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al oscillation), it has no known fair weather standard. The point of 30 inches is taken only as it is a mean. I have known it to commence storming when the barometer was at 30.70, and not to fall before it cleared off, below 30.30. And I have known it to be below 30 for several days consecutively, with fair weather. In our climate there is no reliable fair weather standard for the barometer. It falls below 30 without storming; it rises far above, and storms without falling below. No reliance can be placed upon its elevation, except by comparison; but of that hereafter. The general rule, nevertheless, is, that it falls more or less during storms, whatever its height, and rises sooner or later, more or less, after they clear off. The difference between its highest and lowest points is called its range. The greatest range observed, and recorded, is about 3 inches--from about 28 to 31--but this range is rare. The range, in the trade-wind region, is comparatively small; in this country it is greater than in Europe; and, generally, the range will be found greatest where the volume of counter-trade, and magnetic intensity, and the corresponding amount of precipitation, and extremes of heat and cold are greatest. One of the greatest ranges during one storm, or two successive portions of a storm, in this country, which I have seen recorded, occurred at Boston, in February, 1842. It was as follows--counting the hours as 24, and from midnight: Feb. 15..10h..30.36. " 16..13h..28.47 fall of 1.89 in 27 hours. " 17..19h..30.39 rise of 1.92 in 30 hours. " 18.. 2h..30.39 stationary 5 hours. " 19.. 2h..29.46 fall of 0.93 in 24 hours. " 20.. 2h..30.43 rise of 0.97 in 24 hours. Amount of oscillation, 5.71 in 4 days, 11 hours. These ranges were owing to the alternation of S. E. storms, and N. W. winds. Taking the first range as a basis, and allowing the height of the atmosphere to be 1,100 feet for the first inch, we have nearly 2,000 feet displaced during one day, if we look for the displacement near the earth, or some 30 or 35 miles, if we soar aloft in the upper regions to look for the _lateral overflow_ of Professor Dove, and about the same quantity restored the next. This brings us to the inquiry, how was it done? It is perfectly idle to talk about _difference_ of _temperature_ or _tension_ of _vapor_, the _ascent_ of warm air, or _descent_ of cold in a case like this; or to say that th
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