The Steam Engine Explained and Illustrated (Seventh Edition): With an Account of Its Invention and Progressive Improvement, and Its Application to Navigation and Railways; Including Also a Memoir of WattLardner, Dionysius
History
The Steam Engine Explained and Illustrated (Seventh Edition): With an Account of Its Invention and Progressive Improvement, and Its Application to Navigation and Railways; Including Also a Memoir of Watt
Lardner, Dionysius
Steam-engines; Watt, James, 1736-1819
(27.) There are, however, various other means by which air may be
partially expelled from a vessel besides the direct application of
mechanical force. Thus if heat be applied to [Pg044] the vessel,
the air, as has been already explained, will acquire increased
elasticity, and will rush from the vessel with a force proportionate
to the excess of its elasticity above that of the external air, and
this process may be continued by increasing the heat to which the
vessel is exposed, until a very considerable portion of the air has
been expelled. If the orifice by which the air has escaped be then
closed, and the vessel be allowed to cool, the air within, by having
its temperature reduced to that of the external air, will lose all
the elasticity which it had gained from the heat, and will be in the
same condition as if an equivalent quantity of air had been
withdrawn by any mechanical agent. The external air, therefore, will
have a tendency to rush in with a force corresponding to the
difference of pressures.
The process of filling thermometers with mercury shows one use of
producing a high degree of rarefaction by heat. To construct the
instrument it is necessary to fill the bulb and a part of the tube
with mercury; but the bore of the tube is so small that the
mercury cannot be introduced by any ordinary means. It is
therefore held over flame until heated to a high temperature. The
air within it gradually increasing in pressure as its temperature
is raised, is forced through the small bore of the tube, until the
pressure of the air within becomes no more than equal to the
pressure of the external atmosphere; this air being so rarefied
that quantity in the bulb bears a very small proportion to its
contents at common temperatures. The mouth of the tube is then
plunged into mercury, and as the bulb cools, the air within it
loses its elasticity, and the superior pressure upon the external
surface forces the mercury into the tube. This continues until the
air remaining within the bulb has been so contracted, that its
pressure combined with the weight of the mercury, shall balance
the atmospheric pressure. The tube is then reversed, and the air
which remained rises in a bubble to the surface, and escapes.
Public-domain text, read in full here on John Shaqi.
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