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WIND ENERGY SYSTEMS - Cd3wd

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Chapter 4—Wind Turbine Power 4–9<br />

r m ω m to the wind speed u. Thistip speed ratio is defined as<br />

λ = r mω m<br />

(10)<br />

u<br />

where r m is the maximum radius of the rotating turbine in m, ω m is the mechanical angular<br />

velocity of the turbine in rad/s, and u is the undisturbed wind speed in m/s.<br />

The angular velocity ω m is determined from the rotational speed n (r/min) by the equation<br />

ω m = 2πn<br />

60<br />

rad/s (11)<br />

The variation of C p with λ for the Sandia 17-m Darrieus[10] is shown in Fig. 9. This<br />

particular machine will be used for illustration purposes in this chapter. All horizontal axis<br />

propeller turbines and other Darrieus machines will have generally similar curves. This curve<br />

is for a machine similar to the one shown in Fig. 1.5 with the difference being that each blade<br />

has two struts extending from the blade to the center of the vertical shaft. Performance is<br />

somewhat better without the aerodynamic losses introduced by the struts, but this will not<br />

affect our discussion. This particular machine has a rotor diameter of 16.7 m, a rotor height<br />

of 17 m, and a rotor swept area of 187 m 2 .<br />

Figure 9: Coefficient of performance C p versus tip-speed ratio λ for Sandia 17-m Darrieus<br />

turbine. Two blades; 42 r/min.<br />

The size of this machine was chosen on the basis of available aluminum forming equipment<br />

Wind Energy Systems by Dr. Gary L. Johnson November 21, 2001

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