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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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C C<br />

0.4<br />

0.2<br />

–0<br />

–0.2<br />

–0.4<br />

–0.6<br />

twist). Because <strong>of</strong> this direct relationship between chordwise force <strong>and</strong> rotor torque,<br />

CC serves as a convenient parameter for evaluating an aileron’s braking effectiveness.<br />

Thus, if CC is negative it corresponds to a negative torque producing a rotor<br />

deceleration. Clearly, it is desirable to have a negative value <strong>of</strong> CC available for all<br />

angles <strong>of</strong> attack. Figure 10.28 shows some experimental results, Snyder et al. (1984),<br />

illustrating the variation <strong>of</strong> the chordwise force coefficient with the angle <strong>of</strong> attack, a,<br />

for aileron percent chord <strong>of</strong> 20 <strong>and</strong> 30% for several aileron deflection angles. The<br />

general conclusions to be drawn from these results is that increasing the aileron chord<br />

length <strong>and</strong> the aileron deflection angle contribute to better aerodynamic braking<br />

performance.<br />

Blade tip shapes<br />

–0.8<br />

–10 0 10 20 30 40 50<br />

Angle <strong>of</strong> attack, deg<br />

a = 20% chord<br />

–60 deg<br />

30% chord<br />

–60 deg<br />

30% chord<br />

–90 deg<br />

Wind Turbines 369<br />

FIG. 10.28. Effect <strong>of</strong> chord length on chordwise force coefficient, C C, for a range <strong>of</strong><br />

angles <strong>of</strong> attack. (Adapted from Snyder et al. 1984, unpublished).<br />

The blade geometry determined with various aerodynamic models gives no guidance<br />

<strong>of</strong> an efficient aerodynamic tip shape. From a basic view <strong>of</strong> fluid mechanics, a strong<br />

shed vortex occurs at the blade tip as a result <strong>of</strong> the termination <strong>of</strong> lift <strong>and</strong> this together<br />

with the highly three-dimensional nature <strong>of</strong> the flow at the blade tip causes a loss <strong>of</strong><br />

lift. The effect is exacerbated with a blunt blade end as this increases the intensity <strong>of</strong><br />

the vortex.<br />

Many attempts have been made to improve the aerodynamic efficiency by the addition<br />

<strong>of</strong> various shapes <strong>of</strong> “winglet” at the blade ends. Details <strong>of</strong> field tests on a number<br />

<strong>of</strong> tip shapes intended to improve performance by controlling the shedding <strong>of</strong> the tip<br />

vortex are given by Gyatt <strong>and</strong> Lissaman (1985). According to Tangler (2000), test experience<br />

has shown that rounding the leading-edge corner, Figure 10.29, with a contoured,<br />

streamwise edge (a swept tip) yields good performance. Tip shapes <strong>of</strong> other geometries<br />

are widely used. The sword tip also shown is <strong>of</strong>ten chosen because <strong>of</strong> its low noise<br />

generation, but this is at the expense <strong>of</strong> a reduction in performance.<br />

a

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