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WIND ENERGY SYSTEMS - Cd3wd

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Chapter 2—Wind Characteristics 2–47<br />

meantime it appears that either function may yield acceptable results, with the Weibull being<br />

more accurate and the Rayleigh easier to use.<br />

Although the actual wind speed distribution can be described by either a Weibull or a<br />

Rayleigh density function, there are other quantities which are better described by a normal<br />

distribution. The distribution of monthly or yearly mean speeds is likely to be normally<br />

distributed around a long-term mean wind speed, for example. The normal curve is certainly<br />

the best known and most widely used distribution for a continuous random variable, so we<br />

shall mention a few of its properties.<br />

The density function f(u) of a normal distribution is<br />

f(u) = 1<br />

[<br />

]<br />

σ √ 2π exp (u − ū)2<br />

−<br />

2σ 2<br />

(63)<br />

where ū is the mean and σ is the standard deviation. In this expression, the variable u is<br />

allowed to vary from −∞ to +∞. It is physically impossible for a wind speed to be negative,<br />

of course, so we cannot forget the reality of the observed quantity and follow the mathematical<br />

model past this point. This will not usually present any difficulty in examining mean wind<br />

speeds.<br />

The cumulative distribution function F (u) isgivenby<br />

F (u) =<br />

∫ u<br />

−∞<br />

f(x)dx (64)<br />

This integral does not have a simple closed form solution, so tables of values are determined<br />

from approximate integration methods. The variable in this table is usually defined as<br />

q = u − ū or u =ū + qσ (65)<br />

σ<br />

Thus q is the number of standard deviations that u is away from ū. A brief version of this<br />

table is shown in Table 2.4. We see from the table, for example, that F (u) for a wind speed<br />

one standard deviation below the mean is 0.159. This means there is a 15.9 % probability<br />

that the mean speed for any period of interest will be more than one standard deviation below<br />

the long term mean. Since the normal density function is symmetrical, there is also a 15.9<br />

% probability that the mean speed for some period will be more than one standard deviation<br />

above the long term mean.<br />

Wind Energy Systems by Dr. Gary L. Johnson November 20, 2001

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