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Energy and Human Ambitions on a Finite Planet, 2021a

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5 <str<strong>on</strong>g>Energy</str<strong>on</strong>g> <str<strong>on</strong>g>and</str<strong>on</strong>g> Power Units 71<br />

can be used to make steam that drives a turbine (kinetic energy)<br />

that in turn generates electrical energy (voltage, current).<br />

Any of the forms of energy (e.g., in Table 5.2) can c<strong>on</strong>vert into the other,<br />

directly or indirectly. In each c<strong>on</strong>versi<strong>on</strong>, 100% of the energy is accounted<br />

for. In the general case, the energy branches into multiple paths, so we<br />

do not get 100% efficiency into the channel we want. For instance, the<br />

pendulum example above will eventually bleed its energy into stirring<br />

the air (kinetic energy) <str<strong>on</strong>g>and</str<strong>on</strong>g> fricti<strong>on</strong> (heat) at the pivot point. The stirring<br />

air eventually turns to heat via internal (viscous) fricti<strong>on</strong> of the air.<br />

One useful clarificati<strong>on</strong> is that thermal energy is really just r<str<strong>on</strong>g>and</str<strong>on</strong>g>om<br />

moti<strong>on</strong>s—kinetic energy—of individual atoms <str<strong>on</strong>g>and</str<strong>on</strong>g> molecules. So in<br />

the case of nuclear fissi<strong>on</strong> in Example 5.2.1, the initial kinetic energy<br />

of the nuclear fragments is already thermal in nature, but at a higher<br />

temperature (faster speeds) than the surrounding material. By bumping<br />

into surrounding atoms, the excess speed is diffused into the medium,<br />

raising its temperature while “cooling” the fragments themselves as<br />

they are slowed down.<br />

If accounting for all the possible paths 7 of energy, we are c<strong>on</strong>fident<br />

that they always add up. Nothing is lost. 8 <str<strong>on</strong>g>Energy</str<strong>on</strong>g> is never created or<br />

destroyed in any process we study. It just sloshes from <strong>on</strong>e form to<br />

another, often branching into multiple parallel avenues. The sum total<br />

will always add up to the starting amount. Sec. D.2.3 (p. 396) provides a<br />

supplement for those interested in better underst<str<strong>on</strong>g>and</str<strong>on</strong>g>ing where energy<br />

ultimately goes, <str<strong>on</strong>g>and</str<strong>on</strong>g> why “losing energy to heat” is not actually a loss<br />

but just another reservoir for energy.<br />

The differences between kinetic <str<strong>on</strong>g>and</str<strong>on</strong>g> thermal<br />

energy is about coherence, inthatwe<br />

characterize the kinetic energy of a raindrop<br />

by its bulk moti<strong>on</strong> or velocity. Meanwhile,<br />

water molecules within the drop are zipping<br />

about in r<str<strong>on</strong>g>and</str<strong>on</strong>g>om directi<strong>on</strong>s <str<strong>on</strong>g>and</str<strong>on</strong>g> at very high<br />

speeds exceeding 1,000 meters per sec<strong>on</strong>d.<br />

7: . . . sometimes called channels<br />

8: Actually, the principle is so well established<br />

that new particles (like the neutrino)<br />

have been discovered by otherwise unaccounted<br />

energy in nuclear processes.<br />

5.3 Power (W)<br />

Before getting to the various comm<strong>on</strong> units for energy, we should absorb<br />

the very important c<strong>on</strong>cept <str<strong>on</strong>g>and</str<strong>on</strong>g> units of power.<br />

Definiti<strong>on</strong> 5.3.1 Power is simply defined as energy per time: how much<br />

energy is expended in how much time. The SI unit is therefore J/s, which we<br />

rename Watts (W).<br />

One Watt is simply <strong>on</strong>e Joule per sec<strong>on</strong>d.<br />

While energy is the capacity to do work, it says nothing about how<br />

quickly that work might be accomplished. Power addresses the rate at<br />

which energy is expended. Figure 5.2 provides a sense of typical power<br />

levels of familiar animals <str<strong>on</strong>g>and</str<strong>on</strong>g> appliances.<br />

Example 5.3.1 Lifting a 10 kg box, whose weight is therefore about<br />

100 N, through a vertical distance of 2 m requires about 200 J of energy. Weight is mg. In this case, m is 10 kg. If we’re<br />

If performed in <strong>on</strong>e sec<strong>on</strong>d, the task requires 200 W (200 Joules in <strong>on</strong>e being sticklers, g 9.8 m/s 2 , but for c<strong>on</strong>venience<br />

we can typically use g ≈ 10 m/s<br />

sec<strong>on</strong>d). If stretching the same task out over four sec<strong>on</strong>ds, <strong>on</strong>ly 50 W<br />

2<br />

without significant loss of precisi<strong>on</strong>.<br />

is required.<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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