Nuclear Physics
Summary: Covers atomic structure (linking to Chemistry), isotopes, radioactivity (alpha, beta, gamma), half-life calculations, background radiation, uses and dangers of ionising radiation, nuclear fission (chain reactions, nuclear reactors), and nuclear fusion. This topic ties together physics, chemistry, and real-world energy applications. Tags: igcse physics nuclear radioactivity radiation fission fusion Created: 2026-07-16 Last Updated: 2026-07-16
Atomic Structure (Brief Recap)
An atom consists of:
| Particle | Relative Charge | Relative Mass | Location |
|---|---|---|---|
| Proton | +1 | 1 | Nucleus |
| Neutron | 0 | 1 | Nucleus |
| Electron | −1 | 1/1836 (~0) | Electron shells |
- Atomic number (Z) = number of protons
- Mass number (A) = protons + neutrons
- In a neutral atom: number of protons = number of electrons
For a more detailed treatment of atomic structure, electron configurations, and nuclide notation, see the IGCSE Chemistry Atomic Structure page.
Isotopes
Definition: Isotopes are atoms of the same element (same number of protons/atomic number) with different numbers of neutrons (different mass numbers).
- Same chemical properties (same electron configuration)
- Different physical properties (different mass)
- Some isotopes are radioactive (unstable nucleus — will decay)
Radioactivity
Radioactivity is the spontaneous emission of radiation from an unstable nucleus as it decays to become more stable. This is a random process — it is not possible to predict when an individual nucleus will decay, but the behaviour of a large number of nuclei can be described statistically.
Three types of nuclear radiation:
| Property | Alpha (α) | Beta (β) | Gamma (γ) |
|---|---|---|---|
| Nature | Helium nucleus: ⁴₂He (2 protons + 2 neutrons) | Fast-moving electron: ⁰₋₁e | Electromagnetic wave (high-frequency EM radiation) |
| Charge | +2 | −1 | 0 (no charge) |
| Mass (relative) | 4 | ~0 (1/1836) | 0 |
| Ionising ability | Most ionising (strongly ionises atoms it passes near) | Moderately ionising | Least ionising |
| Penetrating power | Least penetrating — stopped by a few cm of air, a sheet of paper, or dead skin cells | Moderately penetrating — stopped by a few mm of aluminium | Most penetrating — reduced (not completely stopped) by several cm of lead or metres of concrete |
| Deflection in electric field | Deflected towards negative plate (small deflection due to large mass) | Deflected towards positive plate (large deflection due to small mass) | No deflection (no charge) |
| Deflection in magnetic field | Deflected (according to Fleming’s Left Hand Rule, small deflection) | Deflected in opposite direction (large deflection) | No deflection (no charge) |
| Speed | ~5-10% of speed of light | Up to ~90% of speed of light | Speed of light (3 × 10⁸ m/s) |
| Emitted by nuclei with | Too many protons and neutrons (heavy nuclei, e.g., uranium, radium) | Too many neutrons relative to protons (neutron → proton + electron) | Excess energy after alpha or beta decay |
Nuclear equations — when a nucleus decays:
- Alpha decay: mass number decreases by 4, atomic number decreases by 2
- Example: ²³⁸₉₂U → ²³⁴₉₀Th + ⁴₂He (α particle)
- Beta decay: mass number stays the same, atomic number increases by 1 (a neutron changes into a proton + electron)
- Example: ¹⁴₆C → ¹⁴₇N + ⁰₋₁e (β particle)
- Gamma decay: no change to mass number or atomic number. The nucleus just loses excess energy.
Example 1: Radium-226 (²²⁶₈₈Ra) decays by alpha emission. Identify the daughter nucleus.
²²⁶₈₈Ra → ⁴₂He + ²²²₈₆X
X has Z = 86, which is Radon (Rn). So the equation is: ²²⁶₈₈Ra → ²²²₈₆Rn + ⁴₂He
Example 2: Carbon-14 (¹⁴₆C) decays by beta emission. Identify the daughter nucleus.
¹⁴₆C → ⁰₋₁e + ¹⁴₇X
X has Z = 7, which is Nitrogen (N). So the equation is: ¹⁴₆C → ¹⁴₇N + ⁰₋₁e
Half-Life
Definition: The half-life of a radioactive isotope is the time taken for half the radioactive nuclei in a sample to decay. Alternatively: the time for the count rate (activity) of a sample to fall to half its initial value.
Key points:
- Half-life is constant for a given isotope — it cannot be changed by temperature, pressure, or chemical reactions
- Half-lives range from fractions of a second to billions of years
Half-life from a graph (decay curve):
- Read the initial count rate or number of nuclei at time = 0
- Find half of this value on the y-axis
- Read across to the curve and down to the x-axis — this time is the half-life
- Repeat for a second half-life to check consistency
Example 3: A radioactive sample has an initial activity of 800 Bq. Its half-life is 3 hours. What is the activity after 12 hours?
Number of half-lives = 12 / 3 = 4
After 1 half-life: 800 → 400 Bq
After 2 half-lives: 400 → 200 Bq
After 3 half-lives: 200 → 100 Bq
After 4 half-lives: 100 → 50 Bq
Answer: 50 Bq
Example 4: A sample decays from 1000 counts per minute to 125 counts per minute in 9 days. Find the half-life.
1000 → 500 → 250 → 125 (3 half-lives)
3 half-lives = 9 days → half-life = 3 days
Background Radiation
We are constantly exposed to low levels of radiation from natural and artificial sources:
| Source | Type | Typical Contribution |
|---|---|---|
| Radon gas (from rocks containing uranium) | Alpha | ~50% (largest single source) |
| Cosmic rays (from the Sun and outer space) | Various (mostly high-energy particles) | ~10% |
| Rocks and soil (granite contains uranium/thorium) | Alpha, beta, gamma | ~14% |
| Food and drink (e.g., bananas contain potassium-40) | Beta, gamma | ~12% |
| Medical (X-rays, radiotherapy, nuclear medicine) | X-rays, gamma | ~14% |
| Nuclear industry / fallout from testing | Various | <1% |
Measuring background radiation: When performing experiments with radioactive sources, always measure and subtract the background count. Use a Geiger-Muller (GM) tube and counter.
Uses of Radioactivity
| Radiation Type | Application | Why This Type? |
|---|---|---|
| Alpha (α) | Smoke detectors (Americium-241) | Alpha particles ionise air between two electrodes → small current flows. Smoke absorbs alpha particles → current drops → alarm sounds. Alpha is used because: (a) it is highly ionising (creates detectable current), (b) it has very low penetrating power — does not escape the detector housing, making it safe |
| Beta (β) | Thickness gauges in paper/foil/aluminium production | A beta source is placed on one side of the material, a detector on the other. If the material is too thick: fewer beta particles reach detector → rollers adjust to make it thinner. If material too thin: more beta particles reach detector → rollers adjust. Beta used because: penetration is sensitive to thickness of material. Alpha would be stopped by paper; gamma would pass through regardless |
| Gamma (γ) | Sterilising medical equipment and food | Gamma rays kill bacteria/microorganisms by damaging their DNA. Equipment is sealed in packages first (gamma penetrates the packaging). Advantages: no heat needed (can sterilise heat-sensitive items like plastic syringes), no toxic chemicals |
| Gamma (γ) | Cancer radiotherapy | A narrow beam of gamma rays is targeted at a tumour from multiple angles. The tumour receives a high dose (killing cancer cells), while surrounding healthy tissue receives minimal dose from any single beam. Gamma used because it is highly penetrating and can reach deep tumours |
| Gamma (γ) | Industrial radiography / Non-destructive testing | Gamma source placed inside a pipe or behind welded metal; detector on other side checks for cracks, flaws, or corrosion. Gamma penetrates the metal |
| Gamma (γ) | Tracers in medicine and industry (e.g., detecting leaks in underground pipes) | A small amount of gamma-emitting isotope is injected into a system. A detector follows its path/movement. Gamma is used because it can be detected outside the body/pipe (penetrates to the surface). Short half-life isotopes are used to minimise long-term exposure |
Dangers of Ionising Radiation
Ionising radiation (alpha, beta, gamma, X-rays) can damage cells and DNA:
- Low doses: DNA mutations → potentially cancer (leukaemia, thyroid cancer, etc.)
- High doses: radiation sickness (nausea, vomiting, hair loss, organ failure) → death
- Alpha is most dangerous if ingested/inhaled: Inside the body, alpha’s high ionising power causes concentrated damage to a small area of tissue. Alpha cannot penetrate dead skin, so external alpha sources are relatively safe
- Gamma is the most dangerous externally: It can penetrate deep into the body and reach vital organs
Safety precautions when handling radioactive sources:
- Minimise exposure time
- Maximise distance from source (inverse square law — doubling distance reduces exposure to 1/4)
- Use appropriate shielding (lead for gamma, perspex for beta)
- Never point a source directly at anyone
- Handle sources with tongs/forceps (never bare hands)
- Store sources in lead-lined containers when not in use
- Wash hands after handling sources
Nuclear Fission
Nuclear fission is the splitting of a large, unstable nucleus into two (or more) smaller nuclei, releasing energy and neutrons.
Process:
- A large unstable nucleus (e.g., Uranium-235 or Plutonium-239) absorbs a slow/thermal neutron
- The nucleus becomes highly unstable and splits into two smaller daughter nuclei (fission fragments)
- 2 or 3 neutrons are also released (typically 2.5 on average)
- A large amount of energy is released (as kinetic energy of the fission fragments and neutrons, and as gamma radiation)
Example fission equation:
²³⁵₉₂U + ¹₀n → ¹⁴¹₅₆Ba + ⁹²₃₆Kr + 3(¹₀n) + energy
Chain Reaction: The neutrons released by one fission event can be absorbed by other U-235 nuclei, causing them to fission and release more neutrons. This creates a self-sustaining chain reaction.
- Uncontrolled chain reaction → nuclear bomb (all neutrons cause further fissions)
- Controlled chain reaction → nuclear reactor (some neutrons absorbed to maintain a steady rate)
Nuclear Reactor
A nuclear power station uses controlled fission to produce heat → steam → turbine → generator → electricity.
| Component | Function |
|---|---|
| Fuel rods | Contain U-235 (enriched to ~3-5%) or Pu-239. Fission occurs here |
| Moderator (water or graphite) | Slows down the fast neutrons produced by fission. Slow/thermal neutrons are more likely to be captured by U-235 nuclei and cause further fission. The moderator surrounds the fuel rods |
| Control rods (boron or cadmium) | Absorb excess neutrons to control the rate of the chain reaction. Lowered into reactor → absorb more neutrons → reduce rate. Raised → fewer neutrons absorbed → increase rate. In an emergency, fully inserted to SCRAM/shut down reactor |
| Coolant (water, CO₂, or liquid sodium) | Transfers thermal energy from the reactor core to a heat exchanger/steam generator. Circulates through the core and becomes hot |
| Heat exchanger | Hot coolant heats water in a secondary loop → water turns to steam → steam drives turbine → turbine drives generator → electricity |
| Shielding (thick concrete and steel) | Protects workers and the environment from radiation |
Advantages of nuclear power:
- No CO₂ or SO₂ emissions (does not contribute to global warming or acid rain)
- Very high energy density — small amounts of fuel produce huge amounts of energy
- Reliable baseload power (not intermittent like wind/solar)
Disadvantages of nuclear power:
- Radioactive waste products — remain dangerous for thousands of years; need secure long-term storage
- Risk of catastrophic accidents (Chernobyl 1986, Fukushima 2011) — release of radioactive material into environment
- High decommissioning costs — reactors cannot simply be demolished; must be carefully dismantled
- Uranium is a finite (non-renewable) resource
- Public opposition due to safety concerns
Nuclear Fusion
Nuclear fusion is the joining of two light nuclei to form a heavier nucleus, releasing a very large amount of energy.
Example: In the Sun, hydrogen nuclei (protons) fuse to form helium:
⁴(¹₁H) → ⁴₂He + 2(⁰₊₁e) + energy
(This is a simplified version — the actual process in stars is the proton-proton chain)
Conditions required for fusion:
- Very high temperature (~10-100 million °C) — so nuclei have enough kinetic energy to overcome their mutual electrostatic repulsion (both nuclei are positively charged)
- Very high pressure — to bring nuclei close enough for the strong nuclear force (attractive) to take over from the electrostatic force (repulsive)
Nuclear fusion as an energy source on Earth:
- Advantages: virtually unlimited fuel (deuterium and tritium from seawater), no long-lived radioactive waste (main product is helium), no CO₂, safer than fission (no chain reaction to run out of control — if conditions fail, fusion simply stops)
- Disadvantages: currently, a sustained fusion reaction producing net energy output has not yet been achieved on a commercial scale. Temperatures and pressures needed are extremely difficult to achieve and contain (no known material can withstand the temperature). Research continues (ITER project, tokamaks using magnetic confinement; laser-driven inertial confinement)
Fusion in stars: The immense gravity in stars provides the necessary temperature and pressure naturally. This is the process powering the Sun and all stars.
Sources
- BBC Bitesize GCSE Physics — Nuclear/atomic physics guide, BBC (free educational resource)
- OpenStax College Physics — Nuclear Physics chapter, Rice University (free, CC BY 4.0)
- Cambridge IGCSE Physics 0625 — Nuclear physics section, Cambridge Assessment International Education
- CK-12 Physics for High School — Nuclear Physics chapter, CK-12 Foundation (free, CC BY-NC 3.0)
Related Notes
- Atomic Structure (IGCSE Chemistry) — Detailed treatment of atomic structure, electron configuration, and isotopes
- Energy Resources and Transfer — Nuclear power as an energy resource, comparison with fossil fuels and renewables
- Waves — Gamma rays as part of the electromagnetic spectrum
- Space Physics — Nuclear fusion in stars as their energy source
- IGCSE-Phys-Index — Full IGCSE Physics index
Keywords
isotope, radioactivity, alpha, beta, gamma, ionising radiation, half-life, decay curve, background radiation, Geiger-Muller tube, nuclear fission, chain reaction, moderator, control rod, coolant, nuclear reactor, nuclear fusion, plasma, strong nuclear force, electrostatic repulsion
Common Misconceptions
| Misconception | Reality |
|---|---|
| ”All radiation is dangerous” | We are exposed to safe levels of background radiation constantly. The danger depends on the type, dose, and duration of exposure |
| ”Alpha radiation is the least dangerous because it can’t penetrate skin” | Externally, alpha is safest. But if an alpha source is inhaled or ingested, it is the most dangerous because it deposits all its energy in a tiny area of tissue, causing intense localised damage |
| ”Half-life changes with temperature or chemical state” | Half-life is a property of the nucleus and is unaffected by external conditions. Radioactive decay cannot be sped up, slowed down, or stopped |
| ”After two half-lives, all the radioactive material is gone” | After two half-lives, 1/4 remains. After three half-lives, 1/8 remains, and so on. The sample never mathematically reaches zero (though practically it becomes indistinguishable from background) |
| “Nuclear fusion is the same as burning” | Fusion is a nuclear process, not a chemical one. The Sun does not “burn” in the chemical sense — it fuses hydrogen into helium. The energy released is millions of times greater per unit mass |
| ”A nuclear reactor can explode like a nuclear bomb” | Nuclear reactors cannot explode like a nuclear bomb. The fuel enrichment is far too low (~3-5% vs >90% for weapons). Reactor accidents involve steam/hydrogen explosions or meltdowns, not nuclear detonations |
| ”Radioactivity is a man-made phenomenon” | Radioactivity is natural — it has existed since the formation of the Earth. We are surrounded by natural radioactive elements in rocks, air, food, and cosmic rays |