Phase Selection and Morphological Evolution for a Dilute Al-Mg-Si Alloy Under Sub-Rapid Solidification

2019 ◽  
Author(s):  
Ze–Tian Liu ◽  
Cheng Wang ◽  
Hong Ju ◽  
Min Zha ◽  
Zhi–Ping Guan ◽  
...  
2021 ◽  
Vol 85 (4) ◽  
pp. 155-161
Author(s):  
You Hayasaka ◽  
Kazuhiko Kuribayashi ◽  
Suguru Shiratori ◽  
Shumpei Ozawa

2005 ◽  
Vol 475-479 ◽  
pp. 607-612 ◽  
Author(s):  
Heng Zhi Fu ◽  
Lin Liu

Most of materials have long been considered to be mechanical and/or physical anisotropy. Permitting materials to grow along specific orientation by means of directional solidification technique can optimize their structural or functional properties. The present paper attempts to introduce the research work in the field of processing of some advanced materials by innovative directional solidification techniques performed at State Key Laboratory of Solidification Processing and with author’s intended research work. The paper deals with the specific topics on directional solidification of following advanced materials: column and single crystal superalloys under high thermal gradient, Ni-Cu alloys under deep supercooling of the melt, intermetallic compounds with selected preferential crystal orientation, superalloys with container less electromagnetic confinement, high Tc superconducting oxides, high temperature structural ceramics, continuous cast single crystal copper and copper-based composites. The relevant solidification phenomena, such as morphological evolution, phase selection, peritectic reaction and aligned orientation relationship of crystal growth for multi-phases in the processing of directional solidification, are discussed briefly. The trends of developments of directional solidification technique are also prospected.


1983 ◽  
Vol 28 ◽  
Author(s):  
M.J. Kaufman ◽  
H.L. Fraser

ABSTRACTSubmicron powders, amorphous films and melt spun ribbons of various Al-Ge alloys have been analyzed to determine the relative roles of undercooling and cooling rate in the production of non-equilibrium structures. All analyses were performed in transmission electron microscopes equipped with energy dispersive x-ray spectrometers. The submicron powders, produced by electro-hydrodynamic atomization, were analyzed in their as-received condition and then annealed and/or melted using the electron beam as a local heating source. Once molten, the liquid droplets were undercooled at different cooling rates by varying the rate of beam obstruction. In this manner, a number of different microstructures were produced. These included metastable crystalline phases and mixed amorphous/crystalline structures. By combining this technique with a microscope heating stage, it was possible to carry out controlled dynamic undercooling experiments and determine phase selection as a function of undercooling and composition. The amorphous films were rapidly heated with the electron beam in the microscope and metastable as well as stable phases were produced. The results of these complementary analyses will be compared and discussed with reference to current models and theories of rapid solidification.


2020 ◽  
Vol 195 ◽  
pp. 341-357 ◽  
Author(s):  
Vishwanadh Bathula ◽  
Can Liu ◽  
Kai Zweiacker ◽  
Joseph McKeown ◽  
Jörg M.K. Wiezorek

1982 ◽  
Vol 19 ◽  
Author(s):  
J. H. Perepezko ◽  
W. J. Boettinger

ABSTRACTDuring rapid solidification, the nucleation and/or growth of a thermodynamically stable phase may be difficult. In this case the liquidus, solidus or other thermodynamic data for a metastable phase are important for the interpretation and prediction of the phases present in rapidly solidified materials. In this paper various techniques are described to obtain information about metastable equilibrium from measured stable equilibrium data. Extrapolations of phase boundaries as functions of temperature, pressure or composition (including a new component) into regions of metastability can often be constructed directly on the equilibrium diagram. These constructions can be performed more quantitatively with analytical methods using thermodynamic modelling of the free energy functions consistent with measured data. A number of examples are considered including a discussion of metastable liquid miscibility gaps, metastable eutectic and peritectic reactions, pressure diagrams and metastability in ternary alloys to indicate the possible product phase selection. A coupling of metastable phase diagrams with a solidification kinetics analysis can contribute towards effective alloy design and processing during rapid solidification.


Author(s):  
You Hayasaka ◽  
Kazuhiko Kuribayashi ◽  
Suguru Shiratori ◽  
Shumpei Ozawa

Materialia ◽  
2020 ◽  
Vol 13 ◽  
pp. 100850 ◽  
Author(s):  
Ze–Tian Liu ◽  
Cheng Wang ◽  
Qun Luo ◽  
Jiang You ◽  
Xiao–Li Zhou ◽  
...  

2007 ◽  
Vol 22 (10) ◽  
pp. 2953-2963 ◽  
Author(s):  
Feng Liu ◽  
Yuzeng Chen ◽  
Gencang Yang ◽  
Yiping Lu ◽  
Zheng Chen ◽  
...  

Adopting glass fluxing and cyclic superheating, high undercooling up to ∼550 K was achieved in bulk eutectic Ni78.6Si21.4 alloy melt. With increasing undercooling, the as-solidified microstructure shows an interesting evolution, i.e., regular lamellar eutectic, coarse directional dendrite, quasi-spherical dendritic colony, fine directional dendrite, fine quasi-spherical dendritic colony, and superfine anomalous eutectic. In combination with different theories for nucleation and growth, the microstructure evolution was analyzed and described using competitions incorporated in rapid solidification of the bulk undercooled eutectic Ni78.6Si21.4 alloy. For undercooling below and above 180 K, Ni3Si, and α-Ni are primarily solidified, respectively. This phase selection can be ascribed to competitive nucleation. As undercooling increases, a transition of the prevalent nucleation mode from site saturation to continuous nucleation was interpreted in terms of competition of nucleation mode. Accordingly, the superfine anomalous eutectic is obtained, due to the substantially increased continuous nucleation rate, i.e., grain refinement occurring at high undercooling (e.g., ∼550 K).


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