This problem deals with the idea of the escape velocity of a particle from a body such as the Earth's surface. Recall from your course in physics that the potential energy of two masses, $m_{1}$ and $m_{2}$, separated by a distance $r$ is given by
$$
V(r)=-\frac{G m_{1} m_{2}}{r}
$$
(note the similarity with Coulomb's law) where $G=6.67 \times 10^{-11} \mathrm{~J} \cdot \mathrm{m} \cdot \mathrm{kg}^{-1}$ is called the gravitional constant. Suppose a particle of mass $m$ has a velocity $u$ perpendicular to the Earth's surface. Show that the minimum velocity that the particle must have in order to escape the Earth's surface (its escape velocity) is given by
$$
u=\left(\frac{2 G M_{\text {earth }}}{R_{\text {earth }}}\right)^{1 / 2}
$$
Given that $M_{\text {earth }}=5.98 \times 10^{24} \mathrm{~kg}$ is the mass of the Earth and $R_{\text {earth }}=6.36 \times 10^{6} \mathrm{~m}$ is its mean radius, calculate the escape velocity of a hydrogen molecule and a nitrogen molecule. What temperature would each of these molecules have to have so that their average speed exceeds their escape velocity?