Uranium-235 (235U) is an isotope of uranium making up about 0.72% of natural uranium. Unlike the predominant isotope uranium-238, it is fissile, i.e., it can sustain a fission chain reaction. It is the only fissile isotope that is primordial and found in relatively significant quantities in nature.
Uranium metal highly enriched in uranium-235
|Isotope mass||235.0439299 u|
|Excess energy||40914.062 ± 1.970 keV|
|Binding energy||1783870.285 ± 1.996 keV|
|Decay mode||Decay energy (MeV)|
|Isotopes of uranium |
Complete table of nuclides
Uranium-235 has a half-life of 703.8 million years. It was discovered in 1935 by Arthur Jeffrey Dempster. Its fission cross section for slow thermal neutrons is about 584.994 barns. For fast neutrons it is on the order of 1 barn. Most but not all neutron absorptions result in fission; a minority result in neutron capture forming uranium-236.
Natural decay chainEdit
The fission of one atom of uranium-235 releases 202.5 MeV = 3.24 × 10−11 J inside the reactor. That corresponds to 19.54 TJ/mol, or 83.14 TJ/kg. This is around 2.5 million times more than the energy released from burning coal. Another 8.8 MeV escapes the reactor as anti-neutrinos. When 235
92U nuclides are bombarded with neutrons, one of the many fission reactions that it can undergo is the following (shown in the adjacent image):
0n + 235
92U → 141
56Ba + 92
36Kr + 3 1
Heavy water reactors, and some graphite moderated reactors, can use natural uranium, but light water reactors must use low enriched uranium because of the higher neutron absorption of light water. Uranium enrichment removes some of the uranium-238 and increases the proportion of uranium-235. Highly enriched uranium (HEU), which contains an even greater proportion of uranium-235, is sometimes used in nuclear submarines and nuclear weapons.
If at least one neutron from uranium-235 fission strikes another nucleus and causes it to fission, then the chain reaction will continue. If the reaction will sustain itself, it is said to be critical, and the mass of U-235 required to produce the critical condition is said to be a critical mass. A critical chain reaction can be achieved at low concentrations of U-235 if the neutrons from fission are moderated to lower their speed, since the probability for fission with slow neutrons is greater. A fission chain reaction produces intermediate mass fragments which are highly radioactive and produce further energy by their radioactive decay. Some of them produce neutrons, called delayed neutrons, which contribute to the fission chain reaction. The power output of nuclear reactors is adjusted by the location of control rods containing elements that strongly absorb neutrons, e.g., boron, cadmium, or hafnium, in the reactor core. In nuclear bombs, the reaction is uncontrolled and the large amount of energy released creates a nuclear explosion.
The Little Boy gun type atomic bomb dropped on Hiroshima on August 6, 1945 was made of highly enriched uranium with a large tamper. The nominal spherical critical mass for an untampered 235U nuclear weapon is 56 kilograms (123 lb), a sphere 17.32 cm (6.8") in diameter. The material must be 85% or more of 235U and is known as weapons grade uranium, though for a crude, inefficient weapon 20% is sufficient (called weapon(s)-usable). Even lower enrichment can be used, but then the required critical mass rapidly increases. Use of a large tamper, implosion geometries, trigger tubes, polonium triggers, tritium enhancement, and neutron reflectors can enable a more compact, economical weapon using one-fourth or less of the nominal critical mass, though this would likely only be possible in a country that already had extensive experience in engineering nuclear weapons. Most modern nuclear weapon designs use plutonium-239 as the fissile component of the primary stage, however HEU is often used in the secondary stage.
|Source||Average energy released [MeV]|
|Instantaneously released energy|
|Kinetic energy of fission fragments||169.1|
|Kinetic energy of prompt neutrons||4.8|
|Energy carried by prompt γ-rays||7.0|
|Energy from decaying fission products|
|Energy of β−-particles||6.5|
|Energy of delayed γ-rays||6.3|
|Energy released when those prompt neutrons which don't (re)produce fission are captured||8.8|
|Total energy converted into heat in an operating thermal nuclear reactor||202.5|
|Energy of anti-neutrinos||8.8|
- ""Some Physics of Uranium", UIC.com.au". Archived from the original on July 17, 2007. Retrieved 2009-01-18. Cite uses deprecated parameter
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- Nuclear fission and fusion, and neutron interactions, National Physical Laboratory.
- Energy Content in Common Energy Sources, EngineeringToolBox.com.
- FAS Nuclear Weapons Design FAQ, accessed 2010-9-2. There are numerous other references on the net, and with modern computers, this is fairly easy to calculate, so secrecy cannot aid security.
- FAS contributors (ed.). Nuclear Weapon Design. Federation of American Scientists.
- Miner, William N.; Schonfeld, Fred W. (1968). "Plutonium". In Clifford A. Hampel (ed.). The Encyclopedia of the Chemical Elements. New York (NY): Reinhold Book Corporation. p. 541. LCCN 68029938.
- Schmidt, Glen (February 2011). "SNAP Overview – general background" (PDF). American Nuclear Society. Retrieved 27 August 2012.
- "RORSAT (Radar Ocean Reconnaissance Satellite)". daviddarling.info.
- Table of Nuclides.
- DOE Fundamentals handbook: Nuclear Physics and Reactor theory Vol. 1, Vol. 2.
- Uranium | Radiation Protection Program | US EPA
- NLM Hazardous Substances Databank - Uranium, Radioactive
- "The Miracle of U-235", Popular Mechanics, January 1941—one of the earliest articles on U-235 for the general public
|Uranium-235 is an
isotope of uranium
|Decay product of:
|Decays to: |