An aneutronic fusion scheme burns deuterium with helium-3: ^ 2 H + ^ 3 He ^ 4 He + ^ 1 H

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

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

Problem

An aneutronic fusion scheme burns deuterium with helium-3: 2H+3He→4He+1H.^{2}\mathrm{H} + {}^{3}\mathrm{He} \to {}^{4}\mathrm{He} + {}^{1}\mathrm{H}. Neutral-atom masses: 2H^{2}\mathrm{H}, 2.014102 u2.014102\ \mathrm{u}; 3He^{3}\mathrm{He}, 3.016029 u3.016029\ \mathrm{u}; 4He^{4}\mathrm{He}, 4.002603 u4.002603\ \mathrm{u}; 1H^{1}\mathrm{H}, 1.007825 u1.007825\ \mathrm{u}. Take 1 u c2=931.494 MeV1\ \mathrm{u}\,c^2 = 931.494\ \mathrm{MeV}. A student reasons: “A helium-4 nucleus is made, and its binding energy is 28.30 MeV28.30\ \mathrm{MeV}, so 28.30 MeV28.30\ \mathrm{MeV} is released per reaction.” ((a)) Show that the electrons balance, so that neutral-atom masses may be used, and compute the energy released QQ in MeV. ((b)) Say in one or two sentences what is wrong with the student's reasoning.

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