Catechism of the locomotiveForney, Matthias N. (Matthias Nace)
Science
Catechism of the locomotive
Forney, Matthias N. (Matthias Nace)
Locomotives -- Handbooks, manuals, etc.
_Answer._ By _latent heat_ is meant that heat which _apparently_
disappears when water or other liquids are vaporized. Thus, it
is found that if any quantity of water is converted into steam at
any pressure, it is necessary not only to heat it to a temperature
equivalent to that of the steam, or to the boiling-point, but after
it has reached that temperature an additional amount of heat must be
added in order to keep up the process of boiling. Notwithstanding this
addition of heat to the water, the temperature of the steam produced
will not be higher than that of the boiling water, thus showing that a
considerable quantity of heat is absorbed, the only effect of which is
to change the water into a gas or steam. This apparent disappearance
of heat can be shown if we take a pound of boiling water whose
temperature is 212 degrees and mix it with a pound of ice-cold water
at 32 degrees. The result will be a mixture of two pounds of water of
a mean temperature of 122 degrees. If now we convert a pound of water
into steam at atmospheric pressure, the steam will heat 6.37 lbs. of
ice-cold water up to 122 degrees, showing that a pound of steam at
atmospheric pressure contains over six times as much heat as a pound
of water of the same temperature as indicated by a thermometer. A
similar apparent disappearance of heat occurs when other liquids are
evaporated, and when ice or any other solid is converted into a liquid.
QUESTION 39. _What is the explanation of these phenomena?_
_Answer._ The exact reasons which will explain them fully are probably
not yet clearly understood, but it is at least extremely probable that
when any substance is changed from a solid to a liquid, or from a
liquid to a gaseous condition, “a large portion of the heat is spent
_in doing work_ against the force of cohesion.”[11] The particles of
solid bodies, as we know, are so united that it requires more or less
force, according to the nature of the substance, to tear them apart.
Now we can conceive that the heat is changed into a form of energy,
and in that condition resists this attraction of the particles to each
other, and that being thus transformed it has lost the capacity of
expanding the mercury in the thermometer. A similar effect takes place
when a liquid is converted into a gas. In the former condition the
particles move freely about each other and have little or no attraction
for each other, but when it becomes a gas they have a _repulsion from_
each other. The heat is thus converted into the energy of repulsion,
and therefore is in reality no longer in the condition of heat and
consequently does not affect the thermometer. We can illustrate this by
supposing that by using steam heat is converted into work by raising
the weight, or drop as it is called, of a pile-driving machine. When
the weight is raised to the top of the guides from which it falls,
although, as already explained, the heat is converted into _potential
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