The star Vega delivers an energy flux at the Earth and lies at a distance

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 star Vega delivers an energy flux f=2.1×10−8 W m−2f = 2.1 \times 10^{-8}\ \mathrm{W\,m^{-2}} at the Earth and lies at a distance d=7.68 pcd = 7.68\ \mathrm{pc}, with 1 pc=3.086×1016 m1\ \mathrm{pc} = 3.086 \times 10^{16}\ \mathrm{m}. Assume it radiates isotropically and that nothing absorbs its light on the way. Vega burns hydrogen mainly through the CNO cycle, whose first step is the proton capture 12C+1H→13N+γ^{12}\mathrm{C} + {}^1\mathrm{H} \to {}^{13}\mathrm{N} + \gamma; the relevant atomic masses are m(12C)=12.000000 um(^{12}\mathrm{C}) = 12.000000\ \mathrm{u}, m(1H)=1.007825 um(^{1}\mathrm{H}) = 1.007825\ \mathrm{u} and m(13N)=13.005739 um(^{13}\mathrm{N}) = 13.005739\ \mathrm{u}. 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)) Convert the mass difference of that first CNO step into an energy in MeV. ((b)) Estimate Vega's luminosity. ((c)) Estimate the rate at which Vega loses mass by radiating, in kg s−1\mathrm{kg\,s^{-1}}.

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