The Popular Science Monthly, August, 1900: Vol. 57, May, 1900 to October, 1900 — John Shaqi
The Popular Science Monthly, August, 1900: Vol. 57, May, 1900 to October, 1900Various
Science
The Popular Science Monthly, August, 1900: Vol. 57, May, 1900 to October, 1900
Various
Science -- Periodicals; Technology -- Periodicals
For this purpose there is only one of the imposed rhythms of practical
value, namely, the precessional; but that one is, in my judgment, of
high value. The tidal rhythm can not be expected to characterize any
thick formation. The annual is liable to confusion with a variety of
original rhythms, especially those connected with storms. The rhythm
of eccentricity, being theoretically expressed only as an accentuation
of the precessional, can not ordinarily be distinguished from it. But
none of these qualifications apply to the precessional. It is not
liable to confusion with the tidal and annual because its period is
so much longer, being more than 2,000 times that of the annual. It has
an eminently practical and convenient magnitude, in that its physical
manifestation is well above the microscopic plane, and yet not so large
as to prevent the frequent bringing of several examples into a single
view. It is also practically regular in period, rarely deviating from
the average length by more than the tenth part.
From the greater number of original rhythms it is distinguished, just
as from the annual and tidal, by magnitude. The practical geologist
would never confuse the deposit occasioned by a single storm, for
example, with the sediments accumulated during an astronomic cycle
of 20,000 years. But there are other original rhythms, known or
surmised, which might have magnitudes of the same general order, and
to discriminate the precessional from these it is necessary to employ
other characters. Such characters are found in its regularity or
evenness of period, and in its practical perpetuity. The diversion of
the mouth of a great river such as the Hoang Ho or the Mississippi
might recur only after long intervals; but from what we know of the
behavior of smaller streams we may be sure that such events would be
very irregular in time as well as in other ways. The intervals between
volcanic eruptions at a particular vent or in a particular district
may at times amount to thousands of years, but their irregularity is
a characteristic feature. The same is true of the recurrent uplifts
by which mountains grow, so far as we may judge them by the related
phenomena of earthquakes; and the same category would seem to hold also
the theoretically recurrent collapse of the globe under the strains
arising from the slowing of rotation. The carbon-dioxide rhythm,
known as yet only in the field of hypothesis, is hypothetically a
running-down oscillation, like the lessening sway of the cradle when
the push is no longer given.
But the precessional motion pulses steadily on through the ages, like
the swing of a frictionless pendulum. Its throb may or may not be
caught by the geologic process which obtains in a particular province
and in a particular era, but whenever the conditions are favorable and
the connection is made, the record should reflect the persistence and
the regularity of the inciting rhythm.
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