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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> 262<br />

15.4.6 Nuclear Weap<strong>on</strong>s <str<strong>on</strong>g>and</str<strong>on</strong>g> Proliferati<strong>on</strong><br />

Nuclear bombs are the most destructive weap<strong>on</strong>s we have managed<br />

to create. The first bombs from the 1940s were based <strong>on</strong> either highly<br />

235 239<br />

enriched U or <strong>on</strong> Pu. For uranium bombs, the idea is shockingly<br />

simple. Two separate lumps of the bomb material are held apart until<br />

det<strong>on</strong>ati<strong>on</strong> is desired, at which point they are slammed together. 48 It’s not<br />

the collisi<strong>on</strong> that creates the explosi<strong>on</strong>, but a runaway process based <strong>on</strong><br />

having a high c<strong>on</strong>centrati<strong>on</strong> of fissile material <str<strong>on</strong>g>and</str<strong>on</strong>g> no neutr<strong>on</strong> absorbers<br />

present to c<strong>on</strong>trol the resulting chain reacti<strong>on</strong>. The c<strong>on</strong>cept is critical<br />

mass. The combined lump exceeds the critical mass, <str<strong>on</strong>g>and</str<strong>on</strong>g> explodes. 49<br />

As simple as nuclear weap<strong>on</strong>s are to build, the bottleneck becomes<br />

obtaining fissile material. Plut<strong>on</strong>ium does not exist in nature, since its<br />

24,100 yr half-life means nothing is left over from the astrophysical<br />

processes that gave us uranium <str<strong>on</strong>g>and</str<strong>on</strong>g> thorium (Box 15.4). We <strong>on</strong>ly still<br />

have the latter two thanks to their l<strong>on</strong>g half lives. So fissile material has to<br />

start with uranium. But as we have seen, natural uranium is <strong>on</strong>ly 0.72%<br />

235<br />

fissile ( U). In order to be explosive, the uranium must be enriched<br />

235<br />

to at least 20% U, <str<strong>on</strong>g>and</str<strong>on</strong>g> generally much higher (85%). Reactor fuel, at<br />

235<br />

3–5% U will experience meltdown if the critical mass is exceeded,<br />

but will not explode. Enrichment is technically difficult, <str<strong>on</strong>g>and</str<strong>on</strong>g> attempts<br />

to acquire <str<strong>on</strong>g>and</str<strong>on</strong>g> enrich uranium are m<strong>on</strong>itored closely. Often we hear of<br />

countries pursuing uranium enrichment, claiming that they are <strong>on</strong>ly<br />

interested in domestic energy producti<strong>on</strong>—a peaceful purpose. And it<br />

is true that the first step in nuclear power generati<strong>on</strong> is also enrichment.<br />

So it is very difficult to ascertain true intenti<strong>on</strong>s. Once a country has<br />

the ability to enrich uranium enough for a nuclear plant, they can in<br />

principle keep the process running l<strong>on</strong>ger to arrive at weap<strong>on</strong>s-grade<br />

235<br />

U.<br />

48: For plut<strong>on</strong>ium, this process is fouled<br />

by the presence of 240 Pu, forcing a different<br />

approach in which a sphere below critical<br />

mass is imploded to create high density.<br />

49: Never stack lumps of fissile material<br />

together <strong>on</strong> a shelf, or a nasty surprise may<br />

be in store.<br />

235<br />

While we worry about U falling into the wr<strong>on</strong>g h<str<strong>on</strong>g>and</str<strong>on</strong>g>s, perhaps<br />

239 235<br />

more disturbing is Pu. Having a much shorter half-life than U<br />

(24 kyr vs. 704 Myr), it is more dangerous to h<str<strong>on</strong>g>and</str<strong>on</strong>g>le. 50 But plut<strong>on</strong>ium is 50: . . . much higher rate of radioactive decay<br />

otherwise easy to deal with, since it requires no enrichment <str<strong>on</strong>g>and</str<strong>on</strong>g> can be<br />

chemically separated to achieve purity. It is the material of choice for<br />

nuclear weap<strong>on</strong>s.<br />

Serious pursuit of breeder reactors effectively means manufacturing lots<br />

of plut<strong>on</strong>ium, leading to proliferati<strong>on</strong> of nuclear materials: it becomes<br />

harder to track <str<strong>on</strong>g>and</str<strong>on</strong>g> keep away from mal-intenti<strong>on</strong>ed groups. The world<br />

becomes more dangerous under a breeder program. Thorium breeding<br />

233<br />

(Box 15.5) is less risky in this regard because the U prize is mixed with<br />

232<br />

a ridiculously dangerous U isotope that puts plut<strong>on</strong>ium to shame, so<br />

working with it is pretty deadly, which may deter would-be pursuit of<br />

this material by rogue groups.<br />

A related c<strong>on</strong>cern involves proliferati<strong>on</strong> of the abundant radioactive<br />

waste from fissi<strong>on</strong> plants, which could be mixed into c<strong>on</strong>venti<strong>on</strong>al explosives<br />

51 to radioactively c<strong>on</strong>taminate a city or local regi<strong>on</strong>—pois<strong>on</strong>ing<br />

51: . . . called a “dirty bomb”<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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