The average height of the column of mercury in a barometer is about
thirty inches, and, consequently, the whole instrument cannot well be
made less than three feet long, so that when account is taken of the
glass tube, and the amount of mercury it contains, it is long, fragile
and heavy. To avoid the disadvantages inherent in such an instrument,
the method of measuring the pressure of the air by the compression of a
spring holding apart the sides of an air-free flexible metallic box was
devised, and the aneroid barometer invented. The aneroid is graduated
on the dial in “inches,” _i.e._, divisions each of which corresponds to
a change of atmospheric pressure, equal to that measured by one inch of
mercury in a standard barometer. Although a carefully constructed aneroid
is a very useful instrument indeed, it is not to be trusted like a
mercurial barometer kept in a proper place. But a good aneroid is likely
to be much more serviceable to the ordinary traveller on the march than
a standard mercurial barometer, every packing and unpacking of which
exposes it to the risk of breakage, or to the equally fatal risk of air
obtaining access to the vacuous space at the top of the tube. The scale
of a barometer may be divided into millimetres, or, as now recommended
by the British Meteorological Office, into millibars or thousandths of
a hypothetical “atmosphere.” We shall describe the Fortin barometer,
which is best adapted for use at a fixed station, and one devised by
Prof. Collie and Capt. Deasy, which is portable enough for the use of
travellers.
Public-domain text, read in full here on John Shaqi.
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