A windmill, such as that in the opening photograph of this chapter, turns in response to a force of high-speed air resistance, $R=\frac{1}{2} D \rho A v^{2}$ . The power available is $9^{p}=R v=$ $\frac{1}{2} D \rho \pi r^{2} v^{3},$ where $v$ is the wind speed and we have assumed a circular face for the windmill, of radius $r$ . Take the drag coefficient as $D=1.00$ and the density of air from the front endpaper. For a home windmill with $r=1.50 \mathrm{m},$ calculate the power available if $(a) v=8.00 \mathrm{m} / \mathrm{s}$ and (b) $v=24.0 \mathrm{m} / \mathrm{s}$ . The power delivered to the generator is limited by the efficiency of the system, which is about 25$\%$ . For comparison, a typical home needs about 3 $\mathrm{kW}$ of electric power.