Experience with melting plate glass at high temperatures

1962 ◽  
Vol 19 (2) ◽  
pp. 62-68
Author(s):  
V. V. Pollyak ◽  
V. D. Soskova ◽  
A. K. Mazur
Keyword(s):  
High Temperatures ◽  
Plate Glass ◽  
Melting Plate

Means of increasing the output of tank furnaces melting plate glass

1962 ◽  
Vol 18 (8) ◽  
pp. 388-392
Author(s):  
M. G. Stepanenko ◽  
V. S. Pavlov
Keyword(s):  
Plate Glass ◽  
Melting Plate

The use of aluminum, hydroxide for melting plate glass for floatless drawing

1961 ◽  
Vol 18 (4) ◽  
pp. 199-200
Author(s):  
O. K. Zaporozhtseva ◽  
S. V. Gorbai
Keyword(s):  
Aluminum Hydroxide ◽  
Plate Glass ◽  
Melting Plate

VI. On the microscopic characters of some specimens of devitrified glass; with notes on certain analogous structures in rocks

1885 ◽  
Vol 38 (235-238) ◽  
pp. 422-424
Keyword(s):  
High Temperatures ◽  
Thick Plate ◽  
Plate Glass ◽  
First Case ◽  
Fractured Surface

This paper relates first to the changes brought about in glass solids bounded by plane surfaces, by exposure to high temperatures, the main object of the paper being to elucidate the changes which have taken place in vitreous, and once vitreous, rocks by comparing the phenomena of natural devitrification with similar phenomena effected by artificial means. The first case considered is that of a piece of thick plate glass which has been totally devitrified under conditions described in detail in the paper. In the roughly broken specimen the fractured surface sufficiently reveals the fact that crystallisation has taken place throughout the mass, while other specimens subsequently described by the authors demonstrate beyond question that the crystallisation has started at the surfaces and has travelled inwards. In this particular specimen the crystallisation has advanced from the different surfaces until the various sets of crystals have arrested one another in very definite planes, whose traces are clearly perceptible on a fractured surface.

Microstructural and Microchemical Characterization of Nickel Sulfide Inclusions in Plate Glass

1991 ◽  
Vol 49 ◽  
pp. 962-963
Author(s):  
J. Cooper ◽  
O. Popoola ◽  
W. M. Kriven
Keyword(s):  
Thermal Expansion ◽  
Phase Transformation ◽  
Glass Matrix ◽  
Nickel Sulfide ◽  
Plate Glass ◽  
Thermal Expansion Mismatch ◽  
Volume Increase ◽  
Β Phase ◽  
Microchemical Characterization

Nickel sulfide inclusions have been implicated in the spontaneous fracture of large windows of tempered plate glass. Two alternative explanations for the fracture-initiating behaviour of these inclusions have been proposed: (1) the volume increase which accompanies the α to β phase transformation in stoichiometric NiS, and (2) the thermal expansion mismatch between the nickel sulfide phases and the glass matrix. The microstructure and microchemistry of the small inclusions (80 to 250 μm spheres), needed to determine the cause of fracture, have not been well characterized hitherto. The aim of this communication is to report a detailed TEM and EDS study of the inclusions.

In situ REM imaging of surface processes on ceramic bulk crystals from 300 to 1670 K in a conventional TEM

1991 ◽  
Vol 49 ◽  
pp. 660-661
Author(s):  
Z. L. Wang ◽  
J. Bentley
Keyword(s):  
High Temperatures ◽  
Image Resolution ◽  
Atomic Processes ◽  
Crystal Surfaces ◽  
Beam Radiation ◽  
Surface Areas ◽  
Transmission Electron ◽  
Reflection Electron Microscopy ◽  
Gas Reactions

Studying the behavior of surfaces at high temperatures is of great importance for understanding the properties of ceramics and associated surface-gas reactions. Atomic processes occurring on bulk crystal surfaces at high temperatures can be recorded by reflection electron microscopy (REM) in a conventional transmission electron microscope (TEM) with relatively high resolution, because REM is especially sensitive to atomic-height steps.Improved REM image resolution with a FEG: Cleaved surfaces of a-alumina (012) exhibit atomic flatness with steps of height about 5 Å, determined by reference to a screw (or near screw) dislocation with a presumed Burgers vector of b = (1/3)<012> (see Fig. 1). Steps of heights less than about 0.8 Å can be clearly resolved only with a field emission gun (FEG) (Fig. 2). The small steps are formed by the surface oscillating between the closely packed O and Al stacking layers. The bands of dark contrast (Fig. 2b) are the result of beam radiation damage to surface areas initially terminated with O ions.

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