Degrees Equal Parts
of Heat. of Heat.
0 0 Freezing point of water.
1 12 Blood-heat.
2 24 Heat of melting wax.
3 48 Melting point of equal parts of tin and
bismuth.
4 96 Melting point of lead.
5 192 Heat of a small coal-fire.
The first column of this table contains the degrees of heat
in arithmetical progression, and the second in geometrical
progression,—the second degree being twice as great as the first, and
so on. It is obvious from this table, that the heat at which equal
parts of tin and bismuth melt is _four_ times greater than that of
blood-heat, the heat of melting lead _eight_ times greater, and the
heat of a small coal-fire _sixteen_ times greater.
This table was constructed by the help of a thermometer, and of red-hot
iron. By the former he measured all heats as far as that of melting
tin; and by the latter he measured all the higher heats. For the heat
which heated iron loses in a given time is as the total heat of the
iron; and therefore, if the times of cooling are taken equal, the heats
will be in a geometrical progression, and may therefore be easily found
by a table of logarithms.
He found by a thermometer constructed with linseed oil, that if the
oil, when the thermometer was placed in melting snow, occupied a space
of 1000 parts, the same oil, rarefied with _one_ degree of heat, or
that of the human body, occupied a space of 10256; in the heat of water
beginning to boil, a space of 10705; in the heat of water boiling
violently, 10725; in the heat of melted tin beginning to cool, and
putting on the consistency of an amalgam, 11516, and when the tin had
become solid, 11496. Hence the oil was rarefied in the ratio of 40 to
39 by the heat of the human body; of 15 to 14 by the heat of boiling
water; of 15 to 13 in the heat of melting tin beginning to solidify;
and of 23 to 20 in the same tin when solid. The rarefaction of air
was, with the same heat, _ten_ times greater than that of oil, and
the rarefaction of oil _fifteen_ times greater than that of spirit of
wine. By making the heats of oil proportional to its rarefaction, and
by calling the heat of the human body 12 parts, we obtain the heat of
water beginning to boil, 33; of water boiling violently, 34; of melted
tin beginning to solidify, 72; and of the same become solid, 70.
Public-domain text, read in full here on John Shaqi.
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