Constraints on Nuclear Fusion Reactions
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Transcript of Constraints on Nuclear Fusion Reactions
Constraints on Nuclear Fusion Reactions
• Binary reactions dominate• Energy Conservation (Energy release)• Charge conservation (d=2H nucleus)
– pp d+e++Energy +??
• Angular momentum conservation– Proton, electron spin = (1/2)[h/(2π)]– Deuteron spin = h/(2π)
• Neutrino predicted by E.Fermi – pp d+e++ +Energy– Detected in 1950s by Reines and Cowen next to a nuclear
reactors
• Weak Interactions (lepton number conservation)– n p + e+ anti-. Half Life 12,33 year– Weak interactions are Weak Reaction Rates are slow
Light Nuclei, http://www.nndc.bnl.gov/chart/
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No stable A=5 nuclei
pp chains in Sun
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pp→D+ e+ +ν e
pD→3He+γ
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3He+3He→4He+H +H
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3He+4He→7Be+γ
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7Be+ e−→7Li+ν e7Li+ p→7Be→4He+4He
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7Be+ p→8B+γ8B→8Be+ e+ +ν e8Be→4He+4He
69%
(pp I)
(pp II) (pp III)
31%
99.7%0.3%
pp chainsH+H+H+H4He+2e+2e++2
First Step• pp D + e+ + + MeV
– Weak interaction process• D=(pn) = nucleus of 2H.• Neutron half life = 10.23 min
– Suppressed by pp Coulomb repulsion• Quantum Tunneling required• Protons are waves
– If Kinetic energy = E-U > 0= h/p
– If Kinetic energy = E-U < 0– Wave is exponentially damped exp(-r)
= [U-E]1/2.
Billiard Ball model of pp collisions
• Proton density , Temperature T• Velocity distribution (Maxwell-Boltzman)
– P(v;T) = exp(-mv2/(2KT)) / [2πkT]3/2.
– <mv2/2>= <mvx2/2> +<mvy
2/2> +<mvz2/2> =3kT/2
– vrms ≈ [kT/m]1/2.
• Collision rate per unit volume: R. ≈ (m)2.– Rate R ≈ 2v|≈ 2 [kT/m]1/2.Volume = v t
Ballistic Burn Time of Sun
• Number density of sun = /MH.– Average = 8 1029 /m3.– Central = 1032 /m3.
• Temperature, rms Velocity vrms ≈ [kT/mc2]1/2
– Surface kT = 0.5 eV. vrms ≈ 7000 m/s– Central kT = 1KeV. vrms ≈ 3 105 m/s
• Proton Mass = 0.9 GeV• Time for all protons to collide / R = /[ |v|]
– Surface 1/[|v|] ≈ 10-4 s– Center ≈ 30 ns
• Crucial role of Coulomb Repulsion and Weak interactions to regulate nuclear fusion rate in sun
pp fusion slowed by coulomb repulsion
• Kinetic energy required to bring two protons to within 1 fm– e2/(4π0 r) = 1.4 MeV– Center of sun kT ≈ 1 KeV– Maxwell Boltzmann distribution
• P(v) = exp{-[mv2/(2kT)]}• P[-(1.4MeV)/(1 KeV)] ≈ exp(-1000)
• Classical pp Collision rate in sun ≈ 0– No pp fusion, even worse for heavier elements
• Quantum barrier penetration