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Stellar Alchemy: The Origin of the Chemical Elements Rick Norman Dept. of Nuclear Engineering UC Berkeley Atomic and Nuclear Stucture • Atom - smallest unit of a chemical element – Size on the order of 10-8 cm (1 Angstrom) – Contains Z electrons (Qe = -1e) » and – Nucleus – – – – – – – – Size on the order of 10-13 cm (1 femtometer ) Contains more than 99.9% of the mass of the atom Made of Z protons and N neutrons Proton (Qp = +1e) Neutron (Qn = 0) A = Atomic mass = Z + N Held together by strong nuclear force A ZXN where X = chemical symbol A look inside an atom Stars Visible EM Spectrum What is the universe made of ? • Hydrogen = 75%, by mass • Helium = 23 % • Everything Else = 2% Hertzsprung-Russell Diagram Our Sun Mass = 2 x 1033 grams Luminosity = 4 x 1033 ergs/second Age = 4.5 x 109 years Over the life of the Sun, it has produced a total of 6 x 1050 ergs or 3 x 1017 ergs/gram Where does this energy come from? Chemical Reactions ? Maximum energy release = 2 x 1012 ergs/gram Thus, chemical reactions could power the Sun for only 30,000 years Gravitational Contraction ? V = 3/5 (GM2/R) = 2 x1048 ergs → 1015 ergs/gram No where near enough energy! Nuclear Reactions Can Produce Large Amounts of Energy Consider combining 4 hydrogen nuclei to make one 4He nucleus: 4 M(1H) > M(4He) But, E = mc2 Thus, for each 4He produced, 4.2 x10-5 ergs are released This represents 6.3 x 1018 ergs/gram Therefore over the life of the Sun, only 5% of the hydrogen needs to be “burned’ into helium to account for its energy output The Sun shines by nuclear fusion reactions! Solar neutrino flux at Earth Pioneers in Solar Neutrino Science Ray Davis Nobel Prize 2002 37Cl + νe → 1968 First Solar Neutrino Telescope 37Ar + e- SuperKamiokande Cherenkov Nobel prize 1958 Cherenkov Radiation SuperKamiokande Solar Neutrino Results Neutrino Image of Sun Sudbury Neutrino Observatory Why did SNO use $300M worth of heavy water? νe + d p +p +e- Charged Current Neutral Current νx + d p +n +ν νx’ Evidence for νe νµτ Fluxes (106 cm-2 s-1) ν e: 1.76(11) νµτ: 3.41(66) νtotal: 5.09(64) νSSM: 5.05 Helium Burning in Red-Giant Stars Burbidge, Burbidge, Fowler, Hoyle and then, 12C + 4He 16O + γ B2FH (1957) Fate of Stars For stars with masses < 10 MSun No further nuclear reactions possible White Dwarf (maximum mass = 1.4 MSun) For more massive stars, No such quiet fate possible Neutron Star or Black Hole Advanced stellar burning 12C + 12C 24Mg + γ, 16O + 16O 32S + γ, 20Ne + 4He 28Si + 4He Then through successive captures of 4He, 28Si 56Ni At this point the star is on its deathbed, No further energy generation possible Late stage massive star Burning Stage Temperature (keV) Density (g/cm3) Timescale Hydrogen 5 5 7 x 106 years Helium 20 700 5 x 105 years Carbon 80 2 x 105 600 years Neon 150 4 x 106 1 year Oxygen 200 1 x 107 6 months Silicon 350 3 x 107 1 day Collapse 600 3 x 109 seconds Bounce 3000 1014 milliseconds Explosion 100 - 600 varies 0.1 – 10 seconds Supernova Explosion Temperature goes up Density goes up p + e- n + ν e e+ +e- ν + ν 99% of SN energy comes off in neutrinos SN 1987a Neutrinos from SN1987a observed by Kamiokande and IMB underground telescopes Compton Gamma-Ray Observatory 56Co gamma rays observed from SN1987a β +/EC 56Co t1/2 = 77 days 847 keV 56Fe stable 44Ti gamma rays observed from CasA Origin of Heavy elements Neutron capture reactions slow (s) process produces half of nuclei from 56Fe 209Bi occurs during He-burning in red giant stars rapid (r) process produces other half of nuclei heavier than 56Fe plus Th and U occurs in supernovae ? s and r processes r-process path Source of stellar energies Nuclear reactions in stars Origin of chemical elements I believe a leaf of grass is no less than the journeywork of the stars