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WIND ENERGY SYSTEMS - Cd3wd

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Chapter 3—Wind Measurements 3–11<br />

Figure 7: Anemometer response to a step function change in wind speed.<br />

next time constant, τ increases by 0.63 of the amount remaining, and so on until it ultimately<br />

reaches its final value.<br />

During the transient period the anemometer will indicate a wind speed u i different from<br />

the actual ambient wind speed u. This indicated wind speed will be proportional to the<br />

anemometer angular velocity ω.<br />

u i = K i ω (10)<br />

For a cup-type anemometer, the tip speed of the cups will be approximately equal to<br />

the wind speed, which means that K i would be approximately the radius of rotation of the<br />

cup assembly. Propeller type anemometers will have a higher tip speed to wind speed ratio,<br />

perhaps up to a factor of five or six, which means that K i would be proportionately smaller<br />

for this type of anemometer.<br />

At equilibrium, u i = u o and ω = ω o ,so<br />

u o = K i ω o (11)<br />

When Eqs. 10 and 11 are substituted into Eq. 8 we get an expression for the indicated<br />

wind speed u i :<br />

u i = K i ω = K i<br />

[ ωo u i<br />

K i ω o<br />

+(u o − u 1 ) ω o<br />

K i ω o<br />

e −t/τ ]<br />

Wind Energy Systems by Dr. Gary L. Johnson November 12, 2001

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