Outlines of a mechanical theory of storms : $b containing the true law of lunar influence, with practical instructions to the navigator, to enable him approximately to calculate the coming changes of the wind and weather, for any given day, and for any part of the oceanBassnett, Thomas
Science
Outlines of a mechanical theory of storms : $b containing the true law of lunar influence, with practical instructions to the navigator, to enable him approximately to calculate the coming changes of the wind and weather, for any given day, and for any part of the ocean
Bassnett, Thomas
Weather
From the invariability of the axis of rotation, we must conclude that
whatever form is the true form, it is one of equilibrium. In casting our
eyes over the map of the world, we perceive that the surface is very
unequally divided into land and sea; and that the land is very unequally
arranged, both north and south, and east and west. If we compare the
northern and southern hemisphere, we find the land to the water about 3
to 1. If we take the Pacific portion, and consider the north end of New
Zealand as a centre, we can describe a great circle taking in one half
the globe, which shall not include one-tenth of the whole land. Yet the
average height of the remaining nine-tenths, above the level of the sea,
is nearly 1,000 feet. Call this nine-tenths nearly equal to one-fourth
of the whole surface, and the protuberant land in the hemisphere,
opposite the South Pacific, amounts to 1/30,000 part of the whole mass
of the earth, or about 1/700 of the mass of the moon. Again, the mean
density of the earth is about 5½--water being unity,--and the mean
density of the surface land is only about half this: but three-fourths
of the whole surface is water. Hence, we see that the materials of the
interior of the earth must be either metallic or very compressible. To
assign a metallic nucleus to the earth, is repugnant to analogy; and it
is not rendered even probable by facts, as we find volcanic emissions to
contain no heavier elements than the sedimentary layers. Besides, there
are indications of a gradual increase of density downwards, such as
would arise from the compressibility of the layers. Seeing, therefore,
the equilibrium of the whole mass, and the consequent hydrostatic
balance of the land in the sea,--seeing also the small compressibility
of the solid portions, and the great compressibility of the fluid, the
inference is legitimate that the whole is hydrostatically balanced, and
that our globe is a globe of water, with an intermediate shell of land,
specifically lighter than the fluid in which it is suspended. Where this
shell is of great thickness, it penetrates to greater depths, and
attains to greater elevations above the surface of the aqueous globe;
where it is less thick, it is found below the surface, and forms the
bottom of the upper ocean. Recent soundings give much greater depths to
some parts of the ocean, than the most elevated land upon the globe.
Captain Denham, of H. B. M. ship Herald, lately sounded in 37° south and
37° west, and found bottom at 7,706 fathoms, or about nine English
miles.
Public-domain text, read in full here on John Shaqi.
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