The development of preferred orientations during the freezing of metals and alloys

Previous work with columnar castings of lead has shown that there exists a connexion between the solidification texture and the morphologies of the decanted freezing interfaces. This has been explained in terms of crystal growth from the melt by the extension of relatively large (one micron) steps or platelets which are visible on many decanted interfaces. The present work consists of an examination of preferred orientations and interface morphologies in castings of lead and of metals having structures other than face-centred cubic. Metal castings have been prepared in which the orientations of columnar grains could be correlated directly with the morphologies of the corresponding decanted solid/liquid interfaces. Experiments have been carried out with lead, zinc, magnesium, tin, bismuth and a β-brass alloy, and except in the last case, the morphologies of the freezing interfaces were controlled by varying the purities of the metals for given conditions of casting. Except in the case of tin the preferred orientations are determined by the morphologies of the freezing interfaces. The results can be satisfactorily explained if the mechanism of crystal growth is one of edgewise extension of closely packed planes in directions lying close to the plane of the actual solid/liquid interface. The origin of the platelet structure on decanted interfaces is discussed, and the appearances of decanted interfaces are compared with structures visible on the free surfaces of rapidly frozen metal sheets. It is suggested that there may be some connection between the platelet formation on decanted interfaces and those seen on the solid/gaseous interfaces, and that the existence of a residual liquid layer over the freshly decanted surfaces might give rise to a structure which is not typical of the original solid/liquid interface. The thickness of this residual liquid film is ~20 μm, but under the conditions of these experiments the liquid freezes in less time than is. required for the nucleation of new grain structures or even of eutectic lamellae. It is concluded that decanted surfaces are probably an approximate representation of the true solid/liquid interfaces, but that it is uncertain how far this is true of the platelet structure.

Crystals ◽  
2020 ◽  
Vol 11 (1) ◽  
pp. 25
Author(s):  
Xia Tang ◽  
Botao Liu ◽  
Yue Yu ◽  
Sheng Liu ◽  
Bing Gao

The difficulties in growing large-size bulk β-Ga2O3 single crystals with the Czochralski method were numerically analyzed. The flow and temperature fields for crystals that were four and six inches in diameter were studied. When the crystal diameter is large and the crucible space becomes small, the flow field near the crystal edge becomes poorly controlled, which results in an unreasonable temperature field, which makes the interface velocity very sensitive to the phase boundary shape. The effect of seed rotation with increasing crystal diameter was also studied. With the increase in crystal diameter, the effect of seed rotation causes more uneven temperature distribution. The difficulty of growing large-size bulk β-Ga2O3 single crystals with the Czochralski method is caused by spiral growth. By using dynamic mesh technology to update the crystal growth interface, the calculation results show that the solid–liquid interface of the four-inch crystal is slightly convex and the center is slightly concave. With the increase of crystal growth time, the symmetry of cylindrical crystal will be broken, which will lead to spiral growth. The numerical results of the six-inch crystal show that the whole solid–liquid interface is concave and unstable, which is not conducive to crystal growth.


2020 ◽  
Vol 10 (16) ◽  
pp. 5362-5385
Author(s):  
Leila Negahdar ◽  
Christopher M. A. Parlett ◽  
Mark A. Isaacs ◽  
Andrew M. Beale ◽  
Karen Wilson ◽  
...  

Many industrially important chemical transformations occur at the interface between a solid catalyst and liquid reactants. In situ and operando spectroscopies offer unique insight into the reactivity of such catalytically active solid–liquid interfaces.


1994 ◽  
Vol 29 (15) ◽  
pp. 3997-4000 ◽  
Author(s):  
Wang Fengquan ◽  
Chen Shiyu ◽  
He Deping ◽  
Wei Bingbo ◽  
Shu Guangji

1988 ◽  
Author(s):  
S B. Trivedi ◽  
T S. Ananthanarayanan ◽  
R G. Rosemeier ◽  
J J. Kennedy

Author(s):  
J. M. Howe

A number of different theoretical approaches have been used to model the atomic structure and properties of solid-liquid interfaces. Most calculations indicate that ordering occurs in the first several layers of the liquid, adjacent to the crystal surface. In contrast to the numerous theoretical investigations, there have been no direct experimental observations of the atomic structure of a solid-liquid interface for comparison. Saka et al. examined solid-liquid interfaces in In and In-Sb at lattice-fringe resolution in the TEM, but their data do not reveal information about the atomic structure of the liquid phase. The purpose of this study is to determine the atomic structure of a solid-liquid interface using a highly viscous supercooled liquid, i.e., a crystal-amorphous interface.


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