The Sun radiates isotropically with luminosity

PHYSICS · Multi-part · Fermi University Physics · Relativity & Gravitation · Astrophysics & Cosmology · Relativistic dynamics and fields in flat spacetime

Relativity and Gravitation, Ch Mass as energy: binding, defect and annihilation

Problem

The Sun radiates isotropically with luminosity L⊙=3.828×1026 WL_\odot = 3.828 \times 10^{26}\ \mathrm{W}. The net effect of the proton-proton chain in its core is that four hydrogen atoms are replaced by one helium-4 atom. Take the atomic masses m(1H)=1.007825 um(^1\mathrm{H}) = 1.007825\ \mathrm{u} and m(4He)=4.002603 um(^4\mathrm{He}) = 4.002603\ \mathrm{u}, and assume that all the energy released is eventually radiated away (the small fraction carried off by neutrinos is ignored). Use 1 u=1.660539×10−27 kg=931.494 MeV/c21\ \mathrm{u} = 1.660539 \times 10^{-27}\ \mathrm{kg} = 931.494\ \mathrm{MeV}/c^2 and c=2.998×108 m s−1c = 2.998 \times 10^8\ \mathrm{m\,s^{-1}}. ((a)) Estimate the mass difference of the net reaction in u\mathrm{u} and the energy it releases in MeV. ((b)) Estimate the rate at which the Sun's mass decreases, in kg s−1\mathrm{kg\,s^{-1}}. ((c)) Estimate how many helium-4 nuclei the Sun must form each second.

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