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Gliding 1950 - Lakes Gliding Club

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VUDClrY PIJLAItt· CMMYP$<br />

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A;S~~CT RATIO 5.7<br />

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FIG. 5<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

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