This mini-lesson walks you through the whole of AQA Topic 4.3 — Particle Model of Matter: density, the three states and how particles are arranged, changes of state, internal energy, specific heat capacity and latent heat, and how gas particles create pressure.
Work through each screen, answer the questions as you go (some are wordy, some are calculations) and collect ⭐ stars. Press Start when you're ready.
Density tells you how much mass is squeezed into a given volume. A dense material has a lot of mass in a small space.
The symbol ρ is the Greek letter "rho". Density can also be quoted in g/cm³ — just keep your units consistent.
A metal block has a mass of 240 g and a volume of 30 cm³.
ρ = 240 ÷ 30 = 8 g/cm³
The particle model explains why the same substance is usually densest as a solid and least dense as a gas:
Required practical: find density with a balance and ρ = m ÷ V. For a regular solid, measure sides and calculate the volume. For an irregular solid or a liquid, use a eureka (displacement) can — the volume of water pushed out equals the object's volume.
Tap the state that matches each particle description.
Adding or removing energy moves a substance between states. Each change has a name:
Key idea: changes of state are physical, not chemical. No new substance is made, the mass is conserved, and you can always get the original substance back by reversing the change (e.g. freeze the water and you have ice again).
Watch out — particles don't change size. When something melts, boils or expands, the particles themselves stay exactly the same size and number. What changes is only their spacing and how they move — they spread out and move more freely, they do not grow or shrink.
The internal energy of a substance is the total energy of all its particles. It is made of two parts:
Heating a substance raises its internal energy. That extra energy does one of two jobs:
Don't confuse internal energy with temperature. Internal energy = total kinetic + total potential energy of all the particles. Temperature only tracks the kinetic part. So on a plateau the temperature is fixed, yet the internal energy is still rising (the potential part is going up).
Heat ice steadily and plot temperature against time (or energy supplied). The two flat sections are the changes of state — the temperature stays constant while particles gain potential energy and the forces between them are overcome.
Analogy — the "unlocking" energy: on a flat plateau the energy isn't speeding the particles up, it's spent unlocking them from one another (pulling them apart against their attractions). That's why the thermometer pauses — kinetic energy isn't changing, only potential energy is.
Tap an event, then tap whether the supplied energy raises the temperature or changes the state.
When energy raises the temperature (the sloped parts of the graph), use the specific heat capacity equation:
The specific heat capacity c is the energy to raise 1 kg of a substance by 1 °C. Water's is high (4200 J/kg°C).
Analogy — water is a "thermal sponge". A high specific heat capacity means a substance soaks up a lot of energy for only a small temperature rise (and gives it back slowly when cooling). That is why water is slow to heat and slow to cool — handy for car radiators and central-heating systems, and why coastal climates are milder.
Heating 0.5 kg of water (c = 4200) by 30 °C:
ΔE = 0.5 × 4200 × 30 = 63 000 J (63 kJ)
To change state at constant temperature (the flat parts of the graph) you need the specific latent heat L — the energy to change the state of 1 kg of a substance with no temperature change:
Melting 2 kg of ice (specific latent heat of fusion L = 334 000 J/kg):
E = 2 × 334 000 = 668 000 J (668 kJ)
Physics only: this gas-pressure section is on the Physics paper, not the Combined Science Trilogy paper.
Gas particles move quickly and randomly. Each time one collides with a wall it bounces off and gives the wall a tiny push. Billions of collisions every second add up to a steady pressure on the container.
Analogy — drumming on the walls: picture thousands of tiny rubber balls thrown nonstop at the inside of a box. No single ball does much, but the constant drumming of all of them keeps a steady outward push — that push, per unit area, is the gas pressure.
Raise the temperature at constant volume and the particles move faster, so they hit the walls harder and more often — the pressure rises.
For a fixed mass of gas at constant temperature, pressure and volume are linked:
Squeeze the gas into a smaller volume and the same particles hit the walls more often, so the pressure rises. Also, doing work on a gas (e.g. quickly pushing a bike pump) transfers energy to it and can raise its temperature.
Analogy — same balls, half the room. The number of particles never changes. Halve the volume and you crowd exactly the same particles into half the space, so each one reaches a wall in half the time and hits it twice as often — double the volume, halve the pressure; halve the volume, double the pressure. That's why p × V stays constant.
Gas at p₁ = 100 kPa fills V₁ = 6 m³. It is squeezed to V₂ = 2 m³ at constant temperature. Find p₂.
p₂ = p₁V₁ ÷ V₂ = (100 × 6) ÷ 2 = 300 kPa
Density: ρ = m ÷ V
Heating (temperature change): ΔE = m c Δθ
Changing state (latent heat): E = m L
Gas (constant temperature): p₁V₁ = p₂V₂ (Physics only)
You've covered all of AQA 4.3 — density & the states of matter, changes of state & internal energy, specific heat capacity, latent heat, and gas pressure. Press Finish to see your score.
You've worked through the Particle Model of Matter for AQA GCSE Physics. 🎉
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