Conversations on Natural Philosophy, in which the Elements of that Science are Familiarly ExplainedMarcet, Mrs. (Jane Haldimand)
Science
Conversations on Natural Philosophy, in which the Elements of that Science are Familiarly Explained
Marcet, Mrs. (Jane Haldimand)
Physics
_Mrs. B._ I beg your pardon. It is true that there must never be so
great a distance as 32 feet, from the level of the water in the well, to
the valve in the piston, otherwise the water would not rise through that
valve; but when once the water has passed that opening, it is no longer
the pressure of air on the reservoir, which makes it ascend; it is
raised by lifting it up, as you would raise it in a bucket, of which the
piston formed the bottom. This common pump is, therefore, called the
sucking, or lifting pump, as it is constructed on both these principles.
The rod to which the piston is attached, must be made sufficiently long,
to allow the piston to be within 32 feet of the surface of the water in
the well, however deep it may be. There is another sort of pump, called
the forcing pump: it consists of a forcing power, added to the sucking
part of the pump. This additional power, is exactly on the principle of
the syringe: by raising the piston, you draw the water into the pump,
and by causing it to descend, you force the water out.
_Caroline._ But the water must be forced out at the upper part of the
pump; and I cannot conceive how that can be done by the descent of the
piston.
_Mrs. B._ Figure 5, plate 14, will explain the difficulty. The large
pipe, A B, represents the sucking part of the pump, which differs from
the lifting pump, only in its piston P, being unfurnished with a valve,
in consequence of which the water cannot rise above it. When, therefore,
the piston descends, it shuts the valve Y, and forces the water (which
has no other vent) into the pipe D: this is likewise furnished with a
valve V, which, opening upwards, admits the water to pass, but prevents
its return.
The water, is thus first raised in the pump, and then forced into the
pipe, by the alternate ascending, and descending motion of the piston,
after a few strokes of the handle to fill the pipe, from whence the
water issues at the spout.
_Emily._ Does not the air pump, which you used in the experiments, on
pneumatics, operate upon the same principles as the sucking pump?
_Mrs. B._ Exactly. The air pump which I used (plate 1, fig. 2,) has two
hollow, brass cylinders, called barrels, which are made perfectly true.
In each of those barrels, there is a piston; these are worked up, and
down, by the same handle; the pistons, are furnished with valves,
opening upwards, like those of the common pump: there are valves also,
placed at the lower part of each barrel, which open upwards; there are
therefore two pumps, united to produce the same effect: two tubes,
connect these barrels with the plate, upon which I placed the receivers,
which were to be exhausted.
_Emily._ I now understand how the air pump acts; the receiver contains
air, which is exhausted, just as it is by the common pump, before the
water begins to rise.
Public-domain text, read in full here on John Shaqi.
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