Authors: Goro Miyamoto, Poorganji Behrang, Tadashi Furuhara
Abstract: Demands for medium carbon steels with high strength used for forging parts in automobile have been increasing. V addition to such steels leads to interphase boundary precipitation (IBP) of VC and thus an increase of strength. However, mechanism and strengthening effect of IBP have not been clarified in detail. In this study, precipitation of VC accompanying ferrite and pearlite transformations and its effect on hardness have been examined in medium carbon steels microalloyed with 0.3%V. Specimens transformed in a temperature range between 873 and 973K consist of pearlite and small amount of proeutectoid ferrite. Hardness increase by the V addition becomes larger by lowering transformation temperature at these temperatures. Meanwhile the alloying effect of V on the hardness remarkably decreases at 823K where bainite transformation takes place partly. TEM characterization has revealed that VC are precipitated in both of proeutectoid and pearlitic ferrites in the manner of fine rows parallel to the austenite / ferrite interphase boundary. The size of VC decreases and its number density increases by lowering transformation temperature, corresponding to the larger hardness increase. Orientation relationship analyses between ferrite and austenite in the V-added specimen based of EBSD measurements reveals that proeutectoid ferrite grows preferentially towards an austenite grain with which ferrite does not hold a specific orientation relationship, indicating that classical ledge mechanism does not play a role for interphase boundary precipitation of VC in this alloy.
420
Authors: Pierre Blaineau, Lionel Germain, Michel Humbert, Nathalie Gey
Abstract: We propose a new approach to automatically reconstruct the orientation map from the ’ map inherited by the bainitic or martensitic ’ phase transformation. Our model comprises two main steps (1) identification of reliable fractions of parent grains – each fraction orientation is determined from neighbouring variants related to a unique orientation with a low tolerance angle; (2) expansion of these fractions by collecting adjacent variants being in orientation relation (OR) with the orientation of the initial fraction - using now a higher tolerance around the strict OR. The code was tested on ’ maps we built from reference maps to control some characteristics of the transformation, i.e. the type of OR used, the spread around OR, the number of inherited variants. The results show that even with a large spread around OR, the shape and orientation of most of the grains are accurately calculated.
203
Authors: Heidrun Sowa, Helmut Klein, Lars Raue
Abstract: In order to get information about the transition mechanism, the temperature-induced transformation in the binary com¬pound NiS was investigated. Above 379 °C, a single crystal of millerite -NiS transforms to polycrystalline NiAs type -NiS with a sharp texture. Pole figures of both phases in the same orientation were measured using synchrotron radiation and an imaging plate detector. The Rietveld texture analysis showed that there are at least three components of the high-temperature -NiS phase. The main component shows the following orientation relations:
[001]NiAs type [001]millerite, [100]NiAs type [210]millerite, [210]NiAs type [100]millerite.
The broad peaks of the recovered polycrystalline millerite occur at the same positions as the reflections of the original single crystal.
177
Authors: Claude Esling, Dao Yong Cong, Jing Bai, Yu Dong Zhang, Jean Marc Raulot, Xiang Zhao, Liang Zuo
Abstract: This paper summarizes some of our recent results on crystal structure, microstructure, orientation relationship between martensitic variants and crystallographic features of martensitic transformation in Ni-Mn-Ga FSMAs. It was shown that Ni53Mn25Ga22 has a tetragonal I4/mmm martensitic structure at room temperature. The neighboring martensitic variants in Ni53Mn25Ga22 have a compound twinning relationship with the twinning elements K1={112}, K2={11-2}, η1=<11-1>, η2=<111>, P={1-10} and s=0.379. The ratio of the relative amounts of twins within the same initial austenite grain is ~1.70. The main orientation relationship between austenite and martensite is Kurdjumov-Sachs (K-S) relationship. Based on the crystallographic phenomenological theory, the calculated habit plane is {0.690 -0.102 0.716}A (5.95° from {101}A), and the magnitude, direction and shear angle of the macroscopic transformation shear are 0.121, <-0.709 0.105 0.698>A (6.04° from <-101>A) and 6.88°, respectively.
2040
Authors: Nobuaki Sekido, Yoko Yamabe-Mitarai
Abstract: A Laves phase Ir2Y is found to exhibit a temperature dependent solubility, which yields
Ir3Y precipitation within the Ir2Y matrix of an arc-melted Ir-30at.%Y alloy. Microstructure
observations have confirmed that the precipitation of Ir3Y has already started in the as-cast state.
Upon annealing of an as-cast Ir-30at.%Y, the volume fraction of Ir3Y precipitates increases and
finally reaches about 50%. The orientation relationship between Ir3Y and Ir2Y has been identified
as: (0001)Ir3Y//(111)Ir2Y and [21
_
1 _
0]Ir3Y//[1
_
10]Ir2Y. The orientation relationship is rationalized by
the atom matching at the habit plane between the two phases.
1400
Authors: Loïc Malet, Pascal J. Jacques, Stéphane Godet
Abstract: The orientation relationships that apply to the fcc (γ) – bcc (α) phase transformation in high-performance hot-rolled TRIP-aided steels were characterised by EBSD techniques. A statistical treatment of the experimental data allows the mean orientation relationship to be determined. This mean orientation relationship was compared to the models commonly proposed in the literature and confronted qualitatively to the predictions of the phenomenological theory of martensite crystallography (PTMC). The variant selection phenomenon was also characterized quantitatively at the level of individual austenite grains. The reconstruction of the EBSD maps evidences that bainite grows by packets in which the bainite laths share a common {111}γ plane in the austenite. This growth mechanism is not influenced by the prior hot deformation of the austenite. The hot deformation has a critical influence on the number of packets that forms. The analysis of the crystallographic features of the bainite packets reveals that all possible variants are formed in a packet, though in different proportions.
359
Authors: G. Jyoti, R. Tewari, K.D. Joshi, Dinesh Srivastava, G.K. Dey, S.C. Gupta, S.K. Sikka, S. Banerjee
Abstract: In the present study, specimens of Zr were subjected to shock compression of 11.6 GPa.
TEM examination of the recovered samples revealed that during shock compression the a phase
has transformed into the w phase. The orientation relationships (ORs) between the a and w phase
have been determined using both the stereographic projection method and the correspondence
matrix method. Our ORs have been found to belong to the Variant I OR given by Usikov and
Zilbershtein (UZ) for statically compressed Zr samples. Our ORs are the same as the one reported
by Song and Gray (SG) on dynamically compressed samples. In the present paper it has been
shown that the OR of SG is a subset of the OR of UZ and is not apart from it. The mechanism of
a®w transition with respect to occurrence of an intermediate b (bcc) structure, during the
transition has also been explored. We also show in this study that the amount of the transformed w
phase decreases with increasing oxygen content in the samples that were shock loaded to the same
peak pressure, as is revealed by both the TEM and XRD results.
133
Authors: H. Landheer, S. Erik Offerman, R.H. Petrov, Leo A.I. Kestens
Abstract: The role of the α/γ orientation relationships during ferrite nucleation is investigated.
EBSD measurements were performed on an especially developed high purity ternary iron-based
alloy with 20 wt.% Cr and 12 wt.% Ni with both austenite and ferrite present at room temperature to
measure the orientation relationship between the austenite and ferrite crystallites. The experimental
results are compared to the nucleation models of Clemm and Fisher and Aaronson and co-workers.
1413
Authors: Takeshi Imamura, Yasuyuki Hayakawa, Mineo Muraki
Abstract: Cold-rolled micro-texture of polycrystalline 3%Si-Fe was investigated using
high-resolution Electron BackScattering Patterns (EBSP) method. There were deformation bands
near grain boundaries. The orientation relationship between the deformation bands and the
surrounding deformed grains is explained by the orientation rotation around a <211> axis. The
activated slip to generate these deformation bands is estimated from the <211> rotation. The
S-value, which is a geometrical index of slip operation against applied stress, of this slip system
was not maximum value of all, but it had a common slip plane with an adjacent grain. A
hypothesis that the slip system having a common slip plane with an adjacent grain is activated
was proposed from the present results.
885
Authors: Di Zhang, Zhi Feng Yang, Wei Jie Lu, Dong Xu
Abstract: Novel hybrid TiB, TiC and rare earth oxide (Re2O3) reinforced titanium matrix composites were
in situ synthesized utilizing the reaction between Ti, B4C (or C), rare earth (Re) and B2O3 through
homogeneously melting in a non-consumable vacuum arc remelting furnace. In this work, Nd and Y
were chosen as rare earth (Re) added in the in situ reaction. The thermodynamics of in situ synthesis
reaction was studied. The results of X-ray diffraction (XRD) proved that no other phases appeared
except for TiB, TiC and Re2O3. The microstructures of the composites were examined by scanning
electron microscope (SEM) and backscattered scanning electron microscope (SEM). The results
showed that there were mainly three kinds of reinforcements: TiB whiskers, TiC particles and
Re2O3 particles. The reinforcements were fine and were homogeneously distributed in the matrix.
The interfaces of TiB-TiC and Nd2O3-Ti were examined by high-resolution transmission electron
microscopy (HREM).Transmission electron microscopy (TEM) and selected area diffraction (SAD)
were used to analyze the orientation relationships of TiB-TiC and Nd2O3-Ti. The orientation
relationship between TiB and TiC can be described as: [001] TiB //[001] TiC , (010) TiB //(110) TiC . The
orientation relationship of Nd2O3 and α-Ti can be described as: [110] Nd2O3 //[ 1213 ] Ti ,
(111) Nd2O3 //(1101) Ti , ( 001) Nd2O3 //( 2110 ) Ti .
155