Six original Cambridge-style questions on mass defect, binding energy and E = Δmc², binding energy per nucleon as the measure of stability, and the energy released in fusion and fission.
Define the mass defect of a nucleus and its binding energy, and state the relation between them.
A carbon-12 nucleus contains 6 protons and 6 neutrons and has a mass of 11.99671 u. The mass of a proton is 1.00728 u and the mass of a neutron is 1.00867 u. Calculate the mass defect of the nucleus in u, its binding energy in MeV, and its binding energy per nucleon. (1 u is equivalent to 931 MeV.)
The mass defect of an oxygen-16 nucleus is 0.1370 u. Working in SI units, calculate the binding energy of the nucleus in joules, convert it to MeV, and find the binding energy per nucleon. (1 u = 1.66 × 10⁻²⁷ kg.)
The graph of binding energy per nucleon against nucleon number rises steeply for light nuclei, reaches a maximum near A = 56 and falls slowly for heavier nuclei. Use the graph to explain why energy is released when a uranium-235 nucleus undergoes fission, and explain why fusing two iron-56 nuclei together would not release energy.
Two deuterium nuclei fuse to form a helium-3 nucleus and a neutron: ²₁H + ²₁H → ³₂He + ¹₀n. The masses are: ²₁H 2.01410 u, ³₂He 3.01603 u, neutron 1.00867 u. Calculate the energy released in one fusion, in MeV and in joules. (1 u is equivalent to 931 MeV.)
One possible fission of uranium-235 is ²³⁵₉₂U + ¹₀n → ¹⁴¹₅₆Ba + ⁹²₃₆Kr + 3 ¹₀n. The masses are: U-235 235.0439 u, Ba-141 140.9144 u, Kr-92 91.9262 u, neutron 1.00867 u. (1 u is equivalent to 931 MeV.)
(a) Calculate the decrease in mass in this fission, in u. (b) Calculate the energy released, in MeV and in joules. (c) A reactor produces 1.0 GW of thermal power from this reaction alone. Calculate the number of fissions per second.
Mark this once you have attempted all six and checked your working. It records a Practiced badge on the topic and adds a one-time bonus. Revealing the solutions alone does not count.