Unraveling the Origin of Structural Disorder in High Temperature Transition Al2O3: Structure of θ-Al2O3

2015 ◽  
Vol 27 (20) ◽  
pp. 7042-7049 ◽  
Author(s):  
Libor Kovarik ◽  
Mark Bowden ◽  
Dachuan Shi ◽  
Nancy M. Washton ◽  
Amity Andersen ◽  
...  
2020 ◽  
Author(s):  
Libor Kovarik ◽  
Mark Bowden ◽  
Amity Andersen ◽  
Nicholas R. Jaegers ◽  
Nancy Washton ◽  
...  

<p>High temperature exposure of gamma-Al<sub>2</sub>O<sub>3</sub> can lead to a series of polymorphic transformations, including the formation of delta-Al<sub>2</sub>O<sub>3</sub> and theta-Al<sub>2</sub>O<sub>3</sub>. Quantification of the microstructure in the delta/theta-Al<sub>2</sub>O<sub>3</sub> formation range represents a formidable challenge as both phases accommodate a high degree of structural disorder. In this work, we explore the use of XRD recursive stacking formalism for quantification of high temperature transition aluminas. We formulate the recursive stacking methodology for modelling of disorder in delta-Al<sub>2</sub>O<sub>3 </sub>and twinning in theta-Al<sub>2</sub>O<sub>3</sub> and show that explicitly accounting for the disorder is necessary to reliably model the XRD patterns of high temperature transition alumina. In the second part, we use the recursive stacking approach to study phase transformation during high temperature (1050 ºC) treatment. We show that the two different intergrowth modes of delta-Al<sub>2</sub>O<sub>3</sub> have different transformation characteristics, and that a significant portion of delta-Al<sub>2</sub>O<sub>3</sub> is stabilized with theta-Al<sub>2</sub>O<sub>3 </sub>even after prolonged high-temperature exposures. In discussions, we outline the limitation of the current XRD approach and discuss a possible multimodal XRD and NMR approach which can improve analysis of complex transition aluminas.</p>


2020 ◽  
Author(s):  
Libor Kovarik ◽  
Mark Bowden ◽  
Amity Andersen ◽  
Nicholas R. Jaegers ◽  
Nancy Washton ◽  
...  

<p>High temperature exposure of gamma-Al<sub>2</sub>O<sub>3</sub> can lead to a series of polymorphic transformations, including the formation of delta-Al<sub>2</sub>O<sub>3</sub> and theta-Al<sub>2</sub>O<sub>3</sub>. Quantification of the microstructure in the delta/theta-Al<sub>2</sub>O<sub>3</sub> formation range represents a formidable challenge as both phases accommodate a high degree of structural disorder. In this work, we explore the use of XRD recursive stacking formalism for quantification of high temperature transition aluminas. We formulate the recursive stacking methodology for modelling of disorder in delta-Al<sub>2</sub>O<sub>3 </sub>and twinning in theta-Al<sub>2</sub>O<sub>3</sub> and show that explicitly accounting for the disorder is necessary to reliably model the XRD patterns of high temperature transition alumina. In the second part, we use the recursive stacking approach to study phase transformation during high temperature (1050 ºC) treatment. We show that the two different intergrowth modes of delta-Al<sub>2</sub>O<sub>3</sub> have different transformation characteristics, and that a significant portion of delta-Al<sub>2</sub>O<sub>3</sub> is stabilized with theta-Al<sub>2</sub>O<sub>3 </sub>even after prolonged high-temperature exposures. In discussions, we outline the limitation of the current XRD approach and discuss a possible multimodal XRD and NMR approach which can improve analysis of complex transition aluminas.</p>


1967 ◽  
Vol 40 (4) ◽  
pp. 1105-1110 ◽  
Author(s):  
Stuart L. Cooper ◽  
Arthur V. Tobolsky

Abstract Viscoelastic behavior of linear segmented elastomers was examined. The unusual properties found in spandex systems are also observable in hydrocarbon block co-polymers, indicating that hydrogen bonding interactions are perhaps not essential. Low temperature properties of segmented systems are governed by the structural nature of the associated flexible segments, which determines the value of the major glass transition temperature (Tg). It appears that an association of the hard segments provides a broad temperature range of enhanced rubbery modulus. This occurs between the major Tg and a secondary high temperature transition.


2003 ◽  
Vol 44 (6) ◽  
pp. 975-979 ◽  
Author(s):  
S. A. Kovyazina ◽  
L. A. Perelyaeva ◽  
I. A. Leonidov ◽  
Yu. A. Bakhteeva

1999 ◽  
Vol 60 (14) ◽  
pp. 10504-10507 ◽  
Author(s):  
G. Balestrino ◽  
A. Crisan ◽  
S. Lavanga ◽  
P. G. Medaglia ◽  
G. Petrocelli ◽  
...  

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