Geology, Vol. 1 [of 3] : $b Geologic processes and their resultsSalisbury, Rollin D.
Science
Geology, Vol. 1 [of 3] : $b Geologic processes and their results
Salisbury, Rollin D.
Geology
Snow crystals often continue to grow so long as they are in the
atmosphere; but if they pass through an under-saturated stratum of
air or a stratum whose temperature is above 32° Fahr., they suffer
from evaporation or melting. When they reach the ground, the processes
of growth and decadence continue, and the crystals grow or diminish
according to circumstances.
A glacier is a colossal aggregation of crystals grown from snowflakes
to granules of much greater sizes. The microscopic study of new-fallen
snow reveals the mode of change from flakes to granules. The slender
points and angles of the former yield to melting and evaporation more
than the more massive central portions, and this change probably
illustrates a law of vital importance. It may often be seen that the
water melted from the periphery of a flake gathers about its center,
and if the temperature be right, it freezes there. This is a first
step toward the pronounced granulation of snow which has lain for some
time on the ground. If measured systematically from day to day, the
larger granules taken from beneath the surface of this coarse-grained
snow are found to be growing. In a series of experiments[133] to
determine the law of growth it was found that when the temperature of
the atmosphere was above the melting-point the growth was appreciably
more rapid than when the air was colder, but there was, on the average,
_an increase under all conditions of temperature_. A portion of this
average increase of the larger granules appears to come from the
diminution and destruction of the smaller ones, for the total number
of granules steadily diminishes. A portion of the growth doubtless
comes from the moisture of the atmosphere which penetrates the snow
and another portion from the moisture derived from surface melting;
but beneath the surface of a large body of snow the growth of the
large granules is probably chiefly at the expense of the small ones.
To follow the process it should be noted that the free surface of
every granule is constantly throwing off particles of water-vapor
(evaporation); that the rate at which the particles are thrown off is
dependent, among other things, on the curvature of the surface, being
greater the sharper the curve; that the surfaces of the granules are
at the same time liable to receive and retain molecules thrown from
other granules, and that, other things being equal, the retention
of particles also depends on the curvature of the surface, the less
curved surface retaining more than the sharply curved one. Under these
laws, it is obvious that the larger granules of smaller curvature will
lose less and gain more, on the average, than the smaller granules of
greater curvature. It follows that the larger granules will grow at the
expense of the smaller. It is also to be noted that, other things being
equal, small granules melt more readily than large ones, and that where
the temperature is nicely adjusted between melting and freezing, the
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