All About Engines
Forfatter: Edward Cressy
År: 1918
Forlag: Cassell and Company, LTD
Sted: London, New York, Toronto and Melbourne
Sider: 352
UDK: 621 1
With a coloured Frontispiece, and 182 halftone Illustrations and Diagrams.
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How a Modern Engine Works 21
A body or a machine which, as in these examples,
is capable of doing work, is said to possess energy.
Energy due to position, as in the case of the weight,
is called potential energy, and energy due to motion,
as in the case of the grindstone, the mangle, or the
flywheel, is called kinetic energy. The energy stored
up in the gas may, for the present, remain unclassified.
We shall need these ideas later.
Now work may be done quickly, or it may be done
slowly. A thousand ft.-lb. may be done in an hour,
or it may be done in a minute, and the rate of doing
this amount of work is sixty times greater in the
second case than it is in the first. To measure the
rate at which work is done we need a unit, and that
chosen is 33,000 ft.-lb. per minute. It is called a
horse-power, though it would require a pretty strong
horse to raise nearly 15 tons one foot high in one
minute or 1 lb. 33,000 feet high in the same interval
of time. If, therefore, the number of ft.-lb. of work
done in a minute is divided by 33,000 it gives the
rate in horse-power. How, then, is the horse-power
of an engine calculated ?
Consider the piston in the cylinder with the steam
pressing on it, and let the average pressure per
square inch throughout the stroke be represented by
P. If the piston is A square inches in area the total
force acting on it will be P x A. In one stroke of
length L feet, the work done will be P x A x L
ft.-lb., and in N strokes P x A x L x N ft.-lb., or
arranging the letters so that they are easily re-
membered, P.L.A.N. Lastly, since 1 horse-power is