rger in dimensions than the balloon. This jar is
open at top, and is furnished with the brass cap h i, and stop-cock l
m. One of these slop-cocks is represented separately at Fig. 11.

We first determine the exact capacity of the balloon by filling it with
water, and weighing it both full and empty. When emptied of water, it is
dried with a cloth introduced through its neck d e, and the last
remains of moisture are removed by exhausting it once or twice in an
air-pump.

When the weight of any gas is to be ascertained, this apparatus is used
as follows: Fix the balloon A to the plate of an air-pump by means of
the screw of the stop-cock f g, which is left open; the balloon is to
be exhausted as completely as possible, observing carefully the degree
of exhaustion by means of the barometer attached to the air-pump. When
the vacuum is formed, the stop-cock f g is shut, and the weight of the
balloon determined with the most scrupulous exactitude. It is then fixed
to the jar BCD, which we suppose placed in water in the shelf of the
pneumato chemical apparatus Fig. 1.; the jar is to be filled with the
gas we mean to weigh, and then, by opening the stop-cocks f g and l
m, the gas ascends into the balloon, whilst the water of the cistern
rises at the same time into the jar. To avoid very troublesome
corrections, it is necessary, during this first part of the operation,
to sink the jar in the cistern till the surfaces of the water within the
jar and without exactly correspond. The stop-cocks are again shut, and
the balloon being unscrewed from its connection with the jar, is to be
carefully weighed; the difference between this weight and that of the
exhausted balloon is the precise weight of the air or gas contained in
the balloon. Multiply this weight by 1728, the number of cubical inches
in a cubical foot, and divide the product by the number of cubical
inches contained in the balloon, the quotient is the weight of a cubical
foot of the gas or air submitted to experiment.

Exact account must be kept of the barometrical height and temperature of
the thermometer during the above experiment; and from these the
resulting weight of a cubical foot is easily corrected to the standard
of 28 inches and 10 deg., as directed in the preceding section. The small
portion of air remaining in the balloon after forming the vacuum must
likewise be attended to, which is easily determined by the barometer
attached to the air-pump. If that barome