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:

ParticleRelative ChargeRelative MassLocation
Proton+11Nucleus
Neutron01Nucleus
Electron−11/1836 (~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:

PropertyAlpha (α)Beta (β)Gamma (γ)
NatureHelium nucleus: ⁴₂He (2 protons + 2 neutrons)Fast-moving electron: ⁰₋₁eElectromagnetic wave (high-frequency EM radiation)
Charge+2−10 (no charge)
Mass (relative)4~0 (1/1836)0
Ionising abilityMost ionising (strongly ionises atoms it passes near)Moderately ionisingLeast ionising
Penetrating powerLeast penetrating — stopped by a few cm of air, a sheet of paper, or dead skin cellsModerately penetrating — stopped by a few mm of aluminiumMost penetrating — reduced (not completely stopped) by several cm of lead or metres of concrete
Deflection in electric fieldDeflected 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 fieldDeflected (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 lightUp to ~90% of speed of lightSpeed of light (3 × 10⁸ m/s)
Emitted by nuclei withToo 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):

  1. Read the initial count rate or number of nuclei at time = 0
  2. Find half of this value on the y-axis
  3. Read across to the curve and down to the x-axis — this time is the half-life
  4. 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:

SourceTypeTypical 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 testingVarious<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 TypeApplicationWhy 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 productionA 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 foodGamma 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 radiotherapyA 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 testingGamma 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:

  1. A large unstable nucleus (e.g., Uranium-235 or Plutonium-239) absorbs a slow/thermal neutron
  2. The nucleus becomes highly unstable and splits into two smaller daughter nuclei (fission fragments)
  3. 2 or 3 neutrons are also released (typically 2.5 on average)
  4. 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.

ComponentFunction
Fuel rodsContain 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 exchangerHot 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)
  • 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

MisconceptionReality
”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