Sounding the Ocean of Air: Being Six Lectures Delivered Before the Lowell Institute of Boston, in December 1898Rotch, Abbott Lawrence
Science
Sounding the Ocean of Air: Being Six Lectures Delivered Before the Lowell Institute of Boston, in December 1898
Rotch, Abbott Lawrence
Atmosphere; Balloons; Clouds; Kites (Meteorology)
will not rise in a suction pump more than thirty-two feet. In 1643
Torricelli executed this famous experiment: he took a glass tube,
sealed at one end, and filled it with mercury, then, closing the open
end with his finger, he inverted it in a basin of mercury. The mercury
fell to about thirty inches, which was recognized to be the weight of
a column having the area of the tube and of the height of the
atmosphere. The application of the barometer was due to Blaise Pascal,
who repeated at Rouen Torricelli's experiment with a much longer tube
filled with water, which being thirteen times lighter than mercury,
stood thirteen times higher, or thirty-two feet, in the tube. Pascal,
being himself at Paris in 1648, got his brother-in-law Perier to carry
a barometric tube filled with mercury to the top of the Puy de DÙme, a
mountain in Auvergne rising about 3500 feet above the city of
Clermont. The mercury fell in the tube with the ascent, and at the top
of the mountain it stood some three inches lower than at the base,
showing that the lower layers of the atmosphere are denser than the
upper. Pascal repeated the experiment on the Tower of St. Jacques in
Paris, and it is interesting to note that more than two hundred years
afterwards, meteorological stations were established both there and on
the Puy de DÙme. It was soon perceived that not only did the level of
the mercury in the tube change with height, but that it oscillated
continually at the same place, and from its observed relation to the
state of the weather its name "weather-glass" is derived. In 1650 the
weight of the air was demonstrated in another manner by Otto von
Guericke, burgomaster of Magdeburg, who by means of an air-pump of his
invention performed the experiment, which Aristotle had tried
unsuccessfully, of weighing a vessel full of air and the same vessel
exhausted of air. He also showed the pressure of the air in all
directions by the famous experiment of the Magdeburg hemispheres,
which, being hollow, were placed together, and after the air was
exhausted from the sphere so formed sixteen horses were unable to pull
them apart. Soon afterwards Robert Boyle experimented further upon the
weight and "spring of the air," as he called it, and gave the name to
the barometer. Both Boyle in England and Mariotte in France discovered
the law, bearing indifferently their names, that the pressure of gases
is proportional to their density. Halley, a few years later, showed
that the rate of decrease in pressure differed from the rate of
increase in height, and developed formulÊ for measuring heights by the
barometer, which were afterwards perfected by Laplace. Knowing the
heights of the barometer at a high and at a low-level station, and the
mean temperature of the air lying between them, it is possible to
compute accurately the difference of height of the two stations, or,
conversely, given this height, the difference in barometric pressure
can be calculated.
Public-domain text, read in full here on John Shaqi.
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