For a given amount of gas at low density, two empirical laws describe its behaviour. Boyle's law (Robert Boyle, 1662): at constant temperature, the pressure of a gas is inversely proportional to its volume, P∝V1. Charles' law (Jacques Charles): at constant pressure, the volume of a gas is directly proportional to its absolute temperature, V∝T. Combining the two gives PV=CT, where the constant C turns out to be proportional to the number of gas particles N (considering two identical gas containers merged into one doubles both V and N while P,T stay fixed): C=Nk, where k is the universal Boltzmann constant, k=1.381×10−23 J K−1. This gives the ideal gas law, PV=NkT. Writing N=μNA (with Avogadro's number NA=6.023×1023 mol−1, the number of carbon atoms in exactly 12 g of 12C) and defining the universal gas constant R=NAk=8.314 J mol−1K−1 turns this into PV=μRT for μ moles of gas -- the equation of state for an ideal gas, valid only at thermodynamic equilibrium. One mole of any ideal gas occupies 22.4 L at STP (273 K, 1.013×10⁵ Pa) and about 24.6 L at room temperature (300 K).