Experiments and Observations on Different Kinds of AirPriestley, Joseph
History
Experiments and Observations on Different Kinds of Air
Priestley, Joseph
Air -- Early works to 1800; Chemistry -- Early works to 1800
In order to draw air out of a vessel which has its mouth immersed in
water, and thereby to raise the water to whatever height may be
necessary, it is very convenient to make use of a glass _syphon_, fig.
13, putting one of the legs up into the vessel, and drawing the air out
at the other end by the mouth. If the air be of a noxious quality, it
may be necessary to have a syringe fastened to the syphon, the manner of
which needs no explanation. I have not thought it safe to depend upon a
valve at the top of the vessel, which Dr. Hales sometimes made use of.
If, however, a very small hole be made at the top of a glass vessel, it
may be filled to any height by holding it under water, while the air is
issuing out at the hole, which may then be closed with wax or cement.
If the generated air will neither be absorbed by water, nor diminish
common air, it may be convenient to put part of the materials into a
cup, supported by a stand, and the other part into a small glass
vessel, placed on the edge of it, as at _f_, fig. 1. Then having, by
means of a syphon, drawn the air to at convenient height, the small
glass vessel may be easily pushed into the cup, by a wire introduced
through the water; or it may be contrived, in a variety of ways, only to
discharge the contents of the small vessel into the larger. The distance
between the boundary of air and water, before and after the operation,
will shew the quantity of the generated air. The effect of processes
that _diminish_ air may also be tried by the same apparatus.
When I want to admit a particular kind of air to any thing that will not
bear wetting, and yet cannot be conveniently put into a phial, and
especially if it be in the form of a powder, and must be placed upon a
stand (as in those experiments in which the focus of a burning mirror is
to be thrown upon it) I first exhaust a receiver, in which it is
previously placed; and having a glass tube, bended for the purpose, as
in fig. 14, I screw it to the stem of a transfer of the air pump on
which the receiver had been exhausted, and introducing it through the
water into a jar of that kind of air with which I would fill the
receiver, I only turn the cock, and I gain my purpose. In this method,
however, unless the pump be very good, and several contrivances, too
minute to be particularly described, be made use of a good deal of
common air will get into the receiver.
When I want to measure the goodness of any kind of air, I put two
measures of it into a jar standing in water; and when I have marked upon
the glass the exact place of the boundary of air and water, I put to it
one measure of nitrous air; and after waiting a proper time, note the
quantity of its diminution. If I be comparing two kinds of air that are
nearly alike, after mixing them in a large jar, I transfer the mixture
into a long glass tube, by which I can lengthen my scale to what degree
I please.
Public-domain text, read in full here on John Shaqi.
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