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Energy and Human Ambitions on a Finite Planet, 2021a

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15 Nuclear <str<strong>on</strong>g>Energy</str<strong>on</strong>g> 245<br />

Example 15.2.2 What will the fate of<br />

15.4?<br />

8He<br />

be, according to Figure<br />

We can play this chess game! According to the chart, the primary<br />

decay mechanism of He8 is β − with a half-life of about a tenth of a<br />

8<br />

sec<strong>on</strong>d. It will become Li, which hangs around for about a sec<strong>on</strong>d<br />

before undergoing another β − 8<br />

decay to Be. This <strong>on</strong>e lasts almost no<br />

time at all (∼ 10 −16 s) before α decay into two alpha particles (two<br />

4<br />

He). Such a sequence is called a decay chain.<br />

As is evident in Figure 15.8, unstable isotopes above the stable track in<br />

Figure 15.3 tend to undergo β + decays to drive toward stable nuclei,<br />

while those below the track tend to experience β − decays to drive up<br />

toward the stable track. The α decays are more comm<strong>on</strong> for heavy nuclei<br />

(around uranium), which drive toward the end of the train of stable<br />

elements in Figure 15.3, ending up around lead (Pb). We can underst<str<strong>on</strong>g>and</str<strong>on</strong>g><br />

the abundance of lead as a byproduct of heavy-element decay chains.<br />

stable<br />

alpha ()<br />

beta-minus ( – )<br />

beta-plus ( ) or e – capture<br />

sp<strong>on</strong>taneous fissi<strong>on</strong><br />

neutr<strong>on</strong> emissi<strong>on</strong> (n)<br />

prot<strong>on</strong> emissi<strong>on</strong> (p)<br />

Figure 15.8: Another view of the Chart of<br />

the Nuclides, color coded to indicate prevailing<br />

decay modes as a functi<strong>on</strong> of positi<strong>on</strong><br />

<strong>on</strong> the chart. Note that β + sometimes<br />

captures an electr<strong>on</strong> rather than emitting a<br />

positr<strong>on</strong>, but amounting to the same thing,<br />

essentially. From U.S. DoE.<br />

Box 15.1: The Weak Nuclear Force<br />

An aside worth making is that having discussed beta decays, governed<br />

by the weak nuclear force, we have now covered all four<br />

known forces of nature: gravity, electromagnetism, the weak nuclear<br />

force, <str<strong>on</strong>g>and</str<strong>on</strong>g> the str<strong>on</strong>g nuclear force. That’s it: a small menu, really.<br />

The latter three are unified into a St<str<strong>on</strong>g>and</str<strong>on</strong>g>ard Model of Physics, but<br />

gravity—described by General Relativity—has defied all attempts at<br />

“gr<str<strong>on</strong>g>and</str<strong>on</strong>g> unificati<strong>on</strong>,” or a “theory of everything” trying to unite all<br />

four forces under a single theoretical framework. One implicati<strong>on</strong> is<br />

that known physics offers no other “magic” soluti<strong>on</strong>s to our energy<br />

needs. No new forces have come to light in more than half-a-century,<br />

despite dramatic advances in tools to probe the fundamental nature<br />

of physics.<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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