Flying Machines TodayEnnis, William D. (William Duane)
History
Flying Machines Today
Ennis, William D. (William Duane)
Aeronautics; Flying-machines
The air that surrounds us weighs about one-thirteenth of a pound per
cubic foot and exerts a pressure, at sea level, of nearly fifteen
pounds per square inch. Its temperature varies from 30° below to 100°
above the Fahrenheit zero. The pressure of the air decreases about
one-half pound for each thousand feet of altitude; at the top of Mt.
Blanc it would be, therefore, only about six pounds per square inch.
The temperature also decreases with the altitude. The weight of a cubic
foot, or _density_, which, as has been stated, is one-thirteenth of a
pound ordinarily, varies with the pressure and with the temperature.
The variation with pressure may be described by saying that the
_quotient_ of the pressure by the density is constant: one varies in
the same ratio as the other. Thus, at the top of Mt. Blanc (if the
temperature were the same as at sea level), the density of air would be
about 6/15 × 1/13 = 2/65: less than half what it is at sea level. As to
temperature, if we call our Fahrenheit zero 460°, and correspondingly
describe other temperatures--for instance, say that water boils at
672°--then (pressure being unchanged) the _product_ of the density
and the temperature is constant. If the density at sea level and zero
temperature is one-thirteenth pound, then that at sea level and 460°
Fahrenheit would be
(0 + 460)/(460 + 460) × 1/13 = 1/26.
These relations are particularly important in the design of all
balloons, and in computations relating to aeroplane flight at
high altitudes. We shall be prepared to appreciate some of their
applications presently.
Generally speaking, the atmosphere is always in motion, and moving air
is called wind. Our meteorologists first studied winds near the surface
of the ground: it is only of late years that high altitude measurements
have been considered practically desirable. Now, records are obtained
by the aid of kites up to a height of nearly four miles: estimates of
cloud movements have given data on wind velocities at heights above six
miles: and much greater heights have been obtained by free balloons
equipped with instruments for recording temperatures, pressures,
altitude, time, and other data.
When the Eiffel Tower was completed, it was found that the average wind
velocity at its summit was about four times that at the base. Since
that time, much attention has been given to the contrasting conditions
of surface and upper breezes as to direction and velocity.
Public-domain text, read in full here on John Shaqi.
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