Question 6.10: Average Power in the Wind. Estimate the average power in the......

Average Power in the Wind. Estimate the average power in the wind at a height of 50 m when the windspeed at 10 m averages 6 m/s. Assume Rayleigh statistics, a standard friction coefficient α = 1/7, and standard air density ρ = 1.225 kg/m³.

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We first adjust the winds at 10 m to those expected at 50 m using (6.15):

\left(\frac{v}{v_{0}} \right) \ = \ \left(\frac{H}{H_{0}} \right) ^{\alpha } (6.15)

\bar{v} _{50} \ = \ \bar{v} _{10} \ \left(\frac{H_{50}}{H_{10}} \right) ^{\alpha } \ = \ 6 \ \left(\frac{50}{10} \right) ^{{1}/{7}} \ = \ 7.55 \ {m}/{s}

So, using (6.48), the average wind power density would be

\bar{P} \ = \ \frac{6}{\pi} \ \cdot \ \frac{1}{2} \rho A \bar{v} ^{3} \quad \left(\text{Rayleigh assumptions}\right) (6.48)

\bar{P} _{50} \ = \ \frac{6}{\pi } \ \cdot \ \frac{1}{2} \rho \bar{v} ^{3} \ = \ \frac{6}{\pi } \ \cdot \ \frac{1}{2} \ \cdot \ 1.225 \ \cdot \ \left(7.55\right)^{3} \ = \ 504 \ {W}/{m^{2}}

We also could have found average power at 10 m and then adjust it to 50 m using (6.17):

\left(\frac{P}{P_{0}} \right) \ = \ \left(\frac{{1}/{2} \rho A v^{3}}{{1}/{2} \rho A v^{3}_{0}} \right) \ = \ \left(\frac{v}{v_{0}} \right) \ = \ \left(\frac{H}{H_{0}} \right)^{3\alpha } (6.17)

\begin{matrix} \bar{P}_{10} \ = \ \frac{6}{\pi} \ \cdot \ \frac{1}{2} \cdot \ 1.225 \ \cdot \ 6^{3} \ = \ 252.67 \ {W}/{m^{2}} \quad \quad \quad \quad \quad \\ \bar{P}_{50} \ = \ \bar{P}_{10} \ \left(\frac{H_{50}}{H_{10}}\right)^{3\alpha } \ = \ 252.67 \ \left(\frac{50}{10} \right)^{3\times {1}/{7}} \ = \ 504 \ {W}/{m^{2}} \end{matrix}

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