Scientific American Supplement, No. 360, November 25, 1882Various
Science
Scientific American Supplement, No. 360, November 25, 1882
Various
Science -- Periodicals
We now know--thanks to the labors of Joule, Lyon Playfair, Clausius,
Tyndall, Helmholtz, etc.--that heat itself is a mode of motion, a form
of convertible energy, which can be made to do useful or productive
work, and be expressed in terms of actual work done. Modern experiment
shows that all our energy is derived from that of food, and, in
particular from the non-nitrogenous part of it, that is, the fat,
starch, and sugar. The nutrition of man is best maintained when he is
provided with a due admixture of all the four classes of aliment which
we have mentioned, and not only that, but he is also better off if he
has a variety of each class. Thus he may and ought to have albumen,
fibrine, gluten, and casein among the albuminates, or at least two of
them; butter and lard, or suet, or oil among the fats; starch of wheat,
potato, rice, peas, etc., and cane-sugar, and milk-sugar among the
carbo-hydrates. The salts cannot be replaced, so far as we know. Life
may be maintained in fair vigor for some time on albuminates only, but
this is done at the expense of the tissues, especially the fat of the
body, and the end must soon come; with fat and carbo hydrates alone
vigor may also be maintained for some time, at the expense of the
tissues also, but the limit is a near one, In either of these cases we
suppose sufficient water and salts to be provided.
We must now inquire into the quantities of food necessary; and this
necessitates a little consideration of the way in which the work of
the body is carried on. We must look upon the human body exactly as a
machine; like an engine with which we are all so familiar. A certain
amount of work requires to be done, say, a certain number of miles of
distance to be traversed; we know that to do this a certain number of
pounds, or hundredweights, or tons of coal must be put into the fire of
the boiler in order to furnish the requisite amount of energy through
the medium of steam. This amount of fuel must bear a certain proportion
to the work, and also to the velocity with which it is done, so both
quantity and time have to be accounted for.
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