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Origin of elements and their isotopes star formation atomic structure nuclear fusion steller evolution alpha decay slow neutron capture r process beta decay abundance of elements
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DM Sherman, University of Bristol
Geochemistry, DM Sherman University of Bristol
NASA/WMAP
DM Sherman, University of Bristol
DM Sherman, University of Bristol
DM Sherman, University of Bristol
Nuclear fusion occurs between light nuclei when subjected to extremely high pressures and temperatures: Mass deficit (Δm) releases energy (E= mc^2 )
4p → 4 He In a medium star’s interior, temperatures and pressures are high enough to cause fusion of H atoms (protons) into 2 H, 3 He, 4 He nuclei. Hydrogen burning: (^1) H + 1 H → 2 H + γ (^2) H + 1 H → 3 He + γ (^3) He + 3 He → 4 He + 2 (^1) H + γ Plus trace Li, Be and B
DM Sherman, University of Bristol
Synthesis of elements with Z > 26 (Fe) is not favored by direct fusion. Fusion Fission
Alpha decay is a type of nuclear fission that occurs by spontaneous emission of an alpha particle (^4 He)
DM Sherman, University of Bristol
Nuclei with even numbers of protons and neutrons are more stable than those with odd numbers. In particular, nuclei with 2, 8, 20, 28, 50, 82 and 126 nucleons (protons or neutrons) are especially stable. (^4) He 16 O 40 Ca 48 Ca 208 Pb 2 8 20 20 82 This motivates the shell model of the nucleus in analogy with electronic configurations.
Neutrons Protons β- Z N Z N Z- N- Z- N+ Z+ N- β+
DM Sherman, University of Bristol
DM Sherman, University of Bristol
Li, Be and B have low binding energies Li, Be and B are destroyed in steller interiors. Although some 7 Li formed in the big bang; other Li isotopes along with Be and B formed by spallation processes.
DM Sherman, University of Bristol Summary