This mini-lesson covers the whole of 4PH1 Section 5: density and pressure, pressure in a liquid column, change of state and the particle model, and the kinetic theory of gases with the Kelvin scale and the gas laws.
Work through each screen, answer the questions as you go (some wordy, some calculations) and collect ⭐ stars. Press Start when you're ready.
Section 5 expects you to work confidently in these SI units:
Paper 2 only (5.2P): for specific heat capacity you also use J/kg °C (joules per kilogram per degree Celsius).
Density tells you how much mass is squeezed into each cubic metre of a material:
Measuring it (5.4 practical): find the mass on a balance. For a regular solid, measure its sides and calculate the volume; for an irregular solid or a liquid, use a displacement can or measuring cylinder. Then divide.
A metal block has mass 240 g (= 0.24 kg) and volume 0.00003 m³.
ρ = 0.24 ÷ 0.00003 = 8000 kg/m³ (this is copper).
Pressure is the force acting on each square metre of a surface:
The same force over a smaller area gives a bigger pressure — which is why a sharp knife or a drawing pin works.
Acts in all directions (5.6): at any point in a gas or a liquid at rest, the pressure pushes equally in every direction — up, down and sideways — not just downwards.
A box pushes down with a force of 600 N over an area of 0.5 m².
p = 600 ÷ 0.5 = 1200 Pa
Dive deeper and the weight of water above you grows, so the pressure difference increases:
Watch out: pressure in a liquid depends on depth and density, not the shape of the container or how much liquid there is in total. A narrow tube and a wide tank give the same pressure at the same depth.
Depth 2 m, water density 1000 kg/m³, g = 10 N/kg.
p = 2 × 1000 × 10 = 20 000 Pa
The kinetic theory explains the states by how the particles are arranged and moving:
Heating (5.8P–5.9P): heating raises the energy stored in the particles, so the temperature rises or the state changes — a solid melts, then the liquid evaporates/boils to a gas. During a change of state the temperature stays constant while bonds are broken.
The specific heat capacity c is the energy needed to change the temperature of 1 kg by 1 °C:
Water has a high c (4200 J/kg °C), so it heats and cools slowly — useful in radiators and for the climate near the sea.
Practical (5.14P): heat a known mass with an electric heater, measure the energy supplied and the temperature rise, then find c = ΔQ ÷ (m × ΔT). A temperature–time graph (5.11P) shows the flat region while a substance changes state.
Heating 0.5 kg of water (c = 4200) by 30 °C:
ΔQ = 0.5 × 4200 × 30 = 63 000 J (63 kJ)
Gas molecules have random motion. Each time one hits a wall it bounces off, exerting a tiny force. Billions of collisions every second add up to a steady pressure:
Watch out: gas pressure is not the gas "pressing because it is heavy" — it is the result of countless molecular collisions with the container walls.
For a fixed amount of gas, tap how the molecular collisions explain each change.
Cool a gas and its molecules slow down. At −273 °C they have the least possible energy — you cannot go colder. This is absolute zero, the start of the Kelvin scale:
Absolute zero = 0 K = −273 °C. There is no such thing as a negative kelvin temperature.
Raising the temperature gives molecules more energy, so on average they move faster. In fact:
This is why temperature is measured from absolute zero: at 0 K the average kinetic energy is (as near as possible) zero, so it makes sense to say the energy is proportional to the Kelvin temperature — that statement would fail with the Celsius scale.
Link to pressure: faster molecules hit the walls harder and more often, so for a fixed volume a higher temperature gives a higher pressure.
For a fixed mass of gas at constant temperature, squeezing it into a smaller volume packs the same molecules into less space, so they hit the walls more often and the pressure rises:
Gas at 100 000 Pa in 0.6 m³ is compressed to 0.2 m³ at constant temperature.
p₂ = p₁V₁ ÷ V₂ = (100 000 × 0.6) ÷ 0.2 = 300 000 Pa
For a fixed mass of gas at constant volume, raising the Kelvin temperature makes the molecules hit the walls harder and more often, so the pressure rises in proportion:
Watch out — use kelvin! The gas laws only work with Kelvin temperatures. Putting °C into p₁/T₁ = p₂/T₂ gives the wrong answer (and dividing by 0 °C is meaningless). Always convert first.
Gas at 100 000 Pa and 300 K is heated to 450 K at constant volume.
p₂ = p₁ × T₂ ÷ T₁ = 100 000 × 450 ÷ 300 = 150 000 Pa
Tap an equation, then tap what it is used for.
Density: ρ = m / V
Pressure: p = F / A
Pressure in a liquid: p = h × ρ × g
Thermal energy (P): ΔQ = m × c × ΔT
°C → K: T = θ + 273 (absolute zero = 0 K = −273 °C)
Boyle's law: p₁V₁ = p₂V₂ (constant T)
Pressure law: p₁/T₁ = p₂/T₂ (constant V, use kelvin!)
You've covered all of 4PH1 Section 5 — units, density & pressure, change of state, and ideal gas molecules. Press Finish to see your score.
You've worked through Solids, Liquids & Gases for Edexcel International GCSE Physics (4PH1). 🎉
Your stars: 0 / 0
Next: test yourself in the Evaluate stage Confidence Quiz, then lock it in with Verify.