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Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

Fluid Mechanics and Thermodynamics of Turbomachinery, 5e

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

C X<br />

0.8<br />

0.6<br />

0.4<br />

0.2<br />

1<br />

2<br />

C L = 1.0<br />

0.8<br />

0.6<br />

3 4 5 6 7<br />

Tip–speed ratio, J<br />

FIG. 10.17. Variation <strong>of</strong> the axial force coefficient Cx vs tip–speed ratio J for three<br />

values <strong>of</strong> the lift coefficient, C L = 0.6, 0.8 <strong>and</strong> 1.0.<br />

Power coefficient, C P<br />

0.5<br />

0.4<br />

0.3<br />

0.2<br />

0.1<br />

0<br />

1<br />

2<br />

C L = 1.0<br />

0.8<br />

3 4 5 6 7<br />

Tip–speed ratio, J<br />

FIG. 10.18. Variation <strong>of</strong> the power coefficient CP vs J for three values <strong>of</strong> the lift<br />

coefficient, C L = 0.6, 0.8 <strong>and</strong> 1.0.<br />

Rotor optimum design criteria<br />

Glauert’s momentum analysis provides a relatively simple yet accurate framework<br />

for the preliminary design <strong>of</strong> wind turbine rotors. An important aspect <strong>of</strong> the analysis<br />

not yet covered was his development <strong>of</strong> the concept <strong>of</strong> the “ideal windmill” which provides<br />

equations for the optimal rotor. In a nutshell, the analysis gives a preferred value<br />

<strong>of</strong> the product CLl for each rotor blade segment as a function <strong>of</strong> the local speed ratio j<br />

defined by<br />

0.6

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