Derive the ideal gas law, Eq. ( 10 ). Begin with the pressure integral (Eq. 9 ) and the Maxwell-Boltzmann velocity distribution functio,
$$n_{v} d v=n\left(\frac{m}{2 \pi k T}\right)^{3 / 2} e^{-m v^{2} / 2 k T} 4 \pi v^{2} d v$$
$$\begin{aligned}&P_{g}=n k T\\&P=\frac{1}{3} \int_{0}^{\infty} m n_{v} v^{2} d v\end{aligned}$$