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Energy and Human Ambitions on a Finite Planet, 2021a

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12 Wind <str<strong>on</strong>g>Energy</str<strong>on</strong>g> 187<br />

able to replace the energy currently derived from fossil fuels.<br />

12.2.1 Wind Turbines<br />

To underst<str<strong>on</strong>g>and</str<strong>on</strong>g> practically-available energy, we back up <str<strong>on</strong>g>and</str<strong>on</strong>g> c<strong>on</strong>sider<br />

how much air hits a wind turbine whose rotor diameter is R. Figure 12.3<br />

illustrates the c<strong>on</strong>cept. If the wind speed is v, the air travels a distance<br />

vΔt in time interval Δt. 9<br />

9: We can pick any value for Δt: a l<strong>on</strong>g<br />

interval makes a very l<strong>on</strong>g cylinder, while a<br />

small Δt results in a short, stubby cylinder.<br />

In the end, the value we chose for Δt will<br />

cancel out, so as not to matter.<br />

v<br />

R<br />

vt<br />

Cylinder volume: R 2 vt<br />

Figure 12.3: Wind power c<strong>on</strong>cept. In time<br />

interval Δt at wind speed v, a volume of<br />

air encounters the rotor having the shape<br />

of a cylinder of radius R <str<strong>on</strong>g>and</str<strong>on</strong>g> length vΔt.<br />

Note that most wind turbines are designed<br />

to pivot about a vertical axis to face into the<br />

wind, whatever the directi<strong>on</strong>.<br />

The cross-secti<strong>on</strong>al area of the wind turbine (rotor) is defined as the<br />

area swept out by the blades, so πR 2 . Thus the volume of the cylinder<br />

of air interacting with the turbine over time interval Δt is the “base”<br />

(circular) area of the cylinder times its “height” (straight length, vΔt),<br />

or V πR 2 vΔt. We know the density of the air, 10 so the mass of the 10: ρ air ≈ 1.25 kg/m 3<br />

cylinder is m ρ air V ρ air πR 2 vΔt. The kinetic energy c<strong>on</strong>tained in this<br />

cylinder of air is therefore K.E. 1 2 mv2 1 2 ρ airπR 2 v 3 Δt. Now let’s get<br />

rid of that pesky Δt. Think for a moment what happens if we divide both<br />

sides by Δt: it will definitely get rid of the Δt <strong>on</strong> the right-h<str<strong>on</strong>g>and</str<strong>on</strong>g>-side, but<br />

what does the left-h<str<strong>on</strong>g>and</str<strong>on</strong>g> side mean: energy over time? Hopefully, this is<br />

familiar by now as the c<strong>on</strong>cept of power.<br />

Table 12.1: Wind power scales as the cube<br />

of wind speed.<br />

Definiti<strong>on</strong> 12.2.1 The power delivered by a wind turbine of radius R in<br />

wind speed v <str<strong>on</strong>g>and</str<strong>on</strong>g> operating at efficiency ε is<br />

P wind 1 2 ερ airπR 2 v 3 . (12.2)<br />

where ρ air ≈ 1.25 kg/m 3 at sea level. Efficiency has been inserted as ε <str<strong>on</strong>g>and</str<strong>on</strong>g><br />

tends to be 40–50% for modern turbines.<br />

Notice that the delivered power scales, sensibly, with the area of the wind<br />

turbine’s blade path, but more importantly <str<strong>on</strong>g>and</str<strong>on</strong>g> perhaps surprisingly<br />

as the velocity cubed (Table 12.1). The cubed part should make you sit<br />

Speed<br />

Power<br />

0 0<br />

1 1<br />

2 8<br />

3 27<br />

4 64<br />

5 125<br />

.<br />

.<br />

10 1,000<br />

© 2021 T. W. Murphy, Jr.; Creative Comm<strong>on</strong>s Attributi<strong>on</strong>-N<strong>on</strong>Commercial 4.0 Internati<strong>on</strong>al Lic.;<br />

Freely available at: https://escholarship.org/uc/energy_ambiti<strong>on</strong>s.

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