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Energy and Human Ambitions on a Finite Planet, 2021a

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6 Putting Thermal <str<strong>on</strong>g>Energy</str<strong>on</strong>g> to Work 91<br />

between them in some way. They can all have exactly 2.0 units of<br />

energy apiece, or can have individual energies of 1.2, 1.8, <str<strong>on</strong>g>and</str<strong>on</strong>g> 3.0 units;<br />

or 3.2, 0.4, <str<strong>on</strong>g>and</str<strong>on</strong>g> 2.4; or any other of myriad combinati<strong>on</strong>s adding to the<br />

same thing. Entropy provides a measure of how many combinati<strong>on</strong>s 27<br />

are possible.<br />

27: It is far bey<strong>on</strong>d the scope of this book to<br />

detail the counting scheme, but it is perhaps<br />

important to appreciate that energy levels<br />

are discrete—or quantized—which prevents<br />

an infinite number of possible energy combinati<strong>on</strong>s.<br />

0:4 (1) 1:3 (16) 2:2 (36) 3:1 (16) 4:0 (1)<br />

Figure 6.3: A box c<strong>on</strong>taining 4 atoms or molecules of <strong>on</strong>e type (white) <str<strong>on</strong>g>and</str<strong>on</strong>g> 4 of another type (red) has many more c<strong>on</strong>figurati<strong>on</strong>s available<br />

(number in parentheses) when species are equally distributed so that left <str<strong>on</strong>g>and</str<strong>on</strong>g> right sides both have two of each. Entropy is related to the<br />

number of ways a system can distribute itself (at the same energy level), acting to favor disordered mixing over (improbable) orderly<br />

separati<strong>on</strong>.<br />

Example 6.4.3 To better elucidate the c<strong>on</strong>necti<strong>on</strong> between entropy <str<strong>on</strong>g>and</str<strong>on</strong>g><br />

disorder, imagine a box of air, c<strong>on</strong>taining both N 2 <str<strong>on</strong>g>and</str<strong>on</strong>g> O 2 molecules.<br />

As Figure 6.3 illustrates, a thoroughly-mixed arrangement has a larger<br />

number of possible c<strong>on</strong>figurati<strong>on</strong>s, thus the highest entropy. Nature<br />

does not give rise to sp<strong>on</strong>taneous organizati<strong>on</strong> in a closed system. 28<br />

The First Law of Thermodynamics is <strong>on</strong>e we already encountered as<br />

c<strong>on</strong>servati<strong>on</strong> of energy:<br />

28: It is, however, possible to see lowered<br />

entropy in <strong>on</strong>e place if balanced by an increase<br />

elsewhere: life organizes matter, but<br />

at the expense of increased entropy in the<br />

wider universe.<br />

Definiti<strong>on</strong> 6.4.3 First Law of Thermodynamics: the energy of a closed<br />

system is c<strong>on</strong>served, <str<strong>on</strong>g>and</str<strong>on</strong>g> cannot change if nothing—including energy—<br />

enters or leaves the system boundaries.<br />

Now we are ready for the Sec<strong>on</strong>d Law.<br />

Definiti<strong>on</strong> 6.4.4 Sec<strong>on</strong>d Law of Thermodynamics: the total entropy of<br />

a closed system may never decrease.<br />

It is entropy that governs which way heat flows (hot to cold, if left al<strong>on</strong>e)<br />

<str<strong>on</strong>g>and</str<strong>on</strong>g> in a deep sense defines the “arrow of time.”<br />

Box 6.2: The Arrow of Time<br />

C<strong>on</strong>sider that if you were shown videos of a rock splashing into<br />

water, a coffee mug shattering <strong>on</strong> the floor, or an icicle melting, you<br />

would have no difficulty differentiating between the forward <str<strong>on</strong>g>and</str<strong>on</strong>g><br />

reverse playbacks of the video.<br />

The reverse acti<strong>on</strong>, you would c<strong>on</strong>clude, is preposterous <str<strong>on</strong>g>and</str<strong>on</strong>g> can<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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