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Lesson 13 Nuclear Astrophysics. Elemental and Isotopic Abundances.

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Presentation on theme: "Lesson 13 Nuclear Astrophysics. Elemental and Isotopic Abundances."— Presentation transcript:

1 Lesson 13 Nuclear Astrophysics

2 Elemental and Isotopic Abundances

3 Elemental and Isotopic Abundances (cont.)

4 Elemental and Isotopic Abundances

5 Overview of the Sun and the Nucleosynthetic Processes Involved

6 Primordial Nucleosynthesis Age of the universe 10-20 billion years with best estimate being 14  1 x 10 9 y. Universe started with the Big Bang. Evidence for the Big Bang: 2.7 K microwave radiation. Photon density ~ 400/cm 3

7 Early history of the Universe

8 Evolution of the Universe 10 -43 s Planck time 10 32 K, vol=10 -31 vol current k B T(eV)=8.5x10 -5 T(K) Matter is QGP, all particle present. 10 -6 s, T ~10 13 K, hadronic matter condenses out. Matter is nucleons, mesons, neutrinos, photons, electrons.

9 Evolution of the Universe 10 -2 s. T~ 10 11 K,  ~ 4 x 10 6 kg/m 3

10 Evolution of the Universe At T=10 12 K, n/p ~ 1, at T=10 11 K n/p ~ 0.86, etc. At T = 10 11 K, no complex nuclei were formed because the temperature was too high to allow deuterons to form. When the temperature fell to T= 10 10 K (t~ 1 s), the creation of e + /e - pairs (pair production) ceased because kT < 1.02 MeV and the neutron/proton ratio was ~ 17/83. At a time of 225s, this ratio was 13/87, the temperature was T ~ 10 9 K, then density was ~ 2 x 10 4 kg/m 3, and the first nucleosynthetic reactions occurred.

11 First Nucleosynthesis Hydrogen burning n + p  d +  p + d  3 He +  n + d  3 H +  He formation 3 H + p  4 He +  3 He + n  4 He +  3 H + d  4 He + n d + d  4 He + 

12 Big Bang Nucleosynthesis After about 30 m, nucleosynthesis ceased. The temperature was ~ 3 x 10 8 K and the density was ~ 30 kg/m 3. Nuclear matter was 76% by mass protons, 24% alpha particles with traces of deuterium, 3 He and 7 Li. The  /n/p ratio is 10 9 /13/87. The relative ratio of p/ 4 He/d/ 3 He/ 7 Li is a sensitive function of the baryon density of the Universe. Chemistry began about 10 6 years later, when the temperature had fallen to 2000K and the electrons and protons could combine to form atoms. Further nucleosynthesis continues to occur in the interiors of stars.

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14 Stellar Nucleosynthesis All elements beyond H and He synthesized in stellar interiors Stellar nucleosynthesis continues to date (2 x 10 5 y 99 Tc lines in stars)

15 Stellar Evolution Population III stars (protostars)--H, He, short lifetimes, now extinct Population II stars (H, He, 1% heavier elements) Population I stars (H, He, 2-5% heavier elements) Includes our sun.

16 Sun Typical Population I star. mass=2 x 10 30 kg radius=7 x 10 6 m  ~1.41 x 10 3 kg/m 3 surface T ~ 6000K Luminosity ~ 3.83 x 10 26 W age ~ 4.5 x 10 9 y.

17 Herzsprung-Russell Diagrams

18 Stellar evolution and H-R diagrams

19 Aside on our Sun ~ 7 x 10 9 more years on main sequence 1.1-1.5 x 10 9 years, luminosity will increase by ~10%, making Earth uninhabitable. Terrestrial life has used up about 3/4 of its lifespan.

20 Supernovas Massive stellar explosions ~10 51 ergs released in a few seconds 2-3/century, last observation was 1987. Some supernovas lead to the formation of neutron stars.

21 Thermonuclear reaction rates

22 But these are charged particle reactions! For p +p, CB ~ 550 keV. kT~ 1.3 keV  barrier penetration problem

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24 Stellar Nucleosynthesis--A Scorecard Big Bang  75% H, 25% He, trace 7 Li From ~ 10 6 years after the Big Bang to present, get nuclear fusion reactions in stars that synthesize the elements up to A ~ 60.

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26 Hydrogen Burning First stage of a star; converts H into He. First reaction(pp): p + p  d + e + + e Q = 0.42 MeV Weak branch (pep) p + e - + p  d + e Q = 1.42 MeV Next Reaction d + p  3 He +  Q = 5.49 MeV. 86% Branch 3 He + 3 He  4 He + 2p Q = 12.96 MeV Net reaction 4p  4 He + 2e + + 2 e Q = 26.7 MeV

27 Hydrogen Burning(ppI chain)

28 Side reaction 3 He + 4 He  7 Be + e e - + 7 Be  7 Li + e Q = 0.86 MeV p + 7 Li  2 4 He This side branch along with the p+p, d+p is called the ppII process

29 Another side branch 7 Be + p  8 B +  8 B  8 Be* + e + + e 8 Be*  2 4 He This sequence along with the p+p, d+p, etc is called the PPIII chain.

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31 12 C + p  13 N +  13 N  13 C + e + + e 13 C + p  14 N +  14 N +p  15 O +  15 O  15 N + e + + e 15 N + p  12 C + 4 He CNO Cycle Net effect is 4p  4 He + 2e + + 2 e

32 CNO Cycle

33 He burning Eventually the H fuel will be exhausted, get gravitational collapse, further heating and red giant formation. Then He burning will commence. The reaction is the 3  process.

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35 12 C + 12 C  20 Ne + 4 He 12 C + 12 C  23 Na + p 12 C + 12 C  23 Mg + n 12 C + 12 C  24 Mg +  16 O + 16 O  24 Mg + 2 4 He 16 O + 16 O  28 Si + 4 He 16 O + 16 O  31 P + p 16 O + 16 O  31 S + n 16 O + 16 O  32 S + 

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37 Synthesis of A > 60 Use neutron capture There are two types of n-capture reactions. one on a slow time scale, the s-process and one on a rapid time scale, the r process. In s process reactions,  - decay intervenes between n captures while in the r process, it does not.

38 s-Process Example 56 Fe + n  57 Fe (stable) +  57 Fe + n  58 Fe (stable) +  58 Fe + n  59 Fe (t 1/2 = 44.5 d) +  59 Fe  59 Co (stable) +  - + Process terminates at 209 Bi

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40 r-process ( in supernovas)

41 p process makes proton-rich nuclei most reactions are photonuclear reactions like ( ,p), ( , n), ( ,  ) probably occurs in supernovas.

42 rp process

43 Solar Neutrinos Sun emits 1.8 x 10 38 neutrinos/s with the flux hitting the Earth being 6.4 x 10 10 neutrinos/s/cm 2.

44 Fluxes and Detectors

45 Solar Neutrino Detectors The most famous detector is the Chlorine detector of Ray Davis. Contained 100,000 gal C 2 Cl 4 in a cavern 1600 m below the earth’s surface in the Homestake kine. Reaction used: Ar nuclei collected as gas, detect 2.8 keV e from Auger from EC Produce ~3 atoms/wk in volume of 10 30 atoms.

46 Gallex detector e + 71 Ga  71 Ge + e - Collect Ge gas product threshold = 0.232 MeV

47 Super K Detect Cerenkov radiation from + e -  + e - threshold = 8 MeV

48 SNO + e -  + e - e + d  2p + e - + d  n + p + Sensitive to all types of neutrinos

49 Results Davis : measured 2.1 +- 0.3 SNU expect 7.9 +- 2.4 SNU 1 SNU = 10 -36 neutrino captures/s/target atom Gallex: measured 77 +- 10 SNU expect 127 SNU

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51 Solution neutrino oscillations imply neutrino has mass

52 Synthesis of Li, Be, B

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