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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> 194<br />

◮ Harnessing wind is relatively low-tech <str<strong>on</strong>g>and</str<strong>on</strong>g> straightforward;<br />

◮ Wind has decent efficiency—typically 40–50%—in extracting energy<br />

from the <strong>on</strong>coming wind;<br />

◮ Life-cycle CO 2 emissi<strong>on</strong>s for wind is <strong>on</strong>ly 2% that of traditi<strong>on</strong>al<br />

fossil fuel electricity [68];<br />

◮ Growth in the wind sector points to ec<strong>on</strong>omic viability;<br />

◮ Wind is able to scale up to cover a meaningful fracti<strong>on</strong> of energy<br />

dem<str<strong>on</strong>g>and</str<strong>on</strong>g>.<br />

[68]: (2020), Life Cycle GHG Emissi<strong>on</strong>s<br />

And the downsides:<br />

◮ Wind is intermittent: power when nature allows, not when people<br />

dem<str<strong>on</strong>g>and</str<strong>on</strong>g>;<br />

◮ Wind is regi<strong>on</strong>ally variable: many places do not produce enough<br />

wind to support development;<br />

◮ Wind can cause envir<strong>on</strong>mental disrupti<strong>on</strong> to habitats—especially<br />

dangerous to birds <str<strong>on</strong>g>and</str<strong>on</strong>g> bats;<br />

◮ Esthetic objecti<strong>on</strong>s to noise <str<strong>on</strong>g>and</str<strong>on</strong>g> degradati<strong>on</strong> of scenery hamper<br />

expansi<strong>on</strong>.<br />

12.5 Problems<br />

1. A modest slap 32 might c<strong>on</strong>sist of about 1 kg of mass moving at 32: ...howpainful can a few Joules be?<br />

2 m/s. How much kinetic energy is this?<br />

2. A hard slap might c<strong>on</strong>sist of about 1 kg of mass moving at 10 m/s.<br />

How much kinetic energy is this, <str<strong>on</strong>g>and</str<strong>on</strong>g> how much warmer would<br />

10 g of skin 33 33: . . . corresp<strong>on</strong>ding to a volume of 10 mL<br />

get if the skin has the heat capacity properties of appropriate to a slap area of 10 cm by 10 cm<br />

water, as in the definiti<strong>on</strong> of a calorie (Sec. 5.5; p. 73 <str<strong>on</strong>g>and</str<strong>on</strong>g> Sec. 6.2; <str<strong>on</strong>g>and</str<strong>on</strong>g> to a depth of 1 mm<br />

p. 85 are relevant)?<br />

3. A 10 kg bowling ball falls from a height of 5 m. Using the c<strong>on</strong>venient<br />

g ≈ 10 m/s 2 , how much gravitati<strong>on</strong>al potential energy does it have?<br />

Just before it hits the ground, all of this potential energy has g<strong>on</strong>e<br />

into kinetic energy. 34 What is the speed of the bowling ball when<br />

it reaches the ground, based <strong>on</strong> kinetic energy?<br />

4. Did the final answer for the speed of the bowling ball at the end of<br />

its drop depend <strong>on</strong> the mass? 35 Write out the math symbolically 36<br />

<str<strong>on</strong>g>and</str<strong>on</strong>g> solve for velocity, v. Does the result depend <strong>on</strong> mass?<br />

5. Thermal energy is just r<str<strong>on</strong>g>and</str<strong>on</strong>g>omized kinetic energy <strong>on</strong> a microscopic<br />

scale. To gain some insight into this, c<strong>on</strong>sider <strong>on</strong>e liter (1 kg) of<br />

water, <str<strong>on</strong>g>and</str<strong>on</strong>g> figure out how much energy it would take to heat it from<br />

absolute zero temperature 37 to 300 K assuming that the definiti<strong>on</strong><br />

of the calorie (Sec. 5.5; p. 73) applies across this entire range. If<br />

this same amount of energy went into kinetic energy—hurling the<br />

water across the room—what would the corresp<strong>on</strong>ding velocity<br />

be?<br />

34: . . . neglecting any energy flow to air<br />

resistance<br />

35: Try it using a different mass.<br />

36: . . . using variables/symbols<br />

37: ...0K,when the kinetic energy is effectively<br />

frozen out, or stopped<br />

i As large as the number is, it is representative<br />

of the speeds of individual molecules<br />

within the water, <str<strong>on</strong>g>and</str<strong>on</strong>g> is, not coincidentally,<br />

similar to the speed of sound in water.<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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