The Steam Engine Familiarly Explained and Illustrated: With an historical sketch of its invention and progressive improvement; its applications to navigation and railways; with plain axioms for railway speculators — John Shaqi
The Steam Engine Familiarly Explained and Illustrated: With an historical sketch of its invention and progressive improvement; its applications to navigation and railways; with plain axioms for railway speculatorsLardner, Dionysius
History
The Steam Engine Familiarly Explained and Illustrated: With an historical sketch of its invention and progressive improvement; its applications to navigation and railways; with plain axioms for railway speculators
Lardner, Dionysius
Steam-engines -- Early works to 1850
During this process, the thermometer will constantly be maintained at
the same elevation of 212°; but if the time be noted, it will be found
that the water will be altogether evaporated, if the same source of
heat be continued to be applied to it six and a half times as long as
was necessary to raise it from the freezing to the boiling-point.
Thus, if the application of the lamp to water at 32°, be capable of
raising that water to 212° in one hour, the same lamp will require to
be applied to the boiling water for six hours and a half, in order to
convert the whole of it into steam. Now if the steam into which it is
thus converted were carefully preserved in a receiver, maintained at
the temperature of 212°, this steam would be found to have that
temperature, and not a greater one; but it would be found to fill a
space about 1700 times greater than the space it occupied in the
liquid state, and it would possess an elastic force equal to the
pressure of the atmosphere under which it was boiled; that is to say,
it would press the sides of the vessel which contained it with a
pressure equivalent to that of a column of mercury of 30 inches in
height; or what is the same thing, at the rate of about 15lb. on every
square inch of surface.
(15.) As the quantity of heat expended in raising the water from 32°
to 212°, is 180°; and as the quantity of heat necessary to convert the
same water into steam is six and a half times this quantity, it
follows that the quantity of heat requisite for converting a given
weight of water into steam, will be found by multiplying 180° by
5-1/2. The product of these numbers being 990°, it follows, that, to
convert a given weight of water at 212° into steam of the same
temperature, under the pressure of the atmosphere, when the barometer
stands at 30 inches, requires as much heat as would be necessary to
raise the same water 990° higher in temperature. The heat, not being
sensible to the thermometer, is latent heat; and accordingly it may be
stated, that the latent heat, necessary to convert water into steam
under this pressure is, in round numbers, 1000°.
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