In 1919, physicist Alfred Betz argued that the maximum efficiency of a wind turbine is around 59%.

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In 1919, physicist Alfred Betz argued that the maximum efficiency of a wind turbine is around 59%. If wind enters a turbine with speed v1 and exits with speed v2, then the power extracted is the difference in kinetic energy per unit time:

1 P : = =  - 1 2 watts

where m is the mass of wind flowing through the rotor per unit time (Figure 22). Betz assumed that m = ρA(v+ v2)/2, where ρ is the density of air and A is the area swept out by the rotor. Wind flowing undisturbed through the same area A would have mass per unit time ρAvand power P= 1/2 ρAv31. The fraction of power extracted by the turbine is F = P/P0.
(a) Show that F depends only on the ratio r = v2/vand is equal to F(r) = 1/2 (1 − r2)(1 + r), where 0 ≤ r ≤ 1.
(b) Show that the maximum value of F, called the Betz Limit, is 16/27 ≈ 0.59.

(c) Explain why Betz’s formula for F is not meaningful for r close to zero. How much wind would pass through the turbine if vwere zero? Is this realistic?

Figure 22

V1 V2 (A) Wind flowing through a turbine. 0.6 0.5 F 0.4+ 0.3 0.2+ 0.1 0.5 (B) F is the fraction of energy

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Calculus

ISBN: 9781319055844

4th Edition

Authors: Jon Rogawski, Colin Adams, Robert Franzosa

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