang Y. Umakoshi 《Metallurgical and Materials Transactions A》2003,34(2):307-318
The dislocation structures induced by the cyclic deformation of Cu-16 at. pct Al alloy single crystals oriented, typically,
as
for single slip and [023] and
for double slip, were studied by transmission electron microscopy (TEM) and compared with the results of Cu single crystals.
Completely unlike the dislocation structures of Cu single crystals of corresponding orientations, the dislocation structures
of these oriented Cu-16 at. pct Al alloy single crystals show a typical planar morphology. As the applied-plastic-stain amplitude
increases, the dislocation configuration changes, on the whole, from multipolar arrays to dislocation tangles in the primary
slip plane and from low-density planar slip bands to well-developed persistent Lüder’s bands (PLBs) in the planes normal to
the primary slip plane, respectively. Secondary slips can be clearly observed to activate from very low plastic-strain amplitudes
in all three Cu-16 at. pct Al single crystals investigated. Interestingly, the crystallographic orientation has almost no
effect on the dislocation structure of Cu-16 at. pct Al single crystals. 相似文献
20.
Twins as barriers to basal slip in hexagonal-close-packed metals 总被引:2,自引:0,他引:2
The boundary structure of
,
,
, and
twins in hexagonal-close-packed (hcp) metals and the interaction of crystal dislocations with the first two twin types have
been studied previously using atomic-scale computer simulation. The interaction of crystal dislocations with
and
twin boundaries is described here and compared with the results for
and
twins. These four twins are found to create barriers to the motion of crystal dislocations gliding on the basal plane, and
the strength of the barrier depends in a relatively complex manner on crystallographic parameters and details of the atomic
structures of the interfaces. In some circumstances, crystal dislocations can be transmitted through the twin boundary, thereby
creating twinning dislocations.
This article is based on a presentation made in the symposium entitled “Defect Properties and Mechanical Behavior of HCP Metals
and Alloys” at the TMS Annual Meeting, February 11–15, 2001, in New Orleans, Louisiana, under the auspices of the following
ASM committees: Materials Science Critical Technology Sector, Structural Materials Division, Electronic, Magnetic & Photonic
Materials Division, Chemistry & Physics of Materials Committee, Joint Nuclear Materials Committee, and Titanium Committee. 相似文献