Laboratory Glass-Working for Scientists - Sciencemadness Dot Org
Laboratory Glass-Working for Scientists - Sciencemadness Dot Org
Laboratory Glass-Working for Scientists - Sciencemadness Dot Org
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Chapter 2<br />
PHYSICAL AND CHEMICAL<br />
PROPERTIES OF GLASS<br />
The Structure of <strong>Glass</strong><br />
A OLAS5 is a product of fusion which has cooled to a rigid condition<br />
Without crystallizing. This definition includes a large number of<br />
<strong>Org</strong>anic glasses, and does not restrict the term 'glass* to inorganic<br />
gubltances, which is a frequent practice in the U.S.A. This restriction<br />
ntnu somewhat arbitrary, particularly when we consider how G.<br />
immann established the general principles of the glass-like state by<br />
•larch on organic glasses, and how the devitrification of technica<br />
hues is paralleled by that of organic glasses. Tammann concluded<br />
|tt a glass could be regarded as a supercooled liquid in which the<br />
National movements of the molecules had been frozen (see W. E.<br />
,, 1952). In fact, as R. Boyle described it about 1660, 'the<br />
of the glass agitated by the heat, were surpriz'd by the cold<br />
they could make an end of those motions which were requisite<br />
| their disposing themselves into the most durable texture.' In<br />
pdarn terminology, a glass is thermodynamically unstable with<br />
to the corresponding crystal.<br />
lalline silica (quartz, tridymite or cristobalite) in its various<br />
lions is built up of Si04 tetrahedra linked together in a<br />
manner so that every oxygen is between two silicons. The<br />
ra there<strong>for</strong>e share corners. The arrangement in space of the<br />
'a is different in the various crystalline <strong>for</strong>ms, but is always<br />
regular. A silica glass, in contrast, again contains Si04 tetrawith<br />
every corner shared; but by slight distortions of the valency<br />
compared with the crystal, a continuous and irregular threeional<br />
network is built up. The orientation about the Si-O-Si<br />
of one Si04 tetrahedron with respect to another can be practirandom.<br />
Thus a two-dimensional picture of a silica glass would<br />
a series of irregular rings, with an average number of about six<br />
ra in each ring, but with the number of tetrahedra in indirings<br />
varying from three to ten or more. The silica glass<br />
Ultflw the condition <strong>for</strong> glass <strong>for</strong>mation proposed by W. H.<br />
7