A New Kinetics-Based Approach to Quantifying the Extent of Metastable → Stable Phase Transformation in Thermally-Grown Al2O3 Scales

2013 ◽  
Vol 79 (3-4) ◽  
pp. 361-381 ◽  
Author(s):  
Wei Zhao ◽  
Zhuoqun Li ◽  
Brian Gleeson
JOM ◽  
2009 ◽  
Vol 61 (7) ◽  
pp. 51-55 ◽  
Author(s):  
P. Y. Hou ◽  
A. P. Paulikas ◽  
B. W. Veal

2013 ◽  
Vol 81 (3-4) ◽  
pp. 357-371 ◽  
Author(s):  
Shigenari Hayashi ◽  
Kouhei Mizumoto ◽  
Suzue Yoneda ◽  
Yasumitsu Kondo ◽  
Hiroshi Tanei ◽  
...  

2013 ◽  
Vol 46 (4) ◽  
pp. 1105-1116 ◽  
Author(s):  
Xiaoke Mu ◽  
Sridhar Neelamraju ◽  
Wilfried Sigle ◽  
Christoph T. Koch ◽  
Nico Totò ◽  
...  

Structural disorder and distortion play a significant role in phase transformations. Experimentally, electron diffraction in the transmission electron microscope offers the ability to characterize disorderviathe pair distribution function (PDF) at high spatial resolution. In this work, energy-filteredin situelectron diffraction is applied to measure PDFs of different phases of MgF2from the amorphous deposit through metastable modifications to the thermodynamically stable phase. Despite the restriction of thick specimens resulting in multiple electron scattering, elaborate data analysis enabled experimental and molecular dynamics simulation data to be matched, thus allowing analysis of the evolution of short-range ordering. In particular, it is possible to explain the theoretically not predicted existence of a metastable phase by the presence of atomic disorder and distortion. The short-range ordering in the amorphous and crystalline phases is elucidated as three steps: (i) an initial amorphous phase exhibiting CaCl2-type short-range order which acts as a crystallization nucleus to guide the phase transformation to the metastable CaCl2-type phase and thus suppresses the direct appearance of the rutile-type phase; (ii) a metastable CaCl2-type phase containing short-range structural features of the stable rutile type; and (iii) the formation of a large volume fraction of disordered intergranular regions which stabilize the CaCl2-type phase. The structure evolution is described within the energy landscape concept.


2020 ◽  
pp. 15-21
Author(s):  
S. V. Davydov ◽  

In the present work low-temperature carbide phase transformations in the system of Fe-C alloys based on ε-сarbide Fe2C with consideration of identification of θ-Fe3C cement as a solid solution were studied. It has been proved that the θ-Fe3C cement slurry is colourfastonide, and the ε-Fe2C carbide slurry is bertollide. When tempering hardened steels, ε-сarbide Fe2C is emitted in the structure of hardened martensite, which is absent in the phase diagram of iron-carbon system alloys. It is believed that ε-сarbide Fe2C is not a stable phase, and since it is metastable, it is formed only in quenched steels under non-equilibrium conditions. The isolation and dissolution of ε-сarbide Fe2C is a classic phase transformation and the absence of this transformation on the diagram is not caused by the metastable phase of ε-сarbide Fe2C, but by the incomplete iron-carbon diagram. The martensite decomposition phase transformation is based on the formation of carbon enriched zones. The processes of carbon segregation on dislocation structures and grid planes of martensite create zones with excess energy. Beginning approximately with temperature 100 °С in structure of martensite begins to allocate ε-сarbide Fe2C, finishing a stage of two-phase segregational disintegration of martensite. At rather small concentrations of carbon in cluster zones the fastest and most effective way of relaxation of redundant energy in these zones, as well as in the tetragonal lattice of martensite is the formation of phases with low value of work of nucleation, first of all ε-сarbide Fe2C and α-Fe(C) or ferrite. The main stages of phase transformations in the peritectoid reaction of martensite decomposition are considered. It is proposed to introduce the peritectoid transformation horizontal at 382 °C and the peritectic transformation horizontal of cement at 1650 °C into the Fe-C alloy state diagram.


2020 ◽  
Vol 94 (1-2) ◽  
pp. 81-93
Author(s):  
Shigenari Hayashi ◽  
Suzue Yoneda ◽  
Yasumitsu Kondo ◽  
Hiroshi Tanei

2010 ◽  
Vol 160 ◽  
pp. 109-116 ◽  
Author(s):  
Jay Chakraborty ◽  
Kishor Kumar ◽  
R. Ranjan ◽  
Sandip Ghosh Chowdhury ◽  
S.R. Singh

{111} fiber textured face centered cubic (fcc) titanium has been found to coexist with the {0002} fiber textured hexagonal close packed (hcp) titanium in polycrystalline titanium (Ti) thin films (thickness: 144 nm to 720 nm) deposited on Si (100) substrate by magnetron sputtering. X-ray diffraction investigation confirms that relative phase fraction of such metastable fcc Ti phase decreases with increasing film thickness indicating thickness dependent fcc-hcp phase transformation of titanium. Texture development in hcp Ti phase was due to film microstructure (thickness effect) rather than the phase trans-formation. Diffraction stress analysis (by d-sin2 method) indicates that fcc to hcp phase transformation is also accompanied by the reduction of compressive stress in the hcp Ti phase with increasing film thickness. Strain energy calculations for both phases of titanium indicate that fcc Ti is a more stable phase compared to hcp Ti at relatively low film thickness (144 nm to 432 nm). It has been concluded that film stress favours fcc to hcp phase transformation towards the higher film thickness. Reverse transformation (hcp to fcc) occurs towards the lower film thickness.


2010 ◽  
Vol 152-153 ◽  
pp. 864-867 ◽  
Author(s):  
Li Lin ◽  
Feng Wang ◽  
Lin Yang ◽  
Li Jia Chen ◽  
Zheng Liu

A novel precipitation sequence, super-saturated-solution → stacking faults → Mg3Gd, i.e. S.S.S. → SF → β1, was established for a Mg-3Zn-2Gd (wt%) alloy. Solute pre-precipitation can occur during the solidification of as-cast alloy and subsequent solution-treatment, resulting in the formation of lamella structures with …ABCABC… stacking sequence. The lamella structure will transform to the Mg3Gd phase, even that Mg3Gd is not the most stable phase in this serial alloys.


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