Solid-State Reaction Kinetics Determination via in Situ Time-Resolved X-Ray Diffraction

1994 ◽  
Vol 108 (1) ◽  
pp. 152-157 ◽  
Author(s):  
K.M. Forster ◽  
J.P. Formica ◽  
J.T. Richardson ◽  
D. Luss
1983 ◽  
Vol 61 (3) ◽  
pp. 594-598 ◽  
Author(s):  
M. Sunitha Kumari ◽  
Etalo A. Secco

The physicochemical aspects of the order–disorder phase transitions occurring in the Na2SO4–K2SO4 system were investigated by thermal analyses, infrared absorption, and X-ray diffraction methods.Kinetic and structural studies on the compounds KNaSO4 and K3Na(SO4)2 are reported in more detail.


2018 ◽  
Vol 51 (4) ◽  
pp. 1133-1140 ◽  
Author(s):  
Andrea Quintero ◽  
Patrice Gergaud ◽  
Joris Aubin ◽  
Jean-Michel Hartmann ◽  
Vincent Reboud ◽  
...  

The Ni/Ge0.9Sn0.1 solid-state reaction was monitored by combining in situ X-ray diffraction, in-plane reciprocal space map measurements and in-plane pole figures. A sequential growth was shown, in which the first phase formed was an Ni-rich phase. Then, at 518 K, the mono-stanogermanide phase Ni(Ge0.9Sn0.1) was observed. This phase was stable up to 873 K. Special attention has been given to the nature and the crystallographic orientation of the Ni-rich phase obtained at low temperature. It is demonstrated, with in-plane pole figure measurements and simulation, that it was the ∊-Ni5(Ge0.9Sn0.1)3 metastable phase with a hexagonal structure.


1993 ◽  
Vol 42 (7) ◽  
pp. 1134
Author(s):  
BAI HAI-YANG ◽  
CHEN HONG ◽  
ZHANG YUN ◽  
WANG WEN-KUI

2009 ◽  
Vol 42 (2) ◽  
pp. 153-160 ◽  
Author(s):  
Zhèn Yáng ◽  
Ashley S. Harvey ◽  
Anna Infortuna ◽  
Ludwig J. Gauckler

Selected compositions of the Ba–Sr–Co–Fe–O system were synthesized from powders by the solid-state reaction method. Samples were equilibrated at 1273 K for 36 000 s in air. The resulting powders were characterized by X-ray diffraction (XRD) at room temperature and by high-temperaturein situXRD. The phases present in the BaxSr1−xCoyFe1−yO3−δsystem are outlined for 1273 K in air. For most of the quaternary compositions, the cubic perovskite is formed, except for the compositions withx= 1 (excludingy= 0.4),y= 1 andx,y= 0.8, where the phases mainly show hexagonal distortions, andx, y= 0, for which a predominant cubic phase is mixed with other phases.


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