Appletons' Popular Science Monthly, February 1900: Vol. 56, November, 1899 to April, 1900 — John Shaqi
Appletons' Popular Science Monthly, February 1900: Vol. 56, November, 1899 to April, 1900Various
Science
Appletons' Popular Science Monthly, February 1900: Vol. 56, November, 1899 to April, 1900
Various
Science -- Periodicals; Technology -- Periodicals
1. _Cause of Yielding to Lateral Pressure along Lines of Thick
Sediments._--The earth was once very hot. It is still very hot within,
and still very slowly cooling. If sediments accumulate upon a sea
bottom the interior heat will tend to rise so as to keep at the same
distance from the surface. If the sediments are very thick, say five to
ten miles, their lower parts will be invaded by a temperature of not
less than 500° to 1,000° F. This temperature, in the presence of water
(the included water of the sediments), would be sufficient to produce
softening or even fusion of the sediments and of the sea floor on which
they rest. This would establish a line of weakness, and therefore a
line of yielding, crushing, folding, bulging, and thus a mountain
range. In the first formation of a range, therefore, there would
necessarily be a sub-mountain mass of fused or semifused matter which
by the lateral crushing might be squeezed into cracks or fissures,
forming dikes. But in any case the sub-mountain mass would cool into
a granite core which by erosion may be exposed along the crest. The
explanation seems to be satisfactory.
2. _Cause of the Lateral Pressure._--No question in geology has been
more discussed than this, and yet none is more difficult and the
solution of which is more uncertain. But the most obvious and as
yet the most probable view is that it is the result of the secular
contraction of the earth which has gone on throughout its whole
history, and is still going on.
It is admitted by all that in an earth cooling from primal
incandescence there must come a time when the surface, having become
substantially cool and receiving heat also from the sun, would no
longer cool or contract, but, the interior being still incandescently
hot, would continue to cool and contract. The interior, therefore,
cooling and contracting faster than the exterior crust, the latter
following down the ever-shrinking nucleus, would be thrust upon itself
by a lateral or tangential pressure which would be simply irresistible.
If the earth crust were a hundred times more rigid than it is, it still
must yield to the enormous pressure. It does yield along its weakest
lines with crushing, folding, bulging, and the formation of mountain
ranges.
Public-domain text, read in full here on John Shaqi.
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