We assume you already met the atom & isotopes in P1 Matter — here we use that model rather than re-teach it. Higher-Tier-only ideas are clearly flagged with a HT badge.
How it works: read each idea, then answer to unlock the next screen. Equations, labelled diagrams, decay-equation drills and two sorting games are all in here. Tap Start.
P5.1 · Wave behaviour
Waves carry energy, not matter
A wave is a way of transferring energy from one place to another without transferring matter. The medium (water, air, a slinky) just oscillates on the spot. There are two shapes:
Transverse: oscillations are at right angles to travel (water ripples, all EM waves). Longitudinal: oscillations are along the travel direction, giving compressions and rarefactions (sound).
Watch out: the slinky (or water) does not move along with the wave — it vibrates about a fixed point. Evidence: a floating duck bobs up and down but doesn't get carried to shore. It's the wave that travels, not the medium.
P5.1 · Wave behaviour
The four words to describe a wave
Amplitude — maximum displacement from rest (metres). Bigger amplitude = more energy.
Wavelength (λ) — distance for one complete cycle, e.g. crest to crest (metres).
Frequency (f) — number of complete waves passing a point each second (hertz, Hz).
Period (T) — time for one complete wave to pass (seconds).
Frequency and period are two views of the same thing:
T = 1 / f
period T (s) = 1 ÷ frequency f (Hz). A 5 Hz wave has period 1 ÷ 5 = 0.2 s.
On the oscilloscope: a sound wave shown as a trace — taller spike = louder (amplitude); spikes closer together = higher pitch (frequency). The trace itself looks transverse, but the sound is still a longitudinal wave.
P5.1 · Wave behaviour
How fast does a wave travel?
Every wave obeys the wave equation:
v = f λ
wave speed v (m/s) = frequency f (Hz) × wavelength λ (m)
You can also find a wave's speed by timing it over a measured distance — this is how you measure the speed of a wave in the required practical (e.g. ripples across a tank, or the speed of sound down a tube):
v = x / t
speed v (m/s) = distance x (m) ÷ time t (s)
Worked example
A wave in a ripple tank has frequency 8 Hz and wavelength 0.05 m.
v = f λ = 8 × 0.05 = 0.4 m/s.
Watch out: wavelength is in metres. If you're told 5 cm, use 0.05 m, or your answer will be 100× too big.
Calculate
Your turn — period
1A water wave has a frequency of 4 Hz. Calculate its period.
s
Hint: T = 1 ÷ f = 1 ÷ 4.
Calculate
Your turn — wave speed
2A sound wave has frequency 170 Hz and wavelength 2 m. Calculate its speed.
m/s
Hint: v = f λ = 170 × 2.
Calculate
Your turn — rearrange
3A radio wave travels at 3 × 10⁸ m/s with a frequency of 1.0 × 10⁸ Hz. Calculate its wavelength.
m
Hint: λ = v ÷ f = (3 × 10⁸) ÷ (1.0 × 10⁸).
P5.1 · Wave behaviour
Waves at a boundary
When a wave meets the boundary between two materials, three things can happen — and usually a mix of all three:
Reflection — the wave bounces back (echoes, a mirror).
Transmission — the wave passes through into the new material.
Absorption — the wave's energy is taken in by the material (it warms up).
Ultrasound (sound above ~20 000 Hz, beyond human hearing) and sonar use partial reflection at boundaries: a pulse is sent in, reflects off a boundary deeper in, and the echo time gives the distance. Uses include foetal scans, detecting flaws in metal, and ships measuring the depth of the sea floor.
distance = ½ × v × t
The pulse travels there and back, so halve the total — speed v (m/s), echo time t (s)
HT extension (P5.1f): when sound passes from one medium to another its speed and wavelength change together, but its frequency stays the same.
P5.1 · Wave behaviour
Modelling & measuring waves
Ripples on water model a transverse wave — you can see crests and troughs and measure λ directly.
Sound in air is a longitudinal wave — you can find its speed by timing an echo, or with two microphones a known distance apart.
Floating objects bob but don't drift along — evidence that the wave, not the water or air, travels.
HT — hearing (P5.1h–i): the ear converts sound waves in air into vibrations of solid parts (eardrum → tiny bones → cochlea). This only works over a limited frequency range — roughly 20 Hz to 20 000 Hz in healthy young humans — and the upper limit drops with age.
Quick check
Which wave is which?
?Sound travelling through air is best described as which type of wave?
P5.2 · The electromagnetic spectrum
The electromagnetic spectrum
EM waves are a family of transverse waves that transfer energy from a source to an absorber. In a vacuum they all travel at the same speed — the speed of light, 3 × 10⁸ m/s. They differ only in frequency and wavelength:
Order from longest wavelength to shortest: Radio → Microwave → Infra-red → Visible → Ultraviolet → X-rays → Gamma. (Mnemonic: Raging Martians Invaded Venus Using X-ray Guns.)
Watch out: a common error is thinking these are separate, unrelated things. They are one continuous spectrum — and crucially, in a vacuum all EM waves travel at the same speed. They are not "faster" or "slower" because of their frequency.
P5.2 · The electromagnetic spectrum
How EM waves are made & detected
Light is an EM wave — visible light is just the thin band our eyes can detect (red → violet). We can only see a tiny slice of the whole spectrum.
EM waves are generated by changes in atoms and nuclei, and are absorbed by them too — so atoms can emit and soak up radiation across a wide frequency range.
HT (P5.2j): radio waves can be produced by — and can themselves induce — oscillations in electrical circuits.
Generated & absorbed: heating an object makes it emit infra-red; nuclear changes can release gamma rays. Absorption is the reverse — energy is transferred from the wave into the absorber.
P5.2 · The electromagnetic spectrum
Uses & dangers
Radio — TV & radio broadcasting, communications.
Microwave — cooking (heats water in food), satellite & mobile-phone signals.
X-rays — medical imaging of bones, airport security. Danger: ionising — can mutate cells & cause cancer.
Gamma — sterilising equipment & food, killing cancer cells (radiotherapy), medical tracers. Danger: highly ionising — kills/mutates cells.
The pattern: the higher the frequency (UV → X-ray → gamma), the more energy each wave carries and the more hazardous to body tissue it is, because it becomes ionising. HT (P5.2i): differences in how tissues absorb/reflect IR, X-rays, gamma and ultrasound let us image structures hidden inside the body.
Order it
Put the spectrum in order
Tap the band that has the longest wavelength of those still left. Build the spectrum radio → gamma.
Quick check
Spot the right statement
?Which statement about electromagnetic waves travelling through a vacuum is correct?
P5.3 · Wave interactions
Lenses & ray diagrams
A lens refracts (bends) light because light changes speed when it enters the glass. OCR expects you to use ray diagrams (qualitative — no equations) to compare two lenses:
A convex lens converges parallel rays to a real focus; a concave lens diverges them so they appear to come from a virtual focus behind the lens. These are used to correct long- and short-sightedness.
HT (P5.3a–b): how much a substance absorbs, transmits, refracts or reflects EM waves can vary with wavelength, and refraction effects come from the wave's change in velocity between substances.
P5.3 · Wave interactions
Colour, filters & reflection
An object's colour comes from differential absorption, transmission and reflection: a red apple reflects red light and absorbs the rest.
A colour filter transmits its own colour and absorbs the others — it does not add colour to the light.
Specular reflection (smooth surface, like a mirror) gives a clear image; diffuse scattering (rough surface) sends rays in all directions.
Watch out: mixing coloured light is not the same as mixing paint. A filter can only remove colours — never create new ones.
Quick check
Lenses & colour
?Parallel rays of light pass through a lens and come together at a single point (a real focus). What kind of lens is it?
P6.1 · Radioactive emissions
Unstable nuclei decay — at random
Some nuclei are unstable. To become more stable they emit radiation. We can't predict when any one nucleus will decay — radioactive decay is a random, spontaneous process. The unstable nuclei can emit:
Alpha (α) — a helium nucleus: 2 protons + 2 neutrons. Symbol 42He (or 42α).
Beta (β) — a fast electron, 0−1e, made when a neutron turns into a proton.
Gamma (γ) — a high-frequency EM wave; carries away energy but no mass or charge.
Neutron (n) — some unstable nuclei can also emit a neutron, 10n.
Use the P1 atom model, don't re-teach it: you already know an atom is a tiny positive nucleus of protons + neutrons surrounded by electrons, and that isotopes are atoms of the same element with different neutron numbers. Here we use that to follow what happens to mass and charge.
P6.1 · Radioactive emissions
Penetration, range & ionising power
The three radiations differ in how far they travel and what stops them:
Alpha is stopped by a sheet of paper (or a few cm of air). Beta passes through paper but is stopped by a few mm of aluminium. Gamma is the most penetrating — only reduced by thick lead or concrete.
Watch out — the trade-off:alpha is the most ionising (it deposits its energy quickly) but the least penetrating. Gamma is the least ionising but the most penetrating. Penetrating power and ionising power run opposite ways.
Match it
Match radiation to its barrier
Tap a radiation on the left, then tap the material that just stops it on the right.
P6.1 · Radioactive emissions
Balancing nuclear equations
In any decay, both the mass number (top) and the charge / atomic number (bottom) must be conserved — the totals on each side are equal.
Alpha: nucleus loses 2 protons + 2 neutrons → mass number falls by 4, atomic number falls by 2.
Beta: a neutron becomes a proton + the emitted electron → mass number unchanged, atomic number rises by 1.
Gamma: only energy leaves — no change to mass number or atomic number.
Check both lines balance: 238 = 234 + 4 ✓ and 92 = 90 + 2 ✓. If they don't add up, your equation is wrong.
Calculate
Balance an alpha decay
422688Ra decays by emitting an alpha particle. What is the mass number of the new nucleus?
(mass no.)
Hint: alpha removes mass 4 → 226 − 4.
Quick check
What changes in beta decay?
?A nucleus emits a beta particle. What happens to its mass number and atomic number?
P6.1 · Radioactive emissions
Half-life
Because decay is random, we describe a source by its half-life: the average time for half the unstable nuclei in a sample to decay (equivalently, the time for the count-rate to halve).
The count halves every half-life: 100 → 50 → 25 → 12.5%. After n half-lives the fraction remaining is (½)ⁿ. The curve flattens but never reaches zero.
HT (P6.1k): after a whole number n of half-lives, the fraction remaining is (½)ⁿ. So the net decline as a ratio after 3 half-lives is 7:1 (1 part left, 7 parts decayed). You should also be able to read half-lives off a graph.
Calculate
Count-rate after n half-lives
5A source has a corrected count-rate of 800 counts/min. Its half-life is 6 hours. What will the corrected count-rate be after 18 hours?
We are always surrounded by low-level background radiation from natural and human-made sources:
Natural: radon gas from rocks & soil, cosmic rays from space, food and drink, building materials.
Human-made: medical X-rays & nuclear medicine, fallout, the nuclear industry (a small fraction of the total).
Watch out — subtract the background: a Geiger–Müller tube always picks up background. To find a source's true activity you measure the background count first and subtract it from your readings to get the corrected count-rate. Always correct before doing half-life sums.
Calculate
Correct for background
6A Geiger counter reads 530 counts/min next to a source. The background count is measured as 30 counts/min. What is the corrected count-rate of the source?
Irradiation — being exposed to radiation from an outside source. The object does not become radioactive itself, and stops being irradiated when the source is removed.
Contamination — getting radioactive atoms onto or inside you. They keep emitting radiation until they decay, so contamination is hard to remove and can be long-lasting.
The hazard depends on the half-life and the type of radiation. Inside the body, alpha is most dangerous (very ionising); outside, gamma and beta are the bigger worry because they penetrate the skin.
Uses: smoke detectors (alpha source — short range makes them suitable & safe), medical tracers to image organs, and radiotherapy to control or destroy cancer tissue.
Watch out: an irradiated apple is not radioactive — irradiation does not make things radioactive. Only contamination transfers radioactive material.
P6.2 · Uses & hazards
Nuclear fission & fusion
Fission — a large unstable nucleus splits into smaller nuclei, releasing energy and neutrons. Those neutrons can split more nuclei — a chain reaction. In a reactor, control rods absorb neutrons to keep the chain reaction steady.
Fusion — small nuclei join to form a larger one, releasing energy. This is how the Sun shines. In fusion, mass is converted into the energy of radiation.
HT note: both fission and fusion release energy because the products are more stable than the starting nuclei. Fusion needs enormous temperatures and pressures, which is why it's so hard to do on Earth.
Quick check
Irradiation or contamination?
?A worker breathes in dust containing radioactive atoms, which lodge in their lungs. This is an example of:
Sort it
Waves or Radioactivity?
Tap a fact, then tap whether it belongs to P5 Waves or P6 Radioactivity.
🌊 P5 Waves
☢️ P6 Radioactivity
Recap
The must-knows
Wave equations: v = f λ · v = x / t · T = 1 / f
Wave types: transverse (vibration ⟂ travel, e.g. EM & ripples) vs longitudinal (∥ travel, e.g. sound).
EM spectrum: Radio → Microwave → Infra-red → Visible → UV → X-ray → Gamma — all transverse, all 3 × 10⁸ m/s in vacuum.
Lenses: convex converges to a real focus; concave diverges from a virtual focus.
Radiation: α (stopped by paper, most ionising) · β (stopped by aluminium) · γ (most penetrating, needs lead).
Decay: mass & charge conserved. Alpha: mass −4, charge −2. Beta: mass same, charge +1.
Half-life: time for half the nuclei (or the count-rate) to decay; fraction left after n half-lives = (½)ⁿ; subtract background first.