The Steam Engine Familiarly Explained and Illustrated: With an historical sketch of its invention and progressive improvement; its applications to navigation and railways; with plain axioms for railway speculatorsLardner, Dionysius
History
The Steam Engine Familiarly Explained and Illustrated: With an historical sketch of its invention and progressive improvement; its applications to navigation and railways; with plain axioms for railway speculators
Lardner, Dionysius
Steam-engines -- Early works to 1850
In cities and places in which it becomes an object to prevent the
waste of water, the waste-pipes proceeding from the feed-cistern C
(fig. 36.) and from the cold cistern containing the condenser and
air-pump, may be conducted to a cistern A B (fig. 37.). Let C be the
pipe from the feeding cistern, and D that from the cold cistern; by
these pipes the waste water, from both these cisterns is deposited in
A B. In the bottom of A B is a valve V, opening upwards, connected
with a float F. When the quantity of water collected in the cistern A
B is such that the level rises considerably, the float F is raised,
and lifts the valve V, and the water flows into the main pipe, which
supplies water for working the engine: G is the cold water-pump for
the supply of the cold cistern.
This arrangement for saving the water discharged from the feeding and
condensing cisterns has been adopted in the printing office of the
Bank of Ireland, and a very considerable waste of water is thereby
prevented.
(68.) It is necessary to have a ready method of ascertaining at all
times the strength of the steam which is used in working the engine.
For this purpose a bent tube containing mercury is inserted into some
part of the apparatus which has free communication with the steam. It
is usually inserted in the _jacket_ of the cylinder (44.). Let A B C
(fig. 38.) be such a tube. The pressure of the steam forces the
mercury down in the leg A B, and up in the leg B C. If the mercury in
both legs be at exactly the same level, the pressure of the steam must
be exactly equal to that of the atmosphere; because the steam pressure
on the mercury in A B balances the atmospheric pressure on the mercury
in B C. If, however, the level of the mercury in B C be above the
level of the mercury in B A, the pressure of the steam will exceed
that of the atmosphere. The excess of its pressure above that of the
atmosphere may be found by observing the difference of the levels of
the mercury in the tubes B C and B A; allowing a pressure of one pound
on each square inch for every two inches in the difference of the
levels.
If, on the contrary, the level of the mercury in B C should fall below
its level in A B, the atmospheric pressure will exceed that of the
steam, and the degree or quantity of the excess may be ascertained
exactly in the same way.
If the tube be glass, the difference of levels of the mercury would be
visible: but it is most commonly made of iron; and in order to
ascertain the level, a thin wooden rod with a float is inserted in the
open end of B C; so that the portion of the stick within the tube
indicates the distance of the level of the mercury from its mouth. A
bulb or cistern of mercury might be substituted for the leg A B, as in
the common barometer. This instrument is called the STEAM-GAUGE.
Public-domain text, read in full here on John Shaqi.
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