pended from four Hargrave cells to a height of forty-two feet above New York Bay.
The later instance referred to is thoroughly verified and reliable. It is the ascent made by Mr. Charles H. Tamson, near Portland, Maine, on June ]9, 1897, to an elevation of fifty feet with a single kite of the form devised by him. In most other exploits of this kind the aëronaut has been drawn up by a pulley to kites already well poised aloft; but Mr. Lamson
A higher ascent was made early in the autumn of 1897 at Blue Hill, when the leader of a tandem, a Lamson kite, reached an elevation of 11,060 feet (two and a tenth miles), where it was broken by the strong wind. The observatory people now hope that, with the Lamson kite as a leader, they will be able to send their instruments to a much greater height.
The elevation of the kites is determined by the same means used for mountains—the pressure of the atmosphere as recorded in the barometer, and calculations with the angle the kites make with the extremities of a base line. The string has too much indeterminate sag to furnish an accurate measurement.
It has been found that with an increase of altitude a constantly lowering temperature is encountered, except rarely, when there is an overlying warm stratum, ushering in a spell of unseasonably warm weather. At the approach of these warm tides, when the