E.4 Fission
- Syllabus
- First assessment 2025
- Topic
- —
- Level
- SL
Model fission
A heavy nucleus can split into two lighter nuclei after absorbing a neutron, or spontaneously in an unstable state. The products have a greater binding energy per nucleon than the original heavy nucleus.
Track the release
The increase in total binding energy appears as kinetic energy of the fission products, neutron energy and radiation. The mass of the products is slightly smaller, with the mass difference converted to energy.
E_{\text{released}}=B_{\text{products}}-B_{\text{reactants}}=\Delta mc^2
Worked example — use binding energy per nucleon
For 235U splitting into 89Kr and 144Ba, use B=A(B/A). With values 7.59, 8.72 and 8.27MeV per nucleon, E=[89(8.72)+144(8.27)]−235(7.59)=1.83×102MeV. The products are more tightly bound, so this positive difference is released.
Understand fissile material
Enrichment increases the fraction of uranium-235 relative to uranium-238, making a sustained fission process more feasible.
Common trap
Do not say energy is created from nothing. It comes from the mass defect and the change in nuclear binding energy.
Questions estimate specific fission energy or identify what enrichment means.
Estimate / Identify
Convert energy per nucleus and mass per nucleus to J kg^-1, or state explicitly that enrichment raises the U-235 fraction.
Confusing enrichment with converting one uranium isotope into another.
Start the chain
A fission event can emit neutrons. If one of them causes another fission, the process becomes a chain reaction.
Control the multiplication
A self-sustaining reactor requires, on average, one effective neutron from each fission to cause the next fission. Neutrons can instead escape, be absorbed by control rods, or be absorbed without causing fission.
Explain moderation
Fast neutrons are slowed by collisions with a moderator because low-energy neutrons have a higher probability of causing the relevant fission in this reactor model.
Common trap
Do not say every emitted neutron continues the chain. Losses and absorption determine whether the reaction dies out, stays critical or grows.
Questions explain why neutron energy is reduced or evaluate possible neutron-loss values in a reactor model.
Outline / Determine
Mention fast neutrons, greater probability for thermal neutrons, and distinguish absorbed, escaping and fission-causing neutrons.
Saying moderation increases neutron energy or treating every absorbed neutron as causing fission.
Follow neutrons, energy and radiation
Each reactor component controls a different part of the process. The moderator changes neutron energy; control rods change how many neutrons remain available; the heat exchanger moves thermal energy; shielding reduces radiation reaching people.
| Component | Direct action | Why it is needed |
|---|---|---|
| Moderator | Slows fast neutrons by collisions | Slow neutrons are more likely to induce fission in the fuel |
| Control rods | Absorb neutrons; insertion absorbs more | Regulates the chain-reaction rate and power |
| Heat exchanger | Transfers thermal energy to a separate working fluid | Produces steam for the turbine while isolating reactor coolant |
| Shielding | Absorbs or attenuates escaping radiation | Reduces radiation exposure outside the reactor |
Track the energy path
Nuclear energy becomes kinetic energy of fission products, then internal energy of coolant, kinetic energy of steam and turbine, and finally electrical energy from the generator. The heat exchanger transfers energy; it does not create or regulate the fission reaction.
Common trap
Both moderator and control rods interact with neutrons, but their jobs differ: the moderator slows them, whereas control rods remove some by absorption.
Questions identify the moderator’s effect or choose a suitable moderator material.
Identify
Match the component to its physical function; for the moderator, state that it decreases neutron kinetic energy.
Confusing moderator with control rods or choosing a material that absorbs rather than slows neutrons.
Identify the products and the hazard
Fission produces two medium-mass fragments, free neutrons, radiation and energy. Many fragments are neutron-rich and radioactive; their decay produces ionizing radiation and continues to release thermal energy after the chain reaction stops.
| Property of waste | Consequence | Management response |
|---|---|---|
| High initial activity and decay heat | Strong radiation and continued heating | Shield and cool spent material, often first in water ponds |
| Mixture of half-lives | Hazard changes over different timescales | Monitor, classify and contain waste according to activity and lifetime |
| Long-lived radionuclides | Isolation is needed beyond normal operational times | Use durable containers and secure long-term storage, such as a suitable geological repository |
Judge the management problem
A long half-life does not automatically mean a greater activity: for the same number of nuclei, a longer half-life means a smaller decay constant. Waste decisions must consider amount, radiation type, activity, heat, containment and timescale together.
Common trap
Do not assume shutting down the chain reaction makes spent fuel immediately safe. Unstable fission products continue to decay after neutron-induced fission has stopped.
Retrieve the chain
Fission converts nuclear binding and mass defect into energy. A controlled chain reaction depends on neutron energy and losses; moderator, control rods, heat exchanger and shielding perform different jobs.
Retrieve the safety boundary
Fission products can be radioactive and require containment, shielding and long-term waste management.