|Isotope mass||12 u|
|Excess energy||0± 0 keV|
|Binding energy||92161.753± 0.014 keV|
Carbon-12 is the more abundant of the two stable isotopes of the element carbon, accounting for 98.89% of carbon; it contains six protons, six neutrons and six electrons. Its abundance is due to the Triple-alpha process by which it is created in stars.
Prior to 1959 both the IUPAP and IUPAC tended to use oxygen to define the mole, the chemists defining the mole as the number of atoms of oxygen which had mass 16 g, the physicists using a similar definition but with the oxygen-16 isotope only. The two organizations agreed in 1959/60 to define the mole as follows.
The mole is the amount of substance of a system which contains as many elementary entities as there are atoms in 0.012 kilogram of carbon 12; its symbol is "mol."
This was adopted by the CIPM (International Committee for Weights and Measures) in 1967, and in 1971 it was adopted by the 14th CGPM (General Conference on Weights and Measures).
In 1961 the isotope carbon-12 was selected to replace oxygen as the standard relative to which the atomic weights of all the other elements are measured.
In 1980 the CIPM clarified the above definition, defining that the carbon-12 atoms are unbound and in their ground state.
The Hoyle state is an excited, resonant, state of carbon-12 produced via the triple-alpha process, as predicted by Fred Hoyle in the 1950s[clarification needed]. The existence of the Hoyle state is essential for the nucleosynthesis of carbon in helium-burning red giant stars, and predicts an amount of carbon production in a stellar environment which matches observations. The existence of the Hoyle state has been confirmed experimentally, but its precise properties are still being investigated. In 2011, an ab initio calculation of the low-lying states of carbon-12 found (in addition to the ground and excited spin-2 state) a resonance with all of the properties of the Hoyle state.
- Avogadro constant
- Isotopes of carbon
- Isotopically pure diamond
- Mole (unit)
- "Atomic Weights and the International Committee — A Historical Review". 2004-01-26.
- Chernykh, M.; Feldmeier, H.; Neff, T.; Von Neumann-Cosel, P.; Richter, A. (2007). "Structure of the Hoyle State in C12". Physical Review Letters 98 (3): 032501. Bibcode:2007PhRvL..98c2501C. doi:10.1103/PhysRevLett.98.032501. PMID 17358679.
- Epelbaum, E.; Krebs, H.; Lee, D.; Meißner, U.-G. (2011). "Ab Initio Calculation of the Hoyle State". Physical Review Letters 106 (19): 192501. arXiv:1101.2547. Bibcode:2011PhRvL.106s2501E. doi:10.1103/PhysRevLett.106.192501. PMID 21668146.
- Hjorth-Jensen, M. (2011). "Viewpoint: The carbon challenge". Physics 4: 38. Bibcode:2011PhyOJ...4...38H. doi:10.1103/Physics.4.38.
- Kenji Takeshita and Masaru Ishidaa (December 2006). "Optimum design of multi-stage isotope separation process by exergy analysis". ECOS 2004 - 17th International Conference on Efficiency, Costs, Optimization, Simulation, and Environmental Impact of Energy on Process Systems 31 (15): 3097–3107. doi:10.1016/j.energy.2006.04.002.
|Carbon-12 is an
isotope of carbon
|Decay product of:
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