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WIND ENERGY SYSTEMS - Cd3wd

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Chapter 4—Wind Turbine Power 4–24<br />

the average power will be as large as possible for a given turbine area. The capital investment<br />

in the turbine will be proportional to the turbine area so maximizing the average power will<br />

minimize the cost per unit of energy produced. If the rated speed is chosen too low, we will<br />

lose too much of the energy in the higher speed winds. If the rated speed is too high, the<br />

turbine will seldom operate at capacity and will lose too much of the energy in the lower speed<br />

winds. This means that the average power output will reach a maximum at a specific value<br />

of rated wind speed. We can determine this value by evaluating Eq. 30 for various values of<br />

u R and P eR .<br />

We can gain some insight into this design step by normalizing Eq. 30. We first observe<br />

that the quantity inside the brackets of Eq. 30 is called the capacity factor CF. Also called<br />

the plant factor, it is an important design item in addition to the average power.<br />

When we combine Eqs. 15, 16, and 30 we get<br />

ρ<br />

P e,ave = P eR (CF) = η o<br />

2 Au3 R<br />

(CF) W (31)<br />

The choice of rated wind speed will not depend on the rated overall efficiency, the air<br />

density, or the turbine area, so these quantities can be normalized out. Also, since the<br />

capacity factor is expressed entirely in normalized wind speeds, it is convenient to do likewise<br />

in normalizing Eq. 31 by dividing the expression by c 3 to get the term (u R /c) 3 . We therefore<br />

define a normalized average power P N as<br />

P N =<br />

( )<br />

P 3 e,ave<br />

η o (ρ/2)Ac 3 =(CF) uR<br />

(32)<br />

c<br />

Plots of P N are given in Fig. 17 for various values of the Weibull shape parameter k and for<br />

two ratios of cut-in to rated speed. As argued earlier, most turbines will have cut-in speeds<br />

between 0.4 and 0.5 of the rated wind speed, so these plots should bracket the designs of<br />

practical interest.<br />

We see that maximum power is reached at different values of u R /c for different values of<br />

k. For u c =0.5u R , the maximum power point varies from u R /c =1.5to2.5ask decreases<br />

from 2.6 to 1.4. As the cut-in speed is lowered to 0.4u R , the maximum power point varies<br />

from u R /c = 1.6 to 3.0. If k = 2 at a particular site, the optimum value of u R /c is between<br />

1.8 and 2.0. We saw in Chapter 2 that c is usually about 12 percent larger than the mean<br />

wind speed, so the optimum design for energy production is a rated speed of about twice the<br />

mean speed. If the mean wind speed at a site is 6 m/s, then the rated speed of the turbine<br />

should be about 12 m/s.<br />

This design choice only holds for wind regimes where k is about 2. In a trade wind regime,<br />

k will be significantly larger than 2, so a rated speed perhaps 1.3 times the mean speed may<br />

be a better choice in such locations.<br />

We see that the curves for P N<br />

are gently rounded near their maximum values so small<br />

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

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