How It Flies; or, The Conquest of the Air: The Story of Man's Endeavors to Fly and of the Inventions by Which He Has SucceededFerris, Richard
Science
How It Flies; or, The Conquest of the Air: The Story of Man's Endeavors to Fly and of the Inventions by Which He Has Succeeded
Ferris, Richard
Aeronautics
Of first importance is the fact that air has _weight_. That is, in
common with all other substances, it is attracted by the mass of the
earth exerted through the force we call gravity. At the level of the
sea, this attraction causes the air to press upon the earth with a
weight of nearly fifteen pounds (accurately, 14.7 lbs.) to the square
inch, when the temperature is at 32° F. That pressure is the weight of
a column of air one inch square at the base, extending upward to the
outer limit of the atmosphere--estimated to be about 38 miles (some say
100 miles) above sea-level. The practical fact is that normal human
life cannot exist above the level of 15,000 feet, or a little less than
three miles; and navigation of the air will doubtless be carried on at
a much lower altitude, for reasons which will appear as we continue.
The actual weight of a definite quantity of dry air--for instance,
a cubic foot--is found by weighing a vessel first when full of air,
and again after the air has been exhausted from it with an air-pump.
In this way it has been determined that a cubic foot of dry air,
at the level of the sea, and at a temperature of 32° F., weighs 565
grains--about 0.0807 lb. At a height above the level of the sea, a
cubic foot of air will weigh less than the figure quoted, for its
density decreases as we go upward, the pressure being less owing to
the diminished attraction of the earth at the greater distance. For
instance, at the height of a mile above sea-level a cubic foot of air
will weigh about 433 grains, or 0.0619 lb. At the height of five miles
it will weigh about 216 grains, or 0.0309 lb. At thirty-eight miles
it will have no weight at all, its density being so rare as just to
balance the earth’s attraction. It has been calculated that the whole
body of air above the earth, if it were all of the uniform density of
that at sea-level, would extend only to the height of 26,166 feet.
Perhaps a clearer comprehension of the weight and pressure of the ocean
of air upon the earth may be gained by recalling that the pressure of
the 38 miles of atmosphere is just equal to balancing a column of water
33 feet high. The pressure of the air, therefore, is equivalent to the
pressure of a flood of water 33 feet deep.
[Illustration: Comparative Elevations of Earth and Air.]
But air is seldom dry. It is almost always mingled with the vapor
of water, and this vapor weighs only 352 grains per cubic foot at
sea-level. Consequently the mixture--damp air--is lighter than dry air,
in proportion to the moisture it contains.
[Illustration: Apparatus to show effects of heat on air currents. _a_,
alcohol lamp; _b_, ice. The arrows show direction of currents.]
Public-domain text, read in full here on John Shaqi.
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