Langley Memoir on Mechanical Flight, Parts I and II: Smithsonian Contributions to Knowledge, Volume 27 Number 3, Publication 1948, 1911Langley, S. P. (Samuel Pierpont)
History
Langley Memoir on Mechanical Flight, Parts I and II: Smithsonian Contributions to Knowledge, Volume 27 Number 3, Publication 1948, 1911
Langley, S. P. (Samuel Pierpont)
Aeronautics; Flight
No. 5 was tried again on the same day with larger wings, whose area
was 40 square feet. These wings, though stiffer, pocketed a little,
α=20° as before. It flew rapidly, and at first horizontally, to a
distance of 100 feet or more against a five-mile breeze. It then
turned abruptly round through 180°, at first falling (from loss of
headway), then distinctly rising, and at the same time throwing its
head up until it reached an angle of nearly 60° with the vertical,
when it fell backward after a flight of between 6 and 7 seconds. The
wings were evidently not yet strong enough to resist flexure.
November 21. No. 5, in nearly the same condition as before. Two extra
springs had been placed on the launching car, in order to give the
aerodrome a greater initial velocity than before. Everything appeared
favorable, but as it left the launching track a piece flew out of the
port propeller, in spite of which the aerodrome, after dropping 5
feet, rose bodily at an angle of 45° and fell backward into the water
(time, 5 seconds).
Another trial was made the same day with the same aerodrome, under
similar conditions, except that the angle of inclination (α) was
reduced to 7°. It now, with all the other circumstances of launching
like those immediately before, behaved entirely differently, plunging
head downward into the water at a distance of 30 feet. Once more it
was shown beyond dispute that the wings must somehow be made even
stiffer.
December 8. Another trial was undertaken with No. 5, the ‹CG› being
10 cm. in front of the ‹CP› at rest. The root angle of the wings was
18°, tip angle 27°, elevation of midrod 1 in 24. The other changes
made since the previous trial consisted chiefly in the increased
weight due to the longer and stronger frames and shafts that were
made to carry 100 cm. propellers. The flight obtained was so short
that it was as unsatisfactory as before.
The aerodrome rose in the air after leaving the launching apparatus,
and then slid back into the water in the plane of its own wings. On
the first trial, it struck the boat, and was slightly injured; on
the second, with root angle of [p101] wings 10°, tip angle 20°, the
flight partook of the same character, but the machine struck the
water clear of the boat.
The fact that with the ‹CG› 10 cm. in advance of the calculated ‹CP›
the aerodrome steadily rose in front, seems to indicate that the rule
used at that time for calculating the ‹CP› (see Chapter II) was not
very accurate. This rule was based upon the assumption that the tail,
having an area equal to one-third the entire sustaining surface,
supported one-third the total weight (expressed by the formula ‹CP› =
(2‹CP›_{wm} + ‹CP›_{tm})/3, where ‹CP›_{wm} and ‹CP›_{tm} represent
respectively the ‹CP› of the wings and tail in motion), and that the
‹CP› of each surface was one-fifth its width in front of the center
of figure.
Public-domain text, read in full here on John Shaqi.
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