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Questions on fission and fusion
Uranium-235 absorbs a thermal neutron and splits, releasing about 200 MeV and the two or three neutrons that sustain a chain reaction. Below the critical mass too many neutrons escape through the surface for the chain to continue. Fusion of light nuclei instead needs temperatures near 10⁷ K to beat the electrostatic repulsion.
18 original questions · 50 marks · the fission and fusion notes · Nuclear physics
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Describe what happens in induced nuclear fission.
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A heavy nucleus, such as uranium-235, absorbs a slow (thermal) neutron and becomes unstable (1); it splits into two smaller nuclei, releasing two or three neutrons and a large amount of energy (1).Explain what is meant by a chain reaction in a fissile material.
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Neutrons released by one fission are absorbed by other nuclei and cause further fissions (1); each fission releases more neutrons, so the reaction sustains itself and can grow (1).State what is meant by the critical mass of a fissile material.
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The minimum mass for a self-sustaining chain reaction (1); on average at least one neutron per fission goes on to cause another fission rather than escaping from the material (1).State what is meant by a thermal neutron.
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A slow neutron, with kinetic energy comparable to that of particles in thermal motion, which uranium-235 captures far more readily than a fast neutron (1).State the two number balances that must hold in any nuclear reaction equation.
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The total nucleon (mass) number is the same before and after the reaction (1); the total proton (atomic) number is the same before and after (1).State the form in which most of the energy released in a fission event appears.
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As kinetic energy of the two fission fragments (1).In one fission reaction, 23592U + 10n → 14156Ba + 9236Kr + x 10n. Determine the value of x and show that the proton numbers balance.
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Nucleon numbers: 235 + 1 = 141 + 92 + x (1)
236 = 233 + x, so x = 3 neutrons (1)
Proton numbers: 92 + 0 = 56 + 36 = 92, so they balance (1).A single fission event converts a mass of 3.5 × 10−28 kg into energy. Calculate the energy released in joules and in MeV.
c = 3.0 × 108 m s−1, 1 MeV = 1.60 × 10−13 JMark scheme
E = mc2 = 3.5 × 10−28 × (3.0 × 108)2 (1)
E = 3.15 × 10−11 J (1)
E = 3.15 × 10−11/(1.60 × 10−13) = 197 MeV (1)Explain why very high temperatures are needed for nuclear fusion to occur.
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The fusing nuclei are both positively charged, so they repel each other electrostatically (1); they must approach to within the very short range of the strong nuclear force to fuse (1); only at very high temperatures do the nuclei have enough kinetic energy to work against that repulsion and get close enough (1). Beyond what this question requires: even at stellar temperatures the average nucleus falls hundreds of times short of the top of the barrier, and fusion proceeds because quantum tunnelling carries the fastest nuclei through it.A fusion reaction releases 17.6 MeV of energy. Calculate the energy released in joules and the mass converted into energy.
c = 3.0 × 108 m s−1Mark scheme
E = 17.6 × 106 × 1.60 × 10−19 = 2.82 × 10−12 J (1)
m = E/c2 = 2.82 × 10−12/(3.0 × 108)2 (1)
m = 3.13 × 10−29 kg (1)Explain why the fragments produced by the fission of uranium-235 are radioactive, and state the type of decay they undergo.
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The fragments form with roughly the same neutron-to-proton ratio as uranium-235 (1); nuclei of their smaller size are stable at a lower neutron-to-proton ratio, so the fragments are neutron-rich and lie above the line of stability (1); they therefore decay by beta-minus emission, often in chains, until stability is reached (1).In one fusion reaction, two deuterium nuclei form helium-3 and a neutron:
21H + 21H → 32He + 10n
Nuclear masses: 21H 2.01355 u, 32He 3.01493 u, neutron 1.00867 u. Calculate the energy released, in MeV.
1 u = 931.5 MeVMark scheme
Mass before = 2 × 2.01355 = 4.02710 u (1)
Mass after = 3.01493 + 1.00867 = 4.02360 u, so Δm = 0.00350 u (1)
E = 0.00350 × 931.5 = 3.3 MeV (1)A reactor core produces thermal power at a steady 600 MW. Each fission releases about 200 MeV. Calculate the number of fissions occurring each second. Go on to determine the mass converted into energy in one day of operation.
1 MeV = 1.60 × 10−13 J, c = 3.0 × 108 m s−1, 1 day = 86 400 sMark scheme
Energy per fission = 200 × 1.60 × 10−13 = 3.2 × 10−11 J (1)
Rate = P/E = (600 × 106)/(3.2 × 10−11) = 1.9 × 1019 fissions per second (1)
Energy in one day = 600 × 106 × 86 400 = 5.2 × 1013 J (1)
m = E/c2 = 5.2 × 1013/(3.0 × 108)2 = 5.8 × 10−4 kg (about 0.6 g) (1)Each fission of a uranium-235 nucleus releases about 200 MeV. Estimate the energy released by the complete fission of 1.0 kg of uranium-235.
NA = 6.02 × 1023 mol−1, 1 MeV = 1.60 × 10−13 JMark scheme
Number of nuclei in 1.0 kg = NA × 1000/235 = 2.56 × 1024 (1)
Energy per fission = 200 × 1.60 × 10−13 = 3.20 × 10−11 J (1)
Total energy = 2.56 × 1024 × 3.20 × 10−11 (1)
E = 8.2 × 1013 J (1)Compare nuclear fission and nuclear fusion in terms of the fuel used, the conditions required and the products formed.
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Fuel: fission uses heavy nuclei such as uranium-235; fusion uses light nuclei such as hydrogen isotopes (1). Conditions: fission needs slow neutrons and a critical mass, and proceeds at ordinary temperatures (1); fusion needs extremely high temperatures and densities to bring nuclei close against electrostatic repulsion, with quantum tunnelling doing the rest (1). Products: fission gives radioactive fragments plus neutrons; fusion gives helium with far less long-lived radioactive waste (1).Use the binding energy per nucleon curve to explain why energy is released in both fission and fusion.
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In both processes the products have a higher binding energy per nucleon than the original nuclei (1); fusion moves light nuclei up the steep rise of the curve, and fission moves heavy nuclei towards the peak near iron-56 (1); the increase in binding energy per nucleon corresponds to a decrease in mass, and the equivalent energy is released (1).The fusion of deuterium and tritium releases 17.6 MeV from nuclei totalling five nucleons. The fission of uranium-235 releases about 200 MeV from 236 nucleons (the nucleus plus the absorbed neutron). A journalist writes that fission must release more energy per kilogram of fuel, because 200 MeV is far greater than 17.6 MeV. Deduce whether the journalist is correct.
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Equal masses of fuel contain almost equal numbers of nucleons, so energy per kilogram is compared using energy per nucleon (1)
Fusion: 17.6/5 = 3.52 MeV per nucleon (1)
Fission: 200/236 = 0.85 MeV per nucleon (1)
Fusion releases about 4 times more energy per kilogram of fuel, so the journalist is not correct (1)A fixed mass of fissile material can be formed into different shapes. Suggest why a sphere is the shape most likely to sustain a chain reaction.
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Neutrons are lost by escaping through the surface of the material (1); a sphere has the smallest surface area for a given volume (1); so the smallest fraction of neutrons escapes and the largest fraction remains to cause further fissions, making a self-sustaining chain most likely (1).
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