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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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368 <strong>Fluid</strong> <strong>Mechanics</strong>, <strong>Thermodynamics</strong> <strong>of</strong> <strong>Turbomachinery</strong><br />

(a)<br />

Direction <strong>of</strong><br />

rotation<br />

(b)<br />

coefficient). CC is a combination <strong>of</strong> both the lift <strong>and</strong> drag coefficients, as described<br />

below:<br />

C = C sina -C<br />

cosa<br />

C L D<br />

Plain<br />

<br />

p<br />

Direction<br />

<strong>of</strong> rotation<br />

Aileron<br />

blade tip<br />

Wind<br />

Balanced<br />

FIG. 10.26. Aileron control surfaces: (a) showing position <strong>of</strong> ailerons on two-bladed<br />

rotor; (b) two types <strong>of</strong> aileron in fully deflected position (adapted from Miller <strong>and</strong><br />

Sirocky 1985).<br />

C L<br />

1.5<br />

1<br />

0.5<br />

–0<br />

0.5<br />

–1<br />

0 deg<br />

–60 deg<br />

–90 deg<br />

0 20 40 60 80 100<br />

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

(a) Lift coefficient<br />

(10.65)<br />

where a = angle <strong>of</strong> attack.<br />

The reason for using C C to describe aileron-control braking effectiveness is that only<br />

the chordwise force produces torque (assuming a wind turbine blade with no pitch or<br />

C D<br />

1.4<br />

1.2<br />

1<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

0<br />

0<br />

p<br />

s<br />

0 deg<br />

–60 deg<br />

–90 deg<br />

20 40 60 80 100<br />

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

(b) Drag coefficient<br />

FIG. 10.27. Variation <strong>of</strong> (a) lift <strong>and</strong> (b) drag coefficients for the 38% chord ailerons<br />

when set at 0, -60 deg <strong>and</strong> at -90 deg. (Adapted from Savino et al. 1985. Courtesy<br />

<strong>of</strong> NASA.)

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