ProtonProton Chain Step 1 Formation of deuteron p

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Proton-Proton Chain: Step #1 Formation of “deuteron”, p + p d + e+ +

Proton-Proton Chain: Step #1 Formation of “deuteron”, p + p d + e+ + slow weak interaction.

Proton-Proton Chain: Step #2 Formation of “Helium-3” p + d 3 He + Rapid,

Proton-Proton Chain: Step #2 Formation of “Helium-3” p + d 3 He + Rapid, radiative association.

Proton-Proton Chain: 3 He Step #3 Formation of “Helium-4” + 3 He 4 He

Proton-Proton Chain: 3 He Step #3 Formation of “Helium-4” + 3 He 4 He + p Medium time scale.

Proton-Proton Chain: Positrons annihilate with free electrons. Resulting gamma-rays are absorbed locally together with

Proton-Proton Chain: Positrons annihilate with free electrons. Resulting gamma-rays are absorbed locally together with gamma-rays produced in step #2. Neutrinos escape the Sun directly. Prediction! Sun is a source of neutrinos.

Coulomb Barrier: -2. 2 r. N 0. 001 r. C

Coulomb Barrier: -2. 2 r. N 0. 001 r. C

Quantum Mechanical Barrier Penetration:

Quantum Mechanical Barrier Penetration:

Fusion Window:

Fusion Window:

Standard Solar Model:

Standard Solar Model:

Standard Solar Model:

Standard Solar Model:

Standard Solar Model:

Standard Solar Model:

Standard Solar Model: Half way to a helium core!

Standard Solar Model: Half way to a helium core!

Standard Solar Model:

Standard Solar Model:

Carbon-Nitrogen-Oxygen (CNO) cycle: net effect 4 p 4 He “catalysis” p + + 1.

Carbon-Nitrogen-Oxygen (CNO) cycle: net effect 4 p 4 He “catalysis” p + + 1. 99 13 C + e + + e 1. 71 14 N + 7. 55 14 N 15 O + 7. 29 15 O 15 N + e + + e 2. 22 15 N 12 C + 4. 97 12 C 13 N p + 13 C p + Me. V 13 N 4 He 25. 7 Positrons annihilate with free electrons, so add 2 x 0. 511 = 1. 02 Neutrinos carry away 0. 7 and 1, so subtract 1. 7. TOTAL = 25 Me. V per cycle

Proton-Proton versus CNO cycle: CNO begins to dominate energy production for M > 1.

Proton-Proton versus CNO cycle: CNO begins to dominate energy production for M > 1. 3 M The much greater temperature sensitivity of the CNO cycle enables the much higher luminosities of massive stars (recall L ~ M 3).

Binding Energy per Nucleon in Atomic Nuclei: “iron peak” 9 Be

Binding Energy per Nucleon in Atomic Nuclei: “iron peak” 9 Be

Triple alpha reaction: Enables a fusion jump from helium to carbon. 4 He +

Triple alpha reaction: Enables a fusion jump from helium to carbon. 4 He + 4 He 8 Be However, + 8 Be 4 He + 4 He in 2. 6 x 10 -16 s At high temperatures (T>108 K) enough 8 Be remains for an occasional 8 Be + 4 He 12 C* + 12 C + Once carbon is produced, elements can be synthesized up to the iron peak if the temperature is high enough to overcome the Coloumb barriers. For example, 4 He etc. + 12 C 16 O +

Nobel Prize in Physics 1967 For his contributions to theory of nuclear reactions, especially

Nobel Prize in Physics 1967 For his contributions to theory of nuclear reactions, especially his discoveries concerning the energy production is stars. Hans Bethe 1906 -2005

Nobel Prize in Physics 1983 For his theoretical and experimental studies of the nuclear

Nobel Prize in Physics 1983 For his theoretical and experimental studies of the nuclear reactions of importance in the formation of the chemical elements in the universe. William A. Fowler 1911 -1995

Nobel Prize in Physics 2002 For pioneering contributions to astrophysics, in particular for the

Nobel Prize in Physics 2002 For pioneering contributions to astrophysics, in particular for the detection of cosmic neutrinos. Raymond David 1914 Masatoshi Koshiba 1926 -