About
The nucleus holds enormous energy — released either by splitting heavy nuclei (fission) or combining light ones (fusion). This chapter explains both processes, how nuclear reactors work, how stars shine, and how to calculate the energy released in nuclear reactions.
Key Concepts
27.1 Nuclear Reactions
Governed by conservation of:
- Mass number (A)
- Atomic number (Z)
- Energy and momentum
Examples:
- ¹⁹F₉ + ¹H₁ → ¹⁶O₈ + ⁴He₂
- ²⁷Al₁₃ + ¹n₀ → ²⁴Na₁₁ + ⁴He₂
- ²³⁴Th₉₀ → ²³⁴Pa₉₁ + ⁰e₋₁ (β⁻ decay)
- ⁶³Cu₂₉ + ²D₁ → ⁶⁴Zn₃₀ + ¹n₀
Q-value (energy released):
Where .
27.2 Nuclear Fission
The splitting of a heavy nucleus (e.g., ²³⁵U) into two lighter nuclei when bombarded with a neutron, releasing huge energy.
Chain reaction: The released neutrons trigger further fissions — controlled (reactor) or uncontrolled (bomb).
Nuclear reactor components:
- Fuel: ²³⁵U
- Moderator: Slows neutrons (heavy water, graphite)
- Control rods: Absorb neutrons (cadmium, boron)
- Coolant: Transfers heat
27.3 Nuclear Fusion
Combining light nuclei (e.g., hydrogen isotopes) to form heavier ones, releasing energy.
- Requires extremely high temperature (~10⁷ K) — thermonuclear reaction
- Powers the Sun and stars (hydrogen → helium)
- Advantage: abundant fuel, less radioactive waste
- Challenge: confinement of plasma
INTEXT QUESTIONS 27.1
Q1. Complete the nuclear reactions:
(a) ¹⁹F₉ + ¹H₁ → ¹⁶O₈ + ? Ans: A: 19 + 1 − 16 = 4. Z: 9 + 1 − 8 = 2. → ⁴He₂ (α-particle).
(b) ²⁷Al₁₃ + ¹n₀ → ? + ⁴He₂ Ans: A: 27 + 1 − 4 = 24. Z: 13 + 0 − 2 = 11. → ²⁴Na₁₁.
(c) ²³⁴Th₉₀ → ²³⁴Pa₉₁ + ? Ans: A: 0, Z: −1. → ⁰e₋₁ (β-particle).
(d) ⁶³Cu₂₉ + ²D₁ → ⁶⁴Zn₃₀ + ? Ans: A: 63 + 2 − 64 = 1. Z: 29 + 1 − 30 = 0. → ¹n₀ (neutron).
Q2. Calculate energy released in ¹⁰B₅ + ²D₁ → ?
Ans: u u u MeV
Terminal Exercise
-
Distinguish between nuclear fission and nuclear fusion. Give two examples of each.
-
What is a chain reaction? Explain the difference between controlled and uncontrolled chain reactions.
-
Describe the principle and working of a nuclear reactor with a labelled diagram.
-
Explain the proton-proton cycle in stars.
-
Calculate the energy released in the fission of 1 g of ²³⁵U. (Energy per fission ≈ 200 MeV, )
-
Complete the reactions: (a) ²³⁵U₉₂ + ¹n₀ → ¹⁴¹Ba₅₆ + ⁹²Kr₃₆ + ? (b) ²H + ²H → ³He + ?
-
State the advantages and challenges of fusion energy.
-
Calculate the Q-value of: ²H + ³H → ⁴He + n. (Given: m(²H) = 2.014102 u, m(³H) = 3.016049 u, m(⁴He) = 4.002603 u, m(n) = 1.008665 u)
-
Why are neutrons more effective than protons in inducing nuclear reactions?
-
What is critical mass? Why is it important for a chain reaction?
Quick Revision
| Concept | Key Point |
|---|---|
| Fission | Heavy nucleus splits → ~200 MeV |
| Fusion | Light nuclei combine → ~17.6 MeV |
| Chain reaction | Neutrons trigger more fissions |
| Moderator | Slows neutrons (D₂O, graphite) |
| Control rods | Absorb neutrons (Cd, B) |
| Q-value | MeV |
| Conservation | A and Z conserved in nuclear reactions |
