Gliding 1950 - Lakes Gliding Club
Gliding 1950 - Lakes Gliding Club
Gliding 1950 - Lakes Gliding Club
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FIG. 5<br />
4-<br />
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III I~ If- I~ 18 2.0 1.2 2+<br />
11.<br />
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soaring speed, 8.5 metres per second, was<br />
determined by timing the bird around a<br />
complete circle and measuring the diameter<br />
of the circle in terms ,of the known wing<br />
span of the bird. The lift coefficient ,at this<br />
speed is 1.57, a relatively large value<br />
con~dering the Reynold's number at which<br />
this lift ~urs, namely 140,000.<br />
If the same data shown in Fig. 5 are<br />
plotted in terms of the non-dimensional<br />
coefficients of lift and drag, there results<br />
the so-called drag polar Fig. 6. In this polar<br />
the lift coefficient is plotted as the square<br />
so that th:: drag polar, normally a parabola,<br />
is linearized. 'The reason for the bird's<br />
closing his tip feathers for gliding flight is<br />
immediately apparent from this plot. He<br />
does this to leduce his drag. With slots<br />
open he could not attain a lower drag<br />
coefficient than 0.019, but with the slots<br />
closed he can reach a minimum of 0.0058<br />
in drag coefficient. It is also clear that the<br />
dosing of the tip slots reduces the effective<br />
aspect ratio. At high speeds (Iow lift<br />
coefficients) the bird already has a ver) low<br />
mduced drag and strives rather to reduo:<br />
his parasite drag. Actual measurements of<br />
the induced drag and consequently the<br />
effective aspect ratio can best be done at<br />
lift coefficients much higher than those<br />
measured here. There is still left to be<br />
investigated the region 0.7