The Romance of Modern Chemistry
Forfatter: James C. Phillip
År: 1912
Forlag: Seeley, Service & Co. Limited
Sted: London
Sider: 347
UDK: 540 Phi
A Description in non-technical Language of the diverse and wonderful ways in which chemical forces are at work and of their manifold application in modern life.
With 29 illustrations & 15 diagrams.
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FROM SOLUTIONS TO CRYSTALS
soda. Indeed its behaviour in this respect has been
turned to practical account in railway foot-warmers.
When these are filled with a hot, strong solution of
sodium acetate instead of hot water, the store of available
heat is about four times as great
Reluctance to pass into the crystallised state is exhibited
not only by dissolved substances, but also by many fused
compounds. It is possible in the latter case to cool the
molten substance below its freezing-point without crystal-
lisation setting in; the substance is said to be “ super-
cooled.11 As with supersaturated solutions, mere contact
with a crystal is sufficient to induce crystallisation.
There is, however, a remarkable difference in the rates
at which different supercooled substances respond to this
stimulus. This is very well shown by filling a long,
narrow tube with the supercooled liquid and touching
one end of the column with a crystal of the solid material.
Crystallisation starts immediately at the point of contact,
and is propagated through the tube at a rate which is
perfectly regular, but differs from one case to another.
For instance, yellow phosphorus and benzophenone (a
substance well known to the student of organic chemistry)
can both be obtained in the supercooled condition, but
the rates of solidification in narrow tubes are very
different in the two cases. The crystallisation of the
phosphorus proceeds at the very great speed of 39 inches
a second; in the case of benzophenone, the rate is only
yjth of an inch per second.
The most effective way of inducing crystallisation in a
supersaturated solution or in a supercooled substance is,
as already indicated, the addition of a crystal of the solid.
But suppose no solid is available! what then ? This is
the position in which a chemist frequently finds himself
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