Squeeze a syringe and the gas pressure rises; put a balloon in the fridge and it shrinks. Hold one quantity fixed, change another, and the links between a gas’s pressure, volume and temperature appear.
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The container holds 1 mol of ideal gas: 22.4 L at 0 °C and 1 atm. Molecule speeds follow the temperature qualitatively; their number is not the real count. Real gases depart from ideal behaviour at low temperature or high pressure, and may even liquefy.
Gas pressure comes from molecules constantly striking the walls. In 1662 Boyle found that at constant temperature the pressure of a fixed amount of gas is inversely proportional to its volume: PV is constant. Squeeze the gas into less room and the molecules hit the walls more often, so the pressure rises.
Charles and Gay-Lussac studied temperature. At constant pressure a gas’s volume changes linearly with temperature; extend the line and the volume reaches zero near −273 °C. That is absolute zero, which defines the absolute scale T(K) = t(°C) + 273. In absolute temperature V ∝ T, and at constant volume P ∝ T.
Combining these with Avogadro’s law gives the ideal gas equation PV = nRT. Bicycle pumps, hot-air balloons, pressure cookers and tyres that burst on hot days can all be explained with these laws.