The Energy System of Matter: A Deduction from Terrestrial Energy Phenomena — John Shaqi
The Energy System of Matter: A Deduction from Terrestrial Energy PhenomenaWeir, James, active 1883-1912
Science
The Energy System of Matter: A Deduction from Terrestrial Energy Phenomena
Weir, James, active 1883-1912
Force and energy
The pendulum machine described above furnishes certain outstanding
examples of the operation of energy transformation. It will be noted,
however, that it also portrays certain processes of energy transmission.
In this respect it is not peculiar. Most of the material machines in
which energy operates will furnish examples of both energy transmissions
and energy transformations. In some instances, the predominant operation
seems to be transformation, in others, transmission; and the machines
may be classified accordingly. It is, however, largely a matter of
terminology, since both operations are usually found closely associated
in one and the same machine. The apparatus now to be considered is
designed primarily to illustrate the operative features of certain
energy transmissions, but the description of the machines with their
allied phenomena will show that energy transformations also play a very
important part in their constitution and working.
A cylindrical metallic bar about twelve inches long, say, and one inch
in diameter, is placed with its ends immersed in water in two separate
vessels, A and B, somewhat as shown.
[Illustration: FIG. 3]
By the application of heat energy, the temperature of the water in the
vessel A is raised to a point say 100° F. above that of B, and steadily
maintained at that point. It is assumed that B is also kept at the
constant lower temperature. In these circumstances, a transmission of
heat energy takes place from A to B through the metallic bar. When the
steady temperature condition is reached, the transmission will be
continuous and uniform; the rate at which it is carried out will be
determined by the length of the bar, by the material of which it is
composed, and by the temperature difference maintained between its
ends. Now what has really happened is that by a combination of
phenomena the bar has been converted into a machine for the transmission
of heat energy. A full description of these phenomena is, in reality,
the description of this machine, and vice versa. Let us, therefore, now
try to outline some of these phenomena.
The first feature of note is the gradient of temperature which exists
between the ends of the bar. Further research is necessary regarding the
real nature of this gradient--it appears to differ greatly in different
materials--but the existence of such a gradient is one of the main
features of the energy machine, one of the essential conditions of the
transmission process.
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