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A Level · Cambridge (CIE) · 9702

Explain fission, fusion and nuclear energy release

Use the binding-energy curve and mass–energy equivalence to explain why fission or fusion can release energy.

Section 23 · Nuclear physics

Nuclear physics pathway · Cambridge 9702 A Level · 23.1

A Level · Cambridge International Physics 9702, 2025–2027 syllabus. The Topic 23 outcomes were also checked against Cambridge’s 2028–2030 syllabus, which reports no significant teaching changes. Online practice is self-checked and cannot replace supervised practical work, full timed assessment or human subject-teacher review.

Before you begin

  • Use scientific notation, SI units, proportional reasoning and the particle numbers in nuclide notation.

Work on paper. Try each question before revealing help, and explain why your method works.

Quick readiness check

What is nuclear fusion?

What you will learn

  • Explain nuclear fission and fusion
  • Relate fusion of light nuclei and fission of heavy nuclei to higher binding energy per nucleon
  • Calculate the energy released from a supplied mass decrease

Fusion joins light nuclei; fission splits a heavy nucleus

Nuclear fusion is the joining of two lighter nuclei to form a heavier nucleus. Nuclear fission is the splitting of a heavy nucleus into two or more lighter nuclei, often after neutron absorption.

The syllabus asks you to explain these processes using binding energy per nucleon. Avoid describing every fission event as identical: the exact products depend on the reaction.

A rise in total binding energy can release energy

Light nuclei can release energy by fusion when the products are more tightly bound per nucleon. Heavy nuclei can release energy by fission when the products move toward the higher-binding region of the curve.

Calculate released energy from the mass decrease using E = c²Δm, with Δm defined as initial total mass minus final total mass when that decrease is positive. State the mass and energy units and explain the binding-energy change.

Pause and explain

Why can fission of a heavy nucleus release energy?

Put the idea to work

Worked example

A fission reaction has a mass decrease of 3.0 × 10⁻²⁸ kg. Estimate the energy released using c = 3.0 × 10⁸ m s⁻¹.

Show the worked solution
  1. Use E = c²Δm.
  2. c² = 9.0 × 10¹⁶ m² s⁻².
  3. E = 9.0 × 10¹⁶ × 3.0 × 10⁻²⁸ = 2.7 × 10⁻¹¹ J.

Answer 2.7 × 10⁻¹¹ J

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From guided practice to a new situation

Write your answer and reasoning first. Use a hint only if you are stuck. The model solution is for self-checking; your written work is not automatically marked.

1 · Guided

A reaction’s total mass decreases by 4.0 × 10⁻²⁹ kg. Calculate the energy released. Use c = 3.0 × 10⁸ m s⁻¹.

Give me a hint

Square c, then multiply by the positive mass decrease.

Compare my reasoning
  1. c² = 9.0 × 10¹⁶ m² s⁻².
  2. E = c²Δm = 9.0 × 10¹⁶ × 4.0 × 10⁻²⁹.
  3. E = 3.6 × 10⁻¹² J.

3.6 × 10⁻¹² J.

Look for these in your work

  • Uses a positive mass decrease
  • Squares c
  • Gives joules
2 · Independent

Explain why fusion of suitable light nuclei can release energy.

Give me a hint

Connect the product’s position on the binding-energy curve with total binding energy.

Compare my reasoning
  1. The light reactants lie on the rising part of the curve.
  2. Fusion can produce nuclei with greater binding energy per nucleon.
  3. If total binding energy increases, the difference is released as energy.

Suitable fusion products are more tightly bound; the increase in total binding energy can be released as energy.

Look for these in your work

  • Identifies light nuclei
  • Uses the rising curve
  • Connects greater total binding with released energy
3 · Transfer

A student computes a negative mass change as final mass minus initial mass and calls the result negative energy released. Correct the method.

Give me a hint

Define the mass decrease in the direction that is positive for a release.

Compare my reasoning
  1. For released energy, calculate initial total mass − final total mass.
  2. If this mass decrease is positive, use E = c²Δm.
  3. A positive released-energy magnitude is reported; a negative sign would describe the system’s energy change under a different sign convention.

Use Δm = initial mass − final mass for the released-energy magnitude, then E = c²Δm.

Look for these in your work

  • Defines the direction of subtraction
  • Uses the mass decrease
  • Distinguishes energy released from system energy change

Common mistakes

  • Calling fusion the splitting of a nucleus
  • Claiming fission and fusion release energy for every possible pair of nuclei
  • Using Δm with the final mass minus initial mass when asked for energy released
Recall without your notes

What can you explain now?

What is nuclear fusion?

Compare with the explanation

Joining lighter nuclei to form a heavier nucleus

Fusion combines nuclei.

After trying it yourself, choose your next review. This is your self-assessment.

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Make it stick

How does the binding-energy curve explain energy release in fission and fusion?

If you needed the solution, close it and solve the problem again from a blank page. A correct answer is stronger when you can explain the reason for each step.

Keep learning Physics

Course scope and assessment

One hundred and sixty-two original lessons cover all 12 published subject-content outcomes in Topic 1 (sections 1.1–1.4), all nine outcomes in Topic 2 (section 2.1), all 13 outcomes in Topic 3 (sections 3.1–3.3), all 13 outcomes in Topic 4 (sections 4.1–4.3), all 11 outcomes in Topic 5 (sections 5.1–5.2), all 10 outcomes in Topic 6 (sections 6.1–6.2), all 16 outcomes in Topic 7 (sections 7.1–7.5), all 12 outcomes in Topic 8 (sections 8.1–8.4), all 15 outcomes in Topic 9 (sections 9.1–9.3), all 16 outcomes in Topic 10 (sections 10.1–10.3), all 18 outcomes in Topic 11 (sections 11.1–11.2), all seven outcomes in Topic 12 (sections 12.1–12.2), all 12 outcomes in Topic 13 (sections 13.1–13.4), all eight outcomes in Topic 14 (sections 14.1–14.3), and all nine outcomes in Topic 15 (sections 15.1–15.3), plus all four outcomes in Topic 16 (sections 16.1–16.2), and all ten outcomes in Topic 17 (sections 17.1–17.3), plus all 12 outcomes in Topic 18 (sections 18.1–18.5), all nine outcomes in Topic 19 (sections 19.1–19.3), all 19 outcomes in Topic 20 (sections 20.1–20.5), and all eight outcomes in Topic 21 (sections 21.1–21.2), and all 17 outcomes in Topic 22 (sections 22.1–22.4), and all 13 outcomes in Topic 23 (sections 23.1–23.2), and all 16 outcomes in Topic 24 (sections 24.1–24.3), and all 11 outcomes in Topic 25 (sections 25.1–25.3), of the 2025–2027 syllabus. Each lesson has guided, independent and application practice with explained answers. All 25 syllabus topics now have mapped teaching and practice; the 2028–2030 changes outside Topics 23–25 still need reconciliation. Online study cannot demonstrate supervised Paper 3 laboratory competence. Paper 5 planning and analysis, full timed cumulative assessment and human subject-teacher review remain outstanding.

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