Efficiency of wind turbines A wind turbine converts wind energy into
electrical power. Let \(v_{1}\) equal the upstream velocity of the wind before
it encounters the wind turbine, and let \(v_{2}\) equal the downstream velocity
of the wind after it passes through the area swept out by the turbine blades.
a. Assuming that \(v_{1}>0,\) give a physical explanation to show that \(0 \leq
\frac{v_{2}}{v_{1}} \leq 1\)
b. The amount of power extracted from the wind depends on the ratio
\(r=\frac{v_{2}}{v_{1}},\) the ratio of the downstream velocity to upstream
velocity. Let \(R(r)\) equal the fraction of power that is extracted from the
total available power in the wind stream, for a given value of \(r .\) In about
\(1920,\) the German physicist Albert Betz showed that
\(R(r)=\frac{1}{2}(1+r)\left(1-r^{2}\right),\) where \(0 \leq r \leq 1\) (a
derivation of \(R\) is outlined in Exercise 70 ). Calculate \(R(1)\) and explain
how you could have arrived at this value without using the formula for \(R\).
Give a physical explanation of why it is unlikely or impossible for it to be
the case that \(r=1\)
c. Calculate \(R(0)\) and give a physical explanation of why it is unlikely or
impossible for it to be the case that \(r=0\)
d. The maximum value of \(R\) is called the Betz limit. It represents the
theoretical maximum amount of power that can be extracted from the wind. Find
this value and explain its physical meaning.
(IMAGE CAN'T COPY)