COMMUNICATION OF HEAT.
90
portion to the quantity of matter, and consequently to the quantity of
heat, which is to be either communicated or taken away, that it does in
the larger, the quantity of matter being as the cube, and the surface
only as the square of the diameter. And, accordingly, some experiments ¬
made by Sir Iſaac Newton, and by Dr. Martin, agree sufficiently -
with this general rule, which applies equally to all masses of unequal
size, but of the fame matter, and having the fame form, whatever that
be.
This enables us to understand how it happens, that in thoſe arts in
which much heat and fuel are employed, as in the extraction of metals
from their ores, founderies, distilleries, and the like, experience has
ſhewn, that the larger they make their furnaces and stills, and other
such utensils, they do their work with so much the lefs fuel ; for, in
the larger furnaces and stills, and other such utensils, the extent of surface, ¬
communicating with the air, bears a smaller proportion to the
contents of the furnace or still, and to the quantity of fuel employed,
or of heat produced, than in smaller utensils of the fame nature ; and
the waſte of heat is therefore leſs.
We can alfo explain, by the fame general principle, the flowness
with which heat is communicated from one part to another of those
bodies, or afsemblages of bodies, which are uncommonly rare or
spongy, through which it paſses much more flowly than through the
dense and heavy. A thick rod of iron, for example, or copper, if one
end of it be put into the fire, and made red hot, transmits the heat so
quickly, and in such quantity, to the other end, that it cannot be
touched without burning the hand; while a stick of wood of the same
size can easily be held by the one end, while the other is burning.
A piece of cork transmits heat through it still more flowly than the
wood, or is a worse conductor of heat ; and a mass of wool, or feathers,
or furs, excel even the cork in the flowness with which heat is conducted ¬
through them. Such materials compose a mass so spongy and
rare, and between the parts of which there is so little closeness of con¬