Spec-aligned revision resources, group courses, and 1:1 tutoring for GCSE and A Level Physics — built by an experienced teacher and examiner.
The 3- to 6-mark questions in this topic come in four types, and each type gets marked against the same points every time. Choose one, learn its chain, then fill in the details from the question. Every question here is from a real Edexcel paper.
The notes: all four chains, how to mark up a question and every worked answer. Or just the questions, with the chains at the top and the answers at the back.
Choose a question type
“Use the binding energy per nucleon curve to explain…”
…or why fission or fusion releases energy, or why fusion produces large amounts of energy. Any question with the binding energy per nucleon graph in it is this type. If it says “refer to the graph” or “use values from the graph”, a mark is waiting for numbers read off it.
| Fusion | Fission | |
|---|---|---|
| What happens | Two small mass nuclei join to form a larger nucleus | A large mass nucleus splits into two smaller nuclei (plus 2 or 3 neutrons) |
| Nucleon number | Increases | Decreases |
| On the curve | Left side, moving right and up | Right side, moving left and up |
| Binding energy per nucleon | Increases in both, so total mass decreases and energy is released (ΔE = c²Δm) | |
Small nuclei (fusion) or one large nucleus (fission). Find them on the curve.
Where the products sit on the curve. Higher up = more binding energy per nucleon.
“binding energy per nucleon”, “release energy”, “refer to the graph” or “use values from the graph”.
Nuclear fusion involves small nucleiS joining to make larger nucleiE. Nuclear fission involves large nucleiS splitting to become smaller nucleiE. Both of these processes release energy.
(a) The graph shows how the binding energy per nucleon varies with nucleon number for a range of isotopes.
Use the binding energy per nucleon curve to explain how fusion and fission both release energy. (3)
1In fusion, small nuclei join, so the nucleon number increases. On the left of the curve this means the binding energy per nucleon increases.✓ 1 mark
2In fission, a large nucleus splits, so the nucleon number decreases. On the right of the curve this also means the binding energy per nucleon increases.✓ 1 mark
3Both processes move towards iron-56, at the peak of the curve.shows you understand
4When the binding energy per nucleon increases, the products have less mass than the starting nuclei, so energy is released (ΔE = c²Δm).✓ 1 mark
Three marks: one for each direction on the curve, one for why that releases energy.
| Mark scheme says | Link | |
|---|---|---|
| Fusion involves an increase in binding energy (per nucleon) as the number of nucleons increases | 1 | (1) |
| Fission involves an increase in binding energy (per nucleon) as the number of nucleons decreases | 2 | (1) |
| If binding energy per nucleon increases, energy is released in the process | 4–6 | (1) |
| 3 marks. “Larger nuclei” and “smaller nuclei” are accepted for the nucleon number increasing and decreasing. | ||
Mark up the question first (ring what you start with and what you end with, underline the trigger), write your answer, then open the answer to see the mark-up, the chain and the mark scheme.
A fusion research centre was opened in Rotherham in 2021. The centre has a device which tests materials in the extreme conditions found inside a fusion reactor.
(b) The graph shows how the binding energy per nucleon varies with nucleon number for a range of nuclides.
Explain why the fusion of nuclei can produce large amounts of energy. Your answer should refer to information from the graph. (3)
1Small (light) nuclei fuse to form a larger nucleus.✓ 1 mark
2The binding energy per nucleon increases, so the mass decreases and energy is released (ΔE = c²Δm).✓ 1 mark
3From the graph, the binding energy per nucleon rises from about 1 MeV for hydrogen-2 to about 7 MeV for helium-4: an increase of about 6 MeV for every nucleon. The curve is steepest here, so fusing light nuclei releases a lot of energy per nucleon.✓ 1 mark
“Refer to the graph” means numbers. Any two sensible values read off the curve, compared, earn the mark.
| Mark scheme says | Link | |
|---|---|---|
| Small(er) nuclei fuse to form larger nuclei | 1 | (1) |
| The binding energy (per nucleon) increases, releasing energy, or the mass deficit increases and E = c²Δm | 4–6 | (1) |
| Comparison of values from the graph, e.g. H to He is about 7 MeV | 6 | (1) |
| 3 marks. The mark scheme’s own example compares hydrogen and helium. Any correct pair of values from the curve works. | ||
The graph shows how the binding energy per nucleon varies with number of nucleons.
(a) Explain why energy is released when a nucleus undergoes fission. (2)
(b) A nucleus of ²³⁸US undergoes fission. One of the fission products is SnE.
Estimate the energy, in MeV, released in the fission. You should use values from the graph. (3)
2In fission, a large nucleus splits into two smaller nuclei (and some neutrons).✓ 1 mark
4The binding energy per nucleon increases, so the total binding energy increases and the mass decreases: energy is released.✓ 1 mark
(b) The estimate6From the graph: binding energy per nucleon of ²³⁸U ≈ 7.5 MeV and of Sn ≈ 8.5 MeV.✓ 1 mark
6Increase in binding energy per nucleon = 8.5 − 7.5 = 1.0 MeV, for each of the 238 nucleons: increase in binding energy ≈ 238 × 1.0 MeV.✓ 1 mark
6Energy released ≈ 240 MeV✓ 1 mark
Assume every nucleon ends up about as tightly bound as tin. That’s why it’s an estimate.
| Mark scheme says | Link | |
|---|---|---|
| (a) A large nucleus splits (into two nuclei plus neutrons) | 2 | (1) |
| (a) The binding energy (per nucleon) increases, so energy is released, or there is a decrease in (total) mass | 4 | (1) |
| (b) Binding energy per nucleon read from the graph for before and after fission | 6 | (1) |
| (b) Binding energy before and after fission calculated, or the binding energy increase calculated | 6 | (1) |
| (b) Energy released ≈ 240 MeV | 6 | (1) |
| 2 + 3 marks. Mark scheme example: (8.5 − 7.5) MeV = 1.0 MeV; 238 × 1.0 MeV ≈ 240 MeV. | ||
“Explain the conditions required to bring about and maintain fusion…”
…in a star, in the Sun, or in a reactor on Earth (JET, ITER, a hot plasma). It’s often the starred 6-marker. Shorter versions ask why each condition is needed, or just to describe the extreme conditions.
| Condition | Why it’s needed | Which part of the question |
|---|---|---|
| Very high temperature (about 10⁷ K) | Nuclei are positive and repel. They need a high kinetic energy to get close enough (about 10⁻¹⁵ m) for the strong force to pull them together | “bring about” |
| Very high density (or pressure) | Lots of nuclei close together, so collisions happen more frequently and the fusion rate is high enough to keep going | “maintain” |
A star’s core, the Sun, a reactor on Earth. A reactor adds magnetic fields and a plasma.
“the conditions” = both. “each of these two” = both, with a reason for each.
“bring about and maintain”, “explain why” (give reasons) or “describe” (just say what they are).
The energy radiated by starsW is released by nuclear fusion.
* Explain the conditionsH required to bring about and maintain nuclear fusion in stars. (6)
1Fusion requires a very high temperature (about 10⁷ K).✓ 1 mark
2All nuclei are positively charged, so there is a large electrostatic repulsive force between them.✓ 1 mark
3At a very high temperature the nuclei have a high kinetic energy, enough to overcome the repulsion.✓ 1 mark
4So the nuclei get close enough (about 10⁻¹⁵ m) for the strong force to act, and they fuse.✓ 1 mark
Maintaining fusion5Fusion also requires a very high density.✓ 1 mark
6With so many nuclei close together, collisions happen more frequently, so the collision rate is high enough to sustain fusion.✓ 1 mark
Six points in a logical order: 4 marks for the points and 2 for the reasoning. Leaving out any one point costs you a mark.
| Mark scheme says | Link | |
|---|---|---|
| Requires a (very) high temperature | 1 | (1) |
| Nuclei all have positive charge, leading to a large repulsive force between nuclei | 2 | (1) |
| At high temperature nuclei have high kinetic energy, sufficient to overcome repulsion | 3 | (1) |
| Nuclei must get close enough to fuse (accept close enough for the strong force) | 4 | (1) |
| Requires (very) high density | 5 | (1) |
| Collision rate must be high enough to sustain fusion | 6 | (1) |
| 6 marks, indicative content (the * on the question). Six points seen earn 4 marks; the last 2 are for a logical, linked answer. The chain gives you both: every link is a point, and you write them in order. | ||
Same chain, different set-ups. Mark up the question first, write your answer, then open the answer to see the mark-up, the chain and the mark scheme.
(b) It is hoped that the ITER will be the first fusion device on Earth to maintain nuclear fusion for long periods of time.
To achieve fusion in the ITERW, a hot plasma is used. The plasma must
• be at an extremely high temperature
• have sufficient density for fusion.
Explain why each of these two conditionsH must be met. (4)
3The temperature must be extremely high so that the nuclei have enough kinetic energy…✓ 1 mark
2…to overcome the electrostatic repulsion between the positively charged nuclei…✓ 1 mark
4…so that the nuclei come close enough to fuse.✓ 1 mark
Sufficient density6The density must be high enough that collisions happen frequently: the collision rate is high enough for fusion to continue, and the energy released keeps the temperature very high.✓ 1 mark
Five marking points for four marks, so you have one spare. Don’t just repeat the two bullet points: the marks are all in the reasons.
| Mark scheme says | Link | |
|---|---|---|
| Very high temperature so that the nuclei have sufficient kinetic energy | 3 | (1) |
| Nuclei must overcome electrostatic repulsion (allow repulsion due to positively charged nuclei) | 2 | (1) |
| So that the nuclei come close enough to fuse | 4 | (1) |
| Sufficient density so that the collision rate (between nuclei) is high (enough) | 6 | (1) |
| Sufficient collision rate to maintain the (very high) temperature | 6 | (1) |
| Max 4 marks from these 5 points. | ||
A fusion research centre was opened in Rotherham in 2021. The centre has a device which tests materials in the extreme conditions found inside a fusion reactorW.
(a) Describe the extreme conditionsH inside a fusion reactor. (3)
1A very high temperature, about 10⁷–10⁸ K.✓ 1 mark
+The material is a plasma: it is fully ionised.✓ 1 mark
+There is a very high magnetic flux density (strong magnetic field), which holds the plasma away from the walls.✓ 1 mark
+Materials are bombarded by neutrons released in the fusion reactions.a fourth point, spare
“Describe” is a list of what’s there. Very high density or pressure also scores, but the reactor-only points are safer.
| Mark scheme says | Link | |
|---|---|---|
| Very high temperatures (accept T ≈ 10⁷–10⁸ K) | 1 | (1) |
| High magnetic flux density | + | (1) |
| Bombardment by neutrons | + | (1) |
| Material is a plasma, or material is fully ionised | + | (1) |
| Max 3 marks. Conditions for stars are accepted too: high density, high pressure. | ||
“Explain why there is an exponential decrease in the rate of decay…”
…or how a decay constant can be found when decay is random, or how a radioactive sample keeps releasing energy for a long time. The clues: random, a large number of nuclei, exponential, half-life, rate of decay.
“a large number of unstable nuclei”: that’s your permission to use probability.
The rate (activity), the number of nuclei, the decay constant, or the energy released.
“exponential”, “random”, “decay constant”, “half-life”, “over a long period of time”.
Radioactive decay is often described in textbooks as a spontaneous, random process.
* (b) Explain why there is an exponential decrease in the rate of decayQ for a sample containing a large number of unstable nucleiL. (6)
1Each nucleus has a fixed probability of decaying in the next second: the decay constant λ.✓ 1 mark
2Decay is random for an individual nucleus, but for a sample with a large number of unstable nuclei there is a predictable pattern.✓ 1 mark
3The fraction of the nuclei decaying in the next second is equal to the decay constant λ.✓ 1 mark
4So the number of nuclei decaying per second depends on the number of unstable nuclei left: A = λN.✓ 1 mark
5As nuclei decay, the number of unstable nuclei decreases exponentially with time: N = N₀e−λt.✓ 1 mark
6So the rate of decay decreases exponentially with time: A = A₀e−λt.✓ 1 mark
Each link leads into the next. That chain of reasoning is what earns the 2 marks for structure.
| Mark scheme says | Link | |
|---|---|---|
| There is a fixed probability (λ) of an individual nucleus undergoing decay (in the next second) | 1 | (1) |
| For a sample with a large number of unstable nuclei there is a predictable pattern | 2 | (1) |
| The fraction of nuclei decaying in the next second is equal to the decay constant (λ) | 3 | (1) |
| Hence the number of nuclei decaying (in the next second) depends on the number of (unstable) nuclei, or activity = λN | 4 | (1) |
| The number of unstable nuclei decreases exponentially (with time), or N = N₀e−λt | 5 | (1) |
| So the rate of decay decreases exponentially (with time), or A = A₀e−λt | 6 | (1) |
| 6 marks, indicative content (the * on the question). Six points seen earn 4 marks; the last 2 are for a logical, linked answer. The chain gives you both: every link is a point, and you write them in order. | ||
Same chain, used in two different ways. Mark up the question first, write your answer, then open the answer to see the mark-up, the chain and the mark scheme.
Nuclear decay is described as being spontaneous and random.
(a) (ii) Explain why the decay constantQ of an isotope can be determined even though nuclear decay is random. (2)
1The decay constant is the probability that a nucleus decays per unit time, and this probability can be determined…✓ 1 mark
2…because a sample contains a very large number of nuclei, so the fraction decaying per second is predictable even though each decay is random.✓ 1 mark
Two marks, two links. The idea is in the first two links of every decay answer.
| Mark scheme says | Link | |
|---|---|---|
| The probability of decay (in a specified time) may be determined | 1 | (1) |
| (The probability may be applied accurately because) very large numbers are involved | 2 | (1) |
| 2 marks. | ||
* Radium is a radioactive element. The most common isotope of radium has a half-life of almost two thousand years. A sample of radium can remain at a higher temperature than its surroundings for a long period of time.
Explain how a sample of radium is able to release significant amounts of energyQ over a long period of time. (6)
4The rate of decay depends on the number of unstable nuclei in the sample: A = λN.✓ 1 mark
+Radium has a long half-life (small λ), so unstable nuclei are present for a long time and decays keep happening.✓ 1 mark
Where the energy comes from+When a nucleus decays, there is a small decrease in mass.✓ 1 mark
+Energy is released according to ΔE = c²Δm.✓ 1 mark
+Δm is small but c² is very large, so a significant amount of energy is released.✓ 1 mark
+The energy released becomes kinetic energy of the atoms in the sample, so the sample stays above the temperature of its surroundings.✓ 1 mark
Only one link comes straight from the chain. The other five are about energy: mass deficit and ΔE = c²Δm.
| Mark scheme says | Link | |
|---|---|---|
| The rate of decay depends upon the number of unstable nuclei in the sample (A = λN) | 4 | (1) |
| Radium has a large half-life, so unstable nuclei are present in the sample for a long time | + | (1) |
| When a nucleus decays there is a (small) decrease in mass | + | (1) |
| Energy is released according to ΔE = c²Δm | + | (1) |
| Δm is small but c is large, so a significant amount of energy is released | + | (1) |
| Energy released by the decay becomes kinetic energy of the atoms in the sample (hence the sample is above the temperature of the surroundings) | + | (1) |
| 6 marks, indicative content (the * on the question). Six points seen earn 4 marks; the last 2 are for a logical, linked answer. The chain gives you both: every link is a point, and you write them in order. A reference to binding energy increasing is accepted for the decrease in mass. | ||
“Explain which type of radiation is emitted…”
…or describe how to find the type, or the fraction, of radiation from a source using a Geiger–Müller tube. The clues: GM tube, ratemeter, count rate, paper, aluminium, lead, background.
| Radiation | Stopped by | Why |
|---|---|---|
| Alpha (α) | A sheet of paper, or a few cm of air | Most strongly ionising, so it loses its energy quickly |
| Beta (β) | A few mm of aluminium | Less ionising than alpha |
| Gamma (γ) | Never fully stopped: several cm of lead reduces it | Weakly ionising |
Paper, the thickness of aluminium, lead. One link for each.
“no change”, “decreased to background”, “decreased but stayed above background”.
“Explain which” (reason from results) or “Describe how” (write the method).
The penetration of nuclear radiation through materials depends upon the ionising power of the radiation.
(a) A teacher tested an unknown radioactive source. He set up the source and a GM tube, as shown.
The initial count rate is determined without an absorber between the GM tube and the source.
When an aluminium sheet of thickness 0.5 cmA was placed between the source and the GM tube, the count rate decreased to background levelC.
The teacher then removed the aluminium sheet and replaced it with a sheet of paperA. There was no changeC in the initial count rate.
Explain which type of radiation is emitted from the source. You should refer to the penetration of each type of radiation through each sheet of absorber. (4)
3Alpha radiation would not pass through the sheet of paper.✓ 1 mark
3There was no change in the count rate when the paper was placed between the source and the GM tube, so there can’t be any alpha radiation.✓ 1 mark
5Gamma radiation would pass through the aluminium sheet, but the count rate fell to background, so there can’t be any gamma radiation.✓ 1 mark
4So it must be beta radiation: beta passes through paper but not through 0.5 cm of aluminium.✓ 1 mark
One sentence per absorber, then the conclusion: the question asked you to refer to each sheet.
| Mark scheme says | Link | |
|---|---|---|
| Alpha radiation would not pass through the sheet of paper | 3 | (1) |
| No change in count rate when paper placed (between source and GM tube), so there can’t be any alpha radiation | 3 | (1) |
| There can’t be any gamma radiation, as gamma radiation would pass through the aluminium sheet, or as the count rate decreases to background with the aluminium sheet | 5 | (1) |
| It must be beta radiation, as beta radiation would not pass through the aluminium sheet | 4 | (1) |
| 4 marks. | ||
This time you write the method. Mark up the question first, write your answer, then open the answer to see the mark-up, the chain and the mark scheme.
(b) A radioactive source used in a school laboratory emits alpha and beta radiationA.
Describe how the percentage of the activity due to beta radiationC may be determined using a Geiger–Müller tube and ratemeter. (4)
1Measure the background count rate with the source removed.✓ 1 mark
2Measure the count rate from the source, with nothing between it and the GM tube.✓ 1 mark
3Place a sheet of paper between the source and the GM tube to absorb the alpha radiation, and measure the count rate again.✓ 1 mark
6Percentage due to beta = (count rate with paper − background) ÷ (count rate without paper − background) × 100.✓ 1 mark
Keep the distance between the source and the GM tube the same for every reading, so only the absorber changes.
| Mark scheme says | Link | |
|---|---|---|
| Measure the background count (rate) | 1 | (1) |
| Measure count (rate) from source | 2 | (1) |
| Use paper to absorb alpha radiation | 3 | (1) |
| Percentage = (count with paper − background rate) ÷ (count from source − background rate) × 100 | 6 | (1) |
| 4 marks. | ||
Physics With Kate · physicswithkate.com
Spec-aligned revision resources, group courses, and 1:1 tutoring for GCSE and A Level Physics — built by an experienced teacher and examiner.