Section 1 of 9The kinetic model of a gas
The kinetic theory says that all matter is made of tiny particles (atoms or molecules) that are always moving. In a gas the particles are far apart compared with their own size, so there are almost no forces between them except during collisions. They move in straight lines at high speed until they hit something, then change direction.
Section 2 of 9Evidence: Brownian motion
Smoke particles viewed through a microscope in a glass cell jiggle in an irregular way.
Section 3 of 9How a gas produces pressure
Pressure is the force acting normally (at right angles) on each unit of area:
p = F / A
where p is pressure in pascals (Pa, or N m−2), F is force in newtons (N) and A is area in square metres (m2).
When a molecule bounces off a wall its momentum changes direction, so the wall exerts a force on the molecule and, by Newton's third law, the molecule exerts an equal and opposite force on the wall.
Section 4 of 9Changing the pressure
The pressure on the walls depends on two things: how often molecules hit the wall and how hard each hit is.
Section 5 of 9Gases compared with solids and liquids
| Property | Solid | Liquid | Gas |
|---|---|---|---|
| Particle spacing | Close, regular | Close, irregular | Very far apart |
| Movement | Vibrate about fixed positions | Slide past each other | Fast, random, free |
| Compressible? | No | Almost not | Yes, easily |
A gas fills any container because its particles are not held together. A sealed gas exerts pressure on every part of the container, not just the bottom, because the particles move in all directions.
Section 6 of 9Why gases are easy to compress and spread out
Because the particles in a gas are so far apart, there is mostly empty space between them.
The same model explains diffusion.
Link to atmospheric pressure
The air around us is a gas, and the pressure it exerts, about 1.0 × 105 Pa at sea level, is due to the same collisions.
Section 7 of 9Worked examples
A rectangular wall of a gas tank has area 0.40 m2. The gas exerts a force of 40 000 N on it. Calculate the pressure.
p = F / A = 40 000 N / 0.40 m2 = 100 000 Pa (1.0 × 105 Pa). This is roughly atmospheric pressure.
A sealed syringe of air is pushed so that its volume halves while the temperature stays the same. Explain, using particles, why the pressure rises.
The same number of molecules now occupy half the volume, so the molecules are closer together.
Worked examplesEach molecule travels a shorter distance between hits on the walls, so the number of collisions per second on each square metre of wall roughly doubles.Average speed is unchanged (temperature constant), so each collision is as forceful as before.Greater total force per unit area means higher pressure.
Section 8 of 9Key terms
| Term | Meaning |
|---|---|
| Kinetic theory | Model in which matter consists of particles in constant motion. |
| Brownian motion | Random jiggling of visible particles caused by collisions with fast-moving invisible molecules. |
| Pressure | Force acting normally per unit area, p = F / A. |
| Pascal (Pa) | Unit of pressure, equal to 1 N m−2. |
| Random motion | Movement in no fixed direction with a range of speeds. |