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Plutonium

What is Plutonium

Plutonium is a transuranic chemical element with atomic number 94, which means there are 94 protons and 94 electrons in the atomic structure. The chemical symbol for plutonium is Pu. It is a manufactured isotope and is created from uranium in nuclear reactors. Therefore we can find this element in irradiated nuclear fuel or as fissile material in nuclear weapons. Scientists have found trace amounts of naturally occurring plutonium. Four isotopes (238Pu, 239Pu, 240Pu, and 244Pu) can be found in nature.

  • Trace amounts of 239Pu originate in radiative capture of neutron on 238U. Free neutrons come from a spontaneous fission reaction of 238U.
  • Trace amounts of 244Pu originate in its relatively long half-life of about 80 million years.
  • The isotope 240Pu is in a decay chain of the isotope 244Pu.  These nuclei are present in the unalterable proportions of the radioactive equilibrium between 244Pu and 240Pu.
  • Extremely small amounts of 238Pu originate in extremely rare double negative beta decay of naturally-occurring isotope 238U.
Fissile / Fertile Material Cross-sectionsFissile / Fertile Material Cross-sections. Comparison of total fission cross-sections.

Source: JANIS (Java-based Nuclear Data Information Software); ENDF/B-VII.1

Plutonium is mostly produced in nuclear reactors. It is a product of the transmutation and subsequent nuclear decay of fertile isotope 238U. The transmutation and decay chain is shown below:

Equation - Plutonium 239 breeding from Uranium 238

Neutron capture may also be used to create fissile 239Pu from 238U, the dominant constituent of naturally occurring uranium (99.28%). Absorption of a neutron in the 238U nucleus yields 239U. The half-life of 239U is approximately 23.5 minutes. 239U decays (negative beta decay) to 239Np (neptunium), whose half-life is 2.36 days. 239Np decays (negative beta decay)  to 239Pu.

Higher isotopes of plutonium (240Pu, 241Pu and 242Pu) are created by also by neutron radiative capture, but in this case an absorber must be the plutonium nucleus. For example, 240Pu which is the second most common isotope, is formed by radiative capture of a neutron by 239Pu.The transmutation and decay chain is shown below.

Plutonium in Commercial Power Reactors

The nuclear transmutation of 238U into fissile isotopes of plutonium (the plutonium breeding) in the fuel cycle of all commercial light water reactors plays a significant role. In recent years, the commercial power industry has been emphasizing high-burnup fuels (up to 60 – 70 GWd/tU), typically enriched to higher percentages of 235U (up to 5%). As burnup increases, a higher percentage of the total power produced in a reactor is due to the plutonium bred inside the reactor.

At a burnup of 30 GWd/tU (gigawatt-days per metric ton of uranium), about 30% of the total energy released comes from bred plutonium. At 40 GWd/tU, that percentage increases to about forty percent. This corresponds to a breeding ratio for these reactors of about 0.4 to 0.5. That means about half of the fissile fuel in these reactors is bred there. This effect extends the cycle length for such fuels to sometimes nearly twice what it would be otherwise. MOX fuel has a smaller breeding effect than 235U fuel and is thus more challenging and slightly less economical to use due to a quicker drop-off in reactivity through cycle life.

plutonium breedingSource of data: JANIS (Java-based Nuclear Data Information Software); The JEFF-3.1.1 Nuclear Data Library

Isotopes of Plutonium

About twenty plutonium isotopes have been discovered and described. Except for 244Pu, all these isotopes are artificial isotopes. The main isotopes, which have to be considered in the fuel cycle of all commercial light water reactors, are:

  • 238Pu. 238Pu belongs to the group of fertile isotopes. 238Pu decays via alpha decay to 234U with a half-life of 87.7 years. 238Pu generates very high decay heat and has a very high rate of spontaneous fission.
  • 239Pu. 239Pu belongs to the group of fissile isotopes. 239Pu decays via alpha decay to 235U with a half-life of 24100 years. This isotope is the principal fissile isotope in use.
  • 240Pu. 240Pu belongs to the group of fertile isotopes. 240Pu decays via alpha decay to 236U with a half-life of 6560 years. 240Pu has a very high rate of spontaneous fission and a high radiative capture cross-section for thermal and resonance neutrons.
  • 241Pu. 241Pu belongs to the group of fissile isotopes. 241Pu decays via negative beta decay to 241Am with a half-life of 14.3 years. This fissile isotope decays to non-fissile isotope with a high radiative capture cross-section for thermal neutrons. An impact on the reactivity of nuclear fuel is obvious.
  • 242Pu. 242Pu belongs to the group of non-fissile isotopes. 242Pu decays via alpha decay to 238U with a half-life of 37300 years. 242Pu has a very high spontaneous fission rate, but its quantity in the irradiated nuclear fuel is relatively low.

The half-life of Isotopes of Plutonium

Isotope Half-life / Decay mode Product
238Pu 87.7 y / alpha decay 234U
239Pu 24 100 y / alpha decay 235U
240Pu 6 560 y / alpha decay 236U
241Pu  14.3 y / beta decay 241Am
242Pu  373 500 y / alpha decay 238U
243Pu  4.96 d / beta decay 243Am
244Pu  80 000 000 y / alpha decay 240Pu
Half-life of plutonium isotopes.Half-lifes of isotopes of plutonium.
Source: Java-based Nuclear Data Information Software
Library: The JEFF-3.1.1 Nuclear Data Library

Isotope

 
Plutonium 239
Fissile / Fertile Material Cross-sections
Source: JANIS (Java-based Nuclear Data Information Software)
Library: ENDF/B-VII.1

239Pu is a fissile isotope, which means 239Pu can undergo fission reaction after absorbing thermal neutron. Moreover, 239Pu meets also alternative requirement that the amount (~2.88 per one fission by thermal neutron) of neutrons produced by fission of 239Pu is sufficient to sustain a nuclear fission chain reaction. This isotope is the principal fissile isotope of plutonium in use.

It is a manufactured isotope and can be found in irradiated uranium fuel or spent uranium fuel. Isotope 239Pu is formed in a nuclear reactor from fertile isotope 238U, constituting more than 95% of uranium fuel (e.g.,, PWRs and BWRs require 3% – 5% of 235U). Absorption of resonance or thermal neutron by the 238U nucleus yields 239U. The half-life of 239U is approximately 23.5 minutes. 239U decays (negative beta decay) to 239Np (neptunium), whose half-life is 2.36 days. 239Np decays (negative beta decay)  to 239Pu. The transmutation and decay chain is shown below:

Equation - Plutonium 239 breeding from Uranium 238

239Pu itself decays via alpha decay into 235U with a half-life of 24 100 years. 239Pu occasionally decays by spontaneous fission with a very low rate of 0.00000000031%. On the other hand, 239Pu has a very high absorption cross-section for thermal neutrons. When loaded into the reactor core, 239Pu can be easily fissioned by a neutron or transformed into the 240Pu via a radiative capture reaction.

See also: Plutonium 239

Plutonium 240
Fissile / Fertile Material Cross-sections
Source: JANIS (Java-based Nuclear Data Information Software)
Library: ENDF/B-VII.1

240Pu is a fertile isotope because its fission cross-section is very low in comparison with fissile isotopes. Radiative capture of a neutron leads to the formation of fissile 241Pu, similarly to 238U, in which radiative capture leads to the formation of fissile 239Pu.

It is a manufactured isotope and can be found in irradiated uranium fuel or spent uranium fuel. Isotope 240Pu is formed in a nuclear reactor from fissile isotope 239Pu. Absorption of resonance or thermal neutron by the 239Pu nucleus yields 240Pu.  Trace amounts can be found in nature. The isotope 240Pu is in a decay chain of the primordial isotope 244Pu.  These nuclei are present in the unalterable proportions of the radioactive equilibrium between 244Pu and 240Pu.

240Pu has a relatively high radiative capture cross-section (about 290 barns for thermal neutrons).

240Pu decays via alpha decay into 236U with a half-life of 6560 years.

Plutonium 241
241Pu is a fissile isotope, which means 241Pu is capable of undergoing fission reaction after absorbing thermal neutron. Moreover, 241Pu also meets the alternative requirement that the amount of neutrons produced by fission of 241Pu (~2.94 per one fission by thermal neutron) is sufficient to sustain a nuclear fission chain reaction. Its fission cross-section for thermal neutrons is about 1012 barns (for 0.025 eV neutron). For fast neutrons, its fission cross-section is on the order of barns.

Most absorption reactions result in fission reactions, but a part of reactions result in radiative capture forming 242Pu. The cross-section for radiative capture for thermal neutrons is about 363 barns (for 0.025 eV neutron). Therefore about 74% of all absorption reactions result in radiative capture of neutrons. About 26% of all absorption reactions result in fission.

It is a manufactured isotope and can be found in irradiated uranium fuel or spent uranium fuel. Isotope 241Pu is formed in a nuclear reactor from fertile isotope 240Pu. Absorption of resonance or thermal neutron by the 240Pu nucleus yields 241Pu.

241Pu decays via beta decay into 241Am with a half-life of only 14.3 years. 241Am has relatively high cross-section for radiative capture for thermal neutrons (~680 barns – 0.025eV). These two phenomena (decrease in fissile isotope and increase in neutron absorber) cause a slight decrease in reactivity of irradiated fuel when stored in a spent fuel pool.

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Uranium

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Nuclear Fuel

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