All masses are invariant (rest) masses of bare nuclei

PHYSICS · Multi-part · Fermi University Physics · Relativity & Gravitation · Nuclear Physics · Nuclear constituents, size and binding

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

Problem

All masses are invariant (rest) masses of bare nuclei. Use 1 u=931.494 MeV/c21\ \mathrm{u} = 931.494\ \mathrm{MeV}/c^2, mp=1.007276 um_p = 1.007276\ \mathrm{u}, mn=1.008665 um_n = 1.008665\ \mathrm{u}, and the nuclear masses 16O:15.990523 u{}^{16}\mathrm{O}: 15.990523\ \mathrm{u}, 12C:11.996706 u{}^{12}\mathrm{C}: 11.996706\ \mathrm{u}, 4He:4.001506 u{}^{4}\mathrm{He}: 4.001506\ \mathrm{u}. Oxygen-16 contains 88 protons and 88 neutrons. ((a)) Find the mass defect of oxygen-16 in u\mathrm{u}. ((b)) Convert it to the binding energy in MeV and give the binding energy per nucleon. ((c)) A carbon-12 nucleus at rest captures a helium-4 nucleus at rest: 12C+4He→16O+γ{}^{12}\mathrm{C} + {}^{4}\mathrm{He} \to {}^{16}\mathrm{O} + \gamma. Find the energy released, QQ, in MeV.

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