Reactor-grade plutonium (RGPu) is the isotopic grade of plutonium that is found in spent nuclear fuel after the uranium-235 primary fuel that a nuclear power reactor uses has burnt up. The uranium-238 from which most of the plutonium isotopes derive by neutron capture is found along with the U-235 in the low enriched uranium fuel of civilian reactors. In contrast to the low burnup of weeks or months that is commonly required to produce weapons-grade plutonium (WGPu/239Pu), the long time in the reactor that produces reactor-grade plutonium leads to transmutation of much of the fissile, relatively long half-life isotope 239Pu into a number of other isotopes of plutonium that are less fissile or more radioactive. When 239Pu absorbs a neutron, it does not always undergo nuclear fission. Sometimes neutron absorption will instead produce 240Pu at the neutron temperatures and fuel compositions present in typical light water reactors, with the concentration of 240Pu steadily rising with longer irradiation, producing lower and lower grade plutonium as time goes on. Generation II thermal-neutron reactors (today's most numerous nuclear power stations) can reuse reactor-grade plutonium only to a limited degree as MOX fuel, and only for a second cycle. Fast-neutron reactors, of which there are a handful operating today with a half dozen under construction, can use reactor-grade plutonium fuel as a means to reduce the transuranium content of spent nuclear fuel/nuclear waste. Russia has also produced a new type of Remix fuel that directly recycles reactor grade plutonium at 1% or less concentration into fresh or re-enriched uranium fuel imitating the 1% plutonium level of high-burnup fuel.
Classification by isotopic composition
At the beginning of the industrial scale production of plutonium-239 in war era production reactors, trace contamination or co-production with plutonium-240 was initially observed, with these trace amounts resulting in the dropping of the Thin Man weapon-design as unworkable. The difference in purity, of how much, continues to be important in assessing significance in the context of nuclear proliferation and weapons-usability.
The DOE definition of reactor grade plutonium changed in 1976. Before this, three grades were recognised. The change in the definition for reactor grade, from describing plutonium with greater than 7% Pu-240 content prior to 1976, to reactor grade being defined as containing 19% or more Pu-240, coincides with the 1977 release of information about a 1962 "reactor grade nuclear test". The question of which definition or designation applies, that of the old or new scheme, to the 1962 "reactor-grade" test, has not been officially disclosed.
Super weapons grade, less than 3% Pu-240, Weapons grade, less than 7% Pu-240 and Reactor grade, 7% or more Pu-240. From 1976, four grades were recognised:
Super weapons grade, less than 3% Pu-240 Weapons grade, less than 7% Pu-240, Fuel grade, 7% to 19% Pu-240 and Reactor grade, more than 19% Pu-240. Reprocessing or recycling of the spent fuel from the most common class of civilian-electricity-generating or power reactor design, the LWR, (with examples being the PWR or BWR) recovers reactor grade plutonium (as defined since 1976), not fuel grade. The physical mixture of isotopes in reactor-grade plutonium make it extremely difficult to handle and form and therefore explains its undesirability as a weapon-making substance, in contrast to weapons grade plutonium, which can be handled relatively safely with thick gloves. To produce weapons grade plutonium, the uranium nuclear fuel must spend no longer than several weeks in the reactor core before being removed, creating a low fuel burnup. For this to be carried out in a pressurized water reactor - the most common reactor design for electricity generation - the reactor would have to prematurely reach cold shut down after only recently being fueled, meaning that the reactor would need to cool decay heat and then have its reactor pressure vessel be depressurized, followed by a fuel rod defueling. If such an operation were to be conducted, it would be easily detectable, and require prohibitively costly reactor modifications. One example of how this process could be detected in PWRs, is that during these periods, there would be a considerable amount of down time, that is, large stretches of time that the reactor is not producing electricity to the grid. On the other hand, the modern definition of "reactor grade" plutonium is produced only when the reactor is run at high burnups and therefore producing a high electricity generating capacity factor. According to the US Energy Information Administration (EIA), in 2009 the capacity factor of US nuclear power stations was higher than all other forms of energy generation, with nuclear reactors producing power approximately 90.3% of the time and Coal thermal power plants at 63.8%, with down times being for simple routine maintenance and refuelling.
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![Reactor-grade plutonium: An aerial photograph of the Trinity (nuclear test) crater shortly after the test. With an almost identical design to the Fat Man bomb used in Nagasaki, both used what now would be defined as super weapons grade plutonium,[10][11] It employed a natural uranium tamper that contributed approximately 1/4 of the final explosive energy and in total released an estimated energy of 22 kiloton or 22,000 tons of TNT equivalent.[note 1] The smaller crater in the southeast corner was from the earlier calibration test explosion, that used a conventional mass of high explosives of 0.1 kiloton or 108 tons of TNT (450 GJ).](https://upload.wikimedia.org/wikipedia/commons/thumb/0/01/Trinity_crater_%28annotated%29_2.jpg/500px-Trinity_crater_%28annotated%29_2.jpg?utm_source=en.wikipedia.org&utm_campaign=parser&utm_content=thumbnail)

![Reactor-grade plutonium: Separation of uranium and plutonium from spent nuclear fuel by the 1940s-1950s wet-chemical PUREX method.[51] This chemical process is controversial as it is likewise the path that produces chemically pure WGPu.](https://upload.wikimedia.org/wikipedia/commons/thumb/4/4b/Plutonium_and_uranium_extraction_from_nuclear_fuel-eng.svg/1280px-Plutonium_and_uranium_extraction_from_nuclear_fuel-eng.svg.png?utm_source=en.wikipedia.org&utm_campaign=parser&utm_content=thumbnail)
![Reactor-grade plutonium: The 200+ GWd/TU of burnup fuel-cycle,[52]
proposed in the 1990s Integral fast reactor(IFR) concept (color), an animation of the pyroprocessing technology is also available.[53] As opposed to the standard practice worldwide of PUREX separation, plutonium is not separated on its own in this pilot-scale, reprocessing cycle, rather all actinides are "electro-won" or "refined" from the "true waste" of fission products in spent fuel. The plutonium therefore instead comes over mixed with all the gamma and alpha emitting actinides, species that "self-protect" in numerous possible theft scenarios. For a reactor to operate on a full loading of this mixed actinide fuel, Fast neutron-spectrum reactors are without exception, the only variant considered possible.](https://upload.wikimedia.org/wikipedia/commons/thumb/f/fd/Ifr_concept.jpg/500px-Ifr_concept.jpg?utm_source=en.wikipedia.org&utm_campaign=parser&utm_content=thumbnail)

