The principle on which it is constructed may be explained in a few
words, without going into a scientific or too minute detail of its
various parts. The weight of a column of air, which in a common
barometer acts on the mercury, in the aneroid presses on a small
circular metal box, from which nearly all air is extracted; and to this
box is connected, by nice mechanical arrangement, the hand visible over
the face of the instrument. When the atmospheric pressure is lessened on
the vacuum box, a spring acting on levers, turns the hand to the left,
and when the pressure increases, the spring is affected differently, the
hand being turned to the right. It acts in any position, but as it
_often varies several hundredths with such a change_, it should be held
uniformly, while read off.
The known expansion and contraction of metals under varying
temperatures, caused doubts as to the accuracy of the aneroid under such
changes; but they were partly removed by introducing into the vacuum box
a small portion of gas, as a compensation for the effects of heat or
cold. The gas in the box, changing it bulk on a change of temperature,
was intended to compensate for the effect on the metals of which the
aneroid is made. Besides which, a further and more, reliable
compensation has lately been effected by a combination of brass and
steel bars.[35]
METALLIC barometers (in _outer_ shape and size like aneroids) have not
yet been tested adequately in very moist, hot, or cold air for a
sufficient time. They, as well as sympiesometers, are likewise dependent
or secondary instruments, and liable to deterioration. For limited
employment, when sufficiently compared, they may be very useful,
especially in a few cases of electrical changes not foretold or shown by
mercury.
The SYMPIESOMETER is considered to be more sensitive than the marine
barometer, falling sooner, and rising earlier: but this is partly in
consequence of the marine barometer tube being contracted, to prevent
oscillation or "pumping." In the sympiesometer a gas is used, which
presses on the confined surface of the liquid with an uniform pressure
at an equal state of temperature. The liquid is raised or depressed by
an increase or diminution in the density of the atmosphere, and change
of temperature is allowed for, by the sliding scale of the instrument
being always set to agree with the height of the mercury in the attached
thermometer, bringing the _pointer_ on the sliding scale of the
sympiesometer to the same degree on the inverted scale (over which it
slides) as is indicated by the thermometer. The height of the fluid, as
then shown by the sliding scale, indicates the pressure of the
atmosphere.
As the instrument is delicate, great care should be taken, in carrying
or handling, to keep the top always upwards, and to exclude casual rays
of the sun, or a fire, or lamp.
Public-domain text, read in full here on John Shaqi.
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