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Side vi
of the atmospheric pressure of the globe , owing to the comparatively large
number of places from which barometric observations have been obtained , and
to the circumstance that fewer places are required to represent the pressure over
any ...
of the atmospheric pressure of the globe , owing to the comparatively large
number of places from which barometric observations have been obtained , and
to the circumstance that fewer places are required to represent the pressure over
any ...
Side xi
THE WEIGHT OR PRESSURE OF THE ATMOSPHERE , . . . 15 III .
ATMOSPHERIC PRESSURE , ITS DISTRIBUTION OVER THE GLOBE 43 IV .
TEMPERATURE , HOW OBSERVED AND CALCULATED , . . . V .
TEMPERATURE - SOLAR AND ...
THE WEIGHT OR PRESSURE OF THE ATMOSPHERE , . . . 15 III .
ATMOSPHERIC PRESSURE , ITS DISTRIBUTION OVER THE GLOBE 43 IV .
TEMPERATURE , HOW OBSERVED AND CALCULATED , . . . V .
TEMPERATURE - SOLAR AND ...
Side xii
PLATE I . ISOBAROMETRIC LINES SHOWING THE MEAN ATMOSPHERIC
PRESSURE OF THE GLOBE FOR JULY . II . ISOBAROMETRIC LINES
SHOWING THE MEAN ATMOSPHERIC PRESSURE OF THE GLOBE FOR
JANUARY . III .
PLATE I . ISOBAROMETRIC LINES SHOWING THE MEAN ATMOSPHERIC
PRESSURE OF THE GLOBE FOR JULY . II . ISOBAROMETRIC LINES
SHOWING THE MEAN ATMOSPHERIC PRESSURE OF THE GLOBE FOR
JANUARY . III .
Side 15
CHAPTER II . THE WEIGHT OR PRESSURE OF THE ATMOSPHERE . 27 . THE
Barometer is the instrument employed to measure the height of a column of
mercury supported by the pressure of the atmosphere . From this height the
weight of ...
CHAPTER II . THE WEIGHT OR PRESSURE OF THE ATMOSPHERE . 27 . THE
Barometer is the instrument employed to measure the height of a column of
mercury supported by the pressure of the atmosphere . From this height the
weight of ...
Side 16
... if it were composed of layers equally dense throughout . But since , from the
diminished pressure and its great elasticity , air becomes less dense as we
ascend , the real height is very much greater , being , it is supposed , about 210
miles .
... if it were composed of layers equally dense throughout . But since , from the
diminished pressure and its great elasticity , air becomes less dense as we
ascend , the real height is very much greater , being , it is supposed , about 210
miles .
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America amount appear Asia Atlantic atmosphere atmospheric pressure average barometer becomes blow Britain calm causes centre changes charts climate cloud coast cold column compared consequently continued countries course daily diminished direction earth east Edition effect electricity Europe evaporation examined falls feet flow force frequently give given greater greatest heat height Hence higher hour Illustrations important inches increase indicate influence January July land least less light lines lower maximum mean mean temperature mercury Meteorological miles months nearly night northern observations occur ocean passed period Plate position pressure prevail Professor quantity radiation rain rainfall regarded regions relation rises round scale Scotland season seen side soil storms summer surface Table temperature thermometers tion tube upper vapour vols weather whole wind winter
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