Plutonium-239

Plutonium-239, ²³⁹Pu
	A 99.96% pure ring of plutonium
General
Symbol	239Pu
Names	plutonium-239, 239Pu, Pu-239
Protons (Z)	94
Neutrons (N)	145
Nuclide data
Half-life (t1/2)	24110 years
Isotope mass	239.0521634 Da
Spin	+1⁄2
Parent isotopes	243Cm (α); 239Am (EC); 239Np (β−)
Decay products	235U
Decay modes
Decay mode	Decay energy (MeV)
Alpha decay	5.156
	Isotopes of plutonium ; Complete table of nuclides

Plutonium-239 (²³⁹Pu or Pu-239) is an isotope of plutonium. Plutonium-239 is the primary fissile isotope used for the production of nuclear weapons, although uranium-235 is also used for that purpose. Plutonium-239 is also one of the three main isotopes demonstrated usable as fuel in thermal spectrum nuclear reactors, along with uranium-235 and uranium-233. Plutonium-239 has a half-life of 24,110 years.^[1]

Nuclear properties

The nuclear properties of plutonium-239, as well as the ability to produce large amounts of nearly pure ²³⁹Pu more cheaply than highly enriched weapons-grade uranium-235, led to its use in nuclear weapons and nuclear power plants. 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 in a reactor.

Of all the common nuclear fuels, ²³⁹Pu has the smallest critical mass. A spherical untamped critical mass is about 11 kg (24.2 lbs),^[2] 10.2 cm (4") in diameter. Using appropriate triggers, neutron reflectors, implosion geometry and tampers, the critical mass can be less than half of that.

The fission of one atom of ²³⁹Pu generates 207.1 MeV = 3.318 × 10⁻¹¹ J, i.e. 19.98 TJ/mol = 83.61 TJ/kg,^[3] or about 23 gigawatt hours/kg.

radiation source (thermal fission of ²³⁹Pu)	average energy released [MeV]^[3]
Kinetic energy of fission fragments	175.8
Kinetic energy of prompt neutrons	5.9
Energy carried by prompt γ-rays	7.8
Total instantaneous energy	189.5
Energy of β− particles	5.3
Energy of antineutrinos	7.1
Energy of delayed γ-rays	5.2
Total from decaying fission products	17.6
Energy released by radiative capture of prompt neutrons	11.5
Total heat released in a thermal-spectrum reactor (anti-neutrinos do not contribute)	211.5

Production

Plutonium is made from uranium-238. ²³⁹Pu 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 ²³⁸U is exposed to neutron radiation, its nucleus will capture a neutron, changing it to ²³⁹U. This happens more often with lower kinetic energy (as ²³⁸U fission activation is 6.6MeV). The ²³⁹U then rapidly undergoes two β⁻ decays — an emission of an electron and an anti-neutrino ( ${\bar {\nu }}_{e}$ ), leaving a proton in the nucleus — the first β⁻ decay transforming the ²³⁹U into neptunium-239, and the second β⁻ decay transforming the ²³⁹Np into ²³⁹Pu:

{\ce {{}^{238}_{92}U + {}^{1}_{0}n -> {}^{239}_{92}U ->[\beta^-][23.5\ {\ce {min}}] {}^{239}_{93}Np ->[\beta^-][2.356\ {\ce {d}}] {}^{239}_{94}Pu}}

Fission activity is relatively rare, so even after significant exposure, the ²³⁹Pu is still mixed with a great deal of ²³⁸U (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 ²³⁹Pu be chemically separated from the rest of the material to yield high-purity ²³⁹Pu metal.

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

In practice, however, reactor-bred plutonium will invariably contain a certain amount of ²⁴⁰Pu due to the tendency of ²³⁹Pu to absorb an additional neutron during production. ²⁴⁰Pu 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 ²⁴⁰Pu 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. It is because of this limitation that plutonium-based weapons must be implosion-type, rather than gun-type. Moreover, ²³⁹Pu and ²⁴⁰Pu 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% ²⁴⁰Pu; this is achieved by only exposing ²³⁸U to neutron sources for short periods of time to minimize the ²⁴⁰Pu produced.

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

Supergrade 2–3%
Weapons grade 3–7%
Fuel grade 7–18%
Reactor grade 18% or more

A nuclear reactor that is used to produce plutonium for weapons therefore generally has a means for exposing ²³⁸U to neutron radiation and for frequently replacing the irradiated ²³⁸U with new ²³⁸U. A reactor running on unenriched or moderately enriched uranium contains a great deal of ²³⁸U. 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 ²³⁸U 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. 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 ²³⁹Pu it produces in situ; thus, it is not only inherently less proliferative than most reactors, but can even be operated as an "actinide incinerator".^[4] The American IFR (Integral Fast Reactor) can also be operated in an incineration mode, having some advantages in not accumulating the plutonium-242 isotope or the long-lived actinides, which cannot be easily burned except in a fast reactor. Also IFR fuel has a high proportion of burnable isotopes, while in CANDU an inert material is needed to dilute the fuel; this means the IFR can burn a higher fraction of its fuel before needing reprocessing. 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.

Plutonium-239 is more frequently used in nuclear weapons than uranium-235, as it is easier to obtain in a quantity of critical mass. Both plutonium-239 and uranium-235 are obtained from Natural uranium, which primarily consists of uranium-238 but contains traces of other isotopes of uranium such as uranium-235. The process of enriching uranium, i.e. increasing the ratio of ²³⁵U to ²³⁸U to weapons grade, is generally a more lengthy and costly process than the production of plutonium-239 from ²³⁸U and subsequent reprocessing.

Supergrade plutonium

The "supergrade" fission fuel, which has less radioactivity, is used in the primary stage of US Navy nuclear weapons in place of the conventional plutonium used in the Air Force's versions. "Supergrade" is industry parlance for plutonium alloy bearing an exceptionally high fraction of ²³⁹Pu (>95%), leaving a very low amount of ²⁴⁰Pu, which is a high spontaneous fission isotope (see above). Such plutonium is produced from fuel rods that have been irradiated a very short time as measured in MW-day/ton burnup. Such low irradiation times limit the amount of additional neutron capture and therefore buildup of alternate isotope products such as ²⁴⁰Pu in the rod, and also by consequence is considerably more expensive to produce, needing far more rods irradiated and processed for a given amount of plutonium.

Plutonium-240, in addition to being a neutron emitter after fission, is a gamma emitter, and so is responsible for a large fraction of the radiation from stored nuclear weapons. Whether out on patrol or in port, submarine crew members routinely live and work in very close proximity to nuclear weapons stored in torpedo rooms and missile tubes, unlike Air Force missiles where exposures are relatively brief. The need to reduce radiation exposure justifies the additional costs of the premium supergrade alloy used on many naval nuclear weapons. Supergrade plutonium is used in W80 warheads.

In nuclear power reactors

In any operating nuclear reactor containing ²³⁸U, some plutonium-239 will accumulate in the nuclear fuel.^[5] Unlike reactors used to produce weapons-grade plutonium, commercial nuclear power reactors typically operate at a high burnup that allows a significant amount of plutonium to build up in irradiated reactor fuel. Plutonium-239 will be present both in the reactor core during operation and in spent nuclear fuel that has been removed from the reactor at the end of the fuel assembly's service life (typically several years). Spent nuclear fuel commonly contains about 0.8% plutonium-239.

Plutonium-239 present in reactor fuel can absorb neutrons and fission just as uranium-235 can. Since plutonium-239 is constantly being created in the reactor core during operation, the use of plutonium-239 as nuclear fuel in power plants can occur without reprocessing of spent fuel; the plutonium-239 is fissioned in the same fuel rods in which it is produced. Fissioning of plutonium-239 provides more than one-third of the total energy produced in a typical commercial nuclear power plant.^[6] Reactor fuel would accumulate much more than 0.8% plutonium-239 during its service life if some plutonium-239 were not constantly being "burned off" by fissioning.

A small percentage of plutonium-239 can be deliberately added to fresh nuclear fuel. Such fuel is called MOX (mixed oxide) fuel, as it contains a mixture of uranium dioxide (UO₂) and plutonium dioxide (PuO₂). The addition of plutonium-239 reduces the need to enrich the uranium] in the fuel.

Hazards

Plutonium-239 emits alpha particles to become uranium-235. As an alpha emitter, plutonium-239 is not particularly dangerous as an external radiation source, but if it is ingested or breathed in as dust it is very dangerous and carcinogenic. It has been estimated that a pound (454 grams) of plutonium inhaled as plutonium oxide dust could give cancer to two million people.^[7] However, ingested plutonium is by far less dangerous as only a tiny fraction is absorbed in gastrointestinal tract;^[8]^[9] 800 mg would be unlikely to cause a major health risk as far as radiation is concerned.^[7] As a heavy metal, plutonium is also chemically toxic. See also Plutonium#Precautions.

Weapons grade plutonium (with greater than 90% ²³⁹Pu) is used to make nuclear weapons and has many advantages over other fissile material for that purpose. Lower proportions of ²³⁹Pu would make a reliable weapon design difficult or impossible; this is due to the spontaneous fission (and thus neutron production) of the undesirable ²⁴⁰Pu.

References

^ "Physical, Nuclear, and Chemical Properties of Plutonium". Institute for Energy and Environmental Research. Retrieved 20 November 2015.
^ FAS Nuclear Weapons Design FAQ Archived December 26, 2008, at the Wayback Machine, Accessed 2010-9-2
^ ^a ^b "Table of Physical and Chemical Constants, Sec 4.7.1: Nuclear Fission". Kaye & Laby Online. Archived from the original on 2010-03-05. Retrieved 2009-02-01.
^ Whitlock, Jeremy J. (April 14, 2000). "The Evolution of CANDU Fuel Cycles and their Potential Contribution to World Peace".
^ Hala, Jiri; Navratil, James D. (2003). Radioactivity, Ionizing Radiation, and Nuclear Energy. Brno: Konvoj. p. 102. ISBN 80-7302-053-X.
^ "Information Paper 15: Plutonium". World Nuclear Association. Archived from the original on 30 March 2010. Retrieved 15 July 2020.
^ ^a ^b Cohen, Bernard L. (1990). "Chapter 13, Plutonium and bombs". The Nuclear Energy Option. Plenum Press. ISBN 978-0-306-43567-6.
^ Cohen, Bernard L. (1990). "Chapter 11, HAZARDS OF HIGH-LEVEL RADIOACTIVE WASTE — THE GREAT MYTH". The Nuclear Energy Option. Plenum Press. ISBN 978-0-306-43567-6.
^ Emsley, John (2001). "Plutonium". Nature's Building Blocks: An A–Z Guide to the Elements. Oxford (UK): Oxford University Press. pp. 324–329. ISBN 0-19-850340-7.

External links

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)

[1] "Physical, Nuclear, and Chemical Properties of Plutonium". Institute for Energy and Environmental Research. Retrieved 20 November 2015.

[2] FAS Nuclear Weapons Design FAQ Archived December 26, 2008, at the Wayback Machine, Accessed 2010-9-2

[kayelaby-3] "Table of Physical and Chemical Constants, Sec 4.7.1: Nuclear Fission". Kaye & Laby Online. Archived from the original on 2010-03-05. Retrieved 2009-02-01.

[4] Whitlock, Jeremy J. (April 14, 2000). "The Evolution of CANDU Fuel Cycles and their Potential Contribution to World Peace".

[5] Hala, Jiri; Navratil, James D. (2003). Radioactivity, Ionizing Radiation, and Nuclear Energy. Brno: Konvoj. p. 102. ISBN 80-7302-053-X.

[6] "Information Paper 15: Plutonium". World Nuclear Association. Archived from the original on 30 March 2010. Retrieved 15 July 2020.

[tno_chapter13-7] Cohen, Bernard L. (1990). "Chapter 13, Plutonium and bombs". The Nuclear Energy Option. Plenum Press. ISBN 978-0-306-43567-6.

[8] Cohen, Bernard L. (1990). "Chapter 11, HAZARDS OF HIGH-LEVEL RADIOACTIVE WASTE — THE GREAT MYTH". The Nuclear Energy Option. Plenum Press. ISBN 978-0-306-43567-6.

[Emsley2001-9] Emsley, John (2001). "Plutonium". Nature's Building Blocks: An A–Z Guide to the Elements. Oxford (UK): Oxford University Press. pp. 324–329. ISBN 0-19-850340-7.

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