E.4 Fission
Spontaneous and neutron-induced fission, the energy released, chain reactions and critical mass, the parts of a nuclear power station (fuel, moderator, control rods, coolant, heat exchanger, shielding), and nuclear waste.
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In 30 seconds
- In fission a heavy nucleus (uranium-235, plutonium-239) splits into two lighter nuclei and a few neutrons. It can be spontaneous or induced by absorbing a neutron.
- The products have a higher binding energy per nucleon, so the total mass falls and about 200 MeV is released per fission, mostly as kinetic energy of the fragments.
- The released neutrons can cause further fissions: a chain reaction. Above the critical mass it is self-sustaining.
- A reactor controls the chain reaction with a moderator (slows neutrons), control rods (absorb neutrons) and removes the heat with a coolant and heat exchanger.
- E.4 is the same at SL and HL.
By the end you can
- Describe spontaneous and neutron-induced fission and write balanced fission equations.
- Explain the energy released using binding energy and mass defect.
- Explain chain reactions and critical mass.
- Describe the roles of fuel, moderator, control rods, coolant, heat exchanger and shielding.
- Discuss the advantages and problems of nuclear power, including waste.
1Fission
- Thermal neutrons: U-235 captures slow ("thermal") neutrons far more readily than fast ones, which is why reactors need a moderator.
- Energy released: the fragments are near the peak of the binding-energy curve (E.3), so the products are more tightly bound. The mass defect Δm becomes energy Δmc2.
In one fission the total mass falls by 0.186 u. Find the energy released.
- E = 0.186 × 931.5 MeV M1
- = 173 MeV (2.8 × 10−11 J) A1
A 1000 MW (electrical) power station is 33 % efficient. Estimate the mass of U-235 it uses per day (200 MeV per fission).
- thermal power = 3000 MW, so energy per day = 3.0 × 109 × 86 400 = 2.6 × 1014 J M1
- fissions = 2.6 × 1014/(200 × 106 × 1.6 × 10−19) = 8.1 × 1024 M1
- mass = (8.1 × 1024/6.02 × 1023) × 0.235 kg ≈ 3.2 kg A1
2Chain reactions
Critical mass — the smallest mass of fuel in which, on average, exactly one neutron from each fission causes another fission. Below it too many neutrons escape through the surface.
- Subcritical: the reaction dies out. Critical: steady (a reactor). Supercritical: it grows rapidly (a bomb, which reactors are designed never to reach).
3The nuclear reactor
| Part | Job |
|---|---|
| fuel rods | enriched uranium (more U-235 than natural); fission happens here |
| moderator | water or graphite: slows fast neutrons by collisions so U-235 can capture them |
| control rods | boron or cadmium: absorb neutrons; pushed in to slow the reaction or shut down |
| coolant | water or gas: carries thermal energy away from the core |
| heat exchanger | transfers energy from the coolant to water, making steam for the turbine |
| shielding | thick steel and concrete: absorbs neutrons and γ radiation |
4Nuclear power: pros and cons
- For: no CO2 while operating; huge energy density (about 106 times that of fossil fuels, A.3); steady output independent of the weather.
- Against: radioactive waste with long half-lives must be stored safely for thousands of years; risk of accidents (Chernobyl, Fukushima); expensive to build and decommission; proliferation concerns.
- Waste: spent fuel contains highly radioactive fission products and plutonium. It is cooled under water, then vitrified (sealed in glass) and stored deep underground.
Test yourself — cover the answers first
Quick check
- What is induced fission?
- Why is energy released in fission?
- What is the job of the moderator?
- What is the job of the control rods?
- What is critical mass?
Exam-style
- Balance: 23592U + 10n → 14456Ba + 8936Kr + x10n.
- How many fissions per second produce 1.0 W if each releases 200 MeV?
Show answers
- a heavy nucleus splitting after absorbing a neutron
- the products have higher binding energy per nucleon, so mass is lost and becomes energy
- to slow neutrons down
- to absorb neutrons and control the rate
- the mass for which, on average, one neutron per fission causes another fission
- A: 236 = 144 + 89 + x
x = 3 - 200 MeV = 3.2 × 10−11 J
1.0/3.2 × 10−11
= 3.1 × 1010 fissions per second
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