The Journal of Geology, May-June 1893: A Semi-Quarterly Magazone of Geology and Related SciencesVarious
Science
The Journal of Geology, May-June 1893: A Semi-Quarterly Magazone of Geology and Related Sciences
Various
Geology -- Periodicals
The purpose of Dr. Mill’s paper is to show a simple yet adequate
basis on which to build the superstructure of physical geography. It
does not attempt a discussion of the distribution and varieties of
vertical relief. The structure of the earth is stated most simply by
describing it as an irregular stony ball, covered with an ocean and an
envelope of air. If the lithosphere were perfectly smooth and at rest,
with the hydrosphere uniformly spread over its surface, the former
would have the form of the terrestrial spheroid, and the latter would
surround it to a depth of 1.7 miles. The surface of this hypothetical
spheroid Dr. Mill calls _mean sphere level_. Of course, in reality the
surface of the lithosphere is not perfectly smooth. Parts of it are
greatly depressed and parts much elevated, the latter forming the land
of the earth. The writer proceeds to calculate the position of mean
sphere level, and in the absence of accurate data he uses the careful
estimates of Dr. John Murray, which are as follows: Average depths
of oceans = 2.36 miles; average height of land = .426 miles; average
thickness of hydrosphere surrounding smoothed lithosphere = 1.7 mile;
area of land = 55,000,000 square miles; area of oceans = 141,700,000
square miles. Suppose a block of 55,000,000 of square miles area and
1.7 miles deep to be cut out of the smoothed lithosphere and set down
on the surface alongside the depression. No change will take place
in the surface of the hydrosphere. If the surface of the 141,700,000
square miles of lithosphere were reduced to uniformity, the whole
depressed area would lie .66 mile beneath mean sphere level, and
the depth of the ocean becomes 2.36 miles. To raise the land to its
actual mean level above the hydrosphere surface, a sufficient quantity
of matter must be removed from the depressed area and placed on the
elevated block. Let _x_ = the thickness of the belt removed and _y_
equal the thickness of the belt when placed on the elevated block. Then
_x_ + _y_ is the height of the land above the actual hydrosphere level.
From the data given the following equations are easily obtained:
_x_ + _y_ - .426 = 0
141.7 _x_ - 55 _y_ = 0
_x_ = .12 and _y_ = .306 in miles.
The average height of the land above mean sphere level is thus 1.7 +
.306 = 2.006 miles, and the average depth of the depressed portion
beneath mean sphere level is .66 + .12 = .78 mile.
Dr. Mill divides the earth into the three following divisions: (1)
_Abysmal area_, occupying all the depressions beneath the mean surface
of the lithosphere, occupying 50 per cent. of the earth’s surface; (2)
_Transitional area_, comprising all the regions above mean sphere level
covered by the hydrosphere, occupying 22 per cent. of the surface;
(3) _Continental area_, all the lithosphere that projects above the
hydrosphere, or 28 per cent. of the earth’s surface.
J. A. B.
FOOTNOTE
Public-domain text, read in full here on John Shaqi.
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