Energy and Human Ambitions on a Finite Planet, 2021a
Energy and Human Ambitions on a Finite Planet, 2021a
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.