
- Order:
- Duration: 2:12
- Published: 18 Oct 2008
- Uploaded: 22 Jul 2011
- Author: oceanospotamos
Due to the age of the Earth of , this means that the half-life of the given nuclides must be greater than about for practical considerations. E.g. for a nuclide with half-life , this means 77 half-lives have elapsed, meaning that for each mole () of that nuclide being present at the formation of earth, only 6 atoms remain today.
The shortest-lived isotopes (i.e. isotopes with shortest half-lives) in the list of 33 radioactive primordial nuclides are: : ..., , , , , and . These are the 6 nuclides with half-lives comparable to, or less than, the estimated age of the universe. For a complete list of the 33 known primordial radionuclides, including the next 27 with half-lives much longer than the age of the universe, see the complete list in the section below.
The next longest-living nuclide after the end of the list given in the table is niobium-92 with a half-life of . (See list of nuclides for the list of all nuclides with half-lives longer than 60 minutes.) To be detected primordially, 92Nb would have to survive at least 132 half-lives since the Earth's formation, meaning its original concentration will have decreased by a factor of 1040. To date, it has not been detected. It has been found that the next longer-lived nuclide, , with a half-life of is primordial, although just barely, as its concentration in a few ores is nearly 10−18 weight parts. Taking into account that all these nuclides must exist since at least , meaning survive 57 half-lives, their original number is now reduced by a factor of 257 which equals more than 1017.
Although it is estimated that about 33 primordial nuclides are radioactive (list below), it becomes very difficult to determine the exact total number of radioactive primoridals, because the total number of stable nuclides is uncertain. There exist many extremely long-lived isotopes whose half-lives are still unknown. For example, it is known theoretically that all isotopes of tungsten, including those indicated by even the most modern empirical methods to be stable, must be radioactive and can decay by alpha emission, but this could only be measured experimentally for . Nevertheless, the number of nuclides with half-lives so long that they cannot be measured with present instruments—and are considered from this viewpoint to be stable nuclides—is limited. Even when a "stable" nuclide is found to be radioactive, the fact merely moves it from the stable to the unstable list of primordial nuclides, and the total number of primordial nuclides remains unchanged.
There are about 51 nuclides which are radioactive and exist naturally on Earth but are not primordial (making a total of fewer than 340 total nuclides to be found naturally on Earth).
; nuclide column Nuclide identifiers are given by their mass number A and the symbol for the corresponding chemical element (implies a unique proton number). In the rare case that this is not the ground state, this is indicated by a m for metastable appended to the mass number.
; energy column The column labeled "energy" denotes the mass of the average nucleon of this nuclide relative to the mass of a neutron (so all nuclides get a positive value) in MeV, formally: .
; half-life column All times are given in seconds ( = 1 year).
; decay mode column
α | α decay |
β− | β− decay |
K | electron capture |
KK | double electron capture |
β+ | β+ decay |
SF | spontaneous fission |
2 | double β− decay |
β+β+ | double β+ decay |
I | isomeric transition |
p | proton emission |
n | neutron emission |
; decay energy column Multiple values for (maximal) decay energy are mapped to decay modes in their order.
{| class="wikitable sortable" style="text-align:right" !no!!nuclide!!energy!!half-life (seconds)!!decay mode!!decay energy (MeV)!!approx ratio half-life to age of universe |- ||256||128Te||8.743261||||align=center|2 ||align=center|2.530||align=center|160 million million |- ||257||76Ge||9.034656||||align=center|2 ||align=center|2.039||align=center|130,000 million |- ||258||82Se||9.017596||||align=center|2 ||align=center|2.995||align=center|8,000 million |- ||259||116Cd||8.836146||||align=center|2 ||align=center|2.809||align=center|2,000 million |- ||260||48Ca||8.992452||||align=center|2 β− ||align=center|4.274 , 0.0058||align=center|2,000 million |- ||261||96Zr||8.961359||||align=center|2 β− ||align=center|3.4||align=center|1,000 million |- ||262||209Bi||8.158689||||align=center|α ||align=center|3.137||align=center|1,000 million |- ||263||130Te||8.766578||||align=center|2 ||align=center|0.868||align=center|600 million |- ||264||150Nd||8.562594||||align=center|2 ||align=center|3.367||align=center|600 million |- ||265||100Mo||8.933167||||align=center|2 ||align=center|3.035||align=center|600 million |- ||266||151Eu||8.565759||||align=center|α ||align=center|1.9644||align=center|300 million |- ||267||180W||8.347127||||align=center|α ||align=center|2.509||align=center|100 million |- ||268||50V||9.055759||||align=center|β+ β− ||align=center|2.205 , 1.038||align=center|10 million |- ||269||113Cd||8.859372||||align=center|β− ||align=center|0.321||align=center|600,000 |- ||270||148Sm||8.607423||||align=center|α ||align=center|1.986||align=center|500,000 |- ||271||144Nd||8.652947||||align=center|α ||align=center|1.905||align=center|200,000 |- ||272||186Os||8.302508||||align=center|α ||align=center|2.823||align=center|100,000 |- ||273||174Hf||8.392287||||align=center|α ||align=center|2.497||align=center|100,000 |- ||274||115In||8.849910||||align=center|β− ||align=center|0.499||align=center|30,000 |- ||275||152Gd||8.562868||||align=center|α ||align=center|2.203||align=center|8,000 |- ||276||130Ba||8.742574||||align=center| KK ||align=center|2.620||align=center|5,000 |- ||277||190Pt||8.267764||||align=center|α ||align=center|3.252||align=center|60 |- ||278||147Sm||8.610593||||align=center|α ||align=center|2.310||align=center|8 |- ||279||138La||8.698320||||align=center|K β− ||align=center|1.737 , 1.044||align=center|7 |- ||280||87Rb||9.043718||||align=center|β− ||align=center|0.283||align=center|4 |- ||281||187Re||8.291732||||align=center|β− α ||align=center|0.0026 , 1.653||align=center|3 |- ||282||176Lu||8.374665||||align=center|β− ||align=center|1.193||align=center|3 |- ||283||232Th||7.918533||||align=center|α SF ||align=center|4.083||align=center|1 |- ||284||238U||7.872551||||align=center|α SF ||align=center|4.270||align=center|0.3 |- ||285||40K||8.909707||||align=center|β− K β+ ||align=center|1.311 , 1.505 , 1.505||align=center|0.09 |- ||286||235U||7.897198||||align=center|α SF ||align=center|4.679||align=center|0.05 |- ||287||146Sm||8.626136||||align=center|α ||align=center|2.529||align=center|0.008 |- ||288||244Pu||7.826221||||align=center|α SF ||align=center|4.666||align=center|0.006 |}
Category:Geochemistry Category:Geophysics Category:Geochronology Category:Isotopes Category:Chemical element groups Category:Metrology
This text is licensed under the Creative Commons CC-BY-SA License. This text was originally published on Wikipedia and was developed by the Wikipedia community.