Appletons' Popular Science Monthly, November 1898: Volume 54, November 1898Various
Science
Appletons' Popular Science Monthly, November 1898: Volume 54, November 1898
Various
Science -- Periodicals; Technology -- Periodicals
The parts of the atmosphere included within the same limits of
temperature or humidity therefore rarely form concentric or parallel
layers. They constitute regions interlacing zones which the clouds,
thick or scattered in groups, often mark to our eyes, showing us those
which are saturated with the vapor of water. The distribution of these
zones in space depends chiefly on the heat action of the sun, and upon
preceding and present movements of the atmosphere. Now, if a certain
increase of heat is adequate to melt a piece of ice and to transform the
water of the fusion into vapor, in like manner a corresponding cooling
may suffice to cause the vapor to return to the state of a liquid and
then to that of ice. The processes in the atmosphere are not different,
and all showers, results of the more or less extensive condensation of
the vapor of water, may arise from the cooling of that vapor or of the
water which it produces.
A certain volume of atmospheric air is capable of holding in suspension
a quantity of water proportioned to the elevation of its temperature.
But, for each determined temperature, there is a maximum which can not
be exceeded without the excess of vapor returning to the liquid state.
If, therefore, an atmospheric region is saturated with vapor, and its
temperature falls, that region will give rain. Immense and superabundant
causes for the cooling necessary to provoke rain exist in such an
atmosphere as we have described. The cooling may take effect in three
principal ways: first, by the radiation of different regions between
one another and toward interplanetary space, the temperature of which
is extremely low, as has been indicated by measurements made in high
balloon ascensions; second, by the expansion which air rising in the
atmosphere undergoes in being rarefied; and, third, by the mingling of
masses of warm or moist air with cold or dry.
Cooling by mixture is the sufficient cause in the majority of cases;
and this may be effected from above, by descent of the air from the
upper regions; from below, by ascent, with the assistance of rising
currents created by solar radiations; or, finally, in any and every
direction under the influence of the winds and the general movements of
the atmosphere. Furthermore, the cooling need not be very great in order
to provoke rain under certain conditions of temperature and humidity of
frequent occurrence.
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