# Plutonium-239: Wikis

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# Encyclopedia

Plutonium-239
General
Name, symbol Plutonium-239,239Pu
Neutrons 145
Protons 94
Nuclide data
Half-life 24,110 years
Parent isotopes 243Cm (α)
239Am (EC)
239Np (β)
Decay products 235U
Spin
Decay mode Decay energy
Alpha decay 5.245 MeV

Plutonium-239 is an isotope of plutonium. Plutonium-239 is the primary fissile isotope used for the production of nuclear weapons, although uranium-235 has also been used and is currently the secondary isotope. Plutonium-239 is also one of the three main isotopes demonstrated usable as fuel in nuclear reactors, along with uranium-235 and uranium-233. Plutonium-239 has a half life of 24,110 years.

## Nuclear properties

The nuclear properties of plutonium-239, as well as the ability to produce large amounts of nearly pure plutonium-239, led to its use in nuclear weapons and nuclear power. The fissioning of an atom of uranium-235 in the reactor of a nuclear power plant produces two to three neutrons, and these neutrons can be absorbed by uranium-238 to produce plutonium-239 and other isotopes. Plutonium-239 can also absorb neutrons and fission along with the uranium-235. Plutonium fissions provide about one-third of the total energy produced in a typical commercial nuclear power plant. The use of plutonium-239 in power plants occurs without it ever being removed from the nuclear reactor fuel because it is fissioned in the same fuel rods in which it is produced.

The fission of one atom of Pu-239 generates 207.1 MeV = 3.318 × 10−11 J, i.e. 19.98 TJ/mol = 83.61 TJ/kg.[1]

source Average energy released [MeV]
Instantaneously released energy
Kinetic energy of fission fragments 175.8
Kinetic energy of prompt neutrons     5.9
Energy carried by prompt γ-rays     7.8
Energy from decaying fission products
Energy of β−-particles     5.3
Energy of anti-neutrinos     7.1
Energy of delayed γ-rays     5.2
Sum 207.1
Energy released when those prompt neutrons which don't (re)produce fission are captured   11.5
Energy converted into heat in an operating thermal nuclear reactor 211.5

## Manufacturing

Pu-239 is normally created in nuclear reactors by transmutation of individual atoms of one of the isotopes of uranium present in the fuel rods. Occasionally, when an atom of U-238 is exposed to neutron radiation, its nucleus will capture a neutron, changing it to U-239. This happens more easily with lower Kinetic Energy (as U-238 fission activation is 6.6MeV). The U-239 then rapidly undergoes two beta decays. After the 238U absorbs a neutron to become 239U it then emits an electron and an anti-neutrino ($\bar{\nu}_e$) by β decay to become Neptunium-239 (239Np) and then emits another electron and anti-neutrino by a second β decay to become 239Pu:

$\mathrm\hbox{n}+{{}^2{}^{38}_{92}U}\rightarrow\mathrm{{}^2{}^{39}_{92}U}\rightarrow\mathrm{{}^2{}^{39}_{93}Np}+ e^- + \bar{\nu}_e$

$\mathrm{{}^2{}^{39}_{93}Np}\rightarrow\mathrm{{}^2{}^{39}_{94}Pu}+ e^- + \bar{\nu}_e$

Fission activity is relatively rare, so even after significant exposure, the Pu-239 is still mixed with a great deal of U-238 (and possibly other isotopes of uranium), oxygen, other components of the original material, and fission products. Only if the fuel has been exposed for a few days in the reactor, can the Pu-239 be chemically separated from the rest of the material to yield high-purity Pu-239 metal.

Pu-239 has a higher probability for fission than U-235 and a larger number of neutrons produced per fission event, so it has a smaller critical mass. Pure Pu-239 also has a reasonably low rate of neutron emission due to spontaneous fission (10 fission/s-kg), making it feasible to assemble a supercritical mass before predetonation.

In practice, however, reactor-bred plutonium produced will invariably contain a certain amount of Pu-240 due to the tendency of Pu-239 to absorb an additional neutron during production. Pu-240 has a high rate of spontaneous fission events (415,000 fission/s-kg), making it an undesirable contaminant. As a result, plutonium containing a significant fraction of Pu-240 is not well-suited to use in nuclear weapons; it emits neutron radiation, making handling more difficult, and its presence can lead to a "fizzle" in which a small explosion occurs, destroying the weapon but not causing fission of a significant fraction of the fuel. (However, in modern nuclear weapons using neutron generators for initiation and fusion boosting to supply extra neutrons, fizzling may not be an issue.) It is because of this limitation that plutonium-based weapons must be implosion-type, rather than gun-type. (The US has constructed a single experimental bomb using only reactor-grade plutonium.) Moreover, Pu-239 and Pu-240 cannot be chemically distinguished, so expensive and difficult isotope separation would be necessary to separate them. Weapons-grade plutonium is defined as containing no more than 7% Pu-240; this is achieved by only exposing U-238 to neutron sources for short periods of time to minimize the Pu-240 produced. Pu-240 exposed to alpha particles will incite a nuclear fission.[citation needed]

Plutonium is classified according to the percentage of the contaminant plutonium-240 that it contains:

• Weapons grade less than 7%
• Reactor grade 18% or more.

A nuclear reactor that is used to produce plutonium must therefore have a means for exposing U-238 to neutron radiation and for frequently rotating the fuel. A reactor running on unenriched or moderately enriched uranium naturally contains a great deal of U-238. However, most commercial nuclear power reactor designs require the entire reactor to shut down, often for weeks, in order to change the fuel elements. They therefore produce plutonium in a mix of isotopes that is not well-suited to weapon construction. Such a reactor could have machinery added that would permit U-238 slugs to be placed near the core and changed frequently, or it could be shut down frequently, so proliferation is a concern; for this reason, the International Atomic Energy Agency inspects licensed reactors often. A few commercial power reactor designs, such as the reaktor bolshoy moshchnosti kanalniy (RBMK) and pressurized heavy water reactor (PHWR), do permit refueling without shutdowns, and they may pose a proliferation risk. (In fact, the RBMK was built by the Soviet Union during the cold war, so despite their ostensibly peaceful purpose, it is likely that plutonium production was a design criterion.) By contrast, the Canadian CANDU heavy-water moderated natural-uranium fueled reactor can also be refueled while operating, but it normally consumes most of the Pu-239 it produces in situ; thus, it is not only inherently less proliferative than most reactors, but can even be operated as an "actinide incinerator."[2] (The American IFR (Integral Fast Reactor) can also be operated in an "incineration mode," albeit with substantially more effort and less efficiency than the CANDU.)

Most plutonium is produced in research reactors or plutonium production reactors called breeder reactors because they produce more plutonium than they consume fuel; in principle, such reactors make extremely efficient use of natural uranium. In practice, their construction and operation is sufficiently difficult that they are generally only used to produce plutonium. Breeder reactors are generally (but not always) fast reactors, since fast neutrons are somewhat more efficient at plutonium production.

 Lighter: Plutonium-238 Plutonium-239 is an isotope of Plutonium Heavier: Plutonium-240 Decay product of: Curium-243 (α) Americium-239 (EC) Neptunium-239 (β-) Decay chain of Plutonium-239 Decays to: Uranium-235 (α)