Isotopes of uranium
| |||||||||||||||||||||||||||||||||||||||||||||||||||||||
talk |
---|
Natural uranium consists of three main
Uranium-238 is an
Uranium-235 is important for both
List of isotopes
Nuclide [n 1] |
Historic name |
Z | N | Isotopic mass (Da)[6] [n 2][n 3] |
Half-life[1] |
Daughter isotope [n 5][n 6] |
Natural abundance (mole fraction) | ||||||||||||
---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
Excitation energy[n 8] | Normal proportion[1] | Range of variation | |||||||||||||||||
214U[7] | 92 | 122 | 0.52+0.95 −0.21 ms |
α | 210Th | 0+ | |||||||||||||
215U | 92 | 123 | 215.026720(11) | 1.4(0.9) ms | α | 211Th | 5/2−# | ||||||||||||
β+ ?
|
215Pa | ||||||||||||||||||
216U[8] | 92 | 124 | 216.024760(30) | 2.25+0.63 −0.40 ms |
α | 212Th | 0+ | ||||||||||||
216mU | 2206 keV | 0.89+0.24 −0.16 ms |
α | 212Th | 8+ | ||||||||||||||
217U[9] | 92 | 125 | 217.024660(86)# | 19.3+13.3 −5.6 ms |
α | 213Th | (1/2−) | ||||||||||||
β+? | 217Pa | ||||||||||||||||||
218U[8] | 92 | 126 | 218.023505(15) | 650+80 −70 μs |
α | 214Th | 0+ | ||||||||||||
218mU | 2117 keV | 390+60 −50 μs |
α | 214Th | 8+ | ||||||||||||||
IT? | 218U | ||||||||||||||||||
219U | 92 | 127 | 219.025009(14) | 60(7) μs | α | 215Th | (9/2+) | ||||||||||||
β+? | 219Pa | ||||||||||||||||||
221U | 92 | 129 | 221.026323(77) | 0.66(14) μs | α | 217Th | (9/2+) | ||||||||||||
β+? | 221Pa | ||||||||||||||||||
222U | 92 | 130 | 222.026058(56) | 4.7(0.7) μs | α | 218Th | 0+ | ||||||||||||
β+? | 222Pa | ||||||||||||||||||
223U | 92 | 131 | 223.027961(63) | 65(12) μs | α | 219Th | 7/2+# | ||||||||||||
β+? | 223Pa | ||||||||||||||||||
224U | 92 | 132 | 224.027636(16) | 396(17) μs | α | 220Th | 0+ | ||||||||||||
β+? | 224Pa | ||||||||||||||||||
225U | 92 | 133 | 225.029385(11) | 62(4) ms | α | 221Th | 5/2+# | ||||||||||||
226U | 92 | 134 | 226.029339(12) | 269(6) ms | α | 222Th | 0+ | ||||||||||||
227U | 92 | 135 | 227.0311811(91) | 1.1(0.1) min | α | 223Th | (3/2+) | ||||||||||||
β+? | 227Pa | ||||||||||||||||||
228U | 92 | 136 | 228.031369(14) | 9.1(0.2) min | α (97.5%) | 224Th | 0+ | ||||||||||||
EC (2.5%) | 228Pa | ||||||||||||||||||
229U | 92 | 137 | 229.0335060(64) | 57.8(0.5) min | β+ (80%) | 229Pa | (3/2+) | ||||||||||||
α (20%) | 225Th | ||||||||||||||||||
230U | 92 | 138 | 230.0339401(48) | 20.23(0.02) d | α | 226Th | 0+ | ||||||||||||
SF ? | (various) | ||||||||||||||||||
CD (4.8×10−12%) | 208Pb 22Ne | ||||||||||||||||||
231U | 92 | 139 | 231.0362922(29) | 4.2(0.1) d | EC | 231Pa | 5/2+# | ||||||||||||
α (.004%) | 227Th | ||||||||||||||||||
232U | 92 | 140 | 232.0371548(19) | 68.9(0.4) y | α | 228Th | 0+ | ||||||||||||
CD (8.9×10−10%) | 208Pb 24Ne | ||||||||||||||||||
SF (10−12%) | (various) | ||||||||||||||||||
CD? | 204Hg 28Mg | ||||||||||||||||||
233U | 92 | 141 | 233.0396343(24) | 1.592(2)×105 y | α | 229Th | 5/2+ | Trace[n 9] | |||||||||||
CD (≤7.2×10−11%) | 209Pb 24Ne | ||||||||||||||||||
SF ? | (various) | ||||||||||||||||||
CD ? | 205Hg 28Mg | ||||||||||||||||||
234U[n 10][n 11] | Uranium II | 92 | 142 | 234.0409503(12) | 2.455(6)×105 y | α | 230Th | 0+ | [0.000054(5)][n 12] | 0.000050– 0.000059 | |||||||||
SF (1.64×10−9%) | (various) | ||||||||||||||||||
CD (1.4×10−11%) | 206Hg 28Mg | ||||||||||||||||||
CD (≤9×10−12%) | 208Pb 26Ne | ||||||||||||||||||
CD (≤9×10−12%) | 210Pb 24Ne | ||||||||||||||||||
234mU | 1421.257(17) keV | 33.5(2.0) ms | IT
|
234U | 6− | ||||||||||||||
235U[n 13][n 14][n 15] | Actin Uranium Actino-Uranium |
92 | 143 | 235.0439281(12) | 7.038(1)×108 y | α | 231Th | 7/2− | [0.007204(6)] | 0.007198– 0.007207 | |||||||||
SF (7×10−9%) | (various) | ||||||||||||||||||
CD (8×10−10%) | 215Pb 20Ne | ||||||||||||||||||
CD (8×10−10%) | 210Pb 25Ne | ||||||||||||||||||
CD (8×10−10%) | 207Hg 28Mg | ||||||||||||||||||
235m1U | 0.076737(18) keV | 25.7(1) m | IT | 235U | 1/2+ | ||||||||||||||
235m2U | 2500(300) keV | 3.6(18) ms | SF | (various) | |||||||||||||||
236U | Thoruranium[10] | 92 | 144 | 236.0455661(12) | 2.342(3)×107 y | α | 232Th | 0+ | Trace[n 16] | ||||||||||
SF (9.6×10−8%) | (various) | ||||||||||||||||||
CD (≤2.0×10−11%)[11] | 208Hg 28Mg | ||||||||||||||||||
CD (≤2.0×10−11%)[11] | 206Hg 30Mg | ||||||||||||||||||
236m1U | 1052.5(6) keV | 100(4) ns | IT | 236U | 4− | ||||||||||||||
236m2U | 2750(3) keV | 120(2) ns | IT (87%) | 236U | (0+) | ||||||||||||||
SF (13%) | (various) | ||||||||||||||||||
237U | 92 | 145 | 237.0487283(13) | 6.752(2) d | β−
|
237Np | 1/2+ | Trace[n 17] | |||||||||||
237mU | 274.0(10) keV | 155(6) ns | IT | 237U | 7/2− | ||||||||||||||
238U[n 11][n 13][n 14] | Uranium I | 92 | 146 | 238.050787618(15)[12] | 4.468(3)×109 y | α | 234Th | 0+ | [0.992742(10)] | 0.992739– 0.992752 | |||||||||
SF (5.44×10−5%) | (various) | ||||||||||||||||||
β−β− (2.2×10−10%) | 238Pu | ||||||||||||||||||
238mU | 2557.9(5) keV | 280(6) ns | IT (97.4%) | 238U | 0+ | ||||||||||||||
SF (2.6%) | (various) | ||||||||||||||||||
239U | 92 | 147 | 239.0542920(16) | 23.45(0.02) min | β− | 239Np | 5/2+ | Trace[n 18] | |||||||||||
239m1U | 133.7991(10) keV | 780(40) ns | IT | 239U | 1/2+ | ||||||||||||||
239m2U | 2500(900)# keV | >250 ns | SF? | (various) | 0+ | ||||||||||||||
IT? | 239U | ||||||||||||||||||
240U | 92 | 148 | 240.0565924(27) | 14.1(0.1) h | β− | 240Np | 0+ | Trace[n 19] | |||||||||||
α? | 236Th | ||||||||||||||||||
241U[13] | 92 | 149 | 241.06031(5) | ~40 min[14][15] | β− | 241Np | 7/2+# | ||||||||||||
242U | 92 | 150 | 242.06296(10)[14] | 16.8(0.5) min | β− | 242Np | 0+ | ||||||||||||
This table header & footer: |
- ^ mU – Excited nuclear isomer.
- ^ ( ) – Uncertainty (1σ) is given in concise form in parentheses after the corresponding last digits.
- ^ # – Atomic mass marked #: value and uncertainty derived not from purely experimental data, but at least partly from trends from the Mass Surface (TMS).
- ^
Modes of decay:
CD: Cluster decay EC: Electron capture SF: Spontaneous fission - ^ Bold italics symbol as daughter – Daughter product is nearly stable.
- ^ Bold symbol as daughter – Daughter product is stable.
- ^ ( ) spin value – Indicates spin with weak assignment arguments.
- ^ a b # – Values marked # are not purely derived from experimental data, but at least partly from trends of neighboring nuclides (TNN).
- 237Np
- ^ Used in uranium–thorium dating
- ^ a b Used in uranium–uranium dating
- ^ Intermediate decay product of 238U
- ^ a b Primordial radionuclide
- ^ a b Used in Uranium–lead dating
- ^ Important in nuclear reactors
- ^ Intermediate decay product of 244Pu, also produced by neutron capture of 235U
- 237Np
- ^ Neutron capture product; parent of trace quantities of 239Pu
- ^ Intermediate decay product of 244Pu
Actinides vs fission products
Actinides[16] by decay chain | Half-life range (a) |
|||||||
---|---|---|---|---|---|---|---|---|
4n
|
4n + 1
|
4n + 2
|
4n + 3
|
4.5–7% | 0.04–1.25% | <0.001% | ||
228 Ra№
|
4–6 a
|
155 Euþ
|
||||||
244 Cmƒ
|
241Puƒ | 250 Cf
|
227 Ac№
|
10–29 a
|
90Sr | 85Kr | 113m Cdþ
| |
232Uƒ | 238Puƒ | 243 Cmƒ
|
29–97 a
|
137 Cs
|
151 Smþ
|
121m Sn
| ||
248Bk[18]
|
249 Cfƒ
|
242m Amƒ
|
141–351 a |
No fission products have a half-life | ||||
241Amƒ | 251Cfƒ[19]
|
430–900 a | ||||||
226Ra№ | 247 Bk
|
1.3–1.6 ka | ||||||
240Pu | 229 Th
|
246 Cmƒ
|
243 Amƒ
|
4.7–7.4 ka | ||||
245 Cmƒ
|
250 Cm
|
8.3–8.5 ka | ||||||
239Puƒ | 24.1 ka | |||||||
230 Th№
|
231 Pa№
|
32–76 ka | ||||||
236 Npƒ
|
233Uƒ | 234U№ | 150–250 ka | 99Tc₡ | 126 Sn
| |||
248 Cm
|
242Pu | 327–375 ka | 79Se₡ | |||||
1.53 Ma | 93 Zr
| |||||||
237 Npƒ
|
2.1–6.5 Ma | 135 Cs₡
|
107 Pd
| |||||
236U | 247 Cmƒ
|
15–24 Ma | 129I₡ | |||||
244Pu | 80 Ma |
... nor beyond 15.7 Ma[20] | ||||||
232Th№ | 238U№ | 235Uƒ№ | 0.7–14.1 Ga | |||||
|
Uranium-214
Uranium-214 is the lightest known isotope of uranium. It was discovered at the Spectrometer for Heavy Atoms and Nuclear Structure (SHANS) at the Heavy Ion Research Facility in Lanzhou, China in 2021, produced by firing argon-36 at tungsten-182. It undergoes alpha decay with a half-life of 0.5 ms.[21][22][23][24]
Uranium-232
Uranium-232 has a half-life of 68.9 years and is a side product in the
Uranium-233
Uranium-233 is a fissile isotope of uranium that is bred from thorium-232 as part of the thorium fuel cycle. 233U was investigated for use in nuclear weapons and as a reactor fuel. It was occasionally tested but never deployed in nuclear weapons and has not been used commercially as a nuclear fuel.[27] It has been used successfully in experimental nuclear reactors and has been proposed for much wider use as a nuclear fuel. It has a half-life of around 160,000 years.
Uranium-233 is produced by the neutron irradiation of thorium-232. When thorium-232 absorbs a
Uranium-233 usually fissions on neutron absorption but sometimes retains the neutron, becoming
Uranium-234
234U occurs in natural uranium as an indirect decay product of uranium-238, but makes up only 55 parts per
234U
Extraction of rather small amounts of 234U from natural uranium would be feasible using
234U has a
Uranium-235
Uranium-235 makes up about 0.72% of natural uranium. Unlike the predominant isotope
Uranium-235 has a
Uranium-236
Uranium-236 has a half-life of about 23 million years; and is neither fissile with thermal neutrons, nor very good fertile material, but is generally considered a nuisance and long-lived radioactive waste. It is found in spent nuclear fuel and in the reprocessed uranium made from spent nuclear fuel.
Uranium-237
Uranium-237 has a half-life of about 6.75 days. It decays into
Uranium-238
Uranium-238 (238U or U-238) is the most common
About 99.284% of natural uranium is uranium-238, which has a half-life of 1.41×1017 seconds (4.468×109 years). Depleted uranium has an even higher concentration of 238U, and even low-enriched uranium (LEU) is still mostly 238U. Reprocessed uranium is also mainly 238U, with about as much uranium-235 as natural uranium, a comparable proportion of uranium-236, and much smaller amounts of other isotopes of uranium such as uranium-234, uranium-233, and uranium-232.
Uranium-239
Uranium-239 is usually produced by exposing 238U to
239Np then, with a half-life of about 2.356 days, beta-decays to plutonium-239.
Uranium-241
In 2023, in a paper published in Physical Review Letters, a group of researchers based in Korea reported that they had found uranium-241 in an experiment involving 238U+198Pt multinucleon transfer reactions.[35][36] Its half-life is about 40 minutes.[35]
References
- ^ .
- ^ Magurno, B.A.; Pearlstein, S, eds. (1981). Proceedings of the conference on nuclear data evaluation methods and procedures. BNL-NCS 51363, vol. II (PDF). Upton, NY (USA): Brookhaven National Lab. pp. 835 ff. Retrieved 2014-08-06.
- ^ "Standard Atomic Weights: Uranium". CIAAW. 1999.
- ISSN 1365-3075.
- ^ "Uranium Isotopes". GlobalSecurity.org. Retrieved 14 March 2012.
- .
- S2CID 231627674.
- ^ S2CID 251359451.
- . Retrieved 24 June 2023.
- .
- ^ a b Bonetti, R.; Guglielmetti, A. (2007). "Cluster radioactivity: an overview after twenty years" (PDF). Romanian Reports in Physics. 59: 301–310. Archived from the original (PDF) on 19 September 2016.
- ISSN 2469-9985.
- S2CID 257976576.
- ^ ISSN 0971-751X. Retrieved 2023-04-12.
- ^ Yirka, Bob (April 5, 2023). "Previously unknown isotope of uranium discovered". Phys.org. Retrieved 2023-04-12.
- ^ Plus radium (element 88). While actually a sub-actinide, it immediately precedes actinium (89) and follows a three-element gap of instability after polonium (84) where no nuclides have half-lives of at least four years (the longest-lived nuclide in the gap is radon-222 with a half life of less than four days). Radium's longest lived isotope, at 1,600 years, thus merits the element's inclusion here.
- thermal neutron fission of uranium-235, e.g. in a typical nuclear reactor.
- .
"The isotopic analyses disclosed a species of mass 248 in constant abundance in three samples analysed over a period of about 10 months. This was ascribed to an isomer of Bk248 with a half-life greater than 9 [years]. No growth of Cf248 was detected, and a lower limit for the β− half-life can be set at about 104 [years]. No alpha activity attributable to the new isomer has been detected; the alpha half-life is probably greater than 300 [years]." - sea of instability".
- ^ Excluding those "classically stable" nuclides with half-lives significantly in excess of 232Th; e.g., while 113mCd has a half-life of only fourteen years, that of 113Cd is eight quadrillion years.
- ^ "Physicists Discover New Uranium Isotope: Uranium-214". Sci-News.com. 14 May 2021. Retrieved 15 May 2021.
- S2CID 231627674. Retrieved 15 May 2021.
- ^ "Lightest-known form of uranium created". Live Science. 3 May 2021. Retrieved 15 May 2021.
- ^ "Physicists have created a new and extremely rare kind of uranium". New Scientist. Retrieved 15 May 2021.
- ^ "Uranium 232". Nuclear Power. Archived from the original on 26 February 2019. Retrieved 3 June 2019.
- ^ "INCIDENT NEUTRON DATA". atom.kaeri.re.kr. 2011-12-14.
- ^ C. W. Forsburg; L. C. Lewis (1999-09-24). "Uses For Uranium-233: What Should Be Kept for Future Needs?" (PDF). Ornl-6952. Oak Ridge National Laboratory.
- .
- ^ LCCN 89-25332.
- ^ ISSN 1684-2073.
- .
- PMID 21785255.
- ^ CRC Handbook of Chemistry and Physics, 57th Ed. p. B-345
- ^ CRC Handbook of Chemistry and Physics, 57th Ed. p. B-423
- ^ a b Yirka, Bob; Phys.org. "Previously unknown isotope of uranium discovered". phys.org. Retrieved 2023-04-10.
- S2CID 257976576.