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
The reciprocal transmission from the liquid to the solid state, is
called _congelation_, or _solidification_; and the liquid is said to
be _congealed_ or _solidified_.
The transmission of a body from the liquid to the vaporous or aeriform
state, is called _vaporization_, and the liquid is said to be
_vaporized_ or _evaporated_.
The reciprocal transmission of vapour to the liquid state is called
_condensation_, and the vapour is said to be _condensed_.
We shall now examine more minutely the circumstances which attend
these remarkable and important changes in the state of body.
(11.) Let us suppose that a thermometer is imbedded in any solid body;
for example, in a mass of sulphur; and that it stands at the ordinary
temperature of 60 degrees: let the sulphur be placed in a vessel, and
exposed to the action of fire. The thermometer will now be observed
gradually to rise, and it will continue to rise until it exhibit the
temperature of 218°. Here, however, notwithstanding the continued
action of the fire upon the sulphur, the thermometer will become
stationary; proving, that notwithstanding the supply of heat received
from the fire, the sulphur has ceased to become hotter. At the moment
that the thermometer attains this stationary point, it will be
observed that the sulphur has commenced the process of fusion; and
this process will be continued, the thermometer being stationary,
until the whole mass has been liquefied. The moment the liquefaction
is complete, the thermometer will be observed again to rise, and it
will continue to rise until it attain the elevation of 570°. Here,
however, it will once more become stationary; and notwithstanding the
heat supplied to the sulphur by the fire, the liquid will cease to
become hotter: when this happens, the sulphur will boil; and if it
continue to be exposed to the fire a sufficient length of time, it
will be found that its quantity will gradually diminish, until at
length it will all disappear from the vessel which contained it. The
sulphur will, in fact, be converted into vapour.
From this process we infer, that all the heat supplied during the
processes of liquefaction and vaporization is consumed in effecting
these changes in the state of the body; and that under such
circumstances, it does not increase the temperature of the body on
which the change is produced.
These effects are general: all solid bodies would pass into the
liquid state by a sufficient application of heat; and all liquid
bodies would pass into the vaporous state by the same means. In all
cases the thermometer would be stationary during these changes, and
consequently the temperature of the body, in those periods, would be
maintained unaltered.
Public-domain text, read in full here on John Shaqi.
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