Sounding the Ocean of Air: Being Six Lectures Delivered Before the Lowell Institute of Boston, in December 1898Rotch, Abbott Lawrence
Science
Sounding the Ocean of Air: Being Six Lectures Delivered Before the Lowell Institute of Boston, in December 1898
Rotch, Abbott Lawrence
Atmosphere; Balloons; Clouds; Kites (Meteorology)
The observations from balloons at great heights are neither
sufficiently numerous nor accurate to enable us to form an opinion as
to what is the temperature of interplanetary space, which the kinetic
theory of gases places at 460∞ Fahrenheit below zero. This temperature
is called "the absolute zero," and is calculated from the fact that
air under a constant pressure contracts 1/490 of its volume for each
degree Fahrenheit it is cooled below the temperature of freezing
water, and consequently under no pressure it should have an infinite
volume and a temperature of about 490∞ below freezing, or 458∞ below
zero. There are other hypotheses regarding the temperature of space,
but since it can never be measured directly, it will probably remain a
matter of speculation. It is certain, however, that if the earth were
deprived of its atmosphere, the temperature would fall very low, and
even with our atmosphere as a blanket our earth would be
uninhabitable were it not for the aqueous vapour which controls the
selective absorption of the solar rays, transforming them into obscure
rays so that they cannot escape from the atmosphere. Water-vapour,
then, is a very important factor in the physics of the atmosphere, but
it can only be considered briefly here.
=Moisture of the Atmosphere.=--The air is constantly absorbing
moisture from the water on the earth, but the tension of this aqueous
vapour decreases with elevation much faster than does the atmospheric
pressure. At the height of about a mile and a quarter half the
quantity of water-vapour is below, while we must rise about three and
a half miles to reduce the quantity of air one-half, as may be seen in
Plate I. The relative humidity, or the percentage of moisture in the
air, as compared to the amount which it could contain at that
temperature, is nearly the reverse at low and at high levels. It is
found from the kite-observations at Blue Hill, that up to the height
of a mile or two the air is drier during winter and at night, and
damper during summer and in the day-time than it is near the ground.
At great heights probably the air is always very dry. The condensation
of the invisible vapour into a visible form is considered in the next
chapter on clouds.
Public-domain text, read in full here on John Shaqi.
Reviews
Reviews
No reviews yet
Be the first to share your thoughts on this work.
Join the Discussion
Join the discussion
Sign in to leave a comment or review.
Sign InorCreate an account