The new air world : $b The science of meteorology simplifiedMoore, Willis L. (Willis Luther)
Science
The new air world : $b The science of meteorology simplified
Moore, Willis L. (Willis Luther)
Meteorology
=Water Vapor.= It is only a little over one half as dense as
atmospheric air. In the arid regions of the west it may form only a
fraction of one per cent. of the air by weight; while in the humid
regions in the eastern part of the United States it may constitute
as much as five per cent. The temperature being the same, the same
amount is required to saturate a given space, whether it be a vacuum
or whether it be filled with air. Air doubles its capacity for water
vapor with each increase of eighteen to twenty degrees. On a hot day
in summer, near large bodies of water, it may constitute as much as
one twentieth by weight of the lower air, while on a cold day in
winter it may form no more than one thousandth part. When the air
contains all the water vapor it can hold, it is said to be saturated;
no more can be added to it until its temperature is raised, and but
a slight lowering of its temperature will precipitate a part of its
water vapor in the form of dew, frost, rain, hail, or snow. This is
the reason it is usually called water vapor instead of a gas. Under
the influence of heat that is below the freezing point, ice and snow
may be changed from the solid to the gaseous form, and water vapor
may be precipitated as frost or snow without passing through the
liquid state.
=The Dew Point= is the temperature of saturation,—the temperature to
which a body of air must be reduced before condensation can occur and
some of its water vapor return to the liquid or solid state.
=The Relative Humidity= is expressed in percentages of the amount
necessary to saturate. At a temperature of 32° air may continue to
increase its vapor of water until it contains 2.11 grains per cubic
foot, when it will be saturated and its relative humidity be one
hundred per cent. If this same air be suddenly raised in temperature
to 51° its capacity per cubic foot will be increased to twice what
it was at 32°, the 2.11 grains will be equal to only one half the
number necessary to saturate, and the relative humidity be expressed
by fifty per cent. instead of one hundred per cent. In this way does
the capacity of air for water vapor increase. Thus it is seen that
the relative humidity of the air may increase during the cooling of
nighttime without the addition of any vapor of water, and, in fact,
with a decrease. The increase of relative humidity after nightfall
is greater in the country than in the city, where the presence of
pavements and brick buildings retards the loss of heat.
=The Absolute Humidity= is expressed in grains the cubic foot. The
hygrometer is employed to measure the amount of water vapor.
Public-domain text, read in full here on John Shaqi.
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