A gas has no fixed shape or volume — it fills whatever container it is put in. The kinetic theory of gases explains this behaviour by picturing a gas as a huge number of tiny molecules in constant, random motion. Everything we measure about a gas in the lab — its pressure, temperature and volume — is really a large-scale average of what these countless molecules are doing.
An ideal gas is a simplified model that obeys the gas laws exactly at all pressures and temperatures. The kinetic theory rests on a few key assumptions:
- A gas consists of a very large number of identical molecules in continuous random motion.
- The size of a molecule is negligible compared with the average distance between molecules, so the molecules themselves occupy almost no volume.
- There is no force of attraction or repulsion between molecules except during collisions.
- Collisions between molecules and with the walls are perfectly elastic — kinetic energy is conserved — and take negligible time.
- Between collisions a molecule moves in a straight line at constant velocity (no external force).
From these assumptions and from experiment we get the gas laws, each describing how two of the quantities $P$, $V$, $T$ are related when the third is held fixed:
- Boyle's law (constant $T$): $PV=\text{constant}$, so $P\propto\frac{1}{V}$. Squeeze a gas into half the volume and its pressure doubles.
- Charles' law (constant $P$): $\frac{V}{T}=\text{constant}$, so $V\propto T$. Heating a gas at fixed pressure makes it expand.
- Gay-Lussac's law (constant $V$): $\frac{P}{T}=\text{constant}$, so $P\propto T$.
- Avogadro's law: equal volumes of all gases at the same $T$ and $P$ contain equal numbers of molecules.
Combining these gives the ideal gas equation: $PV=nRT$, where $n$ is the number of moles and $R=8.314\ \text{J}\,\text{mol}^{-1}\,\text{K}^{-1}$ is the universal gas constant. Writing $n=\frac{N}{N_A}$ (with $N$ the number of molecules and $N_A=6.022\times10^{23}$ Avogadro's number) and defining the Boltzmann constant $k_B=\frac{R}{N_A}=1.38\times10^{-23}\ \text{J/K}$, the same law becomes $PV=Nk_BT$. Temperatures here are always in kelvin ($T(\text{K})=t(^\circ\text{C})+273$).