Illustrations of the Huttonian Theory of the EarthPlayfair, John
Science
Illustrations of the Huttonian Theory of the Earth
Playfair, John
Geology; Hutton, James, 1726-1797. Theory of the earth
The unstratified, and more crystallized substances, were cast in the
bosom of others, which were solid at the time when they were fluid. In
all this, therefore, there is no indication of a fluidity prevailing
through the whole mass, or even over the whole surface of the earth,
and therefore nothing that can explain the spheroidal figure which it
has acquired. The supposition, then, of the entire body of the earth,
or even of its external crust, having been fluid, though it might
account for the compression at the poles, does not connect that fact
with the other facts in the natural history of the globe, and fails,
therefore, in the point most essential to a theory. It is liable, also,
to other objections, whether it be conceived to have proceeded from
fire or from water; whether it has happened on the principles of Buffon
or of Werner.
431. First, let us suppose that the fluidity of the earth, or of the
external crust of it, at least to a certain depth, proceeded from a
solution of the whole in the waters of the ocean; and, waving all the
objections that have been stated to this hypothesis, on account of
the absolute insolubility of many mineral substances in water, let us
suppose them all soluble in a certain degree, and let us compute the
quantity of the menstruum, which, on the suppositions most favourable
to the system, must have been required to this great geologico-chemical
operation.
The siliceous earth, though not soluble in water _per se_, yet, after
being dissolved in that fluid by means of an alkali, was found by Dr
Black, in his analysis of the Geyser water, to remain suspended in a
quantity of water, between 500 and 1000 times its own weight. This is
one of the facts most favourable to the Neptunian theory; and that
every advantage may be given to that theory, we shall take the least of
the numbers just mentioned, and suppose that siliceous earth may be
dissolved or suspended in 500 times its weight of water.
Taking this for the extreme degree of insolubility of mineral
substances, (though there are many of which the insolubility is
absolute, or, to speak in the language of calculation, infinitely
great,) we may suppose the insolubility of all the rest, or the
quantities of water in which they are dissolved, to be ranged in a
descending scale from 500 to 0, the extreme degree of deliquescence.
Then, taking the arithmetical mean between these extremes, it will give
us 250, as the proportion of water in which mineral substances may at
an average be dissolved. But this average is much less than the truth;
for the quantity of siliceous earth is great in comparison of any of
the rest, and the mineral substances that are extremely soluble in
water are but in a small quantity; therefore, when we suppose mineral
bodies, at a medium, to be soluble in 250 times their own weight of
water, we make a supposition extremely favourable to the Neptunian
system.
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