Meteorology; or, Weather ExplainedM'Pherson, J. G. (John Gordon)
Science
Meteorology; or, Weather Explained
M'Pherson, J. G. (John Gordon)
Meteorology
Returning to Scotland, he continued his observations at Ben Nevis and at
Kingairloch, opposite Appin, Mr. Rankin using the instrument at the top of
the mountain. These observations showed in general that on the mountain
southerly, south-easterly, and easterly winds were more impregnated with
dust-particles, sometimes containing 133,000 per cubic inch. Northerly
winds brought pure air. The observations at sea-level showed a certain
parallelism to those on the summit of the mountain. With a north-westerly
wind the dust-particles reached the low number of 300 per cubic inch, the
lowest recorded at any low-level station.
The general deductions which he made from his numerous observations during
these two years are that (1) air coming from inhabited districts is always
impure; (2) dust is carried by the wind to enormous distances; (3) dust
rises to the tops of mountains during the day; (4) with much dust there is
much haze; (5) high humidity causes great thickness of the atmosphere, if
accompanied by a great amount of dust, whereas there is no evidence that
humidity alone has any effect in producing thickness; (6) and there is
generally a high amount of dust with high temperature, and a low amount of
dust with low temperature.
CHAPTER VIII
A FOG-COUNTER
Next to the enumeration of the dust-particles in the atmosphere is the
marvellous accuracy of counting the number of particles in a fog. The same
ingenious inventor has constructed a fog-counter for the purpose; and the
number of fog-particles in a cubic inch can be ascertained. This
instrument consists of a glass micrometer divided into squares of a known
size, and a strong microscope for observing the drops on the stage. The
space between the micrometer and the microscope is open, so that the air
passes freely over the stage; and the drops that fall on its surface are
easily seen. These drops are very small; many of them when spread on the
glass are no more than the five-hundredth of an inch in diameter.
In observing these drops, the attention requires to be confined to a
limited area of the stage, as many of the drops rapidly evaporate, some
almost as soon as they touch the glass, whilst the large ones remain a few
seconds.
In one set of Dr. Aitken's observations, in February 1891, the fog was so
thick that objects beyond a hundred yards were quite invisible. The number
of drops falling per second varied greatly from time to time. The greatest
number was 323 drops per square inch in one second. The high number never
lasted for long, and in the intervals the number fell as low as 32, or to
one-tenth.
If we knew the size of these drops, we might be able to calculate the
velocity of their fall, and from that obtain the number in a cubic inch.
Public-domain text, read in full here on John Shaqi.
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