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Chapter 16 of 16 · Physics
Nuclear Physics
Nuclear Physics averages 3 MCQs per paper — radioactivity, half-life, mass defect/binding energy, and fission/fusion are top-priority.
Nuclear Physics is a Physics chapter on the official PMDC MDCAT 2026 syllabus, contributing roughly 2 MCQs to the 36-MCQ Physics section. Mastering the core concepts below typically secures the full chapter weightage.
Nuclear structure
A nucleus is described by Z (proton number), N (neutron number), and A = Z+N (mass number). Notation: AZX. Isotopes share Z but differ in N (¹²C and ¹⁴C). Nuclear radius R = R₀A1/3, with R₀ ≈ 1.2 fm. Nuclear density is essentially constant at ~2.3×10¹⁷ kg/m³, independent of A — a hallmark of the strong force's short range and saturation.
Mass defect and binding energy
The actual nuclear mass is less than the sum of constituent nucleons; the deficit Δm is the mass defect. Binding energy BE = Δm·c² = Δm(amu)·931.5 MeV. Binding energy per nucleon peaks around 56Fe at about 8.8 MeV/nucleon — this is why both fission of heavy nuclei and fusion of light ones release energy. The ⁴He nucleus has BE/A ≈ 7.07 MeV (especially stable due to closed-shell structure).
Radioactive decay
Three modes: alpha (α = ⁴2He, A decreases by 4, Z by 2), beta-minus (β⁻: neutron → proton + e⁻ + ν̄, Z increases by 1), and gamma (γ: photon, no change in A or Z). Decay law N(t) = N₀e−λt; half-life t½ = ln 2/λ ≈ 0.693/λ. After n half-lives, fraction remaining = (½)n. Activity A = λN, in becquerels (1 Bq = 1 decay/s) or curies (1 Ci = 3.7×10¹⁰ Bq). Carbon-14 dating uses t½ = 5730 years; ¹³¹I (medical) has t½ = 8 days.
Fission and fusion
Fission: ²³⁵U + n → ¹⁴¹Ba + ⁹²Kr + 3n + ~200 MeV. The chain reaction sustains itself if at least one neutron causes another fission (criticality). Reactor moderators (graphite, heavy water) slow neutrons to thermal energies for higher fission cross-section. Fusion: ²H + ³H → ⁴He + n + 17.6 MeV, the basis of stars and H-bombs. The Sun fuses ~6×10¹¹ kg of hydrogen per second.
Detection and biological effects
Geiger-Müller counter detects ionising radiation via avalanche multiplication; scintillators and semiconductor detectors offer better energy resolution. Absorbed dose: gray (1 Gy = 1 J/kg). Equivalent dose multiplies by quality factor Q (alpha Q ≈ 20, beta/gamma Q ≈ 1) to give sieverts. Deterministic effects appear above thresholds; stochastic (cancer) increase linearly with dose. References: HRW Chapters 42-43, Serway Modern Physics Chapters 29-31, FSc Chapter 21.
Key Concepts
- Radioactive decay
- Half-life
- Nuclear fission & fusion
- Mass defect & binding energy
- Detectors (GM counter)
Worked MCQs
Q1. After 3 half-lives, the fraction of an isotope remaining is:
- A. 1/2
- B. 1/4
- C. 1/8 ✓
- D. 1/16
Explanation: (½)³ = 1/8.
Common trap: Computing 1/3 — half-lives compound multiplicatively, not linearly.
Q2. Mass defect of 0.1 amu corresponds to energy:
- A. 9.31 MeV
- B. 93.15 MeV ✓
- C. 931.5 MeV
- D. 0.931 MeV
Explanation: ΔE = Δm·931.5 = 0.1·931.5 = 93.15 MeV.
Common trap: Picking 931.5 — that's for 1 amu.
Q3. Beta-minus decay increases:
- A. A by 1
- B. Z by 1 ✓
- C. Z by 2
- D. N by 1
Explanation: n → p + e⁻ + ν̄: Z increases by 1, N decreases by 1, A unchanged.
Common trap: Choosing N by 1 — neutrons decrease in β⁻ decay.
Q4. Binding energy per nucleon is maximum near:
- A. ²H
- B. ⁴He
- C. ⁵⁶Fe ✓
- D. ²³⁵U
Explanation: Iron-56 sits at the peak of the BE/A curve at ~8.8 MeV/nucleon.
Common trap: Choosing ⁴He — it is locally stable but below iron's peak.
Q5. Half-life of a sample is 10 days. Initial activity 800 Bq. After 30 days, activity is:
- A. 50 Bq
- B. 100 Bq ✓
- C. 200 Bq
- D. 400 Bq
Explanation: 30/10 = 3 half-lives → 800·(½)³ = 100 Bq.
Common trap: Subtracting linearly gives 500 Bq.
Frequently Asked Questions
Why are heavy nuclei unstable?
Coulomb repulsion among many protons grows faster than the short-range strong force can compensate, lowering BE/A above iron.
What controls a nuclear reactor?
Control rods (cadmium, boron) absorb neutrons to keep the multiplication factor at exactly 1 (critical).
Why is fusion harder to achieve than fission?
Fusion requires temperatures of ~10⁸ K to overcome Coulomb repulsion between positive nuclei; fission is initiated by slow-neutron capture, which has no Coulomb barrier.
Are alpha particles dangerous outside the body?
Less so — they are stopped by skin or paper. Internally (inhaled or ingested) they cause severe damage owing to high quality factor.
Why is carbon-14 useful for dating?
Living organisms maintain a fixed ¹⁴C/¹²C ratio; after death the ratio decays with t_½ = 5730 yr, allowing samples up to ~50 000 years old to be dated.
How Nuclear Physics Is Tested
MDCAT questions on Nuclear Physics are a mix of recall (definitions, classifications), application (predict outcomes, interpret diagrams), and basic numerical/analytical reasoning. PMDC papers from 2020–2025 emphasized the concepts above; older UHS papers (2008–2019) tested them too, with slight variations in question framing.
Practice
Drill Nuclear Physics and the rest of Physics — free, no signup.
See the full MDCAT 2026 syllabus or browse all Physics chapters.