Buffon's Natural History. Volume 10 (of 10): Containing a Theory of the Earth, a General History of Man, of the Brute Creation, and of Vegetables, Minerals, &c. &cBuffon, Georges Louis Leclerc, comte de
History
Buffon's Natural History. Volume 10 (of 10): Containing a Theory of the Earth, a General History of Man, of the Brute Creation, and of Vegetables, Minerals, &c. &c
Buffon, Georges Louis Leclerc, comte de
Natural history
heated so as to become white, is still greater, since it requires a
fire continually animated by the bellows to heat it to that degree.
Newton seems to be sensible of this, for he says, that the heat of iron
in that state seems to be seven or eight times greater than that of
boiling water. This diminishes half the heat of this comet, compared to
that of hot iron.
But this diminution, which is only relative, is nothing in itself, nor
nothing in comparison with that real and very great diminution which
results from our first consideration. For the comet to have received
this heat a thousand times greater than that of red-hot iron, it must
have remained a very long time in the vicinity of the sun, whereas it
only passed very rapidly at a small distance. It was on the 8th of
December, 1680, at 6/1000 distance from the earth to the centre of the
sun; but 24 hours before, and as many after, it was at a distance six
times greater, and where the heat was consequently 36 times less.
To know then the quantity of this heat communicated to the comet by the
sun, we here find how we should make this estimation tolerably just,
and, at the same time, make the comparison with hot iron by the means
of my experiments.
We shall suppose, as a fact, that this comet took up 666 hours to
descend from the point where it then was, and which point was at an
equal distance as the earth is from the sun, consequently it received
an equal heat to what the earth receives from that luminary, and which
I here take for unity; we shall likewise suppose that the comet took
666 hours more to ascend from the lowest point of its perihelium to
this same distance; and supposing also its motion uniform, we shall
perceive, that the comet being at the lowest point of its perihelium,
that is, to 6/1000 of the distance from the earth to the sun, the heat
it received in that motion was 27,766 times greater than that the
earth receives. By giving to this motion a duration of 80 minutes,
viz. 40 for its descent, and 40 for its ascent, we shall have, at 6
distance, 27,776 heat during 80 minutes at 7 distance 20,408 heat also
during 80 minutes, and at 8 distance 15,625 heat during 80 minutes, and
thus, successively, to the distance of 1000, where the heat is one. By
summing up the quantity of heat at each distance we shall find 363,410
to be the total of the heat the comet has received from the sun, as
much in descending as in ascending, which must be multiplied by the
time, that is, by four thirds of an hour; we shall then have 484,547,
which divided by 2,000 represents the solid heat the earth received
in this time of 1332 hours, since the distance is always 1,300, and
the heat always equals one. Thus we shall have 242,547/2000 for the
heat the comet received more than the earth during the whole time of
its perihelium instead of 28,000, as Newton supposed it, because he
took only the extreme point, and paid no attention to the very small
duration of time.
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